summaryrefslogtreecommitdiff
diff options
context:
space:
mode:
authorKarl Berry <karl@freefriends.org>2022-01-27 21:41:19 +0000
committerKarl Berry <karl@freefriends.org>2022-01-27 21:41:19 +0000
commitdf6b587b2e27c8feb1d15b398cafa51305e9ae69 (patch)
tree6efddf5117c7f0accae88493d41a57e088566564
parentfe1ed2642ef6192d34790de9ae036ea97c7f1a9a (diff)
mandi (27jan22)
git-svn-id: svn://tug.org/texlive/trunk@61764 c570f23f-e606-0410-a88d-b1316a301751
Diffstat
-rw-r--r--Master/texmf-dist/doc/latex/mandi/README.md14
-rw-r--r--Master/texmf-dist/doc/latex/mandi/mandi.pdfbin468495 -> 500572 bytes
-rw-r--r--Master/texmf-dist/source/latex/mandi/mandi.dtx886
-rw-r--r--Master/texmf-dist/source/latex/mandi/mandi.ins10
-rw-r--r--Master/texmf-dist/source/latex/mandi/mandiexp.dtx527
-rw-r--r--Master/texmf-dist/source/latex/mandi/mandistudent.dtx987
-rw-r--r--Master/texmf-dist/tex/latex/mandi/mandi.sty512
-rw-r--r--Master/texmf-dist/tex/latex/mandi/mandiexp.sty459
-rw-r--r--Master/texmf-dist/tex/latex/mandi/mandistudent.sty611
9 files changed, 2392 insertions, 1614 deletions
diff --git a/Master/texmf-dist/doc/latex/mandi/README.md b/Master/texmf-dist/doc/latex/mandi/README.md
index 55cb93e783e..b40227e66d6 100644
--- a/Master/texmf-dist/doc/latex/mandi/README.md
+++ b/Master/texmf-dist/doc/latex/mandi/README.md
@@ -1,10 +1,10 @@
-mandi provides commands for introductory physics. To install, open a command
+`mandi` provides commands for introductory physics. To install, open a command
line and type the following, repeating 2-4 until there are no warnings:
-1. lualatex mandi.ins (can also use latex)
-2. lualatex mandi.dtx (lualatex is required)
-3. makeindex -s gind.ist -o mandi.ind mandi.idx
-4. makeindex -s gglo.ist -o mandi.gls mandi.glo
+1. `lualatex mandi.ins` (can also use latex)
+2. `lualatex mandi.dtx` (lualatex is required)
+3. `makeindex -s gind.ist -o mandi.ind mandi.idx`
+4. `makeindex -s gglo.ist -o mandi.gls mandi.glo`
-Move the *.sty files into a directory searched by TeX.
-The vdemo.py file is not needed.
+Move the `*.sty` files into a directory searched by TeX.
+The `vdemo.py` file is not needed and can be deleted.
diff --git a/Master/texmf-dist/doc/latex/mandi/mandi.pdf b/Master/texmf-dist/doc/latex/mandi/mandi.pdf
index edf20e95b69..4fb21eac802 100644
--- a/Master/texmf-dist/doc/latex/mandi/mandi.pdf
+++ b/Master/texmf-dist/doc/latex/mandi/mandi.pdf
Binary files differ
diff --git a/Master/texmf-dist/source/latex/mandi/mandi.dtx b/Master/texmf-dist/source/latex/mandi/mandi.dtx
index f78128d1a44..d3313fc5b48 100644
--- a/Master/texmf-dist/source/latex/mandi/mandi.dtx
+++ b/Master/texmf-dist/source/latex/mandi/mandi.dtx
@@ -1,7 +1,7 @@
% \iffalse meta-comment
% !TEX program = lualatexmk
%
-% Copyright (C) 2021 by Paul J. Heafner <heafnerj@gmail.com>
+% Copyright (C) 2021,2022 by Paul J. Heafner <heafnerj@gmail.com>
% ---------------------------------------------------------------------------
% 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
@@ -53,7 +53,14 @@
%
%<*driver>
\ProvidesFile{mandi.dtx}
-\documentclass[10pt]{ltxdoc}
+% As of 2021-12-02 ltxdoc.cls picks up ltxdoc.cfg and sets
+% the default paper size to a4paper rather than letter.
+% This can be changed in a local ltxdoc.cfg file but it is
+% easier to just use the article class and the doc package
+% instead and force letterpaper size.
+% \documentclass[10pt]{ltxdoc}
+\documentclass[10pt,letterpaper]{article}
+\usepackage{doc}
\PassOptionsToPackage{listings,documentation}{tcolorbox} % prevent option clash
\usepackage{\jobname} % load mandi.sty
\usepackage{mandistudent} % load mandistudent.sty
@@ -79,45 +86,72 @@
colback = gray!10!white,sidebyside,lefthand ratio = 0.5,center},%
listing style = vpython,%
}%
-% Redefine tcolorbox's \tcbdocnew and \tcbdocupdated defaults.
-\renewcommand*{\tcbdocnew}[1]
- {\textcolor{green!50!black}{\sffamily\bfseries N} #1}
-\renewcommand*{\tcbdocupdated}[1]
- {\textcolor{blue!75!black}{\sffamily\bfseries U} #1}
-\hypersetup{colorlinks=true} % colored links; no borders
% See https://tex.stackexchange.com/q/156383/218142
\newcommand*{\pkg}[1]{\textsf{#1}} % typeset package names
\newcommand*{\mandi}{\textsf{mandi}} % typeset mandi
\newcommand*{\mandistudent}{\textsf{mandistudent}} % typeset mandistudent
\newcommand*{\mandiexp}{\textsf{mandiexp}} % typeset mandiexp
-\newcommand*{\GlowScript}{\texttt{GlowScript}} % typeset GlowScript
-\newcommand*{\GlowScriptorg}{\texttt{GlowScript.org}} % typeset GlowScript.org
+\newcommand*{\WebVPython}{\texttt{Web VPython}} % typeset Web VPython
+\newcommand*{\WebVPythonorg}{\texttt{WebVPython.org}} % typeset WebVPython.org
\newcommand*{\VPython}{\texttt{VPython}} % typeset VPython
\newcommand*{\VPythonorg}{\texttt{VPython.org}} % typeset VPython.org
-\newcommand*{\gsurl}{glowscript.org} % GlowScript URL
+\newcommand*{\gsurl}{webvpython.org} % Web VPython URL
\newcommand*{\vpurl}{vpython.org} % VPython URL
\newcommand*{\lualatex}{Lua\LaTeX} % typeset LuaLaTeX
+%%%%% Some local hacks to make things better.
+% Redefine tcolorbox's \tcbdocnew and \tcbdocupdated defaults.
+\renewcommand*{\tcbdocnew}[1]
+ {\textcolor{green!50!black}{\sffamily\bfseries N} #1}
+\renewcommand*{\tcbdocupdated}[1]
+ {\textcolor{blue!75!black}{\sffamily\bfseries U} #1}
+\hypersetup{colorlinks=true} % colored links; no borders
+
% A customized internal hyperref tool to mimic that in tcolorbox.
% In fact, I borrowed it from tcolorbox.
-\NewDocumentCommand{\setplace}{ s m }{%
- \IfBooleanTF {#1}%
- {\phantomsection}%
- {}%
- \label{#2}%
-}%
-\NewDocumentCommand{\linktoplace}{ m m }{%
- \hyperref[#1]{\texttt{#2}%
- \ifnum\getpagerefnumber{#1}=\thepage\relax%
- \else%
- %\textsuperscript{\ding{213}\,{P.}\,\pageref*{#1}}%
- % Changed with tcolorbox 4.51
- \textsuperscript{{\fontfamily{pzd}\fontencoding{U}\fontseries{m}\fontshape{n}\selectfont\char213}
- \,{P.}\,\pageref*{#1}}%
- \fi%
+\NewDocumentCommand{\setplace}{ s m }%
+ {%
+ \IfBooleanTF {#1}%
+ {\phantomsection}%
+ {}%
+ \label{#2}%
+ }%
+\NewDocumentCommand{\linktoplace}{ m m }%
+ {%
+ \hyperref[#1]{\texttt{#2}%
+ \ifnum\getpagerefnumber{#1}=\thepage\relax%
+ \else%
+ %\textsuperscript{\ding{213}\,{P.}\,\pageref*{#1}}%
+ % Changed with tcolorbox 4.51
+ \textsuperscript{{\fontfamily{pzd}\fontencoding{U}\fontseries{m}\fontshape{n}\selectfont\char213}
+ \,{P.}\,\pageref*{#1}}%
+ \fi%
+ }%
}%
+
+% Clean up the Change History entries to get rid of General:
+% and add dates.
+% See https://tex.stackexchange.com/a/283894/218142
+\renewcommand{\generalname}{} % gets rid of General
+\makeatletter
+\renewcommand*{\changes@}[3]{%
+ \protected@edef\@tempa{%
+ \noexpand\glossary{#1 (#2)\levelchar
+ \ifx\saved@macroname\@empty
+ \space\actualchar\generalname
+ \else
+ \expandafter\@gobble\saved@macroname
+ \actualchar
+ \string\verb\quotechar*\verbatimchar\saved@macroname\verbatimchar
+ \fi
+ #3}}% gets rid of colon and adjusts spacing
+ \@tempa
+ \endgroup
+ \@esphack
}%
+\makeatother
+%%%%% End local hacks.
% We need a new command for in-line listings to prevent overfull boxes.
% Anything in |...| will be in small plain text.
@@ -142,7 +176,7 @@
% \IndexPrologue{\section{Index}Page numbers refer to page where the
% corresponding entry is documented and/or referenced.}
%
-% \CheckSum{2171}
+% \CheckSum{2156}
%
% \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
@@ -184,29 +218,29 @@
% \phantomsection
% \addcontentsline{toc}{section}{Acknowledgements}
% \section*{Acknowledgements}
-% To all of the students who have learned \LaTeX\ in my introductory
+% To all of the students who have learned \LaTeXe\ in my introductory
% physics courses over the years, I say a heartfelt thank you. You
% have contributed directly to the state of this software and to its
% use in introductory physics courses and to innovating how physics
% is taught.
%
-% I also acknowledge the \LaTeX\ developers who inhabit the
+% I also acknowledge the \LaTeXe\ developers who inhabit the
% \href{https://tex.stackexchange.com/}{\TeX\ StackExchange} site.
% Entering a new culture is daunting for anyone, especially for
-% newcomers. The \LaTeX\ development culture is no exception. We all
+% newcomers; the \LaTeXe\ development culture is no exception. We all
% share a passion for creating beautiful documents and I have learned
-% much over the past year that improved my ability to do just that.
-% There are too many of you to list individually, and I would surely
-% accidentally omit some were I to try. Collectively, I thank you all
-% for your patience and advice.
+% much over the summers of 2020 and 2021 that improved my ability to
+% do just that. There are too many of you to list individually, and I
+% would surely accidentally omit some were I to try. Collectively, I
+% thank you all for your patience and advice.
% \newpage
% \phantomsection
% \addcontentsline{toc}{section}{Change History}
% \PrintChanges
% \newpage
% \phantomsection
-% \addcontentsline{toc}{section}{List of \texttt{GlowScript} Programs}
-% \listofglowscriptprograms
+% \addcontentsline{toc}{section}{List of \texttt{Web VPython} Programs}
+% \listofwebvpythonprograms
% \phantomsection
% \addcontentsline{toc}{section}{List of \texttt{VPython} Programs}
% \listofvpythonprograms
@@ -215,9 +249,12 @@
% \listoffigures
% \restoregeometry
%
-% \changes{v3.0.0}{2021-08-22}{\mandi\ initial release}
-% \changes{v3.0.0}{2021-08-22}{\mandistudent\ initial release}
-% \changes{v3.0.0}{2021-08-22}{\mandiexp\ initial release}
+% \changes{v3.0.0}{2021-08-22}{\linktoplace{sec:mandipkg}{mandi} Initial release}
+% \changes{v3.0.0}{2021-08-22}{\linktoplace{sec:mandistudentpkg}{mandistudent} Initial release}
+% \changes{v3.0.0}{2021-08-22}{\linktoplace{sec:mandiexppkg}{mandiexp} Initial release}
+% \changes{v3.0.1}{2021-08-24}{\linktoplace{sec:mandipkg}{mandi} Minor doc changes}
+% \changes{v3.0.1}{2021-08-24}{\linktoplace{sec:mandistudentpkg}{mandistudent} Minor doc changes}
+% \changes{v3.0.1}{2021-08-24}{\linktoplace{sec:mandiexppkg}{mandiexp} Minor doc changes}
%
% \section{Introduction}
%
@@ -249,10 +286,21 @@
% as well as new, users is to treat this as a brand new experience. I think
% the most important thing to keep in mind is that I assume users,
% expecially new users, will have a relatively recent TeX distribution
-% (like TeX Live) that includes a recently updated \LaTeX\ kernel. If users
+% (like TeX Live) that includes a recently updated \LaTeXe\ kernel. If users
% report that this is a major problem, I can provide some degree of
-% backwards compatibility.
+% backwards compatibility. However, I use a fully updated TeX Live distribution.
%
+% \changes{v3.1.0}{2022-01-27}
+% {\linktoplace{sec:mandipkg}{mandi} Added GitHub links to code}
+% \section{Code Availability}
+% The \mandi\ source repository's \texttt{main} branch is at
+% \url{https://github.com/heafnerj/mandi}. This code will usually coincide
+% with that found on \href{https://ctan.org/pkg/mandi}{CTAN}. The very latest
+% build can be found on the \texttt{dev} branch found at
+% \url{https://github.com/heafnerj/mandi/tree/dev}. Students and other academic
+% academic users should probably get the \texttt{dev} branch code since it is
+% stable and may contain improvements over the \texttt{main} branch code.
+%
% \newpage
% \section{Student/Instructor Quick Guide}
%
@@ -266,7 +314,7 @@
%\iffalse
%<*example>
%\fi
-\begin{dispExample*}{lefthand ratio=0.80}
+\begin{dispExample*}{lefthand ratio = 0.80}
\( \vec{p} \) or \( \vec*{p} \) \\
\( \vec{p}_{\symup{final}} \) or \( \vec*{p}_{\symup{final}} \) \\
\( \magnitude{\vec{p}} \) or \( \magnitude*{\vec{p}_{\symup{final}}} \) \\
@@ -306,7 +354,7 @@
%\iffalse
%<*example>
%\fi
-\begin{dispExample*}{lefthand ratio=0.70}
+\begin{dispExample*}{lefthand ratio = 0.70}
\( \vacuumpermittivitymathsymbol = \vacuumpermittivity \)
\end{dispExample*}
%\iffalse
@@ -314,12 +362,12 @@
%\fi
%
% Use \refCom{mivector} to typeset symbolic vectors with components.
-% Use the aliases \refCom{direction} to typeset a direction or unit
+% Use the alias \refCom{direction} to typeset a direction or unit
% vector.
%\iffalse
%<*example>
%\fi
-\begin{dispExample*}{sidebyside=false}
+\begin{dispExample*}{sidebyside = false}
\( \mivector{\slot,\slot,\slot} \) or \( \mivector{p_x,p_y,p_z} \) \\
\( \direction{\frac{1}{\sqrt{3}},\frac{1}{\sqrt{3}},\frac{1}{\sqrt{3}}} \) or
\end{dispExample*}
@@ -329,8 +377,8 @@
%
% Use \refEnv{physicsproblem} and \refEnv{parts} and \refCom{problempart}
% for problems. For step-by-step mathematical solutions use
-% \refEnv{physicssolution}. Use \refEnv{glowscriptblock} to typeset
-% \href{https://\gsurl}{\GlowScript} programs. Use \refCom{vpythonfile} to
+% \refEnv{physicssolution}. Use \refEnv{webvpythonblock} to typeset
+% \href{https://\gsurl}{\WebVPython} programs. Use \refCom{vpythonfile} to
% typeset \href{https://\vpurl}{VPython} program files.
%
% \newpage
@@ -341,7 +389,7 @@
%\iffalse
%<*example>
%\fi
-\begin{dispListing*}{sidebyside=false,listing only}
+\begin{dispListing*}{sidebyside = false,listing only}
\usepackage[options]{mandi}
\end{dispListing*}
%\iffalse
@@ -354,7 +402,7 @@
\begin{docCommand}{mandiversion}{}
Typesets the current version and build date.
\end{docCommand}
-\begin{dispExample*}{sidebyside=false}
+\begin{dispExample*}{sidebyside = false}
The version is \mandiversion\ and is a stable build.
\end{dispExample*}
%\iffalse
@@ -391,7 +439,7 @@
%</example>
%\fi
%
-% \subsection{The \texttt{mandisetup} Command}
+% \subsection{The \texttt{\small mandisetup} Command}
%
%\iffalse
%<*example>
@@ -401,14 +449,14 @@
can be done in the preamble or inside the
|\begin{document}...\end{document}| environment.
\end{docCommand}
-\begin{dispListing*}{sidebyside=false,listing only}
+\begin{dispListing*}{sidebyside = false,listing only}
\mandisetup{units=base}
\end{dispListing*}
-\begin{dispListing*}{sidebyside=false,listing only}
+\begin{dispListing*}{sidebyside = false,listing only}
\mandisetup{preciseconstants}
\end{dispListing*}
-\begin{dispListing*}{sidebyside=false,listing only}
- \mandisetup{preciseconstants=false}
+\begin{dispListing*}{sidebyside = false,listing only}
+ \mandisetup{preciseconstants = false}
\end{dispListing*}
%\iffalse
%</example>
@@ -442,11 +490,11 @@
{%
doc new = 2021-02-24,%
doc name = momentumvector,%
- doc parameter = \marg{\ensuremath{c_1,\dots,c_n}},%
+ doc parameter = \marg{\( c_1,\dots,c_n \)},%
},%
{%
doc name = vectormomentum,%
- doc parameter = \marg{\ensuremath{c_1,\dots,c_n}},%
+ doc parameter = \marg{\( c_1,\dots,c_n \)},%
},%
}%
Command for momentum and its vector variants. The default units will depend
@@ -455,7 +503,7 @@
take more than three components. Note the other variants for the quantity's
value and units.
\end{docCommands}
-\begin{dispExample*}{lefthand ratio=0.60}
+\begin{dispExample*}{lefthand ratio = 0.60}
\( \momentum{5} \) \\
\( \momentumvalue{5} \) \\
\( \momentumbaseunits{5} \) \\
@@ -496,7 +544,7 @@
%\iffalse
%<*example>
%\fi
-\begin{docCommand}[doc new = 2021-02-16]{checkquantity}{\marg{name}}
+\begin{docCommand}[doc updated = 2022-01-27]{checkquantity}{\marg{name}}
Command to check and typeset the command, base units,
derived units, and alternate units of a defined physical
quantity.
@@ -527,11 +575,11 @@
{%
doc new = 2021-02-24,%
doc name = accelerationvector,%
- doc parameter = \marg{\ensuremath{c_1,\dots,c_n}},%
+ doc parameter = \marg{\( c_1,\dots,c_n \)},%
},%
{%
doc name = vectoracceleration,%
- doc parameter = \marg{\ensuremath{c_1,\dots,c_n}},%
+ doc parameter = \marg{\( c_1,\dots,c_n \)},%
},%
}%
\end{docCommands}
@@ -548,11 +596,11 @@
{%
doc new = 2021-02-24,%
doc name = angularaccelerationvector,%
- doc parameter = \marg{\ensuremath{c_1,\dots,c_n}},%
+ doc parameter = \marg{\( c_1,\dots,c_n \)},%
},%
{%
doc name = vectorangularacceleration,%
- doc parameter = \marg{\ensuremath{c_1,\dots,c_n}},%
+ doc parameter = \marg{\( c_1,\dots,c_n \)},%
},%
}%
\end{docCommands}
@@ -569,11 +617,11 @@
{%
doc new = 2021-02-24,%
doc name = angularimpulsevector,%
- doc parameter = \marg{\ensuremath{c_1,\dots,c_n}},%
+ doc parameter = \marg{\( c_1,\dots,c_n \)},%
},%
{%
doc name = vectorangularimpulse,%
- doc parameter = \marg{\ensuremath{c_1,\dots,c_n}},%
+ doc parameter = \marg{\( c_1,\dots,c_n \)},%
},%
}%
\end{docCommands}
@@ -587,11 +635,11 @@
{%
doc new = 2021-02-24,%
doc name = angularmomentumvector,%
- doc parameter = \marg{\ensuremath{c_1,\dots,c_n}},%
+ doc parameter = \marg{\( c_1,\dots,c_n \)},%
},%
{%
doc name = vectorangularmomentum,%
- doc parameter = \marg{\ensuremath{c_1,\dots,c_n}},%
+ doc parameter = \marg{\( c_1,\dots,c_n \)},%
},%
}%
\end{docCommands}
@@ -605,11 +653,11 @@
{%
doc new = 2021-02-24,%
doc name = angularvelocityvector,%
- doc parameter = \marg{\ensuremath{c_1,\dots,c_n}},%
+ doc parameter = \marg{\( c_1,\dots,c_n \)},%
},%
{%
doc name = vectorangularvelocity,%
- doc parameter = \marg{\ensuremath{c_1,\dots,c_n}},%
+ doc parameter = \marg{\( c_1,\dots,c_n \)},%
},%
}%
\end{docCommands}
@@ -638,11 +686,11 @@
{%
doc new = 2021-02-24,%
doc name = cmagneticfieldvector,%
- doc parameter = \marg{\ensuremath{c_1,\dots,c_n}},%
+ doc parameter = \marg{\( c_1,\dots,c_n \)},%
},%
{%
doc name = vectorcmagneticfield,%
- doc parameter = \marg{\ensuremath{c_1,\dots,c_n}},%
+ doc parameter = \marg{\( c_1,\dots,c_n \)},%
},%
}%
\end{docCommands}
@@ -668,11 +716,11 @@
{%
doc new = 2021-02-24,%
doc name = currentdensityvector,%
- doc parameter = \marg{\ensuremath{c_1,\dots,c_n}},%
+ doc parameter = \marg{\( c_1,\dots,c_n \)},%
},%
{%
doc name = vectorcurrentdensity,%
- doc parameter = \marg{\ensuremath{c_1,\dots,c_n}},%
+ doc parameter = \marg{\( c_1,\dots,c_n \)},%
},%
}%
\end{docCommands}
@@ -689,11 +737,11 @@
},%
{%
doc name = directionvector,%
- doc parameter = \marg{\ensuremath{c_1,\dots,c_n}},%
+ doc parameter = \marg{\( c_1,\dots,c_n \)},%
},%
{%
doc name = vectordirection,%
- doc parameter = \marg{\ensuremath{c_1,\dots,c_n}},%
+ doc parameter = \marg{\( c_1,\dots,c_n \)},%
},%
}%
\end{docCommands}
@@ -707,11 +755,11 @@
{%
doc new = 2021-02-24,%
doc name = displacementvector,%
- doc parameter = \marg{\ensuremath{c_1,\dots,c_n}},%
+ doc parameter = \marg{\( c_1,\dots,c_n \)},%
},%
{%
doc name = vectordisplacement,%
- doc parameter = \marg{\ensuremath{c_1,\dots,c_n}},%
+ doc parameter = \marg{\( c_1,\dots,c_n \)},%
},%
}%
\end{docCommands}
@@ -728,10 +776,10 @@
{%
doc new = 2021-02-24,%
doc name = electricdipolemomentvector,%
- doc parameter = \marg{\ensuremath{c_1,\dots,c_n}},%
+ doc parameter = \marg{\( c_1,\dots,c_n \)},%
},%
{ doc name = vectorelectricdipolemoment,%
- doc parameter = \marg{\ensuremath{c_1,\dots,c_n}},%
+ doc parameter = \marg{\( c_1,\dots,c_n \)},%
},%
}%
\end{docCommands}
@@ -745,11 +793,11 @@
{%
doc new = 2021-02-24,%
doc name = electricfieldvector,%
- doc parameter = \marg{\ensuremath{c_1,\dots,c_n}},%
+ doc parameter = \marg{\( c_1,\dots,c_n \)},%
},%
{%
doc name = vectorelectricfield,%
- doc parameter = \marg{\ensuremath{c_1,\dots,c_n}},%
+ doc parameter = \marg{\( c_1,\dots,c_n \)},%
},%
}%
\end{docCommands}
@@ -793,11 +841,11 @@
{%
doc new = 2021-02-24,%
doc name = energyfluxvector,%
- doc parameter = \marg{\ensuremath{c_1,\dots,c_n}},%
+ doc parameter = \marg{\( c_1,\dots,c_n \)},%
},%
{%
doc name = vectorenergyflux,%
- doc parameter = \marg{\ensuremath{c_1,\dots,c_n}},%
+ doc parameter = \marg{\( c_1,\dots,c_n \)},%
},%
}%
\end{docCommands}
@@ -814,11 +862,11 @@
{%
doc new = 2021-02-24,%
doc name = forcevector,%
- doc parameter = \marg{\ensuremath{c_1,\dots,c_n}},%
+ doc parameter = \marg{\( c_1,\dots,c_n \)},%
},%
{%
doc name = vectorforce,%
- doc parameter = \marg{\ensuremath{c_1,\dots,c_n}},%
+ doc parameter = \marg{\( c_1,\dots,c_n \)},%
},%
}%
\end{docCommands}
@@ -835,11 +883,11 @@
{%
doc new = 2021-02-24,%
doc name = gravitationalfieldvector,%
- doc parameter = \marg{\ensuremath{c_1,\dots,c_n}},%
+ doc parameter = \marg{\( c_1,\dots,c_n \)},%
},%
{%
doc name = vectorgravitationalfield,%
- doc parameter = \marg{\ensuremath{c_1,\dots,c_n}},%
+ doc parameter = \marg{\( c_1,\dots,c_n \)},%
},%
}%
\end{docCommands}
@@ -859,11 +907,11 @@
{%
doc new = 2021-02-24,%
doc name = impulsevector,%
- doc parameter = \marg{\ensuremath{c_1,\dots,c_n}},%
+ doc parameter = \marg{\( c_1,\dots,c_n \)},%
},%
{%
doc name = vectorimpulse,%
- doc parameter = \marg{\ensuremath{c_1,\dots,c_n}},%
+ doc parameter = \marg{\( c_1,\dots,c_n \)},%
},%
}%
\end{docCommands}
@@ -880,6 +928,9 @@
\begin{docCommand}{linearmassdensity}{\marg{magnitude}}
\end{docCommand}
\checkquantity{linearmassdensity}
+\begin{docCommand}[doc new = 2022-01-27]{lorentzfactor}{\marg{magnitude}}
+\end{docCommand}
+\checkquantity{lorentzfactor}
\begin{docCommand}[doc updated = 2021-05-02]{luminousintensity}{\marg{magnitude}}
\end{docCommand}
\checkquantity{luminousintensity}
@@ -895,11 +946,11 @@
{%
doc new = 2021-02-24,%
doc name = magneticdipolemomentvector,%
- doc parameter = \marg{\ensuremath{c_1,\dots,c_n}},%
+ doc parameter = \marg{\( c_1,\dots,c_n \)},%
},%
{%
doc name = vectormagneticdipolemoment,%
- doc parameter = \marg{\ensuremath{c_1,\dots,c_n}},%
+ doc parameter = \marg{\( c_1,\dots,c_n \)},%
},%
}%
\end{docCommands}
@@ -913,11 +964,11 @@
{%
doc new = 2021-02-24,%
doc name = magneticfieldvector,%
- doc parameter = \marg{\ensuremath{c_1,\dots,c_n}},%
+ doc parameter = \marg{\( c_1,\dots,c_n \)},%
},%
{%
doc name = vectormagneticfield,%
- doc parameter = \marg{\ensuremath{c_1,\dots,c_n}},%
+ doc parameter = \marg{\( c_1,\dots,c_n \)},%
},%
}%
\end{docCommands}
@@ -945,12 +996,12 @@
doc new = 2021-02-24,%
doc name = momentumvector,%
doc label = momentumvectordemo,%
- doc parameter = \marg{\ensuremath{c_1,\dots,c_n}},%
+ doc parameter = \marg{\( c_1,\dots,c_n \)},%
},%
{%
doc name = vectormomentum,%
doc label = vectormomentumdemo,%
- doc parameter = \marg{\ensuremath{c_1,\dots,c_n}} },%
+ doc parameter = \marg{\( c_1,\dots,c_n \)} },%
}%
\end{docCommands}
\checkquantity{momentum}
@@ -963,11 +1014,11 @@
{%
doc new = 2021-02-24,%
doc name = momentumfluxvector,%
- doc parameter = \marg{\ensuremath{c_1,\dots,c_n}},%
+ doc parameter = \marg{\( c_1,\dots,c_n \)},%
},%
{%
doc name = vectormomentumflux,%
- doc parameter = \marg{\ensuremath{c_1,\dots,c_n}},%
+ doc parameter = \marg{\( c_1,\dots,c_n \)},%
},%
}%
\end{docCommands}
@@ -999,11 +1050,11 @@
{%
doc new = 2021-02-24,%
doc name = poyntingvector,%
- doc parameter = \marg{\ensuremath{c_1,\dots,c_n}},%
+ doc parameter = \marg{\( c_1,\dots,c_n \)},%
},%
{%
doc name = vectorpoynting,%
- doc parameter = \marg{\ensuremath{c_1,\dots,c_n}},%
+ doc parameter = \marg{\( c_1,\dots,c_n \)},%
},%
}%
\end{docCommands}
@@ -1053,11 +1104,11 @@
{%
doc new = 2021-02-24,%
doc name = torquevector,%
- doc parameter = \marg{\ensuremath{c_1,\dots,c_n}},%
+ doc parameter = \marg{\( c_1,\dots,c_n \)},%
},%
{%
doc name = vectortorque,%
- doc parameter = \marg{\ensuremath{c_1,\dots,c_n}},%
+ doc parameter = \marg{\( c_1,\dots,c_n \)},%
},%
}%
\end{docCommands}
@@ -1071,12 +1122,17 @@
{%
doc new = 2021-02-24,%
doc name = velocityvector,%
- doc parameter = \marg{\ensuremath{c_1,\dots,c_n}},%
+ doc parameter = \marg{\( c_1,\dots,c_n \)},%
},%
{%
doc name = vectorvelocity,%
- doc parameter = \marg{\ensuremath{c_1,\dots,c_n}},%
+ doc parameter = \marg{\( c_1,\dots,c_n \)},%
},%
+ }%
+\end{docCommands}
+\checkquantity{velocity}
+\begin{docCommands}
+ {%
{%
doc name = velocityc,%
doc parameter = \marg{magnitude},%
@@ -1084,15 +1140,14 @@
{%
doc new = 2021-02-24,%
doc name = velocitycvector,%
- doc parameter = \marg{\ensuremath{c_1,\dots,c_n}},%
+ doc parameter = \marg{\( c_1,\dots,c_n \)},%
},%
{%
doc name = vectorvelocityc,%
- doc parameter = \marg{\ensuremath{c_1,\dots,c_n}},%
+ doc parameter = \marg{\( c_1,\dots,c_n \)},%
},%
}%
\end{docCommands}
-\checkquantity{velocity}
\checkquantity{velocityc}
\begin{docCommand}{volume}{\marg{magnitude}}
\end{docCommand}
@@ -1115,11 +1170,11 @@
{%
doc new = 2021-02-24,%
doc name = wavenumbervector,%
- doc parameter = \marg{\ensuremath{c_1,\dots,c_n}},%
+ doc parameter = \marg{\( c_1,\dots,c_n \)},%
},%
{%
doc name = vectorwavenumber,%
- doc parameter = \marg{\ensuremath{c_1,\dots,c_n}},%
+ doc parameter = \marg{\( c_1,\dots,c_n \)},%
},%
}%
\end{docCommands}
@@ -1148,7 +1203,7 @@
doc name = newscalarquantity,%
},%
{%
- doc new=2021-02-21,%
+ doc new = 2021-02-21,%
doc name = renewscalarquantity,%
},%
}%
@@ -1175,7 +1230,7 @@
doc name = newvectorquantity,%
},%
{%
- doc new=2021-02-21,%
+ doc new = 2021-02-21,%
doc name = renewvectorquantity,%
},%
}%
@@ -1349,10 +1404,10 @@
%\iffalse
%<*example>
%\fi
-\begin{docCommand}[doc updated = 2021-02-26]{checkconstant}{\marg{name}}
- Command to check and typeset the constant's name, base units, derived
- units, alternate units, mathematical symbol, approximate value, and
- precise value.
+\begin{docCommand}[doc updated = 2022-01-27]{checkconstant}{\marg{name}}
+ Command to check and typeset the constant's name, mathematical symbol,
+ approximate value, precise value, base units, derived units, and
+ alternate units.
\end{docCommand}
%\iffalse
%</example>
@@ -1360,14 +1415,14 @@
%
% \subsubsection{Predefined Physical Constants}
%
-% Every other defined physical constant can be treated similarly. Just
-% replace |oofpez| with the constant's name. Unfortunately, there is no
-% universal agreement on the names of every constant so don't fret if
-% the names used here vary from other sources. Here are all the physical
-% constants, with all their units, defined in \mandi.
-% The constants \refCom{coulombconstant} and \refCom{biotsavartconstant} are
-% defined as semantic aliases for, respectively, \refCom{oofpez} and
-% \refCom{mzofp}.
+% Every other defined physical constant can be treated similarly to
+% \refCom{oofpez}. Just replace |oofpez| with the constant's name.
+% Unfortunately, there is no universal agreement on the names of every
+% constant so don't fret if the names used here vary from other sources.
+% Here are all the physical constants, with all their units, defined in
+% \mandi. The constants \refCom{coulombconstant} and
+% \refCom{biotsavartconstant} are defined as semantic aliases for,
+% respectively, \refCom{oofpez} and \refCom{mzofp}.
%
%\iffalse
%<*example>
@@ -1504,7 +1559,7 @@
doc name = newphysicalconstant,%
},%
{%
- doc new=2021-02-21,%
+ doc new = 2021-02-21,%
doc name = renewphysicalconstant,%
},%
}%
@@ -1820,6 +1875,19 @@
%\iffalse
%<*example>
%\fi
+\begin{docCommand}[doc new = 2022-01-27,]{hbar}{}%
+ A better glyph for Planck's constant over \( 2\pi \).
