mandi (27mar18)

git-svn-id: svn://tug.org/texlive/trunk@47150 c570f23f-e606-0410-a88d-b1316a301751

1 files changed, 75 insertions, 73 deletions

diff --git a/Master/texmf-dist/tex/latex/mandi/mandi.sty b/Master/texmf-dist/tex/latex/mandi/mandi.sty
index 2aa2008ba60..0338670e13c 100644
--- a/Master/texmf-dist/tex/latex/mandi/mandi.sty
+++ b/Master/texmf-dist/tex/latex/mandi/mandi.sty
@@ -28,7 +28,7 @@
 %%                                  vdemo.py.
 %% ---------------------------------------------------------------------------
 %% 
-%%\ProvidesPackage{mandi}[2018/01/15 2.7.1 Macros for physics and astronomy]
+%%\ProvidesPackage{mandi}[2018/03/20 2.7.2 Macros for physics and astronomy]
 \NeedsTeXFormat{LaTeX2e}[1999/12/01]
 
 \RequirePackage{amsmath}
@@ -104,13 +104,15 @@
 \newboolean{@optsinglemagbars}
 \newboolean{@optbaseunits}
 \newboolean{@optdrvdunits}
+\newboolean{@optaltnunits}
 \newboolean{@optapproxconsts}
 \newboolean{@optuseradians}
 \setboolean{@optromanvectors}{false}   % this is where you set the default option
 \setboolean{@optboldvectors}{false}    % this is where you set the default option
 \setboolean{@optsinglemagbars}{false}  % this is where you set the default option
 \setboolean{@optbaseunits}{false}      % this is where you set the default option
-\setboolean{@optdrvdunits}{false}      % this is where you set the default option
+\setboolean{@optdrvdunits}{true}       % this is where you set the default option
+\setboolean{@optaltnunits}{false}      % this is where you set the default option
 \setboolean{@optapproxconsts}{false}   % this is where you set the default option
 \setboolean{@optuseradians}{false}     % this is where you set the default option
 \DeclareOption{romanvectors}{\setboolean{@optromanvectors}{true}}
@@ -122,9 +124,9 @@
 \DeclareOption{useradians}{\setboolean{@optuseradians}{true}}
 \ProcessOptions\relax
 \newcommand*{\mandiversion}{\ifmmode%
-    2.7.1\mbox{ dated }2018/01/15%
+    2.7.2\mbox{ dated }2018/03/20%
   \else%
-    2.7.1 dated 2018/01/15%
+    2.7.2 dated 2018/03/20%
   \fi
   }%
 \typeout{                                                }
@@ -208,20 +210,20 @@
     \expandafter\@firstoftwo\expandafter{\iffalse}\fi0 #3}{0 #2}}}%
 \newcommand*\selectbaseunit[3]{#1}
 \newcommand*\selectdrvdunit[3]{#2}
-\newcommand*\selecttradunit[3]{#3}
+\newcommand*\selectaltnunit[3]{#3}
 \newcommand*\selectunit{}
 \newcommand*\perpusebaseunit{\let\selectunit=\selectbaseunit}
 \newcommand*\perpusedrvdunit{\let\selectunit=\selectdrvdunit}
-\newcommand*\perpusetradunit{\let\selectunit=\selecttradunit}
