00:01
Okay, for this problem, it's basically a momentum conservation problem.
00:06
So initially, we have momentum just in the x direction, just moving to the right.
00:11
So that has to stay conserved.
00:13
And then we have none moving up and down.
00:16
So that means afterwards also the vertical has to kind of go in.
00:20
So to figure out these two velocities, what we're going to have to do is realize that mass times the initial velocity of a, that's our initial.
00:30
And this is the x direction, would have to equal, and since these all have the same mass, i'm just going to call them m.
00:38
So m times bfa in the x direction, plus m times bfa in, or, whoops, sorry about that, b, bfb in the x direction.
00:57
So to find those, what we have to do is kind of split these up.
01:01
So for example, we know that this would have a vfb x and then vfb y, and they would combine together to give us just vfb.
01:17
As i kind of look at this, what that means then is that vfb is the hypotenuse.
01:24
So it would equal vfb or actually vfb.
01:31
Is the adjacent side, so it would equal vfb times the cosine of 45 degrees, and vfb y would be vfb times the sign of 45 degrees.
01:49
And then the same thing kind of up here with our vfa.
01:54
Vfa would be the hypotenuse, so we'd have a vfax and a vfa so we can write those that vfax would equal vfa times the cosine of 30 degrees.
02:16
And then vfay would equal vfa times the sine of 30 degrees.
02:25
Now since cosine and sine of 45 are the same, these are actually going to end up being the same.
02:31
These are not going to be the same.
02:33
They will actually be different.
02:34
But we can calculate all of those.
02:36
So the other part we have down here is we also have a y direction.
02:41
And so we originally had zero y motion.
02:45
So what we have is we would have to have mass times the vfa in the y direction, and then it would have to actually e plus mass times the bfb in the y direction.
03:01
And since they both have the same mass, we can actually cancel those masses...