Relativity for people who insist on having a true physical time

In summary, the conversation discusses a way to have both relativity and a "true physical time" and "true physical distance". This is achieved by picking a frame of reference and treating it as the "one true physical frame" in which the rods have their true physical length and the clocks are synchronized. Lorentz contraction and time dilation are considered to be true physical effects and the usual equations are used. However, this approach may have limitations in applying Newton's laws of motion in multiple frames of reference and may not generalize to general relativity.
  • #1
pervect
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Relativity for people who insist on having a "true physical time"

OK, here is the promised thread, on how to have both relativity and a "true physical time" and "true physical distance". The basic idea is really quite simple.

Pick a frame of reference. Pick any frame of reference.. Say that that particular frame of reference is the one that keeps "true physical time". Say that the rods in that particular frame of reference have "their true physical length".

Treat lorentz contraction and time dilation as "true physical effects". Use the usual equations for them. Any rod that is not in the "one true physical frame" has it's length contracted by virtue of its motion by a factor of gamma = 1/sqrt(1-(v^2/c^2) (the lengthis divided by gamma). A clock that's moving is slowed down by the factor of gamma as well.

Make sure that all clocks are synchronized in the "true physical frame".

Make sure that if you apply Newton's laws of motion, you only do so in the "true physical frame".

The result will be equivalent to relativity. The biggest drawback is being able to apply Newton's laws only in the one frame. There may be a way to fix this, but it's not clear to me yet what it is.

Of course, the choice of which particular frame is the "true physical frame' is completely arbitrary, as long as one is consistent. The "true physical frame" must of course never accelerate, it must always be a frame in the Newtonian sense.

ps - personaly, I think this approach is a bit of a dead end, though it does have a very few proponents, such as Bell, who insists that this general approach helped him formulate the Bell inequality. But we seem to see a small but significant number of peole who seem to be "stuck" in absolute time, this viewpoint would be one way for them to do special relativity correctly. (I don't think the approach will generalize well to general relativity, however).
 
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  • #2
pervect said:
OK, here is the promised thread, on how to have both relativity and a "true physical time" and "true physical distance". The basic idea is really quite simple.

Pick a frame of reference. Pick any frame of reference.. Say that that particular frame of reference is the one that keeps "true physical time". Say that the rods in that particular frame of reference have "their true physical length".

Treat lorentz contraction and time dilation as "true physical effects". Use the usual equations for them. Any rod that is not in the "one true physical frame" has it's length contracted by virtue of its motion by a factor of gamma = 1/sqrt(1-(v^2/c^2) (the lengthis divided by gamma). A clock that's moving is slowed down by the factor of gamma as well.

Make sure that all clocks are synchronized in the "true physical frame".

Make sure that if you apply Newton's laws of motion, you only do so in the "true physical frame".

The result will be equivalent to relativity. The biggest drawback is being able to apply Newton's laws only in the one frame. There may be a way to fix this, but it's not clear to me yet what it is.

Of course, the choice of which particular frame is the "true physical frame' is completely arbitrary, as long as one is consistent. The "true physical frame" must of course never accelerate, it must always be a frame in the Newtonian sense.

And just how is this "equivalent to relativity"?
In your reply, it might be helpful if you include the definition of "relativity" you are trying to use, as well as definitions for "true physical time" and "true physical distance". (Operational definitions and mathematical definitions are preferred.)
 
  • #3
pervect,

Newton's Laws only approximate reality when things aren't moving very fast. That fact will not be changed in any inertial reference frame you wish to choose. For example, if you have two charged particles approaching each other at relativistic speeds you cannot find any inertial frame of reference in which the interaction is Newtonian.
 
  • #4
robphy said:
And just how is this "equivalent to relativity"?
In your reply, it might be helpful if you include the definition of "relativity" you are trying to use, as well as definitions for "true physical time" and "true physical distance". (Operational definitions and mathematical definitions are preferred.)

