00:01
We have to consider the case of a mountain biker that is moving on a constant speed along the bottom of a trail circular dip.
00:09
So in this case, we have the dip here, and we're assuming it's circular.
00:14
And then in the second case, we're assuming that there is going over a magnitude when the forest exists over a hill.
00:26
Let's see here.
00:28
So certainly that you and the biker, it doesn't determine the direction of the acceleration of the acceleration.
00:31
At each point and construct a force diagram of each position.
00:36
Okay, across the top.
00:40
Okay, so on the bottom, well, oops, i forgot to write some things in here.
00:46
So this is n -m -g -n -a -r.
00:51
So at the bottom, we have a normal force from the ground, the weight of the bike and the rider, and then the acceleration is always going to, the acceleration, the radial acceleration will always be pointing towards the center of the circle.
01:06
So in this case, it's in this direction.
01:09
And it has a magnitude of v squared over r...