9.8 The Hard-Sphere Gas 431
1
x^1
r
y
2
2
Figure 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 12
1
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.