00:01
For part 8, assume that there is no angular momentum in the thrown -off mass, and so the final angular momentum of the neutron star is equaling the angular momentum before it collapse.
00:11
So we can say l initial equals l final, the initial angular momentum equals the final angular momentum.
00:23
We use the equation for the angular momentum, and we find that here, this would be 2 5th times 8 .0 times the mass of the size.
00:41
Sun times the radius of the sun squared multiplied by the initial angular velocity.
00:49
This would be equalling two -fifths times one -fourth times eight times the mass of the sun times the final radius squared.
01:05
And then we're going to multiply this by the final angular velocity.
01:08
And so the final angular velocity would be equaling two -fifths times 8 .0 mass.
01:16
Of the sun times the radius of the sun squared divided by two -fifths times one -fourth times eight point zero times the mass of the sun times the radius or the final radius squared rather times the initial angular velocity and so this would equal four times the radius of the sun squared divided by the final angular the final radius squared multiplied by the initial angular velocity and we can solve so the final angular velocity would be equaling four times the mass of the sun 6 .96 times 10 to the 8 meters quantity squared times the final radius squared which was 12 times 10 to the third meters quantity squared.
02:15
Multiplied by the initial angular velocity of one revolution for every nine days.
02:24
And so this is giving us 1 .495 times 10 to the 9th revolutions per day.
02:33
And let's convert.
02:37
So this would be again 1 .495 times 10 to the 9th revolutions per day...