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Gravity's Effect on Time

  1. Jun 15, 2011 #1
    Im having a hard time understanding gravitational time dilation. I have two examples I've heard(from shows on the science channel): a theoretical experiment is you leave earth in a space ship and orbit outside the event horizon of a black hole for 1 year, its possible that when you come back to earth its been 10 years or even 100 years on earth when its been only 1 year for you. This shows that as gravity increases time slows down for the person next to the black hole because of the black holes large mass? But this contradicts the fact that when astronauts orbit the earth in the space station they are technically, however small the measurement, younger than us on earth, so they age slower? Because the farther away from earth you are the less stronger gravity is? So this is saying that the less gravity the more time slows, which contradicts the black hole experiment that says more gravity has this effect on time. Can someone please explain this relationship.
     
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  3. Jun 15, 2011 #2

    WannabeNewton

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    The astronauts age relatively slower because they are orbiting the earth at high speeds not because they are in a stronger gravitational field. The earth's gravitational field is too weak to cause any kind of significant time dilation.
     
  4. Jun 15, 2011 #3
    Oh thankyou i understand now. So does that mean the theoretical experiment about the black hole is true?
     
  5. Jun 15, 2011 #4

    WannabeNewton

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    I don't know the exact number but yes the premise is very true.
     
  6. Jun 15, 2011 #5
    I read somewhere on PF that atomic clocks on earth can detect a height difference of as little as three feet.
     
    Last edited: Jun 15, 2011
  7. Jun 15, 2011 #6

    bcrowell

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    This is incorrect. The gravitational and kinematic time dilation effects are of comparable orders of magnitude for satellites in earth orbit. For satellites in low earth orbit (which includes almost all crewed activity), the kinematic effect dominates. But for satellites in higher orbits (e.g., GPS and geosynchronous satellites), the gravitational effect dominates.

    -Ben
     
  8. Jun 15, 2011 #7

    PAllen

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    The black hole case would combine two sources of differential aging. Consider there is a black hole a light year away, that is stationary relative to sun (say, by doppler definition). Ship A goes near the black hole (not too close), circles a while, and comes back to earth. Ship B goes a light year in the opposite direction, circles similarly* and comes back to earth. Both pilots will have aged less than their earth colleagues, but A pilot will have aged less than B pilot.

    *Similarly: Near the black hole, measure speed of A relative to a momentarily coincident (NOT comoving) radial free fall frame (with zero instantaneous radial velocity compared to a coincident stationary observer). In the opposite direction, measure speed (in presumably empty region), relative to sun. The aim is to measure speeds from local Minkowski frames.
     
    Last edited: Jun 15, 2011
  9. Jun 15, 2011 #8

    pervect

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    One interesting side-note. You can't really get much differential aging due to "gravitational time dilation" if you insist on orbiting a black hole, because the photon sphere is at r=3M, and the "gravitational time dilation there" is sqrt(2M/r) = sqrt(2/3).

    While you could get a long time dilation orbiting a black hole near the photon sphere, this would come from your velocity more than the gravitational effect.


    If you consider traveling deep in a black hole's gravity well using rocket thrust, rather than orbiting it, you can get large time dilations due to the gravitational effect.

    The gravitational effect is not due to "gravity", but is better (though someone loosely) described as being due to "gravitational potential". For instance, you'll have a maximum value of time dilation due to gravity on Earth at its center, even thought the gravity there is zero.

    The "gravitational time dilation" is really due to curvature of space-time, but as long as you only consider static observers it's not too terribly misleading to use coordinate time as your base for time and think of physical clocks as ticking faster or slower than coordinate clocks. Pretty much everyone does this, I think.

    Philosophically, though, there's a lot to be said for thinking of the physical clocks as being the "more real" clocks, in which case they always tick at 1 second per second. With this point of view, it's the coordinate clocks that are "off" due to the effects of curvature.
     
  10. Jun 15, 2011 #9

    WannabeNewton

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    My apologies.
     
  11. Jun 15, 2011 #10
    Just to make it clear, WN is correct that astronauts (usually in low orbit) would age slower than people on the ground, but erred a bit when he said Earth's gravitational time dilation effect is insignificant, because gravitational time dilation can dominate at higher orbits. However if you were to be charitable, you could interpret WN to mean gravitational time dilation is less significant than kinematic time dilation, in low orbits where astronauts usually work.
     
  12. Jun 15, 2011 #11

    PAllen

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    Right, which is why I proposed circling with a rocket, rather than orbiting. That way you can make either components (speed, gravity) towards differential aging a large as you want.

    One question is that I get sqrt(1/3) for the innermost unstable circular orbit, sqrt(2/3) for the innermost stable circular orbit. It is the former where the orbital velocity approaches lightspeed. I could have goofed, so let me know.
     
  13. Jun 15, 2011 #12
    I am not sure about the philosophical desirability of this this interpretation. Let us say we have a clock (A) very far from a gravitational source that remains stationary and call this the coordinate clock.

    Now let us lower another clock (B) close to the gravitational source such that clock A seems to be ticking 10 times faster than clock B from B's point of view and clock B appears to be ticking 10 times slower from A's point of view. We interpret this as clock A speeding up by a factor of 10 while clock B continues to tick at 1 second per second. (clock B undergoes no change).

