diff options
author | Karl Berry <karl@freefriends.org> | 2023-11-17 22:02:57 +0000 |
---|---|---|
committer | Karl Berry <karl@freefriends.org> | 2023-11-17 22:02:57 +0000 |
commit | d750d4833a1999a7902080b4a55e3e89eead497d (patch) | |
tree | c5670d1d100bd424cfa1854a6713264cd21cf0ca /Master/texmf-dist/source/latex | |
parent | 6719122c781ae5bcef2f225c8f5246f31dacf704 (diff) |
thermodynamics (17nov23)
git-svn-id: svn://tug.org/texlive/trunk@68881 c570f23f-e606-0410-a88d-b1316a301751
Diffstat (limited to 'Master/texmf-dist/source/latex')
-rw-r--r-- | Master/texmf-dist/source/latex/thermodynamics/thermodynamics.dtx | 4627 | ||||
-rw-r--r-- | Master/texmf-dist/source/latex/thermodynamics/thermodynamics.ins | 13 |
2 files changed, 2618 insertions, 2022 deletions
diff --git a/Master/texmf-dist/source/latex/thermodynamics/thermodynamics.dtx b/Master/texmf-dist/source/latex/thermodynamics/thermodynamics.dtx index a9c8348997d..7d6904c9ee3 100644 --- a/Master/texmf-dist/source/latex/thermodynamics/thermodynamics.dtx +++ b/Master/texmf-dist/source/latex/thermodynamics/thermodynamics.dtx @@ -1,5 +1,5 @@ % \iffalse meta-comment -% File: thermodynamics.dtx Copyright (C) 2021 Karl D. Hammond +% File: thermodynamics.dtx Copyright (C) 2022-2023 Karl D. Hammond % % Karl D. Hammond % Chemical Engineering Program @@ -15,7 +15,7 @@ % version 2005/12/01 or later. % % This work has the LPPL maintenance status `maintained'. -% +% % The Current Maintainer of this work is K. D. Hammond. % % This work consists of the files thermodynamics.dtx and thermodynamics.ins @@ -24,40 +24,54 @@ % \fi % % \iffalse +%^^A FIXME: need correct date of release once you update this +%^^X\GetIdInfo $Id: thermodynamics.dtx 2.00 2023/11/16 Karl D. Hammond <hammondkd@missouri.edu> $ +%^^X {thermodynamics notation} %<*driver> +%^^X\ProvidesFile{\ExplFileName} \ProvidesFile{thermodynamics.dtx} %</driver> % %<package>\NeedsTeXFormat{LaTeX2e} +%<package>\RequirePackage{expl3} %<package>\ProvidesPackage{thermodynamics} %<*package> - [2022/04/29 v1.00 thermodynamics package] + [2023/11/16 v2.00 thermodynamics notation] %</package> -% +%^^X {\ExplFileDate}{\ExplFileVersion}{\ExplFileDescription} %<*driver> \documentclass[11pt,letterpaper]{ltxdoc} -\usepackage[margin=1in,left=1.85in]{geometry} +%^^X\bool_set_false:N \l__codedoc_allow_indexing_bool +\usepackage[margin=0.80in,left=2.05in]{geometry} \usepackage[T1]{fontenc} -\usepackage[full]{textcomp} +\usepackage{textcomp} \usepackage{amsmath} \usepackage{pxfonts} \usepackage{array} \usepackage{booktabs} \usepackage{footmisc} -\usepackage[labelfont=bf,labelsep=period]{caption} -%\EnableCrossrefs -%\CodelineIndex +\usepackage[labelfont=bf,labelsep=period,font=small]{caption} +\GetFileInfo{thermodynamics.dtx} +\usepackage{thermodynamics}[\filedate\space\fileversion] +\DisableCrossrefs +\CodelineIndex \PageIndex \CodelineNumbered \RecordChanges -%\OnlyDescription +%^^X Preparing to use l3doc.cls, but it's not quite mature yet.... +%^^A\DisableDocumentation +%^^A\DisableImplementation +%^^X\ExplSyntaxOff +\let\tn\cs +\let\env\texttt +\let\pkg\textsf \begin{document} \DocInput{thermodynamics.dtx} \end{document} %</driver> % \fi % -% \CheckSum{2286} +% \CheckSum{2387} % % \CharacterTable % {Upper-case \A\B\C\D\E\F\G\H\I\J\K\L\M\N\O\P\Q\R\S\T\U\V\W\X\Y\Z @@ -76,12 +90,28 @@ % Right brace \} Tilde \~} % % \changes{v1.00}{2022/04/29}{Initial public release} +% \changes{v2.00}{2023/11/16}{Revision to use \LaTeX3 +% (\pkg{expl3}/\pkg{xparse}) syntax layer} % -% \GetFileInfo{thermodynamics.dtx} +% \newcommand*{\setmarginparsize}[1] +% {\bgroup +% \RenewExpandableDocumentCommand{\MacroFont}{}{\fontencoding\encodingdefault +% \fontfamily\ttdefault +% \fontseries\mddefault +% \fontshape\shapedefault +% #1} +% } +% \newcommand*{\restoremarginparsize}{\egroup} % +% \GetFileInfo{thermodynamics.dtx} +%^^X \title{The \textsf{thermodynamics} package\thanks{This document +%^^X corresponds to \textsf{thermodynamics}~\ExplFileVersion, +%^^X dated \ExplFileDate.}} % \title{The \textsf{thermodynamics} package\thanks{This document -% corresponds to \textsf{thermodynamics}~\fileversion, dated \filedate.}} +% corresponds to \textsf{thermodynamics}~\fileversion, +% dated \filedate.}} % \author{Karl D. Hammond \\ \texttt{hammondkd@missouri.edu}} +%^^X \date{\ExplFileDate} % \date{\filedate} % \maketitle % @@ -97,48 +127,21 @@ % options. % \end{abstract} % -% \newcommand*{\thermounderline}[1]{% -% \mkern2mu\underline{\mkern-2mu #1\mkern-3mu}\mkern3mu% -% } -% \newcommand*{\thermooverline}[1]{% -% \mkern2mu\overline{\mkern-2mu #1\mkern-2mu}\mkern2mu% -% } -% \newcommand*{\Partial}[3]{\ensuremath{\left(\frac{\partial #1}{\partial #2}\right)_{#3}}} -% \newcommand*{\Ut}{\mkern1mu\underline{\mkern-1mu U\mkern-4mu}\mkern4mu} -% \newcommand*{\Upm}[2][]{\mkern2mu\overline{\mkern-2mu U_{#2}^{#1}\mkern-2mu}\mkern2mu} -% \newcommand*{\Ht}{\mkern1mu\underline{\mkern-1mu H\mkern-4mu}\mkern4mu} -% \newcommand*{\Hm}{H} -% \newcommand*{\Hpm}[2][]{\mkern2mu\overline{\mkern-2mu H_{#2}^{#1}\mkern-1mu}\mkern1mu} -% \newcommand*{\Ft}{\mkern1mu\underline{\mkern-1mu A\mkern-4mu}\mkern4mu} -% \newcommand*{\Gt}{\mkern1mu\underline{\mkern-1mu G\mkern-4mu}\mkern4mu} -% \newcommand*{\Gpm}[2][]{\mkern2mu\overline{\mkern-2mu G_{#2}^{#1}\mkern-1mu}\mkern1mu} -% \newcommand*{\Spm}[2][]{\mkern2mu\overline{\mkern-2mu S_{#2}^{#1}\mkern-1mu}\mkern1mu} -% \newcommand*{\Vpm}[2][]{\mkern1mu\overline{\mkern-1mu V_{\mkern-2mu #2}^{#1}\mkern-2mu}\mkern2mu} -% \newcommand*{\St}{\mkern1mu\underline{\mkern-1mu S\mkern-3mu}\mkern3mu} -% \newcommand*{\Vt}{\mkern3mu\underline{\mkern-3mu V\mkern-4mu}\mkern4mu} -% \newcommand*{\Lt}{\mkern1mu\underline{\mkern-1mu \Omega\mkern-4mu}\mkern4mu} -% \newcommand*{\cPpm}[2][]{\mkern2mu\overline{\mkern-2mu C_{P,#2}^{#1}\mkern-1mu}\mkern1mu} -% -% \newcommand*{\Nt}{n} -% \newcommand*{\allNs}{\vec\Nt} -% \newcommand*{\allNsbut}[2][j]{\Nt_{#1\neq #2}} -% \newcommand*{\allXs}{\vec x} -% +%^^X \begin{documentation} % \section{Introduction} % The purpose of this package is to simplify the typesetting of equations in -% thermodynamics, specifically chemical engineering thermodynamics, which are +% thermodynamics, particularly chemical engineering thermodynamics, which are % often cumbersome to enter. For example, consider the following equation: % \begin{equation} -% d\Ut = \Partial{\Ut}{\St}{\Vt,\allNs} \mkern-10mu d\St -% + \Partial{\Ut}{\Vt}{\St,\allNs} \mkern-10mu d\Vt -% + \sum_{i=1}^C \Partial{\Ut}{\Nt_i}{\St,\Vt,\allNsbut{i}} -% \mkern-10mu d\Nt_i. +% d\Ut = \Partial*{\Ut}{\St}{\Vt,\allNs} \,d\St +% + \Partial*{\Ut}{\Vt}{\St,\allNs} \,d\Vt +% + \sumall_i \Partial*{\Ut}{\Nt_i}{\St,\Vt,\allNsbut{i}} d\Nt_i. % \label{eq:chain-rule-U} % \end{equation} % This equation is pretty basic, and equations like it occur all the time in % thermodynamics. Without this package, you might typeset it like this: % \begin{verbatim} -% d\underline{U} = +% \[ d\underline{U} = % \left(\frac{\partial\underline{U}} % {\partial\underline{S}}\right)_{\underline{V},\vec{n}} % d\underline{S} @@ -147,7 +150,7 @@ % d\underline{V} % + \sum_{i=1}^C \left(\frac{\partial\underline{U}} % {\partial n_i}\right)_{\underline{S},\underline{V},n_{j\neq i}} -% dn_i. +% dn_i. \] %\end{verbatim} % This is a lot of code, and even then the output is slightly clunky: % \[ d\underline{U} = @@ -162,15 +165,19 @@ % dn_i. % \] % It is also frustratingly difficult to change one's notes or handouts from one -% textbook that uses, say, $n_1$ to denotes moles of component 1 to another +% textbook that uses, say, $n_1$ to denote moles of component 1 to another % textbook that uses $N_1$ for the same quantity, or perhaps denotes the % total internal energy as $U$ or $U^t$ rather than $\Ut$. % For example, if you wanted it to be -% \[ -% dU = \Partial{U}{S}{V,N_1,\dotsc,N_n} \mkern-15mu dS -% + \Partial{U}{V}{S,N_1,\dotsc,N_n} \mkern-15mu dV -% + \sum_{i=1}^n \Partial{U}{N_i}{S,V,N_1,\dotsc,[N_i],\dotsc,N_n} -% \mkern-20mu dN_i +% \[\begin{thermomolesrange} +% \begin{thermoextensiveplain} +% \RenewExpandableDocumentCommand{\Nt}{}{N} +% \RenewExpandableDocumentCommand{\ncomponents}{}{\mathcal{C}} +% d\Ut = \Partial*{\Ut}{\St}{\Vt,\allNs} \,d\St +% + \Partial*{\Ut}{\Vt}{\St,\allNs} \,d\Vt +% + \sumall_i \Partial*{\Ut}{\Nt_i}{\St,\Vt,\allNsbut{i}} d\Nt_i. +% \end{thermoextensiveplain} +% \end{thermomolesrange} % \] % without changing any of your code---to update it across all handouts, exams, % and homework sets after changing textbooks, say---you would be out of luck @@ -193,43 +200,36 @@ % % The package handles second derivatives, too. For example, % \begin{verbatim} -% \Partial*{\Hm}{T}{P} = T\Partial*{\Sm}{T}{P} -% = -T\PartialSecond*{\Gm}{T}{P} = \cP +% \[ \Partial*{\Hm}{T}{P} = T\Partial*{\Sm}{T}{P} +% = -T\PartialSecond*{\Gm}{T}{P} = \cP \] %\end{verbatim} % renders (using the default options) -% \[ \left(\frac{\partial H}{\partial T}\right)_P \mkern-8mu -% = T\left(\frac{\partial S}{\partial T}\right)_P \mkern-8mu -% = -T\left(\frac{\partial^2 G}{\partial T^2}\right)_P \mkern-8mu -% = C_P \] +% \[ \Partial*{\Hm}{T}{P} = T\Partial*{\Sm}{T}{P} +% = -T\PartialSecond*{\Gm}{T}{P} = \cP. \] % Similarly, macros are defined for mixed second partial derivatives that allow % things like % \begin{verbatim} -% \Partial*{\Gpm_i}{P}{T,\allNs} +% \[ \Partial*{\Gpm_i}{P}{T,\allNs} % = \PartialMixSecond*{\Gt}{P}{\Nt_i}{T,\allNsbut{i}} % = \PartialMixSecond*{\Gt}{\Nt_i}{P}{T,\allNsbut{i}} -% = \Partial*{Vt}{\Nt_i}{T,P,\allNsbut{i}} = \Vpm_i +% = \Partial*{\Vt}{\Nt_i}{T,P,\allNsbut{i}} = \Vpm_i \], %\end{verbatim} % which renders -% \[ \left(\frac{\partial \Gpm{i}}{\partial P}\right)_{T,\allNs} -% \mkern-15mu% -% = \left(\frac{\partial^2 \Gt}{\partial P\partial n_i}\right)_{T,\allNsbut{i}} -% \mkern-15mu% -% = \left(\frac{\partial^2 \Gt}{\partial n_i\partial P}\right)_{T,\allNsbut{i}} -% \mkern-15mu% -% = \left(\frac{\partial \Vt}{\partial n_i}\right)_{T,P,\allNsbut{i}} -% \mkern-15mu% -% = \Vpm{i} +% \[ \Partial*{\Gpm_i}{P}{T,\allNs} +% = \PartialMixSecond*{\Gt}{P}{\Nt_i}{T,\allNsbut{i}} +% = \PartialMixSecond*{\Gt}{\Nt_i}{P}{T,\allNsbut{i}} +% = \Partial*{\Vt}{\Nt_i}{T,P,\allNsbut{i}} = \Vpm_i % \] % using the defaults. % -% ^^A------------------------------------------------------------------------- +%^^A------------------------------------------------------------------------- % % \section{Using the Package} \label{sec:using} % There are three categories of macros defined in this package: macros % that produce symbols (or groups of them), macros that typeset derivatives, % and macros that are used internally that the user need not know about. -% There are also several environments that allow the user to switch locally -% between different delimiters on partial derivatives. +% There are also several environments that allow the user to change notation +% temporarily. % % \subsection{Predefined Symbols} % The macros used to produce symbols fall into five categories: extensive @@ -255,10 +255,10 @@ % How these symbols are rendered can be customized by package options. As long % as the user consistently uses \cs{Ut} to render the total internal energy, % \cs{Um} to render the molar internal energy, and so forth, switching notation -% from, say, $\thermounderline{U}$ to $U^t$ for extensive properties is trivial. +% from, say, $\Ut$ to $U^t$ for extensive properties is trivial. % -% ^^A \DescribeMacro{\cP} -% ^^A \DescribeMacro{\cV} +% \DescribeMacro{\cP} +% \DescribeMacro{\cV} % \DescribeMacro{\cPt} % \DescribeMacro{\cVt} % \DescribeMacro{\cPs} @@ -268,31 +268,28 @@ % The heat capacities (see Table~\ref{table:conveniences}) are generally % assumed to be molar (e.g., \cs{cP} is interpreted to be the molar heat % capacity). To get the specific heat capacities, the macros \cs{cPs} and -% \cs{cVs} are provided, which by default render as $\hat C_P$ and $\hat C_V$, +% \cs{cVs} are provided, which by default render as $\cPs$ and $\cVs$, % respectively. There are also extensive versions, so \cs{cPt} and \cs{cVt} -% will render as $\thermounderline{C}_P$ and $\thermounderline{C}_V,$ +% will render as $\cPt$ and $\cVt,$ % respectively. Note that \cs{cP} and friends require you to surround -% \cs{text} with brackets if the portion with \cs{text} in it is not the last -% argument. For example, \verb"\cP_i^\text{A}" will work as expected, but -% \verb"\cP^\text{A}_i" will not: you need to use \verb"\cP^{\text{A}}_i". -% Using \verb"\cP^\IG_i" will work as expected. +% \cs{text} with brackets. For example, \verb"\cP_i^\text{A}" will not work, +% nor will \verb"\cP^\text{A}_i"; you need to use \verb"\cP_i^{\text{A}}" and +% \verb"\cP^{\text{A}}_i". Using \verb"\cP^\IG_i" will work as expected. % % You can also get partial molar heat capacities via \cs{cPpm} and \cs{cVpm}, % though the latter's mathematical definition is a bit hard to wrap one's head % around: % \begin{verbatim} -% \[ \cVpm_i = \Partial{\cVt}{\Nt_i}{T,P,\allNsbut{i}} +% \[ \cVpm_i = \Partial*{\cVt}{\Nt_i}{T,P,\allNsbut{i}} % = \frac{\partial}{\partial\Nt_i} % \left[ -T\PartialSecond{\Ft}{T}{\Vt,\allNs} % \right]_{T,P,\allNsbut{i}} \] %\end{verbatim} % yields -% \[ \thermooverline{C_{V,i}} -% = \left(\frac{\partial\thermounderline{C}_V} -% {\partial\Nt_i}\right)_{T,P,\allNsbut{i}} +% \[ \cVpm{i} = \Partial*{\cVt}{\Nt_i}{T,P,\allNsbut{i}} % = \frac{\partial}{\partial\Nt_i} -% \left[ -T\left(\frac{\partial^2\Ft}{\partial T^2}\right)_{\Vt,\allNs} -% \right]_{T,P,\allNsbut{i}} \] +% \left[ -T\PartialSecond{\Ft}{T}{\Vt,\allNs} +% \right]_{T,P,\allNsbut{i}}. \] % % \begin{table} % \caption{Commands defined in this package to represent extensive @@ -300,80 +297,152 @@ % These macros should be used even if the symbol the user % wishes to use does not match the command used (e.g., \cs{Ft} % for total Helmholtz free energy even if it ends up being set as -% $\thermounderline{A}$)\@. +% $\Ft$)\@. % } % \label{table:symbols} -% \SpecialUsageIndex{\Qt}\relax -% \SpecialUsageIndex{\Qm}\relax -% \SpecialUsageIndex{\Qs}\relax -% \SpecialUsageIndex{\Wt}\relax -% \SpecialUsageIndex{\Wm}\relax -% \SpecialUsageIndex{\Ws}\relax -% \SpecialUsageIndex{\Et}\relax -% \SpecialUsageIndex{\Em}\relax -% \SpecialUsageIndex{\Es}\relax -% \SpecialUsageIndex{\Epm}\relax -% \SpecialUsageIndex{\Ut}\relax -% \SpecialUsageIndex{\Um}\relax -% \SpecialUsageIndex{\Us}\relax -% \SpecialUsageIndex{\Upm}\relax -% \SpecialUsageIndex{\Ht}\relax -% \SpecialUsageIndex{\Hm}\relax -% \SpecialUsageIndex{\Hs}\relax -% \SpecialUsageIndex{\Hpm}\relax -% \SpecialUsageIndex{\St}\relax -% \SpecialUsageIndex{\Sm}\relax -% \SpecialUsageIndex{\Ss}\relax -% \SpecialUsageIndex{\Spm}\relax -% \SpecialUsageIndex{\Ft}\relax -% \SpecialUsageIndex{\Fm}\relax -% \SpecialUsageIndex{\Fs}\relax -% \SpecialUsageIndex{\Fpm}\relax -% \SpecialUsageIndex{\Gt}\relax -% \SpecialUsageIndex{\Gm}\relax -% \SpecialUsageIndex{\Gs}\relax -% \SpecialUsageIndex{\Gpm}\relax -% \SpecialUsageIndex{\At}\relax -% \SpecialUsageIndex{\Am}\relax -% \SpecialUsageIndex{\As}\relax -% \SpecialUsageIndex{\Apm}\relax -% \SpecialUsageIndex{\Nt}\relax -% \SpecialUsageIndex{\Lt}\relax -% \SpecialUsageIndex{\Lm}\relax -% \SpecialUsageIndex{\Ls}\relax -% \SpecialUsageIndex{\Lpm}\relax -% \SpecialUsageIndex{\Bt}\relax -% \SpecialUsageIndex{\Bm}\relax -% \SpecialUsageIndex{\Bs}\relax -% \SpecialUsageIndex{\Bpm}\relax -% \SpecialUsageIndex{\Mt}\relax -% \SpecialUsageIndex{\Mm}\relax -% \SpecialUsageIndex{\Ms}\relax -% \SpecialUsageIndex{\Mpm}\relax +%^^A TODO The \leavevmode macro here is to prevent whitespace from building +%^^A up due to a bug in old versions of hypdoc. It should be harmless to +%^^A leave it in there, but consider removing it at some point. +% \leavevmode +% \SpecialMacroIndex{\Qt}\relax +% \SpecialMacroIndex{\Qm}\relax +% \SpecialMacroIndex{\Qs}\relax +% \SpecialMacroIndex{\Wt}\relax +% \SpecialMacroIndex{\Wm}\relax +% \SpecialMacroIndex{\Ws}\relax +% \SpecialMacroIndex{\Et}\relax +% \SpecialMacroIndex{\Em}\relax +% \SpecialMacroIndex{\Es}\relax +% \SpecialMacroIndex{\Epm}\relax +% \SpecialMacroIndex{\EEt}\relax +% \SpecialMacroIndex{\EE}\relax +% \SpecialMacroIndex{\EEs}\relax +% \SpecialMacroIndex{\EEpm}\relax +% \SpecialMacroIndex{\ERt}\relax +% \SpecialMacroIndex{\ER}\relax +% \SpecialMacroIndex{\ERs}\relax +% \SpecialMacroIndex{\ERpm}\relax +% \SpecialMacroIndex{\Ut}\relax +% \SpecialMacroIndex{\Um}\relax +% \SpecialMacroIndex{\Us}\relax +% \SpecialMacroIndex{\Upm}\relax +% \SpecialMacroIndex{\UEt}\relax +% \SpecialMacroIndex{\UE}\relax +% \SpecialMacroIndex{\UEs}\relax +% \SpecialMacroIndex{\UEpm}\relax +% \SpecialMacroIndex{\URt}\relax +% \SpecialMacroIndex{\UR}\relax +% \SpecialMacroIndex{\URs}\relax +% \SpecialMacroIndex{\URpm}\relax +% \SpecialMacroIndex{\Ht}\relax +% \SpecialMacroIndex{\Hm}\relax +% \SpecialMacroIndex{\Hs}\relax +% \SpecialMacroIndex{\Hpm}\relax +% \SpecialMacroIndex{\HEt}\relax +% \SpecialMacroIndex{\HE}\relax +% \SpecialMacroIndex{\HEs}\relax +% \SpecialMacroIndex{\HEpm}\relax +% \SpecialMacroIndex{\HRt}\relax +% \SpecialMacroIndex{\HR}\relax +% \SpecialMacroIndex{\HRs}\relax +% \SpecialMacroIndex{\HRpm}\relax +% \SpecialMacroIndex{\St}\relax +% \SpecialMacroIndex{\Sm}\relax +% \SpecialMacroIndex{\Ss}\relax +% \SpecialMacroIndex{\Spm}\relax +% \SpecialMacroIndex{\SEt}\relax +% \SpecialMacroIndex{\SE}\relax +% \SpecialMacroIndex{\SEs}\relax +% \SpecialMacroIndex{\SEpm}\relax +% \SpecialMacroIndex{\SRt}\relax +% \SpecialMacroIndex{\SR}\relax +% \SpecialMacroIndex{\SRs}\relax +% \SpecialMacroIndex{\SRpm}\relax +% \SpecialMacroIndex{\Ft}\relax +% \SpecialMacroIndex{\Fm}\relax +% \SpecialMacroIndex{\Fs}\relax +% \SpecialMacroIndex{\Fpm}\relax +% \SpecialMacroIndex{\FEt}\relax +% \SpecialMacroIndex{\FE}\relax +% \SpecialMacroIndex{\FEs}\relax +% \SpecialMacroIndex{\FEpm}\relax +% \SpecialMacroIndex{\FRt}\relax +% \SpecialMacroIndex{\FR}\relax +% \SpecialMacroIndex{\FRs}\relax +% \SpecialMacroIndex{\FRpm}\relax +% \SpecialMacroIndex{\Gt}\relax +% \SpecialMacroIndex{\Gm}\relax +% \SpecialMacroIndex{\Gs}\relax +% \SpecialMacroIndex{\Gpm}\relax +% \SpecialMacroIndex{\GEt}\relax +% \SpecialMacroIndex{\GE}\relax +% \SpecialMacroIndex{\GEs}\relax +% \SpecialMacroIndex{\GEpm}\relax +% \SpecialMacroIndex{\GRt}\relax +% \SpecialMacroIndex{\GR}\relax +% \SpecialMacroIndex{\GRs}\relax +% \SpecialMacroIndex{\GRpm}\relax +% \SpecialMacroIndex{\At}\relax +% \SpecialMacroIndex{\Am}\relax +% \SpecialMacroIndex{\As}\relax +% \SpecialMacroIndex{\Apm}\relax +% \SpecialMacroIndex{\Nt}\relax +% \SpecialMacroIndex{\Lt}\relax +% \SpecialMacroIndex{\Lm}\relax +% \SpecialMacroIndex{\Ls}\relax +% \SpecialMacroIndex{\Lpm}\relax +% \SpecialMacroIndex{\LEt}\relax +% \SpecialMacroIndex{\LE}\relax +% \SpecialMacroIndex{\LEs}\relax +% \SpecialMacroIndex{\LEpm}\relax +% \SpecialMacroIndex{\LRt}\relax +% \SpecialMacroIndex{\LR}\relax +% \SpecialMacroIndex{\LRs}\relax +% \SpecialMacroIndex{\LRpm}\relax % \centering -% \begin{minipage}{4.12in}\renewcommand*{\footnoterule}{\vskip-1ex}% -% \centering\small -% \begin{tabular}{l l l l l} +% \begin{minipage}{\linewidth}\renewcommand*{\footnoterule}{\vskip-1.75ex}% +% \centering\scriptsize\setlength{\tabcolsep}{0.05in} +% \begin{tabular}{l l l l l l l l l l l l l} % \toprule -% Property & Total & Molar & Specific & Partial Molar \\ +% & & & & & \multicolumn{4}{c}{Excess} +% & \multicolumn{4}{c}{Residual (Departure)} \\ +% \cmidrule(r{0.5ex}){6-9} +% \cmidrule(l{0.5ex}){10-13} +% Property & Total & Molar & Specific & \parbox[b]{0.45in}{Partial Molar} +% & T & M & S & PM & T & M & S & PM \\ % \midrule -% Heat & \cs{Qt} & \cs{Qm} & \cs{Qs} & N/A \\ -% Work & \cs{Wt} & \cs{Wm} & \cs{Ws} & N/A \\ -% Total energy & \cs{Et} & \cs{Em} & \cs{Es} & \cs{Epm} \\ -% Internal energy & \cs{Ut} & \cs{Um} & \cs{Us} & \cs{Upm} \\ -% Enthalpy & \cs{Ht} & \cs{Hm} & \cs{Hs} & \cs{Hpm} \\ -% Entropy & \cs{St} & \cs{Sm} & \cs{Ss} & \cs{Spm} \\ -% Volume & \cs{Vt} & \cs{Vm} & \cs{Vs} & \cs{Vpm} \\ -% Helmholtz free energy & \cs{Ft} & \cs{Fm} & \cs{Fs} & \cs{Fpm} \\ -% Gibbs free energy & \cs{Gt} & \cs{Gm} & \cs{Gs} & \cs{Gpm} \\ +% Heat & \cs{Qt} & \cs{Qm} & \cs{Qs} & \\ +% Work & \cs{Wt} & \cs{Wm} & \cs{Ws} & \\ +% Total energy & \cs{Et} & \cs{Em} & \cs{Es} & \cs{Epm} +% & \cs{EEt} & \cs{EE} & \cs{EEs} & \cs{EEpm} +% & \cs{ERt} & \cs{ER} & \cs{ERs} & \cs{ERpm} \\ +% Internal energy & \cs{Ut} & \cs{Um} & \cs{Us} & \cs{Upm} +% & \cs{UEt} & \cs{UE} & \cs{UEs} & \cs{UEpm} +% & \cs{URt} & \cs{UR} & \cs{URs} & \cs{URpm} \\ +% Enthalpy & \cs{Ht} & \cs{Hm} & \cs{Hs} & \cs{Hpm} +% & \cs{HEt} & \cs{HE} & \cs{HEs} & \cs{HEpm} +% & \cs{HRt} & \cs{HR} & \cs{HRs} & \cs{HRpm} \\ +% Entropy & \cs{St} & \cs{Sm} & \cs{Ss} & \cs{Spm} +% & \cs{SEt} & \cs{SE} & \cs{SEs} & \cs{SEpm} +% & \cs{SRt} & \cs{SR} & \cs{SRs} & \cs{SRpm} \\ +% Volume & \cs{Vt} & \cs{Vm} & \cs{Vs} & \cs{Vpm} +% & \cs{VEt} & \cs{VE} & \cs{VEs} & \cs{VEpm} +% & \cs{VRt} & \cs{VR} & \cs{VRs} & \cs{VRpm} \\ +% Helmholtz free energy & \cs{Ft} & \cs{Fm} & \cs{Fs} & \cs{Fpm} +% & \cs{FEt} & \cs{FE} & \cs{FEs} & \cs{FEpm} +% & \cs{FRt} & \cs{FR} & \cs{FRs} & \cs{FRpm} \\ +% Gibbs free energy & \cs{Gt} & \cs{Gm} & \cs{Gs} & \cs{Gpm} +% & \cs{GEt} & \cs{GE} & \cs{GEs} & \cs{GEpm} +% & \cs{GRt} & \cs{GR} & \cs{GRs} & \cs{GRpm} \\ % Surface area & \cs{At} & \cs{Am} & \cs{As} & \cs{Apm} \\ % Grand potential\footnote{The grand potential, -% $\Lt(T,\Vt,\vec{\mu}\mkern1mu) = \Ut - T\St - \sum_i^C \mu_i \Nt_i,$ +% $\begin{thermomolesrange}\Lt(T,\Vt,\allmus)\end{thermomolesrange} +% = \Ut - T\St - \sumall_i \mu_i \Nt_i,$ % is also called the Landau free energy by some authors.} -% & \cs{Lt} & \cs{Lm} & \cs{Ls} & \cs{Lpm} \\ -% Moles & \cs{Nt} & N/A & N/A & N/A \\ -% $B$ (generic property) & \cs{Bt} & \cs{Bm} & \cs{Bs} & \cs{Bpm} \\ -% $M$ (generic property) & \cs{Mt} & \cs{Mm} & \cs{Ms} & \cs{Mpm} \\ +% & \cs{Lt} & \cs{Lm} & \cs{Ls} & \cs{Lpm} +% & \cs{LEt} & \cs{LE} & \cs{LEs} & \cs{LEpm} +% & \cs{LRt} & \cs{LR} & \cs{LRs} & \cs{LRpm} \\ +% Moles & \cs{Nt} & \\ % \bottomrule % \end{tabular} % \end{minipage} @@ -383,46 +452,52 @@ % \caption{Convenience macros and their default symbols. % These are generally ``smart'': for example, % \texttt{\textbackslash cP\_i} renders as $C_{P,i}$, as expected, and -% \texttt{\textbackslash cP\_i\^{}\textbackslash circ} renders as +% \texttt{\textbackslash cP\_i\^{}\textbackslash std} renders as % $C_{P,i}^\circ$, also as expected. You can also reverse it: -% \texttt{\textbackslash cP\^{}\textbackslash circ\_i} becomes +% \texttt{\textbackslash cP\^{}\textbackslash std\_i} becomes % $C^\circ_{P,i}$.} % \label{table:conveniences} -% \SpecialUsageIndex{\cP}\relax -% \SpecialUsageIndex{\cV}\relax -% \SpecialUsageIndex{\kappaT}\relax -% \SpecialUsageIndex{\kappaS}\relax -% \SpecialUsageIndex{\alphaP}\relax -% \SpecialUsageIndex{\alphaS}\relax -% \SpecialUsageIndex{\heatcapacitysymbol}\relax -% \SpecialUsageIndex{\compressibilitysymbol}\relax -% \SpecialUsageIndex{\expansivitysymbol}\relax -% \SpecialUsageIndex{\fpure}\relax -% \SpecialUsageIndex{\fmix}\relax -% \SpecialUsageIndex{\fsat}\relax -% \SpecialUsageIndex{\phipure}\relax -% \SpecialUsageIndex{\phimix}\relax -% \SpecialUsageIndex{\phisat}\relax -% \SpecialUsageIndex{\Psat}\relax -% \SpecialUsageIndex{\Pvap}\relax -% \SpecialUsageIndex{\sat}\relax -% \SpecialUsageIndex{\Henryrat}\relax -% \SpecialUsageIndex{\Henrymol}\relax -% \SpecialUsageIndex{\gammarat}\relax -% \SpecialUsageIndex{\gammamol}\relax -% \SpecialUsageIndex{\Deltamix}\relax -% \SpecialUsageIndex{\Deltarxn}\relax -% \SpecialUsageIndex{\Deltavap}\relax -% \SpecialUsageIndex{\Deltasub}\relax -% \SpecialUsageIndex{\Deltafus}\relax -% \SpecialUsageIndex{\mixing}\relax -% \SpecialUsageIndex{\reaction}\relax -% \SpecialUsageIndex{\fusion}\relax -% \SpecialUsageIndex{\vaporization}\relax -% \SpecialUsageIndex{\sublimation}\relax +%^^A TODO The \leavevmode macro here is to prevent whitespace from building +%^^A up due to a bug in old versions of hypdoc. It should be harmless to +%^^A leave it in there, but consider removing it at some point. +% \leavevmode +% \SpecialMacroIndex{\cP}\relax +% \SpecialMacroIndex{\cV}\relax +% \SpecialMacroIndex{\kappaT}\relax +% \SpecialMacroIndex{\kappaS}\relax +% \SpecialMacroIndex{\alphaP}\relax +% \SpecialMacroIndex{\alphaS}\relax +% \SpecialMacroIndex{\muJT}\relax +% \SpecialMacroIndex{\heatcapacitysymbol}\relax +% \SpecialMacroIndex{\compressibilitysymbol}\relax +% \SpecialMacroIndex{\expansivitysymbol}\relax +% \SpecialMacroIndex{\amix}\relax +% \SpecialMacroIndex{\fpure}\relax +% \SpecialMacroIndex{\fmix}\relax +% \SpecialMacroIndex{\fsat}\relax +% \SpecialMacroIndex{\phipure}\relax +% \SpecialMacroIndex{\phimix}\relax +% \SpecialMacroIndex{\phisat}\relax +% \SpecialMacroIndex{\Psat}\relax +% \SpecialMacroIndex{\Pvap}\relax +% \SpecialMacroIndex{\sat}\relax +% \SpecialMacroIndex{\Henryrat}\relax +% \SpecialMacroIndex{\Henrymol}\relax +% \SpecialMacroIndex{\gammarat}\relax +% \SpecialMacroIndex{\gammamol}\relax +% \SpecialMacroIndex{\Deltamix}\relax +% \SpecialMacroIndex{\Deltarxn}\relax +% \SpecialMacroIndex{\Deltavap}\relax +% \SpecialMacroIndex{\Deltasub}\relax +% \SpecialMacroIndex{\Deltafus}\relax +% \SpecialMacroIndex{\mixing}\relax +% \SpecialMacroIndex{\reaction}\relax +% \SpecialMacroIndex{\fusion}\relax +% \SpecialMacroIndex{\vaporization}\relax +% \SpecialMacroIndex{\sublimation}\relax % \begin{minipage}{\linewidth} % \small -% \addtolength{\tabcolsep}{-2pt}\relax +% \addtolength{\tabcolsep}{-2.75pt}\relax % \addtolength{\extrarowheight}{0.75ex}\relax % \renewcommand*{\footnoterule}{\vskip-1.5ex}\relax % \begin{tabular}{l l l l l} @@ -430,76 +505,78 @@ % \\[-1.5\normalbaselineskip] % Name & Macro & Sym. & Definition & Base Symbol Macro \\ % \midrule -% Isobaric heat capacity & \verb"\cP"\footnote{\relax +% Isobaric heat capacity & \cmd\cP\footnote{\relax % Extensive and specific (per-unit-mass) versions are available -% as \texttt{\textbackslash cPt} and \texttt{\textbackslash cPs}, -% respectively, with similar macros for the isochoric heat capacity. -% \label{fn:cP}} -% & $C_P$ & $\displaystyle T\left(\frac{\partial S}{\partial T}\right)_P$ -% & \verb"\heatcapacitysymbol" \\[2.0ex] -% Isochoric heat capacity & \verb"\cV"\footref{fn:cP} & $C_V$ -% & $\displaystyle T\left(\frac{\partial S}{\partial T}\right)_V$ -% & \verb"\heatcapacitysymbol" \\[2.0ex] -% Isothermal compressibility & \verb"\kappaT" & $\kappa_T$ & -% \(\displaystyle -\frac{1}{V} \left(\frac{\partial V}{\partial P}\right)_T \) -% & \verb"\compressibilitysymbol" \\[2.0ex] -% Isentropic compressibility & \verb"\kappaS" & $\kappa_S$ & -% \(\displaystyle -\frac{1}{V} \left(\frac{\partial V}{\partial P}\right)_S\) -% & \verb"\compressibilitysymbol" \\[2.0ex] -% Isobaric expansivity & \verb"\alphaP" & $\alpha_P$ & -% \(\displaystyle \frac{1}{V} \left(\frac{\partial V}{\partial T}\right)_P\) -% & \verb"\expansivitysymbol" \\[2.0ex] -% Isentropic expansivity & \verb"\alphaS" & $\alpha_S$ & -% \(\displaystyle \frac{1}{V} \left(\frac{\partial V}{\partial T}\right)_S\) -% & \verb"\expansivitysymbol" \\[2.0ex] -% Pure fugacity & \verb"\fpure" & $f$ & $\phi P$ \\ -% Mixture fugacity & \verb"\fmix" & $\hat f$ & $\hat f_i = x_i\hat\phi_i P$ \\[0.5ex] -% Saturation fugacity & \verb"\fsat" & $f^\text{sat}$ -% & $\phi^\text{sat} P^\text{sat}$ & \cs{sat} \\ -% Pure fugacity coeff.\ & \verb"\phipure" & $\phi$ & -% \multicolumn{2}{l}{\( \phi_i -% = \exp\left(\frac{1}{RT}\int_0^P V_i(T,p) +% as \cs{cPt} and \cmd\cPs, respectively, with similar macros for the +% isochoric heat capacity.