9.8 The Hard-Sphere Gas 431
1
x^1ry22Figure 9.21 An “Average” (Right-Angle) Collision of Two Hard Spheres of Different
Types.separation is given by the theorem of Pythagoras:rtc[
〈v 1 〉^2 +〈v 2 〉^2] 1 / 2
(9.8-25)
We denote themean relative speedby〈v 12 〉:〈vrel〉〈v 12 〉√
〈v 1 〉^2 +〈v 2 〉^2 √
8 kBT
πm 1+
8 kBT
πm 2〈v 12 〉√
8 kBT
πμ 12(9.8-26)
wherem 1 andm 2 are the two molecular masses and whereμ 12 is called thereduced
massof particles 1 and 2:1
μ 121
m 1+
1
m 2(9.8-27)
μ 12 m 1 m 2
m 1 +m 2(9.8-28)
Our derivation is crude, but Eq. (9.8-26) is the correct expression for the mean relative
speed. For a pair of identical particles,μis equal tom/2, so that Eq. (9.8-26) is valid
for that case as well as for two different substances.