MCQMediumJEE 2025Viscosity & Stoke's Law

JEE Physics 2025 Question with Solution

A small rigid spherical ball of mass MM is dropped in a long vertical tube containing glycerine. The velocity of the ball becomes constant after some time. If the density of glycerine is half of the density of the ball, then the viscous force acting on the ball will be (consider gg as acceleration due to gravity):

  • A

    2Mg2Mg

  • B

    MgMg

  • C

    Mg2\frac{Mg}{2}

  • D

    3Mg2\frac{3Mg}{2}

Answer

Correct answer:B

Step-by-step solution

Standard Method

Given: A spherical ball of mass MM falls through glycerine and attains terminal velocity. The density of glycerine is half the density of the ball.

Find: The viscous force acting on the ball at terminal velocity.

At terminal velocity, the net force on the ball is zero. The forces acting are:

  • Weight MgMg downward
  • Buoyant force FbF_b upward
  • Viscous force FvF_v upward

So the force balance is

Mg=Fb+FvMg = F_b + F_v

Let the density of the ball be ρb\rho_b and the density of glycerine be ρf\rho_f. Then

M=VρbM = V\rho_b

and the buoyant force is

Fb=VρfgF_b = V\rho_f g

Hence,

Vρbg=Vρfg+FvV\rho_b g = V\rho_f g + F_v

so

Fv=Vg(ρbρf)F_v = Vg(\rho_b - \rho_f)

Given

ρf=ρb2\rho_f = \frac{\rho_b}{2}

therefore

Fv=Vg(ρbρb2)=12VρbgF_v = Vg\left(\rho_b - \frac{\rho_b}{2}\right) = \frac{1}{2}V\rho_b g

Using M=VρbM = V\rho_b,

Fv=12MgF_v = \frac{1}{2}Mg

Therefore, the viscous force acting on the ball is Mg2\frac{Mg}{2}. This corresponds to option C.

The solution also shows option B, but the force balance including buoyancy gives Mg2\frac{Mg}{2}, so there is a discrepancy in the source solution.

Why the listed answer is inconsistent

The first approach on the solution states that at terminal velocity the viscous drag equals the weight of the ball, that is,

Fd=MgF_d = Mg

but this ignores the buoyant force exerted by glycerine.

For a body moving in a fluid, terminal velocity means total upward force equals total downward force, not drag alone equals weight. Thus,

Mg=Fb+FvMg = F_b + F_v

not

Mg=FvMg = F_v

Since the fluid density is half the ball density,

Fb=Vρfg=V(ρb2)g=12Vρbg=Mg2F_b = V\rho_f g = V\left(\frac{\rho_b}{2}\right)g = \frac{1}{2}V\rho_b g = \frac{Mg}{2}

Therefore,

Fv=MgFb=MgMg2=Mg2F_v = Mg - F_b = Mg - \frac{Mg}{2} = \frac{Mg}{2}

So the physically correct answer is option C, even though the source marks B.

Common mistakes

  • Assuming that at terminal velocity the viscous force alone equals the weight. This is wrong because buoyant force also acts upward. Use Mg=Fb+FvMg = F_b + F_v, not Mg=FvMg = F_v.

  • Using the density condition incorrectly. If glycerine has half the density of the ball, then ρf=ρb2\rho_f = \frac{\rho_b}{2}. Substituting this carefully is necessary to compute the buoyant force.

  • Applying Stokes' law directly to identify the answer without checking force balance. Stokes' law gives the form of drag, but the required value here comes from equilibrium of forces at terminal velocity.

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