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If \(p_{j}\) and \(p_{j}'\) are the components of the generalised momenta corresponding to the Lagrangians L and L' respectively, where

\[ L' = L + \frac{d}{dt}F(q_{j}, t), \]

then :

  • A.\(p_{j}' = p_{j}\)
  • B.\(p_{j}' = p_{j} + \frac{\partial F}{\partial q_{j}}\)
  • C.\(p_{j}' = p_{j} + \frac{\partial F}{\partial t}\)
  • D.\(p_{j}' = p_{j} + \frac{d}{dt}\left(\frac{\partial F}{\partial q_{j}}\right)\)

Answer: B

The momenta are related by \(p_{j}' = p_{j} + \frac{\partial F}{\partial q_{j}}\).

Expand the total derivative:

\[ \begin{aligned} \frac{dF}{dt} &= \sum_{k} \frac{\partial F}{\partial q_{k}}\dot{q}_{k} \\ &\quad + \frac{\partial F}{\partial t} \end{aligned} \]

Only the first sum contains the velocities, and it is linear in them, so

\[ \begin{aligned} p_{j}' &= \frac{\partial L'}{\partial \dot{q}_{j}} \\ &= p_{j} + \frac{\partial F}{\partial q_{j}} \end{aligned} \]

Adding a total time derivative leaves the equations of motion unchanged but shifts the canonical momenta, so \(p_{j}' = p_{j}\) is wrong. \(\partial F / \partial t\) has no velocity dependence and drops out, and option D differentiates once too often.

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