A small sphere initially at rest, falls in to a viscous liquid. Due to drag, heat is produced. Then the relation between rate of production of heat and the radius of the sphere at terminal velocity, is best represented by:
A
∝r2
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B
∝r5
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C
∝r6
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D
∝r3
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Solution
The correct option is B∝r5
We have that
Terminal velocity, VT=2r2g9η(ρs−ρL)...(i) r→ radius of sphere g→ acceleration due to gravity y→ coefficient of viscosity ρs→ density of sphere ρL→ density of fluid.
& viscous Force (Drag force): F=6πηrVT...(ii) for [v=VT] ∵rate of production of heatdQdt=Rate of energy production ⇒dQdt=Power(P)
Hence we can write as: P=F×VT P=6πηrVT×VT
Substituting from Eq (i)&(ii), P=6πrη[2r2g9η(ρs−ρL)]2
Or, P=6πηr5[2g9η(ρs−ρL)]2 ∴P∝r5