00:01
So in this question, we're told that we have a slender rod of length l, whose mass per unit length varies.
00:13
So this is x equals zero.
00:16
This is x equals l.
00:18
And we have dm by dx equals gamma x.
00:24
So now the total mass, m, is going to be the integral dm by dx, dx, from zero to l.
00:35
So this is gamma times the integral from 0 to l of x, dx, which is a half gamma l squared.
00:44
So that's the total mass.
00:48
So now i equals the integral of r squared dm from the, so this is from the left end.
01:03
So this is going to be the integral of x squared, dm by d x, dx, dx from zero up to l.
01:15
So this is gamma times the integral from zero to l of x cubed dx.
01:21
So this is gamma, so this is going to be a quarter gamma l to the power of four.
01:29
But we want to express this in terms of m and l.
01:32
So this is going to be a half times a half gamma l squared times l squared.
01:40
So this is a half m l squared.
01:45
Now for part c, we have l equals 0 .4 meters, m equals 3 .0 kilograms.
01:56
And it's rotating about the axis as in part b.
02:00
So it's going to have i equals a half m l squared.
02:07
Now the angle, theta of t, equals 1 .1 radiance per second, times t plus 6 .3 radians per second squared times t squared.
02:27
So the kinetic energy, t, is a half i omega squared.
02:37
And omega is the angular velocity, so it's the rate of change of theta.
02:43
So this is a half i times, and we want this when it has rotated 0 .1 revolutions...