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An incompressible fluid flows between a pair of infinite plates separated by a distance L. The top plate is moving with a constant velocity U, whereas the bottom plate is stationary, as shown in the figure. The difference of the stream functions \((\psi_{T}-\psi_{B})\) at the two plates for a laminar and fully-developed flow is equal to

A stationary bottom plate with stream function psi B and a top plate a distance L above moving at U with stream function psi T; the velocity profile between them rises linearly from zero to U

  • A.\(\frac{UL}{2}\)
  • B.UL
  • C.2UL
  • D.4UL

Answer: A

The difference is \(\frac{UL}{2}\).

In plane Couette flow with no pressure gradient the profile is linear, \(u = Uy/L\). The difference in stream function between two streamlines equals the volume flow rate per unit width between them:

\[ \begin{aligned} \psi_{T}-\psi_{B} &= \int_{0}^{L}u\,dy \\ &= \int_{0}^{L}\frac{Uy}{L}\,dy = \frac{UL}{2} \end{aligned} \]

Equivalently, the average velocity is U/2 across a gap L. UL would need the whole gap to move at U, and 2UL and 4UL exceed even that.

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