diff options
| author | Karl Berry <karl@freefriends.org> | 2010-06-12 00:12:11 +0000 |
|---|---|---|
| committer | Karl Berry <karl@freefriends.org> | 2010-06-12 00:12:11 +0000 |
| commit | 452c9d0af12acb085390fe26cc37a9e93d689d5a (patch) | |
| tree | 2a28496b755aa54c3ca3a7c8de80510899f14dbb /Master/texmf-dist | |
| parent | 3ca859b7c25a23c6fa253978191197782df3d799 (diff) | |
pst-magneticfield 1.12 (11jun10)
git-svn-id: svn://tug.org/texlive/trunk@18901 c570f23f-e606-0410-a88d-b1316a301751
Diffstat (limited to 'Master/texmf-dist')
14 files changed, 1234 insertions, 598 deletions
diff --git a/Master/texmf-dist/doc/generic/pst-magneticfield/Changes b/Master/texmf-dist/doc/generic/pst-magneticfield/Changes index 2bf408e520e..ab18ab44275 100644 --- a/Master/texmf-dist/doc/generic/pst-magneticfield/Changes +++ b/Master/texmf-dist/doc/generic/pst-magneticfield/Changes @@ -3,6 +3,12 @@ pst-magneticfield.sty -------- pst-magneticfield.tex -------- +1.12 2010-06-07 - allow density plots + - move PS code into a pro file 1.11 2010-05-20 - change order for the different lines in the 3d view (dashed lines first) (hv) 1.10 2010-05-16 - first CTAN version + + +pst-magneticfield.pro -------- +0.01 2010-06-07 - initial pro file diff --git a/Master/texmf-dist/doc/generic/pst-magneticfield/README b/Master/texmf-dist/doc/generic/pst-magneticfield/README index a7776adf323..f23740077a2 100644 --- a/Master/texmf-dist/doc/generic/pst-magneticfield/README +++ b/Master/texmf-dist/doc/generic/pst-magneticfield/README @@ -1,3 +1,4 @@ +The files ---------------- Save the files pst-magneticfield.sty|tex in a directory, which is part of your local TeX tree. Then do not forget to run texhash to update this tree. @@ -6,3 +7,17 @@ on installing packages into your LATEX distribution or the TeX Frequently Asked Questions: (http://www.tex.ac.uk/cgi-bin/texfaq2html?label=instpackages). + +The documentation ------------------- +To get a smaller size of the generated pdf file run the +Makefile or by hand +"pst2pdf <file> --Iext=.png --Iscale=0.5 --DPI=150". This will +create eps/pdf/png images in a subdirectory images/ and then +using only the png ones for the last _pdflatex_ run. The +file size can be reduced to about 20% of the one created with +ps2pdf. The pdf file is saved as yfile>-pdf.pdf. + +When running the documentation in a traditional way, then +uncomment the line (in the preamble) + +%\newenvironment{postscript}{}{} % uncomment, when running with latex diff --git a/Master/texmf-dist/doc/generic/pst-magneticfield/pst-magneticfield-docDE.bib b/Master/texmf-dist/doc/generic/pst-magneticfield/pst-magneticfield-doc.bib index b96d8703ff5..b96d8703ff5 100644 --- a/Master/texmf-dist/doc/generic/pst-magneticfield/pst-magneticfield-docDE.bib +++ b/Master/texmf-dist/doc/generic/pst-magneticfield/pst-magneticfield-doc.bib diff --git a/Master/texmf-dist/doc/generic/pst-magneticfield/pst-magneticfield-docDE.pdf b/Master/texmf-dist/doc/generic/pst-magneticfield/pst-magneticfield-docDE.pdf Binary files differindex ffd5e4ffefd..4fef5b85367 100644 --- a/Master/texmf-dist/doc/generic/pst-magneticfield/pst-magneticfield-docDE.pdf +++ b/Master/texmf-dist/doc/generic/pst-magneticfield/pst-magneticfield-docDE.pdf diff --git a/Master/texmf-dist/doc/generic/pst-magneticfield/pst-magneticfield-docDE.tex b/Master/texmf-dist/doc/generic/pst-magneticfield/pst-magneticfield-docDE.tex index 3f5c6492df4..441d705c0a5 100644 --- a/Master/texmf-dist/doc/generic/pst-magneticfield/pst-magneticfield-docDE.tex +++ b/Master/texmf-dist/doc/generic/pst-magneticfield/pst-magneticfield-docDE.tex @@ -1,19 +1,16 @@ -%% $Id: pst-magneticfield-docEN.tex 322 2010-05-16 08:07:26Z herbert $ +%% $Id: pst-magneticfield-docDE.tex 343 2010-06-10 15:08:37Z herbert $ \documentclass[11pt,english,BCOR10mm,DIV12,bibliography=totoc,parskip=false,smallheadings headexclude,footexclude,oneside]{pst-doc} \usepackage[latin1]{inputenc} \usepackage{pst-magneticfield} \let\pstMFfv\fileversion + +%\newenvironment{postscript}{}{} % uncomment, when running with latex + \lstset{pos=t,language=PSTricks, morekeywords={psmagneticfield,psmagneticfieldThreeD},basicstyle=\footnotesize\ttfamily} \newcommand\Cadre[1]{\psframebox[fillstyle=solid,fillcolor=black,linestyle=none,framesep=0]{#1}} -\def\bgImage{% -\psset{unit=0.5cm} -\begin{pspicture}(-7,-6)(7,6) -\psmagneticfieldThreeD[N=2,R=2,L=2,linecolor=blue](-7,-8)(7,8) -\ThreeDput{\rput(0,-7){\textbf{HELMHOLTZ-Spule}}} -\end{pspicture} -} +\def\bgImage{} % \begin{document} @@ -80,56 +77,115 @@ Der Befehl \Lcs{psmagneticfieldThreeD} erlaubt eine 3D-Ansicht der Spule und der \section{Einfluss der physikalischen Gr\"{o}{\ss}en auf das Erscheinungsbild der Feldlinien} \subsection{Die L\"{a}nge der Spule} -\begin{LTXexample}[pos=t] +\begin{center} +\begin{postscript} +\psset{unit=0.5cm} +\begin{pspicture*}[showgrid](-7,-8)(7,8) +\psmagneticfield[linecolor={[HTML]{006633}},N=3,R=2,nS=1](-7,-8)(7,8) +\psframe*[linecolor={[HTML]{99FF66}}](-7,-8)(7,-7) +\rput(0,-7.5){[\Cadre{\textcolor{white}{L=4}},N=3,R=2,nS=1]} +\end{pspicture*} +\begin{pspicture*}[showgrid](-7,-8)(7,8) +\psmagneticfield[linecolor={[HTML]{006633}},L=8,N=3,R=2,nS=1,PasB=0.0025,pointsB=5500](-7,-8)(7,8) +\psframe*[linecolor={[HTML]{99FF66}}](-7,-8)(7,-7) +\rput(0,-7.5){[\Cadre{\textcolor{white}{L=8}},N=3,R=2,nS=1]} +\end{pspicture*} +\end{postscript} +\end{center} + +\begin{lstlisting} \psset{unit=0.5cm} \begin{pspicture*}[showgrid](-7,-8)(7,8) -\psmagneticfield[linecolor={[HTML]{006633}},N=3,R=2,nS=1] +\psmagneticfield[linecolor={[HTML]{006633}},N=3,R=2,nS=1](-7,-8)(7,8) \psframe*[linecolor={[HTML]{99FF66}}](-7,-8)(7,-7) \rput(0,-7.5){[\Cadre{\textcolor{white}{L=4}},N=3,R=2,nS=1]} \end{pspicture*} \begin{pspicture*}[showgrid](-7,-8)(7,8) -\psmagneticfield[linecolor={[HTML]{006633}},L=8,N=3,R=2,nS=1,PasB=0.0025,pointsB=5500] +\psmagneticfield[linecolor={[HTML]{006633}},L=8,N=3,R=2,nS=1,PasB=0.0025,pointsB=5500](-7,-8)(7,8) \psframe*[linecolor={[HTML]{99FF66}}](-7,-8)(7,-7) \rput(0,-7.5){[\Cadre{\textcolor{white}{L=8}},N=3,R=2,nS=1]} \end{pspicture*} -\end{LTXexample} +\end{lstlisting} + \textbf{Anmerkung:} Um das Erscheinungsbild der zweiten Spule zu verbessern, mussten wir die Anzahl der Berechungspunkte erh\"{o}hen und die Schrittweite verkleinern, - \Cadre{\textcolor{white}{pointsB=5500,PasB=0.0025}}, was jedoch eine Erh\"{o}hung der Rechenzeit mit sich brachte. + \begin{postscript} +\Cadre{\textcolor{white}{pointsB=5500,PasB=0.0025}} +\end{postscript}, +was jedoch eine Erh\"{o}hung der Rechenzeit mit sich brachte. \clearpage \subsection{Die Anzahl der Windungen} -\begin{LTXexample}[pos=t] + + +\begin{center} +\begin{postscript} \psset{unit=0.5} \begin{pspicture*}[showgrid](-7,-8)(7,8) -\psmagneticfield[linecolor={[HTML]{006633}},N=1,R=2,nS=0] +\psmagneticfield[linecolor={[HTML]{006633}},N=1,R=2,nS=0](-7,-8)(7,8) \psframe*[linecolor={[HTML]{99FF66}}](-7,-8)(7,-7) \rput(0,-7.5){[\Cadre{\textcolor{white}{N=1}},R=2,nS=0]} \end{pspicture*} \begin{pspicture*}[showgrid](-7,-8)(7,8) -\psmagneticfield[linecolor={[HTML]{006633}},N=2,R=2,L=2,PasS=0.003,nS=2] +\psmagneticfield[linecolor={[HTML]{006633}},N=2,R=2,L=2,PasS=0.003,nS=2](-7,-8)(7,8) \psframe*[linecolor={[HTML]{99FF66}}](-7,7)(7,8) \rput(0,7.5){\Cadre{\textcolor{white}{Bobines de Helmholtz}}} \psframe*[linecolor={[HTML]{99FF66}}](-7,-8)(7,-7) \rput(0,-7.5){[\Cadre{\textcolor{white}{N=2}},R=2,L=2,PasS=0.003,nS=2]} \end{pspicture*} -\end{LTXexample} +\end{postscript} +\end{center} -\begin{LTXexample}[pos=t] +\begin{lstlisting} \psset{unit=0.5} \begin{pspicture*}[showgrid](-7,-8)(7,8) -\psmagneticfield[linecolor={[HTML]{006633}},N=4,R=2,numSpires=2 3] +\psmagneticfield[linecolor={[HTML]{006633}},N=1,R=2,nS=0](-7,-8)(7,8) +\psframe*[linecolor={[HTML]{99FF66}}](-7,-8)(7,-7) +\rput(0,-7.5){[\Cadre{\textcolor{white}{N=1}},R=2,nS=0]} +\end{pspicture*} +\begin{pspicture*}[showgrid](-7,-8)(7,8) +\psmagneticfield[linecolor={[HTML]{006633}},N=2,R=2,L=2,PasS=0.003,nS=2](-7,-8)(7,8) +\psframe*[linecolor={[HTML]{99FF66}}](-7,7)(7,8) +\rput(0,7.5){\Cadre{\textcolor{white}{Bobines de Helmholtz}}} +\psframe*[linecolor={[HTML]{99FF66}}](-7,-8)(7,-7) +\rput(0,-7.5){[\Cadre{\textcolor{white}{N=2}},R=2,L=2,PasS=0.003,nS=2]} +\end{pspicture*} +\end{lstlisting} + + +\begin{center} +\begin{postscript} +\psset{unit=0.5} +\begin{pspicture*}[showgrid](-7,-8)(7,8) +\psmagneticfield[linecolor={[HTML]{006633}},N=4,R=2,numSpires=2 3](-7,-8)(7,8) \psframe*[linecolor={[HTML]{99FF66}}](-7,-8)(7,-7) \rput(0,-7.5){[\Cadre{\textcolor{white}{N=4}},R=2,L=4]} \end{pspicture*} \begin{pspicture*}[showgrid](-7,-8)(7,8) -\psmagneticfield[linecolor={[HTML]{006633}},N=5,R=2,L=5,PasS=0.004,nS=2 3 4] +\psmagneticfield[linecolor={[HTML]{006633}},N=5,R=2,L=5,PasS=0.004,numSpires=2 3 4](-7,-8)(7,8) \psframe*[linecolor={[HTML]{99FF66}}](-7,-8)(7,-7) \rput(0,-7.5){[\Cadre{\textcolor{white}{N=5}},R=2,L=5]} \end{pspicture*} -\end{LTXexample} +\end{postscript} +\end{center} + +\begin{lstlisting} +\psset{unit=0.5} +\begin{pspicture*}[showgrid](-7,-8)(7,8) +\psmagneticfield[linecolor={[HTML]{006633}},N=4,R=2,numSpires=2 3](-7,-8)(7,8) +\psframe*[linecolor={[HTML]{99FF66}}](-7,-8)(7,-7) +\rput(0,-7.5){[\Cadre{\textcolor{white}{N=4}},R=2,L=4]} +\end{pspicture*} +\begin{pspicture*}[showgrid](-7,-8)(7,8) +\psmagneticfield[linecolor={[HTML]{006633}},N=5,R=2,L=5,PasS=0.004,numSpires=2 3 4](-7,-8)(7,8) +\psframe*[linecolor={[HTML]{99FF66}}](-7,-8)(7,-7) +\rput(0,-7.5){[\Cadre{\textcolor{white}{N=5}},R=2,L=5]} +\end{pspicture*} +\end{lstlisting} + + \clearpage \section{Optionen f\"{u}r die Linien} @@ -137,81 +193,156 @@ Der Befehl \Lcs{psmagneticfieldThreeD} erlaubt eine 3D-Ansicht der Spule und der Auf Grund der Symmetrie des Problems ist die gew\"{a}hlte Anzahl der Feldlinien \Lkeyword{nL} nur die H\"{a}lfte der tats\"{a}chlich gezeichneten Feldlinien. Hinzu kommt noch eine Feldlinie, die in Richtung der Symmetrieachse der Spule zeigt. Die Anzahl der Feldlinien um die Windungen herum \Lkeyword{nS} kommen auch noch hinzu, diese k\"{o}nnen jedoch mit \Lkeyword{numSpires} individuell ausgew\"{a}hlt werden. -\begin{LTXexample}[pos=t] + + +\begin{center} +\begin{postscript} +\psset{unit=0.5} +\begin{pspicture*}[showgrid](-7,-8)(7,8) +\psmagneticfield[linecolor={[HTML]{000099}},N=1,R=2](-7,-8)(7,8) +\psframe*[linecolor={[HTML]{3399FF}}](-7,-8)(7,-7) +\rput(0,-7.5){[\Cadre{\textcolor{white}{nL=8}},N=1,R=2]} +\end{pspicture*} +\begin{pspicture*}[showgrid](-7,-8)(7,8) +\psmagneticfield[linecolor={[HTML]{000099}},N=1,R=2,nL=12](-7,-8)(7,8) +\psframe*[linecolor={[HTML]{3399FF}}](-7,-8)(7,-7) +\rput(0,-7.5){[\Cadre{\textcolor{white}{nL=12}},N=1,R=2]} +\end{pspicture*} +\end{postscript} +\end{center} + +\begin{lstlisting} \psset{unit=0.5} \begin{pspicture*}[showgrid](-7,-8)(7,8) -\psmagneticfield[linecolor={[HTML]{000099}},N=1,R=2] +\psmagneticfield[linecolor={[HTML]{000099}},N=1,R=2](-7,-8)(7,8) \psframe*[linecolor={[HTML]{3399FF}}](-7,-8)(7,-7) \rput(0,-7.5){[\Cadre{\textcolor{white}{nL=8}},N=1,R=2]} \end{pspicture*} \begin{pspicture*}[showgrid](-7,-8)(7,8) -\psmagneticfield[linecolor={[HTML]{000099}},N=1,R=2,nL=12] +\psmagneticfield[linecolor={[HTML]{000099}},N=1,R=2,nL=12](-7,-8)(7,8) \psframe*[linecolor={[HTML]{3399FF}}](-7,-8)(7,-7) \rput(0,-7.5){[\Cadre{\textcolor{white}{nL=12}},N=1,R=2]} \end{pspicture*} -\end{LTXexample} +\end{lstlisting} \clearpage \subsection{Die Anzahl der Berechnungspunkte und die Schrittweite} Die Feldlinien wurden mit einem numerischen Verfahren (Runge-Kutta 2) berechnet und dementsprechend h\"{a}ngt die Genauigkeit der Linien entscheidend ab von der Schrittweite und der Anzahl der Berechnungspunkte, wie in den folgenden zwei Beispielen gezeigt wird: -\begin{LTXexample}[pos=t] +\begin{center} +\begin{postscript} +\psset{unit=0.5} +\begin{pspicture*}[showgrid](-7,-8)(7,8) +\psmagneticfield[linecolor={[HTML]{660066}},N=2,R=2,L=2,PasB=0.1,nS=0,nL=7,pointsB=100](-7,-8)(7,8) +\psframe*[linecolor={[HTML]{996666}}](-7,7)(7,8) +\rput(0,7.5){\Cadre{\textcolor{white}{Bobines de Helmholtz}}} +\psframe*[linecolor={[HTML]{996666}}](-7,-8)(7,-7) +\rput(0,-7.5){[\Cadre{\textcolor{white}{PasB=0.1,nL=4,pointsB=100}}]} +\end{pspicture*} +\begin{pspicture*}[showgrid](-7,-8)(7,8) +\psmagneticfield[linecolor={[HTML]{660066}},N=2,R=2,L=2,PasB=0.4,nS=0,nL=7,pointsB=100](-7,-8)(7,8) +\psframe*[linecolor={[HTML]{996666}}](-7,7)(7,8) +\rput(0,7.5){\Cadre{\textcolor{white}{Bobines de Helmholtz}}} +\psframe*[linecolor={[HTML]{996666}}](-7,-8)(7,-7) +\rput(0,-7.5){[\Cadre{\textcolor{white}{PasS=0.4,pointsB=100}}]} +\end{pspicture*} +\end{postscript} +\end{center} + +\begin{lstlisting} \psset{unit=0.5} \begin{pspicture*}[showgrid](-7,-8)(7,8) -\psmagneticfield[linecolor={[HTML]{660066}},N=2,R=2,L=2,PasB=0.1,nS=0,nL=7,pointsB=100] +\psmagneticfield[linecolor={[HTML]{660066}},N=2,R=2,L=2,PasB=0.1,nS=0,nL=7,pointsB=100](-7,-8)(7,8) \psframe*[linecolor={[HTML]{996666}}](-7,7)(7,8) \rput(0,7.5){\Cadre{\textcolor{white}{Bobines de Helmholtz}}} \psframe*[linecolor={[HTML]{996666}}](-7,-8)(7,-7) \rput(0,-7.5){[\Cadre{\textcolor{white}{PasB=0.1,nL=4,pointsB=100}}]} \end{pspicture*} \begin{pspicture*}[showgrid](-7,-8)(7,8) -\psmagneticfield[linecolor={[HTML]{660066}},N=2,R=2,L=2,PasB=0.4,nS=0,nL=7,pointsB=100] +\psmagneticfield[linecolor={[HTML]{660066}},N=2,R=2,L=2,PasB=0.4,nS=0,nL=7,pointsB=100](-7,-8)(7,8) \psframe*[linecolor={[HTML]{996666}}](-7,7)(7,8) \rput(0,7.5){\Cadre{\textcolor{white}{Bobines de Helmholtz}}} \psframe*[linecolor={[HTML]{996666}}](-7,-8)(7,-7) \rput(0,-7.5){[\Cadre{\textcolor{white}{PasS=0.4,pointsB=100}}]} \end{pspicture*} -\end{LTXexample} +\end{lstlisting} + Sollten die voreingestellten Werte f\"{u}r eine individuelle Gestaltung nicht passen, dann muss man mit den Werten \Lkeyword{pasB}, \Lkeyword{pointsB} (bzw. \Lkeyword{pasS}, \Lkeyword{pointsS}) spielen, bis es passt. + + \clearpage \section{Der Parameter \nxLkeyword{numSpires}} -\begin{LTXexample}[pos=t,wide] +\begin{center} +\begin{postscript} +\psset{unit=0.5} +\begin{pspicture*}[showgrid](-8,-10)(8,10) +\psset{linecolor=blue} +\psmagneticfield[R=2,L=12,N=8,pointsS=500,nL=14,nS=1,numSpires=1 3 6 8,PasB=0.075](-8,-10)(8,10) +\psframe*[linecolor={[HTML]{99FF66}}](-8,-10)(8,-9) +\rput(0,-9.5){[\Cadre{\textcolor{white}{numSpires=1 3 6 8}},R=2,L=14]} +\multido{\i=0+1}{8}{\rput[l](!6 6 12 7 div \i\space mul sub){\the\multidocount}} +\end{pspicture*}\quad +\begin{pspicture*}[showgrid](0,-10)(16,10) +\psset{linecolor=blue} +\psmagneticfield[R=2,L=12,N=8,pointsS=500,nL=14,numSpires=,nS=1,PasB=0.075](0,-10)(16,10) +\psframe*[linecolor={[HTML]{99FF66}}](0,-10)(16,-9) +\rput(8,-9.5){[\Cadre{\textcolor{white}{numSpires=all}},R=2,L=14]} +\multido{\i=0+1}{8}{\rput[l](!6 6 12 7 div \i\space mul sub){\the\multidocount}} +\end{pspicture*} +\end{postscript} +\end{center} + + +\begin{lstlisting} \psset{unit=0.5} \begin{pspicture*}[showgrid](-8,-10)(8,10) \psset{linecolor=blue} -\psmagneticfield[R=2,L=12,N=8,pointsS=500,nL=14,nS=1,numSpires=1 3 6 8,PasB=0.075] +\psmagneticfield[R=2,L=12,N=8,pointsS=500,nL=14,nS=1,numSpires=1 3 6 8,PasB=0.075](-8,-10)(8,10) \psframe*[linecolor={[HTML]{99FF66}}](-8,-10)(8,-9) \rput(0,-9.5){[\Cadre{\textcolor{white}{numSpires=1 3 6 8}},R=2,L=14]} \multido{\i=0+1}{8}{\rput[l](!6 6 12 7 div \i\space mul sub){\the\multidocount}} \end{pspicture*}\quad \begin{pspicture*}[showgrid](0,-10)(16,10) \psset{linecolor=blue} -\psmagneticfield[R=2,L=12,N=8,pointsS=500,nL=14,numSpires=,nS=1,PasB=0.075] +\psmagneticfield[R=2,L=12,N=8,pointsS=500,nL=14,numSpires=,nS=1,PasB=0.075](0,-10)(16,10) \psframe*[linecolor={[HTML]{99FF66}}](0,-10)(16,-9) \rput(8,-9.5){[\Cadre{\textcolor{white}{numSpires=all}},R=2,L=14]} \multido{\i=0+1}{8}{\rput[l](!6 6 12 7 div \i\space mul sub){\the\multidocount}} \end{pspicture*} -\end{LTXexample} +\end{lstlisting} \clearpage \section{Der Parameter \nxLkeyword{AntiHelmholtz}} -\begin{LTXexample}[pos=t] +\begin{center} +\begin{postscript} \psset{unit=0.75,AntiHelmholtz,N=2, R=2,pointsB=500,pointsS=1000,PasB=0.02,PasS=0.00275,nS=10, nL=2,drawSelf=true,styleSpire=styleSpire,styleCourant=sensCourant} \newpsstyle{grille}{subgriddiv=0,gridcolor=blue!50,griddots=10} \newpsstyle{cadre}{linecolor=yellow!50} \begin{pspicture*}[showgrid](-7,-6)(7,6) -\psframe*[linecolor={[HTML]{996666}}](-7,7)(7,8) +\psframe*[linecolor={[HTML]{996666}}](-7,6)(7,6) \psmagneticfield[linecolor={[HTML]{660066}}] \end{pspicture*} -\end{LTXexample} +\end{postscript} +\end{center} +\begin{lstlisting} +\psset{unit=0.75,AntiHelmholtz,N=2, + R=2,pointsB=500,pointsS=1000,PasB=0.02,PasS=0.00275,nS=10, + nL=2,drawSelf=true,styleSpire=styleSpire,styleCourant=sensCourant} +\newpsstyle{grille}{subgriddiv=0,gridcolor=blue!50,griddots=10} +\newpsstyle{cadre}{linecolor=yellow!50} +\begin{pspicture*}[showgrid](-7,-6)(7,6) +\psframe*[linecolor={[HTML]{996666}}](-7,6)(7,6) +\psmagneticfield[linecolor={[HTML]{660066}}] +\end{pspicture*} +\end{lstlisting} \clearpage @@ -234,24 +365,48 @@ Koordinaten der linken unteren und rechten oberen Ecke des Gitternetzes festgele M\"{o}glichkeiten zur Gestaltung des Gitternetzes zeigen die folgenden zwei Beispiele: -\begin{LTXexample}[pos=t] + +\begin{center} +\begin{postscript} +\psset{unit=0.7cm} +\newpsstyle{grille}{subgriddiv=0,gridcolor=blue!50,griddots=10} +\newpsstyle{cadre}{linecolor=yellow!50} +\begin{pspicture}(-7,-6)(7,6) +\psmagneticfieldThreeD[N=8,R=2,L=8,pointsB=1200,linecolor=blue,pointsS=2000](-7,-6)(7,6) +\end{pspicture} +\end{postscript} +\end{center} + +\begin{lstlisting} \psset{unit=0.7cm} \newpsstyle{grille}{subgriddiv=0,gridcolor=blue!50,griddots=10} \newpsstyle{cadre}{linecolor=yellow!50} \begin{pspicture}(-7,-6)(7,6) -\psmagneticfieldThreeD[N=8,R=2,L=8,pointsB=1200,linecolor=blue,pointsS=1000](-7,-8)(7,8) +\psmagneticfieldThreeD[N=8,R=2,L=8,pointsB=1200,linecolor=blue,pointsS=2000](-7,-6)(7,6) \end{pspicture} -\end{LTXexample} +\end{lstlisting} -\begin{LTXexample}[pos=t] + +\begin{center} +\begin{postscript} +\psset{unit=0.7cm} +\begin{pspicture}(-7,-6)(7,6) +\psmagneticfieldThreeD[N=2,R=2,L=2,linecolor=blue](-7,-6)(7,6) +\ThreeDput{\rput(0,-7){\textbf{Bobines de HELMHOLTZ}}} +\end{pspicture} +\end{postscript} +\end{center} + +\begin{lstlisting} \psset{unit=0.7cm} \begin{pspicture}(-7,-6)(7,6) -\psmagneticfieldThreeD[N=2,R=2,L=2,linecolor=blue](-7,-8)(7,8) -\ThreeDput{\rput(0,-7){\textbf{HELMHOLTZ-Spule}}} +\psmagneticfieldThreeD[N=2,R=2,L=2,linecolor=blue](-7,-6)(7,6) +\ThreeDput{\rput(0,-7){\textbf{Bobines de HELMHOLTZ}}} \end{pspicture} -\end{LTXexample} +\end{lstlisting} -\begin{LTXexample}[pos=t] +\begin{center} +\begin{postscript} \psset{unit=0.75cm,AntiHelmholtz,N=2, R=2,pointsB=500,pointsS=1000,PasB=0.02,PasS=0.00275,nS=10, nL=2,drawSelf,styleSpire=styleSpire,styleCourant=sensCourant} @@ -260,7 +415,76 @@ M\"{o}glichkeiten zur Gestaltung des Gitternetzes zeigen die folgenden zwei Beis \begin{pspicture}(-7,-6)(7,6) \psmagneticfieldThreeD[linecolor={[HTML]{660066}}](-7,-6)(7,6) \end{pspicture} -\end{LTXexample} +\end{postscript} +\end{center} + +\begin{lstlisting} +\psset{unit=0.75cm,AntiHelmholtz,N=2, + R=2,pointsB=500,pointsS=1000,PasB=0.02,PasS=0.00275,nS=10, + nL=2,drawSelf,styleSpire=styleSpire,styleCourant=sensCourant} +\newpsstyle{grille}{subgriddiv=0,gridcolor=blue!50,griddots=10} +\newpsstyle{cadre}{linecolor=yellow!50} +\begin{pspicture}(-7,-6)(7,6) +\psmagneticfieldThreeD[linecolor={[HTML]{660066}}](-7,-6)(7,6) +\end{pspicture} +\end{lstlisting} + +\clearpage + + +\section{Feldstärkendichte} + +\begin{center} +\begin{postscript} +\begin{pspicture}(-6,-4)(6,4) +\psmagneticfield[N=3,R=2,L=2,StreamDensityPlot](-6,-4)(6,4) +\end{pspicture} +\end{postscript} +\end{center} + +\begin{lstlisting} +\begin{pspicture}(-6,-4)(6,4) +\psmagneticfield[N=3,R=2,L=2,StreamDensityPlot](-6,-4)(6,4) +\end{pspicture} +\end{lstlisting} + +\begin{center} +\begin{postscript} +\psset{unit=0.75} +\begin{pspicture}(-6,-5)(6,5) +\psmagneticfield[N=2,R=2,L=1,StreamDensityPlot,setgray](-6,-5)(6,5) +\end{pspicture} +\end{postscript} +\end{center} + +\begin{lstlisting} +\psset{unit=0.75} +\begin{pspicture}(-6,-5)(6,5) +\psmagneticfield[N=2,R=2,L=1,StreamDensityPlot,setgray](-6,-5)(6,5) +\end{pspicture} +\end{lstlisting} + + +\begin{center} +\begin{postscript} +\psset{unit=0.75,AntiHelmholtz, + R=2,pointsB=500,pointsS=2000,PasB=0.02,PasS=0.00275,nS=10, + nL=2,drawSelf=true,styleSpire=styleSpire,styleCourant=sensCourant} +\begin{pspicture*}(-7,-6)(7,6) +\psmagneticfield[linecolor={[HTML]{660066}},StreamDensityPlot](-7,-6)(7,6) +\end{pspicture*} +\end{postscript} +\end{center} + + +\begin{lstlisting} +\psset{unit=0.75,AntiHelmholtz, + R=2,pointsB=500,pointsS=2000,PasB=0.02,PasS=0.00275,nS=10, + nL=2,drawSelf=true,styleSpire=styleSpire,styleCourant=sensCourant} +\begin{pspicture*}(-7,-6)(7,6) +\psmagneticfield[linecolor={[HTML]{660066}},StreamDensityPlot](-7,-6)(7,6) +\end{pspicture*} +\end{lstlisting} \clearpage @@ -272,7 +496,7 @@ M\"{o}glichkeiten zur Gestaltung des Gitternetzes zeigen die folgenden zwei Beis \bgroup \raggedright \bibliographystyle{plain} -\bibliography{\jobname} +\bibliography{pst-magneticfield-doc} \egroup \printindex diff --git a/Master/texmf-dist/doc/generic/pst-magneticfield/pst-magneticfield-docEN.bib b/Master/texmf-dist/doc/generic/pst-magneticfield/pst-magneticfield-docEN.bib deleted file mode 100644 index b96d8703ff5..00000000000 --- a/Master/texmf-dist/doc/generic/pst-magneticfield/pst-magneticfield-docEN.bib +++ /dev/null @@ -1,79 +0,0 @@ -%% -*-bibtex-*- -@STRING{tugboat = {TUGboat} } -@STRING{dtk = {{D}ie {\TeX}nische {K}om{\"o}die} } - -@Book{companion, - author = {Michel Goosens and Frank Mittelbach and Sebastian Rahtz and Dennis Roegel and Herbert Vo\ss}, - title = {The {\LaTeX} {G}raphics {C}ompanion}, - publisher = {{Addison-Wesley Publishing Company}}, - edition = {second}, - year = {2007}, - address = {Reading, Mass.