00:01
We're given the motion of some system at, and let's say the position or whatever it is we're measuring s, is a times cosine omega -t plus fee.
00:12
In engineering, we'd call this the amplitude, the frequency, and the phase of the motion.
00:19
So they ask us to find the velocity and then find times when the velocity is zero.
00:25
Well, to find the velocity, we just take a derivative and use the chain rule.
00:30
So the derivative of the cosine is the minus sign.
00:33
So we have a minus a.
00:36
And then we need to take the derivative of the inside so that we get an omega there and then sign omega -t plus fee.
00:43
So just a simple application of the chain rule that i didn't go through and explicitly define.
00:49
It could have defined this as u and then d -u -d -t is just omega.
00:53
That's why we get this guy here.
00:55
So they want to know when this thing is zero.
00:57
Well, when that thing is zero, i called the, the times when it's 0 t star well that's when this thing is zero assuming these aren't zero they're constant um so we need sign of omega t star plus v equals zero well that happens when sign is zero when its argument is n times pi so some integer times pi so you know zero pi 2 pi um so we're going to solve for t star so t star equals n times pi over omega minus fee over omega...