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Display information for equation id:math.2033.40 on revision:2033

* Page found: Vektorfelder als dynamische Systeme (eq math.2033.40)

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TeX (original user input): 

\begin{matrix}
   \lim   \\
   t\to \infty   \\
\end{matrix}\delta \bar{x}(t)=\begin{matrix}
   \lim   \\
   t\to \infty   \\
\end{matrix}\left( {{c}_{1}}{{{\bar{\xi }}}^{(1)}}{{e}^{\sqrt{\frac{g}{l}}t}}+{{c}_{2}}{{{\bar{\xi }}}^{(2)}}{{e}^{-\sqrt{\frac{g}{l}}t}} \right)=\infty

TeX (checked): 

{\begin{matrix}\lim \\t\to \infty \\\end{matrix}}\delta {\bar {x}}(t)={\begin{matrix}\lim \\t\to \infty \\\end{matrix}}\left({{c}_{1}}{{\bar {\xi }}^{(1)}}{{e}^{{\sqrt {\frac {g}{l}}}t}}+{{c}_{2}}{{\bar {\xi }}^{(2)}}{{e}^{-{\sqrt {\frac {g}{l}}}t}}\right)=\infty

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MathML (16.247 KB / 2.188 KB) :

lim t → ∞ ⁢ δ ⁢ x ¯ ⁢ ( t ) = lim t → ∞ ⁢ ( c 1 ⁢ ξ ¯ ( 1 ) ⁢ e g l ⁢ t + c 2 ⁢ ξ ¯ ( 2 ) ⁢ e - g l ⁢ t ) = ∞ → 𝑡 𝛿 ¯ 𝑥 𝑡 → 𝑡 subscript 𝑐 1 superscript ¯ 𝜉 1 superscript 𝑒 𝑔 𝑙 𝑡 subscript 𝑐 2 superscript ¯ 𝜉 2 superscript 𝑒 𝑔 𝑙 𝑡 {\displaystyle{\displaystyle\begin{matrix}\lim\\ t\to\infty\\ \end{matrix}\delta\bar{x}(t)=\begin{matrix}\lim\\ t\to\infty\\ \end{matrix}\left({{c}_{1}}{{{\bar{\xi}}}^{(1)}}{{e}^{\sqrt{\frac{g}{l}}t}}+{{% c}_{2}}{{{\bar{\xi}}}^{(2)}}{{e}^{-\sqrt{\frac{g}{l}}t}}\right)=\infty}}

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MathML (experimentell; keine Bilder) rendering

MathML (2.286 KB / 457 B) :

limt→∞δx¯(t)=limt→∞(c1ξ¯(1)eglt+c2ξ¯(2)e−glt)=∞

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  • δ
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  • t
  • t
  • c1
  • ξ¯
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  • g
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  • ξ¯
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  • g
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