} -} - -@Article{girou:01:, - author = {Denis Girou}, - title = {Pr\'esentation de {PST}ricks}, - journal = {Cahier {GUT}enberg}, - year = 1994, - volume = {16}, - month = apr, - pages = {21-70} -} - -@Article{girou:02:, - author = {{Timothy Van} Zandt and Denis Girou}, - title = {Inside {PST}ricks}, - journal = TUGboat, - year = 1994, - volume = {15}, - month = sep, - pages = {239-246} -} - -@Book{PostScript, - Author = {Kollock, Nikolai G.}, - Title = {Post{S}cript richtig eingesetzt: vom {K}onzept zum - praktischen {E}insatz}, - Publisher = {IWT}, - Address = {Vaterstetten}, - year = 1989, -} - -@Manual{multido, - Title = {\texttt{multido.tex} - a loop macro, that supports fixed-point addition}, - Author = {{Timothy Van} Zandt}, - Organization = {}, - Address = {\url{CTAN:/graphics/pstricks/generic/multido.tex}}, - Note = {}, - year = 1997 -} - -@Book{PSTricks2, - author = {Herbert Vo\ss{}}, - title = {\texttt{PSTricks} -- {G}rafik f\"ur \TeX{} und \LaTeX}, - edition = {fifth}, - publisher = {DANTE -- Lehmanns}, - year = {2008}, - address = {Heidelberg/Hamburg} -} - -@Book{abramowitz, - author = {M. Abramowitz and I. A. Stegun }, - year = 1964, - title = {Handbook of {M}athematical {F}unctions with {F}ormulas, {G}raphs, and - {M}athematical {T}ables}, - publisher = {National Bureau of Standards Applied Mathematics Series, - U.S. Government Printing Office}, - address = {Washington, D.C., USA}, - Note = {Corrections appeared in later printings up to the 10th Printing}, -} - -@Book{dolan, -author = {Thomas~J. Dolan}, -title = {Fusion {R}esearch, {V}olume {III} ``{T}echnology''}, -publisher= {Pergamon Press}, -year=1982, -Note= {Chapter 20 ``Water-cooled magnets'' , - pages 600 ff ``circular loops'' -- Integrating the Biot-Savart Law (in cylindrical geometry)}, -} diff --git a/Master/texmf-dist/doc/generic/pst-magneticfield/pst-magneticfield-docEN.pdf b/Master/texmf-dist/doc/generic/pst-magneticfield/pst-magneticfield-docEN.pdf Binary files differindex 5cb39a83b04..fa7089315ae 100644 --- a/Master/texmf-dist/doc/generic/pst-magneticfield/pst-magneticfield-docEN.pdf +++ b/Master/texmf-dist/doc/generic/pst-magneticfield/pst-magneticfield-docEN.pdf diff --git a/Master/texmf-dist/doc/generic/pst-magneticfield/pst-magneticfield-docEN.tex b/Master/texmf-dist/doc/generic/pst-magneticfield/pst-magneticfield-docEN.tex index 9425f93f6c5..6755a7eaa97 100644 --- a/Master/texmf-dist/doc/generic/pst-magneticfield/pst-magneticfield-docEN.tex +++ b/Master/texmf-dist/doc/generic/pst-magneticfield/pst-magneticfield-docEN.tex @@ -1,4 +1,4 @@ -%% $Id: pst-magneticfield-docEN.tex 323 2010-05-16 11:39:35Z herbert $ +%% $Id: pst-magneticfield-docEN.tex 343 2010-06-10 15:08:37Z herbert $ \documentclass[11pt,english,BCOR10mm,DIV12,bibliography=totoc,parskip=false,smallheadings headexclude,footexclude,oneside]{pst-doc} \usepackage[latin1]{inputenc} @@ -6,21 +6,17 @@ \let\pstMFfv\fileversion \lstset{pos=t,language=PSTricks, morekeywords={psmagneticfield,psmagneticfieldThreeD},basicstyle=\footnotesize\ttfamily} + +%\newenvironment{postscript}{}{} % uncomment, when running with latex + \newcommand\Cadre[1]{\psframebox[fillstyle=solid,fillcolor=black,linestyle=none,framesep=0]{#1}} -\def\bgImage{% -\psset{unit=0.5cm} -\begin{pspicture}(-7,-6)(7,6) -\psmagneticfieldThreeD[N=2,R=2,L=2,linecolor=blue](-7,-8)(7,8) -\ThreeDput{\rput(0,-7){\textbf{Bobines de HELMHOLTZ}}} -\end{pspicture} -} +\def\bgImage{} % \begin{document} \title{\texttt{pst-magneticfield}} \subtitle{Magnetic field lines of a solenoid; v.\pstMFfv} \author{Juergen Gilg\\ Manuel Luque\\Herbert Vo\ss} -%\docauthor{Juergen Gilg\\Manuel Luque\\Herbert Vo\ss} \date{\today} \maketitle @@ -83,26 +79,54 @@ The route options, with the default values are as follows: A command \Lcs{psmagneticfieldThreeD} allows 3D visualization of the solenoid and field lines. +\begin{BDef} +\Lcs{psmagneticfield}\OptArgs\OptArg*{\coord1}\OptArg*{\coord2}\\ +\Lcs{psmagneticfieldThreeD}\OptArgs\OptArg*{\coord1}\OptArg*{\coord2} +\end{BDef} + +Missing coordinates are substituted to \verb+(-6,-5)(6,5)+! \clearpage \section{Influence of physical parameters on the map magnetic field} + \subsection{The length of the solenoid} -\begin{LTXexample}[pos=t] +\begin{center} +\begin{postscript} \psset{unit=0.5cm} \begin{pspicture*}[showgrid](-7,-8)(7,8) -\psmagneticfield[linecolor={[HTML]{006633}},N=3,R=2,nS=1] +\psmagneticfield[linecolor={[HTML]{006633}},N=3,R=2,nS=1](-7,-8)(7,8) \psframe*[linecolor={[HTML]{99FF66}}](-7,-8)(7,-7) \rput(0,-7.5){[\Cadre{\textcolor{white}{L=4}},N=3,R=2,nS=1]} \end{pspicture*} \begin{pspicture*}[showgrid](-7,-8)(7,8) -\psmagneticfield[linecolor={[HTML]{006633}},L=8,N=3,R=2,nS=1,PasB=0.0025,pointsB=5500] +\psmagneticfield[linecolor={[HTML]{006633}},L=8,N=3,R=2,nS=1,PasB=0.0025,pointsB=5500](-7,-8)(7,8) \psframe*[linecolor={[HTML]{99FF66}}](-7,-8)(7,-7) \rput(0,-7.5){[\Cadre{\textcolor{white}{L=8}},N=3,R=2,nS=1]} \end{pspicture*} -\end{LTXexample} +\end{postscript} +\end{center} + +\begin{lstlisting} +\psset{unit=0.5cm} +\begin{pspicture*}[showgrid](-7,-8)(7,8) +\psmagneticfield[linecolor={[HTML]{006633}},N=3,R=2,nS=1](-7,-8)(7,8) +\psframe*[linecolor={[HTML]{99FF66}}](-7,-8)(7,-7) +\rput(0,-7.5){[\Cadre{\textcolor{white}{L=4}},N=3,R=2,nS=1]} +\end{pspicture*} +\begin{pspicture*}[showgrid](-7,-8)(7,8) +\psmagneticfield[linecolor={[HTML]{006633}},L=8,N=3,R=2,nS=1,PasB=0.0025,pointsB=5500](-7,-8)(7,8) +\psframe*[linecolor={[HTML]{99FF66}}](-7,-8)(7,-7) +\rput(0,-7.5){[\Cadre{\textcolor{white}{L=8}},N=3,R=2,nS=1]} +\end{pspicture*} +\end{lstlisting} + + \textbf{Note:} To refine the layout of the second solenoid, we had to increase the -points and lower the pitch of the route: \Cadre{\textcolor{white}{pointsB=5500,PasB=0.0025}}, which +points and lower the pitch of the route: +\begin{postscript} +\Cadre{\textcolor{white}{pointsB=5500,PasB=0.0025}} +\end{postscript}, which takes more time for the calculations. @@ -110,35 +134,70 @@ takes more time for the calculations. \clearpage \subsection{The number of turns} -\begin{LTXexample}[pos=t] +\begin{center} +\begin{postscript} \psset{unit=0.5} \begin{pspicture*}[showgrid](-7,-8)(7,8) -\psmagneticfield[linecolor={[HTML]{006633}},N=1,R=2,nS=0] +\psmagneticfield[linecolor={[HTML]{006633}},N=1,R=2,nS=0](-7,-8)(7,8) \psframe*[linecolor={[HTML]{99FF66}}](-7,-8)(7,-7) \rput(0,-7.5){[\Cadre{\textcolor{white}{N=1}},R=2,nS=0]} \end{pspicture*} \begin{pspicture*}[showgrid](-7,-8)(7,8) -\psmagneticfield[linecolor={[HTML]{006633}},N=2,R=2,L=2,PasS=0.003,nS=2] +\psmagneticfield[linecolor={[HTML]{006633}},N=2,R=2,L=2,PasS=0.003,nS=2](-7,-8)(7,8) \psframe*[linecolor={[HTML]{99FF66}}](-7,7)(7,8) \rput(0,7.5){\Cadre{\textcolor{white}{Bobines de Helmholtz}}} \psframe*[linecolor={[HTML]{99FF66}}](-7,-8)(7,-7) \rput(0,-7.5){[\Cadre{\textcolor{white}{N=2}},R=2,L=2,PasS=0.003,nS=2]} \end{pspicture*} -\end{LTXexample} +\end{postscript} +\end{center} -\begin{LTXexample}[pos=t] +\begin{lstlisting} \psset{unit=0.5} \begin{pspicture*}[showgrid](-7,-8)(7,8) -\psmagneticfield[linecolor={[HTML]{006633}},N=4,R=2,numSpires=2 3] +\psmagneticfield[linecolor={[HTML]{006633}},N=1,R=2,nS=0](-7,-8)(7,8) +\psframe*[linecolor={[HTML]{99FF66}}](-7,-8)(7,-7) +\rput(0,-7.5){[\Cadre{\textcolor{white}{N=1}},R=2,nS=0]} +\end{pspicture*} +\begin{pspicture*}[showgrid](-7,-8)(7,8) +\psmagneticfield[linecolor={[HTML]{006633}},N=2,R=2,L=2,PasS=0.003,nS=2](-7,-8)(7,8) +\psframe*[linecolor={[HTML]{99FF66}}](-7,7)(7,8) +\rput(0,7.5){\Cadre{\textcolor{white}{Bobines de Helmholtz}}} +\psframe*[linecolor={[HTML]{99FF66}}](-7,-8)(7,-7) +\rput(0,-7.5){[\Cadre{\textcolor{white}{N=2}},R=2,L=2,PasS=0.003,nS=2]} +\end{pspicture*} +\end{lstlisting} + + +\begin{center} +\begin{postscript} +\psset{unit=0.5} +\begin{pspicture*}[showgrid](-7,-8)(7,8) +\psmagneticfield[linecolor={[HTML]{006633}},N=4,R=2,numSpires=2 3](-7,-8)(7,8) +\psframe*[linecolor={[HTML]{99FF66}}](-7,-8)(7,-7) +\rput(0,-7.5){[\Cadre{\textcolor{white}{N=4}},R=2,L=4]} +\end{pspicture*} +\begin{pspicture*}[showgrid](-7,-8)(7,8) +\psmagneticfield[linecolor={[HTML]{006633}},N=5,R=2,L=5,PasS=0.004,numSpires=2 3 4](-7,-8)(7,8) +\psframe*[linecolor={[HTML]{99FF66}}](-7,-8)(7,-7) +\rput(0,-7.5){[\Cadre{\textcolor{white}{N=5}},R=2,L=5]} +\end{pspicture*} +\end{postscript} +\end{center} + +\begin{lstlisting} +\psset{unit=0.5} +\begin{pspicture*}[showgrid](-7,-8)(7,8) +\psmagneticfield[linecolor={[HTML]{006633}},N=4,R=2,numSpires=2 3](-7,-8)(7,8) \psframe*[linecolor={[HTML]{99FF66}}](-7,-8)(7,-7) \rput(0,-7.5){[\Cadre{\textcolor{white}{N=4}},R=2,L=4]} \end{pspicture*} \begin{pspicture*}[showgrid](-7,-8)(7,8) -\psmagneticfield[linecolor={[HTML]{006633}},N=5,R=2,L=5,PasS=0.004,numSpires=2 3 4] +\psmagneticfield[linecolor={[HTML]{006633}},N=5,R=2,L=5,PasS=0.004,numSpires=2 3 4](-7,-8)(7,8) \psframe*[linecolor={[HTML]{99FF66}}](-7,-8)(7,-7) \rput(0,-7.5){[\Cadre{\textcolor{white}{N=5}},R=2,L=5]} \end{pspicture*} -\end{LTXexample} +\end{lstlisting} \clearpage @@ -152,19 +211,35 @@ these turns can be selected individually \Lkeyword{numSpires}. -\begin{LTXexample}[pos=t] +\begin{center} +\begin{postscript} +\psset{unit=0.5} +\begin{pspicture*}[showgrid](-7,-8)(7,8) +\psmagneticfield[linecolor={[HTML]{000099}},N=1,R=2](-7,-8)(7,8) +\psframe*[linecolor={[HTML]{3399FF}}](-7,-8)(7,-7) +\rput(0,-7.5){[\Cadre{\textcolor{white}{nL=8}},N=1,R=2]} +\end{pspicture*} +\begin{pspicture*}[showgrid](-7,-8)(7,8) +\psmagneticfield[linecolor={[HTML]{000099}},N=1,R=2,nL=12](-7,-8)(7,8) +\psframe*[linecolor={[HTML]{3399FF}}](-7,-8)(7,-7) +\rput(0,-7.5){[\Cadre{\textcolor{white}{nL=12}},N=1,R=2]} +\end{pspicture*} +\end{postscript} +\end{center} + +\begin{lstlisting} \psset{unit=0.5} \begin{pspicture*}[showgrid](-7,-8)(7,8) -\psmagneticfield[linecolor={[HTML]{000099}},N=1,R=2] +\psmagneticfield[linecolor={[HTML]{000099}},N=1,R=2](-7,-8)(7,8) \psframe*[linecolor={[HTML]{3399FF}}](-7,-8)(7,-7) \rput(0,-7.5){[\Cadre{\textcolor{white}{nL=8}},N=1,R=2]} \end{pspicture*} \begin{pspicture*}[showgrid](-7,-8)(7,8) -\psmagneticfield[linecolor={[HTML]{000099}},N=1,R=2,nL=12] +\psmagneticfield[linecolor={[HTML]{000099}},N=1,R=2,nL=12](-7,-8)(7,8) \psframe*[linecolor={[HTML]{3399FF}}](-7,-8)(7,-7) \rput(0,-7.5){[\Cadre{\textcolor{white}{nL=12}},N=1,R=2]} \end{pspicture*} -\end{LTXexample} +\end{lstlisting} \clearpage \subsection{The number of points for the path} @@ -173,23 +248,43 @@ follows the step of the route and the number of selected points affect the accur as in the two examples below: -\begin{LTXexample}[pos=t] +\begin{center} +\begin{postscript} \psset{unit=0.5} \begin{pspicture*}[showgrid](-7,-8)(7,8) -\psmagneticfield[linecolor={[HTML]{660066}},N=2,R=2,L=2,PasB=0.1,nS=0,nL=7,pointsB=100] +\psmagneticfield[linecolor={[HTML]{660066}},N=2,R=2,L=2,PasB=0.1,nS=0,nL=7,pointsB=100](-7,-8)(7,8) \psframe*[linecolor={[HTML]{996666}}](-7,7)(7,8) \rput(0,7.5){\Cadre{\textcolor{white}{Bobines