    Let lower one more clock (C) even closer to the gravitational source so that from A's point of view C's clock is ticking 100 times slower and from C's point of view A's clock is ticking 100 times faster. We interpret this as clock A speeding up by a factor of 100 while clock C continues to tick at 1 second per second. (clock C undergoes no change).

    Now we have agreed that neither clock B nor clock C have undergone any sort of change and yet they are ticking at different rates to each other when initially they were ticking at the same rate when they were adjacent to each other. They have changed, but they have not changed. A bit paradoxical.

    Meanwhile clock A, that has remained stationary all the while, is now the one that is really ticking 10 times faster relative to B and ticking 100 times faster relative to C. Since clocks B and C have undergone no change, clock A must be doing all the changing even though it is the only clock that that has no reason to change because it has not changed its velocity or gravitational potential. If A was originally ticking at 1 second per second what is its clock rate now? Is it 10 seconds per second which is what B says it is or is it 100 seconds per second which is what C says it is? Again, a bit paradoxical. Alternatively we say all clocks tick at one second per second (in their own rest frame) independent of their relative motion or gravitational potential which makes things a lot simpler, but completely glosses over the fact that clocks are measured to run at different rates.

    To me it makes a whole lot more sense to say that the tick rates of clocks B and C change because they are the clocks that have changed their location in the gravitational field. This explains why the tick rates of both B and C have changed relative to each other (from everyone's point of view). Clock A, that has undergone no change in velocity or gravitational potential undergoes no change in tick rate, because it has no reason to. I think the main reason this common sense interpretation is avoided, is because when followed to its conclusion, it implies that clocks stop ticking at the event horizon and that is a bit awkward.
     
  14. Jun 15, 2011 #13

    bcrowell

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    Not trying to be too hard on WN. Charitability isn't one of my strong points :-)
     
  15. Jun 15, 2011 #14
    The help you give people here and the educational information you provide on your website seems pretty charitable to me :wink:
     
  16. Jun 16, 2011 #15

    pervect

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    Time for one of my favorite analogy.

    You're on the surface of the Earth, and you mark off coordinates for lattitude and longitude. You have a sailing ship on the equator, and it covers 20 arc-minute of longitude in 1 hour.

    You move up to closer to the north pole - and you observer it covers 40 arc-minutes of longitude in 1 hour.

    If we followed the same rules that we did for time dilation we'd be talking about "distance contraction" as the ship moved further up north.

    This idea wouldn't be totally wrong, at least not for navigational purposes, but aside from navigation, it'd be pretty confusing to think of your meter stick as changing as you moved north and south. One might even say it was wrong, for anything except navigational purposes. And, we don't actually do that. Nor do we say that "ships go faster near the North pole", or anything like that. We recognize that the "real" speed of the ships is the same near the poles and near the equator, that this speed is independent of the coordinates we use to describe the surface of the Earth, and that a meter is also independent of the coordinates, and that what happens is that we need to convert coordinate arc-minutes into physical meters by a conversion factor that depends on lattitude - the spatial "metric" of the Earth.

    And we might well explain this phenomenon briefly just by saying that the paths we draw in order to compare the distances are curved.

    In relativity, it's the concept of a static observer that allows us to compare the distant clocks at all, and it's this particular concept of time comparison, the particular concept of simultaneity used by static observers, that makes the physical clocks deeper in the gravity well appear to run slowly when measured according to "coordinate time".
     
  17. Jun 16, 2011 #16
    Commenting on:
    "Philosophically, [..] there's a lot to be said for thinking of the physical clocks as being the "more real" clocks, in which case they always tick at 1 second per second. [..]"
    I fully agree - but hey it appears to be a matter of how one's brains are wired. :tongue2:

    Pervect commented:
    I don't see that example as support for "always 1 second per [nominal] second". In this example it would be "always N meters per degree longitude". And that's obviously not true. So, my brain is wired differently from yours. :biggrin:

    Moreover the interpretation that clocks near mass tick slower than clocks far from mass (ceteris paribus), is independent of the observer and independent of the units.

    Harald
     
  18. Jun 16, 2011 #17
    That is a really good analogy, requires a fair bit of background knowledge. But conceptualy really gets the main points across.
     
  19. Jun 16, 2011 #18

    pervect

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    The interpretation that clocks near mass tick slower than clocks far away is not independent of the observer, if one includes relativistically moving observers. It is only for the special class of static observers that it really works, when there's a "special" method of comparing them that defines simultaneity.

    One of the points of the analogy is that the Schwarzschild coordinates (r, theta, and phi) are just coordinates, like lattitude and longitude.

    To put the coordinate description before the actual physics of what you measure with real instruments is quite literally putting DesCartes before the horse :-).
     
  20. Jun 16, 2011 #19

    bcrowell

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    Oh...no...
     
  21. Jun 17, 2011 #20
    Evidently an elaboration is necessary: I wrote ceteris paribus and that includes relativistically moving observers. Surely all observers agree that clocks tick slower near co-moving masses; this is the actual physics of what you will measure with real instruments.
    Else you would get the kind of contradictions that the OP imagined. :tongue2:
     
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