+\end{docCommand}
+\begin{dispExample}
+ \( \hbar \)
+\end{dispExample}
+%\iffalse
+%</example>
+%\fi
+%
+%\iffalse
+%<*example>
+%\fi
\begin{docCommands}[%
doc parameter = \marg{number},%
]%
@@ -1848,22 +1916,23 @@
%\iffalse
%<*example>
%\fi
-\begin{docCommand}{mivector}{%
- \oarg{delimiter}\marg{\ensuremath{c_1,\dots,c_n}}\oarg{units}
+\begin{docCommand}[doc updated = 2022-01-27]{mivector}{%
+ \oarg{delimiter}\marg{\( c_1,\dots,c_n \)}\oarg{units}
}%
Typesets a vector as either numeric or symbolic components with an
- optional unit (for numerical components only). There can be more
- than three components. The delimiter used in the list of components
- can be specified; the default is a comma. The notation mirrors that of
+ optional unit (for numerical components only). There must be more
+ than one component, and there can be more than three components.
+ The delimiter used in the list of components can be specified;
+ the default is a comma. The notation mirrors that of
\emph{Matter \& Interactions}.
\end{docCommand}
-\begin{dispExample*}{lefthand ratio=0.65}
- \( \mivector{p_0,p_1,p_2,p_3} \) \\
- \( \mivector{\gamma m v_x,\gamma m v_y,\gamma m v_z} \) \\
- \( \mivector{\frac{Q_1Q_2}{x^2},0,0} \) \\
- \( \mivector{-1,0,0} \) \\
- \( \mivector{-1,0,0}[\velocityonlyderivedunits] \) \\
- \( \mivector{-1,0,0}[\meter\per\second] \) \\
+\begin{dispExample*}{lefthand ratio = 0.70}
+ \( \mivector{p_0,p_1,p_2,p_3} \) \\
+ \( \mivector{\gamma mc,\gamma mv_x,\gamma mv_y,\gamma mv_z} \) \\
+ \( \mivector{\frac{Q_1Q_2}{x^2},0,0} \) \\
+ \( \mivector{-1,0,0} \) \\
+ \( \mivector{-1,0,0}[\velocityonlyderivedunits] \) \\
+ \( \mivector{-1,0,0}[\meter\per\second] \) \\
\( \velocity{\mivector{-1,0,0}} \)
\end{dispExample*}
%\iffalse
@@ -1883,11 +1952,13 @@
% |\makeatother|. This simplifies defining internal commands (with |@|
% in the name) that are not for the user to know about.
%
+% \changes{v3.1.0}{2022-01-27}
+% {\linktoplace{sec:mandipkg}{mandi} Code formatted for better readability}
% \begin{macrocode}
-\def\mandi@version{3.0.0}
-\def\mandi@date{2021-08-22}
+\def\mandi@version{3.1.0}
+\def\mandi@date{2022-01-27}
\NeedsTeXFormat{LaTeX2e}[2020-02-02]
-\DeclareRelease{v3.0.0}{2021-08-22}{mandi.sty}
+\DeclareRelease{v3.1.0}{2022-01-27}{mandi.sty}
\DeclareCurrentRelease{v\mandi@version}{\mandi@date}
\ProvidesPackage{mandi}
[\mandi@date\space v\mandi@version\space Macros for physical quantities]
@@ -1902,16 +1973,24 @@
% Load third party packages, documenting why each one is needed.
%
% \begin{macrocode}
-\RequirePackage{pgfopts} % needed for key-value interface
-\RequirePackage{array} % needed for \checkquantity and \checkconstant
-\RequirePackage{iftex} % needed for requiring LuaLaTeX
-\RequirePackage{unicode-math} % needed for Unicode support
-\RequireLuaTeX % require this engine
+\RequirePackage{pgfopts} % needed for key-value interface
+\RequirePackage{array} % needed for \checkquantity and \checkconstant
+\RequirePackage{iftex} % needed for requiring LuaLaTeX
+\RequirePackage{unicode-math} % needed for Unicode support
+% \end{macrocode}
+%
+% \changes{v3.1.0}{2022-01-27}
+% {\linktoplace{sec:mandipkg}{mandi} \pkg{xparse} is loaded for older formats}
+% \begin{macrocode}
+\IfFormatAtLeastTF {2020-10-01} % load xparse if necessary
+ {}%
+ {\RequirePackage{xparse}}%
+\RequireLuaTeX % require this engine
% \end{macrocode}
%
% Parts of the unit engine have been rewritten with
% \href{https://www.ctan.org/pkg/xparse}{\pkg{xparse}} for both clarity
-% and power. Note that \pkg{xparse} is now part of the \LaTeX\ kernel.
+% and power. Note that \pkg{xparse} is now part of the \LaTeXe\ kernel.
% Other parts have been rewriten in
% \href{https://www.ctan.org/pkg/expl}{\pkg{expl}} with a look to the
% future.
@@ -1981,6 +2060,8 @@
% First, define the keys. The key handlers require certain commands defined
% by the unit engine.
%
+% \changes{v3.1.0}{2022-01-27}
+% {\linktoplace{sec:mandipkg}{mandi} Unknown package options handled safely}
% \begin{macrocode}
\newif\ifusingpreciseconstants
\pgfkeys{%
@@ -1995,6 +2076,10 @@
units/alternate/.style={/mandi/options/buffered@units=alternate},%
units/base/.style={/mandi/options/buffered@units=base},%
units/derived/.style={/mandi/options/buffered@units=derived},%
+ .unknown/.code={%
+ \typeout{}%
+ \typeout{mandi: You used unknown option '\pgfkeyscurrentname'.}%
+ },%
}%
% \end{macrocode}
%
@@ -2037,14 +2122,16 @@
% when called with new options. A new banner is written to the console.
%
% \begin{macrocode}
-\NewDocumentCommand{\mandisetup}{ m }{%
- \IfValueT{#1}{%
- \pgfqkeys{/mandi/options}{#1}
- \typeout{}%
- \typeout{mandi: mandisetup options...}
- \mandi@do@setup
+\NewDocumentCommand{\mandisetup}{ m }%
+ {%
+ \IfValueT{#1}%
+ {%
+ \pgfqkeys{/mandi/options}{#1}
+ \typeout{}%
+ \typeout{mandi: mandisetup options...}
+ \mandi@do@setup
+ }%
}%
-}%
% \end{macrocode}
%
% Define units and related constructs to be used with the unit engine.
@@ -2053,6 +2140,8 @@
% \href{https://ctan.org/pkg/siunits}{\pkg{SIunits}} package.
% We make use of |\symup{...}| from the \pkg{unicode-math} package.
%
+% \changes{v3.1.0}{2022-01-27}
+% {\linktoplace{sec:mandipkg}{mandi} Added a negative space to \refCom{lightspeed}}
% \begin{macrocode}
\NewDocumentCommand{\per}{}{/}
\NewDocumentCommand{\usk}{}{\cdot}
@@ -2072,7 +2161,7 @@
\NewDocumentCommand{\kev}{}{\kiloelectronvolt}
\NewDocumentCommand{\kiloelectronvolt}{}{\symup{keV}}
\NewDocumentCommand{\kilogram}{}{\symup{kg}}
-\NewDocumentCommand{\lightspeed}{}{\symup{c}}
+\NewDocumentCommand{\lightspeed}{}{\!\symup{c}}
\NewDocumentCommand{\megaelectronvolt}{}{\symup{MeV}}
\NewDocumentCommand{\meter}{}{\symup{m}}
\NewDocumentCommand{\metre}{}{\meter}
@@ -2102,23 +2191,25 @@
\NewDocumentCommand{\xtento}{ m }{\times\tento{#1}}
% \end{macrocode}
%
+% \changes{v3.1.0}{2022-01-27}
+% {\linktoplace{sec:mandipkg}{mandi} \LaTeX3 code now conforms to formatting standards}
% \begin{macrocode}
\ExplSyntaxOn
-\cs_new:Npn \mandi_newscalarquantity #1#2#3#4
-{%
- \cs_new:cpn {#1} ##1 {\unit{##1}{\mandi@selectunits{#2}{#3}{#4}}}%
- \cs_new:cpn {#1value} ##1 {##1}%
- \cs_new:cpn {#1baseunits} ##1 {\unit{##1}{\mandi@selectbaseunits{#2}{#3}{#4}}}%
- \cs_new:cpn {#1derivedunits} ##1 {\unit{##1}{\mandi@selectderivedunits{#2}{#3}{#4}}}%
- \cs_new:cpn {#1alternateunits} ##1 {\unit{##1}{\mandi@selectalternateunits{#2}{#3}{#4}}}%
- \cs_new:cpn {#1onlybaseunits} {\mandi@selectbaseunits{#2}{#3}{#4}}%
- \cs_new:cpn {#1onlyderivedunits} {\mandi@selectderivedunits{#2}{#3}{#4}}%
- \cs_new:cpn {#1onlyalternateunits} {\mandi@selectalternateunits{#2}{#3}{#4}}%
-}%
-\NewDocumentCommand{\newscalarquantity}{ m m O{#2} O{#2} }%
-{%
- \mandi_newscalarquantity { #1 }{ #2 }{ #3 }{ #4 }%
-}%
+\cs_new:Npn \__mandi_newscalarquantity:nnnn #1#2#3#4
+ {
+ \cs_new:cpn {#1} ##1 {\unit{##1}{\mandi@selectunits{#2}{#3}{#4}}}
+ \cs_new:cpn {#1value} ##1 {##1}
+ \cs_new:cpn {#1baseunits} ##1 {\unit{##1}{\mandi@selectbaseunits{#2}{#3}{#4}}}
+ \cs_new:cpn {#1derivedunits} ##1 {\unit{##1}{\mandi@selectderivedunits{#2}{#3}{#4}}}
+ \cs_new:cpn {#1alternateunits} ##1 {\unit{##1}{\mandi@selectalternateunits{#2}{#3}{#4}}}
+ \cs_new:cpn {#1onlybaseunits} {\mandi@selectbaseunits{#2}{#3}{#4}}
+ \cs_new:cpn {#1onlyderivedunits} {\mandi@selectderivedunits{#2}{#3}{#4}}
+ \cs_new:cpn {#1onlyalternateunits} {\mandi@selectalternateunits{#2}{#3}{#4}}
+ }
+\NewDocumentCommand{\newscalarquantity}{ m m O{#2} O{#2} }
+ {
+ \__mandi_newscalarquantity:nnnn { #1 }{ #2 }{ #3 }{ #4 }
+ }
\ExplSyntaxOff
% \end{macrocode}
%
@@ -2126,21 +2217,21 @@
%
% \begin{macrocode}
\ExplSyntaxOn
-\cs_new:Npn \mandi_renewscalarquantity #1#2#3#4
-{%
- \cs_set:cpn {#1} ##1 {\unit{##1}{\mandi@selectunits{#2}{#3}{#4}}}%
- \cs_set:cpn {#1value} ##1 {##1}%
- \cs_set:cpn {#1baseunits} ##1 {\unit{##1}{\mandi@selectbaseunits{#2}{#3}{#4}}}%
- \cs_set:cpn {#1derivedunits} ##1 {\unit{##1}{\mandi@selectderivedunits{#2}{#3}{#4}}}%
- \cs_set:cpn {#1alternateunits} ##1 {\unit{##1}{\mandi@selectalternateunits{#2}{#3}{#4}}}%
- \cs_set:cpn {#1onlybaseunits} {\mandi@selectbaseunits{#2}{#3}{#4}}%
- \cs_set:cpn {#1onlyderivedunits} {\mandi@selectderivedunits{#2}{#3}{#4}}%
- \cs_set:cpn {#1onlyalternateunits} {\mandi@selectalternateunits{#2}{#3}{#4}}%
-}%
-\NewDocumentCommand{\renewscalarquantity}{ m m O{#2} O{#2} }%
-{%
- \mandi_renewscalarquantity { #1 }{ #2 }{ #3 }{ #4 }%
-}%
+\cs_new:Npn \__mandi_renewscalarquantity:nnnn #1#2#3#4
+ {
+ \cs_set:cpn {#1} ##1 {\unit{##1}{\mandi@selectunits{#2}{#3}{#4}}}
+ \cs_set:cpn {#1value} ##1 {##1}
+ \cs_set:cpn {#1baseunits} ##1 {\unit{##1}{\mandi@selectbaseunits{#2}{#3}{#4}}}
+ \cs_set:cpn {#1derivedunits} ##1 {\unit{##1}{\mandi@selectderivedunits{#2}{#3}{#4}}}
+ \cs_set:cpn {#1alternateunits} ##1 {\unit{##1}{\mandi@selectalternateunits{#2}{#3}{#4}}}
+ \cs_set:cpn {#1onlybaseunits} {\mandi@selectbaseunits{#2}{#3}{#4}}
+ \cs_set:cpn {#1onlyderivedunits} {\mandi@selectderivedunits{#2}{#3}{#4}}
+ \cs_set:cpn {#1onlyalternateunits} {\mandi@selectalternateunits{#2}{#3}{#4}}
+ }
+\NewDocumentCommand{\renewscalarquantity}{ m m O{#2} O{#2} }
+ {
+ \__mandi_renewscalarquantity:nnnn { #1 }{ #2 }{ #3 }{ #4 }
+ }
\ExplSyntaxOff
% \end{macrocode}
%
@@ -2148,30 +2239,30 @@
%
% \begin{macrocode}
\ExplSyntaxOn
-\cs_new:Npn \mandi_newvectorquantity #1#2#3#4
-{%
- \mandi_newscalarquantity { #1 }{ #2 }{ #3 }{ #4 }%
- \cs_new:cpn {vector#1} ##1 {\unit{\mivector{##1}}{\mandi@selectunits{#2}{#3}{#4}}}%
- \cs_new:cpn {#1vector} ##1 {\unit{\mivector{##1}}{\mandi@selectunits{#2}{#3}{#4}}}%
- \cs_new:cpn {vector#1value} ##1 {\mivector{##1}}%
- \cs_new:cpn {#1vectorvalue} ##1 {\mivector{##1}}%
- \cs_new:cpn {vector#1baseunits} ##1 {\unit{\mivector{##1}}{\mandi@selectbaseunits{#2}{#3}{#4}}}%
- \cs_new:cpn {#1vectorbaseunits} ##1 {\unit{\mivector{##1}}{\mandi@selectbaseunits{#2}{#3}{#4}}}%
- \cs_new:cpn {vector#1derivedunits} ##1 {\unit{\mivector{##1}}{\mandi@selectderivedunits{#2}{#3}{#4}}}%
- \cs_new:cpn {#1vectorderivedunits} ##1 {\unit{\mivector{##1}}{\mandi@selectderivedunits{#2}{#3}{#4}}}%
- \cs_new:cpn {vector#1alternateunits} ##1 {\unit{\mivector{##1}}{\mandi@selectalternateunits{#2}{#3}{#4}}}%
- \cs_new:cpn {#1vectoralternateunits} ##1 {\unit{\mivector{##1}}{\mandi@selectalternateunits{#2}{#3}{#4}}}%
- \cs_new:cpn {vector#1onlybaseunits} {\mandi@selectbaseunits{#2}{#3}{#4}}%
- \cs_new:cpn {#1vectoronlybaseunits} {\mandi@selectbaseunits{#2}{#3}{#4}}%
- \cs_new:cpn {vector#1onlyderivedunits} {\mandi@selectderivedunits{#2}{#3}{#4}}%
- \cs_new:cpn {#1vectoronlyderivedunits} {\mandi@selectderivedunits{#2}{#3}{#4}}%
- \cs_new:cpn {vector#1onlyalternateunits} {\mandi@selectalternateunits{#2}{#3}{#4}}%
- \cs_new:cpn {#1vectoronlyalternateunits} {\mandi@selectalternateunits{#2}{#3}{#4}}%
-}%
-\NewDocumentCommand{\newvectorquantity}{ m m O{#2} O{#2} }%
-{%
- \mandi_newvectorquantity { #1 }{ #2 }{ #3 }{ #4 }%
-}%
+\cs_new:Npn \__mandi_newvectorquantity:nnnn #1#2#3#4
+ {
+ \__mandi_newscalarquantity:nnnn { #1 }{ #2 }{ #3 }{ #4 }
+ \cs_new:cpn {vector#1} ##1 {\unit{\mivector{##1}}{\mandi@selectunits{#2}{#3}{#4}}}
+ \cs_new:cpn {#1vector} ##1 {\unit{\mivector{##1}}{\mandi@selectunits{#2}{#3}{#4}}}
+ \cs_new:cpn {vector#1value} ##1 {\mivector{##1}}
+ \cs_new:cpn {#1vectorvalue} ##1 {\mivector{##1}}
+ \cs_new:cpn {vector#1baseunits} ##1 {\unit{\mivector{##1}}{\mandi@selectbaseunits{#2}{#3}{#4}}}
+ \cs_new:cpn {#1vectorbaseunits} ##1 {\unit{\mivector{##1}}{\mandi@selectbaseunits{#2}{#3}{#4}}}
+ \cs_new:cpn {vector#1derivedunits} ##1 {\unit{\mivector{##1}}{\mandi@selectderivedunits{#2}{#3}{#4}}}
+ \cs_new:cpn {#1vectorderivedunits} ##1 {\unit{\mivector{##1}}{\mandi@selectderivedunits{#2}{#3}{#4}}}
+ \cs_new:cpn {vector#1alternateunits} ##1 {\unit{\mivector{##1}}{\mandi@selectalternateunits{#2}{#3}{#4}}}
+ \cs_new:cpn {#1vectoralternateunits} ##1 {\unit{\mivector{##1}}{\mandi@selectalternateunits{#2}{#3}{#4}}}
+ \cs_new:cpn {vector#1onlybaseunits} {\mandi@selectbaseunits{#2}{#3}{#4}}
+ \cs_new:cpn {#1vectoronlybaseunits} {\mandi@selectbaseunits{#2}{#3}{#4}}
+ \cs_new:cpn {vector#1onlyderivedunits} {\mandi@selectderivedunits{#2}{#3}{#4}}
+ \cs_new:cpn {#1vectoronlyderivedunits} {\mandi@selectderivedunits{#2}{#3}{#4}}
+ \cs_new:cpn {vector#1onlyalternateunits} {\mandi@selectalternateunits{#2}{#3}{#4}}
+ \cs_new:cpn {#1vectoronlyalternateunits} {\mandi@selectalternateunits{#2}{#3}{#4}}
+ }
+\NewDocumentCommand{\newvectorquantity}{ m m O{#2} O{#2} }
+ {
+ \__mandi_newvectorquantity:nnnn { #1 }{ #2 }{ #3 }{ #4 }
+ }
\ExplSyntaxOff
% \end{macrocode}
%
@@ -2179,30 +2270,30 @@
%
% \begin{macrocode}
\ExplSyntaxOn
-\cs_new:Npn \mandi_renewvectorquantity #1#2#3#4
-{%
- \mandi_renewscalarquantity { #1 }{ #2 }{ #3 }{ #4 }%
- \cs_set:cpn {vector#1} ##1 {\unit{\mivector{##1}}{\mandi@selectunits{#2}{#3}{#4}}}%
- \cs_set:cpn {#1vector} ##1 {\unit{\mivector{##1}}{\mandi@selectunits{#2}{#3}{#4}}}%
- \cs_set:cpn {vector#1value} ##1 {\mivector{##1}}%
- \cs_set:cpn {#1vectorvalue} ##1 {\mivector{##1}}%
- \cs_set:cpn {vector#1baseunits} ##1 {\unit{\mivector{##1}}{\mandi@selectbaseunits{#2}{#3}{#4}}}%
- \cs_set:cpn {#1vectorbaseunits} ##1 {\unit{\mivector{##1}}{\mandi@selectbaseunits{#2}{#3}{#4}}}%
- \cs_set:cpn {vector#1derivedunits} ##1 {\unit{\mivector{##1}}{\mandi@selectderivedunits{#2}{#3}{#4}}}%
- \cs_set:cpn {#1vectorderivedunits} ##1 {\unit{\mivector{##1}}{\mandi@selectderivedunits{#2}{#3}{#4}}}%
- \cs_set:cpn {vector#1alternateunits} ##1 {\unit{\mivector{##1}}{\mandi@selectalternateunits{#2}{#3}{#4}}}%
- \cs_set:cpn {#1vectoralternateunits} ##1 {\unit{\mivector{##1}}{\mandi@selectalternateunits{#2}{#3}{#4}}}%
- \cs_set:cpn {vector#1onlybaseunits} {\mandi@selectbaseunits{#2}{#3}{#4}}%
- \cs_set:cpn {#1vectoronlybaseunits} {\mandi@selectbaseunits{#2}{#3}{#4}}%
- \cs_set:cpn {vector#1onlyderivedunits} {\mandi@selectderivedunits{#2}{#3}{#4}}%
- \cs_set:cpn {#1vectoronlyderivedunits} {\mandi@selectderivedunits{#2}{#3}{#4}}%
- \cs_set:cpn {vector#1onlyalternateunits} {\mandi@selectalternateunits{#2}{#3}{#4}}%
- \cs_set:cpn {#1vectoronlyalternateunits} {\mandi@selectalternateunits{#2}{#3}{#4}}%
-}%
-\NewDocumentCommand{\renewvectorquantity}{ m m O{#2} O{#2} }%
-{%
- \mandi_renewvectorquantity { #1 }{ #2 }{ #3 }{ #4 }%
-}%
+\cs_new:Npn \__mandi_renewvectorquantity:nnnn #1#2#3#4
+ {
+ \__mandi_renewscalarquantity:nnnn { #1 }{ #2 }{ #3 }{ #4 }
+ \cs_set:cpn {vector#1} ##1 {\unit{\mivector{##1}}{\mandi@selectunits{#2}{#3}{#4}}}
+ \cs_set:cpn {#1vector} ##1 {\unit{\mivector{##1}}{\mandi@selectunits{#2}{#3}{#4}}}
+ \cs_set:cpn {vector#1value} ##1 {\mivector{##1}}
+ \cs_set:cpn {#1vectorvalue} ##1 {\mivector{##1}}
+ \cs_set:cpn {vector#1baseunits} ##1 {\unit{\mivector{##1}}{\mandi@selectbaseunits{#2}{#3}{#4}}}
+ \cs_set:cpn {#1vectorbaseunits} ##1 {\unit{\mivector{##1}}{\mandi@selectbaseunits{#2}{#3}{#4}}}
+ \cs_set:cpn {vector#1derivedunits} ##1 {\unit{\mivector{##1}}{\mandi@selectderivedunits{#2}{#3}{#4}}}
+ \cs_set:cpn {#1vectorderivedunits} ##1 {\unit{\mivector{##1}}{\mandi@selectderivedunits{#2}{#3}{#4}}}
+ \cs_set:cpn {vector#1alternateunits} ##1 {\unit{\mivector{##1}}{\mandi@selectalternateunits{#2}{#3}{#4}}}
+ \cs_set:cpn {#1vectoralternateunits} ##1 {\unit{\mivector{##1}}{\mandi@selectalternateunits{#2}{#3}{#4}}}
+ \cs_set:cpn {vector#1onlybaseunits} {\mandi@selectbaseunits{#2}{#3}{#4}}
+ \cs_set:cpn {#1vectoronlybaseunits} {\mandi@selectbaseunits{#2}{#3}{#4}}
+ \cs_set:cpn {vector#1onlyderivedunits} {\mandi@selectderivedunits{#2}{#3}{#4}}
+ \cs_set:cpn {#1vectoronlyderivedunits} {\mandi@selectderivedunits{#2}{#3}{#4}}
+ \cs_set:cpn {vector#1onlyalternateunits} {\mandi@selectalternateunits{#2}{#3}{#4}}
+ \cs_set:cpn {#1vectoronlyalternateunits} {\mandi@selectalternateunits{#2}{#3}{#4}}
+ }
+\NewDocumentCommand{\renewvectorquantity}{ m m O{#2} O{#2} }
+ {
+ \__mandi_renewvectorquantity:nnnn { #1 }{ #2 }{ #3 }{ #4 }
+ }
\ExplSyntaxOff
% \end{macrocode}
%
@@ -2210,26 +2301,26 @@
%
% \begin{macrocode}
\ExplSyntaxOn
-\cs_new:Npn \mandi_newphysicalconstant #1#2#3#4#5#6#7
-{%
- \cs_new:cpn {#1} {\unit{\mandi@selectprecision{#3}{#4}}{\mandi@selectunits{#5}{#6}{#7}}}%
- \cs_new:cpn {#1mathsymbol} {#2}%
- \cs_new:cpn {#1approximatevalue} {#3}%
- \cs_new:cpn {#1precisevalue} {#4}%
- \cs_new:cpn {#1baseunits}
- {\unit{\mandi@selectprecision{#3}{#4}}{\mandi@selectbaseunits{#5}{#6}{#7}}}%
- \cs_new:cpn {#1derivedunits}
- {\unit{\mandi@selectprecision{#3}{#4}}{\mandi@selectderivedunits{#5}{#6}{#7}}}%
- \cs_new:cpn {#1alternateunits}
- {\unit{\mandi@selectprecision{#3}{#4}}{\mandi@selectalternateunits{#5}{#6}{#7}}}%
- \cs_new:cpn {#1onlybaseunits} {\mandi@selectbaseunits{#5}{#6}{#7}}%
- \cs_new:cpn {#1onlyderivedunits} {\mandi@selectderivedunits{#5}{#6}{#7}}%
- \cs_new:cpn {#1onlyalternateunits} {\mandi@selectalternateunits{#5}{#6}{#7}}%
-}%
-\NewDocumentCommand{\newphysicalconstant}{ m m m m m O{#5} O{#5} }%
-{%
- \mandi_newphysicalconstant { #1 }{ #2 }{ #3 }{ #4 }{ #5 }{ #6 }{ #7 }%
-}%
+\cs_new:Npn \__mandi_newphysicalconstant:nnnnnnn #1#2#3#4#5#6#7
+ {
+ \cs_new:cpn {#1} {\unit{\mandi@selectprecision{#3}{#4}}{\mandi@selectunits{#5}{#6}{#7}}}
+ \cs_new:cpn {#1mathsymbol} {#2}
+ \cs_new:cpn {#1approximatevalue} {#3}
+ \cs_new:cpn {#1precisevalue} {#4}
+ \cs_new:cpn {#1baseunits}
+ {\unit{\mandi@selectprecision{#3}{#4}}{\mandi@selectbaseunits{#5}{#6}{#7}}}
+ \cs_new:cpn {#1derivedunits}
+ {\unit{\mandi@selectprecision{#3}{#4}}{\mandi@selectderivedunits{#5}{#6}{#7}}}
+ \cs_new:cpn {#1alternateunits}
+ {\unit{\mandi@selectprecision{#3}{#4}}{\mandi@selectalternateunits{#5}{#6}{#7}}}
+ \cs_new:cpn {#1onlybaseunits} {\mandi@selectbaseunits{#5}{#6}{#7}}
+ \cs_new:cpn {#1onlyderivedunits} {\mandi@selectderivedunits{#5}{#6}{#7}}
+ \cs_new:cpn {#1onlyalternateunits} {\mandi@selectalternateunits{#5}{#6}{#7}}
+ }
+\NewDocumentCommand{\newphysicalconstant}{ m m m m m O{#5} O{#5} }
+ {
+ \__mandi_newphysicalconstant:nnnnnnn { #1 }{ #2 }{ #3 }{ #4 }{ #5 }{ #6 }{ #7 }
+ }
\ExplSyntaxOff
% \end{macrocode}
%
@@ -2237,26 +2328,26 @@
%
% \begin{macrocode}
\ExplSyntaxOn
-\cs_new:Npn \mandi_renewphysicalconstant #1#2#3#4#5#6#7
-{%
- \cs_set:cpn {#1} {\unit{\mandi@selectprecision{#3}{#4}}{\mandi@selectunits{#5}{#6}{#7}}}%
- \cs_set:cpn {#1mathsymbol} {#2}%
- \cs_set:cpn {#1approximatevalue} {#3}%
- \cs_set:cpn {#1precisevalue} {#4}%
- \cs_set:cpn {#1baseunits}
- {\unit{\mandi@selectprecision{#3}{#4}}{\mandi@selectbaseunits{#5}{#6}{#7}}}%
- \cs_set:cpn {#1derivedunits}
- {\unit{\mandi@selectprecision{#3}{#4}}{\mandi@selectderivedunits{#5}{#6}{#7}}}%
- \cs_set:cpn {#1alternateunits}
- {\unit{\mandi@selectprecision{#3}{#4}}{\mandi@selectalternateunits{#5}{#6}{#7}}}%
- \cs_set:cpn {#1onlybaseunits} {\mandi@selectbaseunits{#5}{#6}{#7}}%
- \cs_set:cpn {#1onlyderivedunits} {\mandi@selectderivedunits{#5}{#6}{#7}}%
- \cs_set:cpn {#1onlyalternateunits} {\mandi@selectalternateunits{#5}{#6}{#7}}%
-}%
-\NewDocumentCommand{\renewphysicalconstant}{ m m m m m O{#5} O{#5} }%
-{%
- \mandi_renewphysicalconstant { #1 }{ #2 }{ #3 }{ #4 }{ #5 }{ #6 }{ #7 }%
-}%
+\cs_new:Npn \__mandi_renewphysicalconstant:nnnnnnn #1#2#3#4#5#6#7
+ {
+ \cs_set:cpn {#1} {\unit{\mandi@selectprecision{#3}{#4}}{\mandi@selectunits{#5}{#6}{#7}}}
+ \cs_set:cpn {#1mathsymbol} {#2}
+ \cs_set:cpn {#1approximatevalue} {#3}
+ \cs_set:cpn {#1precisevalue} {#4}
+ \cs_set:cpn {#1baseunits}
+ {\unit{\mandi@selectprecision{#3}{#4}}{\mandi@selectbaseunits{#5}{#6}{#7}}}
+ \cs_set:cpn {#1derivedunits}
+ {\unit{\mandi@selectprecision{#3}{#4}}{\mandi@selectderivedunits{#5}{#6}{#7}}}
+ \cs_set:cpn {#1alternateunits}
+ {\unit{\mandi@selectprecision{#3}{#4}}{\mandi@selectalternateunits{#5}{#6}{#7}}}
+ \cs_set:cpn {#1onlybaseunits} {\mandi@selectbaseunits{#5}{#6}{#7}}
+ \cs_set:cpn {#1onlyderivedunits} {\mandi@selectderivedunits{#5}{#6}{#7}}
+ \cs_set:cpn {#1onlyalternateunits} {\mandi@selectalternateunits{#5}{#6}{#7}}
+ }
+\NewDocumentCommand{\renewphysicalconstant}{ m m m m m O{#5} O{#5} }
+ {
+ \__mandi_renewphysicalconstant:nnnnnnn { #1 }{ #2 }{ #3 }{ #4 }{ #5 }{ #6 }{ #7 }
+ }
\ExplSyntaxOff
% \end{macrocode}
%
@@ -2290,14 +2381,14 @@
% [\kilogram\usk\meter\tothetwo\per(\second\usk\radian)]%
% [\newton\usk\meter\usk\second\per\radian]%
%\else
- \newvectorquantity{angularimpulse}%
- {\kilogram\usk\meter\tothetwo\usk\second\inverse}%
- [\kilogram\usk\meter\tothetwo\per\second]% % also \joule\usk\second
- [\kilogram\usk\meter\tothetwo\per\second]% % also \newton\usk\meter\usk\second
- \newvectorquantity{angularmomentum}%
- {\kilogram\usk\meter\tothetwo\usk\second\inverse}%
- [\kilogram\usk\meter\tothetwo\per\second]% % also \joule\usk\second
- [\kilogram\usk\meter\tothetwo\per\second]% % also \newton\usk\meter\usk\second
+\newvectorquantity{angularimpulse}%
+ {\kilogram\usk\meter\tothetwo\usk\second\inverse}%
+ [\kilogram\usk\meter\tothetwo\per\second]% % also \joule\usk\second
+ [\kilogram\usk\meter\tothetwo\per\second]% % also \newton\usk\meter\usk\second
+\newvectorquantity{angularmomentum}%
+ {\kilogram\usk\meter\tothetwo\usk\second\inverse}%
+ [\kilogram\usk\meter\tothetwo\per\second]% % also \joule\usk\second
+ [\kilogram\usk\meter\tothetwo\per\second]% % also \newton\usk\meter\usk\second
%\fi
\newvectorquantity{angularvelocity}%
{\radian\usk\second\inverse}%
@@ -2439,6 +2530,13 @@
{\kilogram\usk\meter\inverse}%
[\kilogram\per\meter]%
[\kilogram\per\meter]%
+% \end{macrocode}
+%
+% \changes{v3.1.0}{2022-01-27}
+% {\linktoplace{sec:mandipkg}{mandi} Added \refCom{lorentzfactor}}
+% \begin{macrocode}
+\newscalarquantity{lorentzfactor}%
+ {}%
\newscalarquantity{luminousintensity}%
{\candela}%
\newscalarquantity{magneticcharge}%
@@ -2584,53 +2682,70 @@
[\newton\per\meter\tothetwo]%
% \end{macrocode}
%
+% We need a better glyph for Planck's constant over \( 2\pi \).
+%
+% \changes{v3.1.0}{2022-01-27}
+% {\linktoplace{sec:mandipkg}{mandi} Added \refCom{hbar}}
+% \begin{macrocode}
+\AtBeginDocument{%
+ \DeclareRobustCommand{\hbar}{{\mathpalette\hbar@\relax\symup{h}}}%
+}%
+\newcommand*{\hbar@}[2]{%
+ \makebox[0pt][l]{\raisebox{-0.07\height}{\(\m@th#1\mkern-2mu\mathchar"AF\)}}%
+ % optional line to make the bar thicker; must use -0.11
+ \makebox[0pt][l]{\raisebox{-0.11\height}{\(\m@th#1\mkern-2mu\mathchar"AF\)}}%
+}%
+% \end{macrocode}
+%
% Define physical constants for introductory physics, again alphabetically
% for convenience.