\label{fn:cP}} +% & \(cP\) & \(\displaystyle T\Partial{\Sm}{T}{P}\) +% & \cmd\heatcapacitysymbol \\[2.0ex] +% Isochoric heat capacity & \verb"\cV"\footref{fn:cP} & \(\cV\) +% & \(\displaystyle T\Partial{\Sm}{T}{\Vm}\) +% & \cmd\heatcapacitysymbol \\[2.0ex] +% Isothermal compressibility & \cmd\kappaT & $\kappaT$ +% & \(\displaystyle -\frac{1}{\Vm} \Partial{\Vm}{P}{T} \) +% & \cmd\compressibilitysymbol \\[2.0ex] +% Isentropic compressibility & \cmd\kappaS & $\kappaS$ +% & \(\displaystyle -\frac{1}{\Vm} \Partial{\Vm}{P}{\Sm}\) +% & \cmd\compressibilitysymbol \\[2.0ex] +% Isobaric expansivity & \cmd\alphaP & $\alphaP$ +% & \(\displaystyle \frac{1}{\Vm} \Partial{\Vm}{T}{P}\) +% & \cmd\expansivitysymbol \\[2.0ex] +% Isentropic expansivity & \cmd\alphaS & $\alphaS$ +% & \(\displaystyle \frac{1}{\Vm} \Partial{\Vm}{T}{\Sm}\) +% & \cmd\expansivitysymbol \\[2.0ex] +% Joule--Thomson coeff. & \cmd\muJT & $\muJT$ +% & \(\displaystyle \Partial{T}{P}{\Hm}\) & \cmd\JTsymbol \\ +% Pure fugacity & \cmd\fpure & $f$ & $\phi P$ \\ +% Mixture fugacity & \cmd\fmix & $\fmix$ +% & $\fmix_i = x_i\phimix_i P$ \\[0.5ex] +% Saturation fugacity & \cmd\fsat & $\fsat$ +% & $\phisat \Psat$ & \cmd\sat \\ +% Pure fugacity coefficient & \cmd\phipure & $\phipure$ & +% \multicolumn{2}{l}{\( \phipure_i +% = \exp\left(\frac{1}{RT}\int_0^P \Vm_i(T,p) % - \frac{RT}{p}\,dp\right) \)} \\ -% Mixture fugacity coeff.\ & \verb"\phimix" & $\hat\phi$ -% & \multicolumn{2}{l}{\( \hat\phi_i +% Mixture fugacity coeff.\ & \cmd\phimix & $\phimix$ +% & \multicolumn{2}{l}{\( \phimix_i % = \exp\left(\frac{1}{RT}\int_0^P \Vpm{i}(T,p,\allXs) % - \frac{RT}{p}\,dp\right) \)} \\ -% Henry's constant (rational) & \verb"\Henryrat" & $h$ +% Henry's constant (rational) & \cmd\Henryrat & $\Henryrat$ % & $\gamma_i^\infty f_i$ \\ -% Henry's constant (molal) & \verb"\Henrymol" & $\mathcal{H}$ +% Henry's constant (molal) & \cmd\Henrymol & $\Henrymol$ % & $M_s \gamma_i^\infty f_i$ \\ -% Rational activity coeff.\ & \verb"\gammarat" & $\gamma^\ast$ +% Rational activity coeff.\ & \cmd\gammarat & $\gammarat$ % & $\gamma/\gamma^\infty$ \\ -% Molal activity coeff.\ & \verb"\gammamol" & $\gamma^\square$ +% Molal activity coeff.\ & \cmd\gammamol & $\gammamol$ % & $x_s \gamma/\gamma^\infty$ \\ -% Saturation fugacity coeff.\ & \verb"\phisat" & $\phi^\text{sat}$ -% & $\phi(T,P^\text{sat})$ & \cs{sat} \\ -% Saturation pressure & \verb"\Psat" & $P^\text{sat}$ && \cs{sat} \\ -% Vapor pressure & \verb"\Pvap" & \multicolumn{3}{l}{Currently a synonym +% Saturation fugacity coeff.\ & \cmd\phisat & $\phisat$ +% & $\phipure(T,\Psat)$ & \cmd\sat \\ +% Saturation pressure & \cmd\Psat & $\Psat$ && \cmd\sat \\ +% Vapor pressure & \cmd\Pvap & \multicolumn{3}{l}{Currently a synonym % for \cs{Psat}\footnote{If you want \cs{Pvap} to produce $P^\text{vap}$ -% instead of $P^\text{sat}$, you should redefine the \cs{sat} macro.}} \\ -% Standard state & \verb"\std"\footnote{Typical usage would be +% instead of $\Psat$, you should redefine the \cs{sat} macro.}} \\ +% Standard state & \cmd\std\footnote{Typical usage would be % \texttt{\$\cs{mu}\_i = \cs{mu}\textasciicircum\cs{std}\_i % + RT \cs{log} a\_i\$}, -% yielding $\mu_i = \mu_i^\circ + RT \log a_i$.} & $\circ$ \\ -% Standard pressure & \verb"\Pstd" & $P^\circ$ & & \cs{std} \\ -% Standard fugacity & \verb"\fstd" & $f^\circ$ & $f(T,P^\circ)$ & \cs{std} +% yielding $\mu_i = \mu_i^\std + RT \log a_i$.} & $\std$ \\ +% Standard pressure & \cmd\Pstd & $\Pstd$ & & \cs{std} \\ +% Standard fugacity & \cmd\fstd & $\fstd$ & $\fpure(T,\Pstd)$ & \cs{std} % \\ -% Change on mixing & \verb"\Deltamix"\footnote{The usual usage would be +% Change on mixing & \cmd\Deltamix\footnote{The usual usage would be % something like % \texttt{\$\cs{Deltamix}\cs{Vm}\textasciicircum\cs{IGM} = 0\$}.\relax % \label{fn:Deltausage}} % & $\Delta M$\textsubscript{mix} -% & $M - \sum_i x_i M_i$ & \verb"\mixing" \\ -% Change on reaction & \verb"\Deltarxn"\footref{fn:Deltausage} -% & $\Delta M_\text{rxn}$ -% & $\sum_i \nu_i M_i$ & \verb"\reaction" \\ -% Change on melting & \verb"\Deltafus"\footref{fn:Deltausage} -% & $\Delta M^\text{fus}$ & $M^L - M^S$ & \verb"\fusion" \\ -% Change on boiling & \verb"\Deltavap"\footref{fn:Deltausage} -% & $\Delta M^\text{vap}$ & $M^V - M^L$ & \verb"\vaporization" \\ -% Change on subliming & \verb"\Deltasub"\footref{fn:Deltausage} -% & $\Delta M^\text{sub}$ & $M^V - M^S$ & \verb"\sublimation" \\ +% & $M - \sumall_i x_i M_i$ & \cmd\mixing \\ +% Change on reaction & \cmd\Deltarxn\footref{fn:Deltausage} +% & $\Deltarxn M$ +% & $\sumall_i \nu_i M_i$ & \cmd\reaction \\ +% Change on melting & \cmd\Deltafus\footref{fn:Deltausage} +% & $\Deltafus M$ & $M^L - M^S$ & \cmd\fusion \\ +% Change on boiling & \cmd\Deltavap\footref{fn:Deltausage} +% & $\Deltavap M$ & $M^V - M^L$ & \cmd\vaporization \\ +% Change on subliming & \cmd\Deltasub\footref{fn:Deltausage} +% & $\Deltasub M$ & $M^V - M^S$ & \cmd\sublimation \\ % \bottomrule % \end{tabular} % \end{minipage} @@ -507,19 +584,19 @@ % % \subsection{Partial Molar Properties} % \DescribeMacro{\Upm} -% \DescribeMacro{\Hpm} -% Partial molar quantities are typically defined with the suffix \verb"pm". +% \DescribeMacro{\Vpm} +% Partial molar quantities are defined with the suffix \verb"pm". % For example, \cs{Upm} refers to the partial molar internal energy. There % are two options for how to enter partial molar quantities: as commands or % as super/subscripts. For example, % \begin{verbatim} -% \[ \Upm{i} \quad \Upm[\IG]{i} \quad \Hpm_i \quad \Hpm^\IG_i \] +% \[ \Upm{i} \quad \Upm[\IG]{i} \quad \Vpm_i \quad \Vpm^\IG_i \] %\end{verbatim} % will typeset as -% \[ \Upm{i} \quad \Upm[\text{IG}]{i} \quad \Hpm{i} \quad \Hpm[\text{IG}]{i}\] -% There are also partial molar heat capacities available via \cs{cPpm} and -% \cs{cVpm}. -% \textbf{Important}: The \cs{text} command defined by the \verb"amstext" +% \[ \Upm{i} \quad \Upm[\text{IG}]{i} \quad \Vpm{i} \quad \Vpm^{\text{IG}}_i.\] +% There are also partial molar heat capacities available via the macros +% \cs{cPpm} and \cs{cVpm}. +% \textbf{Important}: The \tn{text} command defined by the \pkg{amstext} % package is usually robust enough that something like \verb"\Um^\text{L}" will % work as expected, without additional braces. This does \emph{not} work for % partial molar properties; for example, \verb"\Hpm^\text{L}_i" will produce an @@ -530,15 +607,63 @@ % New partial molar properties can be defined for any ``simple'' symbol using % the \cs{partialmolar} macro. ``Simple'' means it has no subscripts or % superscripts. For example, the macro for the partial molar Gibbs free energy -% is defined via the macro +% is effectively defined via the macro % \DescribeMacro{\Gpm} % \begin{verbatim} -% \newcommand*{\Gpm}{\partialmolar{\Gibbs@symbol}} +% \NewDocumentCommand{\Gpm}{}{\partialmolar{G}}. %\end{verbatim} % A list of pre-defined macros for total, molar, specific, and partial molar % quantities commonly used in thermodynamics is included in % Table~\ref{table:symbols}. % +% \subsection{Defining New Properties} +% \DescribeMacro{\NewExtensiveProperty} +% Users can create new properties using a family of commands. Typically, a +% user would want to define at least the total, molar, and specific properties, +% which can be accomplished by the \cs{NewExtensiveProperty} command. +% For example, +% \begin{verbatim} +% \NewExtensiveProperty{J}{K} +%\end{verbatim} +% \NewExtensiveProperty{J}{K}\relax +% would define the commands \cs{Jt}, \cs{Jm}, and \cs{Js}, which would produce +% (using the default package options) the symbols $\Jt$, $K$, and $\hat{K}$, +% respectively. +% +% \DescribeMacro{\NewPartialMolarProperty}% +% Partial molar properties can be created either with the \cs{partialmolar} +% macro directly as described above or with \cs{NewPartialMolarProperty}, which +% has the same argument style as \cs{NewExtensiveProperty}. +% +% \DescribeMacro{\NewExcessProperty}% +% \DescribeMacro{\NewResidualProperty}% +% Similarly, one can define commands for the total, molar, and specific excess +% properties using \cs{NewExcessProperty} in a similar manner, and similar +% commands for the residual properties with \cs{NewResidualProperty}. +% +% \setmarginparsize{\footnotesize} +% \DescribeMacro{\NewThermodynamicProperty}\relax +% \restoremarginparsize +% \NewThermodynamicProperty{B}{B}\relax +% \NewExtensiveProperty{M}{M}\relax +% It is common that a user wants the total, molar, specific, and partial molar +% commands for a new symbol, as well as excess and residual (departure) +% properties for each case. Users can define such properties---common examples +% are $\Bt$ and $\Mt$ to represent uncommon or arbitrary properties---by using +% \cs{NewThermodynamicProperty}, which calls all four of the aforementioned +% declarations on the same command/\allowbreak{}symbol combinations. For +% example, +% \begin{verbatim} +% \NewThermodynamicProperty{B}{B} +%\end{verbatim} +% defines the commands \cs{Bt}, \cs{Bm}, \cs{Bs}, and \cs{Bpm}, which define +% the total, molar, specific, and partial molar properties, respectively. +% It also defines \cs{BEt}, \cs{BE}, \cs{BEs}, and \cs{BEpm} for the +% corresponding excess properties, and \cs{BRt}, \cs{BR}, \cs{BRs}, and +% \cs{BRpm} for residual (departure) properties. These produce, respectively, +% $\Bt, \Bm, \Bs, \Bpm{i}, \BEt, \BE, \BEs, \BEpm{i}, \BRt, \BR, \BRs,$ and +% $\BRpm{i}$ using the defaults. +% % \subsection{Other Predefined Symbols and Modifiers} % There are a number of predefined symbols and modifiers. % While these symbols could be defined or used without these macros, such use @@ -562,12 +687,20 @@ % \cs{expansivitysymbol}, which is done automatically by some of the % package options that create notation specific to a particular textbook. % +% \subsubsection{Joule--Thomson Coefficients} +% \changes{v2.00}{2023/11/16}{Added \cs{muJT} to represent Joule--Thomson +% coefficients (which have different notation across textbooks).} +% \DescribeMacro{\muJT} +% The Joule--Thomson coefficient is produced with \cs{muJT}, which be default +% is rendered $\muJT$. Some books call this coefficient $\alpha_H$; this is +% handled automatically for books of which the package author is aware. +% % \subsubsection{Fugacities and Fugacity Coefficients} % \DescribeMacro{\fpure} % \DescribeMacro{\fmix} % \DescribeMacro{\phipure} % \DescribeMacro{\phimix} -% Different textbooks use different modifications of the symbol $f$ for +% Different textbooks use different variations on the symbol $f$ for % fugacity, so it is recommended to use the macro \cs{fpure} to denote the % pure-component fugacity and \cs{fmix} to denote the mixture fugacity. % Similarly, the pure-component fugacity coefficient should be generated with @@ -576,25 +709,30 @@ % For example, the following markup is an example of a common equation in % mixture thermodynamics: % \begin{verbatim} -% \[ \fmix_j = x_j \phimix_j P = x_j \gamma_j \fpure_j. \] +% \[ \fmix_j = x_j \phimix_j P = x_j \gamma_j \fpure_j +% = x_j \gamma_j \phipure_j P. \] %\end{verbatim} % With the default package options, this produces -% \[ \hat f_j = x_j \hat\phi_j P = x_j \gamma_j f_j. \] +% \[ \fmix_j = x_j \phimix_j P = x_j \gamma_j \fpure_j +% = x_j \gamma_j \phipure_j P. \] % With the |Thompson| package option, however, the same markup produces -% \[ \hat f_j = x_j \hat\phi_j P = x_j \gamma_j f^\bullet_j. \] +% \[ \hat f_j = x_j \hat\phi_j P = x_j \gamma_j f^\bullet_j +% = x_j \gamma_j \phi^\bullet_j P. \] % Similarly, the |Prausnitz| package option causes it to generate -% \[ f_j = x_j \phi_j P = x_j \gamma_j f_{\text{pure},j}, \] +% \[ f_j = x_j \phi_j P = x_j \gamma_j f_{\text{pure},j} +% = x_j \gamma_j \phi_{\text{pure},j} P, \] % and the |Sandler| option causes it to generate -% \[ \bar f_j = x_j \bar \phi_j P = x_j \gamma_j f_j. \] +% \[ \bar f_j = x_j \bar \phi_j P = x_j \gamma_j f_j +% = x_j \gamma_j \phi_j P. \] % % \subsubsection{Activity Coefficients and Henry's Constants} % \DescribeMacro{\gammarat} % \DescribeMacro{\gammamol} % \DescribeMacro{\Henryrat} % \DescribeMacro{\Henrymol} -% The activity coefficient can be generated with \cs{gamma}, as usual. -% The Henry's Law activity coefficients should be produced with \cs{gammarat} -% (rational basis) and \cs{gammamol} (molal basis). +% The activity coefficient based on the Lewis--Randall rule can be generated +% with \cs{gamma}, as usual. The Henry's Law activity coefficients should be +% produced with \cs{gammarat} (rational basis) and \cs{gammamol} (molal basis). % There are also macros to generate the Henry's law constants for both the % rational basis (\cs{Henryrat}) and the molal basis (\cs{Henrymol}). % These are interrelated: @@ -603,9 +741,24 @@ % = C_i \gammamol_i \Henrymol_i \] %\end{verbatim} % produces -% \[ \hat f_i = x_i \gamma_i f_i = x_i \gamma^*_i h_i -% = C_i \gamma^\square_i \mathcal{H}_i \] +% \[ \fmix_i = x_i \gamma_i \fpure_i = x_i \gammarat_i \Henryrat_i +% = C_i \gammamol_i \Henrymol_i \] % using the default options. +% These symbols can be customized either directly or by using package options. +% For example, the |TesterModell| package option changes the equation +% above to +% \[ \hat f_i = x_i \gamma_i f_i = x_i \gamma_i^{**} f_i^{**} +% = C_i \gamma_i^* f_i^* \] +% without any changes in markup. +% +% Note that some books (e.g., |ElliottLira|) prefer the atmospheric chemistry +% convention for the molal basis, namely +% \[ \fmix_i = x_i \gamma_i \fpure_i = x_i \gammarat_i \Henryrat_i +%%^^A = C_i \gammamol_i \Henrymol_i +% = C_i \gammamol_i / K_{H,i} \] +% (that is, using $1/K_{H,i}$ in place of $\Henrymol_i$). +% Unfortunately, this makes it impossible to change symbols without any edits +% to markup, so this convention is \emph{not} supported by this package. % % \subsubsection{Saturation Properties} % \DescribeMacro{\Psat} @@ -620,11 +773,11 @@ % % \DescribeMacro{\sat} % The \cs{sat} macro is used ``behind the scenes'' as part of -% \cs{Psat}, \cs{fsat}, and \cs{phisat}, which produce $P^\text{sat}$, -% $f^\text{sat}$, and $\phi^\text{sat}$, respectively. If you wanted to +% \cs{Psat}, \cs{fsat}, and \cs{phisat}, which produce $\Psat$, +% $\fsat$, and $\phisat$, respectively (using the defaults). If you wanted to % redefine them to be $P^\text{vap}$, $f^\text{vap}$, and $\phi^\text{vap}$, % you could simply redefine \cs{sat} with -% \verb"\renewcommand*{\sat}{{\text{vap}}}". +% \verb"\RenewDocumentCommand{\sat}{}{{\text{vap}}}". % This is done automatically using package option |Sandler|. % % \subsubsection{Standard States} @@ -635,21 +788,19 @@ % This is intended to be easy to change should the user want to replace % $P^\circ$ with $P^\ominus$, say. This is accessed via the \cs{std} macro. % The macro \cs{Pstd} is defined as |P^\std| for convenience to denote -% standard pressures, and \cs{fstd} is defined for standard fugacities so as to -% ease implementation across textbooks. +% standard pressures, and \cs{fstd} is defined for standard fugacities so as +% to ease implementation across textbooks. % % The usual usage would be something like this: % \begin{verbatim} % \[ \Deltarxn\Gm = \sumall_i \nu_i \mu_i = \sumall_i \left[ \nu_i \mu^\std_i % + \nu_i RT \log\left(\frac{\fmix_i}{\fstd_i}\right) \right] -% = \Deltarxn\Gm^\std + RT \log\left[\prodall_i a_i^{\nu_i} \right] \] +% = \Deltarxn\Gm^\std + RT \log\left[\prodall_i a_i^{\nu_i} \right] \], %\end{verbatim} % which produces -% \[ \Delta G_\text{rxn} = \sum_{i=1}^C \nu_i \mu_i -% = \sum_{i=1}^C \left[ \nu_i \mu^\circ_i -% + \nu_i RT \log\left(\frac{\hat f_i}{f_i^\circ}\right) \right] -% = \Delta G^\circ_\text{rxn} -% + RT \log\left[\prod_{i=1}^C a_i^{\nu_i} \right] \] +% \[ \Deltarxn\Gm = \sumall_i \nu_i \mu_i = \sumall_i \left[ \nu_i \mu^\std_i +% + \nu_i RT \log\left(\frac{\fmix_i}{\fstd_i}\right) \right] +% = \Deltarxn\Gm^\std + RT \log\left[\prodall_i a_i^{\nu_i} \right] \] % with the default settings. % % \subsubsection{Changes on Mixing, Reaction, Fusion, Vaporization, and @@ -658,11 +809,11 @@ % Mixing properties are handled via the \cs{Deltamix} macro, and are used as in % the following example: % \begin{verbatim} -% \[ \Deltamix\Gm = \Gm - \sumall_i x_i \Gm_i = \Deltamix\Hm - T\Deltamix\Sm \] +% \[ \Deltamix\Gm = \Gm - \sumall_i x_i \Gm_i +% = \Deltamix\Hm - T\Deltamix\Sm \], %\end{verbatim} -% which yields -% \[ \Delta G_\text{mix} = G - \sum_{i=1}^C x_i G_i -% = \Delta H_\text{mix} - T\Delta S_\text{mix}. \] +% which yields, using the default options, +% \[ \Deltamix\Gm = \Gm - \sumall_i x_i \Gm_i = \Deltamix\Hm - T\Deltamix\Sm \] % Some textbooks (|Sandler|, |Thompson|) choose to typeset these with the word % ``mix'' \emph{before} the symbol, which is handled automatically by this % package. @@ -678,13 +829,15 @@ % vaporization (boiling), respectively. Their use is straightforward, viz., % \begin{verbatim} % \[ \Deltasub\Hm = \Hm^V - \Hm^S = \Hm^V - \Hm^L + (\Hm^L - \Hm^S) -% = \Deltafus\Hm + \Deltavap\Hm \] +% = \Deltafus\Hm + \Deltavap\Hm \], %\end{verbatim} % yielding -% \[ \Delta\Hm^\text{sub} = \Hm^V - \Hm^S = \Hm^V - \Hm^L + (\Hm^L - \Hm^S) -% = \Delta\Hm^\text{vap} + \Delta\Hm^\text{fus} \] +% \[ \Deltasub\Hm = \Hm^V - \Hm^S = \Hm^V - \Hm^L + (\Hm^L - \Hm^S) +% = \Deltafus\Hm + \Deltavap\Hm \] % with the default options. Note that some textbooks (e.g., |Sandler|) typeset -% these quantities quite differently. +% these quantities quite differently; this is handled automatically. Other +% textbooks (e.g., |Koretsky|) typeset them as subscripts; this is also +% handled automatically. % % \DescribeMacro{\Deltaf} % \DescribeMacro{\Deltarxn} @@ -694,7 +847,7 @@ % \[ \Deltarxn\Hm^\std = \sumall_i \nu_i \Deltaf\Hm_i^\std \] %\end{verbatim} % results in -% \[ \Delta\Hm_\text{rxn}^\circ = \sum_{i=1}^C \nu_i \Delta\Hm_{f,i}^\circ. \] +% \[ \Deltarxn\Hm^\std = \sumall_i \nu_i \Deltaf\Hm_i^\std. \] % It is not anticipated that this command will be combined with something like % a heat capacity, which already has a (potentially double) subscript, but as % there is no ``formation'' heat capacity, that should not present a problem. @@ -713,50 +866,54 @@ % molar properties. These macros follow the same pattern: \cs{UR}, \cs{URt}, % \cs{URs}, and \cs{URpm} typeset the molar, total, specific, and partial molar % residual internal energies, respectively, and by default expand to $U^R,$ -% $\thermounderline{U}^R,$ $\hat U^R, $ and $\smash[t]{\Upm[R]{i}}$ (the last +% $\URt,$ $\URs, $ and $\smash[t]{\URpm{i}}$ (the last % is called as \verb"\URpm{i}" or \verb"\URpm_i"). Similarly, \cs{UE}, % \cs{UEt}, \cs{UEs}, and \cs{UEpm} typeset the corresponding excess % properties. The first character of the macros for other properties follow the % same pattern as in Table~\ref{table:symbols}. % -% \DescribeMacro{\excess} -% \DescribeMacro{\residual} % The $R$ and $E$ characters are generated by the macros \cs{residual} and % \cs{excess}, respectively. These macros can be redefined; for example, if you -% want \cs{SE}, which normally produces $S^E$, to give you $S^{EX}$---and let's +% \DescribeMacro{\excess} +% \DescribeMacro{\residual} +% want \cs{SE}, which normally produces $\SE$, to give you $S^{EX}$---and let's % be honest, who doesn't want that?\footnote{You knew that joke was % coming.}---then you can redefine it with % \begin{verbatim} -% \renewcommand*{\excess}{{EX}} +% \RenewDocumentCommand{\excess}{}{{EX}}, %\end{verbatim} % or possibly % \begin{verbatim} -% \renewcommand*{\excess}{{\mathrm{EX}}} +% \RenewDocumentCommand{\excess}{}{{\mathrm{EX}}} %\end{verbatim} % or even % \begin{verbatim} -% \renewcommand*{\excess}{\text{EX}} +% \RenewDocumentCommand{\excess}{}{\text{EX}}, %\end{verbatim} % which cause \cs{SE} to expand to $S^{EX},$ $S^\mathrm{EX},$ and % $S^\text{EX},$ respectively. % -% It is generally not possible to use superscripts with the excess or -% residual properties; in the event the user needs this, the \cs{excess} and -% \cs{residual} macros can be used directly, viz., +% It is generally possible to use superscripts with the excess or residual +% properties; in the event this fails, the \cs{excess} and \cs{residual} macros +% can be used directly, viz., % \begin{verbatim} % \begin{gather*} -% \Hm^{\excess,\std} = \HE(T,\Pstd) \\ -% \renewcommand*{\excess}{EX} -% \Hm^{\excess,\std} = \HE(T,\Pstd) -% \end{gather*} +% \HE^\std = \Hm^{\excess,\std} = \HE(T,\Pstd) +% = \HR(T,\Pstd) - \HR^\IS(T,\Pstd) = \HR^\std - \HR^{\IS,\std} \\ +% \RenewDocumentCommand{\excess}{{EX}} +% \HE^\std = \Hm^{\excess,\std} = \HE(T,\Pstd) +% = \HR(T,\Pstd) - \HR^\IS(T,\Pstd) +% \end{gather*}, %\end{verbatim} % which yields % \begin{gather*} -% \Hm^{E,\circ} = H^E(T,P^\circ) \\ -% \Hm^{EX,\circ} = H^{EX}(T,P^\circ) +% \HE^\std = \Hm^{\excess,\std} = \HE(T,\Pstd) +% = \HR(T,\Pstd) - \HR^\IS(T,\Pstd) = \HR^\std - \HR^{\IS,\std} \\ +% \RenewDocumentCommand{\excess}{}{{EX}} +% \HE^\std = \Hm^{\excess,\std} = \HE(T,\Pstd) +% = \HR(T,\Pstd) - \HR^\IS(T,\Pstd) % \end{gather*} % using the default options. -% \clearpage % % \subsection{Partial Derivatives} % \DescribeMacro{\Partial}% @@ -764,18 +921,36 @@ % Partial derivatives are easily rendered using the \cs{Partial} command. % There is a starred form (\cs{Partial*}) that additionally adjusts the % spacing after the closing symbol to remove some of the space, anticipating -% that the following binary operator will overhang the subscripts. Compare -% the following: +% that the following binary operator will overhang the subscripts. +% Compare the following: % \begin{verbatim} -% \begin{gather*} -% \Partial{\Hm}{T}{P} = \cP \qquad \Partial*{\Hm}{T}{P} = \cP -% \end{gather*} +% \[ \Partial{\Hm}{T}{P} = \cP \qquad \Partial*{\Hm}{T}{P} = \cP \], %\end{verbatim} % which yields -% \begin{gather*} -% \left(\frac{\partial\Hm}{\partial T}\right)_{P} = C_P \qquad -% \left(\frac{\partial\Hm}{\partial T}\right)_{P} \mkern-8mu = C_P -% \end{gather*} +% \[ \Partial{\Hm}{T}{P} = \cP \qquad \Partial*{\Hm}{T}{P} = \cP. \] +% +% \DescribeMacro{\Partialinline}% +% Inline first derivatives\footnote{The ``inline'' versions of +% partial derivatives are ``sticky'': if you issue \cs{Partialinline} or +% its second-order equivalents anywhere in a line, all subsequent +% \cs{Partial} and \cs{Partial[Mix]Second} macros on the same line +% (technically, anywhere in the same \TeX\ ``group'') will +% expand inline as well. To prevent this, enclose your \cs{Partialinline} and +% associated arguments in its own group (i.e., +% \texttt{\{\cs{Partialinline}\dots\}}).% +% \label{fn:inline}} +% can be entered the same way; compare: +% \begin{verbatim} +% \[ \Partial*{\Hm}{T}{P} = \Partialinline{\Hm}{T}{P} +% = T\Partial{\Sm}{T}{P} \], +%\end{verbatim} +% which results in +% \[ \Partial*{\Hm}{T}{P} = \Partialinline{\Hm}{T}{P} +% = T\Partial{\Sm}{T}{P}. \] +% There is no need for an inline starred form, as the subscripts do not +% extend far enough below the baseline. +% +% \subsubsection{Second-Order Partial Derivatives} % \DescribeMacro{\PartialSecond}% % \DescribeMacro{\PartialSecond*}% % \DescribeMacro{\PartialMixSecond}% @@ -793,35 +968,46 @@ % = \Partial{\Gpm_i}{P}{T,\allNs} \] %\end{verbatim} % looks like -% \[ \Vpm{i} = \left(\frac{\partial\Vt} -% {\partial\Nt_i}\right)_{T,P,\allNsbut{i}} -% \mkern-15mu -% = \left(\frac{\partial^2\Gt} -% {\partial\Nt_i\partial P}\right)_{T,\allNsbut{i}} -% \mkern-15mu -% = \left(\frac{\partial^2\Gt} -% {\partial P\partial\Nt_i}\right)_{T,\allNsbut{i}} -% \mkern-15mu -% = \left(\frac{\partial\Gpm{i}}{\partial P}\right)_{T,\allNs}. \] -% \DescribeMacro{\PartialBigg} -% \SpecialUsageIndex{\PartialBigg*}\relax -% \DescribeMacro{\PartialSecondBigg} -% \SpecialUsageIndex{\PartialSecondBigg*}\relax -% \DescribeMacro{\PartialMixSecondBigg} -% \SpecialUsageIndex{\PartialMixSecondBigg*}\relax -% \DescribeMacro{\Partialbigg} -% \SpecialUsageIndex{\Partialbigg*}\relax -% \DescribeMacro{\PartialSecondbigg} -% \SpecialUsageIndex{\PartialSecondbigg*}\relax -% \DescribeMacro{\PartialMixSecondbigg} -% \SpecialUsageIndex{\PartialMixSecondbigg*}\relax +% \[ \Vpm_i = \Partial*{\Vt}{\Nt_i}{T,P,\allNsbut{i}} +% = \PartialMixSecond*{\Gt}{\Nt_i}{P}{T,\allNsbut{i}} +% = \PartialMixSecond*{\Gt}{P}{\Nt_i}{T,\allNsbut{i}} +% = \Partial{\Gpm_i}{P}{T,\allNs}. \] +% \DescribeMacro{\PartialSecondinline}% +% \DescribeMacro{\PartialMixSecondinline}% +% Inline versions\footref{fn:inline} of second-order derivatives are handled +% with \cs{PartialSecondinline} and \cs{PartialMixSecondinline}, viz., +% \begin{verbatim} +% \begin{equation} +% \Vpm_i = \Partialinline{\Vt}{\Nt_i}{T,P,\allNsbut{i}} +% = \PartialMixSecondinline{\Gt}{\Nt_i}{P}{T,\allNsbut{i}} +% = \PartialMixSecondinline{\Gt}{P}{\Nt_i}{T,\allNsbut{i}} +% = \Partialinline{\Gpm_i}{P}{T,\allNs} \] +% \end{equation} +%\end{verbatim} +% looks like +% \begin{equation} +% \Vpm_i = \Partialinline{\Vt}{\Nt_i}{T,P,\allNsbut{i}} +% = \PartialMixSecondinline{\Gt}{\Nt_i}{P}{T,\allNsbut{i}} +% = \PartialMixSecondinline{\Gt}{P}{\Nt_i}{T,\allNsbut{i}} +% = \Partialinline{\Gpm_i}{P}{T,\allNs}. +% \label{eq:Vpm-inline} +% \end{equation} +% \pagebreak[0]% +% +% \subsubsection{Delimiter Sizing} +% \DescribeMacro{\PartialBigg}% +% \DescribeMacro{\PartialSecondBigg}% +% \DescribeMacro{\PartialMixSecondBigg}% +% \DescribeMacro{\Partialbigg}% +% \DescribeMacro{\PartialSecondbigg}% +% \DescribeMacro{\PartialMixSecondbigg}% % There are instances (such as the line above) when \cs{Partial} causes % parentheses that are slightly % too tall but do not need to be---particularly when partial molar properties, % specific quantities, or fugacities are involved. The macro \cs{PartialBigg} -% uses \verb"amsmath"'s \cs{Biggl} and \cs{Biggr} macros in place of \cs{left} -% and \cs{right} to size the parentheses accordingly; \cs{Partiallbigg} uses -% \cs{biggl} and \cs{biggr} in a similar fashion. For example, compare the +% uses \pkg{amsmath}'s \tn{Biggl} and \tn{Biggr} macros in place of \tn{left} +% and \tn{right} to size the delimiters accordingly; \cs{Partialbigg} uses +% \tn{biggl} and \tn{biggr} in a similar fashion. For example, compare the % following: % \begin{verbatim} % \[ \Vpm_i = \Partial*{\Vt}{\Nt_i}{T,P,\allNsbut{i}} @@ -829,55 +1015,65 @@ % = \PartialBigg*{\Gpm_i}{P}{T,\allNs} % = RT\Partial*{\log\fmix_i}{P}{T,\allNs} % = RT\,\PartialBigg*{\log\fmix_i}{P}{T,\allNs} -% = RT\,\Partialbigg{\log\fmix_i}{P}{T,\allNs} \] +% = RT\,\Partialbigg{\log\fmix_i}{P}{T,\allNs} \], %\end{verbatim} % which typesets as -% \[ \Vpm{i} -% = \left(\frac{\partial\Vt}{\partial \Nt_i}\right)_{T,P,\allNsbut{i}} -% \mkern-15mu -% = \left(\frac{\partial\Gpm{i}}{\partial P}\right)_{T,\allNs} -% \mkern-15mu -% = \Biggl(\frac{\partial\Gpm{i}}{\partial P}\Biggr)_{T,\allNs} -% \mkern-15mu -% = RT\left(\frac{\partial\log\hat f_i}{\partial P}\right)_{T,\allNs} -% \mkern-15mu -% = RT\,\Biggl(\frac{\partial\log\hat f_i}{\partial P}\Biggr)_{T,\allNs} -% \mkern-15mu -% = RT\,\biggl(\frac{\partial\log\hat f_i}{\partial P}\biggr)_{T,\allNs} \] +% \[ \Vpm{i} = \Partial*{\Vt}{\Nt_i}{T,P,\allNsbut{i}} +% = \Partial*{\Gpm{i}}{P}{T,\allNs} +% = \PartialBigg*{\Gpm{i}}{P}{T,\allNs} +% = RT\Partial*{\log\fmix_i}{P}{T,\allNs} +% = RT\,\PartialBigg*{\log\fmix_i}{P}{T,\allNs} +% = RT\,\Partialbigg{\log\fmix_i}{P}{T,\allNs}. \] % Note that a similar effect---possibly with other side effects---can be -% achieved with \verb"amsmath"'s \cs{smash} command, which has the effect of +% achieved with \pkg{amsmath}'s \tn{smash} command, which has the effect of % removing all vertical space associated with a particular character. % Observe: % \begin{verbatim} -% \[ \Vpm_i = \Partial{\Vt}{\Nt_i}{T,P,\allNsbut{i}} +% \[ \Vpm_i = \Partial*{\Vt}{\Nt_i}{T,P,\allNsbut{i}} % = \Partial{\smash{\Gpm_i}}{P}{T,\allNs} \] -% \end{verbatim} +%\end{verbatim} % produces -% \[ \Vpm{i} -% = \left(\frac{\partial\Vt}{\partial \Nt_i}\right)_{T,P,\allNsbut{i}} -% = \left(\frac{\partial\smash{\Gpm{i}}}{\partial