texlive[47150] Master/texmf-dist: mandi (27mar18)
commits+karl at tug.org
commits+karl at tug.org
Tue Mar 27 23:24:51 CEST 2018
Revision: 47150
http://tug.org/svn/texlive?view=revision&revision=47150
Author: karl
Date: 2018-03-27 23:24:50 +0200 (Tue, 27 Mar 2018)
Log Message:
-----------
mandi (27mar18)
Modified Paths:
--------------
trunk/Master/texmf-dist/doc/latex/mandi/mandi.pdf
trunk/Master/texmf-dist/source/latex/mandi/mandi.dtx
trunk/Master/texmf-dist/tex/latex/mandi/mandi.sty
Modified: trunk/Master/texmf-dist/doc/latex/mandi/mandi.pdf
===================================================================
(Binary files differ)
Modified: trunk/Master/texmf-dist/source/latex/mandi/mandi.dtx
===================================================================
--- trunk/Master/texmf-dist/source/latex/mandi/mandi.dtx 2018-03-27 21:24:36 UTC (rev 47149)
+++ trunk/Master/texmf-dist/source/latex/mandi/mandi.dtx 2018-03-27 21:24:50 UTC (rev 47150)
@@ -32,7 +32,7 @@
%</internal>
%
%<*package>
-%%\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]
%</package>
%
@@ -130,7 +130,7 @@
% \newcommand*{\opt}[1]{\textsf{\textbf{#1}}}
% \newcommand*{\baseunits}{\emph{baseunits}}
% \newcommand*{\drvdunits}{\emph{drvdunits}}
-% \newcommand*{\tradunits}{\emph{tradunits}}
+% \newcommand*{\altnunits}{\emph{altnunits}}
%
% \IndexPrologue{\section{Index}Page numbers refer to page where the
% corresponding entry is described. Not every command defined in the
@@ -230,14 +230,64 @@
% which creates DVI files.
%
% \changes{v2.7.0}{2018/01/11}{Added instructions for Overleaf users.}
+% \changes{v2.7.2}{2018/03/20}{Added expanded instructions for Overleaf users.}
+% \newpage
% \section{Overleaf Users}
-% \href{https://www.overleaf.com}{Overleaf} is an online \LaTeX\ environment with
-% widespread use. It uses a full \TeX/\LaTeX\ installation but doesn't always
-% have the latest version of every package installed. Sometimes packages are updated
-% more frequently than the large distributions are updated. If you want to always be
-% sure you're using the latest version of \mandi\ make sure the files
-% \pkgname{mandi.sty} and \pkgname{mandi.pdf} are in your Overleaf project folder.
+% \href{https://www.overleaf.com}{Overleaf.com} is an online \LaTeX\ environment
+% with widespread use. It uses a full \TeX/\LaTeX\ installation but may not always
+% have the latest version of every package installed (for stability reasons).
+% Sometimes packages are updated more frequently than the large distributions are
+% updated. If you want to always be sure you're using the latest version of \mandi\
+% make sure the files \pkgname{mandi.sty} and \pkgname{mandi.pdf} are in your
+% Overleaf project folder. The package can now be used in your documents.
%
+% If you are a student, here are detailed instructions on how to use \mandi\
+% in your Overleaf project.
+% \begin{enumerate}
+% \item Direct your browser to
+% \href{http://sticksandshadows.com/downloads/index.html}
+% {http://sticksandshadows.com/downloads/index.html} and fetch the file named
+% \texttt{overleaf-template.zip}. You can
+% \href{http://sticksandshadows.com/downloads/files/overleaf-template.zip}
+% {directly fetch the file} if you wish. Open the zip file into a temporary
+% folder.
+% \item Go to the \href{https://www.overleaf.com}{Overleaf.com} website and
+% create a free account and then sign into that account.
+% \item Upon signing in, you should see a list of your current projects. Look
+% for the New Project button on the left and click on it. Click on Basics in
+% the menu of project templates, and then select the Blank Paper template on
+% the right (it's the first template in the list). A new empty project will
+% be created and you will be taken to the \texttt{main.tex} file in that project.
+% \item In the toolbar, click on Project. Your project's folder will be opened
+% and you can see the files present in the folder. At this point, there should
+% be only one, \texttt{main.tex}. Click on Files (just under the Overleaf logo
+% in the toolbar, and select the option for where your template files reside on
+% your computer.
