TIME DILATION. WHY do clocks that are

  • #151
Ernst Jan said:
If a light source moves from back to front it has no effect on the speed of the light, but if a light source moves sideways there suddenly is some mysterious sideways velocity of the light.
You are comