00:01
So we first want to find the centroid.
00:05
So consider the fact that i will call it xc is the position in the x -axis where the amount of mass on the left and the right are the same.
00:17
So it's the x -coordinate of the center of mass.
00:21
Since the hemisphere is symmetrical about the x -axis, we know that the center, the x -coordinate of a centroid is just zero.
00:29
And the same for the y coordinate.
00:32
So that's the case right here.
00:36
Then we want to find z, and this is going to be a c right here.
00:42
We want to find the center point for z.
00:47
We know that that's going to be equal to the partial derivative of m of x, y over m.
00:57
So we're going to have some value, we'll call it alpha.
01:03
Of x, y, z, being the density of the function of the hemisphere.
01:14
So m is equal to, since the density is constant, we're just going to call it k.
01:29
So m is going to be the integral of this constant density bv, the volume.
01:39
We can pull this k out, and then we have this right here.
01:45
We know we're going to do this with spherical coordinates.
01:53
So what we'll end up having is, since we're having spherical coordinates of a hemisphere, we know that a hemisphere has volume, we know that a sphere has volume for a cubed over 3 pi, or 4 pi a cubed over 3.
02:19
So if we just want the hemisphere, it's just going to be 2 instead of 4 pi a cubed over 3.
02:30
Then what we have as a result having this, we want to evaluate the partial derivative x, y.
02:41
So when we do that, what we'll end up getting is that m xy is equal to k -a to the fourth pi over four.
03:01
So our actual centroid, or the z -coordinate, since it's the partial derivative of m -x -y over m, we're going to take this right here and divide it by m, which is ultimately to multiply by the reciprocal.
03:25
So we see that the k, the pi, and the a cube will all cancel, leaving us with just an a.
03:36
And then that's going to be 3a over 8...