Pick a frame, any frame, and declare it to be the "one true frame". That's the definition. (We know that the aether isn't detectable, so the good news is we can define it any way we like -- since it has no physical consequences, it's basically a mental crutch for those who need crutches).

It's equivalent to relativity because we are essentially using the Lorentz transformations, just changing the philosophical baggage around a bit.

i.e.
x' = gamma*(x-vt), t'=gamma*(t-vx)

It doesn't really matter what we call 'real', as long as we can get the right answer.

My particular formulation didn't really address the clock synchronization issue, except by not allowing people to use anything other than one frame. This could probably be improved, it's extremely useful to be able to use more than one frame. Since I personally don't use this formulation (I think it's a bit of a dead end if one wants to progress beyond special relativity), I'd have to think some more about the best way to "wrap it up". I'm not sure of the origin of this formulation, but one of its main proponents was Bell.
 
  • #5
Tide said:
pervect,

Newton's Laws only approximate reality when things aren't moving very fast. That fact will not be changed in any inertial reference frame you wish to choose. For example, if you have two charged particles approaching each other at relativistic speeds you cannot find any inertial frame of reference in which the interaction is Newtonian.

A couple of good points, as if we can't switch frames, we'll always have to deal with situations where things are moving very fast. So I think we'd have to re-define momentum to be gamma*m*v, instead of m*v.

We don't currently teach people electrodynamics until after they've had basic relativity, so I'm not sure how much of this I would want to explain. We'd basically have the usual effects of electric field lines getting "squished", we'd just describe this as being a "real" squish. We'd still need the magnetic field, and we'd still need the electromagnetic field to carry energy and momentum to "balance the books", but we already need that.

Probably I'd need to be able to provide at least a consistent philosophical interpretation of Maxwell's equations to make the scheme viable. Since I don't actually think about relativity in this way, I'd have to scratch my head for a bit to come up with this, but I'm pretty sure it's possible.




,
 
  • #6
That was just an example. Replace the charged particles with relativistic billiard balls and you're back to the same problem! :-)
 
  • #7
Your suggestion is that in order to arrive at the same result as SR we use instead the modified Lorentz Ether Theory (actual physical contraction and actual time dilation). Since this theory uses the same equations as SR, you get the same answers - at least in most cases. This theory still has a following though it be a minority - it does simplify the twin and triplet problem because there is no need to speculate as to the effects of acceleration - time dilation being actual, the moving twin's clock always runs slow relative to the universal ether frame where light is defined as isotropic. The hard part to swallow is just what is themechanism responsible for actual physical contraction - this so bothered the early thinkers that they rapidly gravitated toward SR as a better way to envision the world (to make a pun).
 

1. What is the theory of relativity?

The theory of relativity is a cornerstone principle in modern physics that explains the relationship between time and space. It was developed by Albert Einstein in the early 20th century and is divided into two parts: the Special Theory of Relativity and the General Theory of Relativity.

2. How does relativity affect our understanding of time?

Relativity states that time is not absolute, but rather is relative to the observer's frame of reference. This means that time can appear to pass differently for different observers depending on their relative motion and the strength of gravity in their location.

3. What is the concept of time dilation in relativity?

Time dilation is a phenomenon predicted by the theory of relativity where time appears to pass slower for objects in motion or in strong gravitational fields. This effect has been confirmed through numerous experiments and has significant implications for space travel and GPS technology.

4. Does relativity disprove the existence of absolute time?

Yes, according to the theory of relativity, there is no absolute time that applies universally to all observers. Instead, time is relative and can only be measured in relation to the observer's frame of reference.

5. How does relativity impact our understanding of the universe?

Relativity has revolutionized our understanding of the universe, providing a more accurate and comprehensive model of how space, time, matter, and energy interact. It has also led to advancements in technology, such as GPS and atomic clocks, and has opened up new areas of research, such as black holes and the Big Bang theory.

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