+\newcommand*\perpusealtnunit{\let\selectunit=\selectaltnunit}
 \newcommand*\hereusebaseunit[1]{%
   \begingroup\perpusebaseunit#1\endgroup}%
 \newcommand*\hereusedrvdunit[1]{%
   \begingroup\perpusedrvdunit#1\endgroup}%
-\newcommand*\hereusetradunit[1]{%
-  \begingroup\perpusetradunit#1\endgroup}%
+\newcommand*\hereusealtnunit[1]{%
+  \begingroup\perpusealtnunit#1\endgroup}%
 \newenvironment{usebaseunit}{\perpusebaseunit}{}%
 \newenvironment{usedrvdunit}{\perpusedrvdunit}{}%
-\newenvironment{usetradunit}{\perpusetradunit}{}%
+\newenvironment{usealtnunit}{\perpusealtnunit}{}%
 \newcommand*\newphysicsquantity{\definephysicsquantity{\newcommand}}
 \newcommand*\redefinephysicsquantity{\definephysicsquantity{\renewcommand}}
 \newcommandx*\definephysicsquantity[5][4=,5=]{%
@@ -238,11 +240,11 @@
   \mi@name#4{#5}#7{\unit{#8}{\selectunit{#3}{#1}{#2}}}%
   \mi@name#4{#5baseunit}#7{\unit{#8}{#3}}%
   \mi@name#4{#5drvdunit}#7{\unit{#8}{#1}}%
-  \mi@name#4{#5tradunit}#7{\unit{#8}{#2}}%
+  \mi@name#4{#5altnunit}#7{\unit{#8}{#2}}%
   \mi@name#4{#5onlyunit}{\selectunit{#3}{#1}{#2}}%
   \mi@name#4{#5onlybaseunit}{\ensuremath{#3}}%
   \mi@name#4{#5onlydrvdunit}{\ensuremath{#1}}%
-  \mi@name#4{#5onlytradunit}{\ensuremath{#2}}%
+  \mi@name#4{#5onlyaltnunit}{\ensuremath{#2}}%
   \mi@name#4{#5value}#7{\ensuremath{#8}}%
   \mi@forkifnull{#7}{%
     \ifx#4\renewcommand\mi@name\let{#5mathsymbol}=\relax\fi
@@ -261,8 +263,8 @@
   {\ifthenelse{\boolean{@optdrvdunits}}
      {\perpusedrvdunit %
       \typeout{mandi: You'll get derived units.}}
-     {\perpusetradunit %
-      \typeout{mandi: You'll get traditional units.}}}
+     {\perpusealtnunit %
+      \typeout{mandi: You'll get alternate units.}}}
 \ifthenelse{\boolean{@optapproxconsts}}
   {\typeout{mandi: You'll get approximate constants.}}
   {\typeout{mandi: You'll get precise constants.}}
@@ -322,7 +324,7 @@
 \newcommand*{\insolarD}[1]{\unit{#1}{\Dsolar}}
 \newcommand*{\insolard}[1]{\unit{#1}{\dsolar}}
 \newcommand*{\velocityc}[1]{\ensuremath{#1c}}
-\newcommand*{\lorentz}[1]{\ensuremath{#1}}
+\newcommand*{\lorentzfactor}[1]{\ensuremath{#1}}
 \newcommand*{\speed}{\velocity}
 \newphysicsquantity{displacement}%
   {\m}%
@@ -434,16 +436,16 @@
   []
 \newphysicsquantity{work}%
   {\m\squared\usk\kg\usk\s\reciprocalsquared}%
-  [\N\usk\m]%
-  [\J]
+  [\J]%
+  [\N\usk\m]
 \newphysicsquantity{energy}%
   {\m\squared\usk\kg\usk\s\reciprocalsquared}%
-  [\N\usk\m]%
-  [\J]
+  [\J]%
+  [\N\usk\m]
 \newphysicsquantity{power}%
   {\m\squared\usk\kg\usk\s\reciprocalcubed}%
-  [\J\per\s]%
-  [\W]
+  [\W]%
+  [\J\per\s]
 \newphysicsquantity{specificheatcapacity}%