de Helmholtz}}} \psframe*[linecolor={[HTML]{996666}}](-7,-8)(7,-7) \rput(0,-7.5){[\Cadre{\textcolor{white}{PasB=0.1,nL=4,pointsB=100}}]} \end{pspicture*} \begin{pspicture*}[showgrid](-7,-8)(7,8) -\psmagneticfield[linecolor={[HTML]{660066}},N=2,R=2,L=2,PasB=0.4,nS=0,nL=7,pointsB=100] +\psmagneticfield[linecolor={[HTML]{660066}},N=2,R=2,L=2,PasB=0.4,nS=0,nL=7,pointsB=100](-7,-8)(7,8) \psframe*[linecolor={[HTML]{996666}}](-7,7)(7,8) \rput(0,7.5){\Cadre{\textcolor{white}{Bobines de Helmholtz}}} \psframe*[linecolor={[HTML]{996666}}](-7,-8)(7,-7) \rput(0,-7.5){[\Cadre{\textcolor{white}{PasS=0.4,pointsB=100}}]} \end{pspicture*} -\end{LTXexample} +\end{postscript} +\end{center} + +\begin{lstlisting} +\psset{unit=0.5} +\begin{pspicture*}[showgrid](-7,-8)(7,8) +\psmagneticfield[linecolor={[HTML]{660066}},N=2,R=2,L=2,PasB=0.1,nS=0,nL=7,pointsB=100](-7,-8)(7,8) +\psframe*[linecolor={[HTML]{996666}}](-7,7)(7,8) +\rput(0,7.5){\Cadre{\textcolor{white}{Bobines de Helmholtz}}} +\psframe*[linecolor={[HTML]{996666}}](-7,-8)(7,-7) +\rput(0,-7.5){[\Cadre{\textcolor{white}{PasB=0.1,nL=4,pointsB=100}}]} +\end{pspicture*} +\begin{pspicture*}[showgrid](-7,-8)(7,8) +\psmagneticfield[linecolor={[HTML]{660066}},N=2,R=2,L=2,PasB=0.4,nS=0,nL=7,pointsB=100](-7,-8)(7,8) +\psframe*[linecolor={[HTML]{996666}}](-7,7)(7,8) +\rput(0,7.5){\Cadre{\textcolor{white}{Bobines de Helmholtz}}} +\psframe*[linecolor={[HTML]{996666}}](-7,-8)(7,-7) +\rput(0,-7.5){[\Cadre{\textcolor{white}{PasS=0.4,pointsB=100}}]} +\end{pspicture*} +\end{lstlisting} If the defaults do not suit it must be found by testing the @@ -200,38 +295,72 @@ values that give a correct path. \clearpage \section{The parameter \nxLkeyword{numSpires}} -\begin{LTXexample}[pos=t,wide] +\begin{center} +\begin{postscript} +\psset{unit=0.5} +\begin{pspicture*}[showgrid](-8,-10)(8,10) +\psset{linecolor=blue} +\psmagneticfield[R=2,L=12,N=8,pointsS=500,nL=14,nS=1,numSpires=1 3 6 8,PasB=0.075](-8,-10)(8,10) +\psframe*[linecolor={[HTML]{99FF66}}](-8,-10)(8,-9) +\rput(0,-9.5){[\Cadre{\textcolor{white}{numSpires=1 3 6 8}},R=2,L=14]} +\multido{\i=0+1}{8}{\rput[l](!6 6 12 7 div \i\space mul sub){\the\multidocount}} +\end{pspicture*}\quad +\begin{pspicture*}[showgrid](0,-10)(16,10) +\psset{linecolor=blue} +\psmagneticfield[R=2,L=12,N=8,pointsS=500,nL=14,numSpires=,nS=1,PasB=0.075](0,-10)(16,10) +\psframe*[linecolor={[HTML]{99FF66}}](0,-10)(16,-9) +\rput(8,-9.5){[\Cadre{\textcolor{white}{numSpires=all}},R=2,L=14]} +\multido{\i=0+1}{8}{\rput[l](!6 6 12 7 div \i\space mul sub){\the\multidocount}} +\end{pspicture*} +\end{postscript} +\end{center} + + +\begin{lstlisting} \psset{unit=0.5} \begin{pspicture*}[showgrid](-8,-10)(8,10) \psset{linecolor=blue} -\psmagneticfield[R=2,L=12,N=8,pointsS=500,nL=14,nS=1,numSpires=1 3 6 8,PasB=0.075] +\psmagneticfield[R=2,L=12,N=8,pointsS=500,nL=14,nS=1,numSpires=1 3 6 8,PasB=0.075](-8,-10)(8,10) \psframe*[linecolor={[HTML]{99FF66}}](-8,-10)(8,-9) \rput(0,-9.5){[\Cadre{\textcolor{white}{numSpires=1 3 6 8}},R=2,L=14]} \multido{\i=0+1}{8}{\rput[l](!6 6 12 7 div \i\space mul sub){\the\multidocount}} \end{pspicture*}\quad \begin{pspicture*}[showgrid](0,-10)(16,10) \psset{linecolor=blue} -\psmagneticfield[R=2,L=12,N=8,pointsS=500,nL=14,numSpires=,nS=1,PasB=0.075] +\psmagneticfield[R=2,L=12,N=8,pointsS=500,nL=14,numSpires=,nS=1,PasB=0.075](0,-10)(16,10) \psframe*[linecolor={[HTML]{99FF66}}](0,-10)(16,-9) \rput(8,-9.5){[\Cadre{\textcolor{white}{numSpires=all}},R=2,L=14]} \multido{\i=0+1}{8}{\rput[l](!6 6 12 7 div \i\space mul sub){\the\multidocount}} \end{pspicture*} -\end{LTXexample} +\end{lstlisting} \clearpage \section{The parameter \nxLkeyword{AntiHelmholtz}} -\begin{LTXexample}[pos=t] +\begin{center} +\begin{postscript} \psset{unit=0.75,AntiHelmholtz,N=2, R=2,pointsB=500,pointsS=1000,PasB=0.02,PasS=0.00275,nS=10, nL=2,drawSelf=true,styleSpire=styleSpire,styleCourant=sensCourant} \newpsstyle{grille}{subgriddiv=0,gridcolor=blue!50,griddots=10} \newpsstyle{cadre}{linecolor=yellow!50} \begin{pspicture*}[showgrid](-7,-6)(7,6) -\psframe*[linecolor={[HTML]{996666}}](-7,7)(7,8) +\psframe*[linecolor={[HTML]{996666}}](-7,6)(7,6) \psmagneticfield[linecolor={[HTML]{660066}}] \end{pspicture*} -\end{LTXexample} +\end{postscript} +\end{center} +\begin{lstlisting} +\psset{unit=0.75,AntiHelmholtz,N=2, + R=2,pointsB=500,pointsS=1000,PasB=0.02,PasS=0.00275,nS=10, + nL=2,drawSelf=true,styleSpire=styleSpire,styleCourant=sensCourant} +\newpsstyle{grille}{subgriddiv=0,gridcolor=blue!50,griddots=10} +\newpsstyle{cadre}{linecolor=yellow!50} +\begin{pspicture*}[showgrid](-7,-6)(7,6) +\psframe*[linecolor={[HTML]{996666}}](-7,6)(7,6) +\psmagneticfield[linecolor={[HTML]{660066}}] +\end{pspicture*} +\end{lstlisting} \clearpage @@ -255,24 +384,59 @@ is encapsulated as the field map for \Lcs{psframe}. We can use the option In the following example we can see the handling of these two psstyles. -\begin{LTXexample}[pos=t] +\begin{center} +\begin{postscript} +\psset{unit=0.7cm} +\newpsstyle{grille}{subgriddiv=0,gridcolor=blue!50,griddots=10} +\newpsstyle{cadre}{linecolor=yellow!50} +\begin{pspicture}(-7,-6)(7,6) +\psmagneticfieldThreeD[N=8,R=2,L=8,pointsB=1200,linecolor=blue,pointsS=2000](-7,-6)(7,6) +\end{pspicture} +\end{postscript} +\end{center} + +\begin{lstlisting} \psset{unit=0.7cm} \newpsstyle{grille}{subgriddiv=0,gridcolor=blue!50,griddots=10} \newpsstyle{cadre}{linecolor=yellow!50} \begin{pspicture}(-7,-6)(7,6) -\psmagneticfieldThreeD[N=8,R=2,L=8,pointsB=1200,linecolor=blue,pointsS=1000](-7,-8)(7,8) +\psmagneticfieldThreeD[N=8,R=2,L=8,pointsB=1200,linecolor=blue,pointsS=2000](-7,-6)(7,6) +\end{pspicture} +\end{lstlisting} + + +\begin{center} +\begin{postscript} +\psset{unit=0.7cm} +\begin{pspicture}(-7,-6)(7,6) +\psmagneticfieldThreeD[N=2,R=2,L=2,linecolor=blue](-7,-6)(7,6) +\ThreeDput{\rput(0,-7){\textbf{Bobines de HELMHOLTZ}}} \end{pspicture} -\end{LTXexample} +\end{postscript} +\end{center} -\begin{LTXexample}[pos=t] +\begin{lstlisting} \psset{unit=0.7cm} \begin{pspicture}(-7,-6)(7,6) -\psmagneticfieldThreeD[N=2,R=2,L=2,linecolor=blue](-7,-8)(7,8) +\psmagneticfieldThreeD[N=2,R=2,L=2,linecolor=blue](-7,-6)(7,6) \ThreeDput{\rput(0,-7){\textbf{Bobines de HELMHOLTZ}}} \end{pspicture} -\end{LTXexample} +\end{lstlisting} + +\begin{center} +\begin{postscript} +\psset{unit=0.75cm,AntiHelmholtz,N=2, + R=2,pointsB=500,pointsS=1000,PasB=0.02,PasS=0.00275,nS=10, + nL=2,drawSelf,styleSpire=styleSpire,styleCourant=sensCourant} +\newpsstyle{grille}{subgriddiv=0,gridcolor=blue!50,griddots=10} +\newpsstyle{cadre}{linecolor=yellow!50} +\begin{pspicture}(-7,-6)(7,6) +\psmagneticfieldThreeD[linecolor={[HTML]{660066}}](-7,-6)(7,6) +\end{pspicture} +\end{postscript} +\end{center} -\begin{LTXexample}[pos=t] +\begin{lstlisting} \psset{unit=0.75cm,AntiHelmholtz,N=2, R=2,pointsB=500,pointsS=1000,PasB=0.02,PasS=0.00275,nS=10, nL=2,drawSelf,styleSpire=styleSpire,styleCourant=sensCourant} @@ -281,9 +445,65 @@ In the following example we can see the handling of these two psstyles. \begin{pspicture}(-7,-6)(7,6) \psmagneticfieldThreeD[linecolor={[HTML]{660066}}](-7,-6)(7,6) \end{pspicture} -\end{LTXexample} +\end{lstlisting} + +\clearpage +\section{Density plots} +The optional argument \Lkeyword{StreamDensityPlot} allows to plot the +magnetic field as a colored stream density. A gray colored output is possioble +with setting the keyword \Lkeyword{setgray}. + +\begin{center} +\begin{postscript} +\begin{pspicture}(-6,-4)(6,4) +\psmagneticfield[N=3,R=2,L=2,StreamDensityPlot](-6,-4)(6,4) +\end{pspicture} +\end{postscript} +\end{center} + +\begin{lstlisting} +\begin{pspicture}(-6,-4)(6,4) +\psmagneticfield[N=3,R=2,L=2,StreamDensityPlot](-6,-4)(6,4) +\end{pspicture} +\end{lstlisting} + +\begin{center} +\begin{postscript} +\psset{unit=0.75} +\begin{pspicture}(-6,-5)(6,5) +\psmagneticfield[N=2,R=2,L=1,StreamDensityPlot,setgray](-6,-5)(6,5) +\end{pspicture} +\end{postscript} +\end{center} + +\begin{lstlisting} +\psset{unit=0.75} +\begin{pspicture}(-6,-5)(6,5) +\psmagneticfield[N=2,R=2,L=1,StreamDensityPlot,setgray](-6,-5)(6,5) +\end{pspicture} +\end{lstlisting} + + +\begin{center} +\begin{postscript} +\psset{unit=0.75,AntiHelmholtz, + R=2,pointsB=500,pointsS=2000,PasB=0.02,PasS=0.00275,nS=10, + nL=2,drawSelf=true,styleSpire=styleSpire,styleCourant=sensCourant} +\begin{pspicture*}(-7,-6)(7,6) +\psmagneticfield[linecolor={[HTML]{660066}},StreamDensityPlot](-7,-6)(7,6) +\end{pspicture*} +\end{postscript} +\end{center} +\begin{lstlisting} +\psset{unit=0.75,AntiHelmholtz, + R=2,pointsB=500,pointsS=2000,PasB=0.02,PasS=0.00275,nS=10, + nL=2,drawSelf=true,styleSpire=styleSpire,styleCourant=sensCourant} +\begin{pspicture*}(-7,-6)(7,6) +\psmagneticfield[linecolor={[HTML]{660066}},StreamDensityPlot](-7,-6)(7,6) +\end{pspicture*} +\end{lstlisting} \clearpage @@ -295,7 +515,7 @@ In the following example we can see the handling of these two psstyles. \bgroup \raggedright \bibliographystyle{plain} -\bibliography{\jobname} +\bibliography{pst-magneticfield-doc} \egroup diff --git a/Master/texmf-dist/doc/generic/pst-magneticfield/pst-magneticfield-docFR.bib b/Master/texmf-dist/doc/generic/pst-magneticfield/pst-magneticfield-docFR.bib deleted file mode 100644 index 14a8466e948..00000000000 --- a/Master/texmf-dist/doc/generic/pst-magneticfield/pst-magneticfield-docFR.bib +++ /dev/null @@ -1,79 +0,0 @@ -%% -*-bibtex-*- -@STRING{tugboat = {TUGboat} } -@STRING{dtk = {{D}ie {\TeX}nische {K}om{\"o}die} } - -@Book{companion, - author = {Michel Goosens and Frank Mittelbach and Sebastian Rahtz and Dennis Roegel and Herbert Vo\ss}, - title = {The {\LaTeX} {G}raphics {C}ompanion}, - publisher = {{Addison-Wesley Publishing Company}}, - edition = {second}, - year = {2007}, - address = {Reading, Mass.} -} - -@Article{girou:01:, - author = {Denis Girou}, - title = {Pr\'esentation de {PST}ricks}, - journal = {Cahier {GUT}enberg}, - year = 1994, - volume = {16}, - month = apr, - pages = {21-70} -} - -@Article{girou:02:, - author = {{Timothy Van} Zandt and Denis Girou}, - title = {Inside {PST}ricks}, - journal = TUGboat, - year = 1994, - volume = {15}, - month = sep, - pages = {239-246} -} - -@Book{PostScript, - Author = {Kollock, Nikolai G.