00:01
Time dilation occurs in both the special theory and the general theory of relativity, but behaves a little differently, naturally.
00:12
So a reminder that in the special theory of relativity, there's the idea of proper time.
00:18
So you measure proper time if you are carrying the clock with you.
00:24
And if there is another observer who is moving relative to you, and remember, you can can't tell who's actually doing the moving in special relativity.
00:34
There's no preferred frame.
00:38
But if two observers are moving with relative motion v, then each of them thinks that the other person's clock with that other person is ticking slowly.
00:55
So a moving clock relative to you will appear to click to tick more slowly.
01:01
And the person will appear to age less than you.
01:08
And that time dilation, delta t, is given as the time observed by the person not in the proper frame.
01:20
So b, looking at a's clock, or a's age, would be a delta t, or a looking at b's clock.
01:30
Whereas the proper time t0, delta t0, is a looking at their own clock or b looking at their own clock.
01:41
And that time difference gets expanded more the faster the relative motion is compared to the speed of light.
01:53
In general relativity, the thing that occurs is a curvature of space time due to a massive object.
02:01
So the idea is that there's no time difference between two observers if they are stationary, not only not moving relative to each other, but if they are the same distance away from a massive object.
02:22
But if one of the observers is placed closer to a massive object, the other observer is going to see the in this case observer b's clock tick more slowly, but there is an asymmetry that only one of the observers in this situation, the one who is far away, sees a time slowing in the other person's frame.
02:57
So this is the idea that if someone were approaching a black hole and you were observing them from far away, you would see their time slow more and more and more until they got to the event horizon and then it would appear like their clock entirely stopped.
03:19
We can see that in the time difference, time dilation formula, the clock in frame b observed by a gets dilated by the factor 1 over the square root, of 1 minus 2gm over d, c squared.
03:42
And that factor 2gm over c squared is called the schwarzschild radius and gives kind of a limit of how close that observer b can get to the center of the mass.
04:03
Of course, for a normal mass like a planet, we don't fall within the short shield radius.
04:11
In any event, the time dilation factor gets worse, not only for a more massive object, but as the observer b gets closer to the center or if there's a bigger separation between a and b.
04:36
So what evidence do we have that time dilation, gravitational time dilation works like this? the biggest evidence is that we've got a series of satellites that go around the earth.
04:51
The first series were called gps, but i believe we have more than one set of gps satellites at this point in time.
05:01
And these gps satellites are necessary for locating your position down on earth.
05:12
So notice that there is a difference in the time frame between the satellites.
05:18
And the people on earth who are trying to use these satellites for location.
05:24
So if these satellites do not get synchronized very carefully, your position is going to get off on earth.
05:34
They will not be able to figure out your location very well with the algorithms built in the receivers.
05:42
So time dilation, gravitational time dilation, is very important in the case of synchronizing gps.
05:57
And it's sort of complicated, so we won't get into that...