A body of density ρ is dropped from rest from a height h into a lake of density σ(σ>ρ) The maximum depth the body sinks inside the liquid is (neglect viscous effect of liquid):
A
hρσ−ρ
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B
hσσ−ρ
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C
hρσ
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D
hσρ
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Solution
The correct option is Ahρσ−ρ Velocity of the ball as it reaches water surface is √2gh Net upward force acting on the body F=σVg−ρVg ⇒ma=σVg−ρVg ⇒(ρV)a=Vg(σ−ρ) ⇒a=g(σ−ρρ) in upward direction lets say it sinks to the depth H, at this instant final velocity becomes v=0, so we have 0=(√2gh)2−2×g(σ−ρρ)×H∵v2=u2+2as ⇒H=(hρσ−ρ)