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Chemical Kinetics and Nuclear Chemistry question

2014 · Shift 2 · Q12
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Chemical Kinetics and Nuclear Chemistry question

2014 · Shift 2 · Q12

JEE AdvancedChemistryChemical Kinetics and Nuclear ChemistryMCQ+3 / −1
X and Y are two volatile liquids with molar weights of 10 g mol −-− 1 and 40 g mol −-− 1, respectively. Two cotton plugs, one soaked in X and the other soaked in Y, are simultaneously placed at the ends of a tube of length L = 24 cm, as shown in the figure. The tube is filled with an inert gas at 1 atmosphere pressure and a temperature of 300 K. Vapours of X and Y react to form a product which is first observed at a distance d cm from the plug soaked in X. Take X and Y to have equal molecular diameters and assume ideal behaviour for the inert gas and the two vapours. JEE Advanced 2014 Paper 2 Offline Chemistry - Chemical Kinetics and Nuclear Chemistry Question 11 English ComprehensionThe experimental value of d is found to be smaller than the estimate obtained using Graham's law. This is due to
  1. A
    larger mean free path for X as compared to that of Y.
  2. B
    larger mean free path for Y as compared to that of X.
  3. C
    increased collision frequency of Y with the inert gas as compared to that of X with the inert gas.
  4. D
    increased collision frequency of X with the inert gas as compared to that of Y with the inert gas.
View written solutionFree

Correct answer: D

  1. What Graham's law would predict

For two gases/vapours diffusing from opposite ends, Graham's law gives

rXrY=MYMX=4010=2.\frac{r_X}{r_Y}=\sqrt{\frac{M_Y}{M_X}}=\sqrt{\frac{40}{10}}=2.rY​rX​​=MX​MY​​​=1040​​=2.

If the first visible product forms where the two fronts meet, then the distances travelled satisfy

dL−d=rXrY=2.\frac{d}{L-d}=\frac{r_X}{r_Y}=2.L−dd​=rY​rX​​=2.

With L=24 cmL=24\,\text{cm}L=24cm,

d24−d=2  ⟹  d=16 cm.\frac{d}{24-d}=2 \implies d=16\,\text{cm}.24−dd​=2⟹d=16cm.

So Graham's law predicts the product should first appear at 16 cm16\,\text{cm}16cm from the plug soaked in XXX.

But experimentally, ddd is smaller than this. That means the product forms closer to the X end than Graham's law predicts. Hence, in reality, XXX diffuses less effectively relative to YYY than Graham's law estimate suggests.


  1. Why Graham's law is not exact here

Graham's law is most appropriate when comparing diffusion/effusion under simplified conditions. Here, both vapours diffuse through an inert gas already present at 1 atm. So each vapour undergoes repeated collisions mainly with inert-gas molecules.

Thus, the relative diffusion is controlled not only by molar masses of XXX and YYY, but also by how frequently each collides with the inert gas.


  1. Compare molecular speeds of X and Y

At the same temperature,

vˉ∝1M.\bar v \propto \frac{1}{\sqrt{M}}.vˉ∝M​1​.

Since

MX=10,MY=40,M_X=10, \qquad M_Y=40,MX​=10,MY​=40,

we have

vˉX>vˉY.\bar v_X > \bar v_Y.vˉX​>vˉY​.

So molecules of XXX move faster and therefore collide more frequently with inert-gas molecules than molecules of YYY do.


  1. Effect on diffusion distance

More frequent collisions with the inert gas hinder the net progress of XXX more strongly. Therefore, compared to the Graham's law estimate, XXX does not advance as far as expected. So the meeting point shifts towards the X end, making ddd smaller.

This matches the observation.


  1. Check options
  • A: larger mean free path for XXX than for YYY
    This would help XXX diffuse farther, making ddd larger, not smaller. Incorrect.

  • B: larger mean free path for YYY than for XXX
    While this could shift the point toward XXX, the more direct kinetic explanation here is collision frequency with inert gas.

  • C: increased collision frequency of YYY with inert gas compared to XXX
    This would hinder YYY more, pushing meeting point away from XXX, so ddd would increase. Incorrect.

  • D: increased collision frequency of XXX with inert gas compared to YYY
    This hinders XXX more, so the product appears closer to the XXX end and ddd becomes smaller. Correct.


  1. Final answer

The correct option is

D\boxed{\text{D}}D​
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