00:01
So we have a diagram here with a fulcrum and, whoops, two masses.
00:22
L1 is here, l2 is here.
00:26
Okay.
00:29
So we're told that l1 is 20 centimeters, and l2 is 80 centimeters.
00:49
Okay.
00:50
With the magnitude of the accelerations on particles 1 and 2.
01:15
Okay.
01:17
So, the inertia of this system would be the sum of the masses times the distance is squared.
01:32
I don't think we're told numbers for the mass, but they're the same.
01:39
So the inertia would be, and i'm making this the positive direction, anyway, it would be, well, total inertia, it doesn't matter on the direction.
01:56
It's just going to be the sum of the mr squares, which would be mass times l1 squared plus mass times l2 squared.
02:07
But i'm just going to change that to factor out the m.
02:14
Okay.
02:15
Now, the torque net, this is where i need the direction, is going to be m times g at l1.
02:35
So m -g -l -1 minus m -g -l -2.
02:45
That's going to be i alpha we're trying to figure out alpha so alpha is going to be factoring out the m g who m g it's not a not a subscript l1 minus l2 over i but i is m l1 squared plus l2 squared oops, i erase a draw.
03:27
Okay.
03:29
So, then the acceleration at 1 is going to be alpha times the distance to 1, which would be l1.
03:41
The acceleration at 2 is going to be alpha times the distance to 1, to l2.
03:53
So putting this all together in a calculator, i'm going to write, first of all, i'm going to declare l1 and l2.
04:05
And i finally figured out, if you just type l1, it puts in a subscript automatically.
04:10
E equals 0 .02...