P}\right)_{T,\allNs}. \] -% Note that the vertical spacing is not quite as good here as it was above. -% This can be fixed by using the optional argument to \cs{smash}, viz., +% \[ \Vpm_i = \Partial*{\Vt}{\Nt_i}{T,P,\allNsbut{i}} +% = \Partial{\smash{\Gpm_i}}{P}{T,\allNs}. \] +% +% \setmarginparsize{\footnotesize}% +% \DescribeMacro{\Partialinlinetext}% +% \DescribeMacro{\PartialSecondinlinetext}% +% \restoremarginparsize +% \setmarginparsize{\scriptsize} +% \DescribeMacro{\PartialMixSecondinlinetext}% +% \restoremarginparsize +% Similarly, there are times when \cs{Partialinline} causes parentheses that +% are too big for inline text, and they do not need to be---particularly for +% symbols with overlines, underlines, or other decorations. In this case, the +% macros \cs{Partialinlinetext}, \cs{PartialSecondinlinetext}, and +% \cs{PartialMixSecondinlinetext} come in handy; using these macros like so, % \begin{verbatim} -% \[ \Vpm_i = \Partial{\Vt}{\Nt_i}{T,P,\allNsbut{i}} -% = \Partial{\smash[t]{\Gpm_i}}{P}{T,\allNs} \] +% \[ \Vpm_i = \Partialinlinetext{\Vt}{\Nt_i}{T,P,\allNsbut{i}} +% = \PartialMixSecondinlinetext{\Gt}{\Nt_i}{P}{T,\allNsbut{i}} +% = \PartialMixSecondinlinetext{\Gt}{P}{\Nt_i}{T,\allNsbut{i}} +% = \Partialinlinetext{\Gpm_i}{P}{T,\allNs} \], %\end{verbatim} -% \[ \Vpm{i} -% = \left(\frac{\partial\Vt}{\partial \Nt_i}\right)_{T,P,\allNsbut{i}} -% = \left(\frac{\partial\smash[t]{\Gpm{i}}}{\partial P}\right)_{T,\allNs}. \] +% Equation~\eqref{eq:Vpm-inline} looks like +% \[ \Vpm{i} = \Partialinlinetext{\Vt}{\Nt_i}{T,P,\allNsbut{i}} +% = \PartialMixSecondinlinetext{\Gt}{\Nt_i}{P}{T,\allNsbut{i}} +% = \PartialMixSecondinlinetext{\Gt}{P}{\Nt_i}{T,\allNsbut{i}} +% = \Partialinlinetext{\Gpm{i}}{P}{T,\allNs}. \] +% +% \subsubsection{Higher-Order Derivatives} % It is possible to ``fake'' higher-order derivatives via some trickery. % For example, % \begin{verbatim} -% \[ \cPpm_i = T\Partial{\Spm_i}{T}{P,\allXs} -% = T\PartialSecond{\St}{T}{\Nt_i}{P,\allNsbut{i}} +% \[ \cPpm_i = T\Partial*{\Spm_i}{T}{P,\allXs} +% = T\PartialMixSecond*{\St}{T}{\Nt_i}{P,\allNsbut{i}} % = -T\Partial{^3\Gt}{T^2\partial\Nt_i}{P,\allNsbut{i}} \] %\end{verbatim} % gives -% \[ \cPpm{i} = T\Partial{\Spm{i}}{T}{P,\allXs} -% = T\Partial{^2\St}{T\partial\Nt_i}{P,\allNsbut{i}} +% \[ \cPpm{i} = T\Partial*{\Spm{i}}{T}{P,\allXs} +% = T\PartialMixSecond*{\St}{T}{\Nt_i}{P,\allNsbut{i}} % = -T\Partial{^3\Gt}{T^2\partial\Nt_i}{P,\allNsbut{i}}, \] % which is probably pretty close to what you wanted. Using this trickery with -% the package option \verb"nosubscripts" will not work as well, and the use of +% the package option \verb"nosubscripts" will not work, and the use of % third- and higher-order derivatives with this package should generally be % considered unsupported. % @@ -895,16 +1091,22 @@ % \DescribeMacro{\allWs}% % \DescribeMacro{\allWsbut}% % It is common in thermodynamics to use notation such as -% \[ \Vpm{k} = \left(\frac{\partial\Vt}{\partial\Nt_k}\right)_{T,P,\Nt_{j\neq k}} \] +% \[ \Vpm_k = \Partial{\Vt}{\Nt_k}{T,P,\allNsbut{k}}, \] % or perhaps -% \[ \Vpm{k} = \left(\frac{\partial\Vt}{\partial\Nt_k}\right)_{T,P,\Nt_1,\dotsc,[\Nt_k],\dots,\Nt_C} \] +% \begin{thermomolesrange} +% \[ \Vpm{k} = \Partial{\Vt}{\Nt_k}{T,P,\allNsbut{k}} \] +% \end{thermomolesrange} +% or +% \[ \Vpm{k} = \left(\frac{\partial\Vt}{\partial\Nt_k}\right)_{T,P,\Nt_j[k]} \] % to mean partial derivatives that hold the number of moles of each species % constant \emph{except} the one being changed. % Similarly, a property determined with all mole fractions held % constant might be written -% \[ C_P = \left(\frac{\partial\Hm}{\partial T}\right)_{P,\vec{x}} \] +% \[ \cP = \Partial{\Hm}{T}{P,\allXs}, \] % or perhaps -% \[ C_P = \left(\frac{\partial\Hm}{\partial T}\right)_{P,x_1,\dotsc,x_C}. \] +% \begin{thermomolesrange}\relax +% \[ \cP = \Partial{\Hm}{T}{P,\allXs}. \] +% \end{thermomolesrange}\relax % There are several macros that standardize such constructs. % The \cs{allNs} macro expands to something meaning the number of moles of all % species; by default, this is $\vec{n}$ (package option @@ -915,62 +1117,106 @@ % fractions, namely \cs{allXs} and \cs{allXsbut} for $x$ and \cs{allYs} and % \cs{allYsbut} for $y$, as well as \cs{allWs} and \cs{allWsbut} for mass % fractions---these implicitly assume that all mole or mass fractions -% \emph{except} the last are used as variables. The macros \cs{allNsbut}, -% \cs{allMsbut}, \cs{allmusbut}, \cs{allXsbut}, \cs{allYsbut}, and -% \cs{allWsbut} take an optional argument; for example, +% \emph{except} the last are used as variables. +% These macros all take an optional argument; for example, % \begin{verbatim} -% \Partial{\Ht}{\Nt_1}{T,P,\allNsbut{1}} = -% \Partial{\Ht}{\Nt_1}{T,P,\allNsbut[m]{1}} = \Hpm_1 +% \[ \Partial{\Ht}{\Nt_1}{T,P,\allNsbut{1}} = +% \Partial{\Ht}{\Nt_1}{T,P,\allNsbut[m]{1}} = \Hpm_1 \] %\end{verbatim} % typesets as -% \[ \left(\frac{\partial\Ht}{\partial\Nt_1}\right)_{T,P,\Nt_{j\neq 1}} -% = \left(\frac{\partial\Ht}{\partial\Nt_1}\right)_{T,P,\Nt_{m\neq 1}} -% = \Hpm{1} \] +% \[ \Partial{\Ht}{\Nt_1}{T,P,\allNsbut{1}} = +% \Partial{\Ht}{\Nt_1}{T,P,\allNsbut[m]{1}} = \Hpm{1}. \] % Similarly, % \begin{verbatim} -% \Partial{\Hm}{x_i}{T,P,\allXsbut{i}} = -% \Partial{\Hm}{x_i}{T,P,\allXsbut[m]{i}} = \Hpm_i - \Hpm_\ncomponents +% \[ \Partial{\Hm}{x_i}{T,P,\allXsbut{i}} +% = \Partial{\Hm}{x_i}{T,P,\allXsbut[m]{i}} +% = \Hpm_i - \Hpm_\ncomponents \] %\end{verbatim} % becomes -% \[ \left(\frac{\partial\Hm}{\partial x_i}\right)_{T,P,x_{j\neq i,C}} -% = \left(\frac{\partial\Hm}{\partial x_i}\right)_{T,P,x_{m\neq i,C}} -% = \Hpm{i} - \Hpm{C} \] -% The user must supply their own redefinition if they wish to hold something -% other than \cs{ncomponents} constant in addition to the argument. +% \[ \Partial{\Hm}{x_i}{T,P,\allXsbut{i}} +% = \Partial{\Hm}{x_i}{T,P,\allXsbut[m]{i}} +% = \Hpm{i} - \Hpm{\ncomponents}. \] +% Users must supply their own redefinitions if they wish to hold something +% other than \cs{ncomponents} constant in addition to the argument for mole +% and mass fractions. % Using the \verb"moles-range" package option, for which \verb"\allXsbut{k}" -% expands to $x_1,\dotsc,[x_k],\dotsc,x_{C-1}$ rather than $x_{j \neq k,C}$, -% the optional argument is ignored. +% expands to +% \( \begin{thermomolesrange}\allXsbut{k}\end{thermomolesrange} \) +% rather than \( \allXsbut{k} \), the optional argument is ignored. +% +% The optional argument to \cs{allNs} and similar commands is ignored when +% using the default options; it is relevant for package options that redefine +% \cs{allNs} to make $N_i$, for example; in this case, one can enter +% \cs{allNs[j]} to make \TeX\ render $N_j$ instead of $N_i$. This is useful +% if you are using $i$ somewhere else in the equation. % % \DescribeMacro{\allbut} % \DescribeMacro{\allbutlastand} % Users can define new ``all but'' macros using the \cs{allbut} and % \cs{allbutlastand} commands. For example, % \begin{verbatim} -% \newcommand*{\allNsbut}[2][j]{\allbut[#1]{#2}{\Nt}} -% \newcommand*{\allXsbut}[2][j]{\allbutlastand[#1]{#2}{x}} +% \NewDocumentCommand{\allNsbut}{O{j} m}{\allbut[#1]{#2}{\Nt}} +% \NewDocumentCommand{\allXsbut}{O{j} m}{\allbutlastand[#1]{#2}{x}} %\end{verbatim} % are the definitions of \cs{allNsbut} and \cs{allXsbut}, respectively. % +% \subsection{Jacobians} +% \DescribeMacro{\Jacobian}% +% \DescribeMacro{\Jacobiandet}% +% The Jacobian determinant is often denoted with Leibnitz-like notation, viz., +% \begin{verbatim} +% \[ \Jacobian{K,L}{X,Y} = \Jacobiandet{K,L}{X,Y} \], +%\end{verbatim} +% which produces (assuming the \pkg{amsmath} package has been loaded) +% \[ \Jacobian{K,L}{X,Y} = \Jacobiandet{K,L}{X,Y}. \] +% There are two optional arguments to \cs{Jacobiandet}. The first will be +% pre-pended before every element of the matrix (typically \cs{textstyle} or +% \cs{displaystyle}); the second is the extra spacing added between rows +% (default is 1.25~ex for text-style fractions and 2.75~ex for display-style +% fractions). More than two variables can be specified, viz., +% \begin{verbatim} +% \[ \Jacobian{K,L,M}{X,Y,Z} +% = \Jacobiandet[\displaystyle][3ex]{K,L,M}{X,Y,Z} \] +%\end{verbatim} +% will produce +% \[ \Jacobian{K,L,M}{X,Y,Z} = \Jacobiandet[\displaystyle][3ex]{K,L,M}{X,Y,Z}. +% \] +% The \cs{Jacobiandet} macro will understand implied multicomponent Jacobians, +% too, namely, +% \begin{verbatim} +% \[ \Jacobian{f_1,\dots,f_m}{x_1,\dots,x_m} = +% \Jacobiandet{f_1,\dots,f_m}{x_1,\dots,x_m} \] +%\end{verbatim} +% typesets as +% \[ \Jacobian{f_1,\dots,f_m}{x_1,\dots,x_m} = +% \Jacobiandet{f_1,\dots,f_m}{x_1,\dots,x_m}. \] +% If the option |moles-range| or the \env{thermomolesrange} environment is +% used, the same code produces +% \begin{thermomolesrange} +% \[ \Jacobian{f_1,\dots,f_m}{x_1,\dots,x_m} = +% \Jacobiandet{f_1,\dots,f_m}{x_1,\dots,x_m}. \] +% \end{thermomolesrange} +% % \subsection{Sums and Products} % \DescribeMacro{\sumall} % \DescribeMacro{\sumallbutlast} % \DescribeMacro{\prodall} % It is common to require sums and products such as -% \[ \sum_{i=1}^C x_i = 1 \quad \text{or} \quad -% x_C = 1 - \sum_{i=1}^{C-1} x_i \quad \text{or} \quad -% \Gt = \sum_{j=1}^C \mu_j\Nt_j \quad \text{and} \quad -% K = \prod_{k=1}^C a_k^{\nu_k}. \] +% \[ \sumall_i x_i = 1 \quad \text{or} \quad +% x_\ncomponents = 1 - \sumallbutlast_i x_i \quad \text{or} \quad +% \Gt = \sumall_j \mu_j\Nt_j \quad \text{and} \quad +% K = \prodall_k a_k^{\nu_k}. \] % This package defines shortcuts to typeset such terms thus: % \begin{verbatim} % \[ \sumall_i x_i = 1 \quad \text{or} \quad % x_\ncomponents = 1 - \sumallbutlast_i x_i \quad \text{or} \quad % \Gt = \sumall_j \mu_j\Nt_j \quad \text{and} \quad -% K = \prodall_k a_k^{\nu_k}. \] +% K = \prodall_k a_k^{\nu_k} \]. %\end{verbatim} -% The symbol $C$ can be changed by redefining \cs{ncomponents}. This is done -% automatically by some package options (e.g., |TesterModell| changes it to -% $n$; |Sandler| changes it to $\mathcal{C}$; |Thompson| changes it to -% $c$). +% The symbol $C$ can be changed by redefining the expandable macro +% \cs{ncomponents}. This is done automatically by some package options (e.g., +% |TesterModell| changes it to $n$; |Sandler| changes it to $\mathcal{C}$; +% |Thompson| changes it to $c$). % % \section{Loading the Package} \label{sec:loading} % To load the package with the defaults enabled, load it the usual way: @@ -981,9 +1227,11 @@ % \verb"parentheses", \verb"intensive-plain", and \verb"moles-index". % These define, respectively, the default symbols to use for total energy, % internal energy, Helmholtz free energy, and so forth; the manner of writing -% partial derivatives; the delimiters around partial derivatives; and the -% manner of denoting extensive, molar, and specific properties. The default -% behavior can be altered by options in the following section. +% partial derivatives; the delimiters around partial derivatives; the +% manner of denoting extensive, molar, and specific properties; and the +% manner of writing the number of moles of all or most species in partial +% derivatives. The default behavior can be altered by options in the following +% section. % % \subsection{Package Options} % There are three categories of options: options that affect which symbols are @@ -995,6 +1243,10 @@ % energy, internal energy, Helmholtz free energy, and so forth. These are % summarized in Table~\ref{table:symbol-sets}. The default is \verb"EUAGHan". % +% \NewExtensiveProperty{f}{F} +% \NewExtensiveProperty{a}{A} +% \NewExtensiveProperty{ee}{\mathcal{E}} +% \NewExtensiveProperty{aa}{\mathcal{A}} % \begin{table} % \caption{Options controlling which symbols to use by default. The % macros \cs{Et}, \cs{Ut}, \cs{Ft}, \cs{Gt}, \cs{Ht}, \cs{At}, and @@ -1010,169 +1262,79 @@ % Option & \verb"\Et" & \verb"\Ut" & \verb"\Ft" & \verb"\Gt" & \verb"\Ht" % & \verb"\At" & \verb"\Nt" \\ % \midrule -% \verb"EUAGHan" & $\thermounderline{E}$ -% & $\thermounderline{U}$ -% & $\thermounderline{A}$ -% & $\thermounderline{G}$ -% & $\thermounderline{H}$ -% & $\thermounderline{a}$ -% & $n$ -% \\ -% \verb"EUAGHaN" & $\thermounderline{E}$ -% & $\thermounderline{U}$ -% & $\thermounderline{A}$ -% & $\thermounderline{G}$ -% & $\thermounderline{H}$ -% & $\thermounderline{a}$ -% & $N$ -% \\ -% \verb"EUHAGan" & \multicolumn{7}{l}{(synonym for \texttt{EUAGHan})} \\ -% \verb"EUHAGaN" & \multicolumn{7}{l}{(synonym for \texttt{EUAGHaN})} \\ -% \verb"EUFGHAn" & $\thermounderline{E}$ -% & $\thermounderline{U}$ -% & $\thermounderline{F}$ -% & $\thermounderline{G}$ -% & $\thermounderline{H}$ -% & $\thermounderline{A}$ -% & $n$ -% \\ -% \verb"EUFGHAN" & $\thermounderline{E}$ -% & $\thermounderline{U}$ -% & $\thermounderline{F}$ -% & $\thermounderline{G}$ -% & $\thermounderline{H}$ -% & $\thermounderline{A}$ -% & $N$ -% \\ -% \verb"EEFGHAn" & $\thermounderline{E}$ -% & $\thermounderline{E}$ -% & $\thermounderline{F}$ -% & $\thermounderline{G}$ -% & $\thermounderline{H}$ -% & $\thermounderline{A}$ -% & $n$ -% \\ -% \verb"EEFGHAn" & $\thermounderline{E}$ -% & $\thermounderline{E}$ -% & $\thermounderline{F}$ -% & $\thermounderline{G}$ -% & $\thermounderline{H}$ -% & $\thermounderline{A}$ -% & $N$ -% \\ -% \verb"EEFGHan" & $\thermounderline{E}$ -% & $\thermounderline{E}$ -% & $\thermounderline{F}$ -% & $\thermounderline{G}$ -% & $\thermounderline{H}$ -% & $\thermounderline{a}$ -% & $n$ -% \\ -% \verb"EEFGHaN" & $\thermounderline{E}$ -% & $\thermounderline{E}$ -% & $\thermounderline{F}$ -% & $\thermounderline{G}$ -% & $\thermounderline{H}$ -% & $\thermounderline{a}$ -% & $N$ -% \\ -% \verb"EEAGHaN" & $\thermounderline{E}$ -% & $\thermounderline{E}$ -% & $\thermounderline{A}$ -% & $\thermounderline{G}$ -% & $\thermounderline{H}$ -% & $\thermounderline{a}$ -% & $N$ -% \\ -% \verb"EUAGHAn" & $\thermounderline{E}$ -% & $\thermounderline{U}$ -% & $\thermounderline{A}$ -% & $\thermounderline{G}$ -% & $\thermounderline{H}$ -% & $\thermounderline{A}$ -% & $n$ -% \\ -% \verb"EUAGHAN" & $\thermounderline{E}$ -% & $\thermounderline{U}$ -% & $\thermounderline{A}$ -% & $\thermounderline{G}$ -% & $\thermounderline{H}$ -% & $\thermounderline{A}$ -% & $N$ -% \\ -% \verb"EUFGHan" & $\thermounderline{E}$ -% & $\thermounderline{U}$ -% & $\thermounderline{F}$ -% & $\thermounderline{G}$ -% & $\thermounderline{H}$ -% & $\thermounderline{a}$ -% & $n$ -% \\ -% \verb"EUFGHaN" & $\thermounderline{E}$ -% & $\thermounderline{U}$ -% & $\thermounderline{F}$ -% & $\thermounderline{G}$ -% & $\thermounderline{H}$ -% & $\thermounderline{a}$ -% & $N$ -% \\ +% |EUAGHan| & $\Et$ & $\Ut$ & $\Ft$ & $\Gt$ & $\Ht$ & $\At$ & $n$ \\ +% |EUAGHaN| & $\Et$ & $\Ut$ & $\Ft$ & $\Gt$ & $\Ht$ & $\At$ & $N$ \\ +% |EUHAGan| & \multicolumn{7}{l}{(synonym for \texttt{EUAGHan})} \\ +% |EUHAGaN| & \multicolumn{7}{l}{(synonym for \texttt{EUAGHaN})} \\ +% |EUFGHAn| & $\Et$ & $\Ut$ & $\ft$ & $\Gt$ & $\Ht$ & $\at$ & $n$ \\ +% |EUFGHAN| & $\Et$ & $\Ut$ & $\ft$ & $\Gt$ & $\Ht$ & $\at$ & $N$ \\ +% |EEFGHAn| & $\eet$ & $\Et$ & $\ft$ & $\Gt$ & $\Ht$ & $\at$ & $n$ \\ +% |EEFGHAN| & $\eet$ & $\Et$ & $\ft$ & $\Gt$ & $\Ht$ & $\at$ & $N$ \\ +% |EEFGHan| & $\eet$ & $\Et$ & $\ft$ & $\Gt$ & $\Ht$ & $\At$ & $n$ \\ +% |EEFGHaN| & $\eet$ & $\Et$ & $\ft$ & $\Gt$ & $\Ht$ & $\At$ & $N$ \\ +% |EEAGHaN| & $\eet$ & $\Et$ & $\Ft$ & $\Gt$ & $\Ht$ & $\At$ & $N$ \\ +% |EEAGHAN| & $\eet$ & $\Et$ & $\Ft$ & $\Gt$ & $\Ht$ & $\aat$ & $n$ \\ +% |EUAGHAN| & $\Et$ & $\Ut$ & $\Ft$ & $\Gt$ & $\Ht$ & $\aat$ & $N$ \\ +% |EUFGHan| & $\Et$ & $\Ut$ & $\ft$ & $\Gt$ & $\Ht$ & $\At$ & $n$ \\ +% |EUFGHaN| & $\Et$ & $\Ut$ & $\ft$ & $\Gt$ & $\Ht$ & $\At$ & $N$ \\ % \bottomrule % \end{tabular} % \end{table} % % Using \verb"EUAGHan" (the default), we might use the following markup: % \begin{verbatim} -% \[ \Ft = \Ut - T\St = -P\Vt + \sum_i \mu_i \Nt_i + \sigma d\At -% \qquad \Hm = \Um + P\Vm \qquad \Et = \Ut + \frac12 mv^2 \] +% \[ \Ft = \Ut - T\St = -P\Vt + \sumall_i \mu_i \Nt_i + \sigma \At +% \qquad \Hm = \Um + P\Vm \qquad \Et = \Ut + \frac12 mv^2 \], %\end{verbatim} % which would look like -% \[ \thermounderline{A} -% = \thermounderline{U} - T\thermounderline{S} -% = -P\thermounderline{V} + \sum_i \mu_i n_i + \sigma d\thermounderline{a} -% \qquad H = U + PV -% \qquad \thermounderline{E} = \thermounderline{U} + \frac12 mv^2. \] -% Using the \verb"EUFGHAN" option, the same markup would yield -% \[ \thermounderline{F} -% = \thermounderline{U} - T\thermounderline{S} -% = -P\thermounderline{V} + \sum_i \mu_i N_i + \sigma d\thermounderline{A} +% \[ \Ft = \Ut - T\St = -P\Vt + \sumall_i \mu_i \Nt_i + \sigma \At +% \qquad \Hm = \Um + P\Vm \qquad \Et = \Ut + \frac12 mv^2 \] +% Using the \verb"EEFGHAN" option, the same markup would yield +% \[ \ft +% = \Et - T\St +% = -P\Vt + \sumall_i \mu_i N_i + \sigma \at % \qquad H = U + PV -% \qquad \thermounderline{E} = \thermounderline{U} + \frac12 mv^2. \] +% \qquad \eet = \Et + \frac12 mv^2. \] % % \subsubsection{Options for Extensive vs.\ Molar Properties} % There are four sets of notation that define how extensive properties are % represented, as shown in Table~\ref{table:extensive}. % The default is \verb"intensive-plain", which (using the volume as an % example) represents the total, molar, specific, and partial molar volumes, -% respectively, as $\thermounderline{V},$ $V,$ $\hat V,$ and $\Vpm{j},$ +% respectively, as $\Vt,$ $\Vm,$ $\Vs,$ and $\Vpm{j},$ % respectively. % % For example, the definition of the partial molar enthalpy would be different % depending on which set of notation is used. The markup % \begin{verbatim} -% \Hpm_i = \Partial{\Ht}{\Nt_i}{T,P,\allNsbut{i}} -% = \Partial{\Nt\Hm}{\Nt_i}{T,P,\allNsbut{i}} +% \[ \Hpm_i = \Partial*{\Ht}{\Nt_i}{T,P,\allNsbut{i}} +% = \Partial{\Nt\Hm}{\Nt_i}{T,P,\allNsbut{i}} \] %\end{verbatim} % yields the following, depending on the package option loaded: % \begin{align*} -% \Hpm{i} &= \left(\frac{\partial\thermounderline{H}} -% {\partial n_i}\right)_{T,P,n_{j\neq i}} -% = \left(\frac{\partial nH} -% {\partial n_i}\right)_{T,P,n_{j\neq i}} +% \Hpm_i &= \Partial*{\Ht}{\Nt_i}{T,P,\allNsbut{i}} +% = \Partial{\Nt\Hm}{\Nt_i}{T,P,\allNsbut{i}} % && \text{\texttt{intensive-plain}} \\ -% \Hpm{i} &= \left(\frac{\partial H} -% {\partial n_i}\right)_{T,P,n_{j\neq i}} -% = \left(\frac{\partial n\thermounderline{H}} -% {\partial n_i}\right)_{T,P,n_{j\neq i}} +% \Hpm_i &= +% \begin{thermoextensiveplain} +% \Partial*{\Ht}{\Nt_i}{T,P,\allNsbut{i}} +% = \Partial{\Nt\Hm}{\Nt_i}{T,P,\allNsbut{i}} +% \end{thermoextensiveplain} % && \text{\texttt{extensive-plain}} \\ -% \Hpm{i} &= \left(\frac{\partial H^t} -% {\partial n_i}\right)_{T,P,n_{j\neq i}} -% = \left(\frac{\partial nH} -% {\partial n_i}\right)_{T,P,n_{j\neq i}} +% \Hpm_i &= +% \begin{thermoextensivesuperscript} +% \Partial*{\Ht}{\Nt_i}{T,P,\allNsbut{i}} +% = \Partial{\Nt\Hm}{\Nt_i}{T,P,\allNsbut{i}} +% \end{thermoextensivesuperscript} % && \text{\texttt{extensive-superscript}} \\ -% \Hpm{i} &= \left(\frac{\partial H} -% {\partial n_i}\right)_{T,P,n_{j\neq i}} -% = \left(\frac{\partial nh} -% {\partial n_i}\right)_{T,P,n_{j\neq i}} +% \begin{thermointensivelowercase} +% \Hpm_i +% \end{thermointensivelowercase} +% &= +% \begin{thermointensivelowercase} +% \Partial*{\Ht}{\Nt_i}{T,P,\allNsbut{i}} +% = \Partial{\Nt\Hm}{\Nt_i}{T,P,\allNsbut{i}} +% \end{thermointensivelowercase} % && \text{\texttt{intensive-lowercase}} % \end{align*} % The use of \verb"intensive-lowercase" is strongly discouraged. @@ -1183,28 +1345,52 @@ % \begin{table} % \caption{Notation sets that can be set using the options % \texttt{intensive-plain} (the default), \texttt{extensive-plain}, -% \texttt{extensive-superscript}, and \texttt{intensive-lowercase}, -% respectively. Note that specific quantities are generally assumed to -% look like the molar symbol with a caret on top.} +% \texttt{extensive-superscript}, and \texttt{intensive-lowercase}.} % \label{table:extensive} % \centering\small -% \newcommand*{\vpm}[2][]{\mkern1mu\overline{\mkern-1mu v_{\mkern-2mu #2}^{#1}\mkern-2mu}\mkern2mu} % \begin{tabular}{l l l l l l} % \toprule % Option & \verb"\Vt" & \verb"\Vm" & \verb"\Vs" & \verb"\Vpm_i" \\ % \midrule -% \verb"intensive-plain" & $\thermounderline{V}$ & $V$ & $\hat V$ -% & $\Vpm{i}$ \\ -% \verb"extensive-plain" & $V$ & $\thermounderline{V}$ & $\hat V$ -% & $\Vpm{i}$\rule{0pt}{2.5ex} \\ -% \verb"extensive-superscript" & $V^t$ & $V$ & $\hat V$ -% & $\Vpm{i}$\rule{0pt}{2.5ex} \\ -% \verb"intensive-lowercase" & $V$ & $v$ & $\hat v$ -% & $\vpm{i}$\rule{0pt}{2.5ex} \\ +% \verb"intensive-plain" & $\Vt$ & $\Vm$ & $\Vs$ & $\Vpm{i}$ \\[2ex] +% \verb"extensive-plain" & +% \begin{thermoextensiveplain}$\Vt$\end{thermoextensiveplain} & +% \begin{thermoextensiveplain}$\Vm$\end{thermoextensiveplain} & +% \begin{thermoextensiveplain}$\Vs$\end{thermoextensiveplain} & +% \begin{thermoextensiveplain}$\Vpm{i}$\end{thermoextensiveplain} +% \\[2ex] +% \verb"extensive-superscript" & +% \begin{thermoextensivesuperscript}$\Vt$\end{thermoextensivesuperscript} & +% \begin{thermoextensivesuperscript}$\Vm$\end{thermoextensivesuperscript} & +% \begin{thermoextensivesuperscript}$\Vs$\end{thermoextensivesuperscript} & +% \begin{thermoextensivesuperscript}$\Vpm{i}$\end{thermoextensivesuperscript} \\[2ex] +% \verb"intensive-lowercase" & +% \begin{thermointensivelowercase}$\Vt$\end{thermointensivelowercase} & +% \begin{thermointensivelowercase}$\Vm$\end{thermointensivelowercase} & +% \begin{thermointensivelowercase}$\Vs$\end{thermointensivelowercase} & +% \begin{thermointensivelowercase}$\Vpm{i}$\end{thermointensivelowercase} +% \\ % \bottomrule % \end{tabular} % \end{table} % +% \pagebreak[1]\relax +% \setmarginparsize{\footnotesize} +% \DescribeEnv{thermointensiveplain} +% \DescribeEnv{thermoextensiveplain} +% \DescribeEnv{thermoextensivesuperscript} +% \DescribeEnv{thermointensivelowercase} +% \restoremarginparsize +% It is possible to change notation locally, though there are very, very few +% good reasons why you would want to do this in a regular document---normally, +% one would use the corresponding package options. The environment +% \env{thermointensiveplain} means \cs{St} will become $\St$ and \cs{Sm} will +% become $\Sm$ in the text. Similarly, inside \env{thermoextensiveplain}, +% \cs{St} will become $S$ and \cs{Sm} will become $\St$. +% Inside \env{thermoextensivesuperscript}, \cs{St} will become $S^t$ and +% \cs{Sm} will be $S$; and inside \env{thermointensivesubscript}, +% \cs{St} will be $S$ and \cs{Sm} will be $s$. +% % \subsubsection{Options Affecting Partial Derivatives} % There are several options that change how partial derivatives are rendered. % First are the options that affect the delimiters. We will use the following @@ -1214,148 +1400,184 @@ % = \PartialMixSecond{\Gm}{P}{T}{} % = -\Partial{\Sm}{P}{T}. \] %\end{verbatim} -% Using the \verb"parentheses" option (the default), this gives -% \[ \left(\frac{\partial V}{\partial T}\right)_{P} \mkern-8mu -% = \left(\frac{\partial^2 G}{\partial T \partial P}\right) -% = \left(\frac{\partial^2 G}{\partial P \partial T}\right) -% = -\left(\frac{\partial S}{\partial P}\right)_{T}. \] -% The option \verb"brackets" changes the output to -% \[ \left[\frac{\partial V}{\partial T}\right]_{P} \mkern-8mu -% = \left[\frac{\partial^2 G}{\partial T \partial P}\right] -% = \left[\frac{\partial^2 G}{\partial P \partial T}\right] -% = -\left[\frac{\partial S}{\partial P}\right]_{T}. \] +% Using the |parentheses| option (the default), this gives +% \[ \Partial*{\Vm}{T}{P} = \PartialMixSecond{\Gm}{T}{P}{} +% = \PartialMixSecond{\Gm}{P}{T}{} +% = -\Partial{\Sm}{P}{T}. \] +% The option |brackets| changes the output to +% \begin{thermobrackets} +% \[ \Partial*{\Vm}{T}{P} = \PartialMixSecond{\Gm}{T}{P}{} +% = \PartialMixSecond{\Gm}{P}{T}{} +% = -\Partial{\Sm}{P}{T}. \] +% \end{thermobrackets}\relax % The option \verb"bar" changes the output to -% \[ \left.\frac{\partial V}{\partial T}\right\rvert_{P} \mkern-8mu -% = \left.\frac{\partial^2 G}{\partial T \partial P}\right. -% = \left.\frac{\partial^2 G}{\partial P \partial T}\right. -% = -\left.\frac{\partial S}{\partial P}\right\rvert_{T}. \] +% \begin{thermobar} +% \[ \Partial*{\Vm}{T}{P} = \PartialMixSecond{\Gm}{T}{P}{} +% = \PartialMixSecond{\Gm}{P}{T}{} +% = -\Partial{\Sm}{P}{T}. \] +% \end{thermobar}\relax % The option \verb"plain-derivatives" eliminates all delimiters; this forces % the \verb"nosubscripts" option. The output in this case is -% \[ \left.\frac{\partial V(T,P)}{\partial T}\right. -% = \left.\frac{\partial^2 G(T,P)}{\partial T \partial P}\right. -% = \left.\frac{\partial^2 G(P,T)}{\partial P \partial T}\right. -% = -\left.\frac{\partial S(P,T)}{\partial P}\right. \] -% +% \begin{thermoplain}% +% \[ \Partial*{\Vm}{T}{P} = \PartialMixSecond{\Gm}{T}{P}{} +% = \PartialMixSecond{\Gm}{P}{T}{} +% = -\Partial{\Sm}{P}{T}. \] +% \end{thermoplain}\relax % Accompanying the \verb"plain-derivatives" option is the \verb"nosubscripts" % option, which overrides the default option \verb"subscripts". This option % makes partial derivatives such as -% \[ \left(\frac{\partial V}{\partial P}\right)_{T} -% \qquad \text{(\texttt{subscripts} option)}, \] +% \[ \begin{thermosubscripts} +% \Partial{\Vm}{P}{T} \qquad \text{(\texttt{subscripts} option)}, +% \end{thermosubscripts}\relax \] % and instead renders them -% \[ \left(\frac{\partial V(P,T)}{\partial P}\right) -% \qquad \text{(\texttt{nosubscripts} option)}. \] +% \[ \begin{thermoNOsubscripts} +% \Partial{\Vm}{P}{T} \qquad \text{(\texttt{nosubscripts} option)}, +% \end{thermoNOsubscripts} \] % Combined with \verb"plain-derivatives", this would give -% \[ \left.