00:03
Okie -dokey.
00:05
So let's start looking at our problem.
00:09
We're asked to think about a space station with diameter of 800 meters.
00:17
So let's say diameter 800 meters.
00:21
You're just going to do the radius real quick.
00:23
Radius is half the diameter, so 450 meters.
00:28
And we're us to say, how many revolutions do we need to have artificial gravity of 9 .8 if this was a space station? no gravity.
00:38
So we know what our gravity is going to be.
00:42
Maybe it's per second squared.
00:44
So how are we going to be getting this artificial acceleration? artificial gravity.
00:51
Gravity is an acceleration.
00:52
So this is going to be our centripetal acceleration.
00:56
So i'm going to call this ac equals omega squared.
01:01
R, we can just, we remember omega is our linear over revolutions.
01:18
What we want is this omega, we want to know how many revolution, how many rads per second.
01:28
We're going to be going so we can say, hey, i know what i want this to be.
01:32
I want it to be g, omega squared r, i can rearrange g over r equals omega, omega, squared, take the square root, g over r equals omega, and then hey, i know g and i know r, so i can just pull up those right in, and this will get me 0 .1475 rad per second.
02:08
Now remember this is in rads, we were looking for revolutions.
02:12
So how do we go from revolutions to rads.
02:15
Well, starting over here, we do our dimensional analysis.
02:24
We get 0 .1475 rad for every one second.
02:30
I want this to be revolutions per minute.
02:32
In, there is, how many rabs does it take to make a revolution? two pi rads make one revolution, because rads are the degrees around a circle.
02:44
How do we go from seconds to minutes, 60 seconds in one minute...