matheinste
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Hello hartlw.
The above is what is actually predicted by SR and so is what happens. I have no idea how physicists observe it.
Matheinste
The discussion centers on the concept of absolute time in relation to General Relativity, asserting that absolute time does not exist as different observers perceive time differently. Key points include the designation of standard time frames such as Greenwich Mean Time and the Earth Centered Inertial frame for GPS systems. The speed of light is identified as the only constant across the universe, suggesting it could serve as a universal time standard in the future. The conversation also emphasizes that time is relational and dependent on the existence of space, energy, and matter, with no absolute reference frame available for measuring time.
PREREQUISITESThis discussion is beneficial for physicists, cosmologists, and anyone interested in the philosophical implications of time in the context of relativity and cosmology.
hartlw said:My answer to the question:
Absolute time is the distance of a spherical light wave from its center measured by an observer at the center.
Distance is the size of the particle which emitted the light wave at the time it emitted the light wave. It is assumed that distance can be preserved by the observer at the center of the light wave.
hartlw said:It would be nice to dispense with the size of the particle and just say that absolute time is the size of the light wave with respect to its center. But you can't quantify this unless you can uniqueley identify a particular position of the light wave.
That would just be relative to the observer at the center.hartlw said:say that absolute time is the size of the light wave with respect to its center.
ckollerer said:Can we agree that "absolute time" began with the big bang? The big bang's origin then would be the point of inertia, prior to all movement. "Absolute distance" is referenced to that one point in the universe. "Absolute speed" is referenced to that point of zero speed prior to the beginning of time. SR still holds.
Of course, identifying that point of zero-time origin is the trick. Since we are not likely to identify the origin of the universe, then, sadly,"absolute time" is not identifiable or quantifiable, only a hypothetical marvel. Nonetheless, the possibility of "absolute time" exists. And this answers the OP's question, albeit sans scientific usefulness.
The Dagda said:Because of the nature of the singularity we could not be sure exactly when it began even if we knew, at least to pin it down exactly. So no. The possibility of absolute time does not exist and it never has. Even at t=10-87 it was subject to relativistic concerns anyway.
ckollerer said:I think we agree, except for the definition of "possible." To me, just because something is impossible to identify or measure does not preclude the possibility of its existence.
The Dagda said:Philosophical possibilities are best left to the appropriate area of the forum. In this case SR would have to be violated and the quantum mechanics of the singularity for it to be possible. I can't say absolutely it doesn't exist in another universe, or that it has never existed. But I can say it's pointless arm waving. Logically speaking anything can exist, and science cannot prove something doesn't exist. But then that's the remit of philosophers: to argue the unarguable.
No, I don't agree. The current estimate is that the big bang occurred 13.7 billion years ago. So, which law of physics would be different in a coordinate system where the current time t=13.7 billion years vs t=0? If you cannot identify such a law then that is not absolute time.ckollerer said:Can we agree that "absolute time" began with the big bang?
DaleSpam said:The point of the principle of relativity is that you can do physics in whatever coordinate system you like. You don't need to determine irrelevant details like the age of the universe in order to calculate the acceleration of a box sliding down a frictionless inclined plane.
hartlw said:I believe the question was is there the possibility of "absolute time."
Taking into account relativity, no matter how small the effect, how do you calculate the acceleration of a box sliding down a frictionless plane.
DaleSpam said:No, I don't agree. The current estimate is that the big bang occurred 13.7 billion years ago. So, which law of physics would be different in a coordinate system where the current time t=13.7 billion years vs t=0? If you cannot identify such a law then that is not absolute time.
The point of the principle of relativity is that you can do physics in whatever coordinate system you like. You don't need to determine irrelevant details like the age of the universe in order to calculate the acceleration of a box sliding down a frictionless inclined plane.
hartlw said:Time is not an abstract philosophical concept.
Without a specific definition of time physical theories are meaningless. How can you discuss motion without a specific definition of time? The objective is to come up with a reasonable definition of time in an arbitrary coordinate system.
hartlw said:Without a specific definition of time physical theories are meaningless. How can you discuss motion without a specific definition of time? The objective is to come up with a reasonable definition of time in an arbitrary coordinate system.
hartlw said:Create a frame in a vacuum with a fluorescent marker at an equal distance on each of the three axes. Let a flash of light occur at the origin. If the observer at the origin sees all the flashes return simultaneously, a repeatable time interval, clock, is established in this frame. Define this particular frame and the distance and time interval as absolute. Proceed from there. Good luck. Let me know how you make out.
Easy, use Newton's 2nd law, f=dp/dt. You can use 3-vectors for the Newtonian version or 4-vectors if you want to be anal about it and include the SR corrections, but the law is the same in either case.hartlw said:Taking into account relativity, no matter how small the effect, how do you calculate the acceleration of a box sliding down a frictionless plane.
This is absurd.hartlw said:Create a frame in a vacuum with a fluorescent marker at an equal distance on each of the three axes. Let a flash of light occur at the origin. If the observer at the origin sees all the flashes return simultaneously, a repeatable time interval, clock, is established in this frame. Define this particular frame and the distance and time interval as absolute. Proceed from there.
Do you not see the blatantly obvious problem here? As you noticed there is no physical basis on which to choose one over the other. Therefore neither can be absolute.hartlw said:Refer the second to the first. Or make the second absolute. Then refer the first to the second.
matheinste said:Perhaps an agreed definition of absolute time may be useful here.
Matheinste
Reference frames, coordinates and the Lorentz transformation
Relativity theory depends on "reference frames". A reference frame is an observational perspective in space at rest, or in uniform motion, from which a position can be measured along 3 spatial axes. In addition, a reference frame has the ability to determine measurements of the time of events using a 'clock' (any reference device with uniform periodicity).
An event is an occurrence that can be assigned a single unique time and location in space relative to a reference frame: it is a "point" in space-time. Since the speed of light is constant in relativity in each and every reference frame, pulses of light can be used to unambiguously measure distances and refer back the times that events occurred to the clock, even though light takes time to reach the clock after the event has transpired.
For example, the explosion of a firecracker may be considered to be an "event". We can completely specify an event by its four space-time coordinates: The time of occurrence and its 3-dimensional spatial location define a reference point. Let's call this reference frame S.
In relativity theory we often want to calculate the position of a point from a different reference point.
Suppose we have a second reference frame S', whose spatial axes and clock exactly coincide with that of S at time zero, but it is moving at a constant velocity v\, with respect to S along the x\,-axis.
Since there is no absolute reference frame in relativity theory, a concept of 'moving' doesn't strictly exist, as everything is always moving with respect to some other reference frame. Instead, any two frames that move at the same speed in the same direction are said to be comoving. Therefore S and S' are not comoving.
hartlw said:Define this particular frame and the distance and time interval as absolute. Proceed from there.
hartlw said:You have to be practical. Like the std meter and the std mass.
Accelerate the std meter in Paris to .75c and then call it the standard (absolute) meter. The real problem is communicating (measuring) between frames. An absolute reference allows you to do this. Just define one as absolute.
matheinste said:I agree with you The Dagda. Such a thing as absolute time does not exist in SR and so is undefinable in SR. However hartlw obviously has his own example of what he considers to be absolute time so it may be worth asking for his general definition rather than a specific example.
Matheinste.