}, - Title = {Post{S}cript richtig eingesetzt: vom {K}onzept zum - praktischen {E}insatz}, - Publisher = {IWT}, - Address = {Vaterstetten}, - year = 1989, -} - -@Manual{multido, - Title = {\texttt{multido.tex} - a loop macro, that supports fixed-point addition}, - Author = {{Timothy Van} Zandt}, - Organization = {}, - Address = {\url{CTAN:/graphics/pstricks/generic/multido.tex}}, - Note = {}, - year = 1997 -} - -@Book{PSTricks2, - author = {Herbert Vo\ss{}}, - title = {\texttt{PSTricks} -- {G}rafik f\"ur \TeX{} und \LaTeX}, - edition = {fifth}, - publisher = {DANTE -- Lehmanns}, - year = {2008}, - address = {Heidelberg/Hamburg} -} - -@Book{abramowitz, - author = {M. Abramowitz and I. A. Stegun }, - year = 1964, - title = {Handbook of {M}athematical {F}unctions with {F}ormulas, {G}raphs, and - {M}athematical {T}ables}, - publisher = {National Bureau of Standards Applied Mathematics Series, - U.S. Government Printing Office}, - address = {Washington, D.C., USA}, - Note = {Corrections appeared in later printings up to the 10th Printing}, -} - -@Book{dolan, -author = {Thomas~J. ,Dolan}, -title = {Fusion {R}esearch, {V}olume {III} ``{T}echnology''}, -publisher= {Pergamon Press}, -year=1982, -Note= {Chapter 20 ``Water-cooled magnets'' , - pages 600 ff ``circular loops'' -- Integrating the Biot-Savart Law (in cylindrical geometry)}, -} diff --git a/Master/texmf-dist/doc/generic/pst-magneticfield/pst-magneticfield-docFR.pdf b/Master/texmf-dist/doc/generic/pst-magneticfield/pst-magneticfield-docFR.pdf Binary files differindex 3eff5d5d839..4e5dd583c65 100644 --- a/Master/texmf-dist/doc/generic/pst-magneticfield/pst-magneticfield-docFR.pdf +++ b/Master/texmf-dist/doc/generic/pst-magneticfield/pst-magneticfield-docFR.pdf diff --git a/Master/texmf-dist/doc/generic/pst-magneticfield/pst-magneticfield-docFR.tex b/Master/texmf-dist/doc/generic/pst-magneticfield/pst-magneticfield-docFR.tex index 6a13361b7f4..6b0e5a2b96a 100644 --- a/Master/texmf-dist/doc/generic/pst-magneticfield/pst-magneticfield-docFR.tex +++ b/Master/texmf-dist/doc/generic/pst-magneticfield/pst-magneticfield-docFR.tex @@ -1,19 +1,16 @@ -%% $Id: pst-magneticfield-docFR.tex 323 2010-05-16 11:39:35Z herbert $ +%% $Id: pst-magneticfield-docFR.tex 343 2010-06-10 15:08:37Z herbert $ \documentclass[11pt,english,french,BCOR10mm,DIV12,bibliography=totoc,parskip=false,smallheadings headexclude,footexclude,oneside]{pst-doc} \usepackage[latin1]{inputenc} \usepackage{pst-magneticfield} \let\pstMFfv\fileversion + +%\newenvironment{postscript}{}{} % uncomment, when running with latex + \lstset{pos=t,language=PSTricks, morekeywords={psmagneticfield,psmagneticfieldThreeD},basicstyle=\footnotesize\ttfamily} \newcommand\Cadre[1]{\psframebox[fillstyle=solid,fillcolor=black,linestyle=none,framesep=0]{#1}} -\def\bgImage{% -\psset{unit=0.5cm} -\begin{pspicture}(-7,-6)(7,6) -\psmagneticfieldThreeD[N=2,R=2,L=2,linecolor=blue](-7,-8)(7,8) -\ThreeDput{\rput(0,-7){\textbf{Bobines de HELMHOLTZ}}} -\end{pspicture} -} +\def\bgImage{} % \begin{document} @@ -85,22 +82,42 @@ des lignes de champ. \section{Influence des paramètres physiques sur la carte du champ magnétique} \subsection{La longueur du solénoïde} -\begin{LTXexample}[pos=t] +\begin{center} +\begin{postscript} \psset{unit=0.5cm} \begin{pspicture*}[showgrid](-7,-8)(7,8) -\psmagneticfield[linecolor={[HTML]{006633}},N=3,R=2,nS=1] +\psmagneticfield[linecolor={[HTML]{006633}},N=3,R=2,nS=1](-7,-8)(7,8) \psframe*[linecolor={[HTML]{99FF66}}](-7,-8)(7,-7) \rput(0,-7.5){[\Cadre{\textcolor{white}{L=4}},N=3,R=2,nS=1]} \end{pspicture*} \begin{pspicture*}[showgrid](-7,-8)(7,8) -\psmagneticfield[linecolor={[HTML]{006633}},L=8,N=3,R=2,nS=1,PasB=0.0025,pointsB=5500] +\psmagneticfield[linecolor={[HTML]{006633}},L=8,N=3,R=2,nS=1,PasB=0.0025,pointsB=5500](-7,-8)(7,8) \psframe*[linecolor={[HTML]{99FF66}}](-7,-8)(7,-7) \rput(0,-7.5){[\Cadre{\textcolor{white}{L=8}},N=3,R=2,nS=1]} \end{pspicture*} -\end{LTXexample} +\end{postscript} +\end{center} + +\begin{lstlisting} +\psset{unit=0.5cm} +\begin{pspicture*}[showgrid](-7,-8)(7,8) +\psmagneticfield[linecolor={[HTML]{006633}},N=3,R=2,nS=1](-7,-8)(7,8) +\psframe*[linecolor={[HTML]{99FF66}}](-7,-8)(7,-7) +\rput(0,-7.5){[\Cadre{\textcolor{white}{L=4}},N=3,R=2,nS=1]} +\end{pspicture*} +\begin{pspicture*}[showgrid](-7,-8)(7,8) +\psmagneticfield[linecolor={[HTML]{006633}},L=8,N=3,R=2,nS=1,PasB=0.0025,pointsB=5500](-7,-8)(7,8) +\psframe*[linecolor={[HTML]{99FF66}}](-7,-8)(7,-7) +\rput(0,-7.5){[\Cadre{\textcolor{white}{L=8}},N=3,R=2,nS=1]} +\end{pspicture*} +\end{lstlisting} + \textbf{Remarque :} pour affiner le tracé du deuxième solénoïde, on a du augmenter -le nombre de points et diminuer le pas du tracé : \Cadre{\textcolor{white}{pointsB=5500,PasB=0.0025}}, +le nombre de points et diminuer le pas du tracé : +\begin{postscript} +\Cadre{\textcolor{white}{pointsB=5500,PasB=0.0025}} +\end{postscript}, ce qui rallonge la durée des calculs. @@ -108,35 +125,70 @@ ce qui rallonge la durée des calculs. \clearpage \subsection{Le nombre de spires} -\begin{LTXexample}[pos=t] +\begin{center} +\begin{postscript} \psset{unit=0.5} \begin{pspicture*}[showgrid](-7,-8)(7,8) -\psmagneticfield[linecolor={[HTML]{006633}},N=1,R=2,nS=0] +\psmagneticfield[linecolor={[HTML]{006633}},N=1,R=2,nS=0](-7,-8)(7,8) \psframe*[linecolor={[HTML]{99FF66}}](-7,-8)(7,-7) \rput(0,-7.5){[\Cadre{\textcolor{white}{N=1}},R=2,nS=0]} \end{pspicture*} \begin{pspicture*}[showgrid](-7,-8)(7,8) -\psmagneticfield[linecolor={[HTML]{006633}},N=2,R=2,L=2,PasS=0.003,nS=2] +\psmagneticfield[linecolor={[HTML]{006633}},N=2,R=2,L=2,PasS=0.003,nS=2](-7,-8)(7,8) \psframe*[linecolor={[HTML]{99FF66}}](-7,7)(7,8) \rput(0,7.5){\Cadre{\textcolor{white}{Bobines de Helmholtz}}} \psframe*[linecolor={[HTML]{99FF66}}](-7,-8)(7,-7) \rput(0,-7.5){[\Cadre{\textcolor{white}{N=2}},R=2,L=2,PasS=0.003,nS=2]} \end{pspicture*} -\end{LTXexample} +\end{postscript} +\end{center} + +\begin{lstlisting} +\psset{unit=0.5} +\begin{pspicture*}[showgrid](-7,-8)(7,8) +\psmagneticfield[linecolor={[HTML]{006633}},N=1,R=2,nS=0](-7,-8)(7,8) +\psframe*[linecolor={[HTML]{99FF66}}](-7,-8)(7,-7) +\rput(0,-7.5){[\Cadre{\textcolor{white}{N=1}},R=2,nS=0]} +\end{pspicture*} +\begin{pspicture*}[showgrid](-7,-8)(7,8) +\psmagneticfield[linecolor={[HTML]{006633}},N=2,R=2,L=2,PasS=0.003,nS=2](-7,-8)(7,8) +\psframe*[linecolor={[HTML]{99FF66}}](-7,7)(7,8) +\rput(0,7.5){\Cadre{\textcolor{white}{Bobines de Helmholtz}}} +\psframe*[linecolor={[HTML]{99FF66}}](-7,-8)(7,-7) +\rput(0,-7.5){[\Cadre{\textcolor{white}{N=2}},R=2,L=2,PasS=0.003,nS=2]} +\end{pspicture*} +\end{lstlisting} + + +\begin{center} +\begin{postscript} +\psset{unit=0.5} +\begin{pspicture*}[showgrid](-7,-8)(7,8) +\psmagneticfield[linecolor={[HTML]{006633}},N=4,R=2,numSpires=2 3](-7,-8)(7,8) +\psframe*[linecolor={[HTML]{99FF66}}](-7,-8)(7,-7) +\rput(0,-7.5){[\Cadre{\textcolor{white}{N=4}},R=2,L=4]} +\end{pspicture*} +\begin{pspicture*}[showgrid](-7,-8)(7,8) +\psmagneticfield[linecolor={[HTML]{006633}},N=5,R=2,L=5,PasS=0.004,numSpires=2 3 4](-7,-8)(7,8) +\psframe*[linecolor={[HTML]{99FF66}}](-7,-8)(7,-7) +\rput(0,-7.5){[\Cadre{\textcolor{white}{N=5}},R=2,L=5]} +\end{pspicture*} +\end{postscript} +\end{center} -\begin{LTXexample}[pos=t] +\begin{lstlisting} \psset{unit=0.5} \begin{pspicture*}[showgrid](-7,-8)(7,8) -\psmagneticfield[linecolor={[HTML]{006633}},N=4,R=2,numSpires=2 3] +\psmagneticfield[linecolor={[HTML]{006633}},N=4,R=2,numSpires=2 3](-7,-8)(7,8) \psframe*[linecolor={[HTML]{99FF66}}](-7,-8)(7,-7) \rput(0,-7.5){[\Cadre{\textcolor{white}{N=4}},R=2,L=4]} \end{pspicture*} \begin{pspicture*}[showgrid](-7,-8)(7,8) -\psmagneticfield[linecolor={[HTML]{006633}},N=5,R=2,L=5,PasS=0.004,numSpires=2 3 4] +\psmagneticfield[linecolor={[HTML]{006633}},N=5,R=2,L=5,PasS=0.004,numSpires=2 3 4](-7,-8)(7,8) \psframe*[linecolor={[HTML]{99FF66}}](-7,-8)(7,-7) \rput(0,-7.5){[\Cadre{\textcolor{white}{N=5}},R=2,L=5]} \end{pspicture*} -\end{LTXexample} +\end{lstlisting} \clearpage @@ -150,19 +202,35 @@ avec \Lkeyword{numSpires}. -\begin{LTXexample}[pos=t] +\begin{center} +\begin{postscript} +\psset{unit=0.5} +\begin{pspicture*}[showgrid](-7,-8)(7,8) +\psmagneticfield[linecolor={[HTML]{000099}},N=1,R=2](-7,-8)(7,8) +\psframe*[linecolor={[HTML]{3399FF}}](-7,-8)(7,-7) +\rput(0,-7.5){[\Cadre{\textcolor{white}{nL=8}},N=1,R=2]} +\end{pspicture*} +\begin{pspicture*}[showgrid](-7,-8)(7,8) +\psmagneticfield[linecolor={[HTML]{000099}},N=1,R=2,nL=12](-7,-8)(7,8) +\psframe*[linecolor={[HTML]{3399FF}}](-7,-8)(7,-7) +\rput(0,-7.5){[\Cadre{\textcolor{white}{nL=12}},N=1,R=2]} +\end{pspicture*} +\end{postscript} +\end{center} + +\begin{lstlisting} \psset{unit=0.5} \begin{pspicture*}[showgrid](-7,-8)(7,8) -\psmagneticfield[linecolor={[HTML]{000099}},N=1,R=2] +\psmagneticfield[linecolor={[HTML]{000099}},N=1,R=2](-7,-8)(7,8) \psframe*[linecolor={[HTML]{3399FF}}](-7,-8)(7,-7) \rput(0,-7.5){[\Cadre{\textcolor{white}{nL=8}},N=1,R=2]} \end{pspicture*} \begin{pspicture*}[showgrid](-7,-8)(7,8) -\psmagneticfield[linecolor={[HTML]{000099}},N=1,R=2,nL=12] +\psmagneticfield[linecolor={[HTML]{000099}},N=1,R=2,nL=12](-7,-8)(7,8) \psframe*[linecolor={[HTML]{3399FF}}](-7,-8)(7,-7) \rput(0,-7.5){[\Cadre{\textcolor{white}{nL=12}},N=1,R=2]} \end{pspicture*} -\end{LTXexample} +\end{lstlisting} \clearpage \subsection{Le nombre de points et le pas du tracé} @@ -170,23 +238,44 @@ Le tracé des lignes de champ est réalisé par une méthode numérique (RK2) et il s le pas du tracé et le nombre de points choisis influent sur la précision du tracé, comme dans les deux exemples ci-dessous : -\begin{LTXexample}[pos=t] +\begin{center} +\begin{postscript} \psset{unit=0.5} \begin{pspicture*}[showgrid](-7,-8)(7,8) -\psmagneticfield[linecolor={[HTML]{660066}},N=2,R=2,L=2,PasB=0.1,nS=0,nL=7,pointsB=100] +\psmagneticfield[linecolor={[HTML]{660066}},N=2,R=2,L=2,PasB=0.1,nS=0,nL=7,pointsB=100](-7,-8)(7,8) \psframe*[linecolor={[HTML]{996666}}](-7,7)(7,8) \rput(0,7.5){\Cadre{\textcolor{white}{Bobines de Helmholtz}}} \psframe*[linecolor={[HTML]{996666}}](-7,-8)(7,-7) \rput(0,-7.5){[\Cadre{\textcolor{white}{PasB=0.1,nL=4,pointsB=100}}]} \end{pspicture*} \begin{pspicture*}[showgrid](-7,-8)(7,8) -\psmagneticfield[linecolor={[HTML]{660066}},N=2,R=2,L=2,PasB=0.4,nS=0,nL=7,pointsB=100] +\psmagneticfield[linecolor={[HTML]{660066}},N=2,R=2,L=2,PasB=0.4,nS=0,nL=7,pointsB=100](-7,-8)(7,8) \psframe*[linecolor={[HTML]{996666}}](-7,7)(7,8) \rput(0,7.5){\Cadre{\textcolor{white}{Bobines de Helmholtz}}} \psframe*[linecolor={[HTML]{996666}}](-7,-8)(7,-7) \rput(0,-7.5){[\Cadre{\textcolor{white}{PasS=0.4,pointsB=100}}]} \end{pspicture*} -\end{LTXexample} +\end{postscript} +\end{center} + +\begin{lstlisting} +\psset{unit=0.5} +\begin{pspicture*}[showgrid](-7,-8)(7,8) +\psmagneticfield[linecolor={[HTML]{660066}},N=2,R=2,L=2,PasB=0.1,nS=0,nL=7,pointsB=100](-7,-8)(7,8) +\psframe*[linecolor={[HTML]{996666}}](-7,7)(7,8) +\rput(0,7.5){\Cadre{\textcolor{white}{Bobines de Helmholtz}}} +\psframe*[linecolor={[HTML]{996666}}](-7,-8)(7,-7) +\rput(0,-7.5){[\Cadre{\textcolor{white}{PasB=0.1,nL=4,pointsB=100}}]} +\end{pspicture*} +\begin{pspicture*}[showgrid](-7,-8)(7,8) +\psmagneticfield[linecolor={[HTML]{660066}},N=2,R=2,L=2,PasB=0.4,nS=0,nL=7,pointsB=100](-7,-8)(7,8) +\psframe*[linecolor={[HTML]{996666}}](-7,7)(7,8) +\rput(0,7.5){\Cadre{\textcolor{white}{Bobines de Helmholtz}}} +\psframe*[linecolor={[HTML]{996666}}](-7,-8)(7,-7) +\rput(0,-7.5){[\Cadre{\textcolor{white}{PasS=0.4,pointsB=100}}]} +\end{pspicture*} +\end{lstlisting} + Si