   {\J\per\K\usk\kg}%
   [\J\per\K\usk\kg]%
@@ -458,18 +460,18 @@
   [\rad\per\s\squared]
 \newphysicsquantity{momentofinertia}%
   {\m\squared\usk\kg}%
-  [\m\usk\kg\squared]%
+  [\m\squared\usk\kg]%
   [\J\usk\s\squared]
 \ifthenelse{\boolean{@optuseradians}}
   {%
   \newphysicsquantity{angularmomentum}%
     {\m\squared\usk\kg\usk\reciprocal\s\usk\reciprocal\rad}%
-    [\N\usk\m\usk\s\per\rad]%
-    [\m\squared\usk\kg\usk\reciprocal\s\usk\reciprocal\rad]
+    [\kg\usk\m\squared\per(\s\usk\rad)]%
+    [\N\usk\m\usk\s\per\rad]
   \newphysicsquantity{angularimpulse}%
     {\m\squared\usk\kg\usk\reciprocal\s\usk\reciprocal\rad}%
-    [\N\usk\m\usk\s\per\rad]%
-    [\J\usk\s\per\rad]
+    [\J\usk\s\per\rad]%
+    [\N\usk\m\usk\s\per\rad]
   \newphysicsquantity{torque}%
     {\m\squared\usk\kg\usk\s\reciprocalsquared\usk\reciprocal\rad}%
     [\N\usk\m\per\rad]%
@@ -478,12 +480,12 @@
   {%
   \newphysicsquantity{angularmomentum}%
     {\m\squared\usk\kg\usk\reciprocal\s}%
-    [\N\usk\m\usk\s]%
-    [\m\squared\usk\kg\usk\reciprocal\s]
+    [\kg\usk\m\squared\per\s]%
+    [\N\usk\m\usk\s]
   \newphysicsquantity{angularimpulse}%
     {\m\squared\usk\kg\usk\reciprocal\s}%
-    [\N\usk\m\usk\s]%
-    [\J\usk\s]
+    [\J\usk\s]%
+    [\N\usk\m\usk\s]
   \newphysicsquantity{torque}%
     {\m\squared\usk\kg\usk\s\reciprocalsquared}%
     [\N\usk\m]%
@@ -515,36 +517,36 @@
   [\C]
 \newphysicsquantity{permittivity}%
   {\m\reciprocalcubed\usk\reciprocal\kg\usk\s\reciprocalquarted\usk\A\squared}%
-  [\F\per\m]%
-  [\C\squared\per\N\usk\m\squared]
+  [\C\squared\per\N\usk\m\squared]%
+  [\F\per\m]
 \newphysicsquantity{permeability}%
   {\m\usk\kg\usk\s\reciprocalsquared\usk\A\reciprocalsquared}%
-  [\henry\per\m]%
-  [\T\usk\m\per\A]
+  [\T\usk\m\per\A]%
+  [\henry\per\m]
 \newphysicsquantity{electricfield}%
   {\m\usk\kg\usk\s\reciprocalcubed\usk\reciprocal\A}%
-  [\V\per\m]%
-  [\N\per\C]
+  [\N\per\C]%
+  [\V\per\m]
 \newphysicsquantity{electricdipolemoment}%
   {\m\usk\s\usk\A}%
   [\C\usk\m]%
   [\C\usk\m]
 \newphysicsquantity{electricflux}%
   {\m\cubed\usk\kg\usk\s\reciprocalcubed\usk\reciprocal\A}%
-  [\V\usk\m]%
-  [\N\usk\m\squared\per\C]
+  [\N\usk\m\squared\per\C]%
+  [\V\usk\m]
 \newphysicsquantity{magneticfield}%
   {\kg\usk\s\reciprocalsquared\usk\reciprocal\A}%
   [\T]%
   [\N\per\C\usk(\m\per\s)] % also \Wb\per\m\squared
 \newphysicsquantity{magneticflux}%
   {\m\squared\usk\kg\usk\s\reciprocalsquared\usk\reciprocal\A}%
-  [\volt\usk\s]%
-  [\T\usk\m\squared] % also \Wb and \J\per\A
+  [\T\usk\m\squared]%
+  [\volt\usk\s] % also \Wb and \J\per\A
 \newphysicsquantity{cmagneticfield}%
