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Display information for equation id:math.2174.31 on revision:2174

* Page found: Transformationsverhalten der Ströme und Felder (eq math.2174.31)

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Hash: fa2d7f28a2b811dc3c5663b732d207b3

TeX (original user input):

{{U}^{i}}_{k}=\left( \begin{matrix}
\frac{1}{\sqrt{1-{{\beta }^{2}}}} & \frac{-\beta }{\sqrt{1-{{\beta }^{2}}}} & 0 & 0  \\
\frac{-\beta }{\sqrt{1-{{\beta }^{2}}}} & \frac{1}{\sqrt{1-{{\beta }^{2}}}} & 0 & 0  \\
0 & 0 & 1 & 0  \\
0 & 0 & 0 & 1  \\
\end{matrix} \right)

LaTeXML (experimentell; verwendet MathML) rendering

MathML (16.329 KB / 1.856 KB) :

U i k = ( 1 1 - β 2 - β 1 - β 2 0 0 - β 1 - β 2 1 1 - β 2 0 0 0 0 1 0 0 0 0 1 ) subscript superscript 𝑈 𝑖 𝑘 1 1 superscript 𝛽 2 𝛽 1 superscript 𝛽 2 0 0 𝛽 1 superscript 𝛽 2 1 1 superscript 𝛽 2 0 0 0 0 1 0 0 0 0 1 {\displaystyle{\displaystyle{{U}^{i}}_{k}=\left(\begin{matrix}\frac{1}{\sqrt{1% -{{\beta}^{2}}}}&\frac{-\beta}{\sqrt{1-{{\beta}^{2}}}}&0&0\\ \frac{-\beta}{\sqrt{1-{{\beta}^{2}}}}&\frac{1}{\sqrt{1-{{\beta}^{2}}}}&0&0\\ 0&0&1&0\\ 0&0&0&1\\ \end{matrix}\right)}}

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MathML (experimentell; keine Bilder) rendering

MathML (2.258 KB / 379 B) :

Uik=(11β2β1β200β1β211β20000100001)

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