I How can the Universe know when you change directions?

Click For Summary
The discussion centers on how changes in an observer's direction affect their perception of light and time. It emphasizes that different observers measure time and space differently based on their inertial frames, and this does not imply that the Universe "instantly knows" of these changes. The frequency of light perceived by an observer depends on their state of motion, not on any alteration of the light itself. The concept of a "frame of the Universe" is deemed nonsensical, as there is no universal frame of reference in physics. Ultimately, the changes in perception are a result of the observer's motion rather than any change in the light or the Universe itself.
  • #31
Nugatory said:
The best way to think about time in physics is from Einstein: “Time is what a clock measures”.
Clocks are always some form of oscillator. Math is using time as a sequence marker to describe the oscillation or periodic effect. Send a pendulum into space and the clock stops measuring what it was measuring. Remember and anticipate are in the brain. How can I see time as more than numbers on a page?
 
Physics news on Phys.org
  • #32
jnhrtmn said:
How can I see time as more than numbers on a page?
The point of Einstein's "time is what clocks measure" is to suggest that you stop philosophising and follow the evidence. Clocks are apparently measuring something because we get repeatable, predictable and consistent measurement from them.

So go back and look at the last diagram I drew. Notice how the spatial axis of the original frame isn't horizontal? That means that a ruler at rest in that frame is not measuring distance in what this frame calls space, but some mixture of space and time. Likewise, the time axis is not vertical, so clocks at rest in that frame do not measure just what this frame calls time, but some mix of space and time. The point is that it's a mistake to think of "time" as a thing in relativity. There is only spacetime. You may split it into space and time, and it's often convenient to do so, but it's an arbitrary distinction that you choose to make.

That flexibility means that there are actually several distinct concepts in relativity that more or less correspond to the Newtonian notion of time. "Proper time" (proper in the Latin sense where "property" comes from) is what clocks measure. There is a concept in spacetime closely analogous to "distance" in space, and proper time is a measure of that analogue of distance that the clock has travelled. As with ordinary distance, the distance along different paths can be different - this is the resolution of the so-called Twin Paradox, where two clocks take paths of different "length" through spacetime and have different readings at the end.

But proper time is personal - two clocks may start at the same place synchronised, separate and return, and be showing different times (not due to mechanical malfunction) when they meet again because they took routes of different "length". It is possible to define a "global" time, which we call coordinate time by having a flock of clocks at rest with respect to each other and synchronised. But it turns out that the synchronisation process is arbitrary, so that global time comes at the cost of being something you can choose differently.

Fundamentally, spacetime is a 4d manifold. Its equivalent of Pythagoras' Theorem is ##\Delta s^2=\Delta x^2+\Delta y^2+\Delta z^2-(c\Delta t)^2##, and that one term having an opposite sign is why one "direction" is different from all the others. You can't freely reverse that direction and you can't freely exchange it with the others, and that is why time is different from space.
 
  • Like
Likes Dale and cianfa72
  • #33
jnhrtmn said:
Send a pendulum into space and the clock stops measuring what it was measuring.

A "pendulum clock" is not a clock. The system of "pendulum clock" and a gravitational field is a clock, according to your own definition:
jnhrtmn said:
Clocks are always some form of oscillator.
 
Last edited:
  • Like
Likes Dale and Ibix
  • #34
jnhrtmn said:
Send a pendulum into space and the clock stops measuring what it was measuring
And when we send a wooden ruler into a sufficiently hot fire the ruler stops measuring what it was measuring.

Whether we’re measuring time or distance, we need measuring devices that won’t fail while we’re measuring. That tells us something about how we should design our measuring devices, but has nothing to do with the definitions of time as what a clock measures or distance as what a ruler measures.
 
  • Like
Likes PeroK, phinds and Sagittarius A-Star
  • #35
Ibix said:
But proper time is personal - two clocks may start at the same place synchronized, separate and return, and be showing different times (not due to mechanical malfunction) when they meet again because they took routes of different "length". It is possible to define a "global" time, which we call coordinate time by having a flock of clocks at rest with respect to each other and synchronized. But it turns out that the synchronization process is arbitrary, so that global time comes at the cost of being something you can choose differently.
Ok, therefore the flocks of clocks entirely filling the space you were talking about, are actually "at rest w.r.t. each other" as measured for instance by constant round-trip travel time of bouncing light/radar pulses exchanged between them. Otherwise which could be a different physical criterion to define "at rest w.r.t. each other" ?
 
