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A fluid is in solid body rotation in a cylindrical container of radius \(R\) rotating with an angular velocity \(\boldsymbol{\Omega} = (0, 0, \Omega)\). The circulation per unit area around a circular loop in the horizontal plane of radius \(r\) (\(r \lt R\)), whose center coincides with the axis of rotation is

  • A.\(2\Omega\)
  • B.\(\Omega^{2}\)
  • C.\(\Omega/2\)
  • D.\(\Omega/4\)

Answer: A

The circulation per unit area is \(2\Omega\).

In solid body rotation the speed at radius r is \(v = \Omega r\). Around the circle of radius r:

\[ \begin{aligned} \Gamma &= \oint \mathbf{v}\cdot d\mathbf{l} = \Omega r \cdot 2\pi r = 2\pi\Omega r^{2} \\ \frac{\Gamma}{\pi r^{2}} &= 2\Omega \end{aligned} \]

This is the vorticity of solid body rotation, twice the angular velocity (Stokes' theorem). \(\Omega/2\) and \(\Omega/4\) divide instead of multiply, and \(\Omega^{2}\) has the wrong dimensions for a vorticity.

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