les valeurs par défaut ne conviennent pas il faut donc trouver par des essais les valeurs qui donnent un tracé correct. @@ -195,38 +284,72 @@ essais les valeurs qui donnent un tracé correct. \clearpage \section{Le paramètre: numSpires} -\begin{LTXexample}[pos=t,wide] +\begin{center} +\begin{postscript} \psset{unit=0.5} \begin{pspicture*}[showgrid](-8,-10)(8,10) \psset{linecolor=blue} -\psmagneticfield[R=2,L=12,N=8,pointsS=500,nL=14,nS=1,numSpires=1 3 6 8,PasB=0.075] +\psmagneticfield[R=2,L=12,N=8,pointsS=500,nL=14,nS=1,numSpires=1 3 6 8,PasB=0.075](-8,-10)(8,10) \psframe*[linecolor={[HTML]{99FF66}}](-8,-10)(8,-9) \rput(0,-9.5){[\Cadre{\textcolor{white}{numSpires=1 3 6 8}},R=2,L=14]} \multido{\i=0+1}{8}{\rput[l](!6 6 12 7 div \i\space mul sub){\the\multidocount}} \end{pspicture*}\quad \begin{pspicture*}[showgrid](0,-10)(16,10) \psset{linecolor=blue} -\psmagneticfield[R=2,L=12,N=8,pointsS=500,nL=14,numSpires=,nS=1,PasB=0.075] +\psmagneticfield[R=2,L=12,N=8,pointsS=500,nL=14,numSpires=,nS=1,PasB=0.075](0,-10)(16,10) \psframe*[linecolor={[HTML]{99FF66}}](0,-10)(16,-9) \rput(8,-9.5){[\Cadre{\textcolor{white}{numSpires=all}},R=2,L=14]} \multido{\i=0+1}{8}{\rput[l](!6 6 12 7 div \i\space mul sub){\the\multidocount}} \end{pspicture*} -\end{LTXexample} +\end{postscript} +\end{center} +\begin{lstlisting} +\psset{unit=0.5} +\begin{pspicture*}[showgrid](-8,-10)(8,10) +\psset{linecolor=blue} +\psmagneticfield[R=2,L=12,N=8,pointsS=500,nL=14,nS=1,numSpires=1 3 6 8,PasB=0.075](-8,-10)(8,10) +\psframe*[linecolor={[HTML]{99FF66}}](-8,-10)(8,-9) +\rput(0,-9.5){[\Cadre{\textcolor{white}{numSpires=1 3 6 8}},R=2,L=14]} +\multido{\i=0+1}{8}{\rput[l](!6 6 12 7 div \i\space mul sub){\the\multidocount}} +\end{pspicture*}\quad +\begin{pspicture*}[showgrid](0,-10)(16,10) +\psset{linecolor=blue} +\psmagneticfield[R=2,L=12,N=8,pointsS=500,nL=14,numSpires=,nS=1,PasB=0.075](0,-10)(16,10) +\psframe*[linecolor={[HTML]{99FF66}}](0,-10)(16,-9) +\rput(8,-9.5){[\Cadre{\textcolor{white}{numSpires=all}},R=2,L=14]} +\multido{\i=0+1}{8}{\rput[l](!6 6 12 7 div \i\space mul sub){\the\multidocount}} +\end{pspicture*} +\end{lstlisting} + \clearpage -\section{The parameter \nxLkeyword{AntiHelmholtz}} -\begin{LTXexample}[pos=t] +\section{Le param\`etre \nxLkeyword{AntiHelmholtz}} +\begin{center} +\begin{postscript} \psset{unit=0.75,AntiHelmholtz,N=2, R=2,pointsB=500,pointsS=1000,PasB=0.02,PasS=0.00275,nS=10, nL=2,drawSelf=true,styleSpire=styleSpire,styleCourant=sensCourant} \newpsstyle{grille}{subgriddiv=0,gridcolor=blue!50,griddots=10} \newpsstyle{cadre}{linecolor=yellow!50} \begin{pspicture*}[showgrid](-7,-6)(7,6) -\psframe*[linecolor={[HTML]{996666}}](-7,7)(7,8) +\psframe*[linecolor={[HTML]{996666}}](-7,6)(7,6) \psmagneticfield[linecolor={[HTML]{660066}}] \end{pspicture*} -\end{LTXexample} +\end{postscript} +\end{center} + +\begin{lstlisting} +\psset{unit=0.75,AntiHelmholtz,N=2, + R=2,pointsB=500,pointsS=1000,PasB=0.02,PasS=0.00275,nS=10, + nL=2,drawSelf=true,styleSpire=styleSpire,styleCourant=sensCourant} +\newpsstyle{grille}{subgriddiv=0,gridcolor=blue!50,griddots=10} +\newpsstyle{cadre}{linecolor=yellow!50} +\begin{pspicture*}[showgrid](-7,-6)(7,6) +\psframe*[linecolor={[HTML]{996666}}](-7,6)(7,6) +\psmagneticfield[linecolor={[HTML]{660066}}] +\end{pspicture*} +\end{lstlisting} \clearpage @@ -251,24 +374,61 @@ Les options du cadre sont, par défaut, les suivantes : \end{verbatim} Ce sont donc celles-ci qu'il faudra modifier si on souhaite en changer, comme dans l'exemple ci-dessous. -\begin{LTXexample}[pos=t] -\psset{unit=0.7} + + +\begin{center} +\begin{postscript} +\psset{unit=0.7cm} \newpsstyle{grille}{subgriddiv=0,gridcolor=blue!50,griddots=10} \newpsstyle{cadre}{linecolor=yellow!50} \begin{pspicture}(-7,-6)(7,6) -\psmagneticfieldThreeD[N=8,R=2,L=8,pointsB=1200,linecolor=blue,pointsS=1000](-7,-8)(7,8) +\psmagneticfieldThreeD[N=8,R=2,L=8,pointsB=1200,linecolor=blue,pointsS=2000](-7,-6)(7,6) \end{pspicture} -\end{LTXexample} +\end{postscript} +\end{center} -\begin{LTXexample}[pos=t] -\psset{unit=0.7} +\begin{lstlisting} +\psset{unit=0.7cm} +\newpsstyle{grille}{subgriddiv=0,gridcolor=blue!50,griddots=10} +\newpsstyle{cadre}{linecolor=yellow!50} +\begin{pspicture}(-7,-6)(7,6) +\psmagneticfieldThreeD[N=8,R=2,L=8,pointsB=1200,linecolor=blue,pointsS=2000](-7,-6)(7,6) +\end{pspicture} +\end{lstlisting} + + +\begin{center} +\begin{postscript} +\psset{unit=0.7cm} \begin{pspicture}(-7,-6)(7,6) -\psmagneticfieldThreeD[N=2,R=2,L=2,linecolor=blue](-7,-8)(7,8) +\psmagneticfieldThreeD[N=2,R=2,L=2,linecolor=blue](-7,-6)(7,6) \ThreeDput{\rput(0,-7){\textbf{Bobines de HELMHOLTZ}}} \end{pspicture} -\end{LTXexample} +\end{postscript} +\end{center} -\begin{LTXexample}[pos=t] +\begin{lstlisting} +\psset{unit=0.7cm} +\begin{pspicture}(-7,-6)(7,6) +\psmagneticfieldThreeD[N=2,R=2,L=2,linecolor=blue](-7,-6)(7,6) +\ThreeDput{\rput(0,-7){\textbf{Bobines de HELMHOLTZ}}} +\end{pspicture} +\end{lstlisting} + +\begin{center} +\begin{postscript} +\psset{unit=0.75cm,AntiHelmholtz,N=2, + R=2,pointsB=500,pointsS=1000,PasB=0.02,PasS=0.00275,nS=10, + nL=2,drawSelf,styleSpire=styleSpire,styleCourant=sensCourant} +\newpsstyle{grille}{subgriddiv=0,gridcolor=blue!50,griddots=10} +\newpsstyle{cadre}{linecolor=yellow!50} +\begin{pspicture}(-7,-6)(7,6) +\psmagneticfieldThreeD[linecolor={[HTML]{660066}}](-7,-6)(7,6) +\end{pspicture} +\end{postscript} +\end{center} + +\begin{lstlisting} \psset{unit=0.75cm,AntiHelmholtz,N=2, R=2,pointsB=500,pointsS=1000,PasB=0.02,PasS=0.00275,nS=10, nL=2,drawSelf,styleSpire=styleSpire,styleCourant=sensCourant} @@ -277,7 +437,65 @@ Ce sont donc celles-ci qu'il faudra modifier si on souhaite en changer, comme da \begin{pspicture}(-7,-6)(7,6) \psmagneticfieldThreeD[linecolor={[HTML]{660066}}](-7,-6)(7,6) \end{pspicture} -\end{LTXexample} +\end{lstlisting} + +\clearpage + +\section{Density plots} +\begin{center} +\begin{postscript} +\begin{pspicture}(-6,-4)(6,4) +\psmagneticfield[N=3,R=2,L=2,StreamDensityPlot](-6,-4)(6,4) +\end{pspicture} +\end{postscript} +\end{center} + +\begin{lstlisting} +\begin{pspicture}(-6,-4)(6,4) +\psmagneticfield[N=3,R=2,L=2,StreamDensityPlot](-6,-4)(6,4) +\end{pspicture} +\end{lstlisting} + +\begin{center} +\begin{postscript} +\psset{unit=0.75} +\begin{pspicture}(-6,-5)(6,5) +\psmagneticfield[N=2,R=2,L=1,StreamDensityPlot,setgray](-6,-5)(6,5) +\end{pspicture} +\end{postscript} +\end{center} + +\begin{lstlisting} +\psset{unit=0.75} +\begin{pspicture}(-6,-5)(6,5) +\psmagneticfield[N=2,R=2,L=1,StreamDensityPlot,setgray](-6,-5)(6,5) +\end{pspicture} +\end{lstlisting} + + +\begin{center} +\begin{postscript} +\psset{unit=0.75,AntiHelmholtz, + R=2,pointsB=500,pointsS=2000,PasB=0.02,PasS=0.00275,nS=10, + nL=2,drawSelf=true,styleSpire=styleSpire,styleCourant=sensCourant} +\begin{pspicture*}(-7,-6)(7,6) +\psmagneticfield[linecolor={[HTML]{660066}},StreamDensityPlot](-7,-6)(7,6) +\end{pspicture*} +\end{postscript} +\end{center} + + +\begin{lstlisting} +\psset{unit=0.75,AntiHelmholtz, + R=2,pointsB=500,pointsS=2000,PasB=0.02,PasS=0.00275,nS=10, + nL=2,drawSelf=true,styleSpire=styleSpire,styleCourant=sensCourant} +\begin{pspicture*}(-7,-6)(7,6) +\psmagneticfield[linecolor={[HTML]{660066}},StreamDensityPlot](-7,-6)(7,6) +\end{pspicture*} +\end{lstlisting} + + + \clearpage @@ -289,7 +507,7 @@ Ce sont donc celles-ci qu'il faudra modifier si on souhaite en changer, comme da \bgroup \raggedright \bibliographystyle{plain} -\bibliography{\jobname} +\bibliography{pst-magneticfield-doc} \egroup diff --git a/Master/texmf-dist/dvips/pst-magneticfield/pst-magneticfield.pro b/Master/texmf-dist/dvips/pst-magneticfield/pst-magneticfield.pro new file mode 100644 index 00000000000..fdd24b8217c --- /dev/null +++ b/Master/texmf-dist/dvips/pst-magneticfield/pst-magneticfield.pro @@ -0,0 +1,303 @@ +%% $Id: pst-magneticfield.pro 339 2010-06-07 20:50:23Z herbert $ +%% +%% This is file `pst-magneticfield.pro', +%% +%% IMPORTANT NOTICE: +%% +%% Package `pst-magneticfield.tex' +%% Jürgen Gilg +%% Manuel Luque +%% Herbert Voss +%% +%% This program can be redistributed and/or modified under the terms +%% of the LaTeX Project Public License Distributed from CTAN archives +%% in directory macros/latex/base/lppl.txt. +%% +%% DESCRIPTION: +%% `pst-magneticfield' is a PSTricks package to draw fields of Helmholtz coils +%% +%% version 0.01 / 2010-06-07 Herbert Voss <hvoss _at_ tug.org> +%% +% +/tx@MFieldDict 60 dict def +tx@MFieldDict begin +% +% helper functions +/setpixel { 1 0 360 arc fill } bind def +% +/fleche { + gsave + x2 y2 moveto + y2 y1 sub x2 x1 sub atan rotate % 1 1 scale + -1 CLW mul 2 CLW mul rlineto + 7 CLW mul -2 CLW mul rlineto + -7 CLW mul -2 CLW mul rlineto + closepath + fill + grestore +} def +/Calcul_B_Spires { + /Bx 0 def + /By 0 def + 1 1 NombreSpires { % on calcule le champ resultant de toutes les spires + /iS ED % numero de la spire + /yi yA iS 1 sub inter mul sub def % position de la spire + /Bx0 { + /arz {1 Radius xP add dup mul yP yi add dup mul add sqrt div} def + yP yi add xP div arz mul + EllipticK neg + Radius dup mul xP dup mul add yP yi add dup mul add + Radius xP sub dup mul yP yi add dup mul add div + EllipticE mul + add + mul + } def + /By0 { + /arz {1 Radius xP add dup mul yP yi add dup mul add sqrt div} def + arz + EllipticK + Radius dup mul xP dup mul sub yP yi add dup mul sub + Radius xP sub dup mul yP yi add dup mul add div + EllipticE mul + add + mul + } def + AntiHelmholtz { iS 2 eq {/Bx0 Bx0 neg def /By0 By0 neg def} if } if + /Bx Bx Bx0 add def + /By By By0 add def + } for +} def +/EllipticKE{ + /K {2 Radius xP mul sqrt mul arz mul} def + /m1 {1 K dup mul sub} def + /m2 {m1 dup mul} def + /m3 {m2 m1 mul} def + /m4 {m2 dup mul} def + /m_1 {1 m1 div} def + /EllipticK { + 0.5 + 0.12498593597 m1 mul add + 0.06880248576 m2 mul add + 0.03328355376 m3 mul add + 0.00441787012 m4 mul add + m_1 ln mul + 1.38629436112 add + 0.09666344259 m1 mul add + 0.03590092383 m2 mul add + 0.03742563713 m3 mul add + 0.01451196212 m4 mul add + } def + /EllipticE { + 0.24998368310 m1 mul + 0.09200180037 m2 mul add + 0.04069697526 m3 mul add + 0.00526449639 m4 mul add + m_1 ln mul + 1 add + 0.44325141463 m1 mul add + 0.062606012206 m2 mul add + 0.04757383546 m3 mul add + 0.01736506451 m4 mul add + } def + Calcul_B_Spires +% au point Pi + /xPi xP def + /yPi yP def + /NormeB Bx dup mul By dup mul add sqrt def + /dX Bx NormeB div Pas mul def + /dXi dX def + /dY By NormeB div Pas mul def + /dYi dY def + /xCi xPi dX add def + /yCi yPi dY add def + /xP xCi def + /yP yCi def + Calcul_B_Spires +% au point C + /NormeB Bx dup mul By dup mul add sqrt def + /dX Bx NormeB div Pas mul def + /dY By NormeB div Pas mul def + /yP yPi dY dYi add 2 div add def +} def +% +%0 0 translate +% +/setValues { % on stack +1 or -1 + /yfactor ED /xfactor ED + Ligne_Champ dup length 1 sub 1.5 div cvi get aload pop + yfactor 0 gt { + /y2 exch