書式/数式/TexCode のバックアップの現在との差分(No.1)

• バックアップ一覧
• 差分 を表示
• 現在との差分 を表示
• ソース を表示
• バックアップ を表示
• 書式/数式/TexCode へ行く。

 \LaTeX 

/home/limg/www/LimgWiki/eq! You can't use `\spacefactor' in math mode.
\@->\spacefactor 
                 \@m 
l.33 $}
       

  1
  2
  3
  4
  5

#spanend
#spanadd
凌宮数学の数式プラグイン## eq ##で使用可能な$$ \text{\TeX} $$コマンド
#spanend
#spanadd

\newcommand{\spc}[2]{{\ooalign{{\hss{$#1$}\hss}\crcr{\phantom{\hss{$#2$}\hss}}}}}\newcommand{\clap}[2]{{\ooalign{{\hss{$#1$}\hss}\crcr{\hss{$#2$}\hss}}}}

\renewcommand{\b}[1]{{\bm {#1}}}\def\:#1{{\b#1}}\def\bi{{\bm i}}

\newcommand{\sx}{ \mathbin{\bm \cdot}} % Dot Product\newcommand{\Sx}{ \mathbin{\spc{\bm \cdot}{\times}}} % Dot Product (Alignment as cross product)\newcommand{\vx}{ \mathbin \times } % Cross Product\newcommand{\wx}{ \mathbin \wedge } % Widge Product\newcommand{\tx}{ \mathbin \otimes } % Tensor Product\newcommand{\wxv}{\mathbin{\clap{\wx}{{}_{{}_v}}}} % Widge Product of Macro vector\newcommand{\wxb}{\mathbin{\clap{\wx}{{}_{{}_b}}}} % Base Product

\newcommand{\grad }{\mathrm{grad}}\newcommand{\rot }{\mathrm{rot}}\newcommand{\diver}{\mathrm{div}}

\newcommand{\perct}{\%}

\newcommand{\pr}{\partial}\newcommand{\dl}{\delta}\newcommand{\Dl}{\varDelta}

\newcommand{\ff} [2]{\frac{\,{#1}\,}{\,{#2}\,}}\newcommand{\dd} [2]{\frac{\,d{#1}\,}{\,d{#2}\,}}\newcommand{\pp} [2]{\frac{\,\pr{#1}\,}{\,\pr{#2}\,}}

\newcommand{\ffd}[2]{\disp{\ff{\disp{#1}\mathstrut}{\disp{#2}\mathstrut}}}\newcommand{\ddd}[2]{\disp{\dd{\disp{#1}\mathstrut}{\disp{#2}\mathstrut}}}\newcommand{\ppd}[2]{\disp{\pp{\disp{#1}\mathstrut}{\disp{#2}\mathstrut}}}

\newcommand{\rt}[2][{\;\;}]{\sqrt[#1]{#2\,}}\newcommand{\Inte}[2][]{\!\int_{#1}^{#2}}\newcommand{\inte}[1][\,\,]{\!\int_{#1\!}}\newcommand{\nte}[1][\,\,]{\!\!\int_{#1\!}}

\newcommand{\hindent}{\hspace{2em}}

\newcommand{\bs}[1]{{\scriptstyle(#1)}}

\newcommand{\fracstrut}{\vphantom{\frac{\mathstrut}{\mathstrut}}}\newcommand{\ffdstrut}{\vphantom{\ffd{\mathstrut}{\mathstrut}}}

\renewcommand{\arraystretch}{1}\newcommand{\arr}[2][c]{{}\!\begin{array}{#1}#2\end{array}\!{}}\newcommand{\arrc}[2][c]{{}\!\left(\arr[#1]{#2}\right)\!{}}\newcommand{\arrs}[2][c]{{}\!\left[\arr[#1]{#2}\right]\!{}}\newcommand{\arrw}[2][c]{{}\!\left\{\arr[#1]{#2}\right\}\!{}}\newcommand{\arrb}[2][c|c]{\!\left[{}\!\arr[#1]{#2}\right]\!\!{}}

\newcommand{\iro}[2][ak]{{\color{#1}#2}}\newcommand{\clr}[2][red]{{\color{#1}#2}}

\newcommand{\omicron }{o}

\newcommand{\varAlpha }{A}\newcommand{\varBega }{B}\newcommand{\varEpsilon}{E}\newcommand{\varZeta }{Z}\newcommand{\varEta }{H}\newcommand{\varIota }{I}\newcommand{\varKapper }{K}\newcommand{\varMu }{M}\newcommand{\varNu }{N}\newcommand{\varOmicron}{O}\newcommand{\varRho }{P}\newcommand{\varTau }{T}\newcommand{\varChi }{X}

