00:01
So we're going to denote the force exerted by the worker on the crate as f equaling 110 newton's.
00:08
And we can say that then the maximum static frictional force would be equaling the coefficient of static friction multiplied by the force normal.
00:17
For part a, when we apply newton's second law here in the vertical direction, we can say that the force normal would be equal to the gravitational force mg.
00:25
And so we can say that the maximum static frictional force would then be equaling.
00:30
To the coefficient of static friction mg.
00:34
This is going to be equalling to 0 .37, multiplied by 35 kilograms, multiplied by the acceleration due to gravity, 9 .8 meters per second squared.
00:45
And we find that then this is equaling approximately 130 newtons, and we can then say that the maximum static frictional force is greater than f.
00:58
For part b, we can see that the block is initially at rest and it stays at rest because the force f is less than the maximum static frictional force.
01:11
If the force can't exceed that maximum static frictional force, then the block will stay at rest.
01:18
And we can say again, block stays at rest.
01:26
And for part c, we can say that applying newton's second law here to the horizontal direction, we can say that the magnitude of the static frictional force exerted here on the crate would be equaling f equaling 110 newton's.
01:44
So that would be your answer for part c, and then for part d, we have that.
01:49
First, we're going to say the upward force exerted by the second worker as f sub 2, exerted by second worker.
02:11
And given this, we can apply, again, newton's second law...