yfactor mul def + /x2 exch xfactor mul def + }{ + /y1 exch yfactor mul def + /x1 exch xfactor mul def + } ifelse + Ligne_Champ dup length 1 sub 1.5 div cvi 1 add get aload pop + yfactor 0 gt { + /y1 exch yfactor mul def + /x1 exch xfactor mul def + }{ + /y2 exch yfactor mul def + /x2 exch xfactor mul def + } ifelse +} def +% +/Lignes_Champ { + /Ligne_Champ [ + NbrePoints {% + EllipticKE + [ xP yP yUnit mul exch xUnit mul exch ] + trace 1 eq {By 0 lt Bx 0 lt and {exit} if} if + AntiHelmholtz not { xP xMax ge yP yMax ge or {exit} if } if + } repeat + ] def +% + Ligne_Champ 0 get aload pop moveto % xP yP + 1 1 Ligne_Champ length 1 sub { + /iCompteur exch def + Ligne_Champ iCompteur get aload pop lineto + } for + stroke +% les flèches (xP,yP) + 1 1 setValues + nCount 0 eq {/yAxe1 y1 def /yAxe2 y2 def} if + fleche +% + Ligne_Champ 0 get aload pop neg moveto % xP -yP + 1 1 Ligne_Champ length 1 sub { + /iCompteur ED + Ligne_Champ iCompteur get aload pop neg lineto + } for + stroke + trace 1 eq { +% (xP,-yP) + 1 -1 setValues + fleche + } if + Ligne_Champ 0 get aload pop exch neg exch moveto % -xP yP + 1 1 Ligne_Champ length 1 sub { + /iCompteur ED + Ligne_Champ iCompteur get aload pop exch neg exch lineto + } for + stroke +% (-xP,yP) + -1 1 setValues + fleche + Ligne_Champ 0 get aload pop exch neg exch neg moveto % -xP -yP + 1 1 Ligne_Champ length 1 sub { + /iCompteur ED + Ligne_Champ iCompteur get aload pop exch neg exch neg lineto + } for + stroke + trace 1 eq { +% (-xP,-yP) + -1 -1 setValues + fleche + } if + } def +% +/MagneticField { +StreamDensityPlot { + /Bmax 0 def + /Pas PasB def + % recherche du Bmax + AntiHelmholtz { + Radius 0.1 sub 0.1 Radius 1.5 mul { + /xP exch def + 0 0.1 yMax { + /yP exch def + EllipticKE + NormeB Bmax gt {/Bmax NormeB def} if + } for + }for + }{ + 0.01 0.1 Radius 0.1 sub { + /xP exch def + 0 0.1 yMax { + /yP exch def + EllipticKE + NormeB Bmax gt {/Bmax NormeB def} if + } for + }for + } ifelse +%/xP 0.001 def +%/yP 0 def +%EllipticKE +%/Bmax NormeB def + /StepPixel + 1 Unit div store + gsave + 0.009 StepPixel xMax { + /xPos ED + /xP xPos def + 0.009 StepPixel yMax { + /yPos ED + /yP yPos def + EllipticKE + /HB NormeB Bmax div store + Setgray { /HB HB 25 mul round 25 div def } if % 25 niveaux de gris + xPos xUnit mul yPos yUnit mul + Setgray { HB setgray setpixel }{ HB 0.7 1 sethsbcolor setpixel } ifelse + xPos xUnit mul neg yPos yUnit mul + Setgray { HB setgray }{ HB 0.7 1 sethsbcolor } ifelse setpixel + xPos xUnit mul neg yPos yUnit mul neg + Setgray { HB setgray }{ HB 0.7 1 sethsbcolor } ifelse setpixel + xPos xUnit mul yPos yUnit mul neg + Setgray { HB setgray }{ HB 0.7 1 sethsbcolor } ifelse setpixel + } for + }for + grestore +} if +% lignes de champ de l'ensemble de la bobine + /trace 1 def + /nCount 0 def +% 0.1 Radius mul StepLines Radius mul 0.9 Radius mul { + StepLines StepLines Radius 1.5 StepLines mul sub { + /NbrePoints NbrePointsB def + /xStart ED + /yStart 0 def + /Pas PasB def + /xP xStart def + /yP yStart Pas sub def + Lignes_Champ + /nCount nCount 1 add def + } for + AntiHelmholtz not { + % l'axe oriente de la bobine + 0 yMin yUnit mul moveto + 0 yMax yUnit mul lineto + stroke + /x1 0 def + /y1 yAxe1 def + /y2 yAxe2 def + /x2 0 def + fleche + %/x1 0 def + /y1 yAxe2 neg def + /y2 yAxe1 neg def + %/x2 0 def + fleche } if + % quelques lignes de champ autour de chaque spire + /trace 0 def + /increment 0.25 Radius mul def + AntiHelmholtz { /Pas PasS def /NbrePoints NbrePointsS def } if + nS { % nS lignes + 0 1 TS length 1 sub { + /nTemp ED + /iS TS nTemp get def % numero de la spire en partant du haut + iS 0 eq { /iS 1 def } if % iS ne peut pas = 0 + iS NombreSpires gt { /iS NombreSpires def } if % iS ne peut pas > nbre spires + /yi yA iS 1 sub inter mul sub def % position du centre de la spire + AntiHelmholtz not { /NbrePoints NbrePointsS def /Pas PasS def } if + /xStart Radius increment add def + /yStart yi def + /xP xStart def + /yP yStart Pas sub def + Lignes_Champ + } for + AntiHelmholtz { /NbrePoints NbrePoints 750 add def } if + /increment increment 0.2 Radius mul add def + } repeat +} def % /MagneticField +end +%% diff --git a/Master/texmf-dist/source/generic/pst-magneticfield/Makefile b/Master/texmf-dist/source/generic/pst-magneticfield/Makefile index 96b8b8a3ef4..5ab44b5e071 100644 --- a/Master/texmf-dist/source/generic/pst-magneticfield/Makefile +++ b/Master/texmf-dist/source/generic/pst-magneticfield/Makefile @@ -1,55 +1,70 @@ -# `Makefile' for `pst-magneticfield.pdf', hv, 2007/03/17 +# `Makefile' for `pst-magneticfield.pdf', Rolf Niepraschk, 2010/05/21 -.SUFFIXES : .tex .ltx .dvi .ps .pdf .eps +.SUFFIXES : .tex .ltx .dvi .ps .pdf .eps .pro PACKAGE = pst-magneticfield +MAIN = $(PACKAGE)-doc +LANGUAGES = FR -MAIN = $(PACKAGE)-docFR +empty= +space=$(empty) $(empty) +DOC_SOURCES = $(addprefix $(PACKAGE)-doc,$(LANGUAGES)$(space)) +DOC_SOURCES := $(addsuffix .tex, $(DOC_SOURCES)) +DOCS = $(DOC_SOURCES:.tex=.pdf) TDS = ~/PSTricks/PSTricks-TDS -LATEX = latex +LATEX = pst2pdf +PDFLATEX = pdflatex +OPTIONS= --Iext=.png --Iscale=0.5 --DPI=150 -ARCHNAME = $(MAIN)-$(shell date +%y%m%d) +ARCHNAME = $(PACKAGE)-$(shell date +%Y%m%d) -ARCHFILES = $(PACKAGE).sty $(PACKAGE).tex $(PACKAGE).pro $(MAIN).tex README Changes Makefile +#PRO = foo.pro -all : doc clean tds -doc: $(MAIN).pdf +ARCHFILES = $(PACKAGE).sty $(PACKAGE).tex $(PACKAGE).pro $(DOC_SOURCES) \ + README Changes Makefile -$(MAIN).pdf : $(MAIN).ps - GS_OPTIONS=-dAutoRotatePages=/None ps2pdf $< +all : $(DOCS) clean -$(MAIN).ps : $(MAIN).dvi - dvips $< +%.pdf : %.tex + $(LATEX) $(basename $<) $(OPTIONS) +# makeindex -s gglo.ist -t $(basename $<)-pdf.glg -o $(basename $<)-pdf.gls $(basename $<)-pdf.glo + makeindex -s pst-doc.ist -t $(basename $<)-pdf.ilg -o $(basename $<)-pdf.ind $(basename $<)-pdf.idx + bibtex $(basename $<)-pdf + $(PDFLATEX) $(basename $<)-pdf + $(PDFLATEX) $(basename $<)-pdf + mv $(basename $<)-pdf.pdf $(basename $<).pdf + rm -f $(basename $<)-tmp.* $(basename $<)-pdf.* -$(MAIN).dvi : $(MAIN).tex - $(LATEX) $< - $(LATEX) $< - if ! test -f $(basename $<).glo ; then touch $(basename $<).glo; fi - if ! test -f $(basename $<).idx ; then touch $(basename $<).idx; fi - makeindex -t $(basename $<).ilg -s pst-doc.ist -o $(basename $<).ind $(basename $<).idx - makeindex -s gglo.ist -t $(basename $<).glg -o $(basename $<).gls \ - $(basename $<).glo - bibtex $(basename $<) - $(LATEX) $< - $(LATEX) $< - -clean : - $(RM) $(addprefix $(MAIN), .log .aux .glg .glo .gls .ilg .idx .ind .tmp .toc .out .blg .bbl ) - $(RM) $(addprefix $(MAIN), .dvi .ps .xcp) +clean : + $(RM) $(foreach i,$(DOC_SOURCES:.tex=),$(addprefix $i, \ + .log .plog .preamble .aux .glg .glo .gls .ilg .idx .ind .tmp .toc .out .blg .bbl)) veryclean : clean - $(RM) $(addprefix $(MAIN), .pdf .bbl .blg) + $(RM) $(foreach i,$(DOC_SOURCES:.tex=),$(addprefix $i, \ + .pdf .bbl .blg)) arch : zip $(ARCHNAME).zip $(ARCHFILES) -tds: +ifneq ($(strip $(PRO)),) +installPRO : + @echo "Installiere PRO-Dateien ($(PRO))..." + cp -u Changes $(TDS)/dvips/$(PACKAGE)/ + cp -u $(PACKAGE).pro $(TDS)/dvips/$(PACKAGE)/ + cp -u $(PACKAGE).pro ~/Links/dvips-local/ +else +installPRO : + @: +endif + +tds : installPRO + @echo "Installiere TeX-Zeug..." cp -u Changes $(TDS)/doc/generic/$(PACKAGE)/ cp -u README $(TDS)/doc/generic/$(PACKAGE)/ - cp -u $(MAIN).pdf $(TDS)/doc/generic/$(PACKAGE)/ + cp -u *.pdf $(TDS)/doc/generic/$(PACKAGE)/ # cp -u Changes $(TDS)/tex/latex/$(PACKAGE)/ cp -u $(PACKAGE).sty $(TDS)/tex/latex/$(PACKAGE)/ @@ -57,14 +72,12 @@ tds: cp -u Changes $(TDS)/tex/generic/$(PACKAGE)/ cp -u $(PACKAGE).tex $(TDS)/tex/generic/$(PACKAGE)/ # -# cp -u Changes $(TDS)/dvips/$(PACKAGE)/ -# cp -u $(PACKAGE).pro $(TDS)/dvips/$(PACKAGE)/ -# cp -u $(PACKAGE).pro ~/Links/dvips-local/ -# cp -u Changes $(TDS)/source/$(PACKAGE)/ - cp -u $(MAIN).tex $(TDS)/source/$(PACKAGE)/ + cp -u *-doc??.tex $(TDS)/source/$(PACKAGE)/ cp -u $(MAIN).bib $(TDS)/source/$(PACKAGE)/ cp -u Makefile $(TDS)/source/$(PACKAGE)/ +debug : + @echo $(DOC_SOURCES) # EOF diff --git a/Master/texmf-dist/tex/generic/pst-magneticfield/pst-magneticfield.tex b/Master/texmf-dist/tex/generic/pst-magneticfield/pst-magneticfield.tex index 5e18949bd2f..417a78dade5 100644 --- a/Master/texmf-dist/tex/generic/pst-magneticfield/pst-magneticfield.tex +++ b/Master/texmf-dist/tex/generic/pst-magneticfield/pst-magneticfield.tex @@ -1,6 +1,6 @@ %% Package `pst-magneticfield.tex' %% -%% Manuel Luque +%% Manuel Luque %% Jürgen Gilg %% Herbert Voß %% @@ -20,14 +20,18 @@ \ifx\MultidoLoaded\endinput\else \input multido.tex\fi \ifx\PSTXKeyLoaded\endinput\else \input pst-xkey \fi % -\def\fileversion{1.11} -\def\filedate{2010/05/16} +\def\fileversion{1.12} +\def\filedate{2010/06/07} \message{`pst-magneticfield' v\fileversion, \filedate\space (ml,jg,hv)} % \edef\PstAtCode{\the\catcode`\@} \catcode`\@=11\relax % \SpecialCoor \pst@addfams{pst-magneticfield} + +%% prologue for postcript +\pstheader{pst-magneticfield.pro}% + % the first three parameter cannot be read with \pst@getint, because \pstFP.. do not like % the values ... used in \psmagenticfieldThreeD \define@key[psset]{pst-magneticfield}{R}[1]{\def\psk@magneticfieldR{#1}}% rayon d'une spire @@ -46,272 +50,73 @@ % \newpsstyle{styleSpire}{linecap=1,linecolor=red,linewidth=2\pslinewidth} \newpsstyle{sensCourant}{linecolor=red,linewidth=2\pslinewidth,arrowinset=0.1} -\newpsstyle{grille}{subgriddiv=0,gridcolor=lightgray,griddots=10} -\newpsstyle{cadre}{linecolor=green!20} % \define@boolkey[psset]{pst-magneticfield}[Pst@]{drawSelf}[true]{} \define@boolkey[psset]{pst-magneticfield}[Pst@]{AntiHelmholtz}[true]{} +\define@boolkey[psset]{pst-magneticfield}[Pst@]{StreamDensityPlot}[true]{} +\define@boolkey[psset]{pst-magneticfield}[Pst@]{setgray}[true]{} % \psset[pst-magneticfield]{R=1,L=4,N=6,pointsB=500,pointsS=1000, PasB=0.02,PasS=0.00275,nS=1,nL=8,drawSelf,styleSpire=styleSpire, - styleCourant=sensCourant,AntiHelmholtz=false} + styleCourant=sensCourant,AntiHelmholtz=false,StreamDensityPlot=false,setgray=false} +% +\def\tx@MFieldDict{ tx@MFieldDict begin } % \def\psmagneticfield{\pst@object{psmagneticfield}} -\def\psmagneticfield@i{% +\def\psmagneticfield@i{\@ifnextchar({\psmagneticfield@ii}{\psmagneticfield@iii(-6,-5)(6,5)}} +\def\psmagneticfield@ii(#1,#2){\@ifnextchar({\psmagneticfield@iii(#1,#2)}{\psmagneticfield@iii(#1,#2)(6,5)}} +\def\psmagneticfield@iii(#1,#2)(#3,#4){% \pst@killglue% - \ifPst@AntiHelmholtz\addbefore@par{N=2}\fi + \ifPst@AntiHelmholtz\addto@par{N=2}\fi \begin@SpecialObj% \pst@Verb{% make it global /NombreSpires \psk@magneticfieldN\space def /Radius \psk@magneticfieldR\space def /nombreLignes \psk@magneticfieldNL\space def /TableauSpires [\psk@magneticfieldChoixSpires] def + /StepLines Radius nombreLignes 1 add div def + NombreSpires 1 eq + { /Longueur 0 def + /inter 0 def } + { /Longueur \psk@magneticfieldL\space def + /inter Longueur NombreSpires 