%
+% \changes{v3.1.0}{2022-01-27}
+% {\linktoplace{sec:mandipkg}{mandi} Constants' values now use only \cs{times}}
% \begin{macrocode}
\newphysicalconstant{avogadro}%
{\symup{N_A}}%
- {6\timestento{23}}{6.02214076\timestento{23}}% % exact 2019 value
+ {6\times10^{23}}{6.02214076\times10^{23}}% % exact 2019 value
{\mole\inverse}%
[\per\mole]%
[\per\mole]%
\newphysicalconstant{biotsavartconstant}% % alias for \mzofp
{\symup{\frac{\mu_o}{4\pi}}}%
- {\tento{-7}}{\tento{-7}}%
+ {10^{-7}}{10^{-7}}%
{\kilogram\usk\meter\usk\ampere\totheinversetwo\usk\second\totheinversetwo}%
[\henry\per\meter]%
[\tesla\usk\meter\per\ampere]%
\newphysicalconstant{bohrradius}%
{\symup{a_o}}%
- {5.3\timestento{-11}}{5.29177210903\timestento{-11}}%
+ {5.3\times10^{-11}}{5.29177210903\times10^{-11}}%
{\meter}%
\newphysicalconstant{boltzmann}%
{\symup{k_B}}%
- {1.4\timestento{-23}}{1.380649\timestento{-23}}% % exact 2019 value
+ {1.4\times10^{-23}}{1.380649\times10^{-23}}% % exact 2019 value
{\kilogram\usk\meter\tothetwo\usk\second\totheinversetwo\usk\kelvin\inverse}%
[\joule\per\kelvin]%
[\joule\per\kelvin]%
\newphysicalconstant{coulombconstant}% % alias for \oofpez
{\symup{\frac{1}{4\pi\epsilon_o}}}%
- {9\timestento{9}}{8.9875517923\timestento{9}}%
+ {9\times10^{9}}{8.9875517923\times10^{9}}%
{\kilogram\usk\meter\tothethree\usk\ampere\totheinversetwo\usk\second\totheinversefour}%
[\meter\per\farad]%
[\newton\usk\meter\tothetwo\per\coulomb\tothetwo]%
\newphysicalconstant{earthmass}%
{\symup{M_{Earth}}}%
- {6.0\timestento{24}}{5.9722\timestento{24}}%
+ {6.0\times10^{24}}{5.9722\times10^{24}}%
{\kilogram}%
\newphysicalconstant{earthmoondistance}%
{\symup{d_{EM}}}%
- {3.8\timestento{8}}{3.81550\timestento{8}}%
+ {3.8\times10^{8}}{3.81550\times10^{8}}%
{\meter}%
\newphysicalconstant{earthradius}%
{\symup{R_{Earth}}}%
- {6.4\timestento{6}}{6.3781\timestento{6}}%
+ {6.4\times10^{6}}{6.3781\times10^{6}}%
{\meter}%
\newphysicalconstant{earthsundistance}%
{\symup{d_{ES}}}%
- {1.5\timestento{11}}{1.496\timestento{11}}%
+ {1.5\times10^{11}}{1.496\times10^{11}}%
{\meter}%
\newphysicalconstant{electroncharge}%
{\symup{q_e}}%
@@ -2646,77 +2761,76 @@
[\coulomb]%
\newphysicalconstant{electronmass}%
{\symup{m_e}}%
- {9.1\timestento{-31}}{9.1093837015\timestento{-31}}%
+ {9.1\times10^{-31}}{9.1093837015\times10^{-31}}%
{\kilogram}%
\newphysicalconstant{elementarycharge}%
{\symup{e}}%
- {1.6\timestento{-19}}{1.602176634\timestento{-19}}% % exact 2019 value
+ {1.6\times10^{-19}}{1.602176634\times10^{-19}}% % exact 2019 value
{\ampere\usk\second}%
[\coulomb]%
[\coulomb]%
\newphysicalconstant{finestructure}%
{\symup{\alpha}}%
- {\frac{1}{137}}{7.2973525693\timestento{-3}}%
+ {\frac{1}{137}}{7.2973525693\times10^{-3}}%
{}%
\newphysicalconstant{hydrogenmass}%
{\symup{m_H}}%
- {1.7\timestento{-27}}{1.6737236\timestento{-27}}%
+ {1.7\times10^{-27}}{1.6737236\times10^{-27}}%
{\kilogram}%
\newphysicalconstant{moonearthdistance}%
{\symup{d_{ME}}}%
- {3.8\timestento{8}}{3.81550\timestento{8}}%
+ {3.8\times10^{8}}{3.81550\times10^{8}}%
{\meter}%
\newphysicalconstant{moonmass}%
{\symup{M_{Moon}}}%
- {7.3\timestento{22}}{7.342\timestento{22}}%
+ {7.3\times10^{22}}{7.342\times10^{22}}%
{\kilogram}%
\newphysicalconstant{moonradius}%
{\symup{R_{Moon}}}%
- {1.7\timestento{6}}{1.7371\timestento{6}}%
+ {1.7\times10^{6}}{1.7371\times10^{6}}%
{\meter}%
\newphysicalconstant{mzofp}%
{\symup{\frac{\mu_o}{4\pi}}}%
- {\tento{-7}}{\tento{-7}}%
+ {10^{-7}}{10^{-7}}%
{\kilogram\usk\meter\usk\ampere\totheinversetwo\usk\second\totheinversetwo}%
[\henry\per\meter]%
[\tesla\usk\meter\per\ampere]%
\newphysicalconstant{neutronmass}%
{\symup{m_n}}%
- {1.7\timestento{-27}}{1.67492749804\timestento{-27}}%
+ {1.7\times10^{-27}}{1.67492749804\times10^{-27}}%
{\kilogram}%
\newphysicalconstant{oofpez}%
{\symup{\frac{1}{4\pi\epsilon_o}}}%
- {9\timestento{9}}{8.9875517923\timestento{9}}%
+ {9\times10^{9}}{8.9875517923\times10^{9}}%
{\kilogram\usk\meter\tothethree\usk\ampere\totheinversetwo\usk\second\totheinversefour}%
[\meter\per\farad]%
[\newton\usk\meter\tothetwo\per\coulomb\tothetwo]%
\newphysicalconstant{oofpezcs}%
{\symup{\frac{1}{4\pi\epsilon_o c^2}}}%
- {\tento{-7}}{\tento{-7}}%
+ {10^{-7}}{10^{-7}}%
{\kilogram\usk\meter\usk\ampere\totheinversetwo\usk\second\totheinversetwo}%
[\tesla\usk\meter\tothetwo]%
[\newton\usk\second\tothetwo\per\coulomb\tothetwo]%
\newphysicalconstant{planck}%
{\symup{h}}%
- {6.6\timestento{-34}}{6.62607015\timestento{-34}}% % exact 2019 value
+ {6.6\times10^{-34}}{6.62607015\times10^{-34}}% % exact 2019 value
{\kilogram\usk\meter\tothetwo\usk\second\inverse}%
[\joule\usk\second]%
[\joule\usk\second]%
% \end{macrocode}
%
% See \url{https://tex.stackexchange.com/a/448565/218142}.
-%
%
% \begin{macrocode}
\newphysicalconstant{planckbar}%
- {\symup{\lower0.18ex\hbox{\mathchar"AF}\mkern-7mu h}}%
- {1.1\timestento{-34}}{1.054571817\timestento{-34}}%
+ {\hbar}%
+ {1.1\times10^{-34}}{1.054571817\times10^{-34}}%
{\kilogram\usk\meter\tothetwo\usk\second\inverse}%
[\joule\usk\second]%
[\joule\usk\second]
\newphysicalconstant{planckc}%
{\symup{hc}}%
- {2.0\timestento{-25}}{1.98644586\timestento{-25}}%
+ {2.0\times10^{-25}}{1.98644586\times10^{-25}}%
{\kilogram\usk\meter\tothethree\usk\second\totheinversetwo}%
[\joule\usk\meter]%
[\joule\usk\meter]%
@@ -2734,35 +2848,35 @@
[\coulomb]%
\newphysicalconstant{protonmass}%
{\symup{m_p}}%
- {1.7\timestento{-27}}{1.672621898\timestento{-27}}%
+ {1.7\times10^{-27}}{1.672621898\times10^{-27}}%
{\kilogram}%
\newphysicalconstant{rydberg}%
{\symup{R_{\infty}}}%
- {1.1\timestento{7}}{1.0973731568160\timestento{7}}%
+ {1.1\times10^{7}}{1.0973731568160\times10^{7}}%
{\meter\inverse}%
\newphysicalconstant{speedoflight}%
{\symup{c}}%
- {3\timestento{8}}{2.99792458\timestento{8}}% % exact value
+ {3\times10^{8}}{2.99792458\times10^{8}}% % exact value
{\meter\usk\second\inverse}%
[\meter\per\second]%
[\meter\per\second]
\newphysicalconstant{stefanboltzmann}%
{\symup{\sigma}}%
- {5.7\timestento{-8}}{5.670374\timestento{-8}}%
+ {5.7\times10^{-8}}{5.670374\times10^{-8}}%
{\kilogram\usk\second\totheinversethree\usk\kelvin\totheinversefour}%
[\watt\per\meter\tothetwo\usk\kelvin\tothefour]%
[\watt\per\meter\tothetwo\usk\kelvin\tothefour]
\newphysicalconstant{sunearthdistance}%
{\symup{d_{SE}}}%
- {1.5\timestento{11}}{1.496\timestento{11}}%
+ {1.5\times10^{11}}{1.496\times10^{11}}%
{\meter}%
\newphysicalconstant{sunmass}%
{\symup{M_{Sun}}}%
- {2.0\timestento{30}}{1.98855\timestento{30}}%
+ {2.0\times10^{30}}{1.98855\times10^{30}}%
{\kilogram}%
\newphysicalconstant{sunradius}%
{\symup{R_{Sun}}}%
- {7.0\timestento{8}}{6.957\timestento{8}}%
+ {7.0\times10^{8}}{6.957\times10^{8}}%
{\meter}%
\newphysicalconstant{surfacegravfield}%
{\symup{g}}%
@@ -2772,19 +2886,19 @@
[\newton\per\kilogram]%
\newphysicalconstant{universalgrav}%
{\symup{G}}%
- {6.7\timestento{-11}}{6.67430\timestento{-11}}%
+ {6.7\times10^{-11}}{6.67430\times10^{-11}}%
{\meter\tothethree\usk\kilogram\inverse\usk\second\totheinversetwo}%
[\newton\usk\meter\tothetwo\per\kilogram\tothetwo]% % also \joule\usk\meter\per\kilogram\tothetwo
[\newton\usk\meter\tothetwo\per\kilogram\tothetwo]%
\newphysicalconstant{vacuumpermeability}%
{\symup{\mu_o}}%
- {4\pi\timestento{-7}}{4\pi\timestento{-7}}% % as of 2018 no longer 4\pi\timestento{-7}
+ {4\pi\times10^{-7}}{4\pi\times10^{-7}}% % as of 2018 no longer 4\pi\times10^{-7}
{\kilogram\usk\meter\usk\ampere\totheinversetwo\usk\second\totheinversetwo}%
[\henry\per\meter]%
[\tesla\usk\meter\per\ampere]%
\newphysicalconstant{vacuumpermittivity}%
{\symup{\epsilon_o}}%
- {9\timestento{-12}}{8.854187817\timestento{-12}}%
+ {9\times10^{-12}}{8.854187817\times10^{-12}}%
{\ampere\tothetwo\usk\second\tothefour\usk\kilogram\inverse\usk\meter\totheinversethree}%
[\farad\per\meter]%
[\coulomb\tothetwo\per\newton\usk\meter\tothetwo]%
@@ -2793,94 +2907,84 @@
% Diagnostic commands to provide sanity checks on commands that
% represent physical quantities and constants.
%
+% \changes{v3.1.0}{2022-01-27}
+% {\linktoplace{sec:mandipkg}{mandi} Improved \refCom{checkquantity}}
+% \changes{v3.1.0}{2022-01-27}
+% {\linktoplace{sec:mandipkg}{mandi} Improved \refCom{checkconstant}}
% \begin{macrocode}
\ExplSyntaxOn
-\NewDocumentCommand{\checkquantity}{ m }%
-{%
- % Works for both scalar and vector quantities (without vector in the name!).
- \begin{center}
- \begin{tabular}{%
- >{\bfseries\small}
- p{0.5\linewidth}
- p{0.1\linewidth}
- p{0.1\linewidth}
- p{0.1\linewidth}
- }%
- name & & & \tabularnewline
- \ttfamily\footnotesize{\token_to_str:c {#1}} & & & \tabularnewline
- \end{tabular}~ % This nonbreaking space is important!
- \begin{tabular}{%
- >{\bfseries\small}p{0.25\linewidth}
- >{\bfseries\small}p{0.25\linewidth}
- >{\bfseries\small}p{0.25\linewidth}
- }%
- base & derived & alternate \tabularnewline
- \footnotesize{\( \use:c {#1onlybaseunits} \)} &
- \footnotesize{\( \use:c {#1onlyderivedunits} \)} &
- \footnotesize{\( \use:c {#1onlyalternateunits} \)}
- \end{tabular}
- \end{center}
-}%
-\NewDocumentCommand{\checkconstant}{ m }%
-{%
- \begin{center}
- \begin{tabular}{%
- >{\bfseries\small}
- p{0.5\linewidth}
- p{0.1\linewidth}
- p{0.1\linewidth}
- p{0.1\linewidth}
- }%
- name & & & \tabularnewline
- \ttfamily\footnotesize{\token_to_str:c {#1}} & & & \tabularnewline
- \end{tabular}~ % This nonbreaking space is important!
- \begin{tabular}{%
- >{\bfseries\small}p{0.25\linewidth}
- >{\bfseries\small}p{0.25\linewidth}
- >{\bfseries\small}p{0.25\linewidth}
- }%
- symbol & approximate & precise \tabularnewline
- \footnotesize{\( \use:c {#1mathsymbol} \)} &
- \footnotesize{\( \use:c {#1approximatevalue} \)} &
- \footnotesize{\( \use:c {#1precisevalue} \)}
- \end{tabular}~ % This nonbreaking space is important!
- \begin{tabular}{%
- >{\bfseries\small}p{0.25\linewidth}
- >{\bfseries\small}p{0.25\linewidth}
- >{\bfseries\small}p{0.25\linewidth}
- }%
- base & derived & alternate \tabularnewline
- \footnotesize{\( \use:c {#1onlybaseunits} \)} &
- \footnotesize{\( \use:c {#1onlyderivedunits} \)} &
- \footnotesize{\( \use:c {#1onlyalternateunits} \)}
- \end{tabular}
- \end{center}
-}%
+\NewDocumentCommand{\@aux}{ m }
+ {
+ \use:c { #1 }
+ }
+\NewDocumentCommand{\@auy}{ m }
+ {
+ \normalfont\ttfamily\token_to_str:c { #1 }
+ }
\ExplSyntaxOff
+\newcolumntype{M}{>{\(}p{0.25\linewidth}<{\)}}
+\NewDocumentCommand{\checkquantity}{ m }
+ {%
+ \begin{center}
+ \begin{tabular}{MMM}
+ \textbf{command} & \multicolumn{2}{l}{\@auy{#1}} \tabularnewline
+ \text{\textbf{base}} & \text{\textbf{derived}} & \text{\textbf{alternate}} \tabularnewline
+ \@aux{#1onlybaseunits} & \@aux{#1onlyderivedunits} & \@aux{#1onlyalternateunits} \tabularnewline
+ \end{tabular}
+ \end{center}
+ }%
+\NewDocumentCommand{\checkconstant}{ m }
+ {%
+ \begin{center}
+ \begin{tabular}{MMM}
+ \textbf{command} & \multicolumn{2}{l}{\@auy{#1}} \tabularnewline
+ \text{\textbf{symbol}} & \text{\textbf{approximate}} & \text{\textbf{precise}} \tabularnewline
+ \@aux{#1mathsymbol} & \@aux{#1approximatevalue} & \@aux{#1precisevalue} \tabularnewline
+ \text{\textbf{base}} & \text{\textbf{derived}} & \text{\textbf{alternate}} \tabularnewline
+ \@aux{#1onlybaseunits} & \@aux{#1onlyderivedunits} & \@aux{#1onlyalternateunits} \tabularnewline
+ \end{tabular}
+ \end{center}
+ }%
% \end{macrocode}
%
-% \refCom{mivector} is a workhorse command.
-% Orginal code provided by |@egreg|.\newline
+% \refCom{mivector} is a workhorse command.\newline
% See \url{https://tex.stackexchange.com/a/39054/218142}.
-%
%
+% \changes{v3.1.0}{2022-01-27}
+% {\linktoplace{sec:mandipkg}{mandi} \refCom{mivector} now
+% requires more than one component}
% \begin{macrocode}
\ExplSyntaxOn
-\NewDocumentCommand{\mivector}{ O{,} m o }%
- {%
- \mi_vector:nn { #1 } { #2 }%
- \IfValueT{#3}{\,{#3}}%
- }%
-\seq_new:N \l__mi_list_seq
-\cs_new_protected:Npn \mi_vector:nn #1 #2
-{%
- \ensuremath{%
- \seq_set_split:Nnn \l__mi_list_seq { , } { #2 }
- \int_compare:nF { \seq_count:N \l__mi_list_seq = 1 } { \left\langle }
- \seq_use:Nnnn \l__mi_list_seq { #1 } { #1 } { #1 }
- \int_compare:nF { \seq_count:N \l__mi_list_seq = 1 } { \right\rangle }
- }%
-}%
+\NewDocumentCommand{\mivector}{ O{,} m o }
+ {
+ \__mandi_vector:nn { #1 } { #2 }
+ \IfValueT{#3}{\,{#3}}
+ }
+\seq_new:N \l__mandi_list_seq
+\cs_new_protected:Npn \__mandi_vector:nn #1#2
+ {
+ \seq_set_split:Nnn \l__mandi_list_seq { , } { #2 }
+ \int_compare:nT { \seq_count:N \l__mandi_list_seq = 1 }
+ {
+ \msg_new:nnnn { mandi } { onecomponent }
+ {
+ More~than~one~component~expected. \iow_newline:
+ You~provided~one~component~to~a~command \iow_newline:
+ that~expects~a~vector.~Either~you~don't \iow_newline:
+ need~a~vector~here~or~you~didn't~supply \iow_newline:
+ all~the~components.
+ }
+ {
+ Decide~whether~or~not~you~really~need~a~vector~command~here. \iow_newline:
+ \msg_see_documentation_text:n { mandi }
+ }
+ \msg_fatal:nn { mandi } { onecomponent }
+
+ }
+ \left\langle
+ \seq_use:Nnnn \l__mandi_list_seq { #1 } { #1 } { #1 }
+ \right\rangle
+ }
\ExplSyntaxOff
% \end{macrocode}
% \restoregeometry
diff --git a/Master/texmf-dist/source/latex/mandi/mandi.ins b/Master/texmf-dist/source/latex/mandi/mandi.ins
index 522a62d88a4..45abce7e591 100644
--- a/Master/texmf-dist/source/latex/mandi/mandi.ins
+++ b/Master/texmf-dist/source/latex/mandi/mandi.ins
@@ -6,7 +6,7 @@
%%
%% mandi.dtx (with options: `install')
%%
-%% Copyright (C) 2021 by Paul J. Heafner <heafnerj@gmail.com>
+%% Copyright (C) 2021,2022 by Paul J. Heafner <heafnerj@gmail.com>
%% ---------------------------------------------------------------------------
%% 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
@@ -29,7 +29,7 @@
%% and includes the derived files mandi.sty
%% mandistudent.sty
%% mandiexp.sty
-%% vdemo.py
+%% vdemo.py (not needed)
%% ---------------------------------------------------------------------------
%%
\input docstrip.tex
@@ -38,7 +38,7 @@
\usedir{tex/latex/mandi}
\preamble
- Copyright (C) 2021 by Paul J. Heafner <heafnerj@gmail.com>
+ Copyright (C) 2021,2022 by Paul J. Heafner <heafnerj@gmail.com>
---------------------------------------------------------------------------
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
@@ -61,7 +61,7 @@
and includes the derived files mandi.sty
mandistudent.sty
mandiexp.sty
- vdemo.py
+ vdemo.py (not needed)
---------------------------------------------------------------------------
\endpreamble
@@ -82,7 +82,7 @@
\Msg{* 3. makeindex -s gind.ist -o mandi.ind mandi.idx *}
\Msg{* 4. makeindex -s gglo.ist -o mandi.gls mandi.glo *}
\Msg{* Move the *.sty files into a directory searched by TeX. *}
-\Msg{* The vdemo.py file is not needed. *}
+\Msg{* The vdemo.py file can be deleted. *}
\Msg{* *}
\Msg{*************************************************************}
\endbatchfile
diff --git a/Master/texmf-dist/source/latex/mandi/mandiexp.dtx b/Master/texmf-dist/source/latex/mandi/mandiexp.dtx
index 8871fe58414..507263bd63d 100644
--- a/Master/texmf-dist/source/latex/mandi/mandiexp.dtx
+++ b/Master/texmf-dist/source/latex/mandi/mandiexp.dtx
@@ -1,7 +1,7 @@
% \iffalse meta-comment
% !TEX program = lualatexmk
%
-% Copyright (C) 2021 by Paul J. Heafner <heafnerj@gmail.com>
+% Copyright (C) 2021,2022 by Paul J. Heafner <heafnerj@gmail.com>
% ---------------------------------------------------------------------------
% 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
@@ -65,7 +65,7 @@
%</driver>
% \fi
%
-% \CheckSum{215}
+% \CheckSum{225}
%
% \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
@@ -104,7 +104,7 @@
%\iffalse
%<*example>
%\fi
-\begin{dispListing*}{sidebyside=false,listing only}
+\begin{dispListing*}{sidebyside = false,listing only}
\usepackage{mandiexp}
\end{dispListing*}
%\iffalse
@@ -117,7 +117,7 @@
\begin{docCommand}{mandiexpversion}{}
Typesets the current version and build date.
\end{docCommand}
-\begin{dispExample*}{sidebyside=false}
+\begin{dispExample*}{sidebyside = false}
The version is \mandiexpversion\ and is a stable build.
\end{dispExample*}
%\iffalse
@@ -313,7 +313,7 @@
doc description = {update form, arrow vectors},%
},%
}%
- Variants of command for typesetting the angularmomentum principle.
+ Variants of command for typesetting the angular momentum principle.
Use starred variants to get arrow notation for vectors.
\end{docCommands}
\begin{dispExample}
@@ -339,10 +339,10 @@
%\iffalse
%<*example>
%\fi
-\begin{docCommand}[doc new=2021-02-13]{energyof}{\marg{label}\oarg{label}}
+\begin{docCommand}[doc new = 2021-02-13]{energyof}{\marg{label}\oarg{label}}
Generic symbol for the energy of some entity.
\end{docCommand}
-\begin{dispExample*}{lefthand ratio=0.6}
+\begin{dispExample*}{lefthand ratio = 0.6}
\( \energyof{\symup{electron}} \) \\
\( \energyof{\symup{electron}}[\symup{final}] \)
\end{dispExample*}
@@ -353,7 +353,7 @@
%\iffalse
%<*example>
%\fi
-\begin{docCommand}[doc new=2021-02-13]{systemenergy}{\oarg{label}}
+\begin{docCommand}[doc new = 2021-02-13]{systemenergy}{\oarg{label}}
Symbol for system energy.
\end{docCommand}
\begin{dispExample}
@@ -367,7 +367,7 @@
%\iffalse
%<*example>
%\fi
-\begin{docCommand}[doc new=2021-02-13]{particleenergy}{\oarg{label}}
+\begin{docCommand}[doc new = 2021-02-13]{particleenergy}{\oarg{label}}
Symbol for particle energy.
\end{docCommand}
\begin{dispExample}
@@ -381,7 +381,7 @@
%\iffalse
%<*example>
%\fi
-\begin{docCommand}[doc new=2021-02-13]{restenergy}{\oarg{label}}
+\begin{docCommand}[doc new = 2021-02-13]{restenergy}{\oarg{label}}
Symbol for rest energy.
\end{docCommand}
\begin{dispExample}
@@ -395,7 +395,7 @@
%\iffalse
%<*example>
%\fi
-\begin{docCommand}[doc new=2021-02-13]{internalenergy}{\oarg{label}}
+\begin{docCommand}[doc new = 2021-02-13]{internalenergy}{\oarg{label}}
Symbol for internal energy.
\end{docCommand}
\begin{dispExample}
@@ -409,7 +409,7 @@
%\iffalse
%<*example>
%\fi
-\begin{docCommand}[doc new=2021-02-13]{chemicalenergy}{\oarg{label}}
+\begin{docCommand}[doc new = 2021-02-13]{chemicalenergy}{\oarg{label}}
Symbol for chemical energy.
\end{docCommand}
\begin{dispExample}
@@ -423,7 +423,7 @@
%\iffalse
%<*example>
%\fi
-\begin{docCommand}[doc new=2021-02-13]{thermalenergy}{\oarg{label}}
+\begin{docCommand}[doc new = 2021-02-13]{thermalenergy}{\oarg{label}}
Symbol for thermal energy.
\end{docCommand}
\begin{dispExample}
@@ -437,7 +437,7 @@
%\iffalse
%<*example>
%\fi
-\begin{docCommand}[doc new=2021-02-13]{photonenergy}{\oarg{label}}
+\begin{docCommand}[doc new = 2021-02-13]{photonenergy}{\oarg{label}}
Symbol for photon energy.
\end{docCommand}
\begin{dispExample}
@@ -452,7 +452,7 @@
%<*example>
%\fi
\begin{docCommands}[%
- doc new=2021-02-13,%
+ doc new = 2021-02-13,%
doc parameter = \oarg{label},%
]%
{%
@@ -466,7 +466,7 @@
Symbol for translational kinetic energy.
The starred variant gives \(E\) notation.
\end{docCommands}
-\begin{dispExample*}{lefthand ratio=0.6}
+\begin{dispExample*}{lefthand ratio = 0.6}
\( \translationalkineticenergy \) \\
\( \translationalkineticenergy[\symup{initial}] \) \\
\( \translationalkineticenergy* \) \\
@@ -480,7 +480,7 @@
%<*example>
%\fi
\begin{docCommands}[%
- doc new=2021-02-13,%
+ doc new = 2021-02-13,%
doc parameter = \oarg{label},%
]%
{%
@@ -494,7 +494,7 @@
Symbol for rotational kinetic energy.
The starred variant gives \(E\) notation.
\end{docCommands}
-\begin{dispExample*}{lefthand ratio=0.6}
+\begin{dispExample*}{lefthand ratio = 0.6}
\( \rotationalkineticenergy \) \\
\( \rotationalkineticenergy[\symup{initial}] \) \\
\( \rotationalkineticenergy* \) \\
@@ -508,7 +508,7 @@
%<*example>
%\fi
\begin{docCommands}[%
- doc new=2021-02-13,%
+ doc new = 2021-02-13,%
doc parameter = \oarg{label},%
]%
{%
@@ -522,7 +522,7 @@
Symbol for vibrational kinetic energy.
The starred variant gives \(E\) notation.
\end{docCommands}
-\begin{dispExample*}{lefthand ratio=0.6}
+\begin{dispExample*}{lefthand ratio = 0.6}
\( \vibrationalkineticenergy \) \\
\( \vibrationalkineticenergy[\symup{initial}] \) \\
\( \vibrationalkineticenergy* \) \\
@@ -535,11 +535,11 @@
%\iffalse
%<*example>
%\fi
-\begin{docCommand}[doc new=2021-02-13]{gravitationalpotentialenergy}
+\begin{docCommand}[doc new = 2021-02-13]{gravitationalpotentialenergy}
{\oarg{label}}
Symbol for gravitational potential energy.
\end{docCommand}
-\begin{dispExample*}{lefthand ratio=0.6}
+\begin{dispExample*}{lefthand ratio = 0.6}
\( \gravitationalpotentialenergy \) \\
\( \gravitationalpotentialenergy[\symup{final}] \)
\end{dispExample*}
@@ -550,10 +550,10 @@
%\iffalse
%<*example>
%\fi
-\begin{docCommand}[doc new=2021-02-13]{electricpotentialenergy}{\oarg{label}}
+\begin{docCommand}[doc new = 2021-02-13]{electricpotentialenergy}{\oarg{label}}
Symbol for electric potential energy.
\end{docCommand}
-\begin{dispExample*}{lefthand ratio=0.6}
+\begin{dispExample*}{lefthand ratio = 0.6}
\( \electricpotentialenergy \) \\
\( \electricpotentialenergy[\symup{final}] \)
\end{dispExample*}
@@ -564,10 +564,10 @@
%\iffalse
%<*example>
%\fi
-\begin{docCommand}[doc new=2021-02-13]{springpotentialenergy}{\oarg{label}}
+\begin{docCommand}[doc new = 2021-02-13]{springpotentialenergy}{\oarg{label}}
Symbol for spring potential energy.
\end{docCommand}
-\begin{dispExample*}{lefthand ratio=0.6}
+\begin{dispExample*}{lefthand ratio = 0.6}
\( \springpotentialenergy \) \\
\( \springpotentialenergy[\symup{final}] \)
\end{dispExample*}
@@ -588,12 +588,16 @@
% |\makeatother|. This simplifies defining internal commands, with |@|
% in the name, that are not for the user to know about.
