00:01
In general, we have a car that is going up a hill with an inclination given by theta.
00:07
So, what is the relation between the normal force and the weight force? well, we have to decompose the weight force to answer that question.
00:16
One component of the weight force is pointing in this direction, and the other component is pointing in that direction.
00:24
So there are two components.
00:26
Let me call this w .y and this w .x.
00:30
Note that this is a rectangle triangle because this is a right angle.
00:35
So we can work with that rectangle triangle as we are used to.
00:40
Let me do a bigger drawing of this rectangle right here.
00:44
Nice.
00:45
Now note that the normal force is countering the y component of the weight force.
00:51
So the normal force is equals to the y component of that weight force.
00:58
Now how can you relate the y component of that weight force? of the weight force with the weight force itself.
01:04
So it takes a little bit of geometry.
01:06
So take a look.
01:07
We can extend this down here and note the following...