What I understand about Time Dilation

In summary, time dilation can occur under gravity or acceleration, which can be referred to as Gravity Time Dilation and can also appear to be happening when two things are in different frames of reference, which can be referred to as Velocity Time Dilation. With Gravity Time Dilation, there has been objective evidence that there is time dilation under gravity or acceleration. With Velocity Time Dilation, the evidence is thought to be relative rather than objective. In the twin paradox experiment, the clock on B2 would be thought to be objectively running slower than the clock on A2. However, if B2 and B1 were in the same frame of reference, then objectively the clock on B1 would be running slower than the clock on A1. Experiments
  • #71
name123 said:
So you are stating that the time dilation will be such that if both satellites had strobe clock's it would be calculated that the strobe clock on the other satellite is flashing at a slower rate?

Does that mean that if the orbit was big enough, or the strobes went off at smaller time intervals or some combination of the two, that there could be a discrepancy between the observed strobe flashes, and the count showing on the satellites clock when it passed?
No, because the rate of strobe flashes that you visually perceive depends on the both the relative speed and direction of that speed relative to you, if you are receding from each other you see a slower strobe rate, if you are closing in on each other you see a faster strobe rate. Again, over the course of one orbit this will add up so that the number of flashes you saw matches the other satellites clock reading. (if you were visually watching the other clock during the orbit, you would also see its tick rate slow down and speed up to match the strobe rate you were seeing.)
 
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  • #72
Ibix said:
There is no inertial frame that covers both satellites at once, except as they pass each other. That's why naive SR assumptions don't work in this case

I am not sure what you mean. I was thinking that they would be in different local inertial frames at all times.
 
  • #73
name123 said:
So you are stating that the time dilation will be such that if both satellites had strobe clock's it would be calculated that the strobe clock on the other satellite is flashing at a slower rate?
Yes. You've worked hard to make the situation symmetrical, so any other answer (implying an asymmetry) would be surprising.
Does that mean that if the orbit was big enough, or the strobes went off at smaller time intervals or some combination of the two, that there could be a discrepancy between the observed strobe flashes, and the count showing on the satellites clock when it passed?
No, and until this is completely unsurprising to you, you might want to work with the less tricky traditional form of the twin paradox. This situation is covered in the "Doppler explanation" section of the FAQ that I linked to earlier.
 
  • #74
Janus said:
No, because the rate of strobe flashes that you visually perceive depends on the both the relative speed and direction of that speed relative to you, if you are receding from each other you see a slower strobe rate, if you are closing in on each other you see a faster strobe rate. Again, over the course of one orbit this will add up so that the number of flashes you saw matches the other satellites clock reading. (if you were visually watching the other clock during the orbit, you would also see its tick rate slow down and speed up to match the strobe rate you were seeing.)

Do you agree that the time dilation will be such that if both satellites had strobe clock's it would be calculated that the strobe clock on the other satellite is flashing at a slower rate?
 
  • #75
name123 said:
Do you agree that the time dilation will be such that if both satellites had strobe clock's it would be calculated that the strobe clock on the other satellite is flashing at a slower rate?
No. I don't mean to sound rude, but this is starting to get repetitive. It feels like you have a slight misconception that you are trying very hard not to let go of. You heard that 'the other guy's clock' is always slower than yours, but that just isn't the case.
 
  • #76
name123 said:
If a satellite had two clocks on board, then could the simultaneity convention not be that their ticks are simultaneous?

A simultaneity convention has to cover events on both satellites if you're going to use it to calculate one satellite's clock rate in the other's frame. And since the satellites are in relative motion, there is no way to construct a simultaneity convention that has all ticks of clocks on both satellites simultaneous.
 
  • #77
Nugatory said:
No, and until this is completely unsurprising to you, you might want to work with the less tricky traditional form of the twin paradox. This situation is covered in the "Doppler explanation" section of the FAQ that I linked to earlier.

I read the http://math.ucr.edu/home/baez/physics/Relativity/SR/TwinParadox/twin_doppler.html part of a link you supplied to me before. Is that what you meant?

I had a slight problem with it. Terrence is supposed to calculate that Stella's clock is running slow, and putting out a flash once every 7 seconds.
---
Terence computes that Stella's clock is really running slow by a factor of about 7 the whole time
---

And that she is traveling for 14 years (according to Terrence).
---
Here's the itinerary according to Terence:

Start Event
Stella flashes past. Clocks are synchronized to 0.
Outbound Leg
Stella coasts along at (say) nearly 99% light speed. At 99% the time dilation factor is a bit over 7, so let's say the speed is just a shade under 99% and the time dilation factor is 7. Let's say this part of the trip takes 7 years (according to Terence, of course).
Turnaround
Stella fires her thrusters for, say, 1 day, until she is coasting back towards Earth at nearly 99% light speed. (Stella is the hardy sort.) Some variations on the paradox call for an instantaneous turnaround; we'll call that the Turnaround Event.
Inbound Leg
Stella coasts back for 7 years at 99% light speed.
Return Event
Stella flashes past Terence in the other direction, and they compare clocks, or grey hairs, or any other sign of elapsed time.
According to Terence, 14 years and a day have elapsed between the Start and Return Events; Stella's clock however reads just a shade over 2 years.
---

So I would expect the amount of flashes Terrence sees to be equal to the number of seconds in 2 years.

