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Heat and Thermodynamics question

2013 · Shift 0 · Q69
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Heat and Thermodynamics question

2013 · Shift 0 · Q69

JEE MainPhysicsHeat and ThermodynamicsMCQ+4 / −1
Assume that a drop of liquid evaporates by decreases in its surface energy, so that its temperature remains unchanged. What should be the minimum radius of the drop for this to be possible ? The surface tension is T,T,T, density of liquid is ρ\rhoρ and LLL is its latent heat of vaporization.
  1. A
    ρL/T\rho L/TρL/T
  2. B
    T/ρL\sqrt {T/\rho L}T/ρL​
  3. C
    T/ρLT/\rho LT/ρL
  4. D
    2T/ρL2T/\rho L2T/ρL
View written solutionFree

Correct answer: D

  1. Idea of the problem

A liquid drop evaporates. If its temperature remains unchanged, then the energy needed for vaporization must come entirely from the decrease in surface energy.

So,

loss in surface energy=latent heat required for evaporated mass\text{loss in surface energy} = \text{latent heat required for evaporated mass}loss in surface energy=latent heat required for evaporated mass

We find the condition for a drop of radius rrr.


  1. Surface energy of the drop

For a spherical drop of radius rrr:

A=4πr2A = 4\pi r^2A=4πr2

Hence surface energy,

U=T⋅4πr2U = T \cdot 4\pi r^2U=T⋅4πr2

where TTT is the surface tension.

If the radius decreases by a small amount drdrdr, then

dU=T d(4πr2)=8πTr drdU = T\,d(4\pi r^2) = 8\pi T r\,drdU=Td(4πr2)=8πTrdr

Since the radius decreases, dr<0dr<0dr<0, so the decrease in surface energy is

−dU=−8πTr dr- dU = -8\pi T r\,dr−dU=−8πTrdr
  1. Mass evaporated when radius decreases by drdrdr

Volume of sphere:

V=43πr3V = \frac{4}{3}\pi r^3V=34​πr3

So,

dV=4πr2drdV = 4\pi r^2 drdV=4πr2dr

Since dr<0dr<0dr<0, the decrease in volume is

−dV=−4πr2dr-dV = -4\pi r^2 dr−dV=−4πr2dr

Hence mass evaporated is

dm=ρ(−dV)=−4πρr2drdm = \rho(-dV)= -4\pi \rho r^2 drdm=ρ(−dV)=−4πρr2dr

Latent heat required for this evaporation:

dQ=L dm=−4πρLr2drdQ = L\,dm = -4\pi \rho L r^2 drdQ=Ldm=−4πρLr2dr
  1. Condition for evaporation using only surface energy

For temperature to remain unchanged, the decrease in surface energy must at least supply the latent heat:

−8πTr dr≥−4πρLr2dr-8\pi T r\,dr \ge -4\pi \rho L r^2 dr−8πTrdr≥−4πρLr2dr

Since −4πr dr>0-4\pi r\,dr >0−4πrdr>0, divide both sides by it:

2T≥ρLr2T \ge \rho L r2T≥ρLr

Thus,

r≤2TρLr \le \frac{2T}{\rho L}r≤ρL2T​

For this to be just possible, the limiting (critical) radius is

rmin⁡/critical=2TρLr_{\min/\text{critical}} = \frac{2T}{\rho L}rmin/critical​=ρL2T​

In the language of the options, the required radius is

2TρL\boxed{\frac{2T}{\rho L}}ρL2T​​
  1. Checking options
  • A: ρLT\dfrac{\rho L}{T}TρL​ — wrong dimensions.
  • B: TρL\sqrt{\dfrac{T}{\rho L}}ρLT​​ — wrong dimensions.
  • C: TρL\dfrac{T}{\rho L}ρLT​ — misses factor 222.
  • D: 2TρL\dfrac{2T}{\rho L}ρL2T​ — correct.

  1. Comparison with stored answer

Stored correct answer: D

Derived answer: D

So they agree.

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