00:01
So how can we write the second law of thermodynamics mathematically? and so there are really two ways depending upon whether the process is spontaneous or whether it's reversible.
00:16
And so if we're dealing with a reversible process, we would say that entropy is conserved.
00:27
It's neither created nor destroyed.
00:30
And so the change in entropy of the human.
00:33
Universe, which is equal to the sum of the change in entropy of the system plus that of the surroundings is going to equal zero.
00:47
But if it's not a reversible process and spontaneous processes fall under this category, well, then it's different.
00:57
Then entropy does not need to be conserved, but essentially the entropy of the universe continually increases under these situations.
01:08
So we would wind up with a value of delta s of the universe that is greater than zero.
01:23
So let's take a look at two examples of what could happen.
01:27
And so the first is, what if we have a spontaneous process? and a spontaneous process is going to be one that is irreversible.
01:42
And we have a delta s of our system that is negative...