00:01
All right, so we have a lot going on in this problem, namely a chair with various forces acting on it.
00:10
So for simplifications, we're going to draw our chair like that, like a nice little square, and then take the forces that are being acted on it in order from easiest to least obvious.
00:23
So i think the most obvious force that is always going to be acting on the chair is the force of gravity.
00:27
That's going to be equal to the chair's mass times the excephalibious.
00:30
Due to gravity.
00:34
And in order for the chair to not go anywhere up or down, we're just sliding horizontally in this problem, there has to be some sort of vertical force to counteract the force of gravity, and this is the normal force of the floor, pushing back up on the chair.
00:50
We do also know that someone, you, are applying a diagonally downward force.
00:58
We're just going to call that f.
01:00
And we know precisely which angle you are applying that force at.
01:06
And that is going to be at theta or in this problem, 37 degrees below the horizontal.
01:14
So theta is going to be equal to 37 degrees.
01:17
And then lastly, we are told that this is not a frictionless surface.
01:22
So because the block is sliding to the right in the way that i've drawn in this problem, we will have a kinetic friction acting to oppose this motion, so that is going to be directed to the left.
01:35
So that completes our free body diagram, and that was part a of the problem, by the way.
01:40
So in part b, we are tasked with calculating the normal force.
01:45
So there are a lot of forces on this block and lots of distractions.
01:50
We tend to associate any frictional force with the normal force via...