Example 9.3
Verify that the rms speed of an ideal-gas molecule is about 9 percent greater than its average speed.
Solution
Equation (9.14) gives the number of molecules with speeds between and din a sample
of Nmolecules. To find their average speed , we multiply n()dby , integrate over all values
of from 0 to , and then divide by N. (See the discussion of expectation values in Sec. 5.5.)
This procedure gives
n() d 4 3 2
^3 em^2 ^2 kTdIf we let a m 2 kT, we see that the integral is the standard one
0x^3 eax2
dxand so
4
3 2
2
Comparing with rmsfrom Eq. (9.15) shows thatrms 1.09
Because the speed distribution of Eq. (9.14) is not symmetrical, the most probable
speed pis smaller than either or rms. To find p, we set equal to zero the derivative
of n() with respect to and solve the resulting equation for . The result isp (9.16)
^2 kT
mMost probable
speed3
83 kT
m8 kT
m2 kT
m1
2m
2 kT1
2 a^2m
2 kT1
N304 Chapter Nine
Figure 9.3Maxwell-Boltzmann speed distribution.v^2 = root-mean-square speed = 3kT/mvp = most probable speed = 2kT/mv = average speed = 8kT/πmvn(v)bei48482_Ch09.qxd 1/22/02 8:45 PM Page 304