9.4 The Distribution of Molecular Speeds 407
Consider a spherical shell of radiusvand thicknessdvas shown in Figure 9.11. This
shell contains all of the points in velocity space that represent speeds betweenvand
v+dv. To find the probability of speeds in this shell we integrate the probability shown
in Eq. (9.4-2) over all values ofθandφfor fixed values ofvanddv:
(
probability that
vlies indv
)
fv(v)dv
(∫
π
0
∫ 2 π
0
g(v)v^2 sin(θ)dφdθ
)
dv
g(v)v^2 dv
∫π
0
sin(θ)dθ
∫ 2 π
0
dφ (9.4-3)
4 πv^2 g(v)dv
Thespeed probability distributionor probability density (probability per unit length
on the speed axis) is denoted byfv:
fv(v) 4 πv^2 g(v) 4 πv^2
(
m
2 πkBT
) 3 / 2
e−mv
(^2) / 2 kBT
(9.4-4)
Exercise 9.12
a.Argue that whileφranges from 0 to 2π,θranges only from 0 toπto cover all possible angles.
b.Carry out the integrals in Eq. (9.4-3) that lead to the factor 4πin Eq. (9.4-3).
vx
vz
dv
v
vy
Figure 9.11 A Spherical Shell of Thicknessdvin Velocity Space.