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8.3: Varying Both Ends

  • Page ID
    29578
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    The argument given above for the incremental change in action from varying the endpoint is clearly equally valid for varying the beginning point of the integral (there will be a sign change, of course), so

    \begin{equation}
    d S\left(q_{i}^{(2)}, t_{2}, q_{i}^{(1)}, \quad t_{1}\right)=\sum_{i} p_{i}^{(2)} d q_{i}^{(2)}-H^{(2)} d t_{2}-\sum_{i} p_{i}^{(1)} d q_{i}^{(1)}+H^{(1)} d t_{1}
    \end{equation}

    The initial and final coordinates and times specify the action and the time development of the system uniquely.

    (Note: We’ll find this equation again in the section on canonical transformations -- the action will be seen there to be the generating function of the time-development canonical transformation, this will become clear when we get to it.)


    This page titled 8.3: Varying Both Ends is shared under a not declared license and was authored, remixed, and/or curated by Michael Fowler.

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