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Heat and Thermodynamics question

2019 · 10 Apr · Shift 1 · Q65
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Heat and Thermodynamics question

2019 · 10 Apr · Shift 1 · Q65

JEE MainPhysicsHeat and ThermodynamicsMCQ+4 / −1
A 25 × 10–3 m3 volume cylinder is filled with 1 mol of O2 gas at room temperature (300K). The molecular diameter of O2, and its root mean square speed, are found to be 0.3 nm, and 200 m/s, respectively. What is the average collision rate (per second) for an O2 molecule ?
  1. A
    ~1013
  2. B
    ~1012
  3. C
    ~1011
  4. D
    ~1010
View written solutionFree

Correct answer: D

  1. Use the mean collision rate formula

For a gas molecule, the average collision rate is

z=vˉλz = \frac{\bar v}{\lambda}z=λvˉ​

where λ\lambdaλ is the mean free path.

For hard-sphere molecules,

λ=12 πd2n\lambda = \frac{1}{\sqrt{2}\,\pi d^2 n}λ=2​πd2n1​

So,

z=vˉ 2 πd2nz = \bar v\,\sqrt{2}\,\pi d^2 nz=vˉ2​πd2n

Here:

  • molecular diameter: d=0.3 nm=0.3×10−9 m=3×10−10 md = 0.3\,\text{nm} = 0.3 \times 10^{-9}\,\text{m} = 3 \times 10^{-10}\,\text{m}d=0.3nm=0.3×10−9m=3×10−10m
  • volume: V=25×10−3 m3V = 25 \times 10^{-3}\,\text{m}^3V=25×10−3m3
  • number of molecules in 111 mol: N=NA=6.022×1023N = N_A = 6.022 \times 10^{23}N=NA​=6.022×1023
  • number density:
n=NV=6.022×102325×10−3n = \frac{N}{V} = \frac{6.022 \times 10^{23}}{25 \times 10^{-3}}n=VN​=25×10−36.022×1023​
  1. Compute number density
n=6.022×10232.5×10−2=2.41×1025 m−3n = \frac{6.022 \times 10^{23}}{2.5 \times 10^{-2}} = 2.41 \times 10^{25}\,\text{m}^{-3}n=2.5×10−26.022×1023​=2.41×1025m−3
  1. Compute collision cross-sectional factor
d2=(3×10−10)2=9×10−20 m2d^2 = (3 \times 10^{-10})^2 = 9 \times 10^{-20}\,\text{m}^2d2=(3×10−10)2=9×10−20m2

Then,

πd2n=π×9×10−20×2.41×1025\pi d^2 n = \pi \times 9 \times 10^{-20} \times 2.41 \times 10^{25}πd2n=π×9×10−20×2.41×1025 =π×21.69×105approx6.81×106= \pi \times 21.69 \times 10^5 approx 6.81 \times 10^6=π×21.69×105approx6.81×106

Now multiply by 2\sqrt{2}2​:

2 πd2n≈1.414×6.81×106≈9.63×106\sqrt{2}\,\pi d^2 n \approx 1.414 \times 6.81 \times 10^6 \approx 9.63 \times 10^62​πd2n≈1.414×6.81×106≈9.63×106
  1. Collision rate using the given speed

The question gives rms speed vrms=200 m/sv_{\text{rms}} = 200\,\text{m/s}vrms​=200m/s. Taking this as the characteristic speed,

z≈vrms 2 πd2nz \approx v_{\text{rms}}\,\sqrt{2}\,\pi d^2 nz≈vrms​2​πd2n z≈200×9.63×106=1.93×109 s−1z \approx 200 \times 9.63 \times 10^6 = 1.93 \times 10^9\,\text{s}^{-1}z≈200×9.63×106=1.93×109s−1

This is of order

109 to 1010 s−1\boxed{10^9 \text{ to } 10^{10}\,\text{s}^{-1}}109 to 1010s−1​

So the nearest option is D.

  1. Check via mean free path
λ=19.63×106≈1.04×10−7 m\lambda = \frac{1}{9.63 \times 10^6} \approx 1.04 \times 10^{-7}\,\text{m}λ=9.63×1061​≈1.04×10−7m

Then,

z=2001.04×10−7≈1.92×109 s−1z = \frac{200}{1.04 \times 10^{-7}} \approx 1.92 \times 10^9\,\text{s}^{-1}z=1.04×10−7200​≈1.92×109s−1

Same result.

  1. Comparison with stored answer

Stored correct answer is B (∼1012\sim 10^{12}∼1012), but the calculation from the given data gives a value near 10910^{9}109–101010^{10}1010, so the nearest option is D.

Hence, I do not agree with the stored answer.

A likely issue is that either:

  • the given molecular speed should have been much larger (realistic rms speed for O2\mathrm{O_2}O2​ at 300 K300\,\text{K}300K is about ∼500 m/s\sim 500\,\text{m/s}∼500m/s, still giving only order 101010^{10}1010), or
  • some data/options were intended differently.

Using the given numbers consistently, the answer is D.

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