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Display information for equation id:math.2033.66 on revision:2033

* Page found: Vektorfelder als dynamische Systeme (eq math.2033.66)

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\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}^{-\gamma +\sqrt{{{\omega }^{2}}+{{\gamma }^{2}}}t}}+{{c}_{2}}{{{\bar{\xi }}}^{(2)}}{{e}^{-\gamma -\sqrt{{{\omega }^{2}}+{{\gamma }^{2}}}t}} \right)=\infty

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lim t → ∞ ⁢ δ ⁢ x ¯ ⁢ ( t ) = lim t → ∞ ⁢ ( c 1 ⁢ ξ ¯ ( 1 ) ⁢ e - γ + ω 2 + γ 2 ⁢ t + c 2 ⁢ ξ ¯ ( 2 ) ⁢ e - γ - ω 2 + γ 2 ⁢ t ) = ∞ → 𝑡 𝛿 ¯ 𝑥 𝑡 → 𝑡 subscript 𝑐 1 superscript ¯ 𝜉 1 superscript 𝑒 𝛾 superscript 𝜔 2 superscript 𝛾 2 𝑡 subscript 𝑐 2 superscript ¯ 𝜉 2 superscript 𝑒 𝛾 superscript 𝜔 2 superscript 𝛾 2 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}^{-\gamma+\sqrt{{{\omega}^% {2}}+{{\gamma}^{2}}}t}}+{{c}_{2}}{{{\bar{\xi}}}^{(2)}}{{e}^{-\gamma-\sqrt{{{% \omega}^{2}}+{{\gamma}^{2}}}t}}\right)=\infty}}

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limt→∞δx¯(t)=limt→∞(c1ξ¯(1)e−γ+ω2+γ2t+c2ξ¯(2)e−γ−ω2+γ2t)=∞

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