00:01
All right, let's start by figuring out what the friction force will be.
00:07
So we know what the, we know that we're looking at a weight force of mass and gravity here.
00:20
We can treat this as a sheet of sand or as a particle.
00:30
It doesn't really matter because we're going to have a friction force that is up the slope of the sand pile.
00:40
We're going to have a weight force that is straight down towards the center of the earth and this weight force is going to be divided into two parts.
00:48
There's going to be the normal force which is going to be m .g.
00:53
Cosine theta and then there's going to be a force that is parallel to the slope of the hill which will call which is going to be m .g.
01:05
Sine theta and this friction force is related to these two forces.
01:11
So this friction force that we're experiencing, it's going to be equal to mu times m g cosine theta.
01:22
And it has to be equal to or less than the parallel force in order to keep this sand from sliding down.
01:33
So we'll just say we're just going to focus on that point where they are equal, since that's or we're looking for, we're looking for the maximum size of the sand pile.
01:43
So we're going to set it equal to mg sine theta...