  • #36
jnhrtmn said:
Clocks are always some form of oscillator. Math is using time as a sequence marker to describe the oscillation or periodic effect. ... How can I see time as more than numbers on a page?
Is the oscillator a number on a page? The math describes the oscillator, but the oscillator is not numbers on a page.
 
  • #37
Ibix said:
The point of Einstein's "time is what clocks measure" is to suggest that you stop philosophising and follow the evidence. Clocks are apparently measuring something because we get repeatable, predictable and consistent measurement from them.
Personally, I think that it is even more than that. The thing that clocks measure is a useful quantity. It deserves a name. That name is "time". If we didn't call it "time" then we would have to call it something else, and as a practical matter that would be the word that we use for talking about when things happen. Time.
 
  • Like
Likes Ibix, PeroK and cianfa72
  • #38
Dale said:
The math describes the oscillator, but the oscillator is not numbers on a page.
You mean that the math provides "a map" that maps what clocks read into a real number.
 
  • #39
cianfa72 said:
Ok, therefore the flocks of clocks entirely filling the space you were talking about, are actually "at rest w.r.t. each other" as measured for instance by constant round-trip travel time of bouncing light/radar pulses exchanged between them. Otherwise which could be a different physical criterion to define "at rest w.r.t. each other" ?
This is drifting into a thread hijack, but be aware that @Ibix is just providing an abridged description of Taylor and Wheeler's ("Spacetime Physics") model of an inertial frame with associated simultaneity convention.

To avoid further drift, you might want to review that section of Taylor and Wheeler and then if you have followup questions, start a new thread.
 
  • Like
Likes Vanadium 50, Ibix and PeterDonis
  • #40
Back to Doppler, it seems overcomplicated. Using 0.6c added to c gives 1.6c, (contracted length) / (speed multiplier), 0.8/1.6=0.5. The other is 0.8/0.4=2 This works throughout. Is it because1.6c can't be real, but even sqrt 1.6 is still 1.265. Using 1 instead of contracted length is the classical version. I don't understand the use of source and observer in the math if the relative velocity between the frames is the only factor.
 
  • #41
jnhrtmn said:
Back to Doppler, it seems overcomplicated. Using 0.6c added to c gives 1.6c, (contracted length) / (speed multiplier), 0.8/1.6=0.5. The other is 0.8/0.4=2 This works throughout.
Yes.
##\sqrt{1+v/c \over 1-v/c} = \sqrt{(1+v/c)(1-v/c) \over (1-v/c)(1-v/c)} = {1 \over \gamma (1-v/c)} [= \gamma (1+v/c)]##

Usually, the ##\gamma## factor in the relativistic Doppler formula is explained via time-dilation, but because of ##c=\lambda f## also an argumentation via length contraction is possible.

jnhrtmn said:
Is it because1.6c can't be real
The closing speed between 2 objects can be greater than ##c##. Only the speeds of each object relativ to the choosen inertial reference frame cannot be greater than ##c##.

jnhrtmn said:
I don't understand the use of source and observer in the math if the relative velocity between the frames is the only factor.
See
https://en.wikipedia.org/wiki/Relativistic_Doppler_effect
 
Last edited:
  • #43
jnhrtmn said:
I don't understand the use of source and observer in the math if the relative velocity between the frames is the only factor.
You need to be careful here. If you and I stand stationary near each other, we share a rest frame. I throw a ball to you. The ball has a different rest frame with a single velocity with respect to our frame. But to you, light from the ball is blue shifted while it is red shifted to me. So the ##v## in the Doppler shift formula cannot be a frame velocity since we couldn't get different Doppler shifts if it were. And we could get opposite Doppler shifts by reversing our ##x## axes so the velocity switched from ##+v## to ##-v##.

The ##v## in the Doppler shift formula is the closing rate (or separation rate, depending on your sign convention) of the source with respect to a specific observer, not a frame velocity. It will typically be equal to plus-or-minus the velocity of the source's rest frame in the observer's frame, but it is a distinct concept.
 

Similar threads

  • · Replies 4 ·
Replies
4
Views
1K
  • · Replies 15 ·
Replies
15
Views
2K
  • · Replies 20 ·
Replies
20
Views
2K
  • · Replies 13 ·
Replies
13
Views
3K
  • · Replies 51 ·
2
Replies
51
Views
4K
  • · Replies 45 ·
2
Replies
45
Views
6K
  • · Replies 15 ·
Replies
15
Views
2K
  • · Replies 6 ·
Replies
6
Views
2K
Replies
8
Views
1K
  • · Replies 5 ·
Replies
5
Views
2K