00:01
Alright, so here we have the earth, and we're interested in looking at a spiral galaxy that's emitting a particular frequency of light.
00:13
And since it's a spiral galaxy, the galaxy is over here, some of it is spinning towards us, and some of it is spinning away from us.
00:25
Now, the whole galaxy altogether is moving at some particular speed v, and when we're looking at some particular speed, v, and when we're looking, at this arm of the galaxy, the net speed is going to be v plus the spinning of the galaxy.
00:44
But when we're looking at this arm of the galaxy, the net speed is going to be v minus whatever s is.
00:54
So this is the net speed away from us, this is the net speed away from us.
00:59
Okay, so the first thing we're going to do is look at v and s.
01:03
V is equal to 3 .2 .4 times 10 to the fifth meters per second.
01:15
S, the spinning of this galaxy, is also just known as little v, but i'm going to call it s because it's easier for me to write down.
01:26
5 .75 times 10 to the fifth meters per year.
01:37
Second.
01:39
So actually we're going to have a net speed coming towards us.
01:43
So i'm just going to call this u towards us.
01:49
This is the net speed, is 3 .24 minus 5 .75 times 10 to the minus 5 .75, which is going to be minus 2 .54, 2 .51 times 10 to the 5th.
02:11
So it's minus in the away direction, which means that the net u coming towards us is actually a positive 2 .51 times 10 to the 5th.
02:24
So if we want to solve for a doppler shift, we know that f prime from our doppler shift equation is going to be equal to f times 1 plus because the spiral arm has a net direction towards.
02:44
Us 2 .51 times 10 to the 5 over 3 times 10 to the 8th...