00:01
So in this section, we're discussing the divergence theorem.
00:05
And ultimately, what we have is a vector field, f, and it is equal to this vector function of x, y, and z, which is just x, the vector x, y, z, and it's equal to the vector r.
00:27
So then we have this surface that encloses the box.
00:38
It's bounded by the planes.
00:40
X equal to y, equal to z, equal to zero.
00:45
And then x equal to y equal to z equal to one.
00:50
So with that in mind, we now have the first surface, which is x, y, y, and z where zero is less than or equal to zero is less than x which is less than equal to one zero is less than y which is less than or equal to one and z equals zero then we know that the unit normal vector is negative k hat um so it's on the face of the plane z equals zero um so that means that the flux across the face is going to be signified by fee, which is equal to this double integral right here across the first surface, f .n .d .s, which is equal to the double integral of xy, negative k, hat, ds, which we know is just going to be equal to zero.
02:19
So on the face of z equals 1 now, we're going to have something similar.
02:24
It's the second surface right here.
02:29
And that's just going to be x, y, x and y, where 0 is less than or equal to x, which is less than or equal to 1.
02:42
And 0 is less than or equal to y, which is less than or equal to 1.
02:47
So based on that, now what we have is fee being equal to the double integral of the second surface of x, y, 1 times, and this is just 0 ,0, 1...