   {\m\usk\kg\usk\s\reciprocalcubed\usk\reciprocal\A}%
-  [\V\per\m]%
-  [\N\per\C]
+  [\N\per\C]%
+  [\V\per\m]
 \newphysicsquantity{linearchargedensity}%
   {\reciprocal\m\usk\s\usk\A}%
   [\C\per\m]%
@@ -571,12 +573,12 @@
   [\C\usk\m\per(\N\per\C)]
 \newphysicsquantity{electricpotential}%
   {\square\m\usk\kg\usk\reciprocalcubic\s\usk\reciprocal\A}%
-  [\J\per\C]%
-  [\V]
+  [\V]%
+  [\J\per\C]
 \newphysicsquantity{emf}%
   {\square\m\usk\kg\usk\reciprocalcubic\s\usk\reciprocal\A}%
-  [\J\per\C]%
-  [\V]
+  [\V]%
+  [\J\per\C]
 \newphysicsquantity{dielectricconstant}%
   {}%
   []%
@@ -611,16 +613,16 @@
   [\ensuremath{\mathrm{e}}\per\s]
 \newphysicsquantity{conventionalcurrent}%
   {\A}%
-  [\C\per\s]%
-  [\A]
+  [\A]%
+  [\C\per\s]
 \newphysicsquantity{magneticdipolemoment}%
   {\square\m\usk\A}%
-  [\J\per\T]%
-  [\A\usk\square\m]
+  [\A\usk\square\m]%
+  [\J\per\T]
 \newphysicsquantity{currentdensity}%
   {\reciprocalsquare\m\usk\A}%
-  [\C\usk\s\per\square\m]%
-  [\A\per\square\m]
+  [\A\per\square\m]%
+  [\C\usk\s\per\square\m]
 \newphysicsquantity{capacitance}%
   {\reciprocalsquare\m\usk\reciprocal\kg\usk\quartic\s\usk\square\A}%
   [\F]%
@@ -631,16 +633,16 @@
   [\volt\usk\s\per\A] % also \square\m\usk\kg\per\C\squared, \Wb\per\A
 \newphysicsquantity{conductivity}%
   {\reciprocalcubic\m\usk\reciprocal\kg\usk\cubic\s\usk\square\A}%
-  [\siemens\per\m]%
-  [(\A\per\square\m)\per(\V\per\m)]
+  [(\A\per\square\m)\per(\V\per\m)]%
+  [\siemens\per\m]
 \newphysicsquantity{resistivity}%
   {\cubic\m\usk\kg\usk\reciprocalcubic\s\usk\reciprocalsquare\A}%
   [\ohm\usk\m]%
   [(\V\per\m)\per(\A\per\square\m)]
 \newphysicsquantity{resistance}%
   {\square\m\usk\kg\usk\reciprocalcubic\s\usk\reciprocalsquare\A}%
-  [\V\per\A]%
-  [\ohm]
+  [\ohm]%
+  [\V\per\A]
 \newphysicsquantity{conductance}%
   {\reciprocalsquare\m\usk\reciprocal\kg\usk\cubic\s\usk\square\A}%
   [\A\per\V]%
@@ -1184,37 +1186,37 @@
   {\ensuremath{\frac{1}{\phantom{_o}4\pi\epsilon_0}}}%
   {\mi@p{9}{8.9875517873681764}\timestento{9}}%
   {\m\cubed\usk\kg\usk\reciprocalquartic\s\usk\A\reciprocalsquared}%
-  [\m\per\farad]%
-  [\newton\usk\m\squared\per\coulomb\squared]
+  [\newton\usk\m\squared\per\coulomb\squared]%
+  [\m\per\farad]
 \newphysicsconstant{oofpezcs}%
   {\ensuremath{\frac{1}{\phantom{_o}4\pi\epsilon_0 c^2\phantom{_o}}}}%
   {\tento{-7}}%
   {\m\usk\kg\usk\s\reciprocalsquared\usk\A\reciprocalsquared}%
-  [\T\usk\m\squared]%
-  [\N\usk\s\squared\per\C\squared]
+  [\N\usk\s\squared\per\C\squared]%
+  [\T\usk\m\squared]
 \newphysicsconstant{vacuumpermittivity}%