%
+% \changes{v3.1.0}{2022-01-27}
+% {\linktoplace{sec:mandiexppkg}{mandiexp} Version number works}
+% \changes{v3.1.0}{2022-01-27}
+% {\linktoplace{sec:mandiexppkg}{mandiexp} Code formatted for better readability}
% \begin{macrocode}
-\def\mandiexp@version{\mandi@version}
-\def\mandiexp@date{\mandi@date}
+\def\mandiexp@version{3.1.0}
+\def\mandiexp@date{2022-01-27}
\NeedsTeXFormat{LaTeX2e}[2020-02-02]
-\DeclareRelease{v3.0.0}{2021-08-22}{mandiexp.sty}
-\DeclareCurrentRelease{v\mandi@version}{\mandi@date}
+\DeclareRelease{v3.1.0}{2022-01-27}{mandiexp.sty}
+\DeclareCurrentRelease{v\mandiexp@version}{\mandiexp@date}
\ProvidesPackage{mandiexp}
[\mandiexp@date\space v\mandiexp@version\space Macros for Matter & Interactions]
% \end{macrocode}
@@ -606,7 +610,17 @@
%
% \begin{macrocode}
\RequirePackage{mandi}
+% \end{macrocode}
%
+% \changes{v3.1.0}{2022-01-27}
+% {\linktoplace{sec:mandiexppkg}{mandiexp} \pkg{xparse} is loaded for older formats}
+% \begin{macrocode}
+\IfFormatAtLeastTF {2020-10-01} % load xparse if necessary
+ {}%
+ {\RequirePackage{xparse}}%
+% \end{macrocode}
+%
+% \begin{macrocode}
\typeout{}%
\typeout{mandiexp: You are using mandiexp \mandiexpversion.}
\typeout{mandiexp: This package requires LuaLaTeX.}%
@@ -614,168 +628,301 @@
%
% Commands specific to Matter & Interactions
% The momentum principle
-\NewDocumentCommand{\lhsmomentumprinciple}{ s }{%
- \Delta
- \IfBooleanTF{#1}%
- {\vec*{p}}%
- {\vec{p}}%
- _{\symup{sys}}%
-}%
-\NewDocumentCommand{\rhsmomentumprinciple}{ s }{%
- \IfBooleanTF{#1}%
- {\vec*{F}}%
- {\vec{F}}%
- _{\symup{sys,net}}\,\Delta t%
-}%
-\NewDocumentCommand{\lhsmomentumprincipleupdate}{ s }{%
- \IfBooleanTF{#1}%
- {\vec*{p}}%
- {\vec{p}}%
- _{\symup{sys,final}}%
-}%
-\NewDocumentCommand{\rhsmomentumprincipleupdate}{ s }{%
- \IfBooleanTF{#1}%
- {\vec*{p}}%
- {\vec{p}}%
- _{\symup{sys,initial}}+%
- \IfBooleanTF{#1}%
- {\vec*{F}}%
- {\vec{F}}%
- _{\symup{sys,net}}\,\Delta t%
-}%
-\NewDocumentCommand{\momentumprinciple}{ s }{%
- \IfBooleanTF{#1}%
- {\lhsmomentumprinciple* = \rhsmomentumprinciple*}%
- {\lhsmomentumprinciple = \rhsmomentumprinciple}%
-}%
-\NewDocumentCommand{\momentumprincipleupdate}{ s }{%
- \IfBooleanTF{#1}%
- {\lhsmomentumprincipleupdate* = \rhsmomentumprincipleupdate*}%
- {\lhsmomentumprincipleupdate = \rhsmomentumprincipleupdate}%
-}%
+\NewDocumentCommand{\lhsmomentumprinciple}{ s }%
+ {%
+ \Delta
+ \IfBooleanTF{#1}%
+ {%
+ \vec*{p}
+ }%
+ {%
+ \vec{p}%
+ }%
+ \sb{\symup{sys}}%
+ }%
+\NewDocumentCommand{\rhsmomentumprinciple}{ s }%
+ {%
+ \IfBooleanTF{#1}%
+ {%
+ \vec*{F}%
+ }%
+ {%
+ \vec{F}%
+ }%
+ \sb{\symup{sys,net}}\,\Delta t%
+ }%
+\NewDocumentCommand{\lhsmomentumprincipleupdate}{ s }%
+ {%
+ \IfBooleanTF{#1}%
+ {%
+ \vec*{p}%
+ }%
+ {%
+ \vec{p}%
+ }%
+ \sb{\symup{sys,final}}%
+ }%
+\NewDocumentCommand{\rhsmomentumprincipleupdate}{ s }%
+ {%
+ \IfBooleanTF{#1}%
+ {%
+ \vec*{p}%
+ }%
+ {%
+ \vec{p}%
+ }%
+ \sb{\symup{sys,initial}}+%
+ \IfBooleanTF{#1}%
+ {%
+ \vec*{F}%
+ }%
+ {%
+ \vec{F}%
+ }%
+ \sb{\symup{sys,net}}\,\Delta t%
+ }%
+\NewDocumentCommand{\momentumprinciple}{ s }%
+ {%
+ \IfBooleanTF{#1}%
+ {%
+ \lhsmomentumprinciple* = \rhsmomentumprinciple*%
+ }%
+ {%
+ \lhsmomentumprinciple = \rhsmomentumprinciple%
+ }%
+ }%
+\NewDocumentCommand{\momentumprincipleupdate}{ s }%
+ {%
+ \IfBooleanTF{#1}%
+ {%
+ \lhsmomentumprincipleupdate* = \rhsmomentumprincipleupdate*%
+ }%
+ {%
+ \lhsmomentumprincipleupdate = \rhsmomentumprincipleupdate%
+ }%
+ }%
% The momentum principle
-\NewDocumentCommand{\lhsenergyprinciple}{}{%
- \Delta E_{\symup{sys}}%
-}%
-\NewDocumentCommand{\rhsenergyprinciple}{ O{} }{%
- W_{\symup{ext}}#1%
-}%
-\NewDocumentCommand{\lhsenergyprincipleupdate}{}{%
- E_{\symup{sys,final}}%
-}%
-\NewDocumentCommand{\rhsenergyprincipleupdate}{ O{} }{%
- E_{\symup{sys,initial}}+%
- W_{\symup{ext}}#1%
-}%
-\NewDocumentCommand{\energyprinciple}{ O{} }{%
- \lhsenergyprinciple = \rhsenergyprinciple[#1]%
-}%
-\NewDocumentCommand{\energyprincipleupdate}{ O{} }{%
- \lhsenergyprincipleupdate = \rhsenergyprincipleupdate[#1]%
-}%
+\NewDocumentCommand{\lhsenergyprinciple}{}%
+ {%
+ \Delta E_{\symup{sys}}%
+ }%
+\NewDocumentCommand{\rhsenergyprinciple}{ O{} }%
+ {%
+ W_{\symup{ext}}#1%
+ }%
+\NewDocumentCommand{\lhsenergyprincipleupdate}{}%
+ {%
+ E_{\symup{sys,final}}%
+ }%
+\NewDocumentCommand{\rhsenergyprincipleupdate}{ O{} }%
+ {%
+ E_{\symup{sys,initial}}+%
+ W_{\symup{ext}}#1%
+ }%
+\NewDocumentCommand{\energyprinciple}{ O{} }%
+ {%
+ \lhsenergyprinciple = \rhsenergyprinciple[#1]%
+ }%
+\NewDocumentCommand{\energyprincipleupdate}{ O{} }%
+ {%
+ \lhsenergyprincipleupdate = \rhsenergyprincipleupdate[#1]%
+ }%
% The angular momentum principle
-\NewDocumentCommand{\lhsangularmomentumprinciple}{ s }{%
- \Delta
- \IfBooleanTF{#1}%
- {\vec*{L}}%
- {\vec{L}}%
- _{A\symup{,sys,net}}%
-}%
-\NewDocumentCommand{\rhsangularmomentumprinciple}{ s }{%
- \IfBooleanTF{#1}%
- {\vec*{\tau}}%
- {\vec{\tau}}%
- _{A\symup{,sys,net}}\,\Delta t%
-}%
-\NewDocumentCommand{\lhsangularmomentumprincipleupdate}{ s }{%
- \IfBooleanTF{#1}%
- {\vec*{L}}%
- {\vec{L}}%
- _{A,\symup{sys,final}}%
-}%
-\NewDocumentCommand{\rhsangularmomentumprincipleupdate}{ s }{%
- \IfBooleanTF{#1}%
- {\vec*{L}}%
- {\vec{L}}%
- _{A\symup{,sys,initial}}+%
- \IfBooleanTF{#1}%
- {\vec*{\tau}}%
- {\vec{\tau}}%
- _{A\symup{,sys,net}}\,\Delta t%
-}%
-\NewDocumentCommand{\angularmomentumprinciple}{ s }{%
- \IfBooleanTF{#1}%
- {\lhsangularmomentumprinciple* = \rhsangularmomentumprinciple*}%
- {\lhsangularmomentumprinciple = \rhsangularmomentumprinciple}%
-}%
-\NewDocumentCommand{\angularmomentumprincipleupdate}{ s }{%
- \IfBooleanTF{#1}%
- {\lhsangularmomentumprincipleupdate* = \rhsangularmomentumprincipleupdate*}%
- {\lhsangularmomentumprincipleupdate = \rhsangularmomentumprincipleupdate}%
-}%
-\NewDocumentCommand{\energyof}{ m o }{%
- E_{#1\IfValueT{#2}{,#2}}%
-}%
-\NewDocumentCommand{\systemenergy}{ o }{%
- E_{\symup{sys}\IfValueT{#1}{,#1}}%
-}%
-\NewDocumentCommand{\particleenergy}{ o }{%
- E_{\symup{particle}\IfValueT{#1}{,#1}}%
-}%
-\NewDocumentCommand{\restenergy}{ o }{%
- E_{\symup{rest}\IfValueT{#1}{,#1}}%
-}%
-\NewDocumentCommand{\internalenergy}{ o }{%
- E_{\symup{internal}\IfValueT{#1}{,#1}}%
-}%
-\NewDocumentCommand{\chemicalenergy}{ o }{%
- E_{\symup{chem}\IfValueT{#1}{,#1}}%
-}%
-\NewDocumentCommand{\thermalenergy}{ o }{%
- E_{\symup{therm}\IfValueT{#1}{,#1}}%
-}%
-\NewDocumentCommand{\photonenergy}{ o }{%
- E_{\symup{photon}\IfValueT{#1}{,#1}}%
-}%
-\NewDocumentCommand{\translationalkineticenergy}{ s d[] }{%
-% d[] must be used because of the way consecutive optional
-% arguments are handled. See xparse docs for details.
-% See https://tex.stackexchange.com/a/569011/218142
- \IfBooleanTF{#1}%
- {E_\bgroup \symup{K}}%
- {K_\bgroup\symup{trans}}%
- \IfValueT{#2}{,#2}%
- \egroup%
-}%
-\NewDocumentCommand{\rotationalkineticenergy}{ s d[] }{%
-% d[] must be used because of the way consecutive optional
-% arguments are handled. See xparse docs for details.
-% See https://tex.stackexchange.com/a/569011/218142
- \IfBooleanTF{#1}%
- {E_\bgroup}%
- {K_\bgroup}%
- \symup{rot}\IfValueT{#2}{,#2}%
- \egroup%
-}%
-\NewDocumentCommand{\vibrationalkineticenergy}{ s d[] }{%
-% d[] must be used because of the way consecutive optional
-% arguments are handled. See xparse docs for details.
-% See https://tex.stackexchange.com/a/569011/218142
- \IfBooleanTF{#1}%
- {E_\bgroup}%
- {K_\bgroup}%
- \symup{vib}\IfValueT{#2}{,#2}%
- \egroup%
-}%
-\NewDocumentCommand{\gravitationalpotentialenergy}{ o }{%
- U_{\symup{g}\IfValueT{#1}{,#1}}%
-}%
-\NewDocumentCommand{\electricpotentialenergy}{ o }{%
- U_{\symup{e}\IfValueT{#1}{,#1}}%
-}%
-\NewDocumentCommand{\springpotentialenergy}{ o }{%
- U_{\symup{s}\IfValueT{#1}{,#1}}%
-}%
+\NewDocumentCommand{\lhsangularmomentumprinciple}{ s }%
+ {%
+ \Delta%
+ \IfBooleanTF{#1}%
+ {%
+ \vec*{L}%
+ }%
+ {%
+ \vec{L}%
+ }%
+ \sb{A\symup{,sys,net}}%
+ }%
+\NewDocumentCommand{\rhsangularmomentumprinciple}{ s }%
+ {%
+ \IfBooleanTF{#1}%
+ {%
+ \vec*{\tau}%
+ }%
+ {%
+ \vec{\tau}%
+ }%
+ \sb{A\symup{,sys,net}}\,\Delta t%
+ }%
+\NewDocumentCommand{\lhsangularmomentumprincipleupdate}{ s }%
+ {%
+ \IfBooleanTF{#1}%
+ {%
+ \vec*{L}%
+ }%
+ {%
+ \vec{L}%
+ }%
+ \sb{A,\symup{sys,final}}%
+ }%
+\NewDocumentCommand{\rhsangularmomentumprincipleupdate}{ s }%
+ {%
+ \IfBooleanTF{#1}%
+ {%
+ \vec*{L}%
+ }%
+ {%
+ \vec{L}%
+ }%
+ \sb{A\symup{,sys,initial}}+%
+ \IfBooleanTF{#1}%
+ {%
+ \vec*{\tau}%
+ }%
+ {%
+ \vec{\tau}%
+ }%
+ \sb{A\symup{,sys,net}}\,\Delta t%
+ }%
+\NewDocumentCommand{\angularmomentumprinciple}{ s }%
+ {%
+ \IfBooleanTF{#1}%
+ {%
+ \lhsangularmomentumprinciple* = \rhsangularmomentumprinciple*%
+ }%
+ {%
+ \lhsangularmomentumprinciple = \rhsangularmomentumprinciple%
+ }%
+ }%
+\NewDocumentCommand{\angularmomentumprincipleupdate}{ s }%
+ {%
+ \IfBooleanTF{#1}%
+ {%
+ \lhsangularmomentumprincipleupdate* = \rhsangularmomentumprincipleupdate*%
+ }%
+ {%
+ \lhsangularmomentumprincipleupdate = \rhsangularmomentumprincipleupdate%
+ }%
+ }%
+\NewDocumentCommand{\energyof}{ m o }%
+ {%
+ E_{#1%
+ \IfValueT{#2}%
+ {,#2}%
+ }%
+ }%
+\NewDocumentCommand{\systemenergy}{ o }%
+ {%
+ E_{\symup{sys}%
+ \IfValueT{#1}%
+ {,#1}%
+ }%
+ }%
+\NewDocumentCommand{\particleenergy}{ o }%
+ {%
+ E_{\symup{particle}%
+ \IfValueT{#1}%
+ {,#1}%
+ }%
+ }%
+\NewDocumentCommand{\restenergy}{ o }%
+ {%
+ E_{\symup{rest}%
+ \IfValueT{#1}%
+ {,#1}%
+ }%
+ }%
+\NewDocumentCommand{\internalenergy}{ o }%
+ {%
+ E_{\symup{internal}%
+ \IfValueT{#1}%
+ {,#1}%
+ }%
+ }%
+\NewDocumentCommand{\chemicalenergy}{ o }%
+ {%
+ E_{\symup{chem}%
+ \IfValueT{#1}%
+ {,#1}%
+ }%
+ }%
+\NewDocumentCommand{\thermalenergy}{ o }%
+ {%
+ E_{\symup{therm}%
+ \IfValueT{#1}%
+ {,#1}%
+ }%
+ }%
+\NewDocumentCommand{\photonenergy}{ o }%
+ {%
+ E_{\symup{photon}%
+ \IfValueT{#1}%
+ {,#1}%
+ }%
+ }%
+\NewDocumentCommand{\translationalkineticenergy}{ s d[] }%
+ {%
+ % d[] must be used because of the way consecutive optional
+ % arguments are handled. See xparse docs for details.
+ % See https://tex.stackexchange.com/a/569011/218142
+ \IfBooleanTF{#1}%
+ {%
+ E_\bgroup \symup{K}%
+ }%
+ {%
+ K_\bgroup\symup{trans}%
+ }%
+ \IfValueT{#2}{,#2}%
+ \egroup%
+ }%
+\NewDocumentCommand{\rotationalkineticenergy}{ s d[] }%
+ {%
+ % d[] must be used because of the way consecutive optional
+ % arguments are handled. See xparse docs for details.
+ % See https://tex.stackexchange.com/a/569011/218142
+ \IfBooleanTF{#1}%
+ {%
+ E_\bgroup%
+ }%
+ {%
+ K_\bgroup%
+ }%
+ \symup{rot}\IfValueT{#2}{,#2}%
+ \egroup%
+ }%
+\NewDocumentCommand{\vibrationalkineticenergy}{ s d[] }%
+ {%
+ % d[] must be used because of the way consecutive optional
+ % arguments are handled. See xparse docs for details.
+ % See https://tex.stackexchange.com/a/569011/218142
+ \IfBooleanTF{#1}%
+ {%
+ E_\bgroup%
+ }%
+ {%
+ K_\bgroup%
+ }%
+ \symup{vib}\IfValueT{#2}{,#2}%
+ \egroup%
+ }%
+\NewDocumentCommand{\gravitationalpotentialenergy}{ o }%
+ {%
+ U_{\symup{g}%
+ \IfValueT{#1}%
+ {,#1}%
+ }%
+ }%
+\NewDocumentCommand{\electricpotentialenergy}{ o }%
+ {%
+ U_{\symup{e}%
+ \IfValueT{#1}%
+ {,#1}%
+ }%
+ }%
+\NewDocumentCommand{\springpotentialenergy}{ o }%
+ {%
+ U_{\symup{s}%
+ \IfValueT{#1}%
+ {,#1}%
+ }%
+ }%
% \end{macrocode}
%
% \restoregeometry
diff --git a/Master/texmf-dist/source/latex/mandi/mandistudent.dtx b/Master/texmf-dist/source/latex/mandi/mandistudent.dtx
index bbeb5d974a6..d27bc93ac54 100644
--- a/Master/texmf-dist/source/latex/mandi/mandistudent.dtx
+++ b/Master/texmf-dist/source/latex/mandi/mandistudent.dtx
@@ -1,7 +1,7 @@
% \iffalse meta-comment
% !TEX program = lualatexmk
%
-% Copyright (C) 2021 by Paul J. Heafner <heafnerj@gmail.com>
+% Copyright (C) 2021,2022 by Paul J. Heafner <heafnerj@gmail.com>
% ---------------------------------------------------------------------------
% 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
@@ -111,7 +111,7 @@ while t < 10:
%</driver>
% \fi
%
-% \CheckSum{706}
+% \CheckSum{745}
%
% \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
@@ -147,7 +147,7 @@ while t < 10:
%\iffalse
%<*example>
%\fi
-\begin{dispListing*}{sidebyside=false,listing only}
+\begin{dispListing*}{sidebyside = false,listing only}
\usepackage{mandistudent}
\end{dispListing*}
%\iffalse
@@ -160,7 +160,7 @@ while t < 10:
\begin{docCommand}{mandistudentversion}{}
Typesets the current version and build date.
\end{docCommand}
-\begin{dispExample*}{sidebyside=false}
+\begin{dispExample*}{sidebyside = false}
The version is \mandistudentversion\ and is a stable build.
\end{dispExample*}
%\iffalse
@@ -173,6 +173,7 @@ while t < 10:
%<*example>
%\fi
\begin{docCommands}[%
+ doc updated = 2021-09-18,%
doc parameter = \marg{symbol}\oarg{labels},%
]%
{%
@@ -192,16 +193,21 @@ while t < 10:
|\symup{...}| for proper typesetting. The starred variant gives arrow
notation whereas without the star you get boldface notation. Subscript
and superscript labels can be arbitrarily mixed, and order doesn't matter.
- This command redefines the default \LaTeX\ |\vec| command.
+ This command redefines the default \LaTeXe |\vec| command.
\end{docCommands}
-\begin{dispExample*}{lefthand ratio=0.6}
- \( \vec{p} \) \\
- \( \vec{p}_{2} \) \\
- \( \vec{p}^{\symup{ball}} \) \\
- \( \vec{p}_{\symup{final}} \) \\
- \( \vec{p}^{\symup{ball}}_{\symup{final}} \) \\
- \( \vec{p}^{\symup{final}}_{\symup{ball}} \) \\
- \( \vec*{p} \)
+\begin{dispExample*}{lefthand ratio = 0.6}
+ \( \vec{p} \) \\
+ \( \vec{p}_{2} \) \\
+ \( \vec{p}^{\symup{ball}} \) \\
+ \( \vec{p}_{\symup{final}} \) \\
+ \( \vec{p}^{\symup{ball}}_{\symup{final}} \) \\
+ \( \vec{p}^{\symup{final}}_{\symup{ball}} \) \\
+ \( \vec*{p} \) \\
+ \( \vec*{p}_{2} \) \\
+ \( \vec*{p}^{\symup{ball}} \) \\
+ \( \vec*{p}_{\symup{final}} \) \\
+ \( \vec*{p}^{\symup{ball}}_{\symup{final}} \) \\
+ \( \vec*{p}^{\symup{final}}_{\symup{ball}} \)
\end{dispExample*}
%\iffalse
%</example>
@@ -211,6 +217,7 @@ while t < 10:
%<*example>
%\fi
\begin{docCommands}[%
+ doc updated = 2021-09-18,%
doc parameter = \marg{symbol}\oarg{labels},%
]%
{%
@@ -226,14 +233,19 @@ while t < 10:
Powerful and intelligent command for typesetting the direction of
a vector. The options are the same as those for \refCom{vec}.
\end{docCommands}
-\begin{dispExample*}{lefthand ratio=0.65}
- \( \dirvec{p} \) \\
- \( \dirvec{p}_{2} \) \\
- \( \dirvec{p}^{\symup{ball}} \) \\
- \( \dirvec{p}_{\symup{final}} \) \\
- \( \dirvec{p}^{\symup{ball}}_{\symup{final}} \) \\
- \( \dirvec{p}^{\symup{final}}_{\symup{ball}} \) \\
- \( \dirvec*{p} \)
+\begin{dispExample*}{lefthand ratio = 0.65}
+ \( \dirvec{p} \) \\
+ \( \dirvec{p}_{2} \) \\
+ \( \dirvec{p}^{\symup{ball}} \) \\
+ \( \dirvec{p}_{\symup{final}} \) \\
+ \( \dirvec{p}^{\symup{ball}}_{\symup{final}} \) \\
+ \( \dirvec{p}^{\symup{final}}_{\symup{ball}} \) \\
+ \( \dirvec*{p} \) \\
+ \( \dirvec*{p}_{2} \) \\
+ \( \dirvec*{p}^{\symup{ball}} \) \\
+ \( \dirvec*{p}_{\symup{final}} \) \\
+ \( \dirvec*{p}^{\symup{ball}}_{\symup{final}} \) \\
+ \( \dirvec*{p}^{\symup{final}}_{\symup{ball}} \)
\end{dispExample*}
%\iffalse
%</example>
@@ -445,7 +457,7 @@ while t < 10:
Commands for geometric relationships, mainly
intended for subscripts.
\end{docCommands}
-\begin{dispExample*}{lefthand ratio=0.6}
+\begin{dispExample*}{lefthand ratio = 0.6}
\( \vec{F}_{\parallelto} + \vec{F}_{\perpendicularto} \)
\end{dispExample*}
%\iffalse
@@ -480,16 +492,16 @@ while t < 10:
begin on a new page. See the examples for how to handle single and
multiple part problems.
\end{docEnvironments}
-\begin{docCommand}[doc new = 2012-02-03]{problempart}{}
+\begin{docCommand}[doc new = 2021-02-03]{problempart}{}
Denotes a part of a problem within a \refEnv{parts}
environment.
\end{docCommand}
-\begin{dispExample*}{sidebyside=false}
+\begin{dispExample*}{sidebyside = false}
\begin{physicsproblem}{Problem 1}
This is a physics problem with no parts.
\end{physicsproblem}
\end{dispExample*}
-\begin{dispExample*}{sidebyside=false}
+\begin{dispExample*}{sidebyside = false}
\begin{physicsproblem}{Problem 2}
This is a physics problem with multiple parts.
The list is vertical.
@@ -500,7 +512,7 @@ while t < 10:
\end{parts}
\end{physicsproblem}
\end{dispExample*}
-\begin{dispExample*}{sidebyside=false}
+\begin{dispExample*}{sidebyside = false}
\begin{physicsproblem*}{Problem 3}
This is a physics problem with multiple parts.
The list is in-line.
@@ -555,7 +567,7 @@ while t < 10:
%\iffalse
%<*example>
%\fi
-\begin{docCommand}[doc updated = 2012-02-26]{reason}{\marg{reason}}
+\begin{docCommand}[doc updated = 2021-02-26]{reason}{\marg{reason}}
Provides an annotation in a step-by-step solution.
Keep reasons short and to the point. Wrap mathematical
content in math mode.
@@ -583,7 +595,7 @@ while t < 10:
%\iffalse
%<*example>
%\fi
-\begin{dispListing*}{sidebyside=false,listing only}
+\begin{dispListing*}{sidebyside = false,listing only}
\begin{physicsproblem}{Combined Problem and Solution}
This is an interesting physics problem.
\begin{physicssolution}
@@ -591,7 +603,7 @@ while t < 10:
\end{physicssolution}
\end{physicsproblem}
\end{dispListing*}
-\begin{dispListing*}{sidebyside=false,listing only}
+\begin{dispListing*}{sidebyside = false,listing only}
\begin{physicsproblem}{Combined Multipart Problem with Solutions}
This is a physics problem with multiple parts.
\begin{parts}
@@ -617,14 +629,14 @@ while t < 10:
%\iffalse
%<*example>
%\fi
-\begin{docCommand}[doc new=2021-02-06]{hilite}{%
+\begin{docCommand}[doc new = 2021-02-06]{hilite}{%
\oarg{color}\marg{target}\oarg{shape}
}%
Hilites the desired target, which can be an entire mathematical expression
or a part thereof. The default color is magenta and the default shape is a
rectangle.
\end{docCommand}
-\begin{dispListing*}{sidebyside=false,listing only}
+\begin{dispListing*}{sidebyside = false,listing only}
\begin{align*}
(\Delta s)^2 &= -(\Delta t)^2 + (\Delta x)^2 + (\Delta y)^2 +
(\Delta z)^2 \\
@@ -656,7 +668,7 @@ while t < 10:
(\Delta y)^{\hilite[blue!50]{2}[circle]} +
(\Delta z)^{\hilite[violet!45]{2}[circle]}
\end{align*}
-\begin{dispListing*}{sidebyside=false,listing only}
+\begin{dispListing*}{sidebyside = false,listing only}
\begin{align*}
\Delta\vec{p} &= \vec{F}_{\sumup{net}}\Delta t \\
\hilite[orange]{\Delta\vec{p}}[circle] &= \vec{F}_{\symup{net}}\Delta t \\
@@ -688,14 +700,14 @@ while t < 10:
%\iffalse
%<*example>
%\fi
-\begin{docCommand}[doc updated = 2021-02-26]{image}{%
+\begin{docCommand}[doc updated = 2021-09-18]{image}{%
\oarg{options}\marg{caption}\marg{label}\marg{image}
}%
Simplified interface for importing an image. The images are treated
as floats, so they may not appear at the most logically intuitive
place.
\end{docCommand}
-\begin{dispListing*}{sidebyside=false,listing only,verbatim ignore percent}
+\begin{dispListing*}{sidebyside = false,listing only,verbatim ignore percent}
\image[scale=0.20]{example-image-1x1}
{Image shown 20 percent actual size.}{reffig1}
\end{dispListing*}
@@ -705,13 +717,13 @@ while t < 10:
Figure \ref{reffig1} is nice.
It's captioned \nameref{reffig1} and is on page \pageref{reffig1}.
\end{dispExample*}
-\begin{dispListing*}{sidebyside=false,listing only,verbatim ignore percent}
+\begin{dispListing*}{sidebyside = false,listing only,verbatim ignore percent}
\image[scale=0.20,angle=45]{example-image-1x1}
{Image shown 20 percent actual size and rotated.}{reffig1}
\end{dispListing*}
\image[scale=0.20,angle=45]{example-image-1x1}
{Image shown 20 percent actual size and rotated.}{reffig2}
-\begin{dispExample*}{sidebyside=false}
+\begin{dispExample*}{sidebyside = false}
Figure \ref{reffig2} is nice.
It's captioned \nameref{reffig2} and is on page \pageref{reffig2}.
\end{dispExample*}
@@ -729,7 +741,7 @@ while t < 10:
%<*example>
%\fi
\begin{docCommands}[%
- doc parameter = \oarg{delimiter}\marg{\ensuremath{c_1,\dots,c_n}},%
+ doc parameter = \oarg{delimiter}\marg{\( c_1,\dots,c_n \)},%
]%
{%
{%
@@ -867,11 +879,14 @@ while t < 10:
%</example>
%\fi
%
+% \changes{v3.1.0}{2022-01-27}
+% {\linktoplace{sec:mandistudentpkg}{mandistudent} \cs{diff} renamed to
+% \refCom{df} for compatibility with the \pkg{numerica} package}
%\iffalse
%<*example>
%\fi
-\begin{docCommand}[doc new=2021-04-06]{diff}{}%
- Intelligent differential (exterior derivative)
+\begin{docCommand}[doc updated = 2022-01-27]{df}{}%
+ Intelligent differential and exterior derivative
operator.
\end{docCommand}
\begin{dispExample}
@@ -879,19 +894,25 @@ while t < 10:
\int x\,dx
\]
\[
- \int x\,\diff{x}
+ \int x\,\df{x}
\]
\[
- \int x\,\diff*{x}
+ \int x\,\df*{x}
\]
\end{dispExample}
%\iffalse
%</example>
%\fi
%
-% \subsection{\GlowScript\ and \VPython\ Program Listings}
+% \changes{v3.1.0}{2022-01-27}
+% {\linktoplace{sec:mandistudentpkg}{mandistudent} All instances of
+% \texttt{GlowScript} have been changed to \texttt{Web VPython}}
+% \subsection{\WebVPython\ and \VPython\ Program Listings}
%
-% \href{https://\gsurl}{\GlowScript}\footnote{\href{https://\gsurl}{https://\gsurl}}
+% \href{https://\gsurl}{\WebVPython}
+% \footnote{On November 9, 2021 \texttt{GlowScript} was renamed to
+% \WebVPython. The website was changed to
+% \href{https://\gsurl}{https://\gsurl}.}
% and
% \href{https://\vpurl}{VPython}\footnote{\href{https://\vpurl}{https://\vpurl}}
% are programming environments (both use \href{https://www.python.org}{Python})
@@ -899,25 +920,39 @@ while t < 10:
% for modeling physical systems. \mandi\ makes including code listings
% very simple for students.
%
-% \subsection{The \texttt{\small glowscriptblock} Environment}
+% \subsection{The \texttt{\small webvpythonblock} Environment}
%
%\iffalse
%<*example>
%\fi
-\begin{docEnvironment}[%
- doc updated = 2021-02-26,doclang/environment content=GlowScript code%
- ]%
- {glowscriptblock}{\oarg{options}(\meta{link})\marg{caption}}
+\begin{docEnvironments}[%
+ doc parameter = {\oarg{options}(\meta{link})\marg{caption}},%
+ doclang/environment content=WebVPython code,%
+ ]%
+ {%
+ {%
+ doc updated = 2022-01-27,%
+ doc name = webvpythonblock,%
+ doc description = now includes a QR code,%
+ },%
+ {%
+ doc new = 2022-01-27,%
+ doc name = webvpythonblock*,%
+ doc description = use this variant to omit QR code,%
+ },%
+ }%
Code placed here is nicely formatted and optionally linked to its source on
- \href{https://\gsurl}{\GlowScriptorg}. Clicking anywhere in the code window
- will open the link in the default browser. A caption is mandatory, and a
- label is internally generated. The listing always begins on a new page. A
- URL shortening utility is recommended to keep the URL from getting unruly.
- For convenience, |https://| is automatically prepended to the URL and can
- thus be omitted. The program must exist in a public, not private, folder.
-\end{docEnvironment}
-\begin{dispListing*}{sidebyside=false}
-\begin{glowscriptblock}(tinyurl.com/y3lnqyn3){A \texttt{GlowScript} Program}
+ \href{https://\gsurl}{\WebVPythonorg}, which must be in a public (not private)
+ folder. Clicking anywhere in the code window will open the link in the default
+ browser. A caption is mandatory, and a label is internally generated. The
+ listing always begins on a new page. A URL shortening utility is recommended
+ to keep the URL from getting unruly. For convenience, |https://| is
+ automatically prepended to the URL and can thus be omitted. The |#| character
+ in a URL should not cause problems. The default URL is that of the \WebVPython\
+ home page.
+\end{docEnvironments}
+\begin{dispListing*}{sidebyside = false}
+\begin{webvpythonblock}(tinyurl.com/y3lnqyn3){A \texttt{Web VPython} Program With QR Code}
GlowScript 3.0 vpython
scene.width = 400
@@ -961,9 +996,9 @@ while t < 10:
ball.pos = ball.pos + (pball / mball) * deltat
spring.axis = ball.pos - ceiling.pos
t = t + deltat
-\end{glowscriptblock}
+\end{webvpythonblock}
\end{dispListing*}
-\begin{glowscriptblock}(tinyurl.com/y3lnqyn3){A \texttt{GlowScript} Program}
+\begin{webvpythonblock}(tinyurl.com/y3lnqyn3){A \texttt{Web VPython} Program With QR Code}
GlowScript 3.0 vpython
scene.width = 400
@@ -1007,18 +1042,128 @@ while t < 10:
ball.pos = ball.pos + (pball / mball) * deltat
spring.axis = ball.pos - ceiling.pos
t = t + deltat
-\end{glowscriptblock}
+\end{webvpythonblock}
+%
%\iffalse
%</example>
%\fi
%
+% \newpage
+% Here is how one would reference this program elsewhere. Notice the
+% references are numbered sequentially within the document.
+%
%\iffalse
%<*example>
%\fi
-\begin{dispExample*}{sidebyside=false}
- \GlowScript\ program \ref{gs:1} is nice.
+\begin{dispExample*}{sidebyside = false}
+ \WebVPython\ program \ref{gs:1} is nice.
It's called \nameref{gs:1} and is on page \pageref{gs:1}.
\end{dispExample*}
+%\iffalse
+%</example>
+%\fi
+%
+% \newpage
+%
+%\iffalse
+%<*example>
+%\fi
+\begin{dispListing*}{sidebyside = false}
+\begin{webvpythonblock*}(tinyurl.com/y3lnqyn3){A \texttt{Web VPython} Program Without QR Code}
+GlowScript 3.0 vpython
+
+scene.width = 400
+scene.height = 760
+# constants and data
+g = 9.8 # m/s^2
+mball = 0.03 # kg
+Lo = 0.26 # m
+ks = 1.8 # N/m
+deltat = 0.01 # s
+
+# objects (origin is at ceiling)
+ceiling = box(pos=vector(0,0,0), length=0.2, height=0.01,
+ width=0.2)
+ball = sphere(pos=vector(0,-0.3,0),radius=0.025,
+ color=color.orange)
+spring = helix(pos=ceiling.pos, axis=ball.pos-ceiling.pos,
+ color=color.cyan,thickness=0.003,coils=40,
+ radius=0.010)
+
+# initial values
+pball = mball * vector(0,0,0) # kg m/s
+Fgrav = mball * g * vector(0,-1,0) # N
+t = 0
+
+# improve the display
+scene.autoscale = False # turn off automatic camera zoom
+scene.center = vector(0,-Lo,0) # move camera down
+scene.waitfor('click') # wait for a mouse click
+
+# initial calculation loop
+# calculation loop
+while t < 10:
+ rate(100)
+ # we need the stretch
+ s = mag(ball.pos) - Lo
+ # we need the spring force
+ Fspring = ks * s * -norm(spring.axis)
+ Fnet = Fgrav + Fspring
+ pball = pball + Fnet * deltat
+ ball.pos = ball.pos + (pball / mball) * deltat
+ spring.axis = ball.pos - ceiling.pos
+ t = t + deltat
+\end{webvpythonblock*}
+\end{dispListing*}
+\begin{webvpythonblock*}(tinyurl.com/y3lnqyn3){A \texttt{Web VPython} Program Without QR Code}
+GlowScript 3.0 vpython
+
+scene.width = 400
+scene.height = 760
+# constants and data
+g = 9.8 # m/s^2
+mball = 0.03 # kg
+Lo = 0.26 # m
+ks = 1.8 # N/m
+deltat = 0.01 # s
+
+# objects (origin is at ceiling)
+ceiling = box(pos=vector(0,0,0), length=0.2, height=0.01,
+ width=0.2)
+ball = sphere(pos=vector(0,-0.3,0),radius=0.025,
+ color=color.orange)
+spring = helix(pos=ceiling.pos, axis=ball.pos-ceiling.pos,
+ color=color.cyan,thickness=0.003,coils=40,
+ radius=0.010)
+
+# initial values
+pball = mball * vector(0,0,0) # kg m/s
+Fgrav = mball * g * vector(0,-1,0) # N
+t = 0
+
+# improve the display
+scene.autoscale = False # turn off automatic camera zoom
+scene.center = vector(0,-Lo,0) # move camera down
+scene.waitfor('click') # wait for a mouse click
+
+# initial calculation loop
+# calculation loop
+while t < 10:
+ rate(100)
+ # we need the stretch
+ s = mag(ball.pos) - Lo
+ # we need the spring force
+ Fspring = ks * s * -norm(spring.axis)
+ Fnet = Fgrav + Fspring
+ pball = pball + Fnet * deltat
+ ball.pos = ball.pos + (pball / mball) * deltat
+ spring.axis = ball.pos - ceiling.pos
+ t = t + deltat
+\end{webvpythonblock*}
+\begin{dispExample*}{sidebyside = false}
+ \WebVPython\ program \ref{gs:2} is nice.
+ It's called \nameref{gs:2} and is on page \pageref{gs:2}.
+\end{dispExample*}
%
%\iffalse
%</example>
@@ -1029,22 +1174,20 @@ while t < 10:
%\iffalse
%<*example>
%\fi
-\begin{docCommand}[doc updated = 2021-02-26]{vpythonfile}
- {\oarg{options}\marg{file}\marg{caption}}
- Command to load and typeset a \VPython\ program. The file is read from
+\begin{docCommand}[doc updated = 2022-01-27]{vpythonfile}
+ {\oarg{options}(\meta{link})\marg{file}\marg{caption}}
+ Command to load and typeset a \VPython\ program, read from local file
\marg{file}. Clicking anywhere in the code window can optionally open
a link, passed as an option, in the default browser. A caption is mandatory,
and a label is internally generated. The listing always begins on a new page.
