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(∫
π0∫ 2 π0g(v)v^2 sin(θ)dφdθ)
dvg(v)v^2 dv∫π0sin(θ)dθ∫ 2 π0dφ (9.4-3) 4 πv^2 g(v)dvThespeed 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.