NVAEasyJEE 2023Viscosity & Stoke's Law

JEE Physics 2023 Question with Solution

A spherical ball of radius 1mm1 \, \text{mm} and density 10.5g/cc10.5 \, \text{g/cc} is dropped in glycerine of coefficient of viscosity 9.8poise9.8 \, \text{poise} and density 1.5g/cc1.5 \, \text{g/cc}. Viscous force on the ball when it attains constant velocity is 3696×107N3696 \times 10^{-7} \, \text{N}. The value of xx is:

Answer

Correct answer:7

Step-by-step solution

Standard Method

Given: radius of ball r=1mm=103mr = 1 \, \text{mm} = 10^{-3} \, \text{m}, density of ball ρb=10.5×103kg/m3\rho_b = 10.5 \times 10^3 \, \text{kg/m}^3, density of glycerine ρ=1.5×103kg/m3\rho_\ell = 1.5 \times 10^3 \, \text{kg/m}^3, and the ball attains terminal velocity so a=0a = 0.

Find: the value of xx in the viscous force expression.

At terminal velocity, the net force is zero, so the viscous force balances the effective weight of the ball:

Fv=VρbgVρgF_v = V \rho_b g - V \rho_\ell g

Therefore,

Fv=Vg(ρbρ)F_v = Vg(\rho_b - \rho_\ell)

The volume of the spherical ball is

V=43πr3V = \frac{4}{3}\pi r^3

Substituting,

Fv=43πr3g(ρbρ)F_v = \frac{4}{3}\pi r^3 g(\rho_b - \rho_\ell)

Now put the given values:

Fv=43×227×(103)3×9.8×(10.5×1031.5×103)F_v = \frac{4}{3} \times \frac{22}{7} \times (10^{-3})^3 \times 9.8 \times (10.5 \times 10^3 - 1.5 \times 10^3) Fv=43×227×109×9.8×9×103F_v = \frac{4}{3} \times \frac{22}{7} \times 10^{-9} \times 9.8 \times 9 \times 10^3 Fv=43×227×109×88.2×103F_v = \frac{4}{3} \times \frac{22}{7} \times 10^{-9} \times 88.2 \times 10^3 Fv=3696×107NF_v = 3696 \times 10^{-7} \, \text{N}

Thus, comparing with the given form, the value of xx is 77.

Therefore, the answer is 77.

Force Balance at Terminal Velocity

Given: the ball moves in glycerine and attains constant velocity, which means terminal velocity.

Find: the unknown exponent-related value xx.

When the velocity becomes constant, acceleration is zero. Hence viscous force equals weight minus buoyant force:

Fv=mgFBF_v = mg - F_B

Using mass and buoyancy in terms of volume,

Fv=VρbgVρgF_v = V\rho_b g - V\rho_\ell g Fv=Vg(ρbρ)F_v = Vg(\rho_b - \rho_\ell)

For a sphere,

V=43πr3V = \frac{4}{3}\pi r^3

So,

Fv=43π(103)3×9.8×(10.51.5)×103F_v = \frac{4}{3}\pi (10^{-3})^3 \times 9.8 \times (10.5 - 1.5) \times 10^3 Fv=3696×107NF_v = 3696 \times 10^{-7} \, \text{N}

Hence, x=7x = 7.

The final answer is 77.

Common mistakes

  • Using Stokes' law directly to find force here is unnecessary because the solution already uses force balance at terminal velocity. At terminal velocity, first equate viscous force to effective weight minus buoyancy.

  • Forgetting buoyant force is incorrect because the liquid also exerts an upward force on the ball. Use Fv=Vg(ρbρ)F_v = Vg(\rho_b - \rho_\ell), not only the weight of the ball.

  • Not converting 1mm1 \, \text{mm} to 103m10^{-3} \, \text{m} leads to a large error because volume depends on r3r^3. Convert the radius before substitution.

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