00:01
Here, we know that the buoyancy force is equaling the mass of the fluid displaced times g.
00:05
And then according to mass, it would simply be the density of that, whatever fluid it is, times the volume of the fluid that is displaced times g.
00:13
We know that the force of gravity of the fluid acts at the center of mass.
00:18
This is known.
00:19
The force of gravity of any object acts at the center of mass.
00:24
On this fluid now, there are only two forces on the fluid, and the system itself is at equilibrium.
00:31
If the system itself is at equilibrium, then the forces, of course, have to be equal in magnitude and in opposite directions.
00:39
And we know that the system itself is in static equilibrium, therefore it is not rotating.
00:47
So because it is not rotating, that means that they both have to, the net torque is essentially zero.
00:55
And if the net torque is essentially zero, and there are only two forces on the fluid, one of them acting at the center of mass.
01:03
We know the force of gravity acting at the center of mass...