00:01
So the average kinetic energy was already given in the problem and it is the expression is integral sum or integral e times density of the states times probability per state and differential the energy over the number of particles per unit volume.
00:30
So here we know that temperature is zero calories.
00:36
Now for f of e will be zero for e larger than firmis energy and it will be one if e is lesser than firmis energy.
00:58
So we also know that we can just express an over me like that but this is actually integration from zero to infinity of the number of particles per energy, well times differential of the energy.
01:18
And of course, further this can be written as g of e, f of e, d .e.
01:28
So this part here gives us some limits on integration, and we can't really integrate from zero to infinity, but actually from zero to the firmies energies.
01:37
And this looks like this.
01:42
So the average energy is this constant.
01:48
D comes from g of e equals some constant d and then e on one half, actually the root of e...