00:01
So we're told we have a horse that's harnessed to a sled.
00:04
The sled has a mass of 236 kilograms.
00:09
The horse must exert a force of 1 ,400, 1 ,240 newtons at an angle of 35 degrees with the horizontal to get the sled moving.
00:21
So we're going to treat the sled as a point particle.
00:24
So again, all these forces basically act through this point here.
00:28
We want to calculate the normal force on the sled when the magnitude of the side.
00:31
The force of the applied force is this value here.
00:37
Well, we can look at forces in the y direction.
00:43
Okay, so we have, let me put a little axes in here.
00:46
We have y and have x.
00:53
So a summation of forces in the y direction is going to be equal to zero because it's not accelerating in that direction.
00:59
So we have n plus f sign of 35 degrees, my minus w equals zero.
01:08
So n equals the weight, mg, minus f sine of 35 degrees, and that winds up being 1 ,600 newtons.
01:19
So you can see here that the force is actually, the horse is actually lifting this off the ground so that the normal force is actually a little bit less, that is less than the weight because the horse is off the, part of the force that the horse is applying is also lifting acting to lift the sled.
01:42
So let's see here.
01:45
That's the normal force.
01:47
So then we want to calculate the coefficient of static friction between the sled and the ground beneath it.
01:51
All right.
01:51
So that means we're going to look at the forces in the x direction.
01:55
And that means we have minus the friction force plus f cosine of 35 degrees.
02:03
And again, we're assuming that it hasn't started accelerating...