A URL shortening utility is recommended to keep the URL from getting unruly.
For convenience, |https://| is automatically prepended to the URL and can
- thus be omitted.
+ thus be omitted. The default URL is that of the \VPython\ home page.
\end{docCommand}
-\begin{dispListing*}{sidebyside=false}
-\vpythonfile[hyperurl interior = https://vpython.org]{vdemo.py}
- {A \VPython\ Program}
+\begin{dispListing*}{sidebyside = false}
+\vpythonfile{vdemo.py}{A \VPython\ Program}
\end{dispListing*}
-\vpythonfile[hyperurl interior = https://vpython.org]{vdemo.py}
- {A \VPython\ Program}
+\vpythonfile{vdemo.py}{A \VPython\ Program}
%\iffalse
%</example>
%\fi
@@ -1052,7 +1195,7 @@ while t < 10:
%\iffalse
%<*example>
%\fi
-\begin{dispExample*}{sidebyside=false}
+\begin{dispExample*}{sidebyside = false}
\VPython\ program \ref{vp:1} is nice.
It's called \nameref{vp:1} and is on page \pageref{vp:1}.
\end{dispExample*}
@@ -1061,7 +1204,7 @@ while t < 10:
%</example>
%\fi
%
-% \subsection{The \texttt{\small glowscriptinline} and
+% \subsection{The \texttt{\small webvpythoninline} and
% \texttt{\small vpythoninline} Commands}
%
%\iffalse
@@ -1072,8 +1215,8 @@ while t < 10:
]%
{%
{%
- doc name = glowscriptinline,%
- doc parameter = \marg{GlowScript code},%
+ doc name = webvpythoninline,%
+ doc parameter = \marg{Web VPython code},%
},%
{%
doc name = vpythoninline,%
@@ -1083,8 +1226,8 @@ while t < 10:
Typesets a small, in-line snippet of code. The snippet should be
less than one line long.
\end{docCommands}
-\begin{dispExample*}{sidebyside=false}
- \GlowScript\ programs begin with \glowscriptinline{GlowScript 3.0 VPython}
+\begin{dispExample*}{sidebyside = false}
+ \WebVPython\ programs begin with \webvpythoninline{GlowScript 3.0 VPython}
and \VPython\ programs begin with \vpythoninline{from vpython import *}.
\end{dispExample*}
%\iffalse
@@ -1104,12 +1247,16 @@ while t < 10:
% |\makeatother|. This simplifies defining internal commands, with |@|
% in the name, that are not for the user to know about.
%
+% \changes{v3.1.0}{2022-01-27}
+% {\linktoplace{sec:mandistudentpkg}{mandistudent} Version number works}
+% \changes{v3.1.0}{2022-01-27}
+% {\linktoplace{sec:mandistudentpkg}{mandistudent} Code formatted for better readability}
% \begin{macrocode}
-\def\mandistudent@version{\mandi@version}
-\def\mandistudent@date{\mandi@date}
+\def\mandistudent@version{3.1.0}
+\def\mandistudent@date{2022-01-27}
\NeedsTeXFormat{LaTeX2e}[2020-02-02]
-\DeclareRelease{v3.0.0}{2021-08-22}{mandistudent.sty}
-\DeclareCurrentRelease{v\mandi@version}{\mandi@date}
+\DeclareRelease{v3.1.0}{2022-01-27}{mandistudent.sty}
+\DeclareCurrentRelease{v\mandistudent@version}{\mandistudent@date}
\ProvidesPackage{mandistudent}
[\mandistudent@date\space v\mandistudent@version\space Macros for introductory physics]
% \end{macrocode}
@@ -1133,11 +1280,22 @@ while t < 10:
\RequirePackage{mandi}
\RequirePackage{mathtools} % needed for paired delimiters; extends amsmath
\RequirePackage{nicematrix} % needed for column and row vectors
+\RequirePackage{qrcode} % needed for QR codes in webvpythonblock
+\qrset{height=1.5cm} % set default size of QR code
\RequirePackage[most]{tcolorbox} % needed for program listings
\RequirePackage{tensor} % needed for index notation
\RequirePackage{tikz} % needed for \hilite
\usetikzlibrary{shapes,fit,tikzmark} % needed for \hilite
\RequirePackage{unicode-math} % needed for Unicode support
+% \end{macrocode}
+%
+%
+% \changes{v3.1.0}{2022-01-27}
+% {\linktoplace{sec:mandistudentpkg}{mandistudent} \pkg{xparse} is loaded for older formats}
+% \begin{macrocode}
+\IfFormatAtLeastTF {2020-10-01} % load xparse if necessary
+ {}%
+ {\RequirePackage{xparse}}%
\RequirePackage{hyperref} % load last
\RequireLuaTeX % require this engine
% \end{macrocode}
@@ -1146,13 +1304,14 @@ while t < 10:
% The \href{https://www.ctan.org/pkg/unicode-math}{\pkg{unicode-math}} package
% loads the \href{https://www.ctan.org/pkg/fontspec}{\pkg{fontspec}} and
% \href{https://www.ctan.org/pkg/xparse}{\pkg{xparse}}
-% packages. Note that \pkg{xparse} is now part of the \LaTeX\ kernel.
+% packages. Note that \pkg{xparse} is now part of the \LaTeXe\ kernel.
% Because \pkg{unicode-math} is required, all documents using \mandi\ must
% be compiled with an engine that supports Unicode. We recommend \lualatex.
%
% \begin{macrocode}
\unimathsetup{math-style=ISO}
\unimathsetup{warnings-off={mathtools-colon,mathtools-overbracket}}
+% \end{macrocode}
%
% Use normal math letters from Latin Modern Math for familiarity with
% textbooks.
@@ -1162,19 +1321,20 @@ while t < 10:
{Latin Modern Math} % default math font; better J
% \end{macrocode}
%
-% Borrow from GeX Gyre DejaVu Math for vectors and tensors to get single-storey g.
+% Borrow from TeX Gyre DejaVu Math for vectors and tensors to get single-storey g.
%
% \begin{macrocode}
\setmathfont[Scale=MatchLowercase,range={sfit/{latin},bfsfit/{latin}}]
{TeX Gyre DejaVu Math} % single-storey lowercase g
% \end{macrocode}
%
-% Borrow from GeX Gyre DejaVu Math to get single-storey g.
+% Borrow from TeX Gyre DejaVu Math to get single-storey g.
%
% \begin{macrocode}
\setmathfont[Scale=MatchLowercase,range={sfup/{latin},bfsfup/{latin}}]
{TeX Gyre DejaVu Math} % single-storey lowercase g
% \end{macrocode}
+%
% Borrow |mathscr| and |mathbfscr| from XITS Math.\newline
% See \url{https://tex.stackexchange.com/a/120073/218142}.
%
@@ -1282,7 +1442,7 @@ while t < 10:
% \end{macrocode}
%
% Tweak the \href{https://www.ctan.org/pkg/esvect}{\pkg{esvect}} package
-% fonts to get the correct font size. Code provided by |@egreg|.\newline
+% fonts to get the correct font size.\newline
% See \url{https://tex.stackexchange.com/a/566676}.
%
% \begin{macrocode}
@@ -1318,23 +1478,32 @@ while t < 10:
% See \url{https://tex.stackexchange.com/q/554706/218142}.\newline
% See also \url{https://tex.stackexchange.com/a/531037/218142}.
%
+% \changes{v3.1.0}{2022-01-27}
+% {\linktoplace{sec:mandistudentpkg}{mandistudent} \refCom{vec}%
+% no longer adds \cs{scriptspace} when no sub/superscript is given}
% \begin{macrocode}
-\RenewDocumentCommand{\vec}{ s m e{_^} }{%
+\RenewDocumentCommand{\vec}{ s m e{_^} }%
+ {%
% Note the \, used to make superscript look better.
- \IfBooleanTF {#1}
- {\vv{#2}% % * gives an arrow
- % Use \sp{} primitive for superscript.
- % Adjust superscript for the arrow.
- \sp{\IfValueT{#4}{\,#4}\vphantom{\smash[t]{\big|}}}
- }%
- {\symbfit{#2} % no * gives us bold
- % Use \sp{} primitive for superscript.
- % No superscript adjustment needed.
- \sp{\IfValueT{#4}{#4}\vphantom{\smash[t]{\big|}}}
- }%
- % Use \sb{} primitive for subscript.
- \sb{\IfValueT{#3}{#3}\vphantom{\smash[b]{|}}}
-}%
+ \IfBooleanTF{#1}
+ {%
+ \vv{#2}% % * gives an arrow
+ % Use \sp{} primitive for superscript.
+ % Adjust superscript for the arrow.
+ \IfValueT{#4}%
+ {\sp{\,#4\vphantom{\smash[t]{\big|}}}}
+ }%
+ {%
+ \symbfit{#2} % no * gives us bold
+ % Use \sp{} primitive for superscript.
+ % No superscript adjustment needed.
+ \IfValueT{#4}%
+ {\sp{#4\vphantom{\smash[t]{\big|}}}}
+ }%
+ % Use \sb{} primitive for subscript.
+ \IfValueT{#3}%
+ {\sb{#3\vphantom{\smash[b]{|}}}}
+ }%
% \end{macrocode}
%
% A command for the direction of a vector.
@@ -1343,53 +1512,68 @@ while t < 10:
% package.\newline
% See \url{https://tex.stackexchange.com/a/391204/218142}.
%
+% \changes{v3.1.0}{2022-01-27}
+% {\linktoplace{sec:mandistudentpkg}{mandistudent} \refCom{dirvec}%
+% no longer adds \cs{scriptspace} when no sub/superscript is given}
% \begin{macrocode}
-\NewDocumentCommand{\dirvec}{ s m e{_^} }{%
- \widehat{\makebox*{\(w\)}{\ensuremath{%
- \IfBooleanTF {#1}
- {%
- #2
- }%
- {%
- \symbfit{#2}
- }%
- }%
+\NewDocumentCommand{\dirvec}{ s m e{_^} }%
+ {%
+ \widehat%
+ {%
+ \makebox*{\(w\)}%
+ {%
+ \ensuremath{%
+ \IfBooleanTF {#1}%
+ {%
+ #2%
+ }%
+ {%
+ \symbfit{#2}%
+ }%
+ }%
+ }%
}%
- }%
- \sb{\IfValueT{#3}{#3}\vphantom{\smash[b]{|}}}
- \sp{\IfValueT{#4}{\,#4}\vphantom{\smash[t]{\big|}}}
-}%
+ \IfValueT{#3}%
+ {\sb{#3\vphantom{\smash[b]{|}}}}%
+ \IfValueT{#4}%
+ {\sp{\,#4\vphantom{\smash[t]{\big|}}}}%
+ }%
% \end{macrocode}
%
% The zero vector.
%
% \begin{macrocode}
-\NewDocumentCommand{\zerovec}{ s }{%
- \IfBooleanTF {#1}
- {\vv{0}}%
- {\symbfup{0}}%
-}%
+\NewDocumentCommand{\zerovec}{ s }%
+ {%
+ \IfBooleanTF {#1}
+ {\vv{0}}%
+ {\symbfup{0}}%
+ }%
% \end{macrocode}
%
-% Notation for column and row vectors.
-% Orginal code provided by |@egreg|.\newline
+% Notation for column and row vectors.\newline
% See \url{https://tex.stackexchange.com/a/39054/218142}.
%
+% \changes{v3.1.0}{2022-01-27}
+% {\linktoplace{sec:mandistudentpkg}{mandistudent} \LaTeX3 code now conforms to formatting standards}
% \begin{macrocode}
\ExplSyntaxOn
-\NewDocumentCommand{\colvec}{ O{,} m }{%
- \vector_main:nnnn { p } { \\ } { #1 } { #2 }
-}%
-\NewDocumentCommand{\rowvec}{ O{,} m }{%
- \vector_main:nnnn { p } { & } { #1 } { #2 }
-}%
-\seq_new:N \l__vector_arg_seq
-\cs_new_protected:Npn \vector_main:nnnn #1 #2 #3 #4 {%
- \seq_set_split:Nnn \l__vector_arg_seq { #3 } { #4 }
- \begin{#1NiceMatrix}[r]
- \seq_use:Nnnn \l__vector_arg_seq { #2 } { #2 } { #2 }
- \end{#1NiceMatrix}
-}%
+\NewDocumentCommand{\colvec}{ O{,} m }
+ {
+ \__mandi_vectormain:nnnn { p } { \\ } { #1 } { #2 }
+ }
+\NewDocumentCommand{\rowvec}{ O{,} m }
+ {
+ \__mandi_vectormain:nnnn { p } { & } { #1 } { #2 }
+ }
+\seq_new:N \l__mandi_vectorarg_seq
+\cs_new_protected:Npn \__mandi_vectormain:nnnn #1#2#3#4
+ {
+ \seq_set_split:Nnn \l__mandi_vectorarg_seq { #3 } { #4 }
+ \begin{#1NiceMatrix}[r]
+ \seq_use:Nnnn \l__mandi_vectorarg_seq { #2 } { #2 } { #2 }
+ \end{#1NiceMatrix}
+ }
\ExplSyntaxOff
% \end{macrocode}
%
@@ -1416,7 +1600,7 @@ while t < 10:
% Some semantic aliases. Because of the way \refCom{vec} and
% \refCom{dirvec} are defined, I reluctantly decided not to
% implement a |\magvec| command. It would require accounting
-% for too mamy options. So \refCom{magnitude} is the new
+% for too many options. So \refCom{magnitude} is the new
% solution.
%
% \begin{macrocode}
@@ -1429,8 +1613,10 @@ while t < 10:
% mainly to be subscripts.
%
% \begin{macrocode}
-\NewDocumentCommand{\parallelto}{}
- {\mkern3mu\vphantom{\perp}\vrule depth 0pt\mkern2mu\vrule depth 0pt\mkern3mu}
+\NewDocumentCommand{\parallelto}{}%
+ {%
+ \mkern3mu\vphantom{\perp}\vrule depth 0pt\mkern2mu\vrule depth 0pt\mkern3mu%
+ }%
\NewDocumentCommand{\perpendicularto}{}{\perp}
% \end{macrocode}
%
@@ -1438,17 +1624,21 @@ while t < 10:
% in-line lists.
%
% \begin{macrocode}
-\NewDocumentEnvironment{physicsproblem}{ m }{%
- \newpage%
- \section*{#1}%
- \newlist{parts}{enumerate}{2}%
- \setlist[parts]{label=\bfseries(\alph*)}}%
+\NewDocumentEnvironment{physicsproblem}{ m }%
+ {%
+ \newpage%
+ \section*{#1}%
+ \newlist{parts}{enumerate}{2}%
+ \setlist[parts]{label=\bfseries(\alph*)}%
+ }%
{}%
-\NewDocumentEnvironment{physicsproblem*}{ m }{%
- \newpage%
- \section*{#1}%
- \newlist{parts}{enumerate*}{2}%
- \setlist[parts]{label=\bfseries(\alph*)}}%
+\NewDocumentEnvironment{physicsproblem*}{ m }%
+ {%
+ \newpage%
+ \section*{#1}%
+ \newlist{parts}{enumerate*}{2}%
+ \setlist[parts]{label=\bfseries(\alph*)}%
+ }%
{}%
\NewDocumentCommand{\problempart}{}{\item}%
% \end{macrocode}
@@ -1456,29 +1646,34 @@ while t < 10:
% An environment for problem solutions.
%
% \begin{macrocode}
-\NewDocumentEnvironment{physicssolution}{ +b }{%
- % Make equation numbering consecutive through the document.
- \begin{align}
- #1
- \end{align}
-}{}%
-\NewDocumentEnvironment{physicssolution*}{ +b }{%
- % Make equation numbering consecutive through the document.
- \begin{align*}
- #1
- \end{align*}
-}{}%
+\NewDocumentEnvironment{physicssolution}{ +b }%
+ {%
+ % Make equation numbering consecutive through the document.
+ \begin{align}
+ #1
+ \end{align}
+ }%
+ {}%
+\NewDocumentEnvironment{physicssolution*}{ +b }%
+ {%
+ % Make equation numbering consecutive through the document.
+ \begin{align*}
+ #1
+ \end{align*}
+ }%
+ {}%
% \end{macrocode}
%
% See \url{https://tex.stackexchange.com/q/570223/218142}.
%
% \begin{macrocode}
-\NewDocumentCommand{\reason}{ O{4cm} m }
- {&&\begin{minipage}{#1}\raggedright\small #2\end{minipage}}
+\NewDocumentCommand{\reason}{ O{4cm} m }%
+ {%
+ &&\begin{minipage}{#1}\raggedright\small #2\end{minipage}%
+ }%
% \end{macrocode}
%
% Command for highlighting parts of, or entire, mathematical expressions.\newline
-% Original code by anonymous user |@abcdefg|, modified by me.\newline
% See \url{https://texample.net/tikz/examples/beamer-arrows/}.\newline
% See also \url{https://tex.stackexchange.com/a/406084/218142}.\newline
% See also \url{https://tex.stackexchange.com/a/570858/218142}.\newline
@@ -1489,34 +1684,40 @@ while t < 10:
%
% \begin{macrocode}
\newcounter{tikzhighlightnode}
-\NewDocumentCommand{\hilite}{ O{magenta!60} m O{rectangle} }{%
- \stepcounter{tikzhighlightnode}%
- \tikzmarknode{highlighted-node-\number\value{tikzhighlightnode}}{#2}%
- \edef\temp{%
- \noexpand\AddToShipoutPictureBG{%
- \noexpand\begin{tikzpicture}[overlay,remember picture]%
- \noexpand\iftikzmarkoncurrentpage{highlighted-node-\number\value{tikzhighlightnode}}%
- \noexpand\node[inner sep=1.0pt,fill=#1,#3,fit=(highlighted-node-\number\value{tikzhighlightnode})]{};%
- \noexpand\fi
- \noexpand\end{tikzpicture}%
+\NewDocumentCommand{\hilite}{ O{magenta!60} m O{rectangle} }%
+ {%
+ \stepcounter{tikzhighlightnode}%
+ \tikzmarknode{highlighted-node-\number\value{tikzhighlightnode}}{#2}%
+ \edef\temp{%
+ \noexpand\AddToShipoutPictureBG{%
+ \noexpand\begin{tikzpicture}[overlay,remember picture]%
+ \noexpand\iftikzmarkoncurrentpage{highlighted-node-\number\value{tikzhighlightnode}}%
+ \noexpand\node[inner sep=1.0pt,fill=#1,#3,fit=(highlighted-node-\number\value{tikzhighlightnode})]{};%
+ \noexpand\fi
+ \noexpand\end{tikzpicture}%
+ }%
}%
+ \temp%
}%
- \temp%
-}%
% \end{macrocode}
%
-% A simplified command for importing images.
+% A simplified command for importing images.\newline
+% See \url{https://tex.stackexchange.com/a/614478/218142}.
%
+% \changes{v3.1.0}{2022-01-27}
+% {\linktoplace{sec:mandistudentpkg}{mandistudent} Slightly modified \refCom{image}}
% \begin{macrocode}
-\NewDocumentCommand{\image}{ O{scale=1} m m m }{%
- \begin{figure}[ht!]
- \begin{center}%
+\NewDocumentCommand{\image}{ O{scale=1} m m m }%
+ {%
+ \par
+ \begin{figure}[ht!]
+ \centering%
\includegraphics[#1]{#2}%
- \end{center}%
- \caption{#3}%
- \label{#4}%
- \end{figure}%
-}%
+ \caption{#3}%
+ \label{#4}%
+ \end{figure}%
+ \par
+ }%
% \end{macrocode}
%
% Intelligent commands for typesetting vector and tensor symbols and
@@ -1525,86 +1726,104 @@ while t < 10:
% coordinate-free.
%
% \begin{macrocode}
-\NewDocumentCommand{\veccomp}{ s m }{%
- % Consider renaming this to \vectorsym.
- \IfBooleanTF{#1}
+\NewDocumentCommand{\veccomp}{ s m }%
{%
- \symnormal{#2}%
- }%
- {%
- \symbfit{#2}%
- }%
-}%
-\NewDocumentCommand{\tencomp}{ s m }{%
- % Consider renaming this to \tensororsym.
- \IfBooleanTF{#1}
- {%
- \symsfit{#2}%
+ % Consider renaming this to \vectorsym.
+ \IfBooleanTF{#1}
+ {%
+ \symnormal{#2}%
+ }%
+ {%
+ \symbfit{#2}%
+ }%
}%
+\NewDocumentCommand{\tencomp}{ s m }%
{%
- \symbfsfit{#2}
+ % Consider renaming this to \tensororsym.
+ \IfBooleanTF{#1}%
+ {%
+ \symsfit{#2}%
+ }%
+ {%
+ \symbfsfit{#2}%
+ }%
}%
-}%
% \end{macrocode}
%
% Command to typeset tensor valence.
%
% \begin{macrocode}
-\NewDocumentCommand{\valence}{ s m m }{%
- \IfBooleanTF{#1}
- {(#2,#3)}
- {\binom{#2}{#3}}
-}%
+\NewDocumentCommand{\valence}{ s m m }%
+ {%
+ \IfBooleanTF{#1}%
+ {%
+ (#2,#3)%
+ }%
+ {%
+ \binom{#2}{#3}%
+ }%
+ }%
% \end{macrocode}
%
% Intelligent notation for contraction on pairs of slots.
%
% \begin{macrocode}
-\NewDocumentCommand{\contraction}{ s m }{%
- \IfBooleanTF{#1}
- {\mathsf{C}}%
- {\symbb{C}}%
- _{#2}
-}%
+\NewDocumentCommand{\contraction}{ s m }%
+ {%
+ \IfBooleanTF{#1}
+ {%
+ \mathsf{C}%
+ }%
+ {%
+ \symbb{C}%
+ }%
+ _{#2}
+ }%
% \end{macrocode}
%
% Intelligent slot command for coordinate-free tensor notation.
%
% \begin{macrocode}
-\NewDocumentCommand{\slot}{ s d[] }{%
- % d[] must be used because of the way consecutive optional
- % arguments are handled. See xparse docs for details.
- \IfBooleanTF{#1}
- {%
- \IfValueTF{#2}
- {% Insert a vector, but don't show the slot.
- \smash{\makebox[1.5em]{\ensuremath{#2}}}
- }%
- {% No vector, no slot.
- \smash{\makebox[1.5em]{\ensuremath{}}}
- }%
- }%
+\NewDocumentCommand{\slot}{ s d[] }%
{%
- \IfValueTF{#2}
- {% Insert a vector and show the slot.
- \underline{\smash{\makebox[1.5em]{\ensuremath{#2}}}}
+ % d[] must be used because of the way consecutive optional
+ % arguments are handled. See xparse docs for details.
+ \IfBooleanTF{#1}
+ {%
+ \IfValueTF{#2}
+ {% Insert a vector, but don't show the slot.
+ \smash{\makebox[1.5em]{\ensuremath{#2}}}
+ }%
+ {% No vector, no slot.
+ \smash{\makebox[1.5em]{\ensuremath{}}}
+ }%
}%
- {% No vector; just show the slot.
- \underline{\smash{\makebox[1.5em]{\ensuremath{}}}}
+ {%
+ \IfValueTF{#2}
+ {% Insert a vector and show the slot.
+ \underline{\smash{\makebox[1.5em]{\ensuremath{#2}}}}
+ }%
+ {% No vector; just show the slot.
+ \underline{\smash{\makebox[1.5em]{\ensuremath{}}}}
+ }%
}%
}%
-}%
% \end{macrocode}
%
% Intelligent differential (exterior derivative) operator.
%
% \begin{macrocode}
-\NewDocumentCommand{\diff}{ s }{%
- \mathop{}\!
- \IfBooleanTF{#1}
- {\symbfsfup{d}}%
- {\symsfup{d}}%
-}%
+\NewDocumentCommand{\df}{ s }%
+ {%
+ \mathop{}\!%
+ \IfBooleanTF{#1}%
+ {%
+ \symbfsfup{d}%
+ }%
+ {%
+ \symsfup{d}%
+ }%
+ }%
% \end{macrocode}
%
% Here is a clever way to color digits in program listsings thanks to
@@ -1633,151 +1852,213 @@ while t < 10:
\definecolor{gspeach} {rgb}{1.00,0.90,0.71} % peach
\definecolor{gspearl} {rgb}{0.94,0.92,0.84} % pearl
\definecolor{gsplum} {rgb}{0.74,0.46,0.70} % plum
-\lstdefinestyle{vpython}{% % style for listings
- backgroundcolor=\color{gsbggray},% % background color
- basicstyle=\colordigits\footnotesize,% % default style
- breakatwhitespace=true% % break at whitespace
- breaklines=true,% % break long lines
- captionpos=b,% % position caption
- classoffset=1,% % STILL DON'T UNDERSTAND THIS
- commentstyle=\color{gsgray},% % font for comments
- deletekeywords={print},% % delete keywords from the given language
- emph={self,cls,@classmethod,@property},% % words to emphasize
- emphstyle=\color{gsorange}\itshape,% % font for emphasis
- escapeinside={(*@}{@*)},% % add LaTeX within your code
- frame=tb,% % frame style
- framerule=2.0pt,% % frame thickness
- framexleftmargin=5pt,% % extra frame left margin
- %identifierstyle=\sffamily,% % style for identifiers
- keywordstyle=\gsfontfamily\color{gsplum},% % color for keywords
- language=Python,% % select language
- linewidth=\linewidth,% % width of listings
- morekeywords={% % VPython/GlowScript specific keywords
- __future__,abs,acos,align,ambient,angle,append,append_to_caption,%
- append_to_title,arange,arrow,asin,astuple,atan,atan2,attach_arrow,%
- attach_trail,autoscale,axis,background,billboard,bind,black,blue,border,%
- bounding_box,box,bumpaxis,bumpmap,bumpmaps,camera,canvas,caption,capture,%
- ceil,center,clear,clear_trail,click,clone,CoffeeScript,coils,color,combin,%
- comp,compound,cone,convex,cos,cross,curve,cyan,cylinder,data,degrees,del,%
- delete,depth,descender,diff_angle,digits,division,dot,draw_complete,%
- ellipsoid,emissive,end_face_color,equals,explog,extrusion,faces,factorial,%
- False,floor,follow,font,format,forward,fov,frame,gcurve,gdisplay,gdots,%
- get_library,get_selected,ghbars,global,GlowScript,graph,graphs,green,gvbars,%
- hat,headlength,headwidth,height,helix,hsv_to_rgb,index,interval,keydown,%
- keyup,label,length,lights,line,linecolor,linewidth,logx,logy,lower_left,%
- lower_right,mag,mag2,magenta,make_trail,marker_color,markers,material,%
- max,min,mouse,mousedown,mousemove,mouseup,newball,norm,normal,objects,%
- offset,one,opacity,orange,origin,path,pause,pi,pixel_to_world,pixels,plot,%
- points,pos,pow,pps,print,print_function,print_options,proj,purple,pyramid,%
- quad,radians,radius,random,rate,ray,read_local_file,readonly,red,redraw,%
- retain,rgb_to_hsv,ring,rotate,round,scene,scroll,shaftwidth,shape,shapes,%
- shininess,show_end_face,show_start_face,sign,sin,size,size_units,sleep,%
- smooth,space,sphere,sqrt,start,start_face_color,stop,tan,text,textpos,%
- texture,textures,thickness,title,trail_color,trail_object,trail_radius,%
- trail_type,triangle,trigger,True,twist,unbind,up,upper_left,upper_right,%
- userpan,userspin,userzoom,vec,vector,vertex,vertical_spacing,visible,%
- visual,vpython,VPython,waitfor,white,width,world,xtitle,yellow,yoffset,%
- ytitle%
- },%
- morekeywords={print,None,TypeError},% % additional keywords
- morestring=[b]{"""},% % treat triple quotes as strings
- numbers=left,% % where to put line numbers
- numbersep=10pt,% % how far line numbers are from code
- numberstyle=\bfseries\tiny,% % set to 'none' for no line numbers
- showstringspaces=false,% % show spaces in strings
- showtabs=false,% % show tabs within strings
- stringstyle=\gsfontfamily\color{gsgreen},% % color for strings
- upquote=true,% % how to typeset quotes
-}%
+\lstdefinestyle{vpython}%
+ {% % style for listings
+ backgroundcolor=\color{gsbggray},% % background color
+ basicstyle=\colordigits\footnotesize,% % default style
+ breakatwhitespace=true% % break at whitespace
+ breaklines=true,% % break long lines
+ captionpos=b,% % position caption
+ classoffset=1,% % STILL DON'T UNDERSTAND THIS
+ commentstyle=\color{gsgray},% % font for comments
+ deletekeywords={print},% % delete keywords from the given language
+ emph={self,cls,@classmethod,@property},% % words to emphasize
+ emphstyle=\color{gsorange}\itshape,% % font for emphasis
+ escapeinside={(*@}{@*)},% % add LaTeX within your code
+ frame=tb,% % frame style
+ framerule=2.0pt,% % frame thickness
+ framexleftmargin=5pt,% % extra frame left margin
+ %identifierstyle=\sffamily,% % style for identifiers
+ keywordstyle=\gsfontfamily\color{gsplum},% % color for keywords
+ language=Python,% % select language
+ linewidth=\linewidth,% % width of listings
+ morekeywords={% % VPython/Web VPython specific keywords
+ __future__,abs,acos,align,ambient,angle,append,append_to_caption,%
+ append_to_title,arange,arrow,asin,astuple,atan,atan2,attach_arrow,%
+ attach_trail,autoscale,axis,background,billboard,bind,black,blue,border,%
+ bounding_box,box,bumpaxis,bumpmap,bumpmaps,camera,canvas,caption,capture,%
+ ceil,center,clear,clear_trail,click,clone,CoffeeScript,coils,color,combin,%
+ comp,compound,cone,convex,cos,cross,curve,cyan,cylinder,data,degrees,del,%
+ delete,depth,descender,diff_angle,digits,division,dot,draw_complete,%
+ ellipsoid,emissive,end_face_color,equals,explog,extrusion,faces,factorial,%
+ False,floor,follow,font,format,forward,fov,frame,gcurve,gdisplay,gdots,%
+ get_library,get_selected,ghbars,global,GlowScript,graph,graphs,green,gvbars,%
+ hat,headlength,headwidth,height,helix,hsv_to_rgb,index,interval,keydown,%
+ keyup,label,length,lights,line,linecolor,linewidth,logx,logy,lower_left,%
+ lower_right,mag,mag2,magenta,make_trail,marker_color,markers,material,%
+ max,min,mouse,mousedown,mousemove,mouseup,newball,norm,normal,objects,%
+ offset,one,opacity,orange,origin,path,pause,pi,pixel_to_world,pixels,plot,%
+ points,pos,pow,pps,print,print_function,print_options,proj,purple,pyramid,%
+ quad,radians,radius,random,rate,ray,read_local_file,readonly,red,redraw,%
+ retain,rgb_to_hsv,ring,rotate,round,scene,scroll,shaftwidth,shape,shapes,%
+ shininess,show_end_face,show_start_face,sign,sin,size,size_units,sleep,%
+ smooth,space,sphere,sqrt,start,start_face_color,stop,tan,text,textpos,%
+ texture,textures,thickness,title,trail_color,trail_object,trail_radius,%
+ trail_type,triangle,trigger,True,twist,unbind,up,upper_left,upper_right,%
+ userpan,userspin,userzoom,vec,vector,vertex,vertical_spacing,visible,%
+ visual,vpython,VPython,waitfor,WebVPython,white,width,world,xtitle,%
+ yellow,yoffset,ytitle%
+ },%
+ morekeywords={print,None,TypeError},% % additional keywords
+ morestring=[b]{"""},% % treat triple quotes as strings
+ numbers=left,% % where to put line numbers
+ numbersep=10pt,% % how far line numbers are from code
+ numberstyle=\bfseries\tiny,% % set to 'none' for no line numbers
+ showstringspaces=false,% % show spaces in strings
+ showtabs=false,% % show tabs within strings
+ stringstyle=\gsfontfamily\color{gsgreen},% % color for strings
+ upquote=true,% % how to typeset quotes
+ }%
% \end{macrocode}
%
-% Introduce a new, more intelligent \refEnv{glowscriptblock} environment.
+% Introduce a new, more intelligent \refEnv{webvpythonblock} environment.\newline
+% See \url{https://tex.stackexchange.com/a/232208/218142}.
%
+% \changes{v3.1.0}{2022-01-27}
+% {\linktoplace{sec:mandistudentpkg}{mandistudent} URLs fixed in \refEnv{webvpythonblock}}
+% \changes{v3.1.0}{2022-01-27}
+% {\linktoplace{sec:mandistudentpkg}{mandistudent} \refEnv{webvpythonblock} now automatically
+% generates QR codes for program listings}
% \begin{macrocode}
-\NewTCBListing[auto counter,list inside=gsprogs]{glowscriptblock}
- { O{} D(){glowscript.org} m }{%
- breakable,%
- center,%
- code = \newpage,%
- %derivpeach,%
- enhanced,%
- hyperurl interior = https://#2,%
- label = {gs:\thetcbcounter},%
- left = 8mm,%
- list entry = \thetcbcounter~~~~~#3,%
- listing only,%
- listing style = vpython,%
- nameref = {#3},%
- title = \texttt{GlowScript} Program \thetcbcounter: #3,%
- width = 0.9\textwidth,%
- {#1},
-}%
+\AtBeginEnvironment{webvpythonblock}{\catcode`\#=12}
+\AtEndEnvironment{webvpythonblock}{\catcode`\#=6}
+\NewTCBListing[auto counter,list inside=gsprogs]{webvpythonblock}{ O{} D(){webvpython.org} m }%
+ {%
+ breakable,%
+ center,%
+ code = \newpage,%
+ %derivpeach,%
+ enhanced,%
+ hyperurl interior = https://#2,%
+ label = {gs:\thetcbcounter},%
+ left = 8mm,%
+ list entry = \thetcbcounter~~~~~#3,%
+ listing only,%
+ listing style = vpython,%
+ nameref = {#3},%
+ title = \begin{minipage}{1.5cm}%
+ \protect\qrcode*{https://#2}%
+ \end{minipage}\hspace{5mm}%
+ \begin{minipage}{0.7\textwidth}%
+ \texttt{Web VPython} Program \thetcbcounter: #3%
+ \end{minipage},%
+ width = 0.9\textwidth,%
+ {#1},
+ }%
% \end{macrocode}
%
-% A new command for generating a list of \GlowScript\ programs.
