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Physics · Ch 9 — Kinetic Theory of Gases

Maxwell-Boltzmann Speed Distribution Function

9.2.8

Maxwell-Boltzmann Speed Distribution Function

Why a distribution function is needed. Even though macroscopic quantities like temperature and pressure are fixed for a gas sample, individual molecules are constantly colliding and exchanging speed with one another, so no single molecule keeps the same speed for long. What genuinely stays fixed, once the gas reaches thermal equilibrium, is the number of molecules whose speed falls within any given range -- if one molecule slows down in a collision, some other molecule speeds up to compensate, so the overall population count in each speed range stays steady. The Maxwell-Boltzmann speed distribution function is the formula that gives this steady population count.

The distribution function. The number of molecules dNvdN_v whose speed lies between vv and v+dvv+dv, out of a total of NN molecules, is given by

dNvdv=4πN(m2πkT)3/2v2 e−mv2/2kT.(9.24)\frac{dN_v}{dv} = 4\pi N\left(\frac{m}{2\pi kT}\right)^{3/2} v^2\, e^{-mv^2/2kT}. \qquad (9.24)

Graphically (Figure 9.3), this function starts at zero, rises, reaches a single peak at the most probable speed vmpv_{mp}, and then falls back toward zero at very high speeds; the area of a thin vertical strip of width dvdv under the curve at speed vv equals exactly Nv dvN_v\,dv, the number of molecules in that narrow speed range. The area under the entire curve equals the total number of molecules NN in the sample.

Shape of the curve. For low speeds, the curve rises roughly as v2v^2 (a parabolic-looking rise), because there are progressively more ways for a molecule's velocity components to combine into a slightly larger speed; but for high speeds, the exponential factor e−mv2/2kTe^{-mv^2/2kT} dominates and forces the curve to fall off sharply. The three characteristic speeds from earlier sections all sit on this one curve, in the fixed order vmp<vˉ<vrmsv_{mp}<\bar v<v_{rms} (Figure 9.3).

Effect of temperature (Figure 9.4). Plotting the distribution at two different temperatures shows that raising the temperature shifts the peak of the curve to the right (toward higher speeds) and flattens/broadens the curve -- meaning the average speed of the molecules increases and the spread of speeds widens. Importantly, the area under both curves stays exactly the same, since it always represents the same fixed total number of molecules; a higher temperature simply redistributes that fixed population toward higher speeds, it never creates or destroys molecules. …

Figure 9.3Maxwell's molecular speed distribution

What this figure shows. A graph plots the number of molecules per unit speed interval, NvN_v, on the vertical axis against speed vv on the horizontal axis. The curve rises from the origin, peaks at a certain speed, and then falls off, and the three characteristic speeds are marked on the horizontal axis in increasing order from left to right: the most probable speed vmpv_{mp} sits exactly at the peak of the curve, the average speed vˉ\bar v sits a little to its right, and the rms speed vrmsv_{rms} sits furthest right of the three. A thin vertical strip of width dvdv is shaded under the curve at some speed vv, and its area, Nv dvN_v\,dv, is labelled as exactly …

Figure 9.4Maxwell distribution graph for two different temperatures

What this figure shows. Two speed-distribution curves are drawn on the same axes, one for a lower temperature and one for a higher temperature. The higher-temperature curve has its peak shifted noticeably to the right (toward higher speeds) compared with the lower-temperature curve, and it is visibly flatter and more spread out, while the lower-temperature curve is taller and narrower with its peak closer to the origin. Both curves enclose exactly the same area underneath them, since that area represents the same fixed total number of gas molecules in the sample regardless of temperature -- only how those molecules are spread across diffe …