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MHT CET 2024 (3 May, Shift 2) · Force due to Surface Tension

Force due to Surface Tension question from MHT CET 2024 (3 May, Shift 2)

Q11MHT CET 2024 · 3 MAY · SHIFT 2Difficult

Force due to Surface Tension

A liquid drop of density ' ρ\rho ' is floating half immersed in a liquid of density ' dd '. If ' TT ' is the surface tension then the diameter of the liquid drop is ( g=g = acceleration due to gravity)

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Answer: (c)

  1. Weight = buoyancy + surface tension force along the waterline: 43πr3ρg=23πr3dg+2πrT\frac{4}{3}\pi r^3\rho g = \frac{2}{3}\pi r^3 d g + 2\pi r T.
  2. 23r2g(2ρ−d)=2T⇒r2=3Tg(2ρ−d)\frac{2}{3} r^2 g(2\rho - d) = 2T \Rightarrow r^2 = \dfrac{3T}{g(2\rho - d)}.
  3. Diameter D=2r⇒D2=12Tg(2ρ−d)D = 2r \Rightarrow D^2 = \dfrac{12T}{g(2\rho - d)}.
  4. So the answer is (c) [12Tg(2ρ−d)]1/2\left[\frac{12T}{g(2\rho - d)}\right]^{1/2}.
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