+% \item Select all the files in the overleaf-template folder you just created.
+% Upload them into your project's folder. You can now delete the \texttt{main.tex}
+% file. Click on the
+% \texttt{NnnnnnnnCCPxx.tex} file and it will become the new main file in the
+% project.
+% \item On the far right of the toolbar, find your name. Click on it and then
+% click on My Projects. You will be taken to your main window where you can
+% see your current projects. Find the one named |\documentname| (it
+% should be the most recently created project). In the lower righthand corner
+% of the project's rectangular window, click on the triangle and select
+% Rename. I suggest renaming the project Master Template or something very similar
+% to that.
+% \item From now on, to start a new document, begin by copying this master
+% project template and creating a new name for the new document. This way,
+% you will build a neatly organize collection of logically named projects
+% and the original Master Template will never have to be modified (but see
+% next step) and every project will have \mandi\ available for use.
+% \item If \mandi\ is updated by the developer, all you need to do is make
+% sure the new \texttt{mandi.sty} and \texttt{mandi.pdf} files, and perhaps
+% a few others if the developer has modified them, are uploaded to your project
+% folders.
+% \item You can now delete the \texttt{overleaf-template.zip} file and the
+% temporary folder you created.
+% \end{enumerate}
+%
% \newpage
% \section{Loading the Package}\label{LoadingthePackage}
% To load \mandi\ with its default options, simply put the line |\usepackage{mandi}|
@@ -257,6 +307,8 @@
% \changes{v2.6.0}{2016/05/23}{Loads the \pkgname{tensor} package for future use.}
% \changes{v2.7.0}{2017/02/02}{Added blank output lines around mandi messages
% during compilation.}
+% \changes{v2.7.2}{2018/03/14}{Changed \emph{tradunits} to \opt{altnunits}.}
+% \changes{v2.7.2}{2018/03/19}{Made \opt{drvdunits} the default.}
%
% \begin{itemize}
% \item \opt{boldvectors} gives bold letters for the kernels of vector names.
@@ -281,18 +333,17 @@
% are used to denote powers of various base units.
% \item \opt{drvdunits} causes all units to be displayed, when possible, in
% \drvdunits\ form, with SI derived units. Students may already be familiar with
-% many of these derived units.
-% \item If neither \opt{baseunits} nor \opt{drvdunits} is specified (the
-% default), units are displayed in what I call \tradunits\ form, which
-% is typically the way they would traditionally appear in textbooks. Units in
-% this form frequently hide the underlying physical meaning and are probably not
-% best pedagogically but are familiar to students and teachers. In this document,
-% the default is to use
+% many of these derived units. This documentation \mandi\ with this option.
+% \item If neither \opt{baseunits} nor \opt{altnunits} is specified, units are
+% displayed in \drvdunits\ form, which is typically the way they would usually
+% appear in textbooks. Units in this form may hide the underlying physical
+% meaning or indeed may do precisely the opposite and enhance conceptual
+% understanding. In this document, the default is to use
% \ifthenelse{\boolean{@optbaseunits}}
% {base}
-% {\ifthenelse{\boolean{@optdrvdunits}}
-% {derived}
-% {traditional}}
+% {\ifthenelse{\boolean{@optaltnunits}}
+% {alternate}
+% {derived}}
% units. As you will see later, there are ways to override these options either
% temporarily or permanently.
% \end{itemize}
@@ -421,6 +472,12 @@
-T_{10} & T_{11} & -T_{12} \\
\hphantom{-}T_{20} & T_{21} & \hphantom{-}T_{22}
\end{vmatrix}\]
+ Alternate notation for the determinant of a matrix.
+ \[\begin{Vmatrix}
+ \hphantom{-}T_{00} & T_{01} & -T_{02} \\
+ -T_{10} & T_{11} & -T_{12} \\
+ \hphantom{-}T_{20} & T_{21} & \hphantom{-}T_{22}
+ \end{Vmatrix}\]
\end{dispExample*}
%\iffalse
%</example>
@@ -489,7 +546,7 @@
% lot about the document that you won't understand at first. Look for a line that
% says |\begin{document}| and a corresponding line that says |\end{document}| You
% will add content between these two lines. Most of your content will be within the
-% \hyperlink{target1}{|problem|} environment. Each use of the |problem| environment
+% \refEnv{problem} environment. Each use of the |problem| environment
% is intended to encapsulate one complete written solution to one physics problem.
% In this way, you can build a library of problem solutions for your own convenience.
%
@@ -498,9 +555,9 @@
% can be tedious to the beginner and some of the commands have been designed to
% minimize the tedium. For example, if you want to calculate something using an
% equation, you typically must write the equation, substitute numerical quantities
-% with units if necessary, do the actual calculation, and then state the final result.
-% Sometimes it is necessary to show intermediate steps in a calculation. \mandi\
-% can help with this.
+% with units if necessary, do the actual calculation, and then state the final
+% result.Sometimes it is necessary to show intermediate steps in a calculation.
+% \mandi\ can help with this.
%
% Here is a set of commands that typeset standard equations with placeholders where
% numerical quantities must be eventually inserted. Note that all of these commands
@@ -1057,7 +1114,7 @@
%<*example>
%\fi
\begin{docCommand}{newphysicsquantity}
-{\marg{newname}\marg{\baseunits}\oarg{\drvdunits}\oarg{\tradunits}}
+{\marg{newname}\marg{\baseunits}\oarg{\drvdunits}\oarg{\altnunits}}
Defines a new physics quantity and its associated commands.
\end{docCommand}
%\iffalse
@@ -1071,7 +1128,7 @@
% takes one mandatory argument, a numerical magnitude. Subsequent use of your
% defined scalar quantity can be invoked by typing \colDef{\cs{newname}}
% \marg{magnitude} and the units will be typeset according to the options
-% given when \mandi\ was loaded. Note that if the \drvdunits\ and \tradunits\
+% given when \mandi\ was loaded. Note that if the \drvdunits\ and \altnunits\
% forms are not specified, they will be populated with the \baseunits\ form.
% \item A command \colDef{\cs{newnamebaseunit}}\marg{magnitude} is created that
% expresses the quantity and its units in \baseunits\ form.
@@ -1078,15 +1135,15 @@
% \item A command \colDef{\cs{newnamedrvdunit}}\marg{magnitude} is created that
% expresses the quantity and its units in \drvdunits\ form. This command is
% created whether or not the first optional argument is provided.
-% \item A command \colDef{\cs{newnametradunit}}\marg{magnitude} is created that
-% expresses the quantity and its units in \tradunits\ form. This command is
+% \item A command \colDef{\cs{newnamealtnunit}}\marg{magnitude} is created that
+% expresses the quantity and its units in \altnunits\ form. This command is
% created whether or not the first optional argument is provided.
% \item A command \colDef{\cs{newnameonlybaseunit}}\marg{magnitude} is created
% that expresses \textbf{only} the quantity's units in \baseunits\ form.
% \item A command \colDef{\cs{newnameonlydrvdunit}}\marg{magnitude} is created
% that expresses \textbf{only} the quantity's units in \drvdunits\ form.
-% \item A command \colDef{\cs{newnameonlytradunit}}\marg{magnitude} is created
-% that expresses \textbf{only} the quantity's units in \tradunits\ form.
+% \item A command \colDef{\cs{newnameonlyaltnunit}}\marg{magnitude} is created
+% that expresses \textbf{only} the quantity's units in \altnunits\ form.
% \item A command \colDef{\cs{newnamevalue}}\marg{magnitude} is created that
% expresses \textbf{only} the quantity's numerical value.