But it then states that because of the doppler effect he sees a flash every 14 seconds on the way out, and 14 flashes per second on the way back.
---
On the Outbound Leg, Terence sees a flash rate of approximately one flash per 14 seconds; on the Inbound Leg, he sees her clock going at about 14 flashes per second.
---
Which seems to me to be equal to the number of seconds in 1/2 year on the way out and the number of seconds in 98 years on the way back. But the clock never flashed that many times. So I guess I have misunderstood.
 
  • #78
russ_watters said:
No. I don't mean to sound rude, but this is starting to get repetitive. It feels like you have a slight misconception that you are trying very hard not to let go of. You heard that 'the other guy's clock' is always slower than yours, but that just isn't the case.

Do you disagree with the first answer Nugatory gave in post #73? Or do you think I have misunderstood it?
 
  • #79
Nugatory said:
That's not what a momentarily comoving inertial frame means

name123 said:
I was thinking that they would be in different local inertial frames at all times.

I think there are some items that need clarification.

A local inertial frame is a set of inertial coordinates (i.e., coordinates that work just like standard inertial coordinates in special relativity) that covers a small patch of spacetime--a small region in space over a small interval of time.

A "momentarily comoving inertial frame" means we pick a particular event on the worldline of some object, like a satellite, and construct a local inertial frame in which the event we picked is the origin and the object we picked is at rest at that event. This amounts to approximating a small segment of that object's worldline as a straight line, if the object is moving in free fall, as the satellites are. But @Nugatory correctly points out that you can also construct a local inertial frame around an event on the worldline of an object that is not in free fall. If you do that, the worldline of the object will not be a straight line, even in the local inertial frame.

If we pick different events on the worldline of the same object, such as different events along the orbit of a satellite, the local inertial frames at these different events each cover only a small region of space and a small interval of time around those different chosen events. And if either the object is accelerating (i.e., nonzero proper acceleration, acceleration that is felt) or spacetime is curved, then these local inertial frames will not "line up", in the sense that the straight lines in one of them will be "at an angle" to the straight lines in the other. But this is a separate matter from the question of what the straight lines in each local inertial frame represent--in particular, whether the worldline of our chosen object is a straight line in any of these local inertial frames (see above).

If we have two objects that are passing each other, then we can construct two local inertial frames centered on the event where they pass. In each of these frames, one of the objects will be at rest (at least momentarily), and the other will be moving; but both objects will be "in" both frames (their worldlines will appear in both frames). And if both objects are in free fall (as the satellites are), then both of their worldlines will be straight lines in either local inertial frame; they just won't be straight lines in the same direction. So each object will only be at rest in one of the two inertial frames; but they will still appear in the other, just not at rest.
 
  • #80
PeterDonis said:
A simultaneity convention has to cover events on both satellites if you're going to use it to calculate one satellite's clock rate in the other's frame. And since the satellites are in relative motion, there is no way to construct a simultaneity convention that has all ticks of clocks on both satellites simultaneous.

Wouldn't the time dilation be calculated by observing the flashes from the other satellite and then taking account of the doppler effect, and then comparing that rate to the on board clocks
 
  • #81
name123 said:
Which seems to me to be equal to the number of seconds in 1/2 year on the way out and the number of seconds in 98 years on the way back.

No. Terence does not see Stella's turnaround at 7 years elapsed on his clock; he sees it at close to 14 years elapsed on his clock. The article goes into all that.

So Terence sees 1 year's worth of flashes coming in from Stella's outbound leg during close to 14 years of his time--or one flash every 14 seconds. He then sees 1 year's worth of flashes coming in from Stella's inbound leg during 1/14th of a year, or 14 flashes per second.
 
  • #82
name123 said:
Do you disagree with the first answer Nugatory gave in post #73? Or do you think I have misunderstood it?
I believe that part of his response was limited to when the satellites are moving away from each other. Otherwise, over the entire orbit, the number of flashes sent and received would not match.

Everyone else is telling you this too...
 
  • #83
PeterDonis said:
No. Terence does not see Stella's turnaround at 7 years elapsed on his clock; he sees it at close to 14 years elapsed on his clock. The article goes into all that.

So Terence sees 1 year's worth of flashes coming in from Stella's outbound leg during close to 14 years of his time--or one flash every 14 seconds. He then sees 1 year's worth of flashes coming in from Stella's inbound leg during 1/14th of a year, or 14 flashes per second.

Doh! Thanks :)
 
  • #84
name123 said:
Wouldn't the time dilation be calculated by observing the flashes from the other satellite and then taking account of the doppler effect, and then comparing that rate to the on board clocks

"Taking account of the doppler effect" requires adopting a simultaneity convention. If the satellite adopts the simultaneity convention of its own local inertial frame, then it gets the result that the other satellite's clock is running slow. But, as I've already explained, there is no way to "add up" these calculations from all the different local inertial frames around the satellite's orbit to conclude that the other satellite's clock will have less elapsed time around one complete orbit. That's because each of those local inertial frames has a different simultaneity convention, so you can't combine their calculations.

I have already explained this at least once. Other people have also explained points to you multiple times. Yet you keep asking the same questions. At this point no new questions are being asked and all of the questions asked have already been answered. So I am closing this thread. All of the answers you seek are here. You just need to take the time to carefully think through what has been said here.
 

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