\frac{\partial V(P,T)}{\partial P}\right. -% \qquad \text{(\texttt{nosubscripts} and \texttt{plain-derivatives} -% options)} . \] -% The order of the variables is determined by the arguments given: it is -% always written with the variable that is changing first, and the other -% variables in the order given in the final argument to \cs{Partial} and -% friends. This will result in things like the following: -% \begin{verbatim} -% \[ \Partial{\Vm}{T}{P} = \PartialMixSecond{\Gm}{T}{P}{} -% = \PartialMixSecond{\Gm}{P}{T}{} = -\Partial{\Sm}{P}{T}, \] -%\end{verbatim} -% which would produce (using \verb"plain-derivatives") -% \[ \frac{\partial V(T,P)}{\partial T} -% = \frac{\partial^2 G(T,P)}{\partial T\partial P} -% = \frac{\partial^2 G(P,T)}{\partial P\partial T} -% = - \frac{\partial S(P,T)}{\partial P} \] -% This is not unclear, but the variables appear in a different order. +% \[ \begin{thermoplain} +% \Partial{\Vm}{P}{T} \qquad \text{(\texttt{nosubscripts} and +% \texttt{plain-derivatives} options)}. +% \end{thermoplain} \] +% The variables are sorted into an order defined by an internal constant, +% meaning $T$ will always be listed before $P$. The order by default is in +% the order that terms appear in the fundamental equations, that is, +% \begin{gather*} +% d\Ut = T \,d\St - P \,d\Vt + \mu \,d\Nt \\ +% d\Ht = T \,d\St + \Vt \,dP + \mu \,d\Nt \\ +% d\Ft = -\St\,dT - P \,d\Vt + \mu \,d\Nt \\ +% \vdots \\ +% d\Lt = -\St\,dT - P \,d\Vt - \Nt\,d\mu, +% \end{gather*} +% with the exception that subscripted variables are (currently) not sortable. +% If \verb"\Nt_i" or some similar construct appears as a variable and +% \verb"\allNsbut{i}" appears in the held-constant list, the package will +% assume that the argument list \emph{should} contain all of the mole numbers. +% Symbols without subscripts that are not in the fundamental equation or one of +% its variants are sorted in alphabetical order. % % \DescribeEnv{thermoparentheses} % \DescribeEnv{thermobrackets} % \DescribeEnv{thermobar} % \DescribeEnv{thermoplain} % If you want to use parentheses \emph{locally}, even though your overall -% document uses another delimiter, the |thermoparentheses| environment will do -% that. Similarly, |thermobrackets| will temporarily switch to brackets, -% |thermobar| will temporarily switch to a tailing vertical bar, and -% |thermoplain| will remove delimiters altogether. +% document uses another delimiter, the \env{thermoparentheses} environment will +% do that. Similarly, \env{thermobrackets} will temporarily switch to brackets, +% \env{thermobar} will temporarily switch to a tailing vertical bar, and +% \env{thermoplain} will remove delimiters altogether. % % \DescribeEnv{thermosubscripts} % \DescribeEnv{thermoNOsubscripts} -% The environments |thermosubscripts| and |thermoNOsubscripts| force the -% use or disuse of subscripts, respectively. +% The environments \env{thermosubscripts} and \env{thermoNOsubscripts} +% force the use or disuse of subscripts, respectively. % % \subsubsection{Options Regarding the Number of Moles} -% \DescribeMacro{\allNs} -% \DescribeMacro{\allNsbut} +% \DescribeMacro{\allNs}% +% \DescribeMacro{\allNsbut}% % The default option \verb"moles-index" defines the macro \cs{allNs} to expand -% to $\vec{n}$ and the macro \verb"\allNsbut{i}" to expand to $n_{j\neq i}$. +% to $\allNs$ and the macro \verb"\allNsbut{i}" to expand to $\allNsbut{i}$. % You can change the dummy index: \verb"\allNsbut[k]{i}" expands to -% $n_{k\neq i}$ by default. This is typically not necessary, however: if you -% type \verb"\allNsbut{j}", the package will figure out that you want -% $\Nt_{k\neq j}$ rather than $\Nt_{j\neq j}$. The time to use the optional +% $\allNsbut[k]{i}$ by default. This is typically not necessary, however: if +% you type \verb"\allNsbut{j}", the package will figure out that you want +% $\allNsbut{j}$ rather than $\Nt_{j\neq j}$. The time to use the optional % argument is in situations such as -% \[ \Partial{\mu_j}{\Nt_k}{\Nt_{i\neq k}}, \] +% \[ \Partial{\mu_j}{\Nt_k}{\allNsbut[i]{k}}, \] % which is incorrect if the dummy index $j$ is used in place of the $i$. % % You can change these to expand to ranges using the \verb"moles-range" -% option, which renders \cs{allNs} as $n_1,\dotsc,n_C$ and \verb"\allNsbut{i}" -% as $n_1,\dotsc,[n_i],\dotsc,n_C$. The optional argument is ignored in this -% set of notation. Examples of these options are shown in -% Table~\ref{table:allNs}. +% option, which renders \cs{allNs} as +% $\begin{thermomolesrange}\allNs\end{thermomolesrange}$ and +% \verb"\allNsbut{i}" as +% $\begin{thermomolesrange}\allNsbut{i}\end{thermomolesrange}.$ +% The optional argument is ignored in this set of notation. Examples of these +% options are shown in Table~\ref{table:allNs}. +% +% \DescribeEnv{thermomolesrange} +% The environment \env{thermomolesrange} temporarily redefines \cs{allNs} and +% other range-oriented macros as though the |moles-range| package option had +% been invoked. % -% \DescribeMacro{\ncomponents} +% \DescribeMacro{\ncomponents}% % You can change the symbol for the number of components (default: $C$) by -% redefining the macro \cs{ncomponents}. +% redefining the macro \cs{ncomponents}. This is done for you by some package +% options that define notation for particular textbooks. % % \begin{table} % \caption{Illustration of the \texttt{moles-index} and \texttt{moles-range} % options and their effects on \cs{allNs} and \cs{allNsbut}.} % \label{table:allNs} -% \SpecialUsageIndex{\allNs}\relax -% \SpecialUsageIndex{\allNsbut}\relax -% \SpecialUsageIndex{\allXs}\relax -% \SpecialUsageIndex{\allXsbut}\relax +%^^A TODO The \leavevmode macro here is to prevent whitespace from building +%^^A up due to a bug in old versions of hypdoc. It should be harmless to +%^^A leave it in there, but consider removing it at some point. +% \leavevmode +% \SpecialMacroIndex{\allNs}\relax +% \SpecialMacroIndex{\allNsbut}\relax +% \SpecialMacroIndex{\allXs}\relax +% \SpecialMacroIndex{\allXsbut}\relax % \centering % \begin{minipage}{4.49in}\renewcommand*{\footnoterule}{\vskip-1.5ex}% % \small % \begin{tabular}{l l l} % \toprule % Macro\footnote{You may use $C$ directly instead of \cs{ncomponents} -% here, but then it will not change $C-1$ to $C-2$ (or, say, $M-1$ to -% $M-2$) if you want to redefine \cs{ncomponents} later.} +% here, but then it will not change to another symbol if you want to +% switch to an option that redefines \cs{ncomponents} later.} % & \verb"moles-index" & \verb"moles-range" \\ % \midrule -% \verb"\allNs" & $\vec{n}$ & $n_1,\dotsc,n_C$ \\ -% \verb"\allNsbut{1}" & $n_{j\neq 1}$ & $n_2,\dotsc,n_C$ \\ -% \verb"\allNsbut{i}" & $n_{j\neq i}$ & $n_1,\dotsc,[n_i],\dotsc,n_C$ \\ -% \verb"\allNsbut{j}" & $n_{k\neq j}$ & $n_1,\dotsc,[n_j],\dotsc,n_C$ \\ -% \verb"\allNsbut{\ncomponents}" & $n_{j\neq C}$ & $n_1,\dotsc,n_{C-1}$ \\ -% \verb"\allNsbut[k]{i}" & $n_{k\neq i}$ & $n_1,\dotsc,[n_i],\dotsc,n_C$ \\ -% \verb"\allXs" & $\vec{x}$ & $x_1,\dotsc,x_{C}$ \\ -% \verb"\allXsbut{1}" & $x_{j\neq 1,C}$ & $x_2,\dotsc,x_{C-1}$ \\ -% \verb"\allXsbut{i}" & $x_{j\neq i,C}$ & $x_1,\dotsc,[x_i],\dotsc,x_{C-1}$ \\ -% \verb"\allXsbut{j}" & $x_{k\neq j,C}$ & $x_1,\dotsc,[x_j],\dotsc,x_{C-1}$ \\ -% \verb"\allXsbut{\ncomponents-1}" & $x_{j\neq C-1,C}$ & $x_1,\dotsc,x_{C-2}$ \\ -% \verb"\allXsbut[k]{\ncomponents-1}" & $x_{k\neq C-1,C}$ & $x_1,\dotsc,x_{C-2}$ \\ +% \verb"\allNs" & $\allNs$ +% & $\begin{thermomolesrange}\allNs\end{thermomolesrange}$ \\ +% \verb"\allNsbut{1}" & $\allNsbut{1}$ +% & $\begin{thermomolesrange}\allNsbut{1}\end{thermomolesrange}$ \\ +% \verb"\allNsbut{i}" & $\allNsbut{i}$ +% & $\begin{thermomolesrange}\allNsbut{i}\end{thermomolesrange}$ \\ +% \verb"\allNsbut{j}" & $\allNsbut{j}$ +% & $\begin{thermomolesrange}\allNsbut{j}\end{thermomolesrange}$ \\ +% \verb"\allNsbut{\ncomponents}" & $\allNsbut{\ncomponents}$ +% & $\begin{thermomolesrange}\allNsbut{\ncomponents}\end{thermomolesrange}$\\ +% \verb"\allNsbut[k]{i}" & $\allNsbut[k]{i}$ +% & $\begin{thermomolesrange}\allNsbut[k]{i}\end{thermomolesrange}$\\ +% \verb"\allXs" & $\allXs$ +% & $\begin{thermomolesrange}\allXs\end{thermomolesrange}$ \\ +% \verb"\allXsbut{1}" & $\allXsbut{1}$ +% & $\begin{thermomolesrange}\allXsbut{1}\end{thermomolesrange}$ \\ +% \verb"\allXsbut{i}" & $\allXsbut{i}$ +% & $\begin{thermomolesrange}\allXsbut{i}\end{thermomolesrange}$ \\ +% \verb"\allXsbut{j}" & $\allXsbut{j}$ +% & $\begin{thermomolesrange}\allXsbut{j}\end{thermomolesrange}$ \\ +% \verb"\allXsbut{\ncomponents-1}" & $\allXsbut{\ncomponents-1}$ +% & $\begin{thermomolesrange}\allXsbut{\ncomponents-1} +% \end{thermomolesrange}$ \\ +% \verb"\allXsbut[k]{\ncomponents-1}" & $\allXsbut[k]{\ncomponents-1}$ +% & $\begin{thermomolesrange}\allXsbut[k]{\ncomponents-1} +% \end{thermomolesrange}$ \\ % \verb"\allXsbut{\ncomponents}"\footnote{This would typically be used -% to denote something like $\Gt(T,P,n,x_1,\dotsc,x_{C-1})$ rather -% than in a subscript, but it looks silly if we don't handle this -% case this way.} -% & $x_{j\neq C}$ & $x_1,\dotsc,x_{C-1}$ \\ +% to denote something like +% \( \begin{thermomolesrange} +% \Gt(T,P,\Nt,\allXsbut{\ncomponents}) +% \end{thermomolesrange} +% \) rather than in a subscript, but it looks silly if we do not +% handle this case this way.} +% & $\allXsbut{\ncomponents}$ +% & $\begin{thermomolesrange}\allXsbut{\ncomponents} +% \end{thermomolesrange}$ \\ % \bottomrule % \end{tabular} % \end{minipage} % \end{table} % % \subsubsection{Other Options} -% \DescribeMacro{\dbar} -% \newcommand*{\dbar}{{\mkern5mu\mathchar'26\mkern-10mu d}}\relax +% \DescribeMacro{\dbar}% % The default for path-dependent one-forms (often called ``inexact % differentials'') is \cs{dbar}, which looks like $\dbar$. This can be changed, % if desired, to a delta ($\delta$) with the \verb"delta" option to the % package. % -% It should be noted that the \cs{dbar} macro is not very stable: changing +% It should be noted that the \cs{dbar} macro is context-dependent: changing % the typeface to something not supported will probably ruin it, as the kerning % is very font-specific. This package currently supports Computer Modern, % Times, Palatino, Bitstream Charter, Garamond, and Utopia, but other typefaces % may require a manual redefinition. % -% \subsubsection{Options for Specific Textbooks} +% \subsubsection{Options for Particular Textbooks} % There are several options that load package options and/or redefine % particular commands to match the notation in a particular textbook. So far % the following textbooks are supported: @@ -1363,22 +1585,24 @@ % \item[Bejan] Notation used by Bejan, \emph{Advanced Engineering % Thermodynamics}, Third Edition. Wiley: Hoboken, 2006. Loads non-default % package options \verb"EUFGHAN", \verb"intensive-lowercase", and -% \verb"delta". Also swaps the definitions of \verb"\@specific" and -% \verb"\@intensive" and redefines \cs{cV}, \cs{cVs}, \cs{cVt}, +% \verb"delta". Also swaps the notation for specific and +% intensive properties and redefines \cs{cV}, \cs{cVs}, \cs{cVt}, % \cs{expansivitysymbol}, and \cs{ncomponents} to match his notation. % \item[CBK] Notation used by \c Cengel, Boles, and Kano\u glu, % \emph{Thermodynamics: An Engineering Approach}, Ninth Edition. % McGraw Hill: Singapore, 2020. Loads the non-default package options % \verb"EUAGHAN" and \verb"intensive-lowercase"; also redefines % partial molar, specific, and molar properties' notation to fit theirs, -% and redefines \cs{pressure@symbol}, \cs{Deltarxn}, +% and redefines the internal symbol for pressure, \cs{Deltarxn}, % \cs{compressibilitysymbol}, and \cs{expansivitysymbol} to fit their -% usage. Their prodigal symbols for specific and total volume are not +% usage. Their prodigal symbols for specific and total volume, which appear +% to be from the font ITC Benguiat Gothic Standard Book Oblique, are not % supported. % \item[ElliottLira] Notation used by Elliott and Lira, \emph{Introductory % Chemical Engineering Thermodynamics}, Second Edition. Prentice Hall: % Upper Saddle River, 2012. Loads the default package options and -% redefines \cs{allcomponents} and \cs{Deltarxn} to fit their notation. +% redefines \cs{IG}, \cs{IGM}, \cs{allcomponents}, and \cs{Deltarxn} to fit +% their notation. % \item[Koretsky] Notation used by Koretsky, \emph{Engineering and Chemical % Thermodynamics}, Second Edition, Wiley: New Caledonia, 2013. % Loads the non-default package options \verb"EUAGHAn", \verb"brackets", @@ -1396,15 +1620,15 @@ % \verb"EUFGHAn", \verb"intensive-lowercase", and \verb"delta"; removes the % left parenthesis in partial derivatives and redefines \cs{IGM}, \cs{IG}, % \cs{expansitivitysymbol}, \cs{allcomponents}, \cs{allbut}, \cs{Ft}, -% \cs{Helmholtz@symbol}, \cs{@intensive}, \cs{@specific}, \cs{fmix}, -% \cs{phimix}, and \cs{pressure@symbol} to fit their somewhat ill-advised -% notation. Also resets \cs{partialmolar} to match their use. +% \cs{fmix}, and \cs{phimix}, as well as symbols for the Helmholtz free +% energy and pressure, intensive and specific property notation, and +% partial molar notation to fit their somewhat ill-advised notation. % \item[Prausnitz] Notation used by Prausnitz, Lichtenthaler, and de Azevedo, % \emph{Molecular Thermodynamics of Fluid-Phase Equilibria}, Third Edition, % Pearson, 1998. Loads the non-default package option % \verb"intensive-lowercase" and redefines \cs{fmix}, \cs{phimix}, -% \cs{fpure}, \cs{phipure}, \cs{residual}, \cs{allcomponents}, and -% \cs{allbut} to fit their notation. +% \cs{fpure}, \cs{phipure}, \cs{Henryrat}, \cs{residual}, +% \cs{allcomponents}, and \cs{allbut} to fit their notation. % \item[Sandler] Notation used by Sandler, \emph{Chemical, Biochemical, and % Engineering Thermodynamics}, Fifth Edition. Wiley: Hoboken, 2017. % Loads non-default package options \verb"EUAGHaN" and @@ -1430,28 +1654,42 @@ % \cs{Henrymol}, \cs{gammarat}, and \cs{gammamol} to fit their style. % \item[Thompson] Notation used by Thompson, \emph{A Unified Introduction to % Chemical Engineering Thermodynamics}, Stillwater Press: Orono, 2000. -% Loads the non-default package options \verb"EUAGHAn" and \verb"delta"; -% also redefines \cs{excess}, \cs{residual}, \cs{allcomponents}, -% \cs{ncomponents}, \cs{IS}, \cs{IG}, \cs{IGM}, \cs{fpure}, \cs{phipure}, -% \cs{mix}, \cs{Deltamix}, \cs{Deltarxn}, \cs{@intensive}, and \cs{allbut} -% to match his notation. Note that he uses $c$, $n_C$, and $\mathrm{n}$ -% for the number of components in various places in the book; I chose $c$ -% for the definition of \cs{ncomponents}, but it is impossible to be -% completely consistent with his notation. +% Loads the non-default package options |EUAGHAn| and |delta|; +% also redefines \cs{excess}, \cs{residual}, \cs{Henryrat}, \cs{Henrymol}, +% \cs{allcomponents}, \cs{ncomponents}, \cs{IS}, \cs{IG}, \cs{IGM}, +% \cs{fpure}, \cs{phipure}, \cs{mix}, \cs{Deltamix}, \cs{Deltarxn}, and +% \cs{allbut} to match his notation, plus adjustments to intensive (molar) +% properties. Note that he uses $c$, $\mathrm{c}$, $n_C$, and +% $\mathrm{n}$ for the number of components in various places in the book; +% I chose $c$ for the definition of \cs{ncomponents}, but it is impossible +% to be completely consistent with his notation. % \end{description} % There may well be some inconsistencies between the notation in these books % and the symbols used here. I will fix such inconsistencies as I become aware % of them. +%^^X \end{documentation} % +% \setcounter{IndexColumns}{2} % \StopEventually{\PrintChanges\PrintIndex} % % ^^A-------------------------------------------------------------------------- % \iffalse %<*package> +%<@@=thermodynamics> % \fi % +%^^X\begin{implementation} % \section{Implementation} -% This package requires the \verb"amstext" package, as \cs{text} is used to +% We set up some non-standard token comparison variants; these are designed +% to catch both \cs{ncomponents}=\cs{ncomponents} and \cs{ncomponents}=$C$ +% (using the default options); we have to define \cs{ncomponents} to be +% expandable to make these work at all. +% \begin{macrocode} +\ExplSyntaxOn +\cs_generate_variant:Nn \tl_if_eq:nnTF { xxTF } +% \end{macrocode} +% +% This package requires the \pkg{amstext} package, as \tn{text} is used to % handle \cs{sat}, \cs{IS}, \cs{IG}, \cs{IGM}, \cs{Henrymol}, \cs{fusion}, % \cs{reaction}, \cs{vaporization}, and \cs{sublimation} by default, as well % as several other macros defined by package options. @@ -1469,47 +1707,57 @@ % We try to determine, at \verb"\begin{document}", which typeface you chose % based on the packages that are loaded and some of their internal definitions. % The \textsf{thermodynamics} package currently supports -% Computer Modern (the default or through \verb"lmodern"), -% Palatino (through \verb"pxfonts" or \verb"newpxmath"), -% Times (through \verb"txfonts", \verb"mathptmx", or \verb"newtxmath"), -% Utopia (through \verb"mathdesign"), -% Bitstream Charter (through \verb"mathdesign"), and -% Garamond (through \verb"mathdesign"). -% Definitions of \cs{dbar} (with \cs{newcommand*} or \cs{providecommand*}) +% Computer Modern (the default or through \pkg{lmodern}), +% Palatino (through \pkg{pxfonts} or \pkg{newpxmath}), +% Times (through \pkg{txfonts}, \pkg{mathptmx}, or \pkg{newtxmath}), +% Utopia (through \pkg{mathdesign}), +% Bitstream Charter (through \pkg{mathdesign}), and +% Garamond (through \pkg{mathdesign}). +% Definitions of \cs{dbar} (with \cs{newcommand*}, \cs{providecommand*}, +% \cs{NewDocumentCommand}, or \cs{ProvideDocumentCommand}) % in the preamble will override the ones here. % \begin{macrocode} \AtBeginDocument{ \@ifpackageloaded{pxfonts}{% - \providecommand*{\dbar}{{\mkern5mu\mathchar'26\mkern-10mu d}}% + \ProvideDocumentCommand{\dbar}{} + {\mkern5mu\mathchar'26\mkern-10mu d} }{} \@ifpackageloaded{newpxmath}{% - \providecommand*{\dbar}{{\mkern5mu\mathchar'26\mkern-10mu d}}% + \ProvideDocumentCommand{\dbar}{} + {\mkern5mu\mathchar'26\mkern-10mu d} }{} \@ifpackageloaded{txfonts}{% - \providecommand*{\dbar}{{\mkern5mu\mathchar'26\mkern-11mu d}}% + \ProvideDocumentCommand{\dbar}{} + {\mkern5mu\mathchar'26\mkern-11mu d} }{} \@ifpackageloaded{mathptmx}{% - \providecommand*{\dbar}{{\mkern5mu\mathchar'26\mkern-10mu d}}% + \ProvideDocumentCommand{\dbar}{} + {\mkern5mu\mathchar'26\mkern-10mu d} }{} \@ifpackageloaded{newtxmath}{% - \providecommand*{\dbar}{{\mkern5mu\mathchar'26\mkern-12mu d}}% + \ProvideDocumentCommand{\dbar}{} + {\mkern5mu\mathchar'26\mkern-11mu d} }{} \@ifpackageloaded{mathdesign}{% - \def\@charter{mdbch}% - \def\@utopia{mdput}% - \def\@garamond{mdugm}% - \ifx\MD@default@family\@utopia - \providecommand*{\dbar}{{\mkern8mu\mathchar'26\mkern-20mu d}}% - \fi - \ifx\MD@default@family\@charter - \providecommand*{\dbar}{{\mkern5mu\mathchar'26\mkern-15mu d}}% - \fi - \ifx\MD@default@family\@garamond - \providecommand*{\dbar}{{\mkern5mu\mathchar'26\mkern-17mu d}}% - \fi + \tl_const:Nn \c_@@_charter_tl {mdbch} + \tl_const:Nn \c_@@_utopia_tl {mdput} + \tl_const:Nn \c_@@_garamond_tl {mdugm} + \tl_if_eq:NNT \MD@default@family \c_@@_utopia_tl + { \ProvideDocumentCommand{\dbar}{} + {\mkern5mu\mathchar'26\mkern-20mu d} + } + \tl_if_eq:NNT \MD@default@family \c_@@_charter_tl + { \ProvideDocumentCommand{\dbar}{} + {\mkern5mu\mathchar'26\mkern-15mu d} + } + \tl_if_eq:NNT \MD@default@family \c_@@_garamond_tl + { \ProvideDocumentCommand{\dbar}{} + {\mkern5mu\mathchar'26\mkern-17mu d} + } }{} % Defaults to Computer Modern - \providecommand*{\dbar}{{\mkern3mu\mathchar'26\mkern-12mu d}} + \ProvideDocumentCommand{\dbar}{} + {\mkern3mu\mathchar'26\mkern-12mu d} } % \end{macrocode} % \end{macro} @@ -1521,30 +1769,16 @@ % their own, but rather accessed through the macros \cs{Ut}, \cs{Um}, and % \cs{Us} (using the internal energy as an example). % -% \begin{macro}{\totalenergy@symbol} -% \begin{macro}{\internalenergy@symbol} -% \begin{macro}{\Helmholtz@symbol} -% \begin{macro}{\Gibbs@symbol} -% \begin{macro}{\Landau@symbol} -% \begin{macro}{\enthalpy@symbol} -% \begin{macro}{\entropy@symbol} -% \begin{macro}{\area@symbol} -% \begin{macro}{\volume@symbol} -% \begin{macro}{\mole@symbol} -% \begin{macro}{\heat@symbol} -% \begin{macro}{\work@symbol} -% \begin{macro}{\temperature@symbol} -% \begin{macro}{\pressure@symbol} % The default symbols are not intended to be easy to change---the intended % mechanism is through package options. If you want to use a non-standard % symbol that is not available through one of the package options, you can -% redefine these macros inside -% \cs{makeatletter}\dots\cs{makeatother}. For example, +% redefine the internal token lists inside +% \cs{ExplSyntaxOn}\dots\cs{ExplSyntaxOff}. For example, % \begin{verbatim} -% \makeatletter -% \renewcommand*{\Helmholtz@symbol}{H} -% \renewcommand*{\enthalpy@symbol}{h} -% \makeatother +% \ExplSyntaxOn +% \tl_gset:Nn \g__thermodynamics_Helmholtz_symbol {H} +% \tl_gset:Nn \g__thermodynamics_enthalpy_symbol {h} +% \ExplSyntaxOff %\end{verbatim} % would define the ill-advised notation that I have nonetheless heard of % that uses $H$ for Helmholtz free energy and $h$ for enthalpy. @@ -1553,208 +1787,236 @@ % capacities; there is no user-level macro for the temperature or the pressure, % so it is up to the user to use consistent symbols for those properties. % \begin{macrocode} -\newcommand*{\totalenergy@symbol}{E} -\newcommand*{\internalenergy@symbol}{U} -\newcommand*{\Helmholtz@symbol}{A} -\newcommand*{\Gibbs@symbol}{G} -\newcommand*{\Landau@symbol}{\Omega} -\newcommand*{\enthalpy@symbol}{H} -\newcommand*{\entropy@symbol}{S} -\newcommand*{\area@symbol}{a} -\newcommand*{\volume@symbol}{V} -\newcommand*{\mole@symbol}{n} -\newcommand*{\heat@symbol}{Q} -\newcommand*{\work@symbol}{W} -\newcommand*{\temperature@symbol}{T} -\newcommand*{\pressure@symbol}{P} +\tl_new:N \g_@@_total_energy_symbol +\tl_new:N \g_@@_internal_energy_symbol +\tl_new:N \g_@@_Helmholtz_symbol +\tl_new:N \g_@@_Gibbs_symbol +\tl_new:N \g_@@_Landau_symbol +\tl_new:N \g_@@_enthalpy_symbol +\tl_new:N \g_@@_entropy_symbol +\tl_new:N \g_@@_area_symbol +\tl_new:N \g_@@_volume_symbol +\tl_new:N \g_@@_mole_symbol +\tl_new:N \g_@@_heat_symbol +\tl_new:N \g_@@_work_symbol +\tl_new:N \g_@@_temperature_symbol +\tl_new:N \g_@@_pressure_symbol + +\tl_gset:Nn \g_@@_total_energy_symbol E +\tl_gset:Nn \g_@@_internal_energy_symbol U +\tl_gset:Nn \g_@@_Helmholtz_symbol A +\tl_gset:Nn \g_@@_Gibbs_symbol G +\tl_gset:Nn \g_@@_Landau_symbol \Omega +\tl_gset:Nn \g_@@_enthalpy_symbol H +\tl_gset:Nn \g_@@_entropy_symbol S +\tl_gset:Nn \g_@@_area_symbol a +\tl_gset:Nn \g_@@_volume_symbol V +\tl_gset:Nn \g_@@_mole_symbol n +\tl_gset:Nn \g_@@_heat_symbol Q +\tl_gset:Nn \g_@@_work_symbol W +\tl_gset:Nn \g_@@_temperature_symbol T +\tl_gset:Nn \g_@@_pressure_symbol P % \end{macrocode} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} % -% \begin{macro}{\thermo@underline} -% \begin{macro}{\thermo@overline} -% We then define two macros and several lengths that we shall use when +% We then define two functions and several lengths that we shall use when % drawing rules above or below a symbol. The default is to use underlined % symbols for extensive quantities, plain symbols for molar quantities, and % carets for specific quantities, but this can be changed using package % options. -% ^^A TODO these would work better as kern 0.1*width, symbol, kern 0.2*width +%^^A TODO these might work better as kern 0.1*width, symbol, kern 0.2*width % \begin{macrocode} -\newcommand*{\thermo@underline}[1]{% - \mkern1mu\underline{\mkern-1mu #1\mkern-4mu}\mkern4mu% -} -\newcommand*{\thermo@overline}[1]{% - \mkern2mu\overline{\mkern-2mu #1\mkern-1mu}\mkern1mu% -} +\cs_new:Nn \@@_underline:n +{ \mkern1mu\underline{\mkern-1mu #1\mkern-4mu}\mkern4mu } +\cs_new:Nn \@@_overline:n +{ \mkern2mu\overline{\mkern-2mu #1\mkern-1mu}\mkern1mu } % \end{macrocode} -% \end{macro} -% \end{macro} % -% \begin{macro}{\PartialOpen} -% \begin{macro}{\PartialClose} -% \begin{macro}{\PartialEmptyClose} +% \begin{macro}{\PartialOpen,\PartialClose,\PartialEmptyClose} % We define three commands to use to denote the beginning and end of partial % derivatives. These symbols can be customized by package options. Default -% is \verb"parentheses", meaning that \verb"\[ \Partial{f}{x}{y} \]" renders as +% is |parentheses|, meaning that \verb"\[ \Partial{f}{x}{y} \]" renders as % \[ \left(\frac{\partial f}{\partial x}\right)_y \] % with the defaults. The macro \cs{PartialEmptyClose} is used when the last -% argument to \cs{Partial} is empty, which is important for the \verb"bar" -% option to the document class or inside the \verb"thermobar" environment. +% argument to \cs{Partial} is empty, which is important for the |bar| +% option to the document class or inside the \env{thermobar} environment. % \begin{macrocode} -\newcommand*{\PartialOpen}{(} -\newcommand*{\PartialClose}{)} -\newcommand*{\PartialEmptyClose}{)} +\tl_new:N \l_@@_PartialOpen_tl +\tl_new:N \l_@@_PartialEmptyClose_tl +\tl_new:N \l_@@_PartialClose_tl + +\tl_set:Nn \l_@@_PartialOpen_tl {(} +\tl_set:Nn \l_@@_PartialClose_tl {)} +\tl_set:Nn \l_@@_PartialEmptyClose_tl {)} % \end{macrocode} % \end{macro} -% \end{macro} -% \end{macro} % % \subsection{Package Options} % We declare a bunch of options for which sets of symbols to use. % These are summarized in Table~\ref{table:symbol-sets}. +% \changes{v1.01}{2023/09/15}{Changed options with two $E$ or two $A$ +% variables to use calligraphic letters for the less-common of the two.} % \begin{macrocode} \DeclareOption{EUAGHan}{}% the default -\DeclareOption{EUAGHaN}{\renewcommand*{\mole@symbol}{N}}% +\DeclareOption{EUAGHaN}{\tl_gset:Nn \g_@@_mole_symbol N}% \DeclareOption{EUHAGan}{\ExecuteOptions{EUAGHan}} \DeclareOption{EUHAGaN}{\ExecuteOptions{EUAGHaN}} -\DeclareOption{EUFGHAn}{% this is my favorite set of symbols - \renewcommand*{\Helmholtz@symbol}{F}% - \renewcommand*{\area@symbol}{A}% -} -\DeclareOption{EUFGHAN}{% this is my second favorite set of symbols - \renewcommand*{\Helmholtz@symbol}{F}% - \renewcommand*{\area@symbol}{A}% - \renewcommand*{\mole@symbol}{N}% -} -\DeclareOption{EEFGHAn}{% this treats all energy the same way(?) - \renewcommand*{\internalenergy@symbol}{E}% - \renewcommand*{\Helmholtz@symbol}{F}% - \renewcommand*{\area@symbol}{A}% -} -\DeclareOption{EEFGHAN}{% this treats all energy the same way(?) - \renewcommand*{\internalenergy@symbol}{E}% - \renewcommand*{\Helmholtz@symbol}{F}% - \renewcommand*{\area@symbol}{A}% - \renewcommand*{\mole@symbol}{N}% +\DeclareOption{EUFGHAn}{% + \tl_gset:Nn \g_@@_Helmholtz_symbol F + \tl_gset:Nn \g_@@_area_symbol A +} +\DeclareOption{EUFGHAN}{% + \tl_gset:Nn \g_@@_Helmholtz_symbol F + \tl_gset:Nn \g_@@_area_symbol A + \tl_gset:Nn \g_@@_mole_symbol N +} +\DeclareOption{EEFGHAn}{% + \tl_gset:Nn \g_@@_total_energy_symbol {\mathcal{E}} + \tl_gset:Nn \g_@@_internal_energy_symbol E + \tl_gset:Nn \g_@@_Helmholtz_symbol F + \tl_gset:Nn \g_@@_area_symbol A +} +\DeclareOption{EEFGHAN}{% + \tl_gset:Nn \g_@@_total_energy_symbol {\mathcal{E}} + \tl_gset:Nn \g_@@_internal_energy_symbol E + \tl_gset:Nn \g_@@_Helmholtz_symbol F + \tl_gset:Nn \g_@@_area_symbol A + \tl_gset:Nn \g_@@_mole_symbol N } \DeclareOption{EEFGHan}{% - \renewcommand*{\internalenergy@symbol}{E}% - \renewcommand*{\Helmholtz@symbol}{F} + \tl_gset:Nn \g_@@_total_energy_symbol {\mathcal{E}} + \tl_gset:Nn \g_@@_internal_energy_symbol E + \tl_gset:Nn \g_@@_Helmholtz_symbol F } \DeclareOption{EEFGHaN}{% - \renewcommand*{\internalenergy@symbol}{E}% - \renewcommand*{\Helmholtz@symbol}{F} - \renewcommand*{\mole@symbol}{N}% + \tl_gset:Nn \g_@@_total_energy_symbol {\mathcal{E}} + \tl_gset:Nn \g_@@_internal_energy_symbol E + \tl_gset:Nn \g_@@_Helmholtz_symbol F + \tl_gset:Nn \g_@@_mole_symbol N } \DeclareOption{EEAGHan}{% - \renewcommand*{\internalenergy@symbol}{E}% + \tl_gset:Nn \g_@@_total_energy_symbol {\mathcal{E}} + \tl_gset:Nn \g_@@_internal_energy_symbol E } \DeclareOption{EEAGHaN}{% - \renewcommand*{\internalenergy@symbol}{E}% - \renewcommand*{\mole@symbol}{N}% + \tl_gset:Nn \g_@@_total_energy_symbol {\mathcal{E}} + \tl_gset:Nn \g_@@_internal_energy_symbol E + \tl_gset:Nn \g_@@_mole_symbol N } -\DeclareOption{EUAGHAn}{% Helmholtz free energy and area look the same here - \renewcommand*{\area@symbol}{A}% +\DeclareOption{EUAGHAn}{% + \tl_gset:Nn \g_@@_area_symbol {\mathcal{A}} } -\DeclareOption{EUAGHAN}{% Helmholtz free energy and area look the same here - \renewcommand*{\area@symbol}{A}% - \renewcommand*{\mole@symbol}{N}% +\DeclareOption{EUAGHAN}{% + \tl_gset:Nn \g_@@_area_symbol {\mathcal{A}} + \tl_gset:Nn \g_@@_mole_symbol N } \DeclareOption{EUFGHan}{% - \renewcommand*{\Helmholtz@symbol}{F}% + \tl_gset:Nn \g_@@_Helmholtz_symbol F } \DeclareOption{EUFGHaN}{% - \renewcommand*{\Helmholtz@symbol}{F}% - \renewcommand*{\mole@symbol}{N}% + \tl_gset:Nn \g_@@_Helmholtz_symbol F + \tl_gset:Nn \g_@@_mole_symbol N } % \end{macrocode} -% The \verb"delta" option redefines \cs{dbar} to produce the symbol $\delta$. +% The |delta| option redefines \cs{dbar} to produce the symbol $\delta$. % The default is to use a $d$ with a slash through it ($\dbar$) for inexact % differentials unless the user overrides it with this option. The macro could % also be redefined manually, of course. % \begin{macrocode} -\DeclareOption{delta}{\let\dbar\delta} +\DeclareOption{delta}{ \cs_set_eq:NN \dbar \delta } % \end{macrocode} % -% \begin{macro}{\@extensive} -% \begin{macro}{\@intensive} -% \begin{macro}{\@specific} % Next, we define options for the set of notation. The default is -% \verb"intensive-plain", which produces things like $V$ for molar volume, +% |intensive-plain|, which produces things like $V$ for molar volume, % $\Vt$ for total volume, and $\hat V$ for specific volume. -% These are defined via the internal macros \verb"\@extensive", -% \verb"\@intensive", and \verb"\@specific". -% \begin{macrocode} -\let\@extensive\relax -\let\@intensive\relax -\let\@specific\hat -% \end{macrocode} -% \end{macro} -% \end{macro} -% \end{macro} +% The symbols themselves are produced via internal (non-user-facing) macros. % \begin{macrocode} -\DeclareOption{extensive-plain}{% - \let\@extensive\relax - \let\@intensive\thermo@underline +\cs_new:Nn \@@_extensive:n {#1} +\cs_new:Nn \@@_intensive:n {#1} +\cs_new:Nn \@@_specific:n {\hat{#1}} + +\cs_new:Npn \@@_set_intensive_plain +{ + \cs_set:Nn \@@_extensive:n {\@@_underline:n{##1}} + \cs_set:Nn \@@_intensive:n {##1} +} +\cs_new:Npn \@@_set_extensive_plain +{ + \cs_set:Nn \@@_extensive:n {##1} + \cs_set:Nn \@@_intensive:n {\@@_underline:n{##1}} } -\DeclareOption{intensive-plain}{% the default - \let\@extensive\thermo@underline - \let\@intensive\relax +\cs_new:Npn \@@_set_lowercase_pms +{ + \RenewDocumentCommand{\partialmolar}{m} + { + \tl_set:Nn \l_@@_pm_symbol_tl {\text_lowercase:n {##1}} + \@@_generic_pm: + } +} +\cs_new:Npn \@@_set_intensive_lowercase +{ + \cs_set:Nn \@@_extensive:n {\text_uppercase:n {##1}} + \cs_set:Nn \@@_intensive:n {\text_lowercase:n {##1}} + \cs_set:Nn \@@_specific:n {\hat{\text_lowercase:n {##1}}} } +\cs_new:Npn \@@_set_extensive_superscripts +{ + \cs_set:Nn \@@_extensive:n {{##1}\c_math_superscript_token t} + \cs_set:Nn \@@_intensive:n {##1} +} +\DeclareOption{extensive-plain}{\@@_set_extensive_plain} +\DeclareOption{intensive-plain}{\@@_set_intensive_plain} % the default \DeclareOption{intensive-lowercase}{% PLEASE don't use this! - \let\@extensive\MakeUppercase - \let\@intensive\MakeLowercase - \def\@specific#1{\MakeLowercase{\hat #1}} - \AtEndOfPackage{ - \renewcommand*{\partialmolar}[1]{% - \gdef\pm@symbol{\MakeLowercase #1}\generic@pm} - \renewcommand*{\heatcapacitysymbol}{c} - } + \@@_set_intensive_lowercase + \AtEndOfPackage{ + \@@_set_lowercase_pms + \RenewDocumentCommand{\heatcapacitysymbol}{}{c} + } } \DeclareOption{extensive-superscript}{% - \gdef\@extensive#1{{#1}^t}% - \let\@intensive\relax% - \AtEndOfPackage{% - \renewcommand*{\URt}{\internalenergy@symbol^{\residual,t}} - \renewcommand*{\HRt}{\enthalpy@symbol^{\residual,t}} - \renewcommand*{\FRt}{\Helmholtz@symbol^{\residual,t}} - \renewcommand*{\GRt}{\Gibbs@symbol^{\residual,t}} - \renewcommand*{\VRt}{\volume@symbol^{\residual,t}} - \renewcommand*{\SRt}{\entropy@symbol^{\residual,t}} - \renewcommand*{\UEt}{\internalenergy@symbol^{\excess,t}} - \renewcommand*{\HEt}{\enthalpy@symbol^{\excess,t}} - \renewcommand*{\FEt}{\Helmholtz@symbol^{\excess,t}} - \renewcommand*{\GEt}{\Gibbs@symbol^{\excess,t}} - \renewcommand*{\VEt}{\volume@symbol^{\excess,t}} - \renewcommand*{\SEt}{\entropy@symbol^{\excess,t}} - } + \@@_set_extensive_superscripts + \AtEndOfPackage{% + \RenewDocumentCommand{\URt}{}{\g_@@_internal_energy_symbol + \c_math_superscript_token{\residual,t}} + \RenewDocumentCommand{\HRt}{}{\g_@@_enthalpy_symbol + \c_math_superscript_token{\residual,t}} + \RenewDocumentCommand{\FRt}{}{\g_@@_Helmoholtz_symbol + \c_math_superscript_token{\residual,t}} + \RenewDocumentCommand{\GRt}{}{\g_@@_Gibbs_symbol + \c_math_superscript_token{\residual,t}} + \RenewDocumentCommand{\VRt}{}{\g_@@_volume_symbol + \c_math_superscript_token{\residual,t}} + \RenewDocumentCommand{\SRt}{}{\g_@@_entropy_symbol + \c_math_superscript_token{\residual,t}} + \RenewDocumentCommand{\UEt}{}{\g_@@_internal_energy_symbol + \c_math_superscript_token{\excess,t}} + \RenewDocumentCommand{\HEt}{}{\g_@@_enthalpy_symbol + \c_math_superscript_token{\excess,t}} + \RenewDocumentCommand{\FEt}{}{\g_@@_Helmoholtz_symbol + \c_math_superscript_token{\excess,t}} + \RenewDocumentCommand{\GEt}{}{\g_@@_Gibbs_symbol + \c_math_superscript_token{\excess,t}} + \RenewDocumentCommand{\VEt}{}{\g_@@_volume_symbol + \c_math_superscript_token{\excess,t}} + \RenewDocumentCommand{\SEt}{}{\g_@@_entropy_symbol + \c_math_superscript_token{\excess,t}} + } } % \end{macrocode} % % The next two options choose whether variables held constant are subscripted -% (the default) or placed next to the function. The \verb"nosubscripts" -% option currently requires that the variable being changed is the first one -% in the argument list. The difference is -% \[ \left(\frac{\partial U}{\partial S}\right)_V \quad\text{versus}\quad -% \left(\frac{\partial U(S,V)}{\partial S}\right) \] +% (the default) or placed next to the function. The difference is +%%^^A \[ \left(\frac{\partial U}{\partial S}\right)_V \quad\text{versus}\quad +%%^^A \left(\frac{\partial U(S,V)}{\partial S}\right) \] +% \[ \Partial{\Um}{\Sm}{\Vm} \quad\text{versus}\quad +% \begin{thermoNOsubscripts} +% \Partial{\Um}{\Sm}{\Vm} +% \end{thermoNOsubscripts} \] % for \verb"subscripts" and \verb"nosubscripts", respectively. % \begin{macrocode} -\newif\if@subscripted -\@subscriptedtrue -\DeclareOption{subscripts}{\@subscriptedtrue} -\DeclareOption{nosubscripts}{\@subscriptedfalse} +\bool_new:N \l_@@_subscripted_bool +\bool_set_true:N \l_@@_subscripted_bool +\DeclareOption{subscripts}{\bool_set_true:N \l_@@_subscripted_bool} +\DeclareOption{nosubscripts}{\bool_set_false:N \l_@@_subscripted_bool} % \end{macrocode} % These options change how \cs{Partial} and friends render derivatives. % The default is parentheses, but other options include brackets, braces, @@ -1762,42 +2024,38 @@ % \begin{macrocode} \DeclareOption{parentheses}{} \DeclareOption{brackets}{% - \renewcommand*{\PartialOpen}{[}% - \renewcommand*{\PartialClose}{]}% - \renewcommand*{\PartialEmptyClose}{]}% + \tl_set:Nn \l_@@_PartialOpen_tl {[} + \tl_set:Nn \l_@@_PartialClose_tl {]} + \tl_set:Nn \l_@@_PartialEmptyClose_tl {]} } \DeclareOption{braces}{% - \renewcommand*{\PartialOpen}{\{}% - \renewcommand*{\PartialClose}{\}}% - \renewcommand*{\PartialEmptyClose}{\}}% + \tl_set:Nn \l_@@_PartialOpen_t1 {\{} + \tl_set:Nn \l_@@_PartialClose_t1 {\}} + \tl_set:Nn \l_@@_PartialEmptyClose_tl {\}} } \DeclareOption{bar}{% - \renewcommand*{\PartialOpen}{.}% - \renewcommand*{\PartialClose}{\rvert}% - \renewcommand*{\PartialEmptyClose}{.}% + \tl_set:Nn \l_@@_PartialOpen_tl {.} + \tl_set:Nn \l_@@_PartialClose_tl {\rvert} + \tl_set:Nn \l_@@_PartialEmptyClose_tl {.} } \DeclareOption{plain-derivatives}{% This implies dU(S,V,N)/dS notation - \renewcommand*{\PartialOpen}{.}% - \renewcommand*{\PartialClose}{.}% - \renewcommand*{\PartialEmptyClose}{.}% - \ExecuteOptions{nosubscripts}% + \tl_set:Nn \l_@@_PartialOpen_tl {.} + \tl_set:Nn \l_@@_PartialClose_tl {.} + \tl_set:Nn \l_@@_PartialEmptyClose_tl {.} + \ExecuteOptions{nosubscripts} } % \end{macrocode} % \subsection{The Number of Moles Macros} % \begin{macro}{\ncomponents} % We define the number of components, default $C$, for use in the ``all moles'' -% and related macros. +% and related macros. The command is expandable so we can perform comparisons +% to user-entered values. % \begin{macrocode} -\newcommand*{\ncomponents}{C} +\NewExpandableDocumentCommand \ncomponents {} {C} % \end{macrocode} % \end{macro} % -% \begin{macro}{\allNs} -% \begin{macro}{\allNsbut} -% \begin{macro}{\allMs} -% \begin{macro}{\allmus} -% \begin{macro}{\allMsbut} -% \begin{macro}{\allmusbut} +% \begin{macro}{\allNs,\allXs,\allYs,\allmus,\allMs,\allWs} % Several macros define a shorthand for ``moles of all species'' (\cs{allNs}) % and ``moles of all species except'' (\cs{allNsbut}), as well as similar % quantities for masses (\cs{allMs}, \cs{allMsbut}) and chemical potentials @@ -1811,25 +2069,15 @@ % masses: \cs{allmus} and \cs{allmusbut} and \cs{allMs} and \cs{allMsbut}, % respectively. % \begin{macrocode} -\newcommand*{\allNs}{\allcomponents{\Nt}} -\newcommand*{\allXs}{\allcomponents{x}} -\newcommand*{\allYs}{\allcomponents{y}} -\newcommand*{\allmus}{\allcomponents{\mu}} -\newcommand*{\allMs}{\allcomponents{m}} -\newcommand*{\allWs}{\allcomponents{w}}% +\NewDocumentCommand{\allNs}{O{i}}{\allcomponents[#1]{\Nt}} +\NewDocumentCommand{\allXs}{O{i}}{\allcomponents[#1]{x}} +\NewDocumentCommand{\allYs}{O{i}}{\allcomponents[#1]{y}} +\NewDocumentCommand{\allmus}{O{i}}{\allcomponents[#1]{\mu}} +\NewDocumentCommand{\allMs}{O{i}}{\allcomponents[#1]{m}} +\NewDocumentCommand{\allWs}{O{i}}{\allcomponents[#1]{w}} % \end{macrocode} % \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% \begin{macro}{\allXs} -% \begin{macro}{\allYs} -% \begin{macro}{\allWs} -% \begin{macro}{\allWsbut} -% \begin{macro}{\allXsbut} -% \begin{macro}{\allYsbut} +% \begin{macro}{\allNsbut,\allXsbut,\allYsbut,\allMsbut,\allWsbut} % Similar commands are defined for mole fractions (\cs{allXs}, \cs{allYs}, % etc.), but these assume the last mole fraction is \emph{not} one of the % variables---that is, \cs{allXsbut} and \cs{allYsbut} assume the argument @@ -1842,98 +2090,89 @@ % \[ \Partial{G}{T}{P,\allXs} = -S \qquad % \Partial{G}{x_i}{T,P,x_{j\neq i,C}} \neq \Gpm{i}. \] % \begin{macrocode} -\newcommand*{\allNsbut}[2][j]{\allbut[#1]{#2}{\Nt}} -\newcommand*{\allXsbut}[2][j]{\allbutlastand[#1]{#2}{x}} -\newcommand*{\allYsbut}[2][j]{\allbutlastand[#1]{#2}{y}} -\newcommand*{\allmusbut}[2][j]{\allbut[#1]{#2}{\mu}} -\newcommand*{\allMsbut}[2][j]{\allbut[#1]{#2}{m}} -\newcommand*{\allWsbut}[2][j]{\allbutlastand[#1]{#2}{w}}% +\NewDocumentCommand{\allNsbut}{O{j} m} {\allbut[#1]{#2}{\Nt}} +\NewDocumentCommand{\allXsbut}{O{j} m} {\allbutlastand[#1]{#2}{x}} +\NewDocumentCommand{\allYsbut}{O{j} m} {\allbutlastand[#1]{#2}{y}} +\NewDocumentCommand{\allmusbut}{O{j} m} {\allbut[#1]{#2}{\mu}} +\NewDocumentCommand{\allMsbut}{O{j} m} {\allbut[#1]{#2}{m}} +\NewDocumentCommand{\allWsbut}{O{j} m} {\allbutlastand[#1]{#2}{w}} % \end{macrocode} % \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% \begin{macro}{\allbutlastand} -% \begin{macro}{\allbut} -% \begin{macro}{\allcomponents} +% \begin{macro}{\allbutlastand,\allbut,\allcomponents} +% \changes{v1.01}{10/04/2023}{Updated \cs{allcomponents} to include an +% optional argument that changes $N_i$ to $N_j$, say, when using +% TesterModell or other options that denote moles of all components that +% way. Similar updates to \cs{allNs} and friends.} % The \cs{allcomponents}, \cs{allbut}, and \cs{allbutlastand} macros can be % used to define new entities; say, if you want to use $z_i$ as a mole % fraction, then use % \begin{verbatim} -% \newcommand*{\allZsbut}[2][j]{\allbutlastand[#1]{#2}{z}} +% \NewDocumentCommand{\allZsbut}{O{j} m}{\allbutlastand[#1]{#2}{z}} %\end{verbatim} % Similarly, something meaning the concentrations of every species could be % defined via % \begin{verbatim} -% \newcommand*{\allCs}{\allcomponents{C}} +% \NewDocumentCommand{\allCs}{O{}}{\allcomponents{C}} %\end{verbatim} % \begin{macrocode} -\newcommand*{\allcomponents}[1]{\vec{#1}} -\newcommand*{\allbut}[3][j]{% - \def\tmp@arg{#2}% - \def\tmp@@arg{#1}% - \ifx\tmp@arg\tmp@@arg - {#3}_{k\neq #2}% - \else - {#3}_{#1\neq #2}% - \fi -} -\newcommand*{\allbutlastand}[3][j]{% - \edef\tmp@arg{#1}% - \edef\tmp@@arg{#2}% - \ifx\tmp@@arg\ncomponents - {#3}_{#1 \neq #2}% - \else - \ifx\tmp@arg\tmp@@arg - {#3}_{k \neq #2,\ncomponents}% - \else - {#3}_{#1 \neq #2,\ncomponents}% - \fi - \fi +\NewDocumentCommand{\allcomponents}{O{} m}{\vec{#2}} +\NewDocumentCommand{\allbut}{O{j} m m} +{ \tl_if_eq:nnTF {#1} {#2} + { {#3}\c_math_subscript_token{k \neq #2} } + { {#3}\c_math_subscript_token{#1 \neq #2} } +} +\NewDocumentCommand{\allbutlastand}{O{j} m m} +{ \tl_if_eq:xxTF {#2} {\ncomponents} + { {#3}\c_math_subscript_token{#1 \neq #2} } + { \tl_if_eq:nnTF {#1} {#2} + { {#3}\c_math_subscript_token{k \neq #2,\ncomponents} } + { {#3}\c_math_subscript_token{#1 \neq #2,\ncomponents} } + } } % \end{macrocode} % \end{macro} -% \end{macro} -% \end{macro} % % We then define two package options that change how to render \cs{allNs} and -% friends. +% friends.\relax +% \changes{v1.01}{2022/05/04}{Fixed bug in \cs{allbutlastand} when using the +% |moles-range| option ($C$ should have been $C-1$ in the last option).} % \begin{macrocode} \DeclareOption{moles-index}{} -\DeclareOption{moles-range}{% - \renewcommand*{\allcomponents}[1]{{#1}_1,\dots,{#1}_{\ncomponents}} - \renewcommand*{\allbut}[3][j]{% - \def\@one{1}% - \edef\tmp@arg{#2}% - \ifx\tmp@arg\@one - {#3}_2,\dots,{#3}_{\ncomponents}% - \else - \ifx\tmp@arg\ncomponents - {#3}_1,\dots,{#3}_{\ncomponents-1}% - \else - {#3}_1,\dots,[{#3}_{#2}],\dots,{#3}_{\ncomponents}% - \fi - \fi +\DeclareOption{moles-range}{ \@@_set_moles_range } +\cs_new:Npn \@@_set_moles_range {% + \RenewDocumentCommand{\allcomponents}{O{} m} + { {##2}\c_math_subscript_token 1,\dots, + {##2}\c_math_subscript_token{\ncomponents} } + \RenewDocumentCommand{\allbut}{O{j} m m} + { \tl_if_eq:nnTF {##2} {1} + { {##3}\c_math_subscript_token 2,\dots, + {##3}\c_math_subscript_token{\ncomponents} } + { \tl_if_eq:xxTF {##2} {\ncomponents} + { {##3}\c_math_subscript_token 1,\dots, + {##3}\c_math_subscript_token{\ncomponents-1} } + { {##3}\c_math_subscript_token 1,\dots, + [{##3}\c_math_subscript_token{##2}], + \dots,{##3}\c_math_subscript_token{\ncomponents} } + } } - \renewcommand*{\allbutlastand}[3][j]{% - \def\@one{1}% - \edef\tmp@arg{#2}% - \edef\@ncminusone{\ncomponents-1}% - \ifx\tmp@arg\@one - {#3}_2,\dots,{#3}_{\ncomponents-1}% - \else - \ifx\tmp@arg\@ncminusone - {#3}_1,\dots,{#3}_{\ncomponents-2}% - \else - \ifx\tmp@arg\ncomponents - {#3}_1,\dots,{#3}_{\ncomponents-1}% - \else - {#3}_1,\dots,[{#3}_{#2}],\dots,{#3}_{\ncomponents}% - \fi - \fi - \fi + \RenewDocumentCommand{\allbutlastand}{O{j} m m} + { \tl_if_eq:nnTF {##2} {1} + { {##3}\c_math_subscript_token 2,\dots, + {##3}\c_math_subscript_token{\ncomponents-1} } + { \tl_if_eq:xxTF {##2} {\ncomponents} + { {##3}\c_math_subscript_token 1,\dots, + {##3}\c_math_subscript_token{\ncomponents-1} + } + { \tl_if_eq:xxTF {##2} {\ncomponents-1} + { {##3}\c_math_subscript_token 1,\dots, + {##3}\c_math_subscript_token{\ncomponents-2} } + { + {##3}\c_math_subscript_token 1,\dots, + [{##3}\c_math_subscript_token{##2}],\dots, + {##3}\c_math_subscript_token{\ncomponents-1} + } + } + } } } % \end{macrocode} @@ -1941,223 +2180,288 @@ % \begin{macrocode} \DeclareOption{Bejan}{ \ExecuteOptions{EUFGHAN,intensive-lowercase,delta} - \let\@specific\MakeLowercase - \def\@intensive#1{\MakeLowercase{\bar #1}} - \AtEndOfPackage{ - \DeclareSubscrSymbol{cV}{\bar\heatcapacitysymbol}{v} - \DeclareSubscrSymbol{cVs}{\heatcapacitysymbol}{v} - \DeclareSubscrSymbol{cVt}{\Nt\heatcapacitysymbol}{v} - \renewcommand*{\expansivitysymbol}{\beta} - \renewcommand*{\ncomponents}{n} - } + \cs_set:Nn \@@_specific:n {\text_lowercase:n {#1}} + \cs_set:Nn \@@_intensive:n {\bar{\text_lowercase:n {#1}}} + \tl_gset:Nn \g_@@_volume_symbol v } \DeclareOption{CBK}{ \ExecuteOptions{EUAGHAN,intensive-lowercase} \AtEndOfPackage{ - \let\thermo@overline\widetilde - \let\@specific\MakeLowercase - \renewcommand*{\@intensive}[1]{\MakeLowercase{\bar{#1}}} - \renewcommand*{\pressure@symbol}{p} - \renewcommand*{\Deltarxn}[1]{#1_R} - \renewcommand*{\compressibilitysymbol}{\beta} - \renewcommand*{\expansivitysymbol}{\alpha} + \cs_set:Nn \@@_overline:n {\widetilde{#1}} + \cs_set:Nn \@@_specific:n {\text_lowercase:n {#1}} + \cs_set:Nn \@@_intensive:n {\bar{\text_lowercase:n{#1}}} + \tl_gset:Nn \g_@@_pressure_symbol p + \RenewDocumentCommand{\Deltarxn}{m}{{#1}\c_math_subscript_token R} + \RenewDocumentCommand{\compressibilitysymbol}{}{\beta} + \RenewDocumentCommand{\expansivitysymbol}{}{\alpha} } } \DeclareOption{ElliottLira}{ \AtEndOfPackage{ - \renewcommand*{\allcomponents}[1]{#1} - \renewcommand*{\Deltarxn}[1]{\Delta #1} + \RenewDocumentCommand{\allcomponents}{O{} m}{#2} + \RenewDocumentCommand{\Deltarxn}{m}{\Delta #1} + \RenewDocumentCommand{\IG}{}{{\text{ig}}} + \RenewDocumentCommand{\IGM}{}{{\text{ig}}} + \RenewDocumentCommand{\IS}{}{{\text{is}}} } } \DeclareOption{Koretsky}{ \ExecuteOptions{EUAGHAn,brackets,intensive-lowercase,delta} \AtEndOfPackage{ - \renewcommand*{\partialmolar}[1]{\gdef\pm@symbol{#1}\generic@pm} - \renewcommand*{\expansivitysymbol}{\beta} - \renewcommand*{\IS}{{\text{ideal}}} - \renewcommand*{\residual}{{\text{dep}}} - \renewcommand*{\IG}{{\text{ideal}}} - \renewcommand*{\IGM}{{\text{ideal}}} - \renewcommand*{\Deltafus}[1]{\Delta{#1}_\fusion} - \renewcommand*{\Deltasub}[1]{\Delta{#1}_\sublimation} - \renewcommand*{\Deltavap}[1]{\Delta{#1}_\vaporization} - \renewcommand*{\Henryrat}{{\mathcal{H}}} - \renewcommand*{\gammarat}{\gamma^\text{Henry's}} - \let\phipure\varphi - \renewcommand*{\phimix}{\hat\varphi} - \renewcommand*{\phisat}{\varphi^\sat} - \let\Delta@fus@sym\relax - \DeclareSubscrSymbol{@Deltafus}{\Delta@fus@sym}{\fusion} - \renewcommand*{\Deltafus}[1]{\def\Delta@fus@sym{\Delta #1}\@Deltafus} - \let\Delta@vap@sym\relax - \DeclareSubscrSymbol{@Deltavap}{\Delta@vap@sym}{\vaporization} - \renewcommand*{\Deltasub}[1]{\def\Delta@sub@sym{\Delta #1}\@Deltasub} - \let\Delta@sub@sym\relax - \DeclareSubscrSymbol{@Deltasub}{\Delta@sub@sym}{\sublimation} - \renewcommand*{\Deltasub}[1]{\def\Delta@sub@sym{\Delta #1}\@Deltasub} + %^^A Undo part of intensive-lowercase + \RenewDocumentCommand{\partialmolar}{m} + { \tl_set:Nn \l_@@_pm_symbol_tl {#1} + \@@_generic_pm: + } + \RenewDocumentCommand{\expansivitysymbol}{}{\beta} + \RenewDocumentCommand{\IS}{}{{\text{ideal}}} + \RenewDocumentCommand{\residual}{}{{\text{dep}}} + \RenewDocumentCommand{\IG}{}{{\text{ideal}}} + \RenewDocumentCommand{\IGM}{}{{\text{ideal}}} + \RenewDocumentCommand{\Henryrat}{}{{\mathcal{H}}} + \RenewDocumentCommand{\gammarat}{} + {\gamma\c_math_superscript_token\text{Henry's}} + \RenewDocumentCommand{\phipure}{}{\varphi} + \RenewDocumentCommand{\phimix}{}{\hat\varphi} + \RenewDocumentCommand{\phisat}{}{\varphi\c_math_superscript_token\sat} + \cs_new:Npn \Delta_fus_sym {} {} + \NewSubscriptedSymbol{\Delta_fus}{\Delta_fus_sym}{\fusion} + \RenewDocumentCommand{\Deltafus}{m}{ + \cs_set:Npn \Delta_fus_sym {} { \Delta #1 } + \Delta_fus + } + \cs_new:Npn \Delta_vap_sym {} {} + \NewSubscriptedSymbol{\Delta_vap}{\Delta_vap_sym}{\vaporization} + \RenewDocumentCommand{\Deltavap}{m}{ + \cs_set:Npn \Delta_vap_sym {} { \Delta #1 } + \Delta_vap + } + \cs_new:Npn \Delta_sub_sym {} {} + \NewSubscriptedSymbol{\Delta_sub}{\Delta_sub_sym}{\sublimation} + %^^A Undo part of intensive-lowercase + \RenewDocumentCommand{\Deltasub}{m}{ + \cs_set:Npn \Delta_sub_sym {} { \Delta #1 } + \Delta_sub + } } } \DeclareOption{MSBB}{ \ExecuteOptions{EUFGHAn,intensive-lowercase,delta} \AtEndOfPackage{ - \renewcommand*{\IGM}{\ast} - \renewcommand*{\IG}{\ast} - \renewcommand*{\expansivitysymbol}{\beta} - \renewcommand*{\allcomponents}[1]{#1} - \renewcommand*{\allbut}[3][j]{% - \def\tmp@arg{#2}% - \def\tmp@@arg{#1}% - \ifx\tmp@arg\tmp@@arg - {#3}_{k}% - \else - {#3}_{#1}% - \fi + \RenewDocumentCommand{\IGM}{}{\ast} + \RenewDocumentCommand{\IG}{}{\ast} + \RenewDocumentCommand{\expansivitysymbol}{}{\beta} + \RenewDocumentCommand{\allcomponents}{O{} m}{#2} + \RenewDocumentCommand{\allbut}{O{j} m m} + { + \tl_if_eq:nnTF {#1} {#2} + { {#3}\c_math_subscript_token k } + { {#3}\c_math_subscript_token{#1} } + } + \tl_gset_eq:NN \g_@@_Helmholtz_symbol \psi + \RenewDocumentCommand{\Ft}{}{\Psi} + \cs_set:Nn \@@_intensive:n {\@@_overline:n{\text_lowercase:n{#1}}} + \cs_set:Nn \@@_specific:n {\text_lowercase:n{#1}} + \RenewDocumentCommand{\fmix}{}{\bar f} + \RenewDocumentCommand{\phimix}{}{\bar\phi} + \RenewDocumentCommand{\phimix}{}{\bar\phi} + \tl_gset:Nn \g_@@_pressure_symbol p + \RenewDocumentCommand{\partialmolar}{m} + { + \tl_set:Nn \l_@@_pm_symbol_tl {#1} + \@@_generic_pm: } - \let\Helmholtz@symbol\psi - \renewcommand*{\Ft}{\Psi} - \def\@intensive#1{\MakeLowercase{\thermo@overline #1}} - \let\@specific\MakeLowercase - \renewcommand*{\partialmolar}[1]{\gdef\pm@symbol{#1}\generic@pm} - \renewcommand*{\fmix}{\bar f} - \renewcommand*{\phimix}{\bar\phi} - \renewcommand*{\pressure@symbol}{p} } } \DeclareOption{Prausnitz}{ \ExecuteOptions{intensive-lowercase} \AtEndOfPackage{ - \renewcommand*{\fmix}{f} - \let\phimix\phi - \renewcommand*{\fsat}{\fpure^\sat} - \DeclareSubscrSymbol{fpure}{f}{{\text{pure}}} - \DeclareSubscrSymbol{phipure}{\phi}{{\text{pure}}} - \renewcommand*{\residual}{{{\mathcal{R}}}} - \renewcommand*{\allcomponents}[1]{{#1}_i} - \renewcommand*{\allbut}[3][j]{% - \def\tmp@arg{#2}% - \def\tmp@@arg{#1}% - \ifx\tmp@arg\tmp@@arg - {#3}_{k}% - \else - {#3}_{#1}% - \fi + \RenewDocumentCommand{\fmix}{}{f} + \RenewDocumentCommand{\phimix}{}{\phi} + \RenewDocumentCommand{\fsat}{}{\fpure\c_math_superscript_token\sat} + % TODO: this should pick up H_2 and make it into H_{2,1} (assuming the + % solvent is always 1...?) + \RenewDocumentCommand{\Henryrat}{}{H} + \RenewDocumentCommand{\residual}{}{{{\mathcal{R}}}} + \RenewDocumentCommand{\allcomponents}{O{i} m} + { {#2}\c_math_subscript_token{#1} } + \RenewDocumentCommand{\allbut}{O{i} m m} + { \tl_if_eq:nnTF {#1} {#2} + { {#3}\c_math_subscript_token k } + { {#3}\c_math_subscript_token{#1} } } + \RenewSubscriptedSymbol{\fpure}{f}{{\text{pure}}} + \RenewSubscriptedSymbol{\phipure}{\phi}{{\text{pure}}} } } \DeclareOption{Sandler}{ \ExecuteOptions{EUAGHaN,extensive-plain} \AtEndOfPackage{ - \renewcommand*{\sat}{{\text{vap}}} - \renewcommand*{\excess}{{\text{{ex}}}} - \renewcommand*{\residual}{{\text{r}}} - \renewcommand*{\ncomponents}{\mathcal{C}} - \renewcommand*{\fmix}{\bar f} - \renewcommand*{\fstd}{\bar f^\circ} - \renewcommand*{\phimix}{\bar\phi} - \renewcommand*{\allcomponents}[1]{\thermo@underline{#1}} - \renewcommand*{\IG}{{\text{IG}}} - \renewcommand*{\IGM}{{\text{IGM}}} - \renewcommand*{\IS}{{\text{IM}}} - \renewcommand*{\Deltamix}[1]{\Delta_\mixing #1} - \renewcommand*{\Deltarxn}[1]{\Delta_\reaction #1} - \renewcommand*{\Deltasub}[1]{\Delta_\sublimation #1} - \renewcommand*{\Deltafus}[1]{\Delta_\fusion #1} - \renewcommand*{\Deltavap}[1]{\Delta_\vaporization #1} - \renewcommand*{\Henryrat}{H} - \DeclareSubscrSymbol{cV}{\heatcapacitysymbol}{\volume@symbol} - \DeclareSubscrSymbol{cP}{\heatcapacitysymbol}{\pressure@symbol} - \DeclareSubscrSymbol{cVt}{\Nt\heatcapacitysymbol}{\volume@symbol} - \DeclareSubscrSymbol{cPt}{\Nt\heatcapacitysymbol}{\pressure@symbol} + \RenewDocumentCommand{\sat}{}{{\text{vap}}} + \RenewDocumentCommand{\excess}{}{{\text{ex}}} + \RenewDocumentCommand{\residual}{}{{\text{r}}} + \RenewExpandableDocumentCommand{\ncomponents}{}{\mathcal{C}} + \RenewDocumentCommand{\fmix}{}{\bar f} + \RenewDocumentCommand{\fstd}{}{\bar f\c_math_superscript_token\std} + \RenewDocumentCommand{\phimix}{}{\bar\phi} + \RenewDocumentCommand{\allcomponents}{O{} m}{\@@_underline:n{#2}} + \RenewDocumentCommand{\IG}{}{{\text{IG}}} + \RenewDocumentCommand{\IGM}{}{{\text{IGM}}} + \RenewDocumentCommand{\IS}{}{{\text{IM}}} + \RenewDocumentCommand{\Deltamix}{m} + {\Delta\c_math_subscript_token\mixing #1} + \RenewDocumentCommand{\Deltarxn}{m} + {\Delta\c_math_subscript_token\reaction #1} + \RenewDocumentCommand{\Deltasub}{m} + {\Delta\c_math_subscript_token\sublimation #1} + \RenewDocumentCommand{\Deltafus}{m} + {\Delta\c_math_subscript_token\fusion #1} + \RenewDocumentCommand{\Deltavap}{m} + {\Delta\c_math_subscript_token\vaporization #1} + \RenewDocumentCommand{\Henryrat}{}{H} + \RenewSubscriptedSymbol{\cV} + {\heatcapacitysymbol}{\g_@@_volume_symbol} + \RenewSubscriptedSymbol{\cP} + {\heatcapacitysymbol}{\g_@@_pressure_symbol} + \RenewSubscriptedSymbol{\cVt} + {\Nt\heatcapacitysymbol}{\g_@@_volume_symbol} + \RenewSubscriptedSymbol{\cPt} + {\Nt\heatcapacitysymbol}{\g_@@_pressure_symbol} } } \DeclareOption{SVNAS}{ \ExecuteOptions{extensive-superscript} \AtEndOfPackage{ - \renewcommand*{\allcomponents}[1]{#1} - \renewcommand*{\allbut}[3][j]{% - \def\tmp@arg{#2}% - \def\tmp@@arg{#1}% - \ifx\tmp@arg\tmp@@arg - {#3}_{k}% - \else - {#3}_{#1}% - \fi + \RenewDocumentCommand{\allcomponents}{O{} m}{#2} + \RenewDocumentCommand{\allbut}{O{j} m m} + { + \tl_if_eq:nnTF {#1} {#2} + { {#3}\c_math_subscript_token k } + { {#3}\c_math_subscript_token{#1} } } - \renewcommand*{\IG}{{ig}} - \renewcommand*{\IGM}{{ig}} - \renewcommand*{\IS}{{id}} - \renewcommand*{\expansivitysymbol}{\beta} - \renewcommand*{\Deltarxn}[1]{\Delta #1} - \DeclareSubscrSymbol{cVt}{\Nt\heatcapacitysymbol}{\volume@symbol} - \DeclareSubscrSymbol{cPt}{\Nt\heatcapacitysymbol}{\pressure@symbol} + \RenewDocumentCommand{\IG}{}{{ig}} + \RenewDocumentCommand{\IGM}{}{{ig}} + \RenewDocumentCommand{\IS}{}{{id}} + \RenewDocumentCommand{\expansivitysymbol}{}{\beta} + \RenewDocumentCommand{\Deltarxn}{m}{\Delta #1} + \RenewSubscriptedSymbol{\cVt} + {\Nt\heatcapacitysymbol}{\g_@@_volume_symbol} + \RenewSubscriptedSymbol{\cPt} + {\Nt\heatcapacitysymbol}{\g_@@_pressure_symbol} } } \DeclareOption{TesterModell}{ \ExecuteOptions{EUAGHaN,delta} \AtEndOfPackage{ - \renewcommand*{\ncomponents}{n} - \renewcommand*{\allcomponents}[1]{{#1}_i} - \renewcommand*{\allbut}[3][j]{% - \def\tmp@arg{#2}% - \def\tmp@@arg{#1}% - \ifx\tmp@arg\tmp@@arg - {#3}_k\relax[#2] - \else - {#3}_{#1}\relax[#2] - \fi + \RenewExpandableDocumentCommand{\ncomponents}{}{n} + \RenewDocumentCommand{\allcomponents}{O{i} m} + { + {#2}\c_math_subscript_token{#1} + } + \RenewDocumentCommand{\allbut}{O{i} m m} + { \tl_if_eq:nnTF {#1} {#2} + { {#3}\c_math_subscript_token{k}[#2] } + { {#3}\c_math_subscript_token{#1}[#2] } } - \renewcommand*{\allbutlastand}[3][j]{% - \edef\tmp@arg{#1}% - \edef\tmp@@arg{#2}% - \ifx\tmp@@arg\ncomponents - {#3}_{#1}\relax[#2]% - \else - \ifx\tmp@arg\tmp@@arg - {#3}\relax[#2,\ncomponents]% - \else - {#3}\relax[#2,\ncomponents]% - \fi - \fi + \RenewDocumentCommand{\allbutlastand}{O{j} m m} + { \tl_if_eq:xxTF {#2} {\ncomponents} + { {#3}\c_math_subscript_token{#1}\relax[#2] } + { \tl_if_eq:nnTF {#1} {#2} + { {#3}\c_math_subscript_token{k}[#2,\ncomponents] } + { {#3}\c_math_subscript_token{#1}[#2,\ncomponents] } + } } - \renewcommand*{\IG}{{ig}} -% Tester & Modell never use "igm" anywhere, and I only found ig once - \renewcommand*{\IGM}{{igm}} - \renewcommand*{\IS}{{ID}} - \renewcommand*{\excess}{{EX}}% - \renewcommand*{\reaction}{{rx}} - \renewcommand*{\Henryrat}{f^{\ast\ast}} - \renewcommand*{\Henrymol}{f^\ast} - \renewcommand*{\gammarat}{\gamma^{\ast\ast}} - \renewcommand*{\gammamol}{\gamma^\ast} + \RenewDocumentCommand{\IG}{}{{o}} + \RenewDocumentCommand{\IGM}{}{{o}} + \RenewDocumentCommand{\IS}{}{{ID}} + \RenewDocumentCommand{\excess}{}{{EX}} + \RenewDocumentCommand{\reaction}{}{{rx}} + \RenewDocumentCommand{\Henryrat}{} + {f\c_math_superscript_token{\ast\ast}} + \RenewDocumentCommand{\Henrymol}{}{f\c_math_superscript_token\ast} + \RenewDocumentCommand{\gammarat}{} + {\gamma\c_math_superscript_token{\ast\ast}} + \RenewDocumentCommand{\gammamol}{} + {\gamma\c_math_superscript_token\ast} + \RenewExpandableDocumentCommand{\JTsymbol}{}{\alpha} + \RenewSubscriptedSymbol{\muJT}{\JTsymbol}{H} } } \DeclareOption{Thompson}{ \ExecuteOptions{EUAGHAn,delta} - \AtEndOfPackage{ - \renewcommand*{\excess}{{EX}} - \renewcommand*{\residual}{{R}} - \renewcommand*{\allcomponents}[1]{{#1}_j} - \renewcommand*{\ncomponents}{c} - \renewcommand*{\IS}{{IS}} - \renewcommand*{\IG}{{IG}} - \let\IGM\IG - \def\@fpure_#1{f_{#1}\@ifnextchar^{}{^\bullet}} - \renewcommand*{\fpure}{\@ifnextchar_{\@fpure}{f}} - \def\@phi@pure_#1{\phi_{#1}\@ifnextchar^{}{^\bullet}} - \renewcommand*{\phipure}{\@ifnextchar_{\@phi@pure}{\phi}} - \renewcommand*{\mixing}{{MIX}} - \renewcommand*{\Deltamix}[1]{\Delta_\mixing #1} - \renewcommand*{\Deltarxn}[1]{\Delta #1} - \def\@@intensive_#1{_{#1}\@ifnextchar^{}{^\bullet}} - \newcommand*{\@intensive}[1]{#1\@ifnextchar_{\@@intensive}{}} - \renewcommand*{\allbut}[3][j]{% - \def\tmp@arg{#2}% - \def\tmp@@arg{#1}% - \ifx\tmp@arg\tmp@@arg - {#3}_{k}\neq{#3}_{#2}% - \else - {#3}_{#1}\neq{#3}_{#2}% - \fi + \AtEndOfPackage + { + \RenewDocumentCommand{\excess}{}{{EX}} + \RenewDocumentCommand{\residual}{}{{R}} + %^^A He uses k_H for both types of Henry's constant, but I changed + %^^A the rational basis one just so there is SOME difference + \RenewSubscriptedSymbol{\Henryrat}{k}{h} + \RenewSubscriptedSymbol{\Henrymol}{k}{H} + \RenewDocumentCommand{\allcomponents}{O{j} m} + { + {#2}\c_math_subscript_token{#1} + } + \RenewDocumentCommand{\allNs}{O{j}}{\allcomponents[#1]{\Nt}} + \RenewDocumentCommand{\allXs}{O{j}}{\allcomponents[#1]{x}} + \RenewDocumentCommand{\allYs}{O{j}}{\allcomponents[#1]{y}} + \RenewDocumentCommand{\allmus}{O{j}}{\allcomponents[#1]{\mu}} + \RenewDocumentCommand{\allMs}{O{j}}{\allcomponents[#1]{m}} + \RenewDocumentCommand{\allWs}{O{j}}{\allcomponents[#1]{w}} + \RenewExpandableDocumentCommand{\ncomponents}{}{c} + \RenewDocumentCommand{\IS}{}{{IS}} + \RenewDocumentCommand{\IG}{}{{IG}} + \RenewDocumentCommand{\IGM}{}{{IG}} + \cs_new:Nn \@@_fpure_one:n + { + f\c_math_subscript_token{#1} + \peek_catcode_remove:NF \c_math_superscript_token + { \c_math_superscript_token\bullet } + } + \RenewDocumentCommand{\fpure}{} + { + \peek_catcode_remove:NTF \c_math_subscript_token + { \@@_fpure_one:n } + { f } + } + \cs_new:Nn \@@_intensive_two:n + { + \c_math_subscript_token{#1} + \peek_catcode:NF \c_math_superscript_token + { + \c_math_superscript_token\bullet + } + } + \cs_set:Nn \@@_intensive:n + { #1 + \peek_catcode_remove:NT \c_math_subscript_token + { \@@_intensive_two:n } + } + \cs_new:Nn \@@_phipure_one:n + { + \phi\c_math_subscript_token{#1} + \peek_catcode:NF \c_math_superscript_token + { \c_math_superscript_token\bullet } + } + \RenewDocumentCommand{\phipure}{} + { + \peek_catcode_remove:NTF \c_math_subscript_token + { + \@@_phipure_one:n + } + {\phi} + } + \RenewDocumentCommand{\mixing}{}{{MIX}} + \RenewDocumentCommand{\Deltamix}{m} + {\Delta\c_math_subscript_token\mixing #1} + \RenewDocumentCommand{\Deltarxn}{m}{\Delta #1} + \RenewDocumentCommand{\allbut}{O{j} m m} + { \tl_if_eq:nnTF {#1} {#2} + { + {#3}\c_math_subscript_token k\neq{#3}\c_math_subscript_token{#2} + } + { + {#3}\c_math_subscript_token{#1}\neq{#3}\c_math_subscript_token{#2} + } } } } @@ -2167,6 +2471,50 @@ \ExecuteOptions{EUAGHan,subscripts,parentheses,intensive-plain,moles-index} \ProcessOptions % \end{macrocode} +% We next encode a routine to sort non-subscripted variables into a consistent +% order. It currently does not sort variables with subscripts. +% \changes{v2.00}{2023/11/16}{Added a sorting routine to make function +% arguments be in a consistent order using the |nosubscripts| option.