Consider a rectangular block of wood moving with a velocity v0 in gas at temperature T and mass density ρ. Assume the velocity is along the x-axis and the area of cross-section of the block perpendicular to v0 is A. Show that the drag force on the block is 4ρAV0kTm, where m is the mass of the gas molecule.

Hint: The drag force will be equal to the rate of momentum transferred by the gas molecules.
Step 1: Find the momentum transferred by the gas molecules.
Consider the diagram.
 
m= mass of the gas
ρ= density of the gas 
Let n = number of molecules per unit volume
vrms= RMS speed of the gas molecules
When the block is moving with speed v0, the relative speed of molecules w.r.t. front face = v+v0 coming head-on
The momentum transferred to the block per collision =2m(v+v0)
where m=mass of the molecule.
The number of collision in time t=12(v+v0)ntA,
where A = area of cross-section of block and factor of 1/2 appears due to particles moving towards the block.
 the momentum transferred in time t=m(v+v0)2nAt from the front surface.
Similarly, momentum transferred in time t=m(v-v0)2nAt (from the back surface)
Step 2: Find the net darg force.
 Net force drag force = mnA[(v+v0)2-(v-v0)2]                    [from front]
                                  =mnA(4vv0)=(4mnAv)v0
=(4ρAv)v0
where we have assumed, ρ=mNV=MV
If v = velocity along x-axis,
Then, we can write,                   KE=12mv2=12kBT
                     v=kBTm                    KB=Bolzmann constant
KE=Kinetic energy
T=Temperature
 From Eq.(i), Drag force=4ρAkBTmv0