   {\ensuremath{\epsilon_0}}%
   {\mi@p{9.0}{8.854187817}\timestento{-12}}%
   {\m\reciprocalcubed\usk\reciprocal\kg\usk\s\quarted\usk\A\squared}%
-  [\F\per\m]%
-  [\C\squared\per\N\usk\m\squared]
+  [\C\squared\per\N\usk\m\squared]%
+  [\F\per\m]
 \newphysicsconstant{mzofp}%
   {\ensuremath{\frac{\phantom{_oo}\mu_0\phantom{_o}}{4\pi}}}%
   {\tento{-7}}%
   {\m\usk\kg\usk\s\reciprocalsquared\usk\A\reciprocalsquared}%
-  [\henry\per\m]%
-  [\tesla\usk\m\per\A]
+  [\tesla\usk\m\per\A]%
+  [\henry\per\m]
 \newphysicsconstant{vacuumpermeability}%
   {\ensuremath{\mu_0}}%
   {4\pi\timestento{-7}}%
   {\m\usk\kg\usk\s\reciprocalsquared\usk\A\reciprocalsquared}%
-  [\henry\per\m]%
-  [\T\usk\m\per\A]
+  [\T\usk\m\per\A]%
+  [\henry\per\m]
 \newphysicsconstant{boltzmann}%
   {\ensuremath{k_B}}%
   {\mi@p{1.4}{1.38064852}\timestento{-23}}%
   {\m\squared\usk\kg\usk\reciprocalsquare\s\usk\reciprocal\K}%
-  [\joule\per\K]%
+  [\J\per\K]%
   [\J\per\K]
 \newphysicsconstant{boltzmannineV}%
   {\ensuremath{k_B}}%
@@ -1226,7 +1228,7 @@
   {\ensuremath{\sigma}}%
   {\mi@p{5.7}{5.670367}\timestento{-8}}%
   {\kg\usk\s\reciprocalcubed\usk\K\reciprocalquarted}%
-  [\W\per\m\squared\usk\K^4]%
+  [\W\per\m\squared\usk\K\quarted]%
   [\W\per\m\squared\usk\K\quarted]
 \newphysicsconstant{planck}%
   {\ensuremath{h}}%
@@ -1292,8 +1294,8 @@
   {\ensuremath{G}}%
   {\mi@p{6.7}{6.67408}\timestento{-11}}%
   {\m\cubed\usk\reciprocal\kg\usk\s\reciprocalsquared}%
-  [\J\usk\m\per\kg\squared]%
-  [\N\usk\m\squared\per\kg\squared]
+  [\N\usk\m\squared\per\kg\squared]%
+  [\J\usk\m\per\kg\squared]
 \newphysicsconstant{surfacegravfield}%
   {\ensuremath{g}}%
   {\mi@p{9.8}{9.807}}%
@@ -2433,9 +2435,9 @@
 \newcommand*{\chkquantity}[1]{%
   \begin{center}
     \begin{tabular}{C{4.5cm} C{4cm} C{4cm} C{4cm}}
-      name    & baseunit & drvdunit & tradunit \tabularnewline
+      name    & baseunit & drvdunit & altnunit \tabularnewline
       \cs{#1} & \csname #1onlybaseunit\endcsname & \csname #1onlydrvdunit\endcsname &
-        \csname #1onlytradunit\endcsname
+        \csname #1onlyaltnunit\endcsname
     \end{tabular}
   \end{center}
 }%
@@ -2445,9 +2447,9 @@
       name    & symbol & value \tabularnewline
       \cs{#1} & \csname #1mathsymbol\endcsname & \csname #1value\endcsname
       \tabularnewline
-      baseunit & drvdunit & tradunit \tabularnewline
+      baseunit & drvdunit & altnunit \tabularnewline
       \csname #1onlybaseunit\endcsname & \csname #1onlydrvdunit\endcsname &
-      \csname #1onlytradunit\endcsname
+      \csname #1onlyaltnunit\endcsname
     \end{tabular}
   \end{center}
 }%