% \end{itemize}
@@ -1095,14 +1152,14 @@
%
% \begin{quotation}
% \begin{tabular}{l l l}
-% |\momentum{3}| &\momentum{3} & unit set by global options \\
-% |\momentumbaseunit{3}| &\momentumbaseunit{3} & quantity with base unit \\
-% |\momentumdrvdunit{3}| &\momentumdrvdunit{3} & quantity with derived unit \\
-% |\momentumtradunit{3}| &\momentumtradunit{3} & quantity with traditional unit \\
-% |\momentumvalue{3}| &\momentumvalue{3} & selects only numerical value \\
-% |\momentumonlybaseunit|&\momentumonlybaseunit & selects only base unit \\
-% |\momentumonlydrvdunit|&\momentumonlydrvdunit & selects only derived unit \\
-% |\momentumonlytradunit|&\momentumonlytradunit & selects only traditional unit
+% |\momentum{3}| &\momentum{3} & unit set by global options \\
+% |\momentumbaseunit{3}| &\momentumbaseunit{3} & quantity with base unit \\
+% |\momentumdrvdunit{3}| &\momentumdrvdunit{3} & quantity with derived unit \\
+% |\momentumaltnunit{3}| &\momentumaltnunit{3} & quantity with alternate unit \\
+% |\momentumvalue{3}| &\momentumvalue{3} & selects only numerical value \\
+% |\momentumonlybaseunit|&\momentumonlybaseunit & selects only base unit \\
+% |\momentumonlydrvdunit|&\momentumonlydrvdunit & selects only derived unit \\
+% |\momentumonlyaltnunit|&\momentumonlyaltnunit & selects only alternate unit
% \end{tabular}
% \end{quotation}
%
@@ -1140,8 +1197,8 @@
% where the notation corresponds to that used in \mi.
%
% \subsubsection{First Semester Physics}
-% The first semester of most traditional introductory calculus-based physics
-% courses focuses on mechanics, dynamics, and statistical mechanics.
+% The first semester of most introductory calculus-based physics courses focuses
+% on mechanics, dynamics, and statistical mechanics.
%
%\changes{v2.6.0}{2016/04/30}{Added \cs{vectordisplacement}.}
%\iffalse
@@ -1755,17 +1812,17 @@
%\fi
%
-
+%\changes{v2.7.2}{2018/03/18}{Changed \cs{lorentz} to \cs{lorentzfactor}.}
%\iffalse
%<*example>
%\fi
-\begin{docCommand}{lorentz}{\marg{magnitude}}
+\begin{docCommand}{lorentzfactor}{\marg{magnitude}}
Command for relativistic Lorentz factor. Obviously this command doesn't do
anything visually, but is included for thinking about calculations where this
quantity is needed.
\end{docCommand}
\begin{dispExample*}{sidebyside}
-\lorentz{2.34}
+\lorentzfactor{2.34}
\end{dispExample*}
%\iffalse
%</example>
@@ -2751,7 +2808,7 @@
% The form of a quantity's unit can be changed on the fly regardless of the
% global format determined by \opt{baseunits} and \opt{drvdunits}. One way,
% as illustrated in the table above, is to append |baseunit|, |drvdunit|,
-% |tradunit| to the quantity's name, and this will override the global options
+% |altnunit| to the quantity's name, and this will override the global options
% for that instance.
%
% A second way is to use the commands that change a quantity's unit on the fly.
@@ -2785,11 +2842,11 @@
%\iffalse
%<*example>
%\fi
-\begin{docCommand}{hereusetradunit}{\marg{magnitude}}
-Command for using traditional units in place.
+\begin{docCommand}{hereusealtnunit}{\marg{magnitude}}
+Command for using alternate units in place.
\end{docCommand}
\begin{dispExample*}{sidebyside}
-\hereusetradunit{\momentum{3}}
+\hereusealtnunit{\momentum{3}}
\end{dispExample*}
%\iffalse
%</example>
@@ -2831,13 +2888,13 @@
%\iffalse
%<*example>
%\fi
-\begin{docEnvironment}{usetradunit}{}
-Environment for using traditional units.
+\begin{docEnvironment}{usealtnunit}{}
+Environment for using alternate units.
\end{docEnvironment}
\begin{dispExample*}{sidebyside}
-\begin{usetradunit}
+\begin{usealtnunit}
\momentum{3}
-\end{usetradunit}
+\end{usealtnunit}
\end{dispExample*}
%\iffalse
%</example>
@@ -2871,14 +2928,37 @@
%\iffalse
%<*example>
%\fi
-\begin{docCommand}{perpusetradunit}{}
-Command for perpetually using traditional units.
+\begin{docCommand}{perpusealtnunit}{}
+Command for perpetually using alternate units.
