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A particle falls vertically under the action of gravity and a frictional force obtainable from dissipation function \(G(v) = \frac{1}{2}kv^{2}\), k is constant. The Lagrange's equation of motion is :

  • A.\(m\ddot{y} + k\dot{y} + mg = 0\)
  • B.\(m\ddot{y} - k\dot{y} - mg = 0\)
  • C.\(m\ddot{y} - k\dot{y} + mg = 0\)
  • D.\(m\ddot{y} + mg = 0\)

Answer: A

The equation is \(m\ddot{y} + k\dot{y} + mg = 0\), with y measured upward.

With a dissipation function G, Lagrange's equation becomes

\[ \begin{aligned} &\frac{d}{dt}\frac{\partial L}{\partial \dot{y}} \\ &\quad - \frac{\partial L}{\partial y} + \frac{\partial G}{\partial \dot{y}} = 0 \end{aligned} \]

Taking \(L = \frac{1}{2}m\dot{y}^{2} - mgy\):

\[ \begin{aligned} \frac{d}{dt}(m\dot{y}) + mg + k\dot{y} &= 0 \\ m\ddot{y} + k\dot{y} + mg &= 0 \end{aligned} \]

The friction term \(k\dot{y}\) always opposes the velocity, so it enters with the same sign as \(m\ddot{y}\). Option D omits friction altogether, and options B and C give the friction term the wrong sign, which would make the resisting force speed the particle up.

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