00:04
So this is an interesting problem that will have a little discussion about, well, no, not this problem, i guess.
00:13
Maybe it's the, yeah, it's coming up here.
00:18
It's not this one.
00:19
I thought it was a, oh yeah, it's 118, not 114.
00:25
Anyway, this is just a simple little problem.
00:28
But we have a volume, a bottle that has a volume of 0 .02.
00:35
Cubic meters.
00:37
It is empty, evacuated, vacuum inside here.
00:42
The air, the surrounding air, is at 20 degrees c and 100 kilopascals.
00:49
M1 is, of course, zero.
00:50
There's nothing in the tank to begin with.
00:55
So we open it up on the air flow in.
00:59
So the amount of air that goes in is the amount of air that's in the tank after it fills.
01:06
And let's see here.
01:07
We know then that the that the temperature after it feels and the pressure after it feels, it's equilibrated with the air and we have some heat transfer out.
01:19
So it all comes back, you know, it winds up being at surrounding temperature and surrounding pressure in the end.
01:27
So we know the energy in minus the energy out is the change in energy in the system.
01:33
So we have minus q out, the heat transfer that occurred, plus the entropy, the transfer of entropy in, and that has to equal the change in internal energy, which there was no initial internal energy, so that's just the internal energy in the end...