Kinetic Theory of Gases: Application Problems (5)

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Question

Calculate the rms speed of nitrogen molecules (M=28 g/molM = 28\text{ g/mol}) at T=300 KT = 300\text{ K}. Take R=8.314 J/(mol⋅K)R = 8.314\text{ J/(mol·K)}.

Solution — Step by Step

From kinetic theory:

vrms=3RTMv_{\text{rms}} = \sqrt{\frac{3RT}{M}}

Here MM must be in kg/mol\text{kg/mol}, not g/mol — a classic units trap.

M=28 g/mol=0.028 kg/molM = 28\text{ g/mol} = 0.028\text{ kg/mol}

vrms=3×8.314×3000.028=7482.60.028=267236v_{\text{rms}} = \sqrt{\frac{3 \times 8.314 \times 300}{0.028}} = \sqrt{\frac{7482.6}{0.028}} = \sqrt{267236}

vrms517 m/sv_{\text{rms}} \approx 517\text{ m/s}

Final answer: vrms517 m/sv_{\text{rms}} \approx 517\text{ m/s}.

Why This Works

The factor of 3 comes from the equipartition theorem: each translational degree of freedom carries 12kBT\frac{1}{2}k_B T of kinetic energy, and there are three translational degrees, so total translational KE per molecule is 32kBT\frac{3}{2}k_B T. Setting this equal to 12mvrms2\frac{1}{2}m v_{\text{rms}}^2 and replacing mm with M/NAM/N_A gives the formula above.

This is why heavier gases (oxygen, argon) move slower at the same temperature than lighter gases (helium, hydrogen). At room temperature, hydrogen molecules zip around at about 1900 m/s1900\text{ m/s}.

Alternative Method

If we don’t have RR, we can use Boltzmann’s constant directly:

vrms=3kBTmv_{\text{rms}} = \sqrt{\frac{3 k_B T}{m}}

where mm is the mass of one molecule. For nitrogen, m=28×1.66×1027 kg=4.65×1026 kgm = 28 \times 1.66 \times 10^{-27}\text{ kg} = 4.65 \times 10^{-26}\text{ kg}. Plug in kB=1.38×1023 J/Kk_B = 1.38 \times 10^{-23}\text{ J/K} — same answer.

Memorise the three speeds in order: vmp:vˉ:vrms=2:8/π:31.41:1.60:1.73v_{\text{mp}} : \bar{v} : v_{\text{rms}} = \sqrt{2} : \sqrt{8/\pi} : \sqrt{3} \approx 1.41 : 1.60 : 1.73 (in units of RT/M\sqrt{RT/M}). Most-probable < average < rms, always.

Common Mistake

Forgetting the kg/mol conversion. Using M=28M = 28 instead of 0.0280.028 gives a speed about 32 times too small. Always sanity-check: gas molecules at room temperature should be a few hundred m/s.

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