1 sub div def } ifelse % intervalle entre 2 spires \ifPst@AntiHelmholtz + /AntiHelmholtz true def TableauSpires length 0 eq {/TS [1 2] def} {/TS TableauSpires def } ifelse + /inter Radius def + /yA Radius 2 div def \else + /AntiHelmholtz false def TableauSpires length 0 eq {/TS [1 1 NombreSpires {} for] def} {/TS TableauSpires def } ifelse + /yA Longueur 2 div def \fi - /StepLines Radius nombreLignes 1 add div def - NombreSpires 1 eq - { /Longueur 0 def - /inter 0 def } - { /Longueur \psk@magneticfieldL\space def - /inter Longueur NombreSpires 1 sub div def } ifelse % intervalle entre 2 spires /NbrePointsB \psk@magneticfieldB\space def /NbrePointsS \psk@magneticfieldS\space def - \ifPst@AntiHelmholtz - /inter Radius def - /yA Radius 2 div def - \else - /yA Longueur 2 div def - \fi /PasB \psk@magneticfieldPasB\space def /PasS \psk@magneticfieldPasS\space def - /nS \psk@magneticfieldNS\space def - }% - \addto@pscode{ - /fleche { - gsave - x2 y2 moveto - y2 y1 sub x2 x1 sub atan rotate % 1 1 scale - -1 CLW mul 2 CLW mul rlineto - 7 CLW mul -2 CLW mul rlineto - -7 CLW mul -2 CLW mul rlineto - closepath - fill - grestore - } def - /Calcul_B_Spires { - /Bx 0 def - /By 0 def - 1 1 NombreSpires { % on calcule le champ resultant de toutes les spires - /iS ED % numero de la spire - /yi yA iS 1 sub inter mul sub def % position de la spire - /Bx0 { - /arz {1 Radius xP add dup mul yP yi add dup mul add sqrt div} def - yP yi add xP div arz mul - EllipticK neg - Radius dup mul xP dup mul add yP yi add dup mul add - Radius xP sub dup mul yP yi add dup mul add div - EllipticE mul - add - mul - } def - /By0 { - /arz {1 Radius xP add dup mul yP yi add dup mul add sqrt div} def - arz - EllipticK - Radius dup mul xP dup mul sub yP yi add dup mul sub - Radius xP sub dup mul yP yi add dup mul add div - EllipticE mul - add - mul - } def - \ifPst@AntiHelmholtz - iS 2 eq {/Bx0 Bx0 neg def /By0 By0 neg def} if - \fi - /Bx Bx Bx0 add def - /By By By0 add def - } for - } def - /EllipticKE{ - /K {2 Radius xP mul sqrt mul arz mul} def - /m1 {1 K dup mul sub} def - /m2 {m1 dup mul} def - /m3 {m2 m1 mul} def - /m4 {m2 dup mul} def - /m_1 {1 m1 div} def - /EllipticK { - 0.5 - 0.12498593597 m1 mul add - 0.06880248576 m2 mul add - 0.03328355376 m3 mul add - 0.00441787012 m4 mul add - m_1 ln mul - 1.38629436112 add - 0.09666344259 m1 mul add - 0.03590092383 m2 mul add - 0.03742563713 m3 mul add - 0.01451196212 m4 mul add - } def - /EllipticE { - 0.24998368310 m1 mul - 0.09200180037 m2 mul add - 0.04069697526 m3 mul add - 0.00526449639 m4 mul add - m_1 ln mul - 1 add - 0.44325141463 m1 mul add - 0.062606012206 m2 mul add - 0.04757383546 m3 mul add - 0.01736506451 m4 mul add - } def - Calcul_B_Spires -% au point Pi - /xPi xP def - /yPi yP def - /NormeB Bx dup mul By dup mul add sqrt def - /dX Bx NormeB div Pas mul def - /dXi dX def - /dY By NormeB div Pas mul def - /dYi dY def - /xCi xPi dX add def - /yCi yPi dY add def - /xP xCi def - /yP yCi def - Calcul_B_Spires -% au point C - /NormeB Bx dup mul By dup mul add sqrt def - /dX Bx NormeB div Pas mul def - /dY By NormeB div Pas mul def - /yP yPi dY dYi add 2 div add def - } def -% - 0 0 translate - /Lignes_Champ { - /Ligne_Champ [ - NbrePoints {% - EllipticKE - [ xP yP \tx@ScreenCoor ] - trace 1 eq {By 0 lt Bx 0 lt and {exit} if} if - } repeat - ] def -% - Ligne_Champ 0 get aload pop moveto % xP yP - 1 1 Ligne_Champ length 1 sub { - /iCompteur exch def - Ligne_Champ iCompteur get aload pop lineto - } for - stroke -% les flèches (xP,yP) - Ligne_Champ dup length 1 sub 3 div cvi get aload pop /y1 exch def /x1 exch def - Ligne_Champ dup length 1 sub 3 div cvi 1 add get aload pop /y2 exch def /x2 exch def - nCount 0 eq {/yAxe1 y1 def /yAxe2 y2 def} if - fleche -% - Ligne_Champ 0 get aload pop neg moveto % xP -yP - 1 1 Ligne_Champ length 1 sub { - /iCompteur ED - Ligne_Champ iCompteur get aload pop neg lineto - } for - stroke - trace 1 eq { -% (xP,-yP) - Ligne_Champ dup length 1 sub 3 div cvi get aload pop /y2 exch neg def /x2 ED - Ligne_Champ dup length 1 sub 3 div cvi 1 add get aload pop /y1 exch neg def /x1 ED - fleche - } if - Ligne_Champ 0 get aload pop exch neg exch moveto % -xP yP - 1 1 Ligne_Champ length 1 sub { - /iCompteur ED - Ligne_Champ iCompteur get aload pop exch neg exch lineto - } for - stroke -% (-xP,yP) - Ligne_Champ dup length 1 sub 3 div cvi get aload pop /y1 exch def /x1 exch neg def - Ligne_Champ dup length 1 sub 3 div cvi 1 add get aload pop /y2 exch def /x2 exch neg def - fleche - Ligne_Champ 0 get aload pop exch neg exch neg moveto % -xP -yP - 1 1 Ligne_Champ length 1 sub { - /iCompteur ED - Ligne_Champ iCompteur get aload pop exch neg exch neg lineto - } for - stroke - trace 1 eq { -% (-xP,-yP) - Ligne_Champ dup length 1 sub 3 div cvi get aload pop /y2 exch neg def /x2 exch neg def - Ligne_Champ dup length 1 sub 3 div cvi 1 add get aload pop /y1 exch neg def /x1 exch neg def - fleche - } if - } def -% -% lignes de champ de l'ensemble de la bobine - /trace 1 def - /nCount 0 def -% 0.1 Radius mul StepLines Radius mul 0.9 Radius mul { - StepLines StepLines Radius 1.5 StepLines mul sub { - /NbrePoints NbrePointsB def - /xStart ED - /yStart 0 def - /Pas PasB def - /xP xStart def - /yP yStart Pas sub def - Lignes_Champ - /nCount nCount 1 add def - } for - \ifPst@AntiHelmholtz\else - % l'axe orienté de la bobine - 0 -10 \tx@ScreenCoor moveto - 0 10 \tx@ScreenCoor lineto - stroke - /x1 0 def - /y1 yAxe1 def - /y2 yAxe2 def - /x2 0 def - fleche - %/x1 0 def - /y1 yAxe2 neg def - /y2 yAxe1 neg def - %/x2 0 def - fleche - \fi - % quelques lignes de champ autour de chaque spire - /trace 0 def - /increment 0.25 Radius mul def - \ifPst@AntiHelmholtz - /Pas PasS def - /NbrePoints NbrePointsS def - \fi - nS { % nS lignes - 0 1 TS length 1 sub { - /nTemp ED - /iS TS nTemp get def % numero de la spire en partant du haut - iS 0 eq { /iS 1 def } if % iS ne peut pas = 0 - iS NombreSpires gt { /iS NombreSpires def } if % iS ne peut pas > nbre spires - /yi yA iS 1 sub inter mul sub def % position du centre de la spire - \ifPst@AntiHelmholtz\else - /NbrePoints NbrePointsS def - /Pas PasS def - \fi - /xStart Radius increment add def - /yStart yi def - /xP xStart def - /yP yStart Pas sub def - Lignes_Champ - } for - \ifPst@AntiHelmholtz /NbrePoints NbrePoints 750 add def \fi - /increment increment 0.2 Radius mul add def - } repeat + /nS \psk@magneticfieldNS\space def +% pour la carte de densite + /xMin #1 def + /xMax #3 def + % NombreSpires 1 eq {/yMax 2 Radius mul def}{/yMax Longueur 2 mul def} ifelse + /yMax #4 def + /yMin #2 def + /Unit \pst@number\psunit def + /xUnit \pst@number\psxunit def + /yUnit \pst@number\psyunit def + /StreamDensityPlot \ifPst@StreamDensityPlot true \else false \fi def + /Setgray \ifPst@setgray true \else false \fi def }% + \addto@pscode{ \tx@MFieldDict MagneticField end} \ifPst@drawSelf \ifPst@AntiHelmholtz \psline[style=\psk@styleSpire](!Radius neg Radius 2 div)(!Radius Radius 2 div) \psline[style=\psk@styleCourant]{<-}(!-0.2 Radius 2 div)(!0.2 Radius 2 div) \psline[style=\psk@styleSpire](!Radius neg Radius 2 div neg)(!Radius Radius 2 div neg) \psline[style=\psk@styleCourant]{->}(!-0.2 Radius 2 div neg)(!0.2 Radius 2 div neg) - \else + \else \multido{\i=1+1}{\psk@magneticfieldN}{% numero de la spire \pst@Verb{ /Yspire yA \i\space 1 sub inter mul sub def } % position de la spire \psline[style=\psk@styleSpire](! Radius neg Yspire)(! Radius Yspire) @@ -321,36 +126,32 @@ \end@SpecialObj% \ignorespaces} % -%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% -%%%%%%%%%%\psmagneticfieldThreeD%%%%%%%%%%%%%%%%%%%%%%%%%%% -%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\newpsstyle{grille}{subgriddiv=0,gridcolor=lightgray,griddots=10} +\newpsstyle{cadre}{linecolor=green!20} % \def\psmagneticfieldThreeD{\pst@object{psmagneticfieldThreeD}} \def\psmagneticfieldThreeD@i(#1,#2)(#3,#4){% - \ifPst@AntiHelmholtz\addbefore@par{N=2}\fi + \ifPst@AntiHelmholtz\addto@par{N=2}\fi \begingroup \use@par \ifPst@AntiHelmholtz - \ThreeDput{% - \psframe*[style=cadre](#1,#2)(#3,#4) - \psgrid[style=grille](#1,#2)(#3,#4)} \pstFPdiv\yA{\psk@magneticfieldR}{2} - \ThreeDput[normal=0 1 0](0,\yA,0){% - \psarc[linecolor=red,linewidth=1\pslinewidth,linestyle=dashed](0,0){\psk@magneticfieldR}{180}{360}} - \ThreeDput[normal=0 1 0](0,-\yA,0){% - \psarc[linecolor=red,linewidth=1\pslinewidth,linestyle=dashed](0,0){\psk@magneticfieldR}{180}{360}} \ThreeDput{% \begin{psclip}{\psframe(#1,#2)(#3,#4)} - \psmagneticfield[drawSelf=false]% + \psframe*[style=cadre](#1,#2)(#3,#4) + \psgrid[style=grille](#1,#2)(#3,#4) + \psmagneticfield[drawSelf=false](#1,#2)(#3,#4)% \end{psclip}} \ThreeDput[normal=0 1 0](0,\yA,0){% \psarc[linecolor=red,linewidth=3\pslinewidth](0,0){\psk@magneticfieldR}{0}{180} - \psarc[linecolor=red,linewidth=3\pslinewidth]{<-}(0,0){\psk@magneticfieldR}{80}{90}} - \ThreeDput[normal=0 1 0](0,-\yA,0){% + \psarc[linecolor=red,linewidth=3\pslinewidth]{<-}(0,0){\psk@magneticfieldR}{80}{90} + \psarc[linecolor=red,linewidth=1\pslinewidth,linestyle=dashed](0,0){\psk@magneticfieldR}{180}{360}} + \ThreeDput[normal=0 1 0](0,-\yA,0){% \psarc[linecolor=red,linewidth=3\pslinewidth](0,0){\psk@magneticfieldR}{0}{180} - \psarc[linecolor=red,linewidth=3\pslinewidth]{->}(0,0){\psk@magneticfieldR}{80}{90}} + \psarc[linecolor=red,linewidth=3\pslinewidth]{->}(0,0){\psk@magneticfieldR}{80}{90} + \psarc[linecolor=red,linewidth=1\pslinewidth,linestyle=dashed](0,0){\psk@magneticfieldR}{180}{360}} \else - \ifnum\psk@magneticfieldN=1 + \ifnum\psk@magneticfieldN=1 \def\MF@inter{0} \def\yA{0} \else @@ -359,24 +160,18 @@ \pstFPdiv\yA{\psk@magneticfieldL}{2} \fi \ThreeDput{% - \psframe*[style=cadre](#1,#2)(#3,#4) - \psgrid[style=grille](#1,#2)(#3,#4)} - \multido{\iN=1+1,\iS=0+1}{\psk@magneticfieldN}{% - \pstFPmul\MF@calcA{\iS}{\MF@inter} - \pstFPsub\posSpire{\yA}{\MF@calcA} - \ThreeDput[normal=0 1 0](0,\posSpire,0){% - \psarc[linecolor=red,linewidth=1\pslinewidth,linestyle=dashed](0,0){\psk@magneticfieldR}{180}{360}} - }% - \ThreeDput{% \begin{psclip}{\psframe(#1,#2)(#3,#4)} - \psmagneticfield[drawSelf=false]% + \psframe*[style=cadre](#1,#2)(#3,#4) + \psgrid[style=grille](#1,#2)(#3,#4) + \psmagneticfield[drawSelf=false](#1,#2)(#3,#4)% \end{psclip}} \multido{\iN=1+1,\iS=0+1}{\psk@magneticfieldN}{% \pstFPmul\MF@calcA{\iS}{\MF@inter} \pstFPsub\posSpire{\yA}{\MF@calcA} \ThreeDput[normal=0 1 0](0,\posSpire,0){% - \psarc[linecolor=red,linewidth=3\pslinewidth](0,0){\psk@magneticfieldR}{0}{180} - \psarc[linecolor=red,linewidth=3\pslinewidth]{->}(0,0){\psk@magneticfieldR}{80}{90}} + \psarc[style=\psk@styleSpire](0,0){\psk@magneticfieldR}{0}{180} + \psarc[style=\psk@styleCourant]{->}(0,0){\psk@magneticfieldR}{80}{90} + \psarc[style=\psk@styleSpire,linestyle=dashed](0,0){\psk@magneticfieldR}{180}{360}}% }% \fi \endgroup} @@ -384,5 +179,5 @@ \catcode`\@=\PstAtCode\relax % %% END -\endinput +\endinput |