Pages

News: Currently the LaTeX and hidden solutions on this blog do not work on Google Reader.
Email me if you have suggestions on how to improve this blog!

Thursday, 11 August 2011

Physics GRE - #10

If $\frac{\partial L}{\partial q_n}=0$, where $L$ is the Lagrangian for a conservative system without constraints and $q_n$ is a generalized coordinate, then the generalized momentum $p_n$ is:

  • an ignorable coordinate
  • constant
  • undefined
  • equal to $\frac{d}{dt}\left(\frac{\partial L}{\partial q_n}\right)$
  • equal to the Hamiltonian for the system

Solution :

The generalized momentum is constant.
Recall that the generalized momentum $p_n$ is \[p_n=\frac{\partial L}{\partial \dot{q_n}}.\]
By the Euler-Lagrange equation, \[\frac{d}{dt}\left(\frac{\partial L}{\partial \dot{q_n}}\right) = \frac{\partial L}{\partial q_n}.\]
Therefore,  \[\frac{\partial L}{\partial q_n}=0\implies\frac{d}{dt}\left(\frac{\partial L}{\partial\dot{q_n}}\right) = 0 \implies \frac{\partial L}{\partial\dot{q_n}} = p_n = const.\]

0 comments:

Post a Comment

This webpage is LaTeX enabled. To type in-line formulae, type your stuff between two '$'. To type centred formulae, type '\[' at the beginning of your formula and '\]' at the end.