} +% \begin{macrocode} +\tl_const:Nn \c_@@_sort_order_tl + {\Et\Em\Es\Ut\Um\Us\Ht\Hm\Hs\Ft\Fm\Fs\Gt\Gm\Gs\Lt\Lm\Ls T\St\Sm\Ss + P\Vt\Vm\Vs\mu\Nt mwxyz\At\Am\As\sigma + ABCDEFGHIJKLMNOPQRSTUVWXYZabcdefghijklnopqrstuvwxyz} +\clist_new:N \l_@@_in_list_clist +\clist_new:N \l_@@_sorted_list_clist +\clist_new:N \l_@@_remaining_list_clist +\cs_new:Nn \@@_sort_clist:n +{% Sort the list in the order of \c_@@_sort_order_tl + + % Wipe out any remnants from the last sort + \clist_clear:N \l_@@_in_list_clist + \clist_clear:N \l_@@_sorted_list_clist + + % Make a copy of the list + \clist_set:Nn \l_@@_remaining_list_clist {#1} + + % Make a list of everything that's in the known sort order list + % and put everything else in the "not in sort order list" list. + \tl_map_inline:Nn \c_@@_sort_order_tl + { + \clist_if_in:NnT \l_@@_remaining_list_clist {##1} + { \clist_put_right:Nn \l_@@_in_list_clist {##1} } + + \clist_remove_all:Nn \l_@@_remaining_list_clist {##1} + } + + % Then merge the lists back together again. + \clist_if_empty:NF \l_@@_in_list_clist + { + \clist_put_right:Nn \l_@@_sorted_list_clist \l_@@_in_list_clist + } + \clist_if_empty:NF \l_@@_remaining_list_clist + { + \clist_put_right:Nn \l_@@_sorted_list_clist \l_@@_remaining_list_clist + } + \clist_use:Nn \l_@@_sorted_list_clist , +} +% \end{macrocode} % % \subsection{Commands for Partial Derivatives} % The \cs{Partial} command and its second-order siblings are defined as below. @@ -2177,423 +2525,710 @@ % The starred forms adjust the spacing after the partial derivative so the % trailing binary operator (assumed to be the same width as an equals sign) % overhangs the variables held constant. -% We thus set \verb"operator@width" to be \emph{just} greater than the width of +% We thus set \verb"operator_width" to be \emph{just} greater than the width of % an equals sign. -%^^A 3/1/2022: changed adjust@width to 2pt (up from 1pt) -%^^A 4/21/2022: changed adjust@width to 0.1\operator@width (from 2pt) % \begin{macrocode} -\newlength{\Partial@const@width} -\newlength{\operator@width} -\settowidth{\operator@width}{=} -\newlength{\adjust@width} -\setlength{\adjust@width}{0.1\operator@width} -\addtolength{\operator@width}{\adjust@width} +\dim_new:N \l_@@_Partial_const_dim +\dim_new:N \l_@@_operator_width_dim +\dim_new:N \l_@@_adjust_width_dim +\settowidth{\l_@@_operator_width_dim}{=} +\dim_set:Nn \l_@@_adjust_width_dim {0.1\l_@@_operator_width_dim} +\dim_add:Nn \l_@@_operator_width_dim \l_@@_adjust_width_dim % \end{macrocode} -% \begin{macro}{\Partial*} % \begin{macro}{\Partial} % The command \cs{Partial} and its friends drastically simplify the creation % of partial derivatives. The command \cs{Partial*} is the same as % \cs{Partial} except that it adjusts the spacing so the (presumably) binary % operator that follows it slightly overlaps the subscripts. +% \changes{v1.01}{2022/03/01}{Changed \cs{adjust@width} to 2pt (up from 1pt)} +% \changes{v1.01}{2022/04/21}{Changed \cs{adjust@width} 0.1\cs{operator@width} +% (from 2pt)} +% \changes{v2.00}{2023/11/16}{Changed length added to +% \cs{l_@@_Partial_const_dim} from $-0.15$ to $-0.20$} % \begin{macrocode} -\def\Partial@start{\left\PartialOpen} -\def\Partial@end{\right\PartialClose} -\def\Partial@empty@end{\right\PartialEmptyClose} -\def\Partial{\@ifstar\Partial@star\Partial@nostar} -%^^A Several ifs to use later (breaks it if these definitions are inside) -\newif\iftwo@has@Nt -\two@has@Ntfalse -\newif\iftwo@has@xory -\two@has@xoryfalse -\newif\ifthree@has@Nt -\three@has@Ntfalse -\newif\ifthree@has@xory -\three@has@xoryfalse -\AtEndOfPackage{% - \edef\thermo@Nt{\Nt}% - \edef\thermo@x{x}% - \edef\thermo@y{y}% -} -\def\thermo@parse@two#1\relax{% - \@tfor\@i:=#1\do{% - \edef\@@i{\@i}% - \ifx\@@i\thermo@Nt - \two@has@Nttrue - \@break@tfor - \fi - \ifx\@@i\thermo@x - \two@has@xorytrue - \@break@tfor - \fi - \ifx\@@i\thermo@y - \two@has@xorytrue - \@break@tfor - \fi +\tl_new:N \l_@@_Partial_start_tl +\tl_new:N \l_@@_Partial_end_tl +\tl_new:N \l_@@_Partial_empty_end_tl +\tl_new:N \l_@@_Partial_middle_tl +\tl_set:Nn \l_@@_Partial_start_tl {\left\l_@@_PartialOpen_tl} +\tl_set:Nn \l_@@_Partial_end_tl {\right\l_@@_PartialClose_tl} +\tl_set:Nn \l_@@_Partial_empty_end_tl {\right\l_@@_PartialEmptyClose_tl} +\tl_set:Nn \l_@@_Partial_middle_tl {\middle} +\cs_set_eq:NN \@@_frac:nn \frac +\NewDocumentCommand{\Partial}{s m m m} +{ \bool_if:nTF {#1} + {% Starred form (recursive) + \settowidth{\l_@@_Partial_const_dim}{\ensuremath{#4}}% + \dim_add:Nn \l_@@_Partial_const_dim {-0.20\l_@@_Partial_const_dim}% + \Partial{#2}{#3}{#4}% + \bool_if:NT \l_@@_subscripted_bool + { \dim_compare:nNnTF \l_@@_operator_width_dim + < \l_@@_Partial_const_dim + { \kern -\l_@@_operator_width_dim } + { \kern -\l_@@_Partial_const_dim } + } + } + {% Unstarred form + \bool_if:NTF \l_@@_subscripted_bool + {% Handle case of empty variables held constant + \tl_if_eq:nnTF {#4} {} + { \l_@@_Partial_start_tl + \@@_frac:nn{\partial #2}{\partial #3}\l_@@_Partial_empty_end_tl + } + { \l_@@_Partial_start_tl\@@_frac:nn{\partial #2} + {\partial #3}\l_@@_Partial_end_tl + \c_math_subscript_token{#4}% + } + } + {% Check whether #4 contains \allNsbut{i} and #3 is \Nt_i + \tl_if_in:nnTF {#3} {\Nt} + { \RenewDocumentCommand{\allbut}{O{j} m m}{\allcomponents{##3}} + \l_@@_Partial_start_tl + \@@_frac:nn{\partial #2(\@@_sort_clist:n{#4})} + {\partial #3}\l_@@_Partial_end_tl + } + { \l_@@_Partial_start_tl + \@@_frac:nn{\partial #2(\@@_sort_clist:n{#3,#4})} + {\partial #3}\l_@@_Partial_end_tl + } + } } -} -\newcommand*{\Partial@nostar}[3]{% - \def\tmp@arg{#3}% - \if@subscripted - % Handles situation of empty variables held constant - \ifx\tmp@arg\@empty - \ensuremath{\Partial@start\frac{\partial #1} - {\partial #2}\Partial@empty@end}% - \else - \ensuremath{\Partial@start\frac{\partial #1} - {\partial #2}\Partial@end_{#3}}% - \fi - \else - % If not subscripted, we put the arguments (if any) in the derivative - \ifx\tmp@arg\@empty - \ensuremath{\Partial@start\frac{\partial #1} - {\partial #2}\Partial@empty@end}% - \else - % Check for whether #3 contains \allNsbut{i}/etc. and #2 is \Nt_i/etc. - \thermo@parse@two#2\relax - \iftwo@has@Nt - \renewcommand*{\allbut}[3][j]{\allcomponents{##3}}% - \ensuremath{\Partial@start\frac{\partial #1(#3)} - {\partial #2}\Partial@end}% - \else - \iftwo@has@xory - \renewcommand*{\allbutlastand}[3][j]{\allbut{\ncomponents}{##3}}% - \ensuremath{\Partial@start\frac{\partial #1(#3)} - {\partial #2}\Partial@end}% - \else - \ensuremath{\Partial@start\frac{\partial #1(#2,#3)} - {\partial #2}\Partial@end}% - \fi - \fi - \fi - \fi -} -\newcommand*{\Partial@star}[3]{% - \settowidth{\Partial@const@width}{\ensuremath{#3}}% - \addtolength{\Partial@const@width}{-0.15\Partial@const@width}% - \Partial@nostar{#1}{#2}{#3}% - \if@subscripted - \ifdim\operator@width<\Partial@const@width - \kern -\operator@width - \else - \kern -\Partial@const@width - \fi - \fi } % \end{macrocode} % \end{macro} -% \end{macro} % % \begin{macro}{\PartialBigg} -% \begin{macro}{\PartialBigg*} -% The \cs{PartialBigg} macro (and its starred form) replace the \cs{left} -% and \cs{right} commands in \cs{Partial} with \verb"amsmath"'s \cs{Biggl} -% and \cs{Biggr} variants. The starred form is inherited from \cs{Partial} +% The \cs{PartialBigg} macro (and its starred form) replace the \tn{left} +% and \tn{right} commands in \cs{Partial} with \pkg{amsmath}'s \tn{Biggl} +% and \tn{Biggr} variants. The starred form is inherited from \cs{Partial} % without modification. % \begin{macrocode} -\def\PartialBigg{% - \def\Partial@start{\Biggl\PartialOpen}% - \def\Partial@end{\Biggr\PartialClose}% - \def\Partial@empty@end{\Biggr\PartialClose}% - \Partial% -} +\NewDocumentCommand{\PartialBigg}{} + { \tl_set:Nn \l_@@_Partial_start_tl {\Biggl\l_@@_PartialOpen_tl} + \tl_set:Nn \l_@@_Partial_end_tl {\Biggr\l_@@_PartialClose_tl} + \tl_set:Nn \l_@@_Partial_Empty_end_tl + {\Biggr\l_@@_PartialEmptyClose_tl} + \Partial + } % \end{macrocode} % \end{macro} -% \end{macro} % \begin{macro}{\Partialbigg} -% \begin{macro}{\Partialbigg*} % The \cs{Partialbigg} macro does the same thing as \cs{PartialBigg}, except -% using \verb"amsmath"'s \cs{biggl}/\cs{biggr} variants. +% using \pkg{amsmath}'s \tn{biggl}/\tn{biggr} variants. % \begin{macrocode} -\def\Partialbigg{% - \def\Partial@start{\biggl\PartialOpen}% - \def\Partial@end{\biggr\PartialClose}% - \def\Partial@empty@end{\biggr\PartialClose}% - \Partial% -} +\NewDocumentCommand{\Partialbigg}{} + { \tl_set:Nn \l_@@_Partial_start_tl {\biggl\l_@@_PartialOpen_tl} + \tl_set:Nn \l_@@_Partial_end_tl {\biggr\l_@@_PartialClose_tl} + \tl_set:Nn \l_@@_Partial_empty_end_tl + {\biggr\l_@@_PartialEmptyClose_tl} + \Partial + } % \end{macrocode} % \end{macro} -% \end{macro} % % \begin{macro}{\PartialSecond} -% \begin{macro}{\PartialSecond*} % The second partial derivatives are defined similarly to \cs{Partial}. % \begin{macrocode} -\def\PartialSecond{\@ifstar\PartialSecond@star\PartialSecond@nostar} -\newcommand*{\PartialSecond@nostar}[3]{% - \def\tmp@arg{#3}% - \if@subscripted - % Handles situation of empty variables held constant - \ifx\tmp@arg\@empty - \ensuremath{\Partial@start\frac{\partial^2 #1} - {\partial #2^2}\Partial@empty@end}% - \else - \ensuremath{\Partial@start\frac{\partial^2 #1} - {\partial #2^2}\Partial@end_{#3}}% - \fi - \else - \ifx\tmp@arg\@empty - \ensuremath{\Partial@start\frac{\partial^2 #1} - {\partial #2^2}\Partial@empty@end}% - \else - % Check for whether #3 contains \allNsbut{i}/etc. and #2 is \Nt_i/etc. - \thermo@parse@two#2\relax - \iftwo@has@Nt - \renewcommand*{\allbut}[3][j]{\allcomponents{##3}}% - \ensuremath{\Partial@start\frac{\partial^2 #1(#3)} - {\partial #2^2}\Partial@end}% - \else - \iftwo@has@xory - \renewcommand*{\allbutlastand}[3][j]{\allbut{\ncomponents}{##3}}% - \ensuremath{\Partial@start\frac{\partial^2 #1(#3)} - {\partial #2^2}\Partial@end}% - \else - \ensuremath{\Partial@start\frac{\partial^2 #1(#2,#3)} - {\partial {#2}^2}\Partial@end}% - \fi - \fi - \fi - \fi -} -\newcommand*{\PartialSecond@star}[3]{% - \settowidth{\Partial@const@width}{\ensuremath{#3}}% - \addtolength{\Partial@const@width}{-0.15\Partial@const@width}% - \PartialSecond@nostar{#1}{#2}{#3}% - \if@subscripted - \ifdim\operator@width<\Partial@const@width - \kern -\operator@width - \else - \kern -\Partial@const@width - \fi - \fi +\NewDocumentCommand{\PartialSecond}{s m m m} +{ + \bool_if:nTF {#1} + {% Starred form + \settowidth{\l_@@_Partial_const_dim}{\ensuremath{#4}}% + \dim_add:Nn \l_@@_Partial_const_dim {-0.20\l_@@_Partial_const_dim} + \PartialSecond{#2}{#3}{#4}% + \bool_if:nT \l_@@_subscripted_bool + { \dim_compare:nNnTF {\l_@@_operator_width_dim} + < {\l_@@_Partial_const_dim} + { \kern -\l_@@_operator_width_dim } + { \kern -\l_@@_Partial_const_dim } + } + } + {% Unstarred form + \bool_if:NTF \l_@@_subscripted_bool + {% Handles case of empty variables held constant + \tl_if_eq:nnTF {#4} {} + { \l_@@_Partial_start_tl + \@@_frac:nn{\partial\c_math_superscript_token 2 #2} + {\partial #3\c_math_superscript_token 2}\l_@@_Partial_empty_end_tl + } + { \l_@@_Partial_start_tl + \@@_frac:nn{\partial\c_math_superscript_token 2 #2} + {\partial #3\c_math_superscript_token 2}\l_@@_Partial_end_tl + \c_math_subscript_token{#4}% + } + } + {% Check whether #4 contains \allNsbut{i} and #3 is \Nt_i + \tl_if_in:nnTF {#2} {\Nt} + { \RenewDocumentCommand{\allbut}{O{j} m m}{\allcomponents{##3}} + \l_@@_Partial_start_tl + \@@_frac:nn{\partial\c_math_superscript_token 2 #2(#4)} + {\partial\c_math_superscript_token 2 #3}\l_@@_Partial_end_tl + } + { \l_@@_Partial_start_tl + \@@_frac:nn{\partial\c_math_superscript_token 2 + #2(\@@_sort_clist:n{#3,#4})} + {\partial #3\c_math_superscript_token 2}\l_@@_Partial_end_tl + } + } + } } % \end{macrocode} % \end{macro} -% \end{macro} % \begin{macro}{\PartialSecondBigg} -% \begin{macro}{\PartialSecondBigg*} % The \cs{PartialSecondBigg} macro and its starred variant replace \cs{left} -% and \cs{right} with \verb"amsmath"'s \cs{Biggl} and \cs{Biggr}. +% and \tn{right} with \pkg{amsmath}'s \cs[module=amsmath]{Biggl} and +% \cs[module=amsmath]{Biggr}. % \begin{macrocode} -\def\PartialSecondBigg{% - \def\Partial@start{\expandafter\Biggl\PartialOpen}% - \def\Partial@end{\expandafter\Biggr\PartialClose}% - \PartialSecond% +\NewDocumentCommand{\PartialSecondBigg}{} +{ \tl_set:Nn \l_@@_Partial_start_tl {\biggl\l_@@_PartialOpen_tl} + \tl_set:Nn \l_@@_Partial_end_tl {\biggl\l_@@_PartialClose_tl} + \tl_set:Nn \l_@@_Partial_empty_end_tl {\biggl\l_@@_PartialClose_tl} + \PartialSecond } % \end{macrocode} % \end{macro} -% \end{macro} % \begin{macro}{\PartialSecondbigg} -% \begin{macro}{\PartialSecondbigg*} -% The \cs{PartialSecondbigg} macro and its starred variant replace \cs{left} -% and \cs{right} with \verb"amsmath"'s \cs{biggl} and \cs{biggr}. +% The \cs{PartialSecondbigg} macro and its starred variant replace \tn{left} +% and \tn{right} with \pkg{amsmath}'s \cs[module=amsmath]{biggl} and +% \cs[module=amsmath]{biggr}. % \begin{macrocode} -\def\PartialSecondbigg{% - \def\Partial@start{\expandafter\biggl\PartialOpen}% - \def\Partial@end{\expandafter\biggr\PartialClose}% - \PartialSecond% +\NewDocumentCommand{\PartialSecondbigg}{} +{ \tl_set:Nn \l_@@_Partial_start_tl {\biggl\l_@@_PartialOpen_tl} + \tl_set:Nn \l_@@_Partial_end_tl {\biggl\l_@@_PartialClose_tl} + \tl_set:Nn \l_@@_Partial_empty_end_tl {\biggl\l_@@_PartialClose_tl} + \PartialSecond } % \end{macrocode} % \end{macro} -% \end{macro} % % \begin{macro}{\PartialMixSecond} -% \begin{macro}{\PartialMixSecond*} % The macro \cs{PartialMixSecond} takes an extra argument, but is otherwise % the same as its same-variable cousin. % \begin{macrocode} -\def\PartialMixSecond{\@ifstar\PartialMixSecond@star\PartialMixSecond@nostar} -\newcommand*{\PartialMixSecond@nostar}[4]{% - \def\tmp@arg{#4}% - \if@subscripted - % Handles situation of empty variables held constant - \ifx\tmp@arg\@empty - \ensuremath{\Partial@start\frac{\partial^2 #1} - {\partial #2\partial#3}\Partial@empty@end}% - \else - \ensuremath{\Partial@start\frac{\partial^2 #1} - {\partial #2\partial#3}\Partial@end_{#4}}% - \fi - \else - \ifx\tmp@arg\@empty - \ensuremath{\Partial@start\frac{\partial^2 #1(#2,#3)} - {\partial #2\partial#3}\Partial@empty@end}% - \else - % This time, we check whether #2 OR #3 are \Nt_i/etc. - \thermo@parse@two#3\relax - \iftwo@has@Nt\three@has@Nttrue\fi - \iftwo@has@xory\three@has@xorytrue\fi - \two@has@Ntfalse - \two@has@xoryfalse - \thermo@parse@two#2\relax - \iftwo@has@Nt - \renewcommand*{\allbut}[3][j]{\allcomponents{##3}}% - \ensuremath{\Partial@start\frac{\partial^2 #1(#3,#4)} - {\partial #2\partial#3}\Partial@end}% - \else - \iftwo@has@xory - \renewcommand*{\allbutlastand}[3][j]{\allbut{\ncomponents}{##3}}% - \ensuremath{\Partial@start\frac{\partial^2 #1(#3,#4)} - {\partial #2\partial#3}\Partial@end}% - \else - \ifthree@has@Nt - \renewcommand*{\allbut}[3][j]{\allcomponents{##3}}% - \ensuremath{\Partial@start\frac{\partial^2 #1(#2,#4)} - {\partial #2\partial#3}\Partial@end}% - \else - \ifthree@has@xory - \PackageWarning{thermodynamics}{GOT HERE} - %\renewcommand*{\allbutlastand}[3][j]{\allbut{\ncomponents}{##3}}% - \renewcommand*{\allbutlastand}[3][j]{SCREW YOU}% - \ensuremath{\Partial@start\frac{\partial^2 #1(#2,#4)} - {\partial #2\partial#3}\Partial@end}% - \else - \ensuremath{\Partial@start\frac{\partial^2 #1(#2,#3,#4)} - {\partial #2\partial#3}\Partial@end}% - \fi - \fi - \fi - \fi - \fi - \fi -} -\newcommand*{\PartialMixSecond@star}[4]{% - \settowidth{\Partial@const@width}{\ensuremath{#4}}% - \addtolength{\Partial@const@width}{-0.25\Partial@const@width}% - \PartialMixSecond@nostar{#1}{#2}{#3}{#4}% - \if@subscripted - \ifdim\operator@width<\Partial@const@width - \kern -\operator@width - \else - \kern -\Partial@const@width - \fi - \fi +\bool_new:N \l_@@_has_x_or_y_bool +\NewDocumentCommand{\PartialMixSecond}{s m m m m} +{ + \bool_if:nTF {#1} + {% Starred version + \settowidth{\l_@@_Partial_const_dim}{\ensuremath{#4}}% + \dim_add:Nn \l_@@_Partial_const_dim {-0.20\l_@@_Partial_const_dim} + \PartialMixSecond{#2}{#3}{#4}{#5} + \bool_if:nT \l_@@_subscripted_bool + { \dim_compare:nNnTF {\l_@@_operator_width_dim} + < {\l_@@_Partial_const_dim} + { \kern -\l_@@_operator_width_dim } + { \kern -\l_@@_Partial_const_dim } + } + } + {% Unstarred version + \bool_if:nTF \l_@@_subscripted_bool + {% subscripted version + \tl_if_eq:nnTF {#5} {} + {% Handle case of empty variables held constant + \l_@@_Partial_start_tl + \@@_frac:nn{\partial\c_math_superscript_token 2 #2} + {\partial #3\partial #4}\l_@@_Partial_empty_end_tl + } + { \l_@@_Partial_start_tl + \@@_frac:nn{\partial\c_math_superscript_token 2 #2} + {\partial #3\partial #4}\l_@@_Partial_end_tl + \c_math_subscript_token{#5} + } + } + {% not subscripted + \tl_if_eq:nnTF {#5} {} + {% empty argument + \l_@@_Partial_start_tl + \@@_frac:nn{\partial\c_math_superscript_token 2 + #2(\@@_sort_clist:n{#3,#4,#5})} + {\partial #3\partial #4}\l_@@_Partial_empty_end_tl + } + {% Check whether #3 OR #4 are \Nt_i/etc. + \tl_if_in:nnTF {#3} {\Nt} + { \RenewDocumentCommand{\allbut}{O{j} m m}{\allcomponents{##3}}% + \l_@@_Partial_start_tl + \@@_frac:nn{\partial\c_math_superscript_token 2 + #2(\@@_sort_clist:n{#4,#5})} + {\partial #3\partial #4}\l_@@_Partial_end_tl + } + { \tl_if_in:nnTF {#4} {\Nt} + { \RenewDocumentCommand{\allbut}{O{j} m m}{\allcomponents{##3}}% + \l_@@_Partial_start_tl + \@@_frac:nn{\partial\c_math_superscript_token 2 + #2(\@@_sort_clist:n{#3,#5})} + {\partial #3\partial #4}\l_@@_Partial_end_tl + } + {% Check for x, y, or w + \bool_set_false:N \l_@@_has_x_or_y_bool + \tl_if_in:nnT {#3} {x} + { \l_@@_has_x_or_y_bool } + \tl_if_in:nnT {#3} {y} + { \l_@@_has_x_or_y_bool } + \tl_if_in:nnT {#3} {w} + { \l_@@_has_x_or_y_bool } + \bool_if:NTF \l_@@_has_x_or_y_bool + { \RenewDocumentCommand{\allbutlastand}{O{j} m m} + {\allcomponents{##3}} + \l_@@_Partial_start_tl + \@@_frac:nn{\partial\c_math_superscript_token 2 + #2(\@@_sort_clist:n{#4,#5})} + {\partial #3\partial #4}\l_@@_Partial_end_tl + } + { + \l_@@_Partial_start_tl + \@@_frac:nn{\partial\c_math_superscript_token 2 + #2(\@@_sort_clist:n{#3,#4,#5})} + {\partial #3\partial #4}\l_@@_Partial_end_tl + } + } + } + } + } + } } % \end{macrocode} % \end{macro} -% \end{macro} -% \begin{macro}{\PartialMixSecondBigg} -% \begin{macro}{\PartialMixSecondBigg*} -% \begin{macro}{\PartialMixSecondbigg} -% \begin{macro}{\PartialMixSecondbigg*} -% The macro \cs{PartialMixSecondBigg} and its starred form are analogous to -% \cs{PartialBigg} and \cs{PartialSecondBigg}. \cs{PartialMixSecondbigg} and -% its starred form are similarly analogous to \cs{Partialbigg} and -% \cs{PartialSecondbigg}. -% \begin{macrocode} -\def\PartialMixSecondBigg{% - \def\Partial@start{\expandafter\Biggl\PartialOpen}% - \def\Partial@end{\expandafter\Biggr\PartialClose}% - \PartialMixSecond% -} -\def\PartialMixSecondbigg{% - \def\Partial@start{\expandafter\biggl\PartialOpen}% - \def\Partial@end{\expandafter\biggr\PartialClose}% - \PartialMixSecond% -} -% \end{macrocode} -% If the user does not load the \verb"amsmath" package, we will not have access -% to \cs{Biggl}, \cs{Biggr}, \cs{biggl}, and \cs{biggr}, so we revert them back +% \begin{macro}{\PartialMixSecondBigg,\PartialMixSecondbigg} +% The macro \cs{PartialMixSecondBigg} is analogous to the aforementioned macros +% \cs{PartialBigg} and \cs{PartialSecondBigg}. \cs{PartialMixSecondbigg} is +% analogous to \cs{Partialbigg} and \cs{PartialSecondbigg}. +% \begin{macrocode} +\NewDocumentCommand{\PartialMixSecondBigg}{} +{ \tl_set:Nn \l_@@_Partial_start_tl {\Biggl\l_@@_PartialOpen_tl} + \tl_set:Nn \l_@@_Partial_end_tl {\Biggl\l_@@_PartialClose_tl} + \tl_set:Nn \l_@@_Partial_empty_end_tl {\Biggl\l_@@_PartialClose_tl} + \PartialMixSecond +} +\NewDocumentCommand{\PartialMixSecondbigg}{} +{ \tl_set:Nn \l_@@_Partial_start_tl {\biggl\l_@@_PartialOpen_tl} + \tl_set:Nn \l_@@_Partial_end_tl {\biggl\l_@@_PartialClose_tl} + \tl_set:Nn \l_@@_Partial_empty_end_tl {\biggl\l_@@_PartialClose_tl} + \PartialMixSecond +} +% \end{macrocode} +% +% If the user does not load the \pkg{amsmath} package, we will not have access +% to \cs[module=amsmath]{Biggl}, \cs{Biggr}, \cs{biggl}, and \cs{biggr}, so we revert them back % to the ordinary \cs{left} and \cs{right} versions and warn the user. % \begin{macrocode} \AtBeginDocument{% \@ifpackageloaded{amsmath}{}{% \PackageWarningNoLine{thermodynamics} - {Package amsmath not loaded; load to make PartialBigg and friends - work correctly}% - \let\PartialBigg\Partial - \let\Partialbigg\Partial - \let\PartialSecondBigg\PartialSecond - \let\PartialSecondbigg\PartialSecond - \let\PartialMixSecondBigg\PartialMixSecond - \let\PartialMixSecondbigg\PartialMixSecond + {Package~amsmath~not~loaded;~load~to~make~PartialBigg~and~friends + ~work~correctly}% + \cs_set_eq:NN \PartialBigg \Partial + \cs_set_eq:NN \Partialbigg \Partial + \cs_set_eq:NN \PartialSecondBigg \PartialSecond + \cs_set_eq:NN \PartialSecondbigg \PartialSecond + \cs_set_eq:NN \PartialMixSecondBigg \PartialMixSecond + \cs_set_eq:NN \PartialMixSecondbigg \PartialMixSecond + \ProvideDocumentCommand{\rvert}{}{|} + \ProvideDocumentCommand{\lvert}{}{|} }% } % \end{macrocode} % \end{macro} +% \changes{v1.01}{2023/09/15}{Added \cs{Partialinline} and friends to +% facilitate in-line (non-display-mode) partial derivatives, with +% corresponding changes to \cs{Partial} and friends for ease of +% implementation. Also added \cs{Partialinlinetext} and friends for +% non-expanding delimiters.} +% \begin{macro}{\Partialinline,\PartialSecondinline,\PartialMixSecondinline} +% Inline partial derivatives. +% \begin{macrocode} +\NewDocumentCommand{\Partialinline}{} +{ + \cs_set:Nn \@@_frac:nn { ##1 \l_@@_Partial_middle_tl / ##2 } + \Partial +} +\NewDocumentCommand{\PartialSecondinline}{} +{ + \cs_set:Nn \@@_frac:nn { ##1 \l_@@_Partial_middle_tl / ##2 } + \PartialSecond +} +\NewDocumentCommand{\PartialMixSecondinline}{} +{ + \cs_set:Nn \@@_frac:nn { ##1 \l_@@_Partial_middle_tl / ##2 } + \PartialMixSecond +} +% \end{macrocode} % \end{macro} +% \pagebreak[1] +% \setmarginparsize{\footnotesize} +% \begin{macro}{\Partialinlinetext} +% \begin{macro}{\PartialSecondinlinetext} +% \begin{macro}{\PartialMixSecondinlinetext} +% Text-only (non-extensible delimiter) versions of \cs{Partialinline} +% and friends. +%^^A TODO: These currently "pollute" other partial derivatives until the end +%^^A of the line (i.e., \Partialinline{z}{x}{y} = \Partial{z}{x}{y} will +%^^A produce identical things on both sides). For now, it's a "feature." +% \begin{macrocode} +\NewDocumentCommand{\Partialinlinetext}{} +{ \cs_set_eq:NN \l_@@_Partial_start_tl \l_@@_PartialOpen_tl + \cs_set_eq:NN \l_@@_Partial_end_tl \l_@@_PartialClose_tl + \cs_set_eq:NN \l_@@_Partial_empty_end_tl \l_@@_PartialEmptyClose_tl + \cs_set_eq:NN \l_@@_Partial_middle_tl \relax + \Partialinline +} +\NewDocumentCommand{\PartialSecondinlinetext}{} +{ \cs_set_eq:NN \l_@@_Partial_start_tl \l_@@_PartialOpen_tl + \cs_set_eq:NN \l_@@_Partial_end_tl \l_@@_PartialClose_tl + \cs_set_eq:NN \l_@@_Partial_empty_end_tl \l_@@_PartialEmptyClose_tl + \cs_set_eq:NN \l_@@_Partial_middle_tl \relax + \PartialSecondinline +} +\NewDocumentCommand{\PartialMixSecondinlinetext}{} +{ \cs_set_eq:NN \l_@@_Partial_start_tl \l_@@_PartialOpen_tl + \cs_set_eq:NN \l_@@_Partial_end_tl \l_@@_PartialClose_tl + \cs_set_eq:NN \l_@@_Partial_empty_end_tl \l_@@_PartialEmptyClose_tl + \cs_set_eq:NN \l_@@_Partial_middle_tl \relax + \PartialMixSecondinline +} +% \end{macrocode} % \end{macro} % \end{macro} +% \end{macro} +% \restoremarginparsize % % \subsection{Local Override of Delimiters} +% We define several environments that \emph{locally} override the delimiters on +% partial derivatives generated with \cs{Partial} and friends, the +% subscript notation for partial derivatives, and/or the definitions of +% range-oriented macros such as \cs{allNs}. These environments can be nested; +% the inner-most one will be honored if conflicts occur. % \begin{environment}{thermoparentheses} -% \begin{environment}{thermobrackets} -% \begin{environment}{thermobraces} -% \begin{environment}{thermobar} -% \begin{environment}{thermoplain} -% We define seven environments that \emph{locally} override the delimiters on -% partial derivatives generated with \cs{Partial} and friends and/or the -% subscript notation for partial derivatives. -% \begin{macrocode} -\newenvironment*{thermoparentheses}{ - \renewcommand*{\PartialOpen}{(}% - \renewcommand*{\PartialClose}{)}% - \renewcommand*{\PartialEmptyClose}{)}% +% Inside this environment, partial derivatives will have parentheses around +% them, regardless of package options. +% \begin{macrocode} +\NewDocumentEnvironment{thermoparentheses}{} +{ \cs_set:Nn \l_@@_PartialOpen_tl {(} + \cs_set:Nn \l_@@_PartialClose_tl {)} + \cs_set:Nn \l_@@_PartialEmptyClose_tl {)} }{} -\newenvironment*{thermobrackets}{% - \renewcommand*{\PartialOpen}{[}% - \renewcommand*{\PartialClose}{]}% - \renewcommand*{\PartialEmptyClose}{]}% +% \end{macrocode} +% \end{environment} +% \begin{environment}{thermobrackets} +% Inside this environment, partial derivatives will have brackets around +% them, regardless of package options. +% \begin{macrocode} +\NewDocumentEnvironment{thermobrackets}{} +{ \tl_set:Nn \l_@@_PartialOpen_tl {[} + \tl_set:Nn \l_@@_PartialClose_tl {]} + \tl_set:Nn \l_@@_PartialEmptyClose_tl {]} }{} -\newenvironment*{thermobraces}{% - \renewcommand*{\PartialOpen}{\{}% - \renewcommand*{\PartialClose}{\}}% - \renewcommand*{\PartialEmptyClose}{\}}% +% \end{macrocode} +% \end{environment} +% \begin{environment}{thermobraces} +% Inside this environment, partial derivatives will have braces around +% them, regardless of package options. +% \begin{macrocode} +\NewDocumentEnvironment{thermobraces}{} +{ \tl_set:Nn \l_@@_PartialOpen_tl {\{} + \tl_set:Nn \l_@@_PartialClose_tl {\}} + \tl_set:Nn \l_@@_PartialEmptyClose_tl {\}} }{} -\newenvironment*{thermobar}{% - \renewcommand*{\PartialOpen}{.}% - \renewcommand*{\PartialClose}{\rvert}% - \renewcommand*{\PartialEmptyClose}{.}% +% \end{macrocode} +% \end{environment} +% \begin{environment}{thermobar} +% Inside this environment, partial derivatives will have a trailing vertical +% bar, regardless of package options. +% \begin{macrocode} +\NewDocumentEnvironment{thermobar}{} +{ \tl_set:Nn \l_@@_PartialOpen_tl {.} + \tl_set:Nn \l_@@_PartialClose_tl {\rvert} + \tl_set:Nn \l_@@_PartialEmptyClose_tl {.} }{} -\newenvironment*{thermoplain}{% - \renewcommand*{\PartialOpen}{.}% - \renewcommand*{\PartialClose}{.}% - \renewcommand*{\PartialEmptyClose}{.}% - \@subscriptedfalse +% \end{macrocode} +% \end{environment} +% \begin{environment}{thermoplain} +% Inside this environment, partial derivatives will have no decorations +% around them, regardless of package options. +% \begin{macrocode} +\NewDocumentEnvironment{thermoplain}{} +{ \tl_set:Nn \l_@@_PartialOpen_tl {.} + \tl_set:Nn \l_@@_PartialClose_tl {.} + \tl_set:Nn \l_@@_PartialEmptyClose_tl {.} + \bool_set_false:N \l_@@_subscripted_bool }{} -\newenvironment*{thermoNOsubscripts}{\@subscriptedfalse}{} -\newenvironment*{thermosubscripts}{\@subscriptedtrue}{} % \end{macrocode} % \end{environment} +% \begin{environment}{thermoNOsubscripts} +% Inside this environment, subscripts will not be displayed to the right of +% partial derivatives, regardless of package options. +% \begin{macrocode} +\NewDocumentEnvironment{thermoNOsubscripts}{} + {\bool_set_false:N \l_@@_subscripted_bool} + {} +% \end{macrocode} +% \begin{environment}{thermosubscripts} +% Inside this environment, subscripts will be displayed to the right of +% partial derivatives, regardless of package options. % \end{environment} +% \begin{macrocode} +\NewDocumentEnvironment{thermosubscripts}{} + {\bool_set_true:N \l_@@_subscripted_bool} + {} +% \end{macrocode} % \end{environment} +% \begin{environment}{thermomolesrange} +% Inside this environment, the macro \cs{allNs} will expand to +% $n_1,\dotsc,n_C$ (or equivalent symbols if \cs{Nt} and/or \cs{ncomponents} +% have been redefined), regardless of package options. Similar expansions will +% result for \cs{allXs}, \cs{allYs}, \cs{allMs}, and so on. +% \changes{v2.00}{2023/11/16}{Added environment to invoke the ``moles-range'' +% definitions of \cs{allNs} and friends locally.} +% \begin{macrocode} +\NewDocumentEnvironment{thermomolesrange}{} + { \@@_set_moles_range } + {} +% \end{macrocode} % \end{environment} +% \begin{environment}{thermointensiveplain} +% \changes{v2.00}{2023/11/16}{Added environment to invoke the +% ``intensive-plain'' option locally.} +% \begin{macrocode} +% \begin{macrocode} +\NewDocumentEnvironment{thermointensiveplain}{} + { \@@_set_intensive_plain } + {} +% \end{macrocode} +% \end{environment} +% \begin{environment}{thermoextensiveplain} +% \changes{v2.00}{2023/11/16}{Added environment to invoke the +% ``extensive-plain'' option locally.} +% \begin{macrocode} +\NewDocumentEnvironment{thermoextensiveplain}{} + { \@@_set_extensive_plain } + {} +% \end{macrocode} +% \end{environment} +% \setmarginparsize{\scriptsize} +% \begin{environment}{thermointensivelowercase} +% \changes{v2.00}{2023/11/16}{Added environment to invoke the +% ``intensive-lowercase'' option locally.} +% \begin{macrocode} +\NewDocumentEnvironment{thermointensivelowercase}{} + {% { +% \RenewExpandableDocumentCommand{\MacroFont}{}{ +% \fontencoding\encodingdefault +% \fontfamily\ttdefault +% \fontseries\mddefault +% \fontshape\shapedefault +% \footnotesize} + + \@@_set_intensive_lowercase + \@@_set_lowercase_pms + } + {} +% \end{macrocode} +% \end{environment} +% \begin{environment}{thermoextensivesuperscript} +% \changes{v2.00}{2023/11/16}{Added environment to invoke the +% ``extensive-superscript'' option locally.} +% \begin{macrocode} +\NewDocumentEnvironment{thermoextensivesuperscript}{} + { + \@@_set_extensive_superscripts + } + {} +% \end{macrocode} % \end{environment} +% \restoremarginparsize % % \subsection{User-Interface Macros to Define Symbols} -% \begin{macro}{\DeclareSubscrSymbol} -% First, we define a (messy!)\ command that serves to create ``subscripted'' +% \begin{macro}{\NewSubscriptedSymbol} +% First, we define a command that serves to create ``subscripted'' % symbols; for example, typing \verb"\cP_i" should yield $C_{P,i}$ rather % than $C_{Pi}$, ${C_P}_i$, or ${C_{P_i}}$. Superscripts are also handled % properly and can be in either order. +% \changes{v2.00}{2023/11/16}{Deleted \cs{DeclareSubscriptedSymbol} in favor +% of \pkg{xparse}-based \cs{NewSubscriptedSymbol} and +% \cs{RenewSubscriptedSymbol}.} +% \begin{macrocode} +\cs_new:Npn \@@_check_definable:nN #1#2 +{ + \bool_set_true:N \l_@@_arg_legal_bool + \tl_trim_spaces_apply:nN {#1} \tl_if_single_token:nTF + { + \str_set:Nx \l_tmp_str {\tl_to_str:n {#1}} + \int_compare:nNnT {\str_count:N \l_tmp_str} = 1 + { \PackageError{thermodynamics} + {First~argument~of~'\tl_trim_spaces:o {\tl_to_str:n {#2}}'~ + must~be~a~command} + {The~first~argument~of~'\tl_trim_spaces:o {\tl_to_str:n {#2}}'~ + should~be~the~macro~that~will~be~used~to~refer~to~the~symbol.~ + The~provided~argument~'\tl_trim_spaces:o {\tl_to_str:n {#1}}'~ + is~a~single~character. + \MessageBreak Perhaps~a~backslash~is~missing?} + } + } + { \PackageError{thermodynamics} + {First~argument~of~'\tl_trim_spaces:o {\tl_to_str:n {#2}}'~ + must~be~a~command} + {The~first~argument~of~'\tl_trim_spaces:o {\tl_to_str:n {#2}}'~ + should~be~the~macro~that~will~be~used~to~refer~to~the~symbol.~ + The~provided~argument~'\tl_trim_spaces:o {\tl_to_str:n {#1}}'~ + contains~more~than~one~token. + \MessageBreak Perhaps~a~backslash~is~missing?} + } +} +\NewDocumentCommand{\NewSubscriptedSymbol}{m m m} +{ + \@@_check_definable:nN {#1} \NewSubscriptedSymbol + \cs_if_exist:NT #1 + { \PackageError{thermodynamics} + {Command~'\tl_trim_spaces:o {\tl_to_str:n {#1}}'~already~defined} + {You~have~used~ + '\tl_trim_spaces:o {\tl_to_str:n {\NewSubscriptedSymbol}}'~ + with~a~command~that~already~has~a~definition} + } + \cs_new:cpn {\cs_to_str:N #1_one:n} ##1 + { + {#2}\c_math_superscript_token{##1} + \peek_catcode_remove:NTF \c_math_subscript_token + { \use:c {\cs_to_str:N #1_three:n} } + { \c_math_subscript_token{#3} } + } + + \cs_new:cpn {\cs_to_str:N #1_two:n} ##1 + { {#2}\c_math_subscript_token{#3,##1} } + + \cs_new:cpn {\cs_to_str:N #1_three:n} ##1 + { \c_math_subscript_token{#3,##1} } + + \NewDocumentCommand{#1}{} + {% @branch + \peek_catcode_remove:NTF \c_math_superscript_token + { \use:c {\cs_to_str:N #1_one:n} } + { \peek_catcode_remove:NTF \c_math_subscript_token + { \use:c {\cs_to_str:N #1_two:n} } + { {#2}\c_math_subscript_token{#3} } + } + } +} +\NewDocumentCommand{\RenewSubscriptedSymbol}{m m m} +{ + \@@_check_definable:nN {#1} \RenewSubscriptedSymbol + \cs_if_exist:NF #1 + { \PackageError{thermodynamics} + {Command~'\tl_trim_spaces:o {\tl_to_str:n {#1}}'~not~defined} + {You~have~used~ + '\tl_trim_spaces:o {\tl_to_str:n {\RenewSubscriptedSymbol}}'~ + with~a~command~that~does~not~have~a~definition} + } + \cs_set:cpn {\cs_to_str:N #1_one:n} ##1 + { + {#2}\c_math_superscript_token{##1} + \peek_catcode_remove:NTF \c_math_subscript_token + { \use:c {\cs_to_str:N #1_three:n} } + { \c_math_subscript_token{#3} } + } + + \cs_set:cpn {\cs_to_str:N #1_two:n} ##1 + { {#2}\c_math_subscript_token{#3,##1} } + + \cs_set:cpn {\cs_to_str:N #1_three:n} ##1 + { \c_math_subscript_token{#3,##1} } + + \RenewDocumentCommand{#1}{} + {% @branch + \peek_catcode_remove:NTF \c_math_superscript_token + { \use:c {\cs_to_str:N #1_one:n} } + { \peek_catcode_remove:NTF \c_math_subscript_token + { \use:c {\cs_to_str:N #1_two:n} } + { {#2}\c_math_subscript_token{#3} } + } + } + +} +% \end{macrocode} +% \end{macro} +% \begin{macro}{\NewSuperscriptedSymbol} +% \changes{v2.00}{2023/11/16}{Created \cs{NewSuperscriptedSymbol} to handle +% superscripted excess and residual properties without intervention.} % \begin{macrocode} -\newcommand*{\DeclareSubscrSymbol}[3]{% - \expandafter\def\csname #1\endcsname{% - \@ifnextchar^{\csname @#1\endcsname} - {\@ifnextchar_{\csname @@#1\endcsname}{{#2}_{#3}}} +\NewDocumentCommand{\NewSuperscriptedSymbol}{m m m} +{ + \@@_check_definable:nN {#1} \NewSuperscriptedSymbol + \cs_if_exist:NT #1 + { \PackageError{thermodynamics} + {Command~'\tl_trim_spaces:o {\tl_to_str:n {#1}}'~already~defined} + {You~have~used~ + '\tl_trim_spaces:o {\tl_to_str:n {\NewSuperscriptedSymbol}}'~ + with~a~command~that~already~has~a~definition} + } + \cs_new:cpn {\cs_to_str:N #1_one:n} ##1 + { + {#2}\c_math_subscript_token{#1} + \peek_catcode_remove:NTF \c_math_superscript_token + { \use:c {\cs_to_str:N #1_one:n} } + { \c_math_subscript_token{#3} } + } + + \cs_new:cpn {\cs_to_str:N #1_two:n} ##1 + { {#2}\c_math_superscript_token{#3,##1} } + + \cs_new:cpn {\cs_to_str:N #1_three:n} ##1 + { {#2}\c_math_superscript_token{#3,##1} } + + \NewDocumentCommand{#1}{} + { + \peek_catcode_remove:NTF \c_math_subscript_token + { \use:c {\cs_to_str:N #1_one:n} } + { \peek_catcode_remove:NTF \c_math_superscript_token + { \use:c {\cs_to_str:N #1_two:n} } + { {#2}\c_math_superscript_token{#3} } + } + } +} +\NewDocumentCommand{\RenewSuperscriptedSymbol}{m m m} +{ + \@@_check_definable:nN {#1} \RenewSuperscriptedSymbol + \cs_if_exist:NF #1 + { \PackageError{thermodynamics} + {Command~'\tl_trim_spaces:o {\tl_to_str:n {#1}}'~not~defined} + {You~have~used~ + '\tl_trim_spaces:o {\tl_to_str:n {\RenewSuperscriptedSymbol}}'~ + with~a~command~that~does~not~have~a~definition} + } + \cs_set:cpn {\cs_to_str:N #1_one:n} ##1 + { + {#2}\c_math_subscript_token{##1} + \peek_catcode_remove:NTF \c_math_superscript_token + { \use:c {\cs_to_str:N #1_three:n} } + { \c_math_superscript_token{#3} } } - \expandafter\def\csname @#1\endcsname ##1##2{% - {#2}^{##2}\@ifnextchar_{\csname @@@#1\endcsname}{_{#3}}% + + \cs_set:cpn {\cs_to_str:N #1_two:n} ##1 + { {#2}\c_math_superscript_token{#3,##1} } + + \cs_set:cpn {\cs_to_str:N #1_three:n} ##1 + { \c_math_superscript_token{#3,##1} } + + \RenewDocumentCommand{#1}{} + {% @branch + \peek_catcode_remove:NTF \c_math_subscript_token + { \use:c {\cs_to_str:N #1_one:n} } + { \peek_catcode_remove:NTF \c_math_superscript_token + { \use:c {\cs_to_str:N #1_two:n} } + { {#2}\c_math_superscript_token{#3} } + } } - \expandafter\def\csname @@#1\endcsname ##1##2{{#2}_{#3,##2}} - \expandafter\def\csname @@@#1\endcsname ##1##2{_{#3,##2}} } % \end{macrocode} % \end{macro} -% \begin{macro}{\heatcapacitysymbol} -% \begin{macro}{\compressibilitysymbol} -% \begin{macro}{\expansivitysymbol} +% \begin{macro}{\heatcapacitysymbol,\compressibilitysymbol,\expansivitysymbol} % Now we define symbols for the heat capacities, compressibilities, and % so forth. % \begin{macrocode} -\newcommand*{\heatcapacitysymbol}{C} -\newcommand*{\compressibilitysymbol}{\kappa} -\newcommand*{\expansivitysymbol}{\alpha} +\NewExpandableDocumentCommand{\heatcapacitysymbol}{}{C} +\NewExpandableDocumentCommand{\compressibilitysymbol}{}{\kappa} +\NewExpandableDocumentCommand{\expansivitysymbol}{}{\alpha} +\NewExpandableDocumentCommand{\JTsymbol}{}{\mu} % \end{macrocode} % \end{macro} -% \end{macro} -% \end{macro} -% \begin{macro}{\cV} -% \begin{macro}{\cP} +% \begin{macro}{\cV,\cP} % The heat capacities are molar by default; we also declare extensive and % specific heat capacities. % The heat capacities themselves are defined to be ``smart'': \verb"\cV_i" will @@ -2601,150 +3236,121 @@ % ${C_V}_i$ or some other unintended symbol. Superscripts are also handled % appropriately and can be in either order. % \begin{macrocode} -\DeclareSubscrSymbol{cV}{\@intensive\heatcapacitysymbol}{\volume@symbol} -\DeclareSubscrSymbol{cP}{\@intensive\heatcapacitysymbol}{\pressure@symbol} +\NewSubscriptedSymbol{\cV}{\@@_intensive:n \heatcapacitysymbol} + {\g_@@_volume_symbol} +\NewSubscriptedSymbol{\cP}{\@@_intensive:n \heatcapacitysymbol} + {\g_@@_pressure_symbol} % \end{macrocode} % \end{macro} -% \end{macro} -% \begin{macro}{\cVt} -% \begin{macro}{\cPt} +% \begin{macro}{\cVt,\cPt} % We also introduce \emph{extensive} (rather than molar) heat capacity macros. % \begin{macrocode} -\DeclareSubscrSymbol{cVt}{\@extensive\heatcapacitysymbol}{\volume@symbol} -\DeclareSubscrSymbol{cPt}{\@extensive\heatcapacitysymbol}{\pressure@symbol} +\NewSubscriptedSymbol{\cVt}{\@@_extensive:n \heatcapacitysymbol} + {\g_@@_volume_symbol} +\NewSubscriptedSymbol{\cPt}{\@@_extensive:n \heatcapacitysymbol} + {\g_@@_pressure_symbol} % \end{macrocode} % \end{macro} -% \end{macro} -% \begin{macro}{\cPs} -% \begin{macro}{\cVs} +% \begin{macro}{\cVs,\cPs} % \cs{cPs} and \cs{cVs} are the specific heat capacities. % \begin{macrocode} -\DeclareSubscrSymbol{cVs}{\@specific\heatcapacitysymbol}{\volume@symbol} -\DeclareSubscrSymbol{cPs}{\@specific\heatcapacitysymbol}{\pressure@symbol} +\NewSubscriptedSymbol{\cVs}{\@@_specific:n \heatcapacitysymbol} + {\g_@@_volume_symbol} +\NewSubscriptedSymbol{\cPs}{\@@_specific:n \heatcapacitysymbol} + {\g_@@_pressure_symbol} % \end{macrocode} % \end{macro} -% \end{macro} % -% \begin{macro}{\kappaT} -% \begin{macro}{\kappaS} +% \begin{macro}{\kappaT,\kappaS} % The isothermal and adiabatic compressibilities are defined similarly, but % those do not have extensive versions for obvious reasons. % \begin{macrocode} -\DeclareSubscrSymbol{kappaT}{\compressibilitysymbol}{\temperature@symbol} -\DeclareSubscrSymbol{kappaS}{\compressibilitysymbol}{\entropy@symbol} +\NewSubscriptedSymbol{\kappaT}{\compressibilitysymbol} + {\g_@@_temperature_symbol} +\NewSubscriptedSymbol{\kappaS}{\compressibilitysymbol} + {\g_@@_entropy_symbol} % \end{macrocode} % \end{macro} -% \end{macro} -% \begin{macro}{\alphaP} -% \begin{macro}{\alphaS} +% \begin{macro}{\alphaP,\alphaS} % The macro \cs{alphaP} is intended to refer to the isobaric volume % expansivity, while \cs{alphaS} is the isentropic volume expansivity. % \begin{macrocode} -\DeclareSubscrSymbol{alphaP}{\expansivitysymbol}{\pressure@symbol} -\DeclareSubscrSymbol{alphaS}{\expansivitysymbol}{\entropy@symbol} +\NewSubscriptedSymbol{\alphaP}{\expansivitysymbol}{\g_@@_pressure_symbol} +\NewSubscriptedSymbol{\alphaS}{\expansivitysymbol}{\g_@@_entropy_symbol} % \end{macrocode} % \end{macro} +% \begin{macro}{\muJT} +% The macro \cs{muJT} renders the Joule--Thomson coefficient. +% \begin{macrocode} +\NewSubscriptedSymbol{\muJT}{\JTsymbol}{JT} +% \end{macrocode} % \end{macro} % -% \begin{macro}{\Psat} -% \begin{macro}{\Pvap} +% \begin{macro}{\Psat,\Pvap,\phisat,\fsat,\sat} % The \cs{Psat} macro (and its clone, the \cs{Pvap} macro) should be used for % the saturation pressure. -% \begin{macro}{\phisat} -% \begin{macro}{\fsat} -% \begin{macro}{\sat} % Similarly, a \cs{phisat} macro typesets the fugacity coefficient at % saturation. The \cs{fsat} macro similarly renders the fugacity at saturation. % Other saturation properties should use \verb"M^\sat" or similar, preferably % by defining another macro such as \verb"\Gmsat". % \begin{macrocode} -\newcommand*{\sat}{{\text{sat}}} -\newcommand*{\Psat}{P^\sat} -\let\Pvap\Psat -\newcommand*{\phisat}{\phi^\sat} -\newcommand*{\fsat}{f^\sat} +\NewDocumentCommand{\sat}{}{{\text{sat}}} +\NewDocumentCommand{\Psat}{}{P\c_math_superscript_token\sat} +\NewDocumentCommand{\Pvap}{}{\Psat} +\NewDocumentCommand{\phisat}{}{\phi\c_math_superscript_token\sat} +\NewDocumentCommand{\fsat}{}{\fpure\c_math_superscript_token\sat} % \end{macrocode} % \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% \begin{macro}{std} -% \begin{macro}{Pstd} -% \begin{macro}{fstd} +% \begin{macro}{\std,\Pstd,\fstd} % The \cs{std} macro denotes standard properties. \cs{Pstd} and \cs{fstd} are % defined for convenience and for consistency across textbooks. % \begin{macrocode} -\let\std\circ -\newcommand*{\Pstd}{P^\std} -\newcommand*{\fstd}{f^\std} +\NewDocumentCommand{\std}{}{\circ} +\NewDocumentCommand{\Pstd}{}{P\c_math_superscript_token \std} +\NewDocumentCommand{\fstd}{}{f\c_math_superscript_token \std} % \end{macrocode} % \end{macro} -% \end{macro} -% \end{macro} % -% \begin{macro}{\Deltamix} -% \begin{macro}{\mixing} -% Mixing properties, such as $\Delta G_\text{mix}$, should be accessed using +% \begin{macro}{\Deltamix,\mixing} +% Mixing properties, such as $\Deltamix\Gm$, should be accessed using % \verb"\Deltamix\Gm" and similar constructions---this construct will typeset -% as $\Delta_{MIX}G$ using the \verb"Thompson" package option, for example, -% and as $\Delta_\text{mix}G$ using the \verb"Sandler" package option. +% as $\Delta_{MIX}G$ using the |Thompson| package option, for example, +% and as $\Delta_\text{mix}\Gt$ using the |Sandler| package option. % \begin{macrocode} -\newcommand*{\mixing}{{\text{mix}}} -\newcommand*{\Deltamix}[1]{\Delta{#1}_\mixing} +\NewDocumentCommand{\mixing}{}{{\text{mix}}} +\NewDocumentCommand{\Deltamix}{m} + {\Delta{#1}\c_math_subscript_token\mixing} % \end{macrocode} % \end{macro} -% \end{macro} % -% \begin{macro}{\Deltafus} -% \begin{macro}{\fusion} -% \begin{macro}{\Deltavap} -% \begin{macro}{\vaporization} -% \begin{macro}{\Deltasub} -% \begin{macro}{\sublimation} -% \begin{macro}{\Deltarxn} -% \begin{macro}{\reaction} +% \pagebreak[2]% +% \begin{macro}{\Deltafus,\fusion,\Deltavap,\vaporization} +% \begin{macro}{\Deltasub,\sublimation,\Deltarxn,\reaction} % Similar entities for property changes on fusion, reaction, sublimation, and -% vaporization are defined. The heat of reaction is handled differently if -% \cs{cP} is its argument: one must typeset $\Delta C_{P,\text{rxn}}$ and -% $\Delta C_{P,\text{rxn}}^\circ$ rather than -% $\Delta{C_P}_\text{rxn}$ and $\Delta{C_P}^\circ_\text{rxn}$. -% \begin{macrocode} -\newcommand*{\fusion}{{\text{fus}}} -\newcommand*{\reaction}{{\text{rxn}}} -\newcommand*{\sublimation}{{\text{sub}}} -\newcommand*{\vaporization}{{\text{vap}}} -\newcommand*{\formation}{f} -\newcommand*{\Deltafus}[1]{\Delta{#1}^\fusion} -\newcommand*{\Deltasub}[1]{\Delta{#1}^\sublimation} -\newcommand*{\Deltavap}[1]{\Delta{#1}^\vaporization} -% TODO It would be nice not to have to handle \cP in a special way.... -\let\Delta@rxn@sym\relax -\DeclareSubscrSymbol{@DeltarxncP}{\Delta@rxn@sym}{\pressure@symbol,\reaction} -\DeclareSubscrSymbol{@Deltarxn}{\Delta@rxn@sym}{\reaction} -\newcommand*{\Deltarxn}[1]{% - \def\tmp@arg{#1}% - \def\tmp@@arg{\cP}% - \ifx\tmp@arg\tmp@@arg\relax - \def\@command{\def\Delta@rxn@sym{\Delta\@intensive\heatcapacitysymbol}% - \@DeltarxncP} - \else - \def\@command{\def\Delta@rxn@sym{\Delta{#1}}\@Deltarxn} - \fi - \@command -} -\let\Delta@f@sym\relax -\DeclareSubscrSymbol{@Deltaf}{\Delta@f@sym}{f} -\newcommand*{\Deltaf}[1]{\def\Delta@f@sym{\Delta{#1}}\@Deltaf} +% vaporization are defined. +% \begin{macrocode} +\NewDocumentCommand{\fusion}{}{{\text{fus}}} +\NewDocumentCommand{\reaction}{}{{\text{rxn}}} +\NewDocumentCommand{\sublimation}{}{{\text{sub}}} +\NewDocumentCommand{\vaporization}{}{{\text{vap}}} +\NewDocumentCommand{\formation}{}{f} +\NewDocumentCommand{\Deltafus}{m} + {\Delta #1\c_math_superscript_token\fusion} +\NewDocumentCommand{\Deltasub}{m} + {\Delta #1\c_math_superscript_token\sublimation} +\NewDocumentCommand{\Deltavap}{m} + {\Delta #1\c_math_superscript_token\vaporization} +\NewDocumentCommand{\Deltarxn}{m} + {\Delta #1\c_math_subscript_token\reaction} +\tl_new:N \l_@@_Deltaf_sym_tl +\NewSubscriptedSymbol{\@@_Deltaf}{\l_@@_Deltaf_sym_tl}{f} +\NewDocumentCommand{\Deltaf}{m} +{ \tl_set:Nn \l_@@_Deltaf_sym_tl {\Delta #1} + \@@_Deltaf +} % \end{macrocode} % \end{macro} % \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} % % \begin{macro}{\fmix} % The \cs{fmix} command is intended to describe fugacities in mixtures. @@ -2753,14 +3359,14 @@ % just $f_i$, and this command creates a consistent way to change between % such options. % \begin{macrocode} -\newcommand*{\fmix}{\hat{f}} +\NewDocumentCommand{\fmix}{}{\hat{f}} % \end{macrocode} % \end{macro} % \begin{macro}{\phimix} % A similar command, \cs{phimix}, renders $\hat\phi$ by default to represent % the fugacity coefficient in the mixture. % \begin{macrocode} -\newcommand*{\phimix}{\hat\phi} +\NewDocumentCommand{\phimix}{}{\hat\phi} % \end{macrocode} % \end{macro} % \begin{macro}{\fpure} @@ -2771,16 +3377,16 @@ % creates a consistent way to change between the these options. A similar % command for $\phi$ is given, \cs{phipure}, for fugacity coefficients. % \begin{macrocode} -\newcommand*{\fpure}{f} -\let\phipure\phi +\NewDocumentCommand{\fpure}{}{f} +\NewDocumentCommand{\phipure}{}{\phi} % \end{macrocode} % \end{macro} % % \subsection{Partial Molar Quantities} % \begin{macro}{\partialmolar} -% Partial molar quantities appear as $\thermooverline{G_i}$ or, -% for residual properties, $\thermooverline{G_i^R}$, rather than something like -% $\thermooverline{G}_i$ or $\thermooverline{G}_i^R$, which looks better but +% Partial molar quantities with superscripts appear as $\Gpm[\IG]{i}$ or +% $\GRpm{i}$, rather than something like +% $\overline{G}^\IG_i$ or $\overline{G}_i^R$; the former looks better but % is harder to implement for obvious reasons. Their definitions allow them to % be used as symbols, something like \verb"\Gpm_i", \verb"\Gpm^{\IGM}_i", % \verb"\Gpm^{\IGM}_i", and even \verb"\Gpm_i^{\IGM}"; @@ -2789,439 +3395,295 @@ % The macro \cs{partialmolar} can be used to create an arbitrary partial % molar symbol. % \begin{macrocode} -\let\pm@symbol\relax -\newcommand*{\partialmolar}[1]{\gdef\pm@symbol{#1}\generic@pm} -% if nextchar is _ -\def\generic@pm{\@ifnextchar_\@generic@pm\@@generic@pm} -% then store the argument -\def\@generic@pm#1#2{% - \gdef\pm@arg{#2}% - % if nextchar after argument is ^ - \@ifnextchar^\@@@generic@pm\@@@@generic@pm -} -% then print it this way -\def\@@@generic@pm#1#2{\thermo@overline{\pm@symbol^{#2}_{\pm@arg}}} -% else do it this way -\def\@@@@generic@pm{\thermo@overline{\pm@symbol_{\pm@arg}}} -% else, check whether there is also a ^ coming, otherwise assume -% it's [] or {} -\def\@@generic@pm{\@ifnextchar^\@@@@@generic@pm\@pm@bracket@check} -\def\@@@@@generic@pm#1#2#3#4{\thermo@overline{\pm@symbol^{#2}_{#4}}} -\def\@pm@bracket@check{\@ifnextchar[\@pm@bracket@yes\@pm@bracket@no} -\def\@pm@bracket@yes[#1]#2{\thermo@overline{\pm@symbol^{#1}_{#2}}} -\def\@pm@bracket@no#1{\thermo@overline{\pm@symbol_{#1}}} +\tl_new:N \l_@@_pm_symbol_tl +\tl_new:N \l_@@_pm_arg_tl +\NewDocumentCommand{\partialmolar}{m} +{ + \tl_set:Nn \l_@@_pm_symbol_tl {#1} + \@@_generic_pm: +} +%% cases to consider: +%% (1) \Mpm{i} +%% (2) \Mpm[S]{i} +%% (3) \Mpm^S_i +%% (4) \Mpm_i^S +%% (5) \Mpm_i +%% note that \Mpm^S with no subscript makes no sense and is thus forbidden +\cs_new:Nn \@@_generic_pm: +{ + \peek_catcode_remove:NTF \c_math_subscript_token + {% case 4 or case 5 + \@@_pm_case_four_or_five + } + {% look for superscript token + \peek_catcode_remove:NTF \c_math_superscript_token + {% case 3: \Mpm^{#1}_{#2} or \Mpm^{#1}{#2} + \@@_pm_case_three + } + {% Look for optional argument [...] + \peek_charcode:NTF [ + {% case 2: \Mpm[S]{i} + \@@_pm_case_two + } + {% case 1: \Mpm{i} + \@@_pm_case_one + } + } + } +} +\cs_new:Npn \@@_pm_case_one #1 +{ + \@@_overline:n {\l_@@_pm_symbol_tl\c_math_subscript_token{#1}} +} +\cs_new:Npn \@@_pm_case_two [#1]#2 +{ + \@@_overline:n {\l_@@_pm_symbol_tl + \c_math_superscript_token{#1}\c_math_subscript_token{#2}} +} +\cs_new:Npn \@@_pm_case_three #1 +{ + \tl_set:Nn \l_@@_pm_arg_tl {#1} + \peek_catcode_remove:NTF \c_math_subscript_token + { \@@_pm_case_three_part_two } + { \@@_pm_case_three_part_two } +} +\cs_new:Npn \@@_pm_case_three_part_two #1 +{ + \@@_overline:n {\l_@@_pm_symbol_tl + \c_math_superscript_token{\l_@@_pm_arg_tl} + \c_math_subscript_token{#1}} +} +\cs_new:Npn \@@_pm_case_four_or_five #1 +{ + \tl_set:Nn \l_@@_pm_arg_tl {#1} + \peek_catcode_remove:NTF \c_math_superscript_token + { \@@_pm_case_four } + { \@@_pm_case_five } +} +\cs_new:Npn \@@_pm_case_four #1 +{ + \@@_overline:n {\l_@@_pm_symbol_tl\c_math_superscript_token{#1} + \c_math_subscript_token{\l_@@_pm_arg_tl}} +} +\cs_new:Npn \@@_pm_case_five +{ + \@@_overline:n {\l_@@_pm_symbol_tl + \c_math_subscript_token{\l_@@_pm_arg_tl}} +} % \end{macrocode} % \end{macro} % % \subsection{Symbol Definitions} % These macros define the user interface to the symbols for energy, volume, -% and so forth. We define the ``extra'' symbols \cs{Bt} and \cs{Mt} to -% represent arbitrary properties. -% \begin{macro}{\Nt} -% \begin{macro}{\Et} -% \begin{macro}{\Ut} -% \begin{macro}{\Ft} -% \begin{macro}{\Gt} -% \begin{macro}{\Ht} -% \begin{macro}{\Lt} -% \begin{macro}{\At} -% \begin{macro}{\St} -% \begin{macro}{\Vt} -% \begin{macro}{\Qt} -% \begin{macro}{\Wt} -% \begin{macro}{\Mt} -% \begin{macro}{\Bt} -% \penalty-600% -% First, the extensive properties. -% \begin{macrocode} -\newcommand*{\Nt}{\mole@symbol} -\newcommand*{\Et}{\@extensive\totalenergy@symbol} -\newcommand*{\Ut}{\@extensive\internalenergy@symbol} -\newcommand*{\Ft}{\@extensive\Helmholtz@symbol} -\newcommand*{\Gt}{\@extensive\Gibbs@symbol} -\newcommand*{\Ht}{\@extensive\enthalpy@symbol} -\newcommand*{\Lt}{\@extensive\Landau@symbol} -\newcommand*{\At}{\@extensive\area@symbol} -\newcommand*{\St}{\@extensive\entropy@symbol} -\newcommand*{\Vt}{\@extensive\volume@symbol} -\newcommand*{\Qt}{\@extensive\heat@symbol} -\newcommand*{\Wt}{\@extensive\work@symbol} -\newcommand*{\Mt}{\@extensive M} -\newcommand*{\Bt}{\@extensive B} -% \end{macrocode} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} +% and so forth. There are five commands that define thermodynamic properties. % -% \begin{macro}{\Em} -% \begin{macro}{\Um} -% \begin{macro}{\Fm} -% \begin{macro}{\Gm} -% \begin{macro}{\Hm} -% \begin{macro}{\Lm} -% \begin{macro}{\Am} -% \begin{macro}{\Sm} -% \begin{macro}{\Vm} -% \begin{macro}{\Qm} -%^^A \penalty-600% -% Then the molar properties. -% \begin{macrocode} -\newcommand*{\Em}{\@intensive\totalenergy@symbol} -\newcommand*{\Um}{\@intensive\internalenergy@symbol} -\newcommand*{\Fm}{\@intensive\Helmholtz@symbol} -\newcommand*{\Gm}{\@intensive\Gibbs@symbol} -\newcommand*{\Hm}{\@intensive\enthalpy@symbol} -\newcommand*{\Lm}{\@intensive\Landau@symbol} -\newcommand*{\Am}{\@intensive\area@symbol} -\newcommand*{\Sm}{\@intensive\entropy@symbol} -\newcommand*{\Vm}{\@intensive\volume@symbol} -\newcommand*{\Qm}{\@intensive\heat@symbol} -% \end{macrocode} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} +% \begin{macro}{\NewExtensiveProperty} +% The command \cs{NewExtensiveProperty} declares macros for a total, molar, and +% specific version of the symbol; for example, a second heat-like property +% could be defined via +% \begin{verbatim} +% \NewExtensiveProperty{R}{\mathcal{Q}} +%\end{verbatim} +% \NewExtensiveProperty{R}{\mathcal{Q}}\relax +% The command above would declare the macros \cs{Rt}, \cs{Rm}, and \cs{Rs} +% that expand to $\Rt$, $\Rm$, and $\Rs$, respectively, using the default +% package options. % \end{macro} +% +% \begin{macro}{\NewPartialMolarProperty} +% The command \cs{NewPartialMolarProperty} declares a macro for the partial +% molar quantity. For example, +% \begin{verbatim} +% \NewPartialMolarProperty{I}{\Psi} +%\end{verbatim} +% \NewPartialMolarProperty{I}{\Psi}\relax +% would create the command \cs{Ipm}, which would typeset a partial molar +% command with the base symbol $\Psi$, yielding $\Ipm{i}$. % \end{macro} -% \begin{macro}{\Wm} -% \begin{macro}{\Mm} -% \begin{macro}{\Bm} -% More molar properties. +% +% \begin{macro}{\NewThermodynamicProperty} +% Declaring a new potential is handled by the +% \cs{NewThermodynamicProperty} macro, which takes two arguments. The first +% is the base of the name, and the second is the base of the symbol. This +% declares four new commands for the extensive, molar, specific, and partial +% molar properties. These commands consist of the first argument followed by +% \verb"t", \verb"m", \verb"s", and \verb"pm", respectively. For example, one +% might define the entropy via +% \begin{verbatim} +% \NewThermodynamicProperty{S}{S} +%\end{verbatim} +% and it would define the macros \cs{St}, \cs{Sm}, \cs{Ss}, and \cs{Spm} that +% yield, respectively, $\St$, S, $\hat S$, and $\Spm{i}$ (assuming the +% subscript to the partial molar quantity was $i$). +% It would also declare residual and excess properties for that base symbol. +% Note that the actual definition of the entropy and the other standard +% properties is slightly more complicated so as to allow for different symbols +% to be used in different textbooks. % \begin{macrocode} -\newcommand*{\Wm}{\@intensive\work@symbol} -\newcommand*{\Mm}{\@intensive M} -\newcommand*{\Bm}{\@intensive B} +\NewDocumentCommand{\NewThermodynamicProperty}{m m} +{ + \NewExtensiveProperty{#1}{#2} + \NewPartialMolarProperty{#1}{#2} + \NewResidualProperty{#1}{#2} + \NewExcessProperty{#1}{#2} +} +\NewDocumentCommand{\NewExtensiveProperty}{m m} +{ + % Extensive property + \exp_after:wN \NewDocumentCommand \exp_after:wN + {\cs:w #1t\cs_end:}{}{\@@_extensive:n {#2}} + % Molar property + \exp_after:wN \NewDocumentCommand \exp_after:wN + {\cs:w #1m\cs_end:}{}{\@@_intensive:n {#2}} + % Specific property + \exp_after:wN \NewDocumentCommand \exp_after:wN + {\cs:w #1s\cs_end:}{}{\@@_specific:n {#2}} +} +\NewDocumentCommand{\NewPartialMolarProperty}{m m} +{ + % Partial molar property + \exp_after:wN \NewDocumentCommand \exp_after:wN + {\cs:w #1pm\cs_end:}{}{\partialmolar{#2}} +} +\NewDocumentCommand{\NewExcessProperty}{m m} +{ + \exp_after:wN \NewSuperscriptedSymbol \exp_after:wN + {\cs:w #1 Et\cs_end:}{\@@_extensive:n{#2}}{\excess} + \exp_after:wN \NewSuperscriptedSymbol \exp_after:wN + {\cs:w #1 E\cs_end:}{\@@_intensive:n{#2}}{\excess} + \exp_after:wN \NewSuperscriptedSymbol \exp_after:wN + {\cs:w #1 Es\cs_end:}{\@@_specific:n{#2}}{\excess} + + %^^A TODO: make super- or subscripted partial molar quantities work + % Excess partial molar property + \exp_after:wN \NewDocumentCommand \exp_after:wN + {\cs:w #1Epm\cs_end:}{}{\partialmolar{#2} + \c_math_superscript_token\excess} +} +\NewDocumentCommand{\NewResidualProperty}{m m} +{ + \exp_after:wN \NewSuperscriptedSymbol \exp_after:wN + {\cs:w #1 Rt\cs_end:}{\@@_extensive:n{#2}}{\residual} + \exp_after:wN \NewSuperscriptedSymbol \exp_after:wN + {\cs:w #1 R\cs_end:}{\@@_intensive:n{#2}}{\residual} + \exp_after:wN \NewSuperscriptedSymbol \exp_after:wN + {\cs:w #1 Rs\cs_end:}{\@@_specific:n{#2}}{\residual} + + % Residual partial molar property + \exp_after:wN \NewDocumentCommand \exp_after:wN + {\cs:w #1Rpm\cs_end:}{}{\partialmolar{#2} + \c_math_superscript_token\residual} +} % \end{macrocode} % \end{macro} -% \end{macro} -% \end{macro} -% -% \begin{macro}{\Es} -% \begin{macro}{\Us} -% \begin{macro}{\Fs} -% \begin{macro}{\Gs} -% \begin{macro}{\Hs} -% \begin{macro}{\Ls} -% \begin{macro}{\As} -% \begin{macro}{\Ss} -% \begin{macro}{\Vs} -% \begin{macro}{\Qs} -% \begin{macro}{\Ws} -% \begin{macro}{\Ms} -% \begin{macro}{\Bs} +% \begin{macro}{\Nt,\Et,\Em,\Es,\Epm} % \penalty-600% -% Now the specific (per unit mass) properties. -% \begin{macrocode} -\newcommand*{\Us}{\@specific\internalenergy@symbol} -\newcommand*{\Es}{\@specific\totalenergy@symbol} -\newcommand*{\Fs}{\@specific\Helmholtz@symbol} -\newcommand*{\Gs}{\@specific\Gibbs@symbol} -\newcommand*{\Hs}{\@specific\enthalpy@symbol} -\newcommand*{\Ls}{\@specific\Landau@symbol} -\newcommand*{\As}{\@specific\area@symbol} -\newcommand*{\Ss}{\@specific\entropy@symbol} -\newcommand*{\Vs}{\@specific\volume@symbol} -\newcommand*{\Qs}{\@specific\heat@symbol} -\newcommand*{\Ws}{\@specific\work@symbol} -\newcommand*{\Ms}{\@specific M} -\newcommand*{\Bs}{\@specific B} -% \end{macrocode} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% -% \begin{macro}{\Epm} -% \begin{macro}{\Upm} -% \begin{macro}{\Hpm} -% \begin{macro}{\Fpm} -% \begin{macro}{\Gpm} -% \begin{macro}{\Apm} -% \begin{macro}{\Spm} -% \begin{macro}{\Vpm} -% \begin{macro}{\Lpm} -% \begin{macro}{\Mpm} -% \begin{macro}{\Bpm} -% Now the partial molar properties. -% \begin{macrocode} -\newcommand*{\Epm}{\partialmolar{\totalenergy@symbol}} -\newcommand*{\Upm}{\partialmolar{\internalenergy@symbol}} -\newcommand*{\Hpm}{\partialmolar{\enthalpy@symbol}} -\newcommand*{\Fpm}{\partialmolar{\Helmholtz@symbol}} -\newcommand*{\Gpm}{\partialmolar{\Gibbs@symbol}} -\newcommand*{\Apm}{\partialmolar{\area@symbol}} -\newcommand*{\Spm}{\partialmolar{\entropy@symbol}} -\newcommand*{\Vpm}{\partialmolar{\volume@symbol}} -\newcommand*{\Lpm}{\partialmolar{\Omega}} -\newcommand*{\Mpm}{\partialmolar{M}} -\newcommand*{\Bpm}{\partialmolar{B}} +% We define \cs{Nt} as the number of moles, as that changes between books a +% lot, but it does not have extensive, molar, and specific equivalents. +% Heat and work are defined, but lack partial molar properties. Area does not +% have excess or residual properties. +% \begin{macrocode} +\NewDocumentCommand{\Nt}{}{\g_@@_mole_symbol} +\NewThermodynamicProperty{E}{\g_@@_total_energy_symbol} +\NewThermodynamicProperty{U}{\g_@@_internal_energy_symbol} +\NewThermodynamicProperty{F}{\g_@@_Helmholtz_symbol} +\NewThermodynamicProperty{G}{\g_@@_Gibbs_symbol} +\NewThermodynamicProperty{H}{\g_@@_enthalpy_symbol} +\NewThermodynamicProperty{L}{\g_@@_Landau_symbol} +\NewThermodynamicProperty{V}{\g_@@_volume_symbol} +\NewThermodynamicProperty{S}{\g_@@_entropy_symbol} +\NewExtensiveProperty{A}{\g_@@_area_symbol} +\NewPartialMolarProperty{A}{\g_@@_area_symbol} +\NewExtensiveProperty{Q}{\g_@@_heat_symbol} +\NewExtensiveProperty{W}{\g_@@_work_symbol} % \end{macrocode} % \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} % -% \begin{macro}{\cPpm} -% \begin{macro}{\cVpm} +% \begin{macro}{\cVpm,\cPpm} % Partial molar heat capacities are \emph{hard}, but the following % implementation seems to work flawlessly\dots so far. % \begin{macrocode} -\newcommand*{\cPpm}{% - \def\@@@generic@pm##1##2{% - \thermo@overline{\pm@symbol^{##2}_{\pressure@symbol,\pm@arg}}}% - \def\@@@@generic@pm{\thermo@overline{\pm@symbol_{\pressure@symbol,\pm@arg}}}% - \def\@@@@@generic@pm##1##2##3##4{% - \thermo@overline{\pm@symbol^{##2}_{\pressure@symbol,##4}}}% - \def\@pm@bracket@yes[##1]##2{% - \thermo@overline{\pm@symbol^{##1}_{\pressure@symbol,##2}}}% - \def\@pm@bracket@no##1{\thermo@overline{\pm@symbol_{\pressure@symbol,##1}}}% - \partialmolar{\heatcapacitysymbol}% -} -\newcommand*{\cVpm}{% - \def\@@@generic@pm##1##2{% - \thermo@overline{\pm@symbol^{##2}_{\volume@symbol,\pm@arg}}}% - \def\@@@@generic@pm{\thermo@overline{\pm@symbol_{\volume@symbol,\pm@arg}}}% - \def\@@@@@generic@pm##1##2##3##4{% - \thermo@overline{\pm@symbol^{##2}_{\volume@symbol,##4}}}% - \def\@pm@bracket@yes[##1]##2{% - \thermo@overline{\pm@symbol^{##1}_{\volume@symbol,##2}}}% - \def\@pm@bracket@no##1{\thermo@overline{\pm@symbol_{\volume@symbol,##1}}}% - \partialmolar{\heatcapacitysymbol}% +\NewDocumentCommand{\cPpm}{} +{ + \cs_set:Npn \@@_pm_case_one ##1 + { + \@@_overline:n {\l_@@_pm_symbol_tl\c_math_subscript_token + {\g_@@_pressure_symbol,##1}} + } + \cs_set:Npn \@@_pm_case_two [##1]##2 + { + \@@_overline:n {\l_@@_pm_symbol_tl\c_math_superscript_token{##1} + \c_math_subscript_token{\g_@@_pressure_symbol,##2}} + } + \cs_set:Npn \@@_pm_case_three_part_two ##1 + { + \@@_overline:n {\l_@@_pm_symbol_tl + \c_math_superscript_token{\l_@@_pm_arg_tl} + \c_math_subscript_token{\g_@@_pressure_symbol,##1}} + } + \cs_set:Npn \@@_pm_case_four ##1 + { + \@@_overline:n {\l_@@_pm_symbol_tl + \c_math_superscript_token{##1}\c_math_subscript_token + {\g_@@_pressure_symbol,\l_@@_pm_arg_tl}} + } + \cs_set:Npn \@@_pm_case_five + { + \@@_overline:n {\l_@@_pm_symbol_tl\c_math_subscript_token + {\g_@@_pressure_symbol,\l_@@_pm_arg_tl}} + } + \partialmolar{\heatcapacitysymbol} +} +\NewDocumentCommand{\cVpm}{} +{ + \cs_set:Npn \@@_pm_case_one ##1 + { + \@@_overline:n {\l_@@_pm_symbol_tl\c_math_subscript_token + {\g_@@_volume_symbol,##1}} + } + \cs_set:Npn \@@_pm_case_two [##1]##2 + { + \@@_overline:n {\l_@@_pm_symbol_tl + \c_math_superscript_token{##1}\c_math_subscript_token + {\g_@@_volume_symbol,##2}} + } + \cs_set:Npn \@@_pm_case_three_part_two ##1 + { + \@@_overline:n {\l_@@_pm_symbol_tl + \c_math_superscript_token{\l_@@_pm_arg_tl} + \c_math_subscript_token{\g_@@_volume_symbol,##1}} + } + \cs_set:Npn \@@_pm_case_four ##1 + { + \@@_overline:n {\l_@@_pm_symbol_tl + \c_math_superscript_token{##1} + \c_math_subscript_token + {\g_@@_volume_symbol,\l_@@_pm_arg_tl}} + } + \cs_set:Npn \@@_pm_case_five + { + \@@_overline:n {\l_@@_pm_symbol_tl\c_math_subscript_token + {\g_@@_volume_symbol,\l_@@_pm_arg_tl}} + } + \partialmolar{\heatcapacitysymbol} } % \end{macrocode} % \end{macro} -% \end{macro} % % \subsection{Residual and Excess Properties} -% \begin{macro}{\residual} -% \begin{macro}{\excess} -% Macros are defined for residual properties (departure from non-ideal gases) +% \begin{macro}{\residual,\excess} +% Macros are defined for residual properties (departure from ideal gases) % and excess properties (departure from ideal solutions). We begin with two % macros to use for defining generic residual and excess properties that are % not already defined. % \begin{macrocode} -\newcommand*{\residual}{R} -\newcommand*{\excess}{E} -% \end{macrocode} -% \end{macro} -% \end{macro} -% -% \begin{macro}{\UR} -% \begin{macro}{\HR} -% \begin{macro}{\FR} -% \begin{macro}{\GR} -% \begin{macro}{\VR} -% \begin{macro}{\SR} -% The ordinary residual properties are molar. -% \begin{macrocode} -\newcommand*{\UR}{\Um^\residual} -\newcommand*{\HR}{\Hm^\residual} -\newcommand*{\FR}{\Fm^\residual} -\newcommand*{\GR}{\Gm^\residual} -\newcommand*{\VR}{\Vm^\residual} -\newcommand*{\SR}{\Sm^\residual} -% \end{macrocode} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% -% \pagebreak[3]% -% \begin{macro}{\URt} -% \begin{macro}{\HRt} -% \begin{macro}{\FRt} -% \begin{macro}{\GRt} -% \begin{macro}{\VRt} -% \begin{macro}{\SRt} -% We define similar macros for the extensive residual properties. These are -% appended by a \verb"t" (for ``total''). -% \begin{macrocode} -\newcommand*{\URt}{\Ut^\residual} -\newcommand*{\HRt}{\Ht^\residual} -\newcommand*{\FRt}{\Ft^\residual} -\newcommand*{\GRt}{\Gt^\residual} -\newcommand*{\VRt}{\Vt^\residual} -\newcommand*{\SRt}{\St^\residual} -% \end{macrocode} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% -% \begin{macro}{\URs} -% \begin{macro}{\HRs} -% \begin{macro}{\FRs} -% \begin{macro}{\GRs} -% \begin{macro}{\VRs} -% \begin{macro}{\SRs} -% Similar macros are declared for the specific residual properties. -% These are appended by an \verb"s". -% \begin{macrocode} -\newcommand*{\URs}{\Us^\residual} -\newcommand*{\HRs}{\Hs^\residual} -\newcommand*{\FRs}{\Fs^\residual} -\newcommand*{\GRs}{\Gs^\residual} -\newcommand*{\VRs}{\Vs^\residual} -\newcommand*{\SRs}{\Ss^\residual} -% \end{macrocode} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% -% \penalty-500 -% \begin{macro}{\URpm} -% \begin{macro}{\HRpm} -% \begin{macro}{\FRpm} -% \begin{macro}{\GRpm} -% \begin{macro}{\VRpm} -% \begin{macro}{\SRpm} -% Now for the partial molar residual properties. -% These are appended by \verb"pm". -% \begin{macrocode} -\newcommand*{\URpm}{\partialmolar{\internalenergy@symbol^\residual}} -\newcommand*{\HRpm}{\partialmolar{\enthalpy@symbol^\residual}} -\newcommand*{\FRpm}{\partialmolar{\Helmholtz@symbol^\residual}} -\newcommand*{\GRpm}{\partialmolar{\Gibbs@symbol^\residual}} -\newcommand*{\VRpm}{\partialmolar{\volume@symbol^\residual}} -\newcommand*{\SRpm}{\partialmolar{\entropy@symbol^\residual}} +\NewDocumentCommand{\residual}{}{R} +\NewDocumentCommand{\excess}{}{E} % \end{macrocode} % \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} % -% \begin{macro}{\UE} -% \begin{macro}{\HE} -% \begin{macro}{\FE} -% \begin{macro}{\GE} -% \begin{macro}{\VE} -% \begin{macro}{\SE} -% Now for the excess molar properties. -% \begin{macrocode} -\newcommand*{\UE}{\Um^\excess} -\newcommand*{\FE}{\Fm^\excess} -\newcommand*{\HE}{\Hm^\excess} -\newcommand*{\GE}{\Gm^\excess} -\newcommand*{\SE}{\Sm^\excess} -\newcommand*{\VE}{\Vm^\excess} -% \end{macrocode} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% -% \begin{macro}{\UEt} -% \begin{macro}{\HEt} -% \begin{macro}{\FEt} -% \begin{macro}{\GEt} -% \begin{macro}{\VEt} -% \begin{macro}{\SEt} -% Similarly, the extensive excess properties. -% \begin{macrocode} -\newcommand*{\UEt}{\Ut^\excess} -\newcommand*{\FEt}{\Ft^\excess} -\newcommand*{\HEt}{\Ht^\excess} -\newcommand*{\GEt}{\Gt^\excess} -\newcommand*{\SEt}{\St^\excess} -\newcommand*{\VEt}{\Vt^\excess} -% \end{macrocode} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% -% \begin{macro}{\UEs} -% \begin{macro}{\HEs} -% \begin{macro}{\FEs} -% \begin{macro}{\GEs} -% \begin{macro}{\VEs} -% \begin{macro}{\SEs} -% Now for the specific excess properties. -% \begin{macrocode} -\newcommand*{\UEs}{\Us^\excess} -\newcommand*{\FEs}{\Fs^\excess} -\newcommand*{\HEs}{\Hs^\excess} -\newcommand*{\GEs}{\Gs^\excess} -\newcommand*{\SEs}{\Ss^\excess} -\newcommand*{\VEs}{\Vs^\excess} -% \end{macrocode} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% -% \pagebreak[3]% -% \begin{macro}{\UEpm} -% \begin{macro}{\HEpm} -% \begin{macro}{\FEpm} -% \begin{macro}{\GEpm} -% \begin{macro}{\VEpm} -% \begin{macro}{\SEpm} -% Finally, the excess partial molar quantities. -% \begin{macrocode} -\newcommand*{\UEpm}{\partialmolar{\internalenergy@symbol^\excess}} -\newcommand*{\HEpm}{\partialmolar{\enthalpy@symbol^\excess}} -\newcommand*{\FEpm}{\partialmolar{\Helmholtz@symbol^\excess}} -\newcommand*{\GEpm}{\partialmolar{\Gibbs@symbol^\excess}} -\newcommand*{\VEpm}{\partialmolar{\volume@symbol^\excess}} -\newcommand*{\SEpm}{\partialmolar{\entropy@symbol^\excess}} -% \end{macrocode} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% \end{macro} -% -% \begin{macro}{\prodall} -% \begin{macro}{\sumall} -% \begin{macro}{\sumallbutlast} +% \pagebreak[1]% +% \begin{macro}{\prodall,\sumall,\summallbutlast} % The \cs{sumall} command and its cousin, \cs{sumallbutlast}, simplify the % typesetting of commonly-used sums; the command \cs{prodall} does the same % thing for products, viz., @@ -3235,102 +3697,194 @@ % K = \exp\left(\frac{-\Delta G_\text{rxn}^\circ}{RT}\right) % = \prod_{i=1}^C a_i^{\nu_i} \] % \begin{macrocode} -\newcommand*{\sumall}{\@ifnextchar_\@sumall\@@sumall} -\def\@sumall#1#2{\sum_{#2=1}^{\ncomponents}} -\def\@@sumall#1{\sum_{#1=1}^{\ncomponents}} -\newcommand*{\sumallbutlast}{\@ifnextchar_\@sumallbutlast\@@sumallbutlast} -\def\@sumallbutlast#1#2{\sum_{#2=1}^{\ncomponents-1}} -\def\@@sumallbutlast#1{\sum_{#1=1}^{\ncomponents-1}} -\newcommand*{\prodall}{\@ifnextchar_\@prodall\@@prodall} -\def\@prodall#1#2{\prod_{#2=1}^{\ncomponents}} -\def\@@prodall#1{\prod_{#1=1}^{\ncomponents}} +\NewDocumentCommand{\sumall}{m m} + { \sum\c_math_subscript_token{#2=1} + \c_math_superscript_token{\ncomponents} } +\NewDocumentCommand{\sumallbutlast}{m m} + { \sum\c_math_subscript_token{#2=1} + \c_math_superscript_token{\ncomponents-1} } +\NewDocumentCommand{\prodall}{m m} + { \prod\c_math_subscript_token{#2=1} + \c_math_superscript_token{\ncomponents} } % \end{macrocode} % \end{macro} -% \end{macro} -% \end{macro} % -% \begin{macro}{\IG} -% \begin{macro}{\IGM} -% \begin{macro}{\IS} +% \begin{macro}{\IG,\IGM,\IS} % The \cs{IG}, \cs{IGM}, and \cs{IS} macros (meaning ``ideal gas,'' ``ideal % gas mixture,'' and ``ideal solution,'' respectively) should be used to -% make clean transitions between textbooks---some use ``IM'' rather than ``IS'' -% for example. +% make clean transitions between textbooks---some use ``IM'' or ``ID'' rather +% than ``IS,'' for example. % \begin{macrocode} -\newcommand*{\IG}{{\text{IG}}} -\newcommand*{\IGM}{{\text{IGM}}} -\newcommand*{\IS}{{\text{IS}}} +\NewDocumentCommand{\IG}{}{{\text{IG}}} +\NewDocumentCommand{\IGM}{}{{\text{IGM}}} +\NewDocumentCommand{\IS}{}{{\text{IS}}} % \end{macrocode} % \end{macro} -% \end{macro} -% \end{macro} % -% \begin{macro}{\Henryrat} -% \begin{macro}{\Henrymol} +% \begin{macro}{\Henryrat,\Henrymol} % The Henry's Law constants for the rational basis ($y_i P = x_i h_i$) and % the molal basis ($y_i P = C_i \mathcal{H}_i$) are given by the macros % \cs{Henryrat} and \cs{Henrymol}, respectively. Using them this way % consistently allows for easy switching back and forth. % \begin{macrocode} -\newcommand*{\Henryrat}{h} -\newcommand*{\Henrymol}{{\mathcal{H}}} +\NewDocumentCommand{\Henryrat}{}{h} +\NewDocumentCommand{\Henrymol}{}{\mathcal{H}} % \end{macrocode} % \end{macro} -% \end{macro} % -% \begin{macro}{\gammarat} -% \begin{macro}{\gammamol} +% \begin{macro}{\gammarat,\gammamol} % The ordinary activity coefficient is universally denoted $\gamma$, so I -% have not defined a special macro for that. However, the Henry's Law activity -% coefficients are far from universal, so I have defined macros to make their -% use consistent. The defaults render \cs{gammarat} as $\gamma^\ast$ and -% \cs{gammamol} as $\gamma^\square$. +% have not defined a special macro for that. However, symbols for the Henry's +% Law activity coefficients are far from universal, so I have defined macros to +% make their use consistent. The defaults render \cs{gammarat} as $\gamma^\ast$ +% and \cs{gammamol} as $\gamma^\square$. % \cs{gammamol} will use \cs{square} from packages if it is defined; if not, -% it ``fakes it'' with the definition below (based on the \textsf{amsthm} -% package). -%^^A Code for \square ripped off from amsthm.sty with tweaks +% it ``fakes it'' with the definition below. +%^^A Backup for \square adapted from amsthm.sty with tweaks to make it +%^^A look reasonably similar to that from newpx (i.e., smaller than the +%^^A amsfonts) version % \begin{macrocode} \AtBeginDocument{% \providecommand*{\square}{% \text{\leavevmode - \hbox to.77778em{% + \hbox to.65em{% \hfil\vrule - \vbox to.6em{\hrule width.6em\vfil\hrule}% + \vbox to.53em{\hrule width.45em\vfil\hrule}% \vrule\hfil}% }% }% } -\newcommand*{\gammarat}{\gamma^\ast} -\newcommand*{\gammamol}{\gamma^\square} +\NewDocumentCommand{\gammarat}{}{\gamma\c_math_superscript_token\ast} +\NewDocumentCommand{\gammamol}{}{\gamma\c_math_superscript_token\square} % \end{macrocode} % \end{macro} -% \end{macro} +% \begin{environment}{thermovmatrix} +% This is a non-user-interface wrapper environment used to detect, in +% effect, whether \pkg{amsmath} has been loaded. If so, it uses its +% \env{vmatrix} environment for Jacobians; if not, it fakes it with +% \env{array} (which does not look nearly as good). +% \begin{macrocode} +\NewDocumentEnvironment{thermovmatrix}{} +{ \cs_if_exist:NTF \vmatrix + { \begin{vmatrix} } + { \left|\begin{array}{c c c c c c c c c c} } +} +{ \cs_if_exist:NTF \endvmatrix + { \end{vmatrix} } + { \end{array}\right| } +} +% \end{macrocode} +% \end{environment} % \begin{macro}{Jacobian} -% The \cs{Jacobian} command typesets the Jacobian, viz., -% \begin{verbatim} -% \[ \Jacobian{K}{L}{X}{Y} = -% \begin{vmatrix} -% \displaystyle \Partial{K}{X}{Y} & \displaystyle \Partial{K}{Y}{X} -% \\[2ex] -% \displaystyle \Partial{L}{X}{Y} & \displaystyle \Partial{L}{Y}{X} -% \end{vmatrix} -% \] -%\end{verbatim} -% produces -% \[ \left(\frac{\partial(K,L)}{\partial(X,Y)}\right) = -% \begin{vmatrix} -% \displaystyle \left(\frac{\partial K}{\partial X}\right)_Y -% & \displaystyle \left(\frac{\partial K}{\partial Y}\right)_X \\[2ex] -% \displaystyle \left(\frac{\partial L}{\partial X}\right)_Y -% & \displaystyle \left(\frac{\partial L}{\partial Y}\right)_X -% \end{vmatrix} -% \] -% This macro is defined purely for convenience. +% The \cs{Jacobian} command typesets the Leibnitz notation for the Jacobian +% determinant. +% \changes{v2.00}{2023/11/16}{Reimplemented \cs{Jacobian} to handle an +% arbitary number of variables and implemented \cs{Jacobiandet} to +% handle the matrix representation of the Jacobian.} % \begin{macrocode} -\newcommand*{\Jacobian}[4]{\frac{\partial{(#1,#2)}}{\partial{(#3,#4)}}}% +\NewDocumentCommand{\Jacobian}{m m} + {\@@_frac:nn{\partial(#1)}{\partial{(#2)}}} % \end{macrocode} % \end{macro} +% \begin{macro}{Jacobiandet} +% Similarly, the \cs{Jacobiandet} macro typesets the actual determinant that +% the Jacobian notation represents. +% \begin{macrocode} +\NewDocumentCommand{\Jacobiandet}{O{} O{} m m} +{ + \@@_Jacobian_set_ncomponents:nn {#3} {#4} + \begin{thermovmatrix} + \@@_Jacobianmatrix:nnnn {#1} {#2} {#3} {#4} + \end{thermovmatrix} +} +\seq_new:N \l_@@_row_seq +\seq_new:N \l_@@_matrix_seq +\clist_new:N \l_@@_other_vars_clist +\clist_new:N \l_@@_other_vars_copy_clist +\tl_new:N \l_@@_Jacobian_x_tl +\tl_new:N \l_@@_Jacobian_n_tl +\tl_new:N \l_@@_Jacobian_temp_tl +\bool_new:N \l_@@_found_dots_bool +\cs_new:Nn \@@_Jacobian_set_ncomponents:nn +{ + % If any entry is \dots, we assume the Jacobian is of the form + % d(f_1,\dots,f_n)/d(x_1,\dots,x_n) where f is some function + % (any symbol) and x is some variable (any symbol). + \tl_if_in:nnTF {#1} {\dots} + {% Has dots + \bool_set_true:N \l_@@_found_dots_bool + % look for what "x" is + \tl_set:Nn \l_@@_Jacobian_x_tl {\tl_head:n {#2}} + % look for what "n" is and set \ncomponents to it + \tl_set:Nx \l_@@_Jacobian_n_tl {\tl_item:nn {#2} {-1}} + \RenewExpandableDocumentCommand{\ncomponents}{}{\l_@@_Jacobian_n_tl} + } + {% Does not have dots; proceed accordingly + \bool_set_false:N \l_@@_found_dots_bool + } +} +\cs_new_protected:Nn \@@_Jacobianmatrix:nnnn +{ + \seq_clear:N \l_@@_matrix_seq + \clist_set:Nn \l_@@_other_vars_clist {#4} + \clist_set_eq:NN \l_@@_other_vars_copy_clist \l_@@_other_vars_clist + + \clist_map_inline:nn {#3} + { + \seq_clear:N \l_@@_row_seq + \tl_if_in:nnTF {##1} {\dots} + {% The current row has "dots" => row is \vdots && \vdots + \seq_put_right:Nn \l_@@_matrix_seq + { \vdots \c_alignment_token \c_alignment_token \vdots } + } + {% Ordinary row + \clist_map_inline:nn {#4} + { + \tl_if_in:nnTF {####1} {\dots} + {% this column has "dots" in it + \seq_put_right:Nn \l_@@_row_seq \dots + } + {% Normal column + \clist_set_eq:NN \l_@@_other_vars_clist + \l_@@_other_vars_copy_clist + \clist_remove_all:Nn \l_@@_other_vars_clist {####1} + \bool_if:NTF \l_@@_found_dots_bool + { \tl_set:Nn \l_@@_Jacobian_temp_tl {\tl_item:nn {####1} {-1}} + \seq_put_right:Nx \l_@@_row_seq + { + #1\Partial{##1}{####1} + {\allbut{\l_@@_Jacobian_temp_tl}{\l_@@_Jacobian_x_tl}} + } + } + { \seq_put_right:Nx \l_@@_row_seq + { + #1\Partial{##1}{####1} + {\clist_use:Nn \l_@@_other_vars_clist ,} + } + } + } + } + \seq_put_right:Nx \l_@@_matrix_seq + { + \seq_use:Nn \l_@@_row_seq { \c_alignment_token } + } + } + } + \tl_if_empty:nTF {#2} + { + \tl_if_eq:nnTF {#1} {\displaystyle} + { \seq_use:Nn \l_@@_matrix_seq { \\[2.75ex] } } + { \seq_use:Nn \l_@@_matrix_seq { \\[1.25ex] } } + } + { + \seq_use:Nn \l_@@_matrix_seq { \\[#2] } + } +} +% \end{macrocode} +% \end{macro} +%^^X\end{implementation} % +% \Finale % \iffalse %</package> %<*example> @@ -3342,6 +3896,7 @@ \author{Karl D. Hammond} \date{} \begin{document} +\NewThermodynamicProperty{B}{B} \maketitle\noindent The combined laws: \begin{align*} @@ -3377,6 +3932,33 @@ Some Maxwell reciprocity relations: = -\Partial*{\St}{\Nt_i}{T,P,\allNsbut{i}} = -\Spm_i \end{gather*} +Temporary changes of derivative delimiters: +\begin{gather*} + \begin{thermobrackets} + \Partial*{\Vt}{T}{P,\allNs} + \end{thermobrackets} + \begin{thermobar} + = \PartialMixSecond*{\Gt}{T}{P}{\allNs} + \end{thermobar} + \begin{thermomolesrange} + = \PartialMixSecond*{\Gt}{P}{T}{\allNs} + \end{thermomolesrange} + \begin{thermobraces} + = -\Partial*{\St}{P}{T,\allNs} + \begin{thermoNOsubscripts} + \begin{thermomolesrange} + = -\Partial{\St}{P}{T,\allNs} + \end{thermomolesrange} + \end{thermoNOsubscripts} + \end{thermobraces} +\end{gather*} +Inline derivatives: +\begin{gather*} + \mu_i = \Partialinline{\Gt}{\Nt_i}{T,P,\allNsbut{i}} + = \Partialinline{\Ft}{\Nt_i}{T,\Vt,\allNsbut{i}} + = \Partialinline{\Ht}{\Nt_i}{\St,P,\allNsbut{i}} + = \Partialinline{\Ut}{\Nt_i}{\St,\Vt,\allNsbut{i}} +\end{gather*} The heat capacities: \begin{gather*} \cV = T \Partial*{\Sm}{T}{\Vm,\allXs} = \Partial*{\Um}{T}{\Vm,\allXs} @@ -3449,7 +4031,7 @@ Fugacity and related properties: \\ a_i = \frac{\fmix_i}{\fstd_i} = x_i \gamma_i - \exp\left(\frac{1}{RT} \int_{\Pstd}^P \Vm_i(T,p) dp\right) + \exp\left(\frac{1}{RT} \int_{\Pstd}^P \Vm_i(T,p)\,dp\right) \approx x_i \gamma_i \\ \begin{split} @@ -3458,9 +4040,9 @@ Fugacity and related properties: = x_i \gammarat_i \Henryrat_i = C_i \gammamol_i \Henrymol_i = x_i \gamma_i \fsat_i - \exp\left(\frac{1}{RT} \int_{\Psat_i}^P \Vm_i(T,p) dp\right) + \exp\left(\frac{1}{RT} \int_{\Psat_i}^P \Vm_i(T,p)\,dp\right) \\ &= x_i \gamma_i \Psat_i \phisat_i - \exp\left(\frac{1}{RT} \int_{\Psat_i}^P \Vm_i(T,p) dp\right) + \exp\left(\frac{1}{RT} \int_{\Psat_i}^P \Vm_i(T,p)\,dp\right) \approx x_i \gamma_i \Psat_i \end{split} \end{gather*} @@ -3518,6 +4100,19 @@ Excess and Residual (Departure) Properties: \SE &= \Sm - \Sm^\IS & \VRpm_k &= \Vpm_k - \Vpm_k^\IGM \end{align*} +Jacobians: +\begin{gather*} + \Jacobian{\St,\Vt}{T,P} = \Jacobiandet{\St,\Vt}{T,P} \\ + \Jacobian{f,g,h}{x,y,z} = \Jacobiandet[\displaystyle]{f,g,h}{x,y,z} \\ + \Jacobian{h_1,\dots,h_k}{z_1,\dots,z_k} = + \Jacobiandet{h_1,\dots,h_k}{z_1,\dots,z_k} \\ + \cP = T\Partial{\Sm}{T}{P} + = T\Jacobian{\Sm,P}{T,P} + = -T\Jacobian{\Sm,P}{T,\Vm} \Jacobian{T,\Vm}{T,P} + = -T\Jacobian{P,\Sm}{\Vm,\Sm} \Jacobian{\Vm,\Sm}{T,\Vm} + \Jacobian{T,\Vm}{T,P} + = \gamma \cV +\end{gather*} \end{document} %</example> % \fi diff --git a/Master/texmf-dist/source/latex/thermodynamics/thermodynamics.ins b/Master/texmf-dist/source/latex/thermodynamics/thermodynamics.ins index 2e5ae9524fa..f2f2b95f40b 100644 --- a/Master/texmf-dist/source/latex/thermodynamics/thermodynamics.ins +++ b/Master/texmf-dist/source/latex/thermodynamics/thermodynamics.ins @@ -1,4 +1,4 @@ -%% File: thermodynamics.ins Copyright (C) 2021 Karl D. Hammond +%% File: thermodynamics.ins Copyright (C) 2022-2023 Karl D. Hammond %% %% Karl D. Hammond, %% Department of Chemical Engineering @@ -14,14 +14,15 @@ %% version 2005/12/01 or later. %% %% This work has the LPPL maintenance status `maintained'. -%% +%% %% The Current Maintainer of this work is K. D. Hammond. %% %% This work consists of the files thermodynamics.dtx and thermodynamics.ins -%% and the derived files thermodynamics.sty and thermodynamics.pdf. +%% and the derived files thermodynamics.sty, thermodynamics.pdf, +%% thermodynamics-examples.tex, and thermodynamics-examples.pdf. %% \fi -\input{docstrip} +\input{l3docstrip} \keepsilent \usedir{tex/latex/thermodynamics} @@ -29,13 +30,13 @@ This is a generated file. -Copyright (C) 2017-2018 by Karl D. Hammond +Copyright (C) 2022-2023 by Karl D. Hammond Karl D. Hammond, Department of Chemical Engineering University of Missouri Contact: hammondkd@missouri.edu - + This work may be distributed and/or modified under the conditions of the LaTeX Project Public License, either version 1.3 of this license or (at your option) any later version. |