00:01
All right, so let's say we have a skier going down an incline like this.
00:05
And if we draw a free body diagram, the weight of the skier is going to go this way.
00:13
The component of the weight along the plane is going to be m .g.
00:17
Sine theta.
00:18
And the component perpendicular to the plane is m .g.
00:22
Coat -sign theta.
00:23
So this is, you know, the weight is just m .g.
00:29
And the frictional force then is going to act this way.
00:34
I think that's all we need.
00:36
So then for part two, so that was part one, part two, we want to solve for the weight of the skier, which is easy.
00:44
It's just 62 kilograms times 9 .8 meters per second squared.
00:55
So 607 .6 newton's question three.
01:01
What is the normal force? so we'll call it it fn.
01:04
This is just going to be the weight times.
01:06
The cosine of the angle...