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Display information for equation id:math.2573.28 on revision:2573

* Page found: Spezifische Wärme zweiatomiger idealer Gase (eq math.2573.28)

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\begin{align}

& {{Z}_{r}}\approx 1+3\exp \left( -\frac{2{{\Theta }_{r}}}{T} \right) \\

& \ln {{Z}_{r}}\approx 3\exp \left( -\frac{2{{\Theta }_{r}}}{T} \right) \\

& \Rightarrow {{U}_{r}}\approx Nk{{T}^{2}}\frac{\partial }{\partial T}\left( 3\exp \left( -\frac{2{{\Theta }_{r}}}{T} \right) \right)=6Nk{{\Theta }_{r}}\left( \exp \left( -\frac{2{{\Theta }_{r}}}{T} \right) \right) \\

& \Rightarrow {{c}_{vr}}=12R{{\left( \frac{{{\Theta }_{r}}}{T} \right)}^{2}}\exp \left( -\frac{2{{\Theta }_{r}}}{T} \right) \\

\end{align}

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Zr1+3exp(2ΘrT)lnZr3exp(2ΘrT)UrNkT2T(3exp(2ΘrT))=6NkΘr(exp(2ΘrT))cvr=12R(ΘrT)2exp(2ΘrT)
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