00:01
So for positive t, you have a particle that's moving in the xy plane here with x equals a plus b times sine kt, y equals a plus b cosine kt.
00:17
Let's see, so if we just to get a handle on this, set a to be zero and b and k to both be one, what we have here sine and cosine, this looks like circular motion, right? but it's not your conventional circular motion because when t is say zero, our x is going to be zero and our y is going to be one.
00:40
This is t equals zero, limbo our x and y, and then when t is, let's say pi over two, right? sine of pi over two is one and cosine of pi over two is zero.
00:56
So here we have t equals pi over two, and we see that our circle actually goes around like this, clockwise as opposed to counterclockwise.
01:09
By increasing k, by changing a, b, and k, we're not actually going to change that basic fact that it's going counterclockwise and starting at the top.
01:22
So this is a circle, i said counterclockwise, but i meant it's going clockwise starting at the top, with a couple more things, right? x actually should start, the center of x should be a as opposed to zero, likewise y should be starting in a, so it's centered at the point a, a.
01:49
The radius we can see is b, and the frequency is, or let's say the period is two pi over k.
02:04
These are all just things that we pull out of the general circular motion formula.
02:10
There's the motion in words, and then now that we've described it like that, it's relatively easy to see what the changes would do.
02:18
Increasing b will increase the radius, right? this b we see is affecting the sine and cosine, so like the oscillatory, the circle parts of the motion.
02:33
If we increase a, we move the circle, and then because it's centered at a, a, it's going to be somewhere on this line y equals x, and as we increase a, move it that way.
02:50
So move circle, i'm just going to call that northeast, that is up and to the right.
02:54
If we increase k, we increase the frequency, or decrease the period...