\end{docCommand}
%\iffalse
%</example>
%\fi
%
+%\subsubsection{Using Alternate Units}
+% In some cases it may be helpful to use unconventional, but pedagogically
+% appropriate, units for certain physical quantities. As an example, consider
+% force. It is normally expressed in newtons, but it can also be expressed in
+% joules per meter. You can redefine a quantity's units on the fly with the
+% \cs{redefinephysicsquantity} command.
+%
+%\changes{v2.7.2}{2018/03/16}{Documented the \cs{redefinephysicsquantity} command.}
+%\iffalse
+%<*example>
+%\fi
+\begin{docCommand}{redefinephysicsquantity}
+{\marg{newname}\marg{\baseunits}\oarg{\drvdunits}\oarg{\altnunits}}
+Redefines an existing physical quantity, allowing for new alternate units. You can
+also change the other units but it strongly discouraged. The new definition takes
+effect immediately.
+\end{docCommand}
+%\iffalse
+%</example>
+%\fi
+%
%\changes{v2.4.0}{2014/12/16}{Added table of all predefined quantities with units.}
+%\changes{v2.7.2}{2018/03/19}{Adjusted units of some predefined quantities and
+% constants.}
%\subsubsection{All Predefined Quantities}
%
%\changes{v2.6.0}{2016/05/20}{Documented \cs{chkquantity}.}
@@ -3006,13 +3086,14 @@
%<*example>
%\fi
\begin{docCommand}{newphysicsconstant}
-{\marg{name}\marg{symbol}{\{\cs{mi at p\marg{approx}\marg{precise}}\}}\marg{\baseunits}\\
-\oarg{\drvdunits}\oarg{\tradunits}%
+{\marg{name}\marg{symbol}{\{\cs{mi at p\marg{approx}\marg{precise}}\}}\marg{\baseunits}
+\\
+\oarg{\drvdunits}\oarg{\altnunits}%
}%
Defines a new physical constant with a name, a symbol, approximate and
precise numerical values, required base units, optional derived units,
-and optional traditional units. The \cs{mi at p} command is defined
+and optional alternate units. The \cs{mi at p} command is defined
internally and is not meant to be otherwise used.
\end{docCommand}
\begin{dispListing}
@@ -3045,17 +3126,37 @@
% the constant and its units in \baseunits\ form.
% \item A command \cs{namedrvdunit} is created that expresses
% the constant and its units in \drvdunits\ form.
-% \item A command \cs{nametradunit} is created that
-% expresses the constant and its units in \tradunits\ form.
+% \item A command \cs{namealtnunit} is created that
+% expresses the constant and its units in \altnunits\ form.
% \item A command \cs{nameonlybaseunit} is created that expresses
% \textbf{only} the constant's units in \baseunits\ form.
% \item A command \cs{nameonlydrvdunit} is created that
% expresses \textbf{only} the constant's units in \drvdunits\ form.
-% \item A command \cs{nameonlytradunit} is created that
-% expresses \textbf{only} the constant's units in \tradunits\ form.
+% \item A command \cs{nameonlyaltnunit} is created that
+% expresses \textbf{only} the constant's units in \altnunits\ form.
% \end{itemize}
% None of these commands takes any arguments.
%
+%
+% There is a command similar to \refCom{redefinephysicsquantity} that allows for
+% redefining physical constants.
+%
+%\changes{v2.7.2}{2018/03/16}{Documented the \cs{redefinephysicsconstant} command.}
+%\iffalse
+%<*example>
+%\fi
+\begin{docCommand}{redefinephysicsconstant}
+{\marg{name}\marg{symbol}{\{\cs{mi at p\marg{approx}\marg{precise}}\}}\marg{\baseunits}
+\\
+\oarg{\drvdunits}\oarg{\altnunits}%
+}%
+Redefines an existing physical constant.
+The new definition takes effect immediately.