+% Here is a variant that omits the QR code.
%
+% \changes{v3.1.0}{2022-01-27}
+% {\linktoplace{sec:mandistudentpkg}{mandistudent} \refEnv{webvpythonblock*} is a variant
+% of \refEnv{webvpythonblock} that omits the QR code}
% \begin{macrocode}
-\NewDocumentCommand{\listofglowscriptprograms}{}{\tcblistof[\section*]{gsprogs}
- {List of \texttt{GlowScript} Programs}}%
+\AtBeginEnvironment{webvpythonblock*}{\catcode`\#=12}
+\AtEndEnvironment{webvpythonblock*}{\catcode`\#=6}
+\NewTCBListing[use counter from=webvpythonblock,list inside=gsprogs]
+ {webvpythonblock*}{ O{} D(){webvpython.org} m }%
+ {%
+ breakable,%
+ center,%
+ code = \newpage,%
+ %derivpeach,%
+ enhanced,%
+ hyperurl interior = https://#2,%
+ label = {gs:\thetcbcounter},%
+ left = 8mm,%
+ list entry = \thetcbcounter~~~~~#3,%
+ listing only,%
+ listing style = vpython,%
+ nameref = {#3},%
+ title = \texttt{Web VPython} Program \thetcbcounter: #3,%
+ width = 0.9\textwidth,%
+ {#1},
+ }%
% \end{macrocode}
%
-% Introduce a new, more intelligent \refCom{vpythonfile} command.
+% A new command for generating a list of \WebVPython\ programs.
%
% \begin{macrocode}
-\NewTCBInputListing[auto counter,list inside=vpprogs]{\vpythonfile}
- { O{} m m }{%
- breakable,%
- center,%
- code = \newpage,%
- %derivgray,%
- enhanced,%
- hyperurl interior = https://,%
- label = {vp:\thetcbcounter},%
- left = 8mm,%
- list entry = \thetcbcounter~~~~~#3,%
- listing file = {#2},%
- listing only,%
- listing style = vpython,%
- nameref = {#3},%
- title = \texttt{VPython} Program \thetcbcounter: #3,%
- width = 0.9\textwidth,%
- {#1},%
-}%
+\NewDocumentCommand{\listofwebvpythonprograms}{}%
+ {%
+ \tcblistof[\section*]{gsprogs}{List of \texttt{Web VPython} Programs}%
+ }%
+% \end{macrocode}
+%
+% Introduce a new, more intelligent \refCom{vpythonfile} command.\newline
+% See \url{https://tex.stackexchange.com/q/616205/218142}.
+%
+% \changes{v3.1.0}{2022-01-27}
+% {\linktoplace{sec:mandistudentpkg}{mandistudent} URLs fixed in \refCom{vpythonfile}}
+% \changes{v3.1.0}{2022-01-27}
+% {\linktoplace{sec:mandistudentpkg}{mandistudent} Default URL for \refCom{vpythonfile}
+% is now \vpurl}
+% \begin{macrocode}
+\newcommand*{\vpythonfile}{\catcode`\#=12 \vpythonfile@auxA}
+\NewDocumentCommand{\vpythonfile@auxA}{ O{} D(){vpython.org} m m }%
+ {%
+ \vpythonfile@auxB[#1](#2){#3}{#4}%
+ \catcode`\#=6
+ }%
+\NewTCBInputListing[auto counter,list inside=vpprogs]
+ {\vpythonfile@auxB}{ O{} D(){vpython.org} m m }%
+ {%
+ breakable,%
+ center,%
+ code = \newpage,%
+ %derivgray,%
+ enhanced,%
+ hyperurl interior = https://#2,%
+ label = {vp:\thetcbcounter},%
+ left = 8mm,%
+ list entry = \thetcbcounter~~~~~#4,%
+ listing file = {#3},%
+ listing only,%
+ listing style = vpython,%
+ nameref = {#4},%
+ title = \texttt{VPython} Program \thetcbcounter: #4,%
+ width = 0.9\textwidth,%
+ {#1},%
+ }%
% \end{macrocode}
%
% A new command for generating a list of \VPython\ programs.
%
% \begin{macrocode}
-\NewDocumentCommand{\listofvpythonprograms}{}{\tcblistof[\section*]{vpprogs}
- {List of \texttt{VPython} Programs}}%
+\NewDocumentCommand{\listofvpythonprograms}{}%
+ {%
+ \tcblistof[\section*]{vpprogs}{List of \texttt{VPython} Programs}%
+ }%
% \end{macrocode}
%
-% Introduce a new \refCom{glowscriptinline} command.
+% Introduce a new \refCom{webvpythoninline} command.
%
% \begin{macrocode}
-\DeclareTotalTCBox{\glowscriptinline}{ m }{%
- bottom = 0pt,%
- bottomrule = 0.0mm,%
- boxsep = 1.0mm,%
- colback = gsbggray,%
- colframe = gsbggray,%
- left = 0pt,%
- leftrule = 0.0mm,%
- nobeforeafter,%
- right = 0pt,%
- rightrule = 0.0mm,%
- sharp corners,%
- tcbox raise base,%
- top = 0pt,%
- toprule = 0.0mm,%
-}{\lstinline[style = vpython]{#1}}%
+\DeclareTotalTCBox{\webvpythoninline}{ m }%
+ {%
+ bottom = 0pt,%
+ bottomrule = 0.0mm,%
+ boxsep = 1.0mm,%
+ colback = gsbggray,%
+ colframe = gsbggray,%
+ left = 0pt,%
+ leftrule = 0.0mm,%
+ nobeforeafter,%
+ right = 0pt,%
+ rightrule = 0.0mm,%
+ sharp corners,%
+ tcbox raise base,%
+ top = 0pt,%
+ toprule = 0.0mm,%
+ }%
+ {\lstinline[style = vpython]{#1}}%
% \end{macrocode}
%
% Define \refCom{vpythoninline}, a semantic alias for \VPython\
% in-line listings.
%
% \begin{macrocode}
-\NewDocumentCommand{\vpythoninline}{}{\glowscriptinline}%
+\NewDocumentCommand{\vpythoninline}{}{\webvpythoninline}%
% \end{macrocode}
%
% \restoregeometry
diff --git a/Master/texmf-dist/tex/latex/mandi/mandi.sty b/Master/texmf-dist/tex/latex/mandi/mandi.sty
index 508e7317e50..8d712ebb943 100644
--- a/Master/texmf-dist/tex/latex/mandi/mandi.sty
+++ b/Master/texmf-dist/tex/latex/mandi/mandi.sty
@@ -6,7 +6,7 @@
%%
%% mandi.dtx (with options: `package')
%%
-%% Copyright (C) 2021 by Paul J. Heafner <heafnerj@gmail.com>
+%% Copyright (C) 2021,2022 by Paul J. Heafner <heafnerj@gmail.com>
%% ---------------------------------------------------------------------------
%% 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
@@ -29,22 +29,25 @@
%% and includes the derived files mandi.sty
%% mandistudent.sty
%% mandiexp.sty
-%% vdemo.py
+%% vdemo.py (not needed)
%% ---------------------------------------------------------------------------
%%
-\def\mandi@version{3.0.0}
-\def\mandi@date{2021-08-22}
+\def\mandi@version{3.1.0}
+\def\mandi@date{2022-01-27}
\NeedsTeXFormat{LaTeX2e}[2020-02-02]
-\DeclareRelease{v3.0.0}{2021-08-22}{mandi.sty}
+\DeclareRelease{v3.1.0}{2022-01-27}{mandi.sty}
\DeclareCurrentRelease{v\mandi@version}{\mandi@date}
\ProvidesPackage{mandi}
[\mandi@date\space v\mandi@version\space Macros for physical quantities]
\newcommand*{\mandiversion}{v\mandi@version\space dated \mandi@date}
-\RequirePackage{pgfopts} % needed for key-value interface
-\RequirePackage{array} % needed for \checkquantity and \checkconstant
-\RequirePackage{iftex} % needed for requiring LuaLaTeX
-\RequirePackage{unicode-math} % needed for Unicode support
-\RequireLuaTeX % require this engine
+\RequirePackage{pgfopts} % needed for key-value interface
+\RequirePackage{array} % needed for \checkquantity and \checkconstant
+\RequirePackage{iftex} % needed for requiring LuaLaTeX
+\RequirePackage{unicode-math} % needed for Unicode support
+\IfFormatAtLeastTF {2020-10-01} % load xparse if necessary
+ {}%
+ {\RequirePackage{xparse}}%
+\RequireLuaTeX % require this engine
\newcommand*{\mandi@selectunits}{}
\newcommand*{\mandi@selectprecision}{}
\newcommand*{\mandi@selectapproximate}[2]{#1} % really \@firstoftwo
@@ -85,6 +88,10 @@
units/alternate/.style={/mandi/options/buffered@units=alternate},%
units/base/.style={/mandi/options/buffered@units=base},%
units/derived/.style={/mandi/options/buffered@units=derived},%
+ .unknown/.code={%
+ \typeout{}%
+ \typeout{mandi: You used unknown option '\pgfkeyscurrentname'.}%
+ },%
}%
\ProcessPgfPackageOptions{/mandi/options}
\typeout{}%
@@ -104,14 +111,16 @@
\typeout{}%
}%
\mandi@do@setup
-\NewDocumentCommand{\mandisetup}{ m }{%
- \IfValueT{#1}{%
- \pgfqkeys{/mandi/options}{#1}
- \typeout{}%
- \typeout{mandi: mandisetup options...}
- \mandi@do@setup
+\NewDocumentCommand{\mandisetup}{ m }%
+ {%
+ \IfValueT{#1}%
+ {%
+ \pgfqkeys{/mandi/options}{#1}
+ \typeout{}%
+ \typeout{mandi: mandisetup options...}
+ \mandi@do@setup
+ }%
}%
-}%
\NewDocumentCommand{\per}{}{/}
\NewDocumentCommand{\usk}{}{\cdot}
\NewDocumentCommand{\unit}{ m m }{{#1}{\,#2}}
@@ -130,7 +139,7 @@
\NewDocumentCommand{\kev}{}{\kiloelectronvolt}
\NewDocumentCommand{\kiloelectronvolt}{}{\symup{keV}}
\NewDocumentCommand{\kilogram}{}{\symup{kg}}
-\NewDocumentCommand{\lightspeed}{}{\symup{c}}
+\NewDocumentCommand{\lightspeed}{}{\!\symup{c}}
\NewDocumentCommand{\megaelectronvolt}{}{\symup{MeV}}
\NewDocumentCommand{\meter}{}{\symup{m}}
\NewDocumentCommand{\metre}{}{\meter}
@@ -159,134 +168,134 @@
\NewDocumentCommand{\timestento}{ m }{\times\tento{#1}}
\NewDocumentCommand{\xtento}{ m }{\times\tento{#1}}
\ExplSyntaxOn
-\cs_new:Npn \mandi_newscalarquantity #1#2#3#4
-{%
- \cs_new:cpn {#1} ##1 {\unit{##1}{\mandi@selectunits{#2}{#3}{#4}}}%
- \cs_new:cpn {#1value} ##1 {##1}%
- \cs_new:cpn {#1baseunits} ##1 {\unit{##1}{\mandi@selectbaseunits{#2}{#3}{#4}}}%
- \cs_new:cpn {#1derivedunits} ##1 {\unit{##1}{\mandi@selectderivedunits{#2}{#3}{#4}}}%
- \cs_new:cpn {#1alternateunits} ##1 {\unit{##1}{\mandi@selectalternateunits{#2}{#3}{#4}}}%
- \cs_new:cpn {#1onlybaseunits} {\mandi@selectbaseunits{#2}{#3}{#4}}%
- \cs_new:cpn {#1onlyderivedunits} {\mandi@selectderivedunits{#2}{#3}{#4}}%
- \cs_new:cpn {#1onlyalternateunits} {\mandi@selectalternateunits{#2}{#3}{#4}}%
-}%
-\NewDocumentCommand{\newscalarquantity}{ m m O{#2} O{#2} }%
-{%
- \mandi_newscalarquantity { #1 }{ #2 }{ #3 }{ #4 }%
-}%
+\cs_new:Npn \__mandi_newscalarquantity:nnnn #1#2#3#4
+ {
+ \cs_new:cpn {#1} ##1 {\unit{##1}{\mandi@selectunits{#2}{#3}{#4}}}
+ \cs_new:cpn {#1value} ##1 {##1}
+ \cs_new:cpn {#1baseunits} ##1 {\unit{##1}{\mandi@selectbaseunits{#2}{#3}{#4}}}
+ \cs_new:cpn {#1derivedunits} ##1 {\unit{##1}{\mandi@selectderivedunits{#2}{#3}{#4}}}
+ \cs_new:cpn {#1alternateunits} ##1 {\unit{##1}{\mandi@selectalternateunits{#2}{#3}{#4}}}
+ \cs_new:cpn {#1onlybaseunits} {\mandi@selectbaseunits{#2}{#3}{#4}}
+ \cs_new:cpn {#1onlyderivedunits} {\mandi@selectderivedunits{#2}{#3}{#4}}
+ \cs_new:cpn {#1onlyalternateunits} {\mandi@selectalternateunits{#2}{#3}{#4}}
+ }
+\NewDocumentCommand{\newscalarquantity}{ m m O{#2} O{#2} }
+ {
+ \__mandi_newscalarquantity:nnnn { #1 }{ #2 }{ #3 }{ #4 }
+ }
\ExplSyntaxOff
\ExplSyntaxOn
-\cs_new:Npn \mandi_renewscalarquantity #1#2#3#4
-{%
- \cs_set:cpn {#1} ##1 {\unit{##1}{\mandi@selectunits{#2}{#3}{#4}}}%
- \cs_set:cpn {#1value} ##1 {##1}%
- \cs_set:cpn {#1baseunits} ##1 {\unit{##1}{\mandi@selectbaseunits{#2}{#3}{#4}}}%
- \cs_set:cpn {#1derivedunits} ##1 {\unit{##1}{\mandi@selectderivedunits{#2}{#3}{#4}}}%
- \cs_set:cpn {#1alternateunits} ##1 {\unit{##1}{\mandi@selectalternateunits{#2}{#3}{#4}}}%
- \cs_set:cpn {#1onlybaseunits} {\mandi@selectbaseunits{#2}{#3}{#4}}%
- \cs_set:cpn {#1onlyderivedunits} {\mandi@selectderivedunits{#2}{#3}{#4}}%
- \cs_set:cpn {#1onlyalternateunits} {\mandi@selectalternateunits{#2}{#3}{#4}}%
-}%
-\NewDocumentCommand{\renewscalarquantity}{ m m O{#2} O{#2} }%
-{%
- \mandi_renewscalarquantity { #1 }{ #2 }{ #3 }{ #4 }%
-}%
+\cs_new:Npn \__mandi_renewscalarquantity:nnnn #1#2#3#4
+ {
+ \cs_set:cpn {#1} ##1 {\unit{##1}{\mandi@selectunits{#2}{#3}{#4}}}
+ \cs_set:cpn {#1value} ##1 {##1}
+ \cs_set:cpn {#1baseunits} ##1 {\unit{##1}{\mandi@selectbaseunits{#2}{#3}{#4}}}
+ \cs_set:cpn {#1derivedunits} ##1 {\unit{##1}{\mandi@selectderivedunits{#2}{#3}{#4}}}
+ \cs_set:cpn {#1alternateunits} ##1 {\unit{##1}{\mandi@selectalternateunits{#2}{#3}{#4}}}
+ \cs_set:cpn {#1onlybaseunits} {\mandi@selectbaseunits{#2}{#3}{#4}}
+ \cs_set:cpn {#1onlyderivedunits} {\mandi@selectderivedunits{#2}{#3}{#4}}
+ \cs_set:cpn {#1onlyalternateunits} {\mandi@selectalternateunits{#2}{#3}{#4}}
+ }
+\NewDocumentCommand{\renewscalarquantity}{ m m O{#2} O{#2} }
+ {
+ \__mandi_renewscalarquantity:nnnn { #1 }{ #2 }{ #3 }{ #4 }
+ }
\ExplSyntaxOff
\ExplSyntaxOn
-\cs_new:Npn \mandi_newvectorquantity #1#2#3#4
-{%
- \mandi_newscalarquantity { #1 }{ #2 }{ #3 }{ #4 }%
- \cs_new:cpn {vector#1} ##1 {\unit{\mivector{##1}}{\mandi@selectunits{#2}{#3}{#4}}}%
- \cs_new:cpn {#1vector} ##1 {\unit{\mivector{##1}}{\mandi@selectunits{#2}{#3}{#4}}}%
- \cs_new:cpn {vector#1value} ##1 {\mivector{##1}}%
- \cs_new:cpn {#1vectorvalue} ##1 {\mivector{##1}}%
- \cs_new:cpn {vector#1baseunits} ##1 {\unit{\mivector{##1}}{\mandi@selectbaseunits{#2}{#3}{#4}}}%
- \cs_new:cpn {#1vectorbaseunits} ##1 {\unit{\mivector{##1}}{\mandi@selectbaseunits{#2}{#3}{#4}}}%
- \cs_new:cpn {vector#1derivedunits} ##1 {\unit{\mivector{##1}}{\mandi@selectderivedunits{#2}{#3}{#4}}}%
- \cs_new:cpn {#1vectorderivedunits} ##1 {\unit{\mivector{##1}}{\mandi@selectderivedunits{#2}{#3}{#4}}}%
- \cs_new:cpn {vector#1alternateunits} ##1 {\unit{\mivector{##1}}{\mandi@selectalternateunits{#2}{#3}{#4}}}%
- \cs_new:cpn {#1vectoralternateunits} ##1 {\unit{\mivector{##1}}{\mandi@selectalternateunits{#2}{#3}{#4}}}%
- \cs_new:cpn {vector#1onlybaseunits} {\mandi@selectbaseunits{#2}{#3}{#4}}%
- \cs_new:cpn {#1vectoronlybaseunits} {\mandi@selectbaseunits{#2}{#3}{#4}}%
- \cs_new:cpn {vector#1onlyderivedunits} {\mandi@selectderivedunits{#2}{#3}{#4}}%
- \cs_new:cpn {#1vectoronlyderivedunits} {\mandi@selectderivedunits{#2}{#3}{#4}}%
- \cs_new:cpn {vector#1onlyalternateunits} {\mandi@selectalternateunits{#2}{#3}{#4}}%
- \cs_new:cpn {#1vectoronlyalternateunits} {\mandi@selectalternateunits{#2}{#3}{#4}}%
-}%
-\NewDocumentCommand{\newvectorquantity}{ m m O{#2} O{#2} }%
-{%
- \mandi_newvectorquantity { #1 }{ #2 }{ #3 }{ #4 }%
-}%
+\cs_new:Npn \__mandi_newvectorquantity:nnnn #1#2#3#4
+ {
+ \__mandi_newscalarquantity:nnnn { #1 }{ #2 }{ #3 }{ #4 }
+ \cs_new:cpn {vector#1} ##1 {\unit{\mivector{##1}}{\mandi@selectunits{#2}{#3}{#4}}}
+ \cs_new:cpn {#1vector} ##1 {\unit{\mivector{##1}}{\mandi@selectunits{#2}{#3}{#4}}}
+ \cs_new:cpn {vector#1value} ##1 {\mivector{##1}}
+ \cs_new:cpn {#1vectorvalue} ##1 {\mivector{##1}}
+ \cs_new:cpn {vector#1baseunits} ##1 {\unit{\mivector{##1}}{\mandi@selectbaseunits{#2}{#3}{#4}}}
+ \cs_new:cpn {#1vectorbaseunits} ##1 {\unit{\mivector{##1}}{\mandi@selectbaseunits{#2}{#3}{#4}}}
+ \cs_new:cpn {vector#1derivedunits} ##1 {\unit{\mivector{##1}}{\mandi@selectderivedunits{#2}{#3}{#4}}}
+ \cs_new:cpn {#1vectorderivedunits} ##1 {\unit{\mivector{##1}}{\mandi@selectderivedunits{#2}{#3}{#4}}}
+ \cs_new:cpn {vector#1alternateunits} ##1 {\unit{\mivector{##1}}{\mandi@selectalternateunits{#2}{#3}{#4}}}
+ \cs_new:cpn {#1vectoralternateunits} ##1 {\unit{\mivector{##1}}{\mandi@selectalternateunits{#2}{#3}{#4}}}
+ \cs_new:cpn {vector#1onlybaseunits} {\mandi@selectbaseunits{#2}{#3}{#4}}
+ \cs_new:cpn {#1vectoronlybaseunits} {\mandi@selectbaseunits{#2}{#3}{#4}}
+ \cs_new:cpn {vector#1onlyderivedunits} {\mandi@selectderivedunits{#2}{#3}{#4}}
+ \cs_new:cpn {#1vectoronlyderivedunits} {\mandi@selectderivedunits{#2}{#3}{#4}}
+ \cs_new:cpn {vector#1onlyalternateunits} {\mandi@selectalternateunits{#2}{#3}{#4}}
+ \cs_new:cpn {#1vectoronlyalternateunits} {\mandi@selectalternateunits{#2}{#3}{#4}}
+ }
+\NewDocumentCommand{\newvectorquantity}{ m m O{#2} O{#2} }
+ {
+ \__mandi_newvectorquantity:nnnn { #1 }{ #2 }{ #3 }{ #4 }
+ }
\ExplSyntaxOff
\ExplSyntaxOn
-\cs_new:Npn \mandi_renewvectorquantity #1#2#3#4
-{%
- \mandi_renewscalarquantity { #1 }{ #2 }{ #3 }{ #4 }%
- \cs_set:cpn {vector#1} ##1 {\unit{\mivector{##1}}{\mandi@selectunits{#2}{#3}{#4}}}%
- \cs_set:cpn {#1vector} ##1 {\unit{\mivector{##1}}{\mandi@selectunits{#2}{#3}{#4}}}%
- \cs_set:cpn {vector#1value} ##1 {\mivector{##1}}%
- \cs_set:cpn {#1vectorvalue} ##1 {\mivector{##1}}%
- \cs_set:cpn {vector#1baseunits} ##1 {\unit{\mivector{##1}}{\mandi@selectbaseunits{#2}{#3}{#4}}}%
- \cs_set:cpn {#1vectorbaseunits} ##1 {\unit{\mivector{##1}}{\mandi@selectbaseunits{#2}{#3}{#4}}}%
- \cs_set:cpn {vector#1derivedunits} ##1 {\unit{\mivector{##1}}{\mandi@selectderivedunits{#2}{#3}{#4}}}%
- \cs_set:cpn {#1vectorderivedunits} ##1 {\unit{\mivector{##1}}{\mandi@selectderivedunits{#2}{#3}{#4}}}%
- \cs_set:cpn {vector#1alternateunits} ##1 {\unit{\mivector{##1}}{\mandi@selectalternateunits{#2}{#3}{#4}}}%
- \cs_set:cpn {#1vectoralternateunits} ##1 {\unit{\mivector{##1}}{\mandi@selectalternateunits{#2}{#3}{#4}}}%
- \cs_set:cpn {vector#1onlybaseunits} {\mandi@selectbaseunits{#2}{#3}{#4}}%
- \cs_set:cpn {#1vectoronlybaseunits} {\mandi@selectbaseunits{#2}{#3}{#4}}%
- \cs_set:cpn {vector#1onlyderivedunits} {\mandi@selectderivedunits{#2}{#3}{#4}}%
- \cs_set:cpn {#1vectoronlyderivedunits} {\mandi@selectderivedunits{#2}{#3}{#4}}%
- \cs_set:cpn {vector#1onlyalternateunits} {\mandi@selectalternateunits{#2}{#3}{#4}}%
- \cs_set:cpn {#1vectoronlyalternateunits} {\mandi@selectalternateunits{#2}{#3}{#4}}%
-}%
-\NewDocumentCommand{\renewvectorquantity}{ m m O{#2} O{#2} }%
-{%
- \mandi_renewvectorquantity { #1 }{ #2 }{ #3 }{ #4 }%
-}%
+\cs_new:Npn \__mandi_renewvectorquantity:nnnn #1#2#3#4
+ {
+ \__mandi_renewscalarquantity:nnnn { #1 }{ #2 }{ #3 }{ #4 }
+ \cs_set:cpn {vector#1} ##1 {\unit{\mivector{##1}}{\mandi@selectunits{#2}{#3}{#4}}}
+ \cs_set:cpn {#1vector} ##1 {\unit{\mivector{##1}}{\mandi@selectunits{#2}{#3}{#4}}}
+ \cs_set:cpn {vector#1value} ##1 {\mivector{##1}}
+ \cs_set:cpn {#1vectorvalue} ##1 {\mivector{##1}}
+ \cs_set:cpn {vector#1baseunits} ##1 {\unit{\mivector{##1}}{\mandi@selectbaseunits{#2}{#3}{#4}}}
+ \cs_set:cpn {#1vectorbaseunits} ##1 {\unit{\mivector{##1}}{\mandi@selectbaseunits{#2}{#3}{#4}}}
+ \cs_set:cpn {vector#1derivedunits} ##1 {\unit{\mivector{##1}}{\mandi@selectderivedunits{#2}{#3}{#4}}}
+ \cs_set:cpn {#1vectorderivedunits} ##1 {\unit{\mivector{##1}}{\mandi@selectderivedunits{#2}{#3}{#4}}}
+ \cs_set:cpn {vector#1alternateunits} ##1 {\unit{\mivector{##1}}{\mandi@selectalternateunits{#2}{#3}{#4}}}
+ \cs_set:cpn {#1vectoralternateunits} ##1 {\unit{\mivector{##1}}{\mandi@selectalternateunits{#2}{#3}{#4}}}
+ \cs_set:cpn {vector#1onlybaseunits} {\mandi@selectbaseunits{#2}{#3}{#4}}
+ \cs_set:cpn {#1vectoronlybaseunits} {\mandi@selectbaseunits{#2}{#3}{#4}}
+ \cs_set:cpn {vector#1onlyderivedunits} {\mandi@selectderivedunits{#2}{#3}{#4}}
+ \cs_set:cpn {#1vectoronlyderivedunits} {\mandi@selectderivedunits{#2}{#3}{#4}}
+ \cs_set:cpn {vector#1onlyalternateunits} {\mandi@selectalternateunits{#2}{#3}{#4}}
+ \cs_set:cpn {#1vectoronlyalternateunits} {\mandi@selectalternateunits{#2}{#3}{#4}}
+ }
+\NewDocumentCommand{\renewvectorquantity}{ m m O{#2} O{#2} }
+ {
+ \__mandi_renewvectorquantity:nnnn { #1 }{ #2 }{ #3 }{ #4 }
+ }
\ExplSyntaxOff
\ExplSyntaxOn
-\cs_new:Npn \mandi_newphysicalconstant #1#2#3#4#5#6#7
-{%
- \cs_new:cpn {#1} {\unit{\mandi@selectprecision{#3}{#4}}{\mandi@selectunits{#5}{#6}{#7}}}%
- \cs_new:cpn {#1mathsymbol} {#2}%
- \cs_new:cpn {#1approximatevalue} {#3}%
- \cs_new:cpn {#1precisevalue} {#4}%
- \cs_new:cpn {#1baseunits}
- {\unit{\mandi@selectprecision{#3}{#4}}{\mandi@selectbaseunits{#5}{#6}{#7}}}%
- \cs_new:cpn {#1derivedunits}
- {\unit{\mandi@selectprecision{#3}{#4}}{\mandi@selectderivedunits{#5}{#6}{#7}}}%
- \cs_new:cpn {#1alternateunits}
- {\unit{\mandi@selectprecision{#3}{#4}}{\mandi@selectalternateunits{#5}{#6}{#7}}}%
- \cs_new:cpn {#1onlybaseunits} {\mandi@selectbaseunits{#5}{#6}{#7}}%
- \cs_new:cpn {#1onlyderivedunits} {\mandi@selectderivedunits{#5}{#6}{#7}}%
- \cs_new:cpn {#1onlyalternateunits} {\mandi@selectalternateunits{#5}{#6}{#7}}%
-}%
-\NewDocumentCommand{\newphysicalconstant}{ m m m m m O{#5} O{#5} }%
-{%
- \mandi_newphysicalconstant { #1 }{ #2 }{ #3 }{ #4 }{ #5 }{ #6 }{ #7 }%
-}%
+\cs_new:Npn \__mandi_newphysicalconstant:nnnnnnn #1#2#3#4#5#6#7
+ {
+ \cs_new:cpn {#1} {\unit{\mandi@selectprecision{#3}{#4}}{\mandi@selectunits{#5}{#6}{#7}}}
+ \cs_new:cpn {#1mathsymbol} {#2}
+ \cs_new:cpn {#1approximatevalue} {#3}
+ \cs_new:cpn {#1precisevalue} {#4}
+ \cs_new:cpn {#1baseunits}
+ {\unit{\mandi@selectprecision{#3}{#4}}{\mandi@selectbaseunits{#5}{#6}{#7}}}
+ \cs_new:cpn {#1derivedunits}
+ {\unit{\mandi@selectprecision{#3}{#4}}{\mandi@selectderivedunits{#5}{#6}{#7}}}
+ \cs_new:cpn {#1alternateunits}
+ {\unit{\mandi@selectprecision{#3}{#4}}{\mandi@selectalternateunits{#5}{#6}{#7}}}
+ \cs_new:cpn {#1onlybaseunits} {\mandi@selectbaseunits{#5}{#6}{#7}}
+ \cs_new:cpn {#1onlyderivedunits} {\mandi@selectderivedunits{#5}{#6}{#7}}
+ \cs_new:cpn {#1onlyalternateunits} {\mandi@selectalternateunits{#5}{#6}{#7}}
+ }
+\NewDocumentCommand{\newphysicalconstant}{ m m m m m O{#5} O{#5} }
+ {
+ \__mandi_newphysicalconstant:nnnnnnn { #1 }{ #2 }{ #3 }{ #4 }{ #5 }{ #6 }{ #7 }
+ }
\ExplSyntaxOff
\ExplSyntaxOn
-\cs_new:Npn \mandi_renewphysicalconstant #1#2#3#4#5#6#7
-{%
- \cs_set:cpn {#1} {\unit{\mandi@selectprecision{#3}{#4}}{\mandi@selectunits{#5}{#6}{#7}}}%
- \cs_set:cpn {#1mathsymbol} {#2}%
- \cs_set:cpn {#1approximatevalue} {#3}%
- \cs_set:cpn {#1precisevalue} {#4}%
- \cs_set:cpn {#1baseunits}
- {\unit{\mandi@selectprecision{#3}{#4}}{\mandi@selectbaseunits{#5}{#6}{#7}}}%
- \cs_set:cpn {#1derivedunits}
- {\unit{\mandi@selectprecision{#3}{#4}}{\mandi@selectderivedunits{#5}{#6}{#7}}}%
- \cs_set:cpn {#1alternateunits}
- {\unit{\mandi@selectprecision{#3}{#4}}{\mandi@selectalternateunits{#5}{#6}{#7}}}%
- \cs_set:cpn {#1onlybaseunits} {\mandi@selectbaseunits{#5}{#6}{#7}}%
- \cs_set:cpn {#1onlyderivedunits} {\mandi@selectderivedunits{#5}{#6}{#7}}%
- \cs_set:cpn {#1onlyalternateunits} {\mandi@selectalternateunits{#5}{#6}{#7}}%
-}%
-\NewDocumentCommand{\renewphysicalconstant}{ m m m m m O{#5} O{#5} }%
-{%
- \mandi_renewphysicalconstant { #1 }{ #2 }{ #3 }{ #4 }{ #5 }{ #6 }{ #7 }%
-}%
+\cs_new:Npn \__mandi_renewphysicalconstant:nnnnnnn #1#2#3#4#5#6#7
+ {
+ \cs_set:cpn {#1} {\unit{\mandi@selectprecision{#3}{#4}}{\mandi@selectunits{#5}{#6}{#7}}}
+ \cs_set:cpn {#1mathsymbol} {#2}
+ \cs_set:cpn {#1approximatevalue} {#3}
+ \cs_set:cpn {#1precisevalue} {#4}
+ \cs_set:cpn {#1baseunits}
+ {\unit{\mandi@selectprecision{#3}{#4}}{\mandi@selectbaseunits{#5}{#6}{#7}}}
+ \cs_set:cpn {#1derivedunits}
+ {\unit{\mandi@selectprecision{#3}{#4}}{\mandi@selectderivedunits{#5}{#6}{#7}}}
+ \cs_set:cpn {#1alternateunits}
+ {\unit{\mandi@selectprecision{#3}{#4}}{\mandi@selectalternateunits{#5}{#6}{#7}}}
+ \cs_set:cpn {#1onlybaseunits} {\mandi@selectbaseunits{#5}{#6}{#7}}
+ \cs_set:cpn {#1onlyderivedunits} {\mandi@selectderivedunits{#5}{#6}{#7}}
+ \cs_set:cpn {#1onlyalternateunits} {\mandi@selectalternateunits{#5}{#6}{#7}}
+ }
+\NewDocumentCommand{\renewphysicalconstant}{ m m m m m O{#5} O{#5} }
+ {
+ \__mandi_renewphysicalconstant:nnnnnnn { #1 }{ #2 }{ #3 }{ #4 }{ #5 }{ #6 }{ #7 }
+ }
\ExplSyntaxOff
\newvectorquantity{acceleration}%
{\meter\usk\second\totheinversetwo}%
@@ -302,14 +311,14 @@
{\radian\usk\second\inverse}%
[\radian\per\second]%
[\radian\per\second]%
- \newvectorquantity{angularimpulse}%
- {\kilogram\usk\meter\tothetwo\usk\second\inverse}%
- [\kilogram\usk\meter\tothetwo\per\second]% % also \joule\usk\second
- [\kilogram\usk\meter\tothetwo\per\second]% % also \newton\usk\meter\usk\second
- \newvectorquantity{angularmomentum}%
- {\kilogram\usk\meter\tothetwo\usk\second\inverse}%
- [\kilogram\usk\meter\tothetwo\per\second]% % also \joule\usk\second
- [\kilogram\usk\meter\tothetwo\per\second]% % also \newton\usk\meter\usk\second
+\newvectorquantity{angularimpulse}%
+ {\kilogram\usk\meter\tothetwo\usk\second\inverse}%
+ [\kilogram\usk\meter\tothetwo\per\second]% % also \joule\usk\second
+ [\kilogram\usk\meter\tothetwo\per\second]% % also \newton\usk\meter\usk\second
+\newvectorquantity{angularmomentum}%
+ {\kilogram\usk\meter\tothetwo\usk\second\inverse}%
+ [\kilogram\usk\meter\tothetwo\per\second]% % also \joule\usk\second
