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Display information for equation id:math.2032.33 on revision:2032

* Page found: Vektorfelder als dynamische Systeme (eq math.2032.33)

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Vektorfelder als dynamische Systeme Eq: math.2033.33

Hash: 8fee8091233c638f015b0faa5d9b1546

TeX (original user input):

\delta \bar{x}(t)=={{c}_{1}}{{\bar{\xi }}^{(1)}}{{e}^{i\omega t}}+{{c}_{2}}{{\bar{\xi }}^{(2)}}{{e}^{-i\omega t}}

TeX (checked):

\delta {\bar {x}}(t)=={{c}_{1}}{{\bar {\xi }}^{(1)}}{{e}^{i\omega t}}+{{c}_{2}}{{\bar {\xi }}^{(2)}}{{e}^{-i\omega t}}

LaTeXML (experimental; uses MathML) rendering

MathML (8.204 KB / 1.379 KB) :

{\displaystyle{\displaystyle\delta\bar{x}(t)=={{c}_{1}}{{\bar{\xi}}^{(1)}}{{e}% ^{i\omega t}}+{{c}_{2}}{{\bar{\xi}}^{(2)}}{{e}^{-i\omega t}}}}

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SVG (0 B / 8 B) :

MathML (experimental; no images) rendering

MathML (1.321 KB / 315 B) :

δ \bar{x} (t) = = c_{1} {\bar{ξ}}^{(1)} e^{i ω t} + c_{2} {\bar{ξ}}^{(2)} e^{- i ω t}

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Translations to Computer Algebra Systems

Translation to Maple

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Translation to Mathematica

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Identifiers

$δ$

$\bar{x}$

$t$

$c_{1}$

$\bar{ξ}$

$e$

$i$

$ω$

$t$

$c_{2}$

$\bar{ξ}$

$e$

$i$

$ω$

$t$

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