00:01
Okay, so here we have a question about buoyancy, and the first question we're asked to, or the first question we're asked is can we combine the two equations given to get the point force in terms of water density and volume? so we're told that the point force is equal to m multiplied by g, and we are also told that what we should know this is that density is equal to mass over volume.
00:24
So what we can do is we can isolate m here by m is equal to row times v and then substitute that into.
00:30
Our point force equation.
00:32
So that's going to give us what? we can say that m is equal to row v.
00:36
Therefore, the point force is equal to row vg.
00:42
And then we are asked to draw and label all the forces in a free body diagram.
00:51
So we have the tension in the string.
00:55
We have the weight downwards.
00:59
There are thereabouts.
01:01
That's going to be mg.
01:03
That's going to be the.
01:04
That's going to be the the actual mass.
01:08
And then we have the buoyant force, which i'll just draw coming up from the bottom there.
01:14
So that's going to be the buoyant force.
01:17
Okay.
01:18
And then we'll ask, what's the total acceleration? well, if this is an equilibrium, then total acceleration is equal to zero.
01:23
So we can write that in.
01:25
We can say that total acceleration equals zero if system is in equilibrium.
01:46
So so we're now asked to use newton second order to add all the forces together and solve for tension.
01:53
So if we think about this, we have the weight downwards and we have the buoyant force upwards and tension upwards.
02:00
So we can say that...