\newcommand{\gal}{\alpha }\newcommand{\gbt}{\beta }\newcommand{\ggm}{\gamma }\newcommand{\gdl}{\delta }\newcommand{\gep}{\varepsilon}\newcommand{\gzt}{\zeta }\newcommand{\get}{\eta }\newcommand{\gth}{\theta }\newcommand{\gio}{\iota }\newcommand{\gkp}{\kappa }\newcommand{\glm}{\lambda }\newcommand{\gmu}{\mu }\newcommand{\gnu}{\nu }\newcommand{\gxi}{\xi }\newcommand{\gom}{ o }\newcommand{\gpi}{\pi }\newcommand{\grh}{\rho }\newcommand{\gsg}{\sigma }\newcommand{\gta}{\tau }\newcommand{\gup}{\upsilon }\newcommand{\gph}{\varphi }\newcommand{\gch}{\chi }\newcommand{\gps}{\psi }\newcommand{\goM}{\omega }\newcommand{\gks}{\xi }

\newcommand{\gAl}{ A }\newcommand{\gBt}{ B }\newcommand{\gGm}{\varGamma }\newcommand{\gDl}{\varDelta }\newcommand{\gEp}{ E }\newcommand{\gZt}{ Z }\newcommand{\gEt}{ H }\newcommand{\gTh}{\varTheta }\newcommand{\gIo}{ I }\newcommand{\gKp}{ K }\newcommand{\gLm}{\varLambda }\newcommand{\gMu}{ M }\newcommand{\gNu}{ N }\newcommand{\gXi}{\varXi }\newcommand{\gOm}{ O }\newcommand{\gPi}{\varPi }\newcommand{\gRh}{ P }\newcommand{\gSg}{\varSigma }\newcommand{\gTa}{ T }\newcommand{\gUp}{\varUpsilon}\newcommand{\gPh}{\varPhi }\newcommand{\gCh}{ X }\newcommand{\gPs}{\varPsi }\newcommand{\gOM}{\varOmega }\newcommand{\gKs}{\varXi }

\newcommand{\wsin}{\spc{\sin}{\cos}}\newcommand{\wcos}{\spc{\cos}{\cos}}\newcommand{\wtan}{\spc{\tan}{\cos}}

\newcommand{\csin}{\spc{{\color{ak}\sin}}{\cos}}\newcommand{\ccos}{\spc{{\color{ao}\cos}}{\cos}}\newcommand{\ctan}{\spc{{\color{md}\tan}}{\cos}}\newcommand{\ci}{\clr[ak]{\bm i}} % i

\newcommand{\tri}{\textrm{tri}}\newcommand{\ctri}{\clr[mr]{\tri}}\newcommand{\cpm}{\clr[mr]{\pm}}\newcommand{\cmp}{\clr[mr]{\mp}}

\def\u#1{{%

	\def\O{\textrm{O}}%
	\def\u{\textrm{u}}%
	\mathcode`\u=\mu
	\mathcode`\O=\Omega

\rm #1}}

\newcommand{\overparenthesis}[2][3pt]%{\mathop{\,\vbox{%

 \baselineskip0ex\lineskip#1\ialign{##%
   \crcr{\downparenthfill}%
   \crcr{$\!\displaystyle{#2}\!$}%
   \crcr%
 }%

}\,}\limits}%\newcommand{\underparenthesis}[2][3.5pt]%{\mathop{\,\vtop{%

 \baselineskip0ex\lineskip#1\ialign{##%
   \crcr{$\!\displaystyle{#2}\!$}%
   \crcr{\upparenthfill}%
   \crcr%
 }%

}\,}\limits}%\newcommand{\overbracket}[2][3pt]%{\mathop{\,\vbox{%

 \baselineskip0ex\lineskip#1\ialign{##%
   \crcr{\downbracketfill}%
   \crcr{$\!\displaystyle{#2}\!$}%
   \crcr%
 }%

}\,}\limits}%\newcommand{\underbracket}[2][3.5pt]%{\mathop{\,\vtop{%

 \baselineskip0ex\lineskip#1\ialign{##%
   \crcr{$\!\displaystyle{#2}\!$}%
   \crcr{\upbracketfill}%
   \crcr%
 }%

}\,}\limits}%

\def\downparenthfill{$\m@th\braceld\leaders\vrule\hfill\bracerd$}

\def\upparenthfill{$\m@th\bracelu\leaders\vrule\hfill\braceru$}

\def\upbracketfill{$\m@th\makesm@sh{\llap{\vrule\@height3\p@\@width.7\p@}}%

 \leaders\vrule\@height.7\p@\hfill
 \makesm@sh{\rlap{\vrule\@height3\p@\@width.7\p@}}$}

\def\downbracketfill{$\m@th

 \makesm@sh{\llap{\vrule\@height.7\p@\@depth2.3\p@\@width.7\p@}}%
 \leaders\vrule\@height.7\p@\hfill
 \makesm@sh{\rlap{\vrule\@height.7\p@\@depth2.3\p@\@width.7\p@}}$}

#code(){{{{{{{{{{{{{{{{

#spandel

#spanend