00:02
So we'll start off with kepler's third law, which basically says that the period of an orbit squared is proportional to the semi -major axis cubed of that orbit.
00:18
And the constant of proportionality works for the orbit around any massive body.
00:24
We'll call that big m.
00:26
So that constant is 4 pi squared divided by universal constant g.
00:33
Times the mass of the body around which the orbit is occurring.
00:40
So p is period and a is semi -major axis, and also interpreted to be the average distance of the orbiting object from the main mass m.
00:59
So we're going to take a look at using this law to do a little bit of rocket science, i suppose.
01:06
So the idea is to put an object in orbit around the earth.
01:11
So mass of the earth is the parent body.
01:15
And we're going to take a little spacecraft that starts at parogy.
01:22
So a parogy is a certain distance from the center of the earth.
01:29
Here we'll call that 6 .67 times 10 to the 6 meters.
01:39
So this is not going to be a scale drawing.
01:42
We're just showing a sketch to give the idea.
01:45
And that is going to go in an elliptical orbit with the endpoint.
01:53
I'm probably not going to draw a very good ellipse, but the endpoint is the moon, the position of the moon.
02:05
And so the appalian distance is from the center of the earth to the moon.
02:14
Which is 3 .85, roughly 3 .84 times 10 to the 8th meters.
02:29
So we could ask how long does this journey take using this elliptical orbit? and we can see that essentially we've gone through one -half of a period.
02:43
So if we found the period, we could determine how long the trip would take...