Q2) A block of weight W slides down an inclined plane on a thin film of oil with terminal velocity V, as shown in Figure Q2, and thus a shear stress will be existed (1). The film contact area is A and its thickness h, oil viscosity u and incline angle 0. Assuming a linear velocity distribution in the film, prove that the analytic expression for the terminal velocity can be V=(hWcos®) /Aµ. For both Group 1 and Group 2 W Oil film, thickness h Figure Q2

Elements Of Electromagnetics
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Q2) A block of weight W slides down an inclined plane on a thin film of oil with
terminal velocity V, as shown in Figure Q2, and thus a shear stress will be existed (t).
The film contact area is A and its thickness h, oil viscosity u and incline angle 0.
Assuming a linear velocity distribution in the film, prove that the analytic expression for
the terminal velocity can be V=(hWcos0) /Aµ.
For both Group 1 and Group 2
Oil film,
thickness h
Figure Q2
Transcribed Image Text:Q2) A block of weight W slides down an inclined plane on a thin film of oil with terminal velocity V, as shown in Figure Q2, and thus a shear stress will be existed (t). The film contact area is A and its thickness h, oil viscosity u and incline angle 0. Assuming a linear velocity distribution in the film, prove that the analytic expression for the terminal velocity can be V=(hWcos0) /Aµ. For both Group 1 and Group 2 Oil film, thickness h Figure Q2
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