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Display information for equation id:math.1110.105 on revision:1110

* Page found: ART-Skript (eq math.1110.105)

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TeX (original user input):

\begin{align}
  & d{{s}^{2}}={{\eta }_{\mu \nu }}\partial {{'}_{\alpha }}{{x}^{\mu }}\partial {{'}_{\beta }}{{x}^{\nu }}dx{{'}^{\alpha }}dx{{'}^{\beta }} \\
 & =g{{'}_{\mu }}_{\nu }dx{{'}^{\mu }}dx{{'}^{\nu }}
\end{align}

TeX (checked):

{\begin{aligned}&d{{s}^{2}}={{\eta }_{\mu \nu }}\partial {{'}_{\alpha }}{{x}^{\mu }}\partial {{'}_{\beta }}{{x}^{\nu }}dx{{'}^{\alpha }}dx{{'}^{\beta }}\\&=g{{'}_{\mu }}_{\nu }dx{{'}^{\mu }}dx{{'}^{\nu }}\end{aligned}}

LaTeXML (experimentell; verwendet MathML) rendering

MathML (17.072 KB / 2.088 KB) :

d s 2 = η μ ν x μ α x ν β d x d α x β = g ν μ d x d μ x ν missing-subexpression fragments d superscript 𝑠 2 subscript 𝜂 𝜇 𝜈 superscript subscript superscript 𝑥 𝜇 𝛼 superscript subscript superscript 𝑥 𝜈 𝛽 d x superscript superscript 𝑑 𝛼 x superscript superscript absent 𝛽 missing-subexpression fragments g superscript subscript 𝜈 𝜇 d x superscript superscript 𝑑 𝜇 x superscript superscript absent 𝜈 {\displaystyle{\displaystyle\begin{aligned} &\displaystyle d{{s}^{2}}={{\eta}_% {\mu\nu}}\partial{{{}^{\prime}}_{\alpha}}{{x}^{\mu}}\partial{{{}^{\prime}}_{% \beta}}{{x}^{\nu}}dx{{{}^{\prime}}^{\alpha}}dx{{{}^{\prime}}^{\beta}}\\ &\displaystyle=g{{{}^{\prime}}_{\mu}}_{\nu}dx{{{}^{\prime}}^{\mu}}dx{{{}^{% \prime}}^{\nu}}\end{aligned}}}

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MathML (experimentell; keine Bilder) rendering

MathML (1.553 KB / 365 B) :

ds2=ημν'αxμ'βxνdx'αdx'β=g'μνdx'μdx'ν

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