+\end{docCommand}
+%\iffalse
+%</example>
+%\fi
+%
% \newpage
% \subsubsection{Predefined Physical Constants}
%
@@ -4099,7 +4200,7 @@
\begin{mysolution*}
\msub{u}{\mu} &= \mivector{\ezero,\eone,\etwo,\ethree} \\
\msub{u}{\mu} &= \mivector[\quad]{\ezero,\eone,\etwo,\ethree} \\
- \vect{v} &= \mivector{1,3,5}[\velocityonlytradunit] \\
+ \vect{v} &= \mivector{1,3,5}[\velocityonlyaltnunit] \\
\vect{E} &= \mivector{\oofpezmathsymbol \frac{Q}{x^2},0,0} \\
\vect{E} &= \mivector[\quad]{\oofpezmathsymbol \frac{Q}{x^2},0,0}
\end{mysolution*}
@@ -4120,7 +4221,7 @@
\end{docCommand}
\begin{dispExample}
\magvectncomps{\velocity{3.12},\velocity{4.04},\velocity{6.73}} \\
-\magvectncomps{3.12,4.04,6.73}[\velocityonlytradunit] \\
+\magvectncomps{3.12,4.04,6.73}[\velocityonlyaltnunit] \\
\magvectncomps{\frac{1}{\sqrt{3}},\frac{1}{\sqrt{3}},\frac{1}{\sqrt{3}}}
\end{dispExample}
%\iffalse
@@ -6495,7 +6596,7 @@
this same idea in other sources. A blank argument generates a placeholder.
\end{docCommand}
\begin{dispExample*}{sidebyside}
-\unitsof{\vect{v}} = \velocityonlytradunit, \unitsof{}
+\unitsof{\vect{v}} = \velocityonlyaltnunit, \unitsof{}
\end{dispExample*}
%\iffalse
%</example>
@@ -6524,7 +6625,7 @@
Another command for scientific notation with an optional unit.
\end{docCommand}
\begin{dispExample*}{sidebyside}
-2.99\xtento{8}[\velocityonlytradunit] \\
+2.99\xtento{8}[\velocityonlyaltnunit] \\
2.99\timestento{-4}
\end{dispExample*}
%\iffalse
@@ -9449,7 +9550,7 @@
%\iffalse
%<*example>
%\fi
-\begin{docCommand}{image}{\oarg{scaleorsizes}\marg{imagefilename}\marg{caption}\marg{label}}
+\begin{docCommand}{image}{\oarg{scalesize}\marg{filename}\marg{caption}\marg{label}}
Centered figure displayed actual size with caption. The optional argument can be
a scale factor (with 1 being the original image size), explicit \texttt{width}
and/or \texttt{height} parameters, or even an \texttt{angle} for rotating the
@@ -9460,7 +9561,8 @@
\image{sampleimage.pdf}{An image shown actual size.}{img-label1}
\image[scale=1.5]{sampleimage.pdf}{An image scaled by 1.5 times.}{img-label2}
\image[height=1cm,width=2cm]{sampleimage.pdf}{An image resized.}{img-label3}
- \image[width=0.8\textwidth]{sampleimage.pdf}{An image 80 percent the text width.}{img-label4}
+ \image[width=0.8\textwidth]{sampleimage.pdf}{An image 80 percent the text width.}
+ {img-label4}
\image[angle=45]{sampleimage.pdf}{An image actual size, rotated.}{img-label5}
\end{dispListing}
%\iffalse
@@ -9606,6 +9708,7 @@
\newboolean{@optsinglemagbars}
\newboolean{@optbaseunits}
\newboolean{@optdrvdunits}
+\newboolean{@optaltnunits}
\newboolean{@optapproxconsts}
\newboolean{@optuseradians}
\setboolean{@optromanvectors}{false} % this is where you set the default option
@@ -9612,7 +9715,8 @@
\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}}
@@ -9627,9 +9731,9 @@
%
% \begin{macrocode}
\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{ }
@@ -9729,20 +9833,20 @@
\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=]{%
@@ -9759,11 +9863,11 @@
\mi at name#4{#5}#7{\unit{#8}{\selectunit{#3}{#1}{#2}}}%
\mi at name#4{#5baseunit}#7{\unit{#8}{#3}}%
\mi at name#4{#5drvdunit}#7{\unit{#8}{#1}}%
- \mi at name#4{#5tradunit}#7{\unit{#8}{#2}}%
+ \mi at name#4{#5altnunit}#7{\unit{#8}{#2}}%
\mi at name#4{#5onlyunit}{\selectunit{#3}{#1}{#2}}%
\mi at name#4{#5onlybaseunit}{\ensuremath{#3}}%
\mi at name#4{#5onlydrvdunit}{\ensuremath{#1}}%
- \mi at name#4{#5onlytradunit}{\ensuremath{#2}}%
+ \mi at name#4{#5onlyaltnunit}{\ensuremath{#2}}%
\mi at name#4{#5value}#7{\ensuremath{#8}}%
\mi at forkifnull{#7}{%
\ifx#4\renewcommand\mi at name\let{#5mathsymbol}=\relax\fi
@@ -9786,8 +9890,8 @@
{\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.}}
@@ -9797,7 +9901,8 @@
\typeout{ }
% \end{macrocode}
%
-% \noindent This is a utility command for picking constants.
