Derivative of Action Integral Equals Generalized Momentum?

In summary, the conversation discusses finding the partial derivative of the action S with respect to the generalized coordinate q(tf). It is stated that the textbook solution is equal to the generalized momentum p(tf). The approach taken involves taking the partial derivative of both sides and using the fact that qi = 0. The final solution is given as p(tf) - p(ti), which is a momentum quantity. It is noted that this may not always be the case, as p(ti) and q(ti) could potentially be non-zero due to a change of coordinates.
  • #1
shinobi20
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Homework Statement


I need to find the partial derivative of the action S with respect to the generalized coordinate q(tf) and according to my textbook, it should equal the generalized momentum p(tf). How can I derive this?

Homework Equations


S = integral of L dt, with boundary ti to tf. (ti and tf are initial and final times)
qi = 0 (initial generalized coordinate)

The Attempt at a Solution


I took the partial derivative of both sides with respect to the generalized coordinate q, so the right side will have partial L partial q (which is equal to (p dot)) so I'm left with integral of (p dot) dt, but this is simple p(tf) - p(ti). Since qi = 0, p(ti) = 0. Hence partial S partial q(tf) = p(tf).

Is this a possible solution? I have also uploaded my solution. Thanks.
 

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  • #2
I think you can stop and declare victory as soon as you get to ##p(t_f)-p(t_i)##. That's a momentum quantity, which is all that's needed.

It is not necessarily the case that ##p(t_i)=0## or that ##q(t_i)=0##. Even if they were, a change of coordinates such as a shift of origin and/or a velocity boost could render them nonzero.
 
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