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A particle of mass m is constrained to move on the arc of a parabola \(x^{2} = 4ay\), where y is vertical axis, under gravity. Then the canonical momentum is given by :

  • A.\(m\dot{x}\)
  • B.\(m(\dot{x} - 2a\dot{y})\)
  • C.\(mx\left(\frac{\dot{x}^{2}}{4a^{2}}\right)\)
  • D.\(m\dot{x}\left(1 + \frac{x^{2}}{4a^{2}}\right)\)

Answer: D

The canonical momentum is \(m\dot{x}\left(1 + \frac{x^{2}}{4a^{2}}\right)\).

On \(x^{2} = 4ay\), \(y = \frac{x^{2}}{4a}\) and \(\dot{y} = \frac{x\dot{x}}{2a}\). With x as the generalised coordinate,

\[ \begin{aligned} L &= \tfrac{1}{2}m\left(\dot{x}^{2} + \tfrac{x^{2}\dot{x}^{2}}{4a^{2}}\right) - mg\tfrac{x^{2}}{4a} \\ p_{x} &= \frac{\partial L}{\partial \dot{x}} = m\dot{x}\left(1 + \frac{x^{2}}{4a^{2}}\right) \end{aligned} \]

\(m\dot{x}\) ignores the vertical motion forced by the constraint. Option B keeps \(\dot{y}\) as if it were independent, and option C is not even linear in \(\dot{x}\).

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