4.3 Solutions 263
mu−
(
d
dz
mu
)
rcosθ
Let dnbe the number of molecules with velocity betweenνandν+dν
per unit volume. The number of molecules with velocityνandν+dνin the
volume element dνis dndν. Molecules within the volume element undergo
collisions and are scattered in various directions.
Fig. 4.2Transport of
momentum of gas molecules
Number of collisions that occur in dVin time dtwill be^12 νλdt. The fac-
tor^12 is introduced to avoid counting each collision twice, since the collision
between molecules 1 and 2 and that between 2 and 1 is same.
Each collision results in two new paths for the scattered molecules. Hence
the number of molecules that are scattered in various directions from this vol-
ume element dVin time dtwill be 2×^12 νλdt×dndVorνλdtdndV.
Now the solid angle subtended by dAof the reference plane at dV is
dAcosθ/r^2.
Assuming the scattering to be isotropic the number of molecules moving
downward toward dAis
ν
λ
dtdndVdAcosθ
4 πr^2
or
νdtdn(2πr^2 sinθdθdr)dAcosθ
λ. 4 πr^2
or
νdtdndAsinθcosθ
2 λ
Transport of momentum downward from molecules in the upper hemi-
sphere through dAin time dtis