MCQMediumJEE 2023Surface Tension & Capillarity

JEE Physics 2023 Question with Solution

A mercury drop of radius 103m10^{-3} \, \text{m} is broken into 125125 equal size droplets. Surface tension of mercury is 0.45N m10.45 \, \text{N m}^{-1}. The gain in surface energy is:

  • A

    2.26×105J2.26 \times 10^{-5} \, \text{J}

  • B

    28×105J28 \times 10^{-5} \, \text{J}

  • C

    17.5×105J17.5 \times 10^{-5} \, \text{J}

  • D

    5×105J5 \times 10^{-5} \, \text{J}

Answer

Correct answer:C

Step-by-step solution

Standard Method

Given: radius of mercury drop R=103mR = 10^{-3} \, \text{m}, number of droplets n=125n = 125, surface tension T=0.45N m1T = 0.45 \, \text{N m}^{-1}.

Find: gain in surface energy after breaking the drop into equal droplets.

Initial surface energy is

Ei=T4πR2E_i = T \cdot 4\pi R^2

So,

Ei=0.45×4π×(103)2E_i = 0.45 \times 4\pi \times (10^{-3})^2

By conservation of volume,

43π(103)3=125×4π3Rnew3\frac{4}{3}\pi (10^{-3})^3 = 125 \times \frac{4\pi}{3} R_{\text{new}}^3

Therefore,

103=5Rnew10^{-3} = 5R_{\text{new}}

Hence,

Rnew=1035mR_{\text{new}} = \frac{10^{-3}}{5} \, \text{m}

Final surface energy is

Ef=0.45×125×4π(1035)2E_f = 0.45 \times 125 \times 4\pi \left(\frac{10^{-3}}{5}\right)^2

Increase in energy is

ΔE=0.45×4π×(103)2[125251]\Delta E = 0.45 \times 4\pi \times (10^{-3})^2 \left[\frac{125}{25} - 1\right] =4×0.45×4π×106= 4 \times 0.45 \times 4\pi \times 10^{-6} =2.26×105J= 2.26 \times 10^{-5} \, \text{J}

Therefore, the gain in surface energy is 2.26×105J2.26 \times 10^{-5} \, \text{J}.

The solution working gives this value, but the solution labels the correct option as C. The numerical value matches option A.

Using surface area increase

Given: one initial drop of radius 103m10^{-3} \, \text{m} is converted into 125125 equal droplets.

Find: change in surface energy.

Surface energy is proportional to surface area:

E=TAE = T A

For the original drop,

Ai=4πR2A_i = 4\pi R^2

For each small drop, radius becomes RnewR_{\text{new}} and total area is

Af=125×4πRnew2A_f = 125 \times 4\pi R_{\text{new}}^2

Using volume conservation,

R3=125Rnew3R^3 = 125R_{\text{new}}^3 Rnew=R5R_{\text{new}} = \frac{R}{5}

Hence,

Af=125×4π(R5)2=5×4πR2A_f = 125 \times 4\pi \left(\frac{R}{5}\right)^2 = 5 \times 4\pi R^2

So the increase in area is

ΔA=AfAi=(51)4πR2=44πR2\Delta A = A_f - A_i = (5-1)4\pi R^2 = 4 \cdot 4\pi R^2

Therefore,

ΔE=TΔA=0.45×4×4π×(103)2\Delta E = T\Delta A = 0.45 \times 4 \times 4\pi \times (10^{-3})^2 =2.26×105J= 2.26 \times 10^{-5} \, \text{J}

Thus the correct numerical result is 2.26×105J2.26 \times 10^{-5} \, \text{J}.

Common mistakes

  • Using surface energy proportional to volume instead of surface area is wrong because surface tension multiplies area, not volume. Always use E=TAE = T A.

  • Equating radii directly after breakup is wrong because volume is conserved, not radius. First write 43πR3=125×43πr3\frac{4}{3}\pi R^3 = 125 \times \frac{4}{3}\pi r^3.

  • Forgetting to subtract the initial surface energy gives final energy instead of gain in energy. Compute ΔE=EfEi\Delta E = E_f - E_i.

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