00:03
All right, so we've got a car sliding into the rear of a car.
00:11
It's heading down a hill.
00:17
The slope of the hill is 12 degrees.
00:30
Draw the two cars here.
00:33
The distance between the two cars was 24 meters.
00:39
Oh, my goodness.
00:40
It's pretty far.
00:41
And the initial speed was 18 meters per second with what speed did.
01:07
So in a, the coefficient of friction was 0 .60.
01:18
And we want to know the speed with which the one car struck the other.
01:28
Okay.
01:29
Okay, so the car here isn't really even very important.
01:41
We've got a car here and we've got an initial velocity, but the forces acting on the car are the weight and the frictional force.
02:03
Okay.
02:07
The weight is mg.
02:12
This angle up here is going to be 90 minus theta.
02:23
And so the weight has two components.
02:30
It has a normal component, what would result in the normal component.
02:38
So i'm going to write f sub -end.
02:41
Is going to be m, g, and then that's going to be the sign of 90 minus data, but the sign of 90 minus theta is the cosine of theta, and then it's going to have a, i don't know, sliding component, which would be mg sine theta.
03:12
Okay, the frictional force is going to be the normal force times mu.
03:30
Okay, so the sliding force, mg, sine theta, minus the frictional force is going to be mass times acceleration.
03:50
So, mg.
03:52
Sine theta minus mu m g cosine what in the world i got them mixed up cosine of theta equals mass times acceleration notice that m cancels out now um what was the question with what speed did the hot car one car hit the other car.
04:35
Okay.
04:36
Well, v is going to be v0 plus a .t.
04:48
But we don't know time.
04:51
So let's try, oops, v squared equals v initial squared plus 2a delta x, which is d.
05:04
So, um, v is going to be the square root of v0 squared, which is 18, plus 2.
05:18
We know d, and we know that a is g sine theta minus mu -g cosine theta.
05:43
Okay.
05:44
So that's it.
05:46
Let me put this into a calendar, not into a calendar, into desmos.
05:57
That's an old problem.
06:01
Okay, so i'm trying to find desmos.
06:03
There it is.
06:07
Here.
06:10
That over.
06:13
Where's my whiteboard? here we go...