+% \noindent This is a utility command for picking constants. Do not use this
+% command manually.
% \begin{macrocode}
\ifthenelse{\boolean{@optapproxconsts}}
{\newcommand*{\mi at p}[2]{#1}} % approximate value
@@ -9882,7 +9987,7 @@
\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}%
@@ -9994,16 +10099,16 @@
[]
\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]%
@@ -10018,18 +10123,18 @@
[\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]%
@@ -10038,12 +10143,12 @@
{%
\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]%
@@ -10075,16 +10180,16 @@
[\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]%
@@ -10091,8 +10196,8 @@
[\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]%
@@ -10099,12 +10204,12 @@
[\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]%
@@ -10131,12 +10236,12 @@
[\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}%
{}%
[]%
@@ -10171,16 +10276,16 @@
[\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]%
@@ -10191,8 +10296,8 @@
[\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]%
@@ -10199,8 +10304,8 @@
[(\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]%
@@ -10745,37 +10850,37 @@
{\ensuremath{\frac{1}{\phantom{_o}4\pi\epsilon_0}}}%
{\mi at 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 at 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 at 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}}%
@@ -10787,7 +10892,7 @@
{\ensuremath{\sigma}}%
{\mi at 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}}%
@@ -10853,8 +10958,8 @@
{\ensuremath{G}}%
{\mi at 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 at p{9.8}{9.807}}%
@@ -11995,9 +12100,9 @@
\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}
}%
@@ -12007,9 +12112,9 @@
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}
}%
Modified: trunk/Master/texmf-dist/tex/latex/mandi/mandi.sty
===================================================================
--- trunk/Master/texmf-dist/tex/latex/mandi/mandi.sty 2018-03-27 21:24:36 UTC (rev 47149)
+++ trunk/Master/texmf-dist/tex/latex/mandi/mandi.sty 2018-03-27 21:24:50 UTC (rev 47150)
@@ -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}
@@ -104,6 +104,7 @@
\newboolean{@optsinglemagbars}
\newboolean{@optbaseunits}
\newboolean{@optdrvdunits}
+\newboolean{@optaltnunits}
\newboolean{@optapproxconsts}
\newboolean{@optuseradians}
\setboolean{@optromanvectors}{false} % this is where you set the default option
@@ -110,7 +111,8 @@
\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 at name#4{#5}#7{\unit{#8}{\selectunit{#3}{#1}{#2}}}%
\mi at name#4{#5baseunit}#7{\unit{#8}{#3}}%
\mi at name#4{#5drvdunit}#7{\unit{#8}{#1}}%
- \mi at name#4{#5tradunit}#7{\unit{#8}{#2}}%
+ \mi at name#4{#5altnunit}#7{\unit{#8}{#2}}%
\mi at name#4{#5onlyunit}{\selectunit{#3}{#1}{#2}}%
\mi at name#4{#5onlybaseunit}{\ensuremath{#3}}%
\mi at name#4{#5onlydrvdunit}{\ensuremath{#1}}%
- \mi at name#4{#5onlytradunit}{\ensuremath{#2}}%
+ \mi at name#4{#5onlyaltnunit}{\ensuremath{#2}}%
\mi at name#4{#5value}#7{\ensuremath{#8}}%
\mi at forkifnull{#7}{%
\ifx#4\renewcommand\mi at 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]%
@@ -515,16 +517,16 @@
[\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]%
@@ -531,8 +533,8 @@
[\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]%
@@ -539,12 +541,12 @@
[\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]%
@@ -631,8 +633,8 @@
[\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]%
@@ -639,8 +641,8 @@
[(\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 at 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 at 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 at 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 at 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 at 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 at 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}
}%
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