Question

Difficulty: Very hardKinetic Theory of Matter and Pressure of Gases

Match each kinetic theory concept or microscopic property of an ideal gas on the left with its corresponding mathematical expression or derivation result on the right.

  • Magnitude of momentum change (Δpx)(\Delta p_x) for a gas molecule of mass mm colliding elastically with a container wall perpendicular to the x-axis at speed vxv_x2mvx2 m v_x
  • Average force (Fx)(F_x) exerted by a single gas molecule moving back and forth between two parallel walls separated by length LLmvx2L\frac{m v_x^2}{L}
  • Translational kinetic energy per unit volume (EkV)\left(\frac{E_k}{V}\right) of an ideal gas operating at pressure PP32P\frac{3}{2} P
  • Root-mean-square speed (vrms)(v_{\text{rms}}) of an ideal gas molecule in terms of molar mass MM, universal gas constant RR, and absolute temperature TT3RTM\sqrt{\frac{3 R T}{M}}

Answer

The correct matches pair the momentum change per collision with 2mvx2 m v_x, the single-molecule average wall force with mvx2L\frac{m v_x^2}{L}, the kinetic energy density with 32P\frac{3}{2} P, and the root-mean-square speed with 3RTM\sqrt{\frac{3 R T}{M}}.
Each kinetic theory quantity is derived directly from fundamental principles of mechanics applied to gas particles. Elastic collision with a wall yields a momentum reversal of magnitude 2mvx2 m v_x. Taking the round-trip collision frequency over length LL yields an average force of mvx2L\frac{m v_x^2}{L}. Linking microscopic kinetic energy density to pressure gives EkV=32P\frac{E_k}{V} = \frac{3}{2} P, and linking pressure to the ideal gas law for one mole yields vrms=3RTMv_{\text{rms}} = \sqrt{\frac{3 R T}{M}}.

Step-by-Step Solution

1
Analyze momentum transfer during elastic collision of a molecule with a wall.
Initial momentum along the x-axis is pi=mvxp_i = m v_x and final momentum after elastic reflection is pf=mvxp_f = -m v_x. The change in momentum is Δpx=pfpi=2mvx\Delta p_x = p_f - p_i = -2 m v_x, which has a magnitude of 2mvx2 m v_x.
Elastic collision conserves kinetic energy and reverses velocity direction perpendicular to the wall.
2
Calculate the time rate of momentum transfer to determine average force.
The round-trip distance between opposite walls separated by length LL is 2L2L, so the time between collisions with the same wall is Δt=2Lvx\Delta t = \frac{2L}{v_x}. The average force is Fx=ΔpΔt=2mvx2L/vx=mvx2LF_x = \frac{\Delta p}{\Delta t} = \frac{2 m v_x}{2L / v_x} = \frac{m v_x^2}{L}.
Newton's second law expresses force as the average rate of change of momentum.
3
Relate total translational kinetic energy density to gas pressure.
From kinetic theory, gas pressure is given by P=13NmVvrms2P = \frac{1}{3} \frac{N m}{V} v_{\text{rms}}^2. Since total kinetic energy Ek=12Nmvrms2E_k = \frac{1}{2} N m v_{\text{rms}}^2, we can express pressure as P=23(EkV)P = \frac{2}{3} \left(\frac{E_k}{V}\right). Rearranging gives energy density EkV=32P\frac{E_k}{V} = \frac{3}{2} P.
Translational kinetic energy density is directly proportional to pressure with a factor of 3/2.
4
Derive the formula for root-mean-square velocity from macroscopic and microscopic gas equations.
Substitute density ρ=MV\rho = \frac{M}{V} (where MM is molar mass) into P=13ρvrms2P = \frac{1}{3} \rho v_{\text{rms}}^2, obtaining P=Mvrms23VP = \frac{M v_{\text{rms}}^2}{3 V}. Since PV=RTP V = R T for one mole of ideal gas, RT=13Mvrms2    vrms=3RTMR T = \frac{1}{3} M v_{\text{rms}}^2 \implies v_{\text{rms}} = \sqrt{\frac{3 R T}{M}}.
Connects microscopic speed distribution parameter with thermodynamic temperature and molar mass.

Key Concept

Kinetic Theory of Matter and Pressure of Gases
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