+ [\kilogram\usk\meter\tothetwo\per\second]% % also \newton\usk\meter\usk\second
\newvectorquantity{angularvelocity}%
{\radian\usk\second\inverse}%
[\radian\per\second]%
@@ -450,6 +459,8 @@
{\kilogram\usk\meter\inverse}%
[\kilogram\per\meter]%
[\kilogram\per\meter]%
+\newscalarquantity{lorentzfactor}%
+ {}%
\newscalarquantity{luminousintensity}%
{\candela}%
\newscalarquantity{magneticcharge}%
@@ -586,49 +597,57 @@
{\kilogram\usk\meter\inverse\usk\second\totheinversetwo}%
[\pascal]%
[\newton\per\meter\tothetwo]%
+\AtBeginDocument{%
+ \DeclareRobustCommand{\hbar}{{\mathpalette\hbar@\relax\symup{h}}}%
+}%
+\newcommand*{\hbar@}[2]{%
+ \makebox[0pt][l]{\raisebox{-0.07\height}{\(\m@th#1\mkern-2mu\mathchar"AF\)}}%
+ % optional line to make the bar thicker; must use -0.11
+ \makebox[0pt][l]{\raisebox{-0.11\height}{\(\m@th#1\mkern-2mu\mathchar"AF\)}}%
+}%
\newphysicalconstant{avogadro}%
{\symup{N_A}}%
- {6\timestento{23}}{6.02214076\timestento{23}}% % exact 2019 value
+ {6\times10^{23}}{6.02214076\times10^{23}}% % exact 2019 value
{\mole\inverse}%
[\per\mole]%
[\per\mole]%
\newphysicalconstant{biotsavartconstant}% % alias for \mzofp
{\symup{\frac{\mu_o}{4\pi}}}%
- {\tento{-7}}{\tento{-7}}%
+ {10^{-7}}{10^{-7}}%
{\kilogram\usk\meter\usk\ampere\totheinversetwo\usk\second\totheinversetwo}%
[\henry\per\meter]%
[\tesla\usk\meter\per\ampere]%
\newphysicalconstant{bohrradius}%
{\symup{a_o}}%
- {5.3\timestento{-11}}{5.29177210903\timestento{-11}}%
+ {5.3\times10^{-11}}{5.29177210903\times10^{-11}}%
{\meter}%
\newphysicalconstant{boltzmann}%
{\symup{k_B}}%
- {1.4\timestento{-23}}{1.380649\timestento{-23}}% % exact 2019 value
+ {1.4\times10^{-23}}{1.380649\times10^{-23}}% % exact 2019 value
{\kilogram\usk\meter\tothetwo\usk\second\totheinversetwo\usk\kelvin\inverse}%
[\joule\per\kelvin]%
[\joule\per\kelvin]%
\newphysicalconstant{coulombconstant}% % alias for \oofpez
{\symup{\frac{1}{4\pi\epsilon_o}}}%
- {9\timestento{9}}{8.9875517923\timestento{9}}%
+ {9\times10^{9}}{8.9875517923\times10^{9}}%
{\kilogram\usk\meter\tothethree\usk\ampere\totheinversetwo\usk\second\totheinversefour}%
[\meter\per\farad]%
[\newton\usk\meter\tothetwo\per\coulomb\tothetwo]%
\newphysicalconstant{earthmass}%
{\symup{M_{Earth}}}%
- {6.0\timestento{24}}{5.9722\timestento{24}}%
+ {6.0\times10^{24}}{5.9722\times10^{24}}%
{\kilogram}%
\newphysicalconstant{earthmoondistance}%
{\symup{d_{EM}}}%
- {3.8\timestento{8}}{3.81550\timestento{8}}%
+ {3.8\times10^{8}}{3.81550\times10^{8}}%
{\meter}%
\newphysicalconstant{earthradius}%
{\symup{R_{Earth}}}%
- {6.4\timestento{6}}{6.3781\timestento{6}}%
+ {6.4\times10^{6}}{6.3781\times10^{6}}%
{\meter}%
\newphysicalconstant{earthsundistance}%
{\symup{d_{ES}}}%
- {1.5\timestento{11}}{1.496\timestento{11}}%
+ {1.5\times10^{11}}{1.496\times10^{11}}%
{\meter}%
\newphysicalconstant{electroncharge}%
{\symup{q_e}}%
@@ -644,71 +663,71 @@
[\coulomb]%
\newphysicalconstant{electronmass}%
{\symup{m_e}}%
- {9.1\timestento{-31}}{9.1093837015\timestento{-31}}%
+ {9.1\times10^{-31}}{9.1093837015\times10^{-31}}%
{\kilogram}%
\newphysicalconstant{elementarycharge}%
{\symup{e}}%
- {1.6\timestento{-19}}{1.602176634\timestento{-19}}% % exact 2019 value
+ {1.6\times10^{-19}}{1.602176634\times10^{-19}}% % exact 2019 value
{\ampere\usk\second}%
[\coulomb]%
[\coulomb]%
\newphysicalconstant{finestructure}%
{\symup{\alpha}}%
- {\frac{1}{137}}{7.2973525693\timestento{-3}}%
+ {\frac{1}{137}}{7.2973525693\times10^{-3}}%
{}%
\newphysicalconstant{hydrogenmass}%
{\symup{m_H}}%
- {1.7\timestento{-27}}{1.6737236\timestento{-27}}%
+ {1.7\times10^{-27}}{1.6737236\times10^{-27}}%
{\kilogram}%
\newphysicalconstant{moonearthdistance}%
{\symup{d_{ME}}}%
- {3.8\timestento{8}}{3.81550\timestento{8}}%
+ {3.8\times10^{8}}{3.81550\times10^{8}}%
{\meter}%
\newphysicalconstant{moonmass}%
{\symup{M_{Moon}}}%
- {7.3\timestento{22}}{7.342\timestento{22}}%
+ {7.3\times10^{22}}{7.342\times10^{22}}%
{\kilogram}%
\newphysicalconstant{moonradius}%
{\symup{R_{Moon}}}%
- {1.7\timestento{6}}{1.7371\timestento{6}}%
+ {1.7\times10^{6}}{1.7371\times10^{6}}%
{\meter}%
\newphysicalconstant{mzofp}%
{\symup{\frac{\mu_o}{4\pi}}}%
- {\tento{-7}}{\tento{-7}}%
+ {10^{-7}}{10^{-7}}%
{\kilogram\usk\meter\usk\ampere\totheinversetwo\usk\second\totheinversetwo}%
[\henry\per\meter]%
[\tesla\usk\meter\per\ampere]%
\newphysicalconstant{neutronmass}%
{\symup{m_n}}%
- {1.7\timestento{-27}}{1.67492749804\timestento{-27}}%
+ {1.7\times10^{-27}}{1.67492749804\times10^{-27}}%
{\kilogram}%
\newphysicalconstant{oofpez}%
{\symup{\frac{1}{4\pi\epsilon_o}}}%
- {9\timestento{9}}{8.9875517923\timestento{9}}%
+ {9\times10^{9}}{8.9875517923\times10^{9}}%
{\kilogram\usk\meter\tothethree\usk\ampere\totheinversetwo\usk\second\totheinversefour}%
[\meter\per\farad]%
[\newton\usk\meter\tothetwo\per\coulomb\tothetwo]%
\newphysicalconstant{oofpezcs}%
{\symup{\frac{1}{4\pi\epsilon_o c^2}}}%
- {\tento{-7}}{\tento{-7}}%
+ {10^{-7}}{10^{-7}}%
{\kilogram\usk\meter\usk\ampere\totheinversetwo\usk\second\totheinversetwo}%
[\tesla\usk\meter\tothetwo]%
[\newton\usk\second\tothetwo\per\coulomb\tothetwo]%
\newphysicalconstant{planck}%
{\symup{h}}%
- {6.6\timestento{-34}}{6.62607015\timestento{-34}}% % exact 2019 value
+ {6.6\times10^{-34}}{6.62607015\times10^{-34}}% % exact 2019 value
{\kilogram\usk\meter\tothetwo\usk\second\inverse}%
[\joule\usk\second]%
[\joule\usk\second]%
\newphysicalconstant{planckbar}%
- {\symup{\lower0.18ex\hbox{\mathchar"AF}\mkern-7mu h}}%
- {1.1\timestento{-34}}{1.054571817\timestento{-34}}%
+ {\hbar}%
+ {1.1\times10^{-34}}{1.054571817\times10^{-34}}%
{\kilogram\usk\meter\tothetwo\usk\second\inverse}%
[\joule\usk\second]%
[\joule\usk\second]
\newphysicalconstant{planckc}%
{\symup{hc}}%
- {2.0\timestento{-25}}{1.98644586\timestento{-25}}%
+ {2.0\times10^{-25}}{1.98644586\times10^{-25}}%
{\kilogram\usk\meter\tothethree\usk\second\totheinversetwo}%
[\joule\usk\meter]%
[\joule\usk\meter]%
@@ -726,35 +745,35 @@
[\coulomb]%
\newphysicalconstant{protonmass}%
{\symup{m_p}}%
- {1.7\timestento{-27}}{1.672621898\timestento{-27}}%
+ {1.7\times10^{-27}}{1.672621898\times10^{-27}}%
{\kilogram}%
\newphysicalconstant{rydberg}%
{\symup{R_{\infty}}}%
- {1.1\timestento{7}}{1.0973731568160\timestento{7}}%
+ {1.1\times10^{7}}{1.0973731568160\times10^{7}}%
{\meter\inverse}%
\newphysicalconstant{speedoflight}%
{\symup{c}}%
- {3\timestento{8}}{2.99792458\timestento{8}}% % exact value
+ {3\times10^{8}}{2.99792458\times10^{8}}% % exact value
{\meter\usk\second\inverse}%
[\meter\per\second]%
[\meter\per\second]
\newphysicalconstant{stefanboltzmann}%
{\symup{\sigma}}%
- {5.7\timestento{-8}}{5.670374\timestento{-8}}%
+ {5.7\times10^{-8}}{5.670374\times10^{-8}}%
{\kilogram\usk\second\totheinversethree\usk\kelvin\totheinversefour}%
[\watt\per\meter\tothetwo\usk\kelvin\tothefour]%
[\watt\per\meter\tothetwo\usk\kelvin\tothefour]
\newphysicalconstant{sunearthdistance}%
{\symup{d_{SE}}}%
- {1.5\timestento{11}}{1.496\timestento{11}}%
+ {1.5\times10^{11}}{1.496\times10^{11}}%
{\meter}%
\newphysicalconstant{sunmass}%
{\symup{M_{Sun}}}%
- {2.0\timestento{30}}{1.98855\timestento{30}}%
+ {2.0\times10^{30}}{1.98855\times10^{30}}%
{\kilogram}%
\newphysicalconstant{sunradius}%
{\symup{R_{Sun}}}%
- {7.0\timestento{8}}{6.957\timestento{8}}%
+ {7.0\times10^{8}}{6.957\times10^{8}}%
{\meter}%
\newphysicalconstant{surfacegravfield}%
{\symup{g}}%
@@ -764,101 +783,86 @@
[\newton\per\kilogram]%
\newphysicalconstant{universalgrav}%
{\symup{G}}%
- {6.7\timestento{-11}}{6.67430\timestento{-11}}%
+ {6.7\times10^{-11}}{6.67430\times10^{-11}}%
{\meter\tothethree\usk\kilogram\inverse\usk\second\totheinversetwo}%
[\newton\usk\meter\tothetwo\per\kilogram\tothetwo]% % also \joule\usk\meter\per\kilogram\tothetwo
[\newton\usk\meter\tothetwo\per\kilogram\tothetwo]%
\newphysicalconstant{vacuumpermeability}%
{\symup{\mu_o}}%
- {4\pi\timestento{-7}}{4\pi\timestento{-7}}% % as of 2018 no longer 4\pi\timestento{-7}
+ {4\pi\times10^{-7}}{4\pi\times10^{-7}}% % as of 2018 no longer 4\pi\times10^{-7}
{\kilogram\usk\meter\usk\ampere\totheinversetwo\usk\second\totheinversetwo}%
[\henry\per\meter]%
[\tesla\usk\meter\per\ampere]%
\newphysicalconstant{vacuumpermittivity}%
{\symup{\epsilon_o}}%
- {9\timestento{-12}}{8.854187817\timestento{-12}}%
+ {9\times10^{-12}}{8.854187817\times10^{-12}}%
{\ampere\tothetwo\usk\second\tothefour\usk\kilogram\inverse\usk\meter\totheinversethree}%
[\farad\per\meter]%
[\coulomb\tothetwo\per\newton\usk\meter\tothetwo]%
\ExplSyntaxOn
-\NewDocumentCommand{\checkquantity}{ m }%
-{%
- % Works for both scalar and vector quantities (without vector in the name!).
- \begin{center}
- \begin{tabular}{%
- >{\bfseries\small}
- p{0.5\linewidth}
- p{0.1\linewidth}
- p{0.1\linewidth}
- p{0.1\linewidth}
- }%
- name & & & \tabularnewline
- \ttfamily\footnotesize{\token_to_str:c {#1}} & & & \tabularnewline
- \end{tabular}~ % This nonbreaking space is important!
- \begin{tabular}{%
- >{\bfseries\small}p{0.25\linewidth}
- >{\bfseries\small}p{0.25\linewidth}
- >{\bfseries\small}p{0.25\linewidth}
- }%
- base & derived & alternate \tabularnewline
- \footnotesize{\( \use:c {#1onlybaseunits} \)} &
- \footnotesize{\( \use:c {#1onlyderivedunits} \)} &
- \footnotesize{\( \use:c {#1onlyalternateunits} \)}
- \end{tabular}
- \end{center}
-}%
-\NewDocumentCommand{\checkconstant}{ m }%
-{%
- \begin{center}
- \begin{tabular}{%
- >{\bfseries\small}
- p{0.5\linewidth}
- p{0.1\linewidth}
- p{0.1\linewidth}
- p{0.1\linewidth}
- }%
- name & & & \tabularnewline
- \ttfamily\footnotesize{\token_to_str:c {#1}} & & & \tabularnewline
- \end{tabular}~ % This nonbreaking space is important!
- \begin{tabular}{%
- >{\bfseries\small}p{0.25\linewidth}
- >{\bfseries\small}p{0.25\linewidth}
- >{\bfseries\small}p{0.25\linewidth}
- }%
- symbol & approximate & precise \tabularnewline
- \footnotesize{\( \use:c {#1mathsymbol} \)} &
- \footnotesize{\( \use:c {#1approximatevalue} \)} &
- \footnotesize{\( \use:c {#1precisevalue} \)}
- \end{tabular}~ % This nonbreaking space is important!
- \begin{tabular}{%
- >{\bfseries\small}p{0.25\linewidth}
- >{\bfseries\small}p{0.25\linewidth}
- >{\bfseries\small}p{0.25\linewidth}
- }%
- base & derived & alternate \tabularnewline
- \footnotesize{\( \use:c {#1onlybaseunits} \)} &
- \footnotesize{\( \use:c {#1onlyderivedunits} \)} &
- \footnotesize{\( \use:c {#1onlyalternateunits} \)}
- \end{tabular}
- \end{center}
-}%
+\NewDocumentCommand{\@aux}{ m }
+ {
+ \use:c { #1 }
+ }
+\NewDocumentCommand{\@auy}{ m }
+ {
+ \normalfont\ttfamily\token_to_str:c { #1 }
+ }
\ExplSyntaxOff
-\ExplSyntaxOn
-\NewDocumentCommand{\mivector}{ O{,} m o }%
- {%
- \mi_vector:nn { #1 } { #2 }%
- \IfValueT{#3}{\,{#3}}%
- }%
-\seq_new:N \l__mi_list_seq
-\cs_new_protected:Npn \mi_vector:nn #1 #2
-{%
- \ensuremath{%
- \seq_set_split:Nnn \l__mi_list_seq { , } { #2 }
- \int_compare:nF { \seq_count:N \l__mi_list_seq = 1 } { \left\langle }
- \seq_use:Nnnn \l__mi_list_seq { #1 } { #1 } { #1 }
- \int_compare:nF { \seq_count:N \l__mi_list_seq = 1 } { \right\rangle }
+\newcolumntype{M}{>{\(}p{0.25\linewidth}<{\)}}
+\NewDocumentCommand{\checkquantity}{ m }
+ {%
+ \begin{center}
+ \begin{tabular}{MMM}
+ \textbf{command} & \multicolumn{2}{l}{\@auy{#1}} \tabularnewline
+ \text{\textbf{base}} & \text{\textbf{derived}} & \text{\textbf{alternate}} \tabularnewline
+ \@aux{#1onlybaseunits} & \@aux{#1onlyderivedunits} & \@aux{#1onlyalternateunits} \tabularnewline
+ \end{tabular}
+ \end{center}
}%
-}%
+\NewDocumentCommand{\checkconstant}{ m }
+ {%
+ \begin{center}
+ \begin{tabular}{MMM}
+ \textbf{command} & \multicolumn{2}{l}{\@auy{#1}} \tabularnewline
+ \text{\textbf{symbol}} & \text{\textbf{approximate}} & \text{\textbf{precise}} \tabularnewline
+ \@aux{#1mathsymbol} & \@aux{#1approximatevalue} & \@aux{#1precisevalue} \tabularnewline
+ \text{\textbf{base}} & \text{\textbf{derived}} & \text{\textbf{alternate}} \tabularnewline
+ \@aux{#1onlybaseunits} & \@aux{#1onlyderivedunits} & \@aux{#1onlyalternateunits} \tabularnewline
+ \end{tabular}
+ \end{center}
+ }%
+\ExplSyntaxOn
+\NewDocumentCommand{\mivector}{ O{,} m o }
+ {
+ \__mandi_vector:nn { #1 } { #2 }
+ \IfValueT{#3}{\,{#3}}
+ }
+\seq_new:N \l__mandi_list_seq
+\cs_new_protected:Npn \__mandi_vector:nn #1#2
+ {
+ \seq_set_split:Nnn \l__mandi_list_seq { , } { #2 }
+ \int_compare:nT { \seq_count:N \l__mandi_list_seq = 1 }
+ {
+ \msg_new:nnnn { mandi } { onecomponent }
+ {
+ More~than~one~component~expected. \iow_newline:
+ You~provided~one~component~to~a~command \iow_newline:
+ that~expects~a~vector.~Either~you~don't \iow_newline:
+ need~a~vector~here~or~you~didn't~supply \iow_newline:
+ all~the~components.
+ }
+ {
+ Decide~whether~or~not~you~really~need~a~vector~command~here. \iow_newline:
+ \msg_see_documentation_text:n { mandi }
+ }
+ \msg_fatal:nn { mandi } { onecomponent }
+
+ }
+ \left\langle
+ \seq_use:Nnnn \l__mandi_list_seq { #1 } { #1 } { #1 }
+ \right\rangle
+ }
\ExplSyntaxOff
\endinput
%%
diff --git a/Master/texmf-dist/tex/latex/mandi/mandiexp.sty b/Master/texmf-dist/tex/latex/mandi/mandiexp.sty
index a6c44a2b290..2dbc81637ee 100644
--- a/Master/texmf-dist/tex/latex/mandi/mandiexp.sty
+++ b/Master/texmf-dist/tex/latex/mandi/mandiexp.sty
@@ -6,7 +6,7 @@
%%
%% mandiexp.dtx (with options: `package')
%%
-%% Copyright (C) 2021 by Paul J. Heafner <heafnerj@gmail.com>
+%% Copyright (C) 2021,2022 by Paul J. Heafner <heafnerj@gmail.com>
%% ---------------------------------------------------------------------------
%% 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
@@ -29,173 +29,318 @@
%% and includes the derived files mandi.sty
%% mandistudent.sty
%% mandiexp.sty
-%% vdemo.py
+%% vdemo.py (not needed)
%% ---------------------------------------------------------------------------
%%
-\def\mandiexp@version{\mandi@version}
-\def\mandiexp@date{\mandi@date}
+\def\mandiexp@version{3.1.0}
+\def\mandiexp@date{2022-01-27}
\NeedsTeXFormat{LaTeX2e}[2020-02-02]
-\DeclareRelease{v3.0.0}{2021-08-22}{mandiexp.sty}
-\DeclareCurrentRelease{v\mandi@version}{\mandi@date}
+\DeclareRelease{v3.1.0}{2022-01-27}{mandiexp.sty}
+\DeclareCurrentRelease{v\mandiexp@version}{\mandiexp@date}
\ProvidesPackage{mandiexp}
[\mandiexp@date\space v\mandiexp@version\space Macros for Matter & Interactions]
\newcommand*{\mandiexpversion}{v\mandiexp@version\space dated \mandiexp@date}
\RequirePackage{mandi}
+\IfFormatAtLeastTF {2020-10-01} % load xparse if necessary
+ {}%
+ {\RequirePackage{xparse}}%
\typeout{}%
\typeout{mandiexp: You are using mandiexp \mandiexpversion.}
\typeout{mandiexp: This package requires LuaLaTeX.}%
\typeout{}%
-\NewDocumentCommand{\lhsmomentumprinciple}{ s }{%
- \Delta
- \IfBooleanTF{#1}%
- {\vec*{p}}%
- {\vec{p}}%
- _{\symup{sys}}%
-}%
-\NewDocumentCommand{\rhsmomentumprinciple}{ s }{%
- \IfBooleanTF{#1}%
- {\vec*{F}}%
- {\vec{F}}%
- _{\symup{sys,net}}\,\Delta t%
-}%
-\NewDocumentCommand{\lhsmomentumprincipleupdate}{ s }{%
- \IfBooleanTF{#1}%
- {\vec*{p}}%
- {\vec{p}}%
- _{\symup{sys,final}}%
-}%
-\NewDocumentCommand{\rhsmomentumprincipleupdate}{ s }{%
- \IfBooleanTF{#1}%
- {\vec*{p}}%
- {\vec{p}}%
- _{\symup{sys,initial}}+%
- \IfBooleanTF{#1}%
- {\vec*{F}}%
- {\vec{F}}%
- _{\symup{sys,net}}\,\Delta t%
-}%
-\NewDocumentCommand{\momentumprinciple}{ s }{%
- \IfBooleanTF{#1}%
- {\lhsmomentumprinciple* = \rhsmomentumprinciple*}%
- {\lhsmomentumprinciple = \rhsmomentumprinciple}%
-}%
-\NewDocumentCommand{\momentumprincipleupdate}{ s }{%
- \IfBooleanTF{#1}%
- {\lhsmomentumprincipleupdate* = \rhsmomentumprincipleupdate*}%
- {\lhsmomentumprincipleupdate = \rhsmomentumprincipleupdate}%
-}%
-\NewDocumentCommand{\lhsenergyprinciple}{}{%
- \Delta E_{\symup{sys}}%
-}%
-\NewDocumentCommand{\rhsenergyprinciple}{ O{} }{%
- W_{\symup{ext}}#1%
-}%
-\NewDocumentCommand{\lhsenergyprincipleupdate}{}{%
- E_{\symup{sys,final}}%
-}%
-\NewDocumentCommand{\rhsenergyprincipleupdate}{ O{} }{%
- E_{\symup{sys,initial}}+%
- W_{\symup{ext}}#1%
-}%
-\NewDocumentCommand{\energyprinciple}{ O{} }{%
- \lhsenergyprinciple = \rhsenergyprinciple[#1]%
-}%
-\NewDocumentCommand{\energyprincipleupdate}{ O{} }{%
- \lhsenergyprincipleupdate = \rhsenergyprincipleupdate[#1]%
-}%
-\NewDocumentCommand{\lhsangularmomentumprinciple}{ s }{%
- \Delta
- \IfBooleanTF{#1}%
- {\vec*{L}}%
- {\vec{L}}%
- _{A\symup{,sys,net}}%
-}%
-\NewDocumentCommand{\rhsangularmomentumprinciple}{ s }{%
- \IfBooleanTF{#1}%
- {\vec*{\tau}}%
- {\vec{\tau}}%
- _{A\symup{,sys,net}}\,\Delta t%
-}%
-\NewDocumentCommand{\lhsangularmomentumprincipleupdate}{ s }{%
- \IfBooleanTF{#1}%
- {\vec*{L}}%
- {\vec{L}}%
- _{A,\symup{sys,final}}%
-}%
-\NewDocumentCommand{\rhsangularmomentumprincipleupdate}{ s }{%
- \IfBooleanTF{#1}%
- {\vec*{L}}%
- {\vec{L}}%
- _{A\symup{,sys,initial}}+%
- \IfBooleanTF{#1}%
- {\vec*{\tau}}%
- {\vec{\tau}}%
- _{A\symup{,sys,net}}\,\Delta t%
-}%
-\NewDocumentCommand{\angularmomentumprinciple}{ s }{%
- \IfBooleanTF{#1}%
- {\lhsangularmomentumprinciple* = \rhsangularmomentumprinciple*}%
- {\lhsangularmomentumprinciple = \rhsangularmomentumprinciple}%
-}%
-\NewDocumentCommand{\angularmomentumprincipleupdate}{ s }{%
- \IfBooleanTF{#1}%
- {\lhsangularmomentumprincipleupdate* = \rhsangularmomentumprincipleupdate*}%
- {\lhsangularmomentumprincipleupdate = \rhsangularmomentumprincipleupdate}%
-}%
-\NewDocumentCommand{\energyof}{ m o }{%
- E_{#1\IfValueT{#2}{,#2}}%
-}%
-\NewDocumentCommand{\systemenergy}{ o }{%
- E_{\symup{sys}\IfValueT{#1}{,#1}}%
-}%
-\NewDocumentCommand{\particleenergy}{ o }{%
- E_{\symup{particle}\IfValueT{#1}{,#1}}%
-}%
-\NewDocumentCommand{\restenergy}{ o }{%
- E_{\symup{rest}\IfValueT{#1}{,#1}}%
-}%
-\NewDocumentCommand{\internalenergy}{ o }{%
- E_{\symup{internal}\IfValueT{#1}{,#1}}%
-}%
-\NewDocumentCommand{\chemicalenergy}{ o }{%
- E_{\symup{chem}\IfValueT{#1}{,#1}}%
-}%
-\NewDocumentCommand{\thermalenergy}{ o }{%
- E_{\symup{therm}\IfValueT{#1}{,#1}}%
-}%
-\NewDocumentCommand{\photonenergy}{ o }{%
- E_{\symup{photon}\IfValueT{#1}{,#1}}%
-}%
-\NewDocumentCommand{\translationalkineticenergy}{ s d[] }{%
- \IfBooleanTF{#1}%
- {E_\bgroup \symup{K}}%
- {K_\bgroup\symup{trans}}%
- \IfValueT{#2}{,#2}%
- \egroup%
-}%
-\NewDocumentCommand{\rotationalkineticenergy}{ s d[] }{%
- \IfBooleanTF{#1}%
- {E_\bgroup}%
- {K_\bgroup}%
- \symup{rot}\IfValueT{#2}{,#2}%
- \egroup%
-}%
-\NewDocumentCommand{\vibrationalkineticenergy}{ s d[] }{%
- \IfBooleanTF{#1}%
- {E_\bgroup}%
- {K_\bgroup}%
- \symup{vib}\IfValueT{#2}{,#2}%
- \egroup%
-}%
-\NewDocumentCommand{\gravitationalpotentialenergy}{ o }{%
- U_{\symup{g}\IfValueT{#1}{,#1}}%
-}%
-\NewDocumentCommand{\electricpotentialenergy}{ o }{%
- U_{\symup{e}\IfValueT{#1}{,#1}}%
-}%
-\NewDocumentCommand{\springpotentialenergy}{ o }{%
- U_{\symup{s}\IfValueT{#1}{,#1}}%
-}%
+\NewDocumentCommand{\lhsmomentumprinciple}{ s }%
+ {%
+ \Delta
+ \IfBooleanTF{#1}%
+ {%
+ \vec*{p}
+ }%
+ {%
+ \vec{p}%
+ }%
+ \sb{\symup{sys}}%
+ }%
+\NewDocumentCommand{\rhsmomentumprinciple}{ s }%
+ {%
+ \IfBooleanTF{#1}%
+ {%
+ \vec*{F}%
+ }%
+ {%
+ \vec{F}%
+ }%
+ \sb{\symup{sys,net}}\,\Delta t%
+ }%
+\NewDocumentCommand{\lhsmomentumprincipleupdate}{ s }%
+ {%
+ \IfBooleanTF{#1}%
+ {%
+ \vec*{p}%
+ }%
+ {%
+ \vec{p}%
+ }%
+ \sb{\symup{sys,final}}%
+ }%
+\NewDocumentCommand{\rhsmomentumprincipleupdate}{ s }%
+ {%
+ \IfBooleanTF{#1}%
+ {%
+ \vec*{p}%
+ }%
+ {%
+ \vec{p}%
+ }%
+ \sb{\symup{sys,initial}}+%
+ \IfBooleanTF{#1}%
+ {%
+ \vec*{F}%
+ }%
+ {%
+ \vec{F}%
+ }%
+ \sb{\symup{sys,net}}\,\Delta t%
+ }%
+\NewDocumentCommand{\momentumprinciple}{ s }%
+ {%
+ \IfBooleanTF{#1}%
+ {%
+ \lhsmomentumprinciple* = \rhsmomentumprinciple*%
+ }%
+ {%
+ \lhsmomentumprinciple = \rhsmomentumprinciple%
+ }%
+ }%
+\NewDocumentCommand{\momentumprincipleupdate}{ s }%
+ {%
+ \IfBooleanTF{#1}%
+ {%
+ \lhsmomentumprincipleupdate* = \rhsmomentumprincipleupdate*%
+ }%
+ {%
+ \lhsmomentumprincipleupdate = \rhsmomentumprincipleupdate%
+ }%
+ }%
+\NewDocumentCommand{\lhsenergyprinciple}{}%
+ {%
+ \Delta E_{\symup{sys}}%
+ }%
+\NewDocumentCommand{\rhsenergyprinciple}{ O{} }%
+ {%
+ W_{\symup{ext}}#1%
+ }%
+\NewDocumentCommand{\lhsenergyprincipleupdate}{}%
+ {%
+ E_{\symup{sys,final}}%
+ }%
+\NewDocumentCommand{\rhsenergyprincipleupdate}{ O{} }%
+ {%
+ E_{\symup{sys,initial}}+%
+ W_{\symup{ext}}#1%
+ }%
+\NewDocumentCommand{\energyprinciple}{ O{} }%
+ {%
+ \lhsenergyprinciple = \rhsenergyprinciple[#1]%
+ }%
+\NewDocumentCommand{\energyprincipleupdate}{ O{} }%
+ {%
+ \lhsenergyprincipleupdate = \rhsenergyprincipleupdate[#1]%
+ }%
+\NewDocumentCommand{\lhsangularmomentumprinciple}{ s }%
+ {%
+ \Delta%
+ \IfBooleanTF{#1}%
+ {%
+ \vec*{L}%
+ }%
+ {%
+ \vec{L}%
+ }%
+ \sb{A\symup{,sys,net}}%
+ }%
+\NewDocumentCommand{\rhsangularmomentumprinciple}{ s }%
+ {%
+ \IfBooleanTF{#1}%
+ {%
+ \vec*{\tau}%
+ }%
+ {%
+ \vec{\tau}%
+ }%
+ \sb{A\symup{,sys,net}}\,\Delta t%
+ }%
+\NewDocumentCommand{\lhsangularmomentumprincipleupdate}{ s }%
+ {%
+ \IfBooleanTF{#1}%
+ {%
+ \vec*{L}%
+ }%
+ {%
+ \vec{L}%
+ }%
+ \sb{A,\symup{sys,final}}%
+ }%
+\NewDocumentCommand{\rhsangularmomentumprincipleupdate}{ s }%
+ {%
+ \IfBooleanTF{#1}%
+ {%
+ \vec*{L}%
+ }%
+ {%
+ \vec{L}%
+ }%
+ \sb{A\symup{,sys,initial}}+%
+ \IfBooleanTF{#1}%
+ {%
+ \vec*{\tau}%
+ }%
+ {%
+ \vec{\tau}%
+ }%
+ \sb{A\symup{,sys,net}}\,\Delta t%
+ }%
+\NewDocumentCommand{\angularmomentumprinciple}{ s }%
+ {%
+ \IfBooleanTF{#1}%
+ {%
+ \lhsangularmomentumprinciple* = \rhsangularmomentumprinciple*%
+ }%
+ {%
+ \lhsangularmomentumprinciple = \rhsangularmomentumprinciple%
+ }%
+ }%
+\NewDocumentCommand{\angularmomentumprincipleupdate}{ s }%
+ {%
+ \IfBooleanTF{#1}%
+ {%
+ \lhsangularmomentumprincipleupdate* = \rhsangularmomentumprincipleupdate*%
+ }%
+ {%
+ \lhsangularmomentumprincipleupdate = \rhsangularmomentumprincipleupdate%
+ }%
+ }%
+\NewDocumentCommand{\energyof}{ m o }%
+ {%
+ E_{#1%
+ \IfValueT{#2}%
+ {,#2}%
+ }%
+ }%
+\NewDocumentCommand{\systemenergy}{ o }%
+ {%
+ E_{\symup{sys}%
+ \IfValueT{#1}%
+ {,#1}%
+ }%
+ }%
+\NewDocumentCommand{\particleenergy}{ o }%
+ {%
+ E_{\symup{particle}%
+ \IfValueT{#1}%
+ {,#1}%
+ }%
+ }%
+\NewDocumentCommand{\restenergy}{ o }%
+ {%
+ E_{\symup{rest}%
+ \IfValueT{#1}%
+ {,#1}%
+ }%
+ }%
+\NewDocumentCommand{\internalenergy}{ o }%
+ {%
+ E_{\symup{internal}%
+ \IfValueT{#1}%
+ {,#1}%
+ }%
+ }%
+\NewDocumentCommand{\chemicalenergy}{ o }%
+ {%
+ E_{\symup{chem}%
+ \IfValueT{#1}%
+ {,#1}%
+ }%
+ }%
+\NewDocumentCommand{\thermalenergy}{ o }%
+ {%
+ E_{\symup{therm}%
+ \IfValueT{#1}%
+ {,#1}%
+ }%
+ }%
+\NewDocumentCommand{\photonenergy}{ o }%
+ {%
+ E_{\symup{photon}%
+ \IfValueT{#1}%
+ {,#1}%
+ }%
+ }%
+\NewDocumentCommand{\translationalkineticenergy}{ s d[] }%
+ {%
+ % d[] must be used because of the way consecutive optional
+ % arguments are handled. See xparse docs for details.
