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Display information for equation id:math.2547.32 on revision:2547

* Page found: Das ideale Fermigas (eq math.2547.32)

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Hash: f3beea3317644b6a0352a12f69b0f484

TeX (original user input): 

\begin{align}

& \ln Y=\frac{2}{3}\beta \sum\limits_{j=1}^{l}{{}}\left\langle {{N}_{j}} \right\rangle {{E}_{j}}=\frac{2}{3}\beta U \\

& U=\left\langle {{E}^{ges.}} \right\rangle  \\

\end{align}

TeX (checked): 

{\begin{aligned}&\ln Y={\frac {2}{3}}\beta \sum \limits _{j=1}^{l}{}\left\langle {{N}_{j}}\right\rangle {{E}_{j}}={\frac {2}{3}}\beta U\\&U=\left\langle {{E}^{ges.}}\right\rangle \\\end{aligned}}

LaTeXML (experimentell; verwendet MathML) rendering

MathML (13.801 KB / 1.928 KB) :

ln ⁡ Y = 2 3 ⁢ β ⁢ ∑ j = 1 l ⟨ N j ⟩ ⁢ E j = 2 3 ⁢ β ⁢ U U = ⟨ E g e s . ⟩ absent 𝑌 2 3 𝛽 superscript subscript 𝑗 1 𝑙 delimited-⟨⟩ subscript 𝑁 𝑗 subscript 𝐸 𝑗 2 3 𝛽 𝑈 absent 𝑈 delimited-⟨⟩ superscript 𝐸 fragments g e s . {\displaystyle{\displaystyle\begin{aligned} \par&\displaystyle\ln Y=\frac{2}{3% }\beta\sum\limits_{j=1}^{l}{{}}\left\langle{{N}_{j}}\right\rangle{{E}_{j}}=% \frac{2}{3}\beta U\\ \par&\displaystyle U=\left\langle{{E}^{ges.}}\right\rangle\\ \par\end{aligned}}}

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MathML (experimentell; keine Bilder) rendering

MathML (1.611 KB / 431 B) :

ln⁡Y=23β∑j=1l⟨Nj⟩Ej=23βUU=⟨Eges.⟩

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