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Display information for equation id:math.2032.44 on revision:2032

* Page found: Vektorfelder als dynamische Systeme (eq math.2032.44)

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Hash: c148413a653029406b5233926dbc825a

TeX (original user input):

\begin{align}
  & \ddot{\phi }+\frac{2\gamma }{m{{l}^{2}}}\dot{\phi }+{{\omega }^{2}}\sin \phi =0 \\
 & {{\omega }^{2}}=\frac{g}{l} \\
\end{align}

TeX (checked):

{\begin{aligned}&{\ddot {\phi }}+{\frac {2\gamma }{m{{l}^{2}}}}{\dot {\phi }}+{{\omega }^{2}}\sin \phi =0\\&{{\omega }^{2}}={\frac {g}{l}}\\\end{aligned}}

LaTeXML (experimentell; verwendet MathML) rendering

MathML (10.44 KB / 1.558 KB) :

ϕ ¨ + 2 γ m l 2 ϕ ˙ + ω 2 sin ϕ = 0 ω 2 = g l missing-subexpression ¨ italic-ϕ 2 𝛾 𝑚 superscript 𝑙 2 ˙ italic-ϕ superscript 𝜔 2 italic-ϕ 0 missing-subexpression superscript 𝜔 2 𝑔 𝑙 {\displaystyle{\displaystyle\begin{aligned} &\displaystyle\ddot{\phi}+\frac{2% \gamma}{m{{l}^{2}}}\dot{\phi}+{{\omega}^{2}}\sin\phi=0\\ &\displaystyle{{\omega}^{2}}=\frac{g}{l}\\ \end{aligned}}}

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MathML (experimentell; keine Bilder) rendering

MathML (1.394 KB / 375 B) :

ϕ¨+2γml2ϕ˙+ω2sinϕ=0ω2=gl

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Identifiers

  • ϕ¨
  • γ
  • m
  • l
  • ϕ˙
  • ω
  • ϕ
  • ω
  • g
  • l

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