00:01
For this problem, let's first consider the conservation of momentum and apply it to the boy and to cart a.
00:12
So the conservation of linear momentum, to be specific, tells us that the momentum of the initial state of the system, mv1, must equal to mv2.
00:36
So initially the boy and the car were both addressed.
00:43
So they have no velocity and hence no momentum.
00:48
And then we have the momentum of the cart which is to the right.
00:54
So we'll take the left direction in this problem to always be positive.
01:00
So for the car a, it has a mass of 80 pounds divided by g, which is 32 .2 feet per square second.
01:09
Times its velocity with which it moves off va plus the momentum due to the boy, which is his weight, 60 pounds over g, which is 32 .2 feet per square second, times his velocity, which is v little b, and this is in the x direction.
01:30
Remember, his velocity is x and y components, whereas the cars have only x components.
01:36
So we're just looking at the conservation of linear momentum, in the x direction so now if we rearrange this equation we show that the velocity of car a is equal to 0 .75 times the x component of the boy boy's velocity vb now we also know that the velocity of the boy is final velocity vb is equal to v a plus vb, b of the boy relative to cart a.
02:25
So the boy's velocity is equal to the velocity of the cart plus his velocity relative to cart a.
02:31
So if we take the x components of this, vb in the x direction is equal to minus v a that only has x components, plus 4 times cosine of theta which is cosine of theta in this case is 12 over 13 in our diagram that's 4 times 12 by 13 and so hence we get vb in the x direction and we get v a from above in terms of vb so we get vb in the x direction to be 2 .11 feet per second...