+ % See https://tex.stackexchange.com/a/569011/218142
+ \IfBooleanTF{#1}%
+ {%
+ E_\bgroup \symup{K}%
+ }%
+ {%
+ K_\bgroup\symup{trans}%
+ }%
+ \IfValueT{#2}{,#2}%
+ \egroup%
+ }%
+\NewDocumentCommand{\rotationalkineticenergy}{ s d[] }%
+ {%
+ % d[] must be used because of the way consecutive optional
+ % arguments are handled. See xparse docs for details.
+ % See https://tex.stackexchange.com/a/569011/218142
+ \IfBooleanTF{#1}%
+ {%
+ E_\bgroup%
+ }%
+ {%
+ K_\bgroup%
+ }%
+ \symup{rot}\IfValueT{#2}{,#2}%
+ \egroup%
+ }%
+\NewDocumentCommand{\vibrationalkineticenergy}{ s d[] }%
+ {%
+ % d[] must be used because of the way consecutive optional
+ % arguments are handled. See xparse docs for details.
+ % See https://tex.stackexchange.com/a/569011/218142
+ \IfBooleanTF{#1}%
+ {%
+ E_\bgroup%
+ }%
+ {%
+ K_\bgroup%
+ }%
+ \symup{vib}\IfValueT{#2}{,#2}%
+ \egroup%
+ }%
+\NewDocumentCommand{\gravitationalpotentialenergy}{ o }%
+ {%
+ U_{\symup{g}%
+ \IfValueT{#1}%
+ {,#1}%
+ }%
+ }%
+\NewDocumentCommand{\electricpotentialenergy}{ o }%
+ {%
+ U_{\symup{e}%
+ \IfValueT{#1}%
+ {,#1}%
+ }%
+ }%
+\NewDocumentCommand{\springpotentialenergy}{ o }%
+ {%
+ U_{\symup{s}%
+ \IfValueT{#1}%
+ {,#1}%
+ }%
+ }%
\endinput
%%
%% End of file `mandiexp.sty'.
diff --git a/Master/texmf-dist/tex/latex/mandi/mandistudent.sty b/Master/texmf-dist/tex/latex/mandi/mandistudent.sty
index ff5edb5e546..3bfe3b00531 100644
--- a/Master/texmf-dist/tex/latex/mandi/mandistudent.sty
+++ b/Master/texmf-dist/tex/latex/mandi/mandistudent.sty
@@ -6,7 +6,7 @@
%%
%% mandistudent.dtx (with options: `package')
%%
-%% Copyright (C) 2021 by Paul J. Heafner <heafnerj@gmail.com>
+%% Copyright (C) 2021,2022 by Paul J. Heafner <heafnerj@gmail.com>
%% ---------------------------------------------------------------------------
%% 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
@@ -29,14 +29,14 @@
%% and includes the derived files mandi.sty
%% mandistudent.sty
%% mandiexp.sty
-%% vdemo.py
+%% vdemo.py (not needed)
%% ---------------------------------------------------------------------------
%%
-\def\mandistudent@version{\mandi@version}
-\def\mandistudent@date{\mandi@date}
+\def\mandistudent@version{3.1.0}
+\def\mandistudent@date{2022-01-27}
\NeedsTeXFormat{LaTeX2e}[2020-02-02]
-\DeclareRelease{v3.0.0}{2021-08-22}{mandistudent.sty}
-\DeclareCurrentRelease{v\mandi@version}{\mandi@date}
+\DeclareRelease{v3.1.0}{2022-01-27}{mandistudent.sty}
+\DeclareCurrentRelease{v\mandistudent@version}{\mandistudent@date}
\ProvidesPackage{mandistudent}
[\mandistudent@date\space v\mandistudent@version\space Macros for introductory physics]
\newcommand*{\mandistudentversion}{v\mandistudent@version\space dated \mandistudent@date}
@@ -50,11 +50,16 @@
\RequirePackage{mandi}
\RequirePackage{mathtools} % needed for paired delimiters; extends amsmath
\RequirePackage{nicematrix} % needed for column and row vectors
+\RequirePackage{qrcode} % needed for QR codes in webvpythonblock
+\qrset{height=1.5cm} % set default size of QR code
\RequirePackage[most]{tcolorbox} % needed for program listings
\RequirePackage{tensor} % needed for index notation
\RequirePackage{tikz} % needed for \hilite
\usetikzlibrary{shapes,fit,tikzmark} % needed for \hilite
\RequirePackage{unicode-math} % needed for Unicode support
+\IfFormatAtLeastTF {2020-10-01} % load xparse if necessary
+ {}%
+ {\RequirePackage{xparse}}%
\RequirePackage{hyperref} % load last
\RequireLuaTeX % require this engine
\unimathsetup{math-style=ISO}
@@ -166,56 +171,73 @@
\typeout{mandistudent: This package changes the default math font(s).}%
\typeout{mandistudent: This package redefines the \protect\vec\space command.}%
\typeout{}%
-\RenewDocumentCommand{\vec}{ s m e{_^} }{%
+\RenewDocumentCommand{\vec}{ s m e{_^} }%
+ {%
% Note the \, used to make superscript look better.
- \IfBooleanTF {#1}
- {\vv{#2}% % * gives an arrow
- % Use \sp{} primitive for superscript.
- % Adjust superscript for the arrow.
- \sp{\IfValueT{#4}{\,#4}\vphantom{\smash[t]{\big|}}}
+ \IfBooleanTF{#1}
+ {%
+ \vv{#2}% % * gives an arrow
+ % Use \sp{} primitive for superscript.
+ % Adjust superscript for the arrow.
+ \IfValueT{#4}%
+ {\sp{\,#4\vphantom{\smash[t]{\big|}}}}
}%
- {\symbfit{#2} % no * gives us bold
- % Use \sp{} primitive for superscript.
- % No superscript adjustment needed.
- \sp{\IfValueT{#4}{#4}\vphantom{\smash[t]{\big|}}}
+ {%
+ \symbfit{#2} % no * gives us bold
+ % Use \sp{} primitive for superscript.
+ % No superscript adjustment needed.
+ \IfValueT{#4}%
+ {\sp{#4\vphantom{\smash[t]{\big|}}}}
}%
- % Use \sb{} primitive for subscript.
- \sb{\IfValueT{#3}{#3}\vphantom{\smash[b]{|}}}
-}%
-\NewDocumentCommand{\dirvec}{ s m e{_^} }{%
- \widehat{\makebox*{\(w\)}{\ensuremath{%
- \IfBooleanTF {#1}
- {%
- #2
- }%
- {%
- \symbfit{#2}
- }%
- }%
+ % Use \sb{} primitive for subscript.
+ \IfValueT{#3}%
+ {\sb{#3\vphantom{\smash[b]{|}}}}
+ }%
+\NewDocumentCommand{\dirvec}{ s m e{_^} }%
+ {%
+ \widehat%
+ {%
+ \makebox*{\(w\)}%
+ {%
+ \ensuremath{%
+ \IfBooleanTF {#1}%
+ {%
+ #2%
+ }%
+ {%
+ \symbfit{#2}%
+ }%
+ }%
+ }%
}%
- }%
- \sb{\IfValueT{#3}{#3}\vphantom{\smash[b]{|}}}
- \sp{\IfValueT{#4}{\,#4}\vphantom{\smash[t]{\big|}}}
-}%
-\NewDocumentCommand{\zerovec}{ s }{%
- \IfBooleanTF {#1}
- {\vv{0}}%
- {\symbfup{0}}%
-}%
+ \IfValueT{#3}%
+ {\sb{#3\vphantom{\smash[b]{|}}}}%
+ \IfValueT{#4}%
+ {\sp{\,#4\vphantom{\smash[t]{\big|}}}}%
+ }%
+\NewDocumentCommand{\zerovec}{ s }%
+ {%
+ \IfBooleanTF {#1}
+ {\vv{0}}%
+ {\symbfup{0}}%
+ }%
\ExplSyntaxOn
-\NewDocumentCommand{\colvec}{ O{,} m }{%
- \vector_main:nnnn { p } { \\ } { #1 } { #2 }
-}%
-\NewDocumentCommand{\rowvec}{ O{,} m }{%
- \vector_main:nnnn { p } { & } { #1 } { #2 }
-}%
-\seq_new:N \l__vector_arg_seq
-\cs_new_protected:Npn \vector_main:nnnn #1 #2 #3 #4 {%
- \seq_set_split:Nnn \l__vector_arg_seq { #3 } { #4 }
- \begin{#1NiceMatrix}[r]
- \seq_use:Nnnn \l__vector_arg_seq { #2 } { #2 } { #2 }
- \end{#1NiceMatrix}
-}%
+\NewDocumentCommand{\colvec}{ O{,} m }
+ {
+ \__mandi_vectormain:nnnn { p } { \\ } { #1 } { #2 }
+ }
+\NewDocumentCommand{\rowvec}{ O{,} m }
+ {
+ \__mandi_vectormain:nnnn { p } { & } { #1 } { #2 }
+ }
+\seq_new:N \l__mandi_vectorarg_seq
+\cs_new_protected:Npn \__mandi_vectormain:nnnn #1#2#3#4
+ {
+ \seq_set_split:Nnn \l__mandi_vectorarg_seq { #3 } { #4 }
+ \begin{#1NiceMatrix}[r]
+ \seq_use:Nnnn \l__mandi_vectorarg_seq { #2 } { #2 } { #2 }
+ \end{#1NiceMatrix}
+ }
\ExplSyntaxOff
\NewDocumentCommand{\changein}{}{\Delta}
\DeclarePairedDelimiterX{\doublebars}[1]{\lVert}{\rVert}{\ifblank{#1}{\:\cdot\:}{#1}}
@@ -227,120 +249,153 @@
\NewDocumentCommand{\magnitude}{}{\doublebars}
\NewDocumentCommand{\norm}{}{\doublebars}
\NewDocumentCommand{\absolutevalue}{}{\singlebars}
-\NewDocumentCommand{\parallelto}{}
- {\mkern3mu\vphantom{\perp}\vrule depth 0pt\mkern2mu\vrule depth 0pt\mkern3mu}
+\NewDocumentCommand{\parallelto}{}%
+ {%
+ \mkern3mu\vphantom{\perp}\vrule depth 0pt\mkern2mu\vrule depth 0pt\mkern3mu%
+ }%
\NewDocumentCommand{\perpendicularto}{}{\perp}
-\NewDocumentEnvironment{physicsproblem}{ m }{%
- \newpage%
- \section*{#1}%
- \newlist{parts}{enumerate}{2}%
- \setlist[parts]{label=\bfseries(\alph*)}}%
+\NewDocumentEnvironment{physicsproblem}{ m }%
+ {%
+ \newpage%
+ \section*{#1}%
+ \newlist{parts}{enumerate}{2}%
+ \setlist[parts]{label=\bfseries(\alph*)}%
+ }%
{}%
-\NewDocumentEnvironment{physicsproblem*}{ m }{%
- \newpage%
- \section*{#1}%
- \newlist{parts}{enumerate*}{2}%
- \setlist[parts]{label=\bfseries(\alph*)}}%
+\NewDocumentEnvironment{physicsproblem*}{ m }%
+ {%
+ \newpage%
+ \section*{#1}%
+ \newlist{parts}{enumerate*}{2}%
+ \setlist[parts]{label=\bfseries(\alph*)}%
+ }%
{}%
\NewDocumentCommand{\problempart}{}{\item}%
-\NewDocumentEnvironment{physicssolution}{ +b }{%
- % Make equation numbering consecutive through the document.
- \begin{align}
- #1
- \end{align}
-}{}%
-\NewDocumentEnvironment{physicssolution*}{ +b }{%
- % Make equation numbering consecutive through the document.
- \begin{align*}
- #1
- \end{align*}
-}{}%
-\NewDocumentCommand{\reason}{ O{4cm} m }
- {&&\begin{minipage}{#1}\raggedright\small #2\end{minipage}}
+\NewDocumentEnvironment{physicssolution}{ +b }%
+ {%
+ % Make equation numbering consecutive through the document.
+ \begin{align}
+ #1
+ \end{align}
+ }%
+ {}%
+\NewDocumentEnvironment{physicssolution*}{ +b }%
+ {%
+ % Make equation numbering consecutive through the document.
+ \begin{align*}
+ #1
+ \end{align*}
+ }%
+ {}%
+\NewDocumentCommand{\reason}{ O{4cm} m }%
+ {%
+ &&\begin{minipage}{#1}\raggedright\small #2\end{minipage}%
+ }%
\newcounter{tikzhighlightnode}
-\NewDocumentCommand{\hilite}{ O{magenta!60} m O{rectangle} }{%
- \stepcounter{tikzhighlightnode}%
- \tikzmarknode{highlighted-node-\number\value{tikzhighlightnode}}{#2}%
- \edef\temp{%
- \noexpand\AddToShipoutPictureBG{%
- \noexpand\begin{tikzpicture}[overlay,remember picture]%
- \noexpand\iftikzmarkoncurrentpage{highlighted-node-\number\value{tikzhighlightnode}}%
- \noexpand\node[inner sep=1.0pt,fill=#1,#3,fit=(highlighted-node-\number\value{tikzhighlightnode})]{};%
- \noexpand\fi
- \noexpand\end{tikzpicture}%
+\NewDocumentCommand{\hilite}{ O{magenta!60} m O{rectangle} }%
+ {%
+ \stepcounter{tikzhighlightnode}%
+ \tikzmarknode{highlighted-node-\number\value{tikzhighlightnode}}{#2}%
+ \edef\temp{%
+ \noexpand\AddToShipoutPictureBG{%
+ \noexpand\begin{tikzpicture}[overlay,remember picture]%
+ \noexpand\iftikzmarkoncurrentpage{highlighted-node-\number\value{tikzhighlightnode}}%
+ \noexpand\node[inner sep=1.0pt,fill=#1,#3,fit=(highlighted-node-\number\value{tikzhighlightnode})]{};%
+ \noexpand\fi
+ \noexpand\end{tikzpicture}%
+ }%
}%
+ \temp%
}%
- \temp%
-}%
-\NewDocumentCommand{\image}{ O{scale=1} m m m }{%
- \begin{figure}[ht!]
- \begin{center}%
+\NewDocumentCommand{\image}{ O{scale=1} m m m }%
+ {%
+ \par
+ \begin{figure}[ht!]
+ \centering%
\includegraphics[#1]{#2}%
- \end{center}%
- \caption{#3}%
- \label{#4}%
- \end{figure}%
-}%
-\NewDocumentCommand{\veccomp}{ s m }{%
- % Consider renaming this to \vectorsym.
- \IfBooleanTF{#1}
+ \caption{#3}%
+ \label{#4}%
+ \end{figure}%
+ \par
+ }%
+\NewDocumentCommand{\veccomp}{ s m }%
{%
- \symnormal{#2}%
+ % Consider renaming this to \vectorsym.
+ \IfBooleanTF{#1}
+ {%
+ \symnormal{#2}%
+ }%
+ {%
+ \symbfit{#2}%
+ }%
}%
+\NewDocumentCommand{\tencomp}{ s m }%
{%
- \symbfit{#2}%
+ % Consider renaming this to \tensororsym.
+ \IfBooleanTF{#1}%
+ {%
+ \symsfit{#2}%
+ }%
+ {%
+ \symbfsfit{#2}%
+ }%
}%
-}%
-\NewDocumentCommand{\tencomp}{ s m }{%
- % Consider renaming this to \tensororsym.
- \IfBooleanTF{#1}
+\NewDocumentCommand{\valence}{ s m m }%
{%
- \symsfit{#2}%
+ \IfBooleanTF{#1}%
+ {%
+ (#2,#3)%
+ }%
+ {%
+ \binom{#2}{#3}%
+ }%
}%
+\NewDocumentCommand{\contraction}{ s m }%
{%
- \symbfsfit{#2}
+ \IfBooleanTF{#1}
+ {%
+ \mathsf{C}%
+ }%
+ {%
+ \symbb{C}%
+ }%
+ _{#2}
}%
-}%
-\NewDocumentCommand{\valence}{ s m m }{%
- \IfBooleanTF{#1}
- {(#2,#3)}
- {\binom{#2}{#3}}
-}%
-\NewDocumentCommand{\contraction}{ s m }{%
- \IfBooleanTF{#1}
- {\mathsf{C}}%
- {\symbb{C}}%
- _{#2}
-}%
-\NewDocumentCommand{\slot}{ s d[] }{%
- % d[] must be used because of the way consecutive optional
- % arguments are handled. See xparse docs for details.
- \IfBooleanTF{#1}
+\NewDocumentCommand{\slot}{ s d[] }%
{%
- \IfValueTF{#2}
- {% Insert a vector, but don't show the slot.
- \smash{\makebox[1.5em]{\ensuremath{#2}}}
+ % d[] must be used because of the way consecutive optional
+ % arguments are handled. See xparse docs for details.
+ \IfBooleanTF{#1}
+ {%
+ \IfValueTF{#2}
+ {% Insert a vector, but don't show the slot.
+ \smash{\makebox[1.5em]{\ensuremath{#2}}}
+ }%
+ {% No vector, no slot.
+ \smash{\makebox[1.5em]{\ensuremath{}}}
+ }%
}%
- {% No vector, no slot.
- \smash{\makebox[1.5em]{\ensuremath{}}}
+ {%
+ \IfValueTF{#2}
+ {% Insert a vector and show the slot.
+ \underline{\smash{\makebox[1.5em]{\ensuremath{#2}}}}
+ }%
+ {% No vector; just show the slot.
+ \underline{\smash{\makebox[1.5em]{\ensuremath{}}}}
+ }%
}%
}%
+\NewDocumentCommand{\df}{ s }%
{%
- \IfValueTF{#2}
- {% Insert a vector and show the slot.
- \underline{\smash{\makebox[1.5em]{\ensuremath{#2}}}}
- }%
- {% No vector; just show the slot.
- \underline{\smash{\makebox[1.5em]{\ensuremath{}}}}
- }%
+ \mathop{}\!%
+ \IfBooleanTF{#1}%
+ {%
+ \symbfsfup{d}%
+ }%
+ {%
+ \symsfup{d}%
+ }%
}%
-}%
-\NewDocumentCommand{\diff}{ s }{%
- \mathop{}\!
- \IfBooleanTF{#1}
- {\symbfsfup{d}}%
- {\symsfup{d}}%
-}%
\directlua{%
luaotfload.add_colorscheme("colordigits",
{["8000FF"] = {"one","two","three","four","five","six","seven","eight","nine","zero"}})
@@ -354,120 +409,162 @@
\definecolor{gspeach} {rgb}{1.00,0.90,0.71} % peach
\definecolor{gspearl} {rgb}{0.94,0.92,0.84} % pearl
\definecolor{gsplum} {rgb}{0.74,0.46,0.70} % plum
-\lstdefinestyle{vpython}{% % style for listings
- backgroundcolor=\color{gsbggray},% % background color
- basicstyle=\colordigits\footnotesize,% % default style
- breakatwhitespace=true% % break at whitespace
- breaklines=true,% % break long lines
- captionpos=b,% % position caption
- classoffset=1,% % STILL DON'T UNDERSTAND THIS
- commentstyle=\color{gsgray},% % font for comments
- deletekeywords={print},% % delete keywords from the given language
- emph={self,cls,@classmethod,@property},% % words to emphasize
- emphstyle=\color{gsorange}\itshape,% % font for emphasis
- escapeinside={(*@}{@*)},% % add LaTeX within your code
- frame=tb,% % frame style
- framerule=2.0pt,% % frame thickness
- framexleftmargin=5pt,% % extra frame left margin
- %identifierstyle=\sffamily,% % style for identifiers
- keywordstyle=\gsfontfamily\color{gsplum},% % color for keywords
- language=Python,% % select language
- linewidth=\linewidth,% % width of listings
- morekeywords={% % VPython/GlowScript specific keywords
- __future__,abs,acos,align,ambient,angle,append,append_to_caption,%
- append_to_title,arange,arrow,asin,astuple,atan,atan2,attach_arrow,%
- attach_trail,autoscale,axis,background,billboard,bind,black,blue,border,%
- bounding_box,box,bumpaxis,bumpmap,bumpmaps,camera,canvas,caption,capture,%
- ceil,center,clear,clear_trail,click,clone,CoffeeScript,coils,color,combin,%
- comp,compound,cone,convex,cos,cross,curve,cyan,cylinder,data,degrees,del,%
- delete,depth,descender,diff_angle,digits,division,dot,draw_complete,%
- ellipsoid,emissive,end_face_color,equals,explog,extrusion,faces,factorial,%
- False,floor,follow,font,format,forward,fov,frame,gcurve,gdisplay,gdots,%
- get_library,get_selected,ghbars,global,GlowScript,graph,graphs,green,gvbars,%
- hat,headlength,headwidth,height,helix,hsv_to_rgb,index,interval,keydown,%
- keyup,label,length,lights,line,linecolor,linewidth,logx,logy,lower_left,%
- lower_right,mag,mag2,magenta,make_trail,marker_color,markers,material,%
- max,min,mouse,mousedown,mousemove,mouseup,newball,norm,normal,objects,%
- offset,one,opacity,orange,origin,path,pause,pi,pixel_to_world,pixels,plot,%
- points,pos,pow,pps,print,print_function,print_options,proj,purple,pyramid,%
- quad,radians,radius,random,rate,ray,read_local_file,readonly,red,redraw,%
- retain,rgb_to_hsv,ring,rotate,round,scene,scroll,shaftwidth,shape,shapes,%
- shininess,show_end_face,show_start_face,sign,sin,size,size_units,sleep,%
- smooth,space,sphere,sqrt,start,start_face_color,stop,tan,text,textpos,%
- texture,textures,thickness,title,trail_color,trail_object,trail_radius,%
- trail_type,triangle,trigger,True,twist,unbind,up,upper_left,upper_right,%
- userpan,userspin,userzoom,vec,vector,vertex,vertical_spacing,visible,%
- visual,vpython,VPython,waitfor,white,width,world,xtitle,yellow,yoffset,%
- ytitle%
- },%
- morekeywords={print,None,TypeError},% % additional keywords
- morestring=[b]{"""},% % treat triple quotes as strings
- numbers=left,% % where to put line numbers
- numbersep=10pt,% % how far line numbers are from code
- numberstyle=\bfseries\tiny,% % set to 'none' for no line numbers
- showstringspaces=false,% % show spaces in strings
- showtabs=false,% % show tabs within strings
- stringstyle=\gsfontfamily\color{gsgreen},% % color for strings
- upquote=true,% % how to typeset quotes
-}%
-\NewTCBListing[auto counter,list inside=gsprogs]{glowscriptblock}
- { O{} D(){glowscript.org} m }{%
- breakable,%
- center,%
- code = \newpage,%
- %derivpeach,%
- enhanced,%
- hyperurl interior = https://#2,%
- label = {gs:\thetcbcounter},%
- left = 8mm,%
- list entry = \thetcbcounter~~~~~#3,%
- listing only,%
- listing style = vpython,%
- nameref = {#3},%
- title = \texttt{GlowScript} Program \thetcbcounter: #3,%
- width = 0.9\textwidth,%
- {#1},
-}%
-\NewDocumentCommand{\listofglowscriptprograms}{}{\tcblistof[\section*]{gsprogs}
- {List of \texttt{GlowScript} Programs}}%
-\NewTCBInputListing[auto counter,list inside=vpprogs]{\vpythonfile}
- { O{} m m }{%
- breakable,%
- center,%
- code = \newpage,%
- %derivgray,%
- enhanced,%
- hyperurl interior = https://,%
- label = {vp:\thetcbcounter},%
- left = 8mm,%
- list entry = \thetcbcounter~~~~~#3,%
- listing file = {#2},%
- listing only,%
- listing style = vpython,%
- nameref = {#3},%
- title = \texttt{VPython} Program \thetcbcounter: #3,%
- width = 0.9\textwidth,%
- {#1},%
-}%
-\NewDocumentCommand{\listofvpythonprograms}{}{\tcblistof[\section*]{vpprogs}
- {List of \texttt{VPython} Programs}}%
-\DeclareTotalTCBox{\glowscriptinline}{ m }{%
- bottom = 0pt,%
- bottomrule = 0.0mm,%
- boxsep = 1.0mm,%
- colback = gsbggray,%
- colframe = gsbggray,%
- left = 0pt,%
- leftrule = 0.0mm,%
- nobeforeafter,%
- right = 0pt,%
- rightrule = 0.0mm,%
- sharp corners,%
- tcbox raise base,%
- top = 0pt,%
- toprule = 0.0mm,%
-}{\lstinline[style = vpython]{#1}}%
-\NewDocumentCommand{\vpythoninline}{}{\glowscriptinline}%
+\lstdefinestyle{vpython}%
+ {% % style for listings
+ backgroundcolor=\color{gsbggray},% % background color
+ basicstyle=\colordigits\footnotesize,% % default style
+ breakatwhitespace=true% % break at whitespace
+ breaklines=true,% % break long lines
+ captionpos=b,% % position caption
+ classoffset=1,% % STILL DON'T UNDERSTAND THIS
+ commentstyle=\color{gsgray},% % font for comments
+ deletekeywords={print},% % delete keywords from the given language
+ emph={self,cls,@classmethod,@property},% % words to emphasize
+ emphstyle=\color{gsorange}\itshape,% % font for emphasis
+ escapeinside={(*@}{@*)},% % add LaTeX within your code
+ frame=tb,% % frame style
+ framerule=2.0pt,% % frame thickness
+ framexleftmargin=5pt,% % extra frame left margin
+ %identifierstyle=\sffamily,% % style for identifiers
+ keywordstyle=\gsfontfamily\color{gsplum},% % color for keywords
+ language=Python,% % select language
+ linewidth=\linewidth,% % width of listings
+ morekeywords={% % VPython/Web VPython specific keywords
+ __future__,abs,acos,align,ambient,angle,append,append_to_caption,%
+ append_to_title,arange,arrow,asin,astuple,atan,atan2,attach_arrow,%
+ attach_trail,autoscale,axis,background,billboard,bind,black,blue,border,%
+ bounding_box,box,bumpaxis,bumpmap,bumpmaps,camera,canvas,caption,capture,%
+ ceil,center,clear,clear_trail,click,clone,CoffeeScript,coils,color,combin,%
+ comp,compound,cone,convex,cos,cross,curve,cyan,cylinder,data,degrees,del,%
+ delete,depth,descender,diff_angle,digits,division,dot,draw_complete,%
+ ellipsoid,emissive,end_face_color,equals,explog,extrusion,faces,factorial,%
+ False,floor,follow,font,format,forward,fov,frame,gcurve,gdisplay,gdots,%
+ get_library,get_selected,ghbars,global,GlowScript,graph,graphs,green,gvbars,%
+ hat,headlength,headwidth,height,helix,hsv_to_rgb,index,interval,keydown,%
+ keyup,label,length,lights,line,linecolor,linewidth,logx,logy,lower_left,%
+ lower_right,mag,mag2,magenta,make_trail,marker_color,markers,material,%
+ max,min,mouse,mousedown,mousemove,mouseup,newball,norm,normal,objects,%
+ offset,one,opacity,orange,origin,path,pause,pi,pixel_to_world,pixels,plot,%
+ points,pos,pow,pps,print,print_function,print_options,proj,purple,pyramid,%
+ quad,radians,radius,random,rate,ray,read_local_file,readonly,red,redraw,%
+ retain,rgb_to_hsv,ring,rotate,round,scene,scroll,shaftwidth,shape,shapes,%
+ shininess,show_end_face,show_start_face,sign,sin,size,size_units,sleep,%
+ smooth,space,sphere,sqrt,start,start_face_color,stop,tan,text,textpos,%
+ texture,textures,thickness,title,trail_color,trail_object,trail_radius,%
+ trail_type,triangle,trigger,True,twist,unbind,up,upper_left,upper_right,%
+ userpan,userspin,userzoom,vec,vector,vertex,vertical_spacing,visible,%
+ visual,vpython,VPython,waitfor,WebVPython,white,width,world,xtitle,%
+ yellow,yoffset,ytitle%
+ },%
+ morekeywords={print,None,TypeError},% % additional keywords
+ morestring=[b]{"""},% % treat triple quotes as strings
+ numbers=left,% % where to put line numbers
+ numbersep=10pt,% % how far line numbers are from code
+ numberstyle=\bfseries\tiny,% % set to 'none' for no line numbers
+ showstringspaces=false,% % show spaces in strings
+ showtabs=false,% % show tabs within strings
+ stringstyle=\gsfontfamily\color{gsgreen},% % color for strings
+ upquote=true,% % how to typeset quotes
+ }%
+\AtBeginEnvironment{webvpythonblock}{\catcode`\#=12}
+\AtEndEnvironment{webvpythonblock}{\catcode`\#=6}
+\NewTCBListing[auto counter,list inside=gsprogs]{webvpythonblock}{ O{} D(){webvpython.org} m }%
+ {%
+ breakable,%
+ center,%
+ code = \newpage,%
+ %derivpeach,%
+ enhanced,%
+ hyperurl interior = https://#2,%
+ label = {gs:\thetcbcounter},%
+ left = 8mm,%
+ list entry = \thetcbcounter~~~~~#3,%
+ listing only,%
+ listing style = vpython,%
+ nameref = {#3},%
+ title = \begin{minipage}{1.5cm}%
+ \protect\qrcode*{https://#2}%
+ \end{minipage}\hspace{5mm}%
+ \begin{minipage}{0.7\textwidth}%
+ \texttt{Web VPython} Program \thetcbcounter: #3%
+ \end{minipage},%
+ width = 0.9\textwidth,%
+ {#1},
+ }%
+\AtBeginEnvironment{webvpythonblock*}{\catcode`\#=12}
+\AtEndEnvironment{webvpythonblock*}{\catcode`\#=6}
+\NewTCBListing[use counter from=webvpythonblock,list inside=gsprogs]
+ {webvpythonblock*}{ O{} D(){webvpython.org} m }%
+ {%
+ breakable,%
+ center,%
+ code = \newpage,%
+ %derivpeach,%
+ enhanced,%
+ hyperurl interior = https://#2,%
+ label = {gs:\thetcbcounter},%
+ left = 8mm,%
+ list entry = \thetcbcounter~~~~~#3,%
+ listing only,%
+ listing style = vpython,%
+ nameref = {#3},%
+ title = \texttt{Web VPython} Program \thetcbcounter: #3,%
+ width = 0.9\textwidth,%
+ {#1},
+ }%
+\NewDocumentCommand{\listofwebvpythonprograms}{}%
+ {%
+ \tcblistof[\section*]{gsprogs}{List of \texttt{Web VPython} Programs}%
+ }%
+\newcommand*{\vpythonfile}{\catcode`\#=12 \vpythonfile@auxA}
+\NewDocumentCommand{\vpythonfile@auxA}{ O{} D(){vpython.org} m m }%
+ {%
+ \vpythonfile@auxB[#1](#2){#3}{#4}%
+ \catcode`\#=6
+ }%
+\NewTCBInputListing[auto counter,list inside=vpprogs]
+ {\vpythonfile@auxB}{ O{} D(){vpython.org} m m }%
+ {%
+ breakable,%
+ center,%
+ code = \newpage,%
+ %derivgray,%
+ enhanced,%
+ hyperurl interior = https://#2,%
+ label = {vp:\thetcbcounter},%
+ left = 8mm,%
+ list entry = \thetcbcounter~~~~~#4,%
+ listing file = {#3},%
+ listing only,%
+ listing style = vpython,%
+ nameref = {#4},%
+ title = \texttt{VPython} Program \thetcbcounter: #4,%
+ width = 0.9\textwidth,%
+ {#1},%
+ }%
+\NewDocumentCommand{\listofvpythonprograms}{}%
+ {%
+ \tcblistof[\section*]{vpprogs}{List of \texttt{VPython} Programs}%
+ }%
+\DeclareTotalTCBox{\webvpythoninline}{ m }%
+ {%
+ bottom = 0pt,%
+ bottomrule = 0.0mm,%
+ boxsep = 1.0mm,%
+ colback = gsbggray,%
+ colframe = gsbggray,%
+ left = 0pt,%
+ leftrule = 0.0mm,%
+ nobeforeafter,%
+ right = 0pt,%
+ rightrule = 0.0mm,%
+ sharp corners,%
+ tcbox raise base,%
+ top = 0pt,%
+ toprule = 0.0mm,%
+ }%
+ {\lstinline[style = vpython]{#1}}%
+\NewDocumentCommand{\vpythoninline}{}{\webvpythoninline}%
\endinput
%%
%% End of file `mandistudent.sty'.
generated by cgit v1.2.3 (git 2.39.1) at 2024-11-14 23:55:06 +0000