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Display information for equation id:math.1325.135 on revision:1325

* Page found: Der Hamiltonsche kanonische Formalismus (eq math.1325.135)

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Hash: c75d29133b30b400161196accfcdcb83

TeX (original user input):

\begin{align}
  & H=\frac{{{p}^{2}}}{2m}+\frac{m{{\omega }^{2}}}{2}{{q}^{2}} \\ 
 & {{M}_{1}}(q,Q)=\frac{m\omega }{2}{{q}^{2}}\cot Q \\ 
 & \Rightarrow p=\frac{\partial {{M}_{1}}}{\partial q}=m\omega q\cot Q \\ 
 & P=-\frac{\partial {{M}_{1}}}{\partial Q}=\frac{m\omega }{2}\frac{{{q}^{2}}}{{{\sin }^{2}}Q} \\ 
 & q={{\left( \frac{2}{m\omega }P \right)}^{\frac{1}{2}}}\sin Q \\ 
 & p={{\left( 2m\omega P \right)}^{\frac{1}{2}}}\cos Q \\ 
 &  \\ 
\end{align}

TeX (checked):

{\begin{aligned}&H={\frac {{p}^{2}}{2m}}+{\frac {m{{\omega }^{2}}}{2}}{{q}^{2}}\\&{{M}_{1}}(q,Q)={\frac {m\omega }{2}}{{q}^{2}}\cot Q\\&\Rightarrow p={\frac {\partial {{M}_{1}}}{\partial q}}=m\omega q\cot Q\\&P=-{\frac {\partial {{M}_{1}}}{\partial Q}}={\frac {m\omega }{2}}{\frac {{q}^{2}}{{{\sin }^{2}}Q}}\\&q={{\left({\frac {2}{m\omega }}P\right)}^{\frac {1}{2}}}\sin Q\\&p={{\left(2m\omega P\right)}^{\frac {1}{2}}}\cos Q\\&\\\end{aligned}}

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MathML (3.946 KB / 569 B) :

H=p22m+mω22q2M1(q,Q)=mω2q2cotQp=M1q=mωqcotQP=M1Q=mω2q2sin2Qq=(2mωP)12sinQp=(2mωP)12cosQ
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