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Question: A body of density \[\rho \] is dropped from rest from a height h into a lake of density \[\sigma \le...

A body of density ρ\rho is dropped from rest from a height h into a lake of density σ(σ>ρ)\sigma \left( {\sigma > \rho } \right) the maximum depth the body sinks inside the liquid is (neglect viscous effect of liquid):
(a)hρ/(σρ)\left( a \right)\,\,h\rho /\left( {\sigma - \rho } \right)
(b)hσ/(σρ)\left( b \right)\,\,h\sigma /\left( {\sigma - \rho } \right)
(c)hρ/σ\left( c \right)\,\,h\rho /\sigma
(d)hσ/ρ\left( d \right)\,\,h\sigma /\rho

Explanation

Solution

A body is dropped into a lake so whenever something is dropped in water the buoyant force will come into picture. Buoyant force- it is a force which is exerted on objects when it is submerged in fluids. Now, we have to find out the velocity with which the body will enter into the lake for that we will use the formula 2gh\sqrt {2gh} . After that we just have to make the work done equal to the change in the kinetic energy which is nothing but a concept of conservation of energy.

Complete Step by step solution:
According to the question there is a body with density ρ\rho which is dropped from rest from a height h into a lake of density σ(σ>ρ)\sigma \left( {\sigma > \rho } \right) . We have to find the maximum depth the body sinks inside the liquid.
Okay, let’s suppose the body is dropped from the height hh . So, velocity with which it will touch the surface of the lake will be given by the equation 2gh\sqrt {2gh} .
Now, with the help of energy conservation
The buoyant force will act in the upward direction and the gravity will act in the downward direction and besides this there will be no force which will be acting on the body.
Let buoyant force be FF' and force due to weight be WW and xx be the distance it moves inside the lake volume if the ball is zz .
Now, the work done will be equal to the change in the kinetic energy
(σzg)(x)+ρzg(x)=01/2zρ(2gh)\Rightarrow \left( {\sigma zg} \right)\left( { - x} \right) + \rho zg\left( x \right) = 0 - 1/2z\rho \left( {2gh} \right) and we will name it equation 11
Where σzg\sigma zg is the buoyant force and x - x , is written because it is acting in the opposite direction and
ρzg\rho zg is weight
And the change is ve - ve because at the deepest point body comes to rest
So by solving the equation 11 we will get the value of which is hρ/(σρ)h\rho /(\sigma - \rho )
Hence, the maximum depth to which the body can sink is hρ/(σρ)h\rho /(\sigma - \rho )

Therefore, the option (a)\left( a \right) is correct.

Note: Remember the key formulas like 2gh\sqrt {2gh} and the process we have followed which will be very helpful for future problem solving. Also, these kinds of questions can be very tricky and confusing. So, try to go step by step to get the desired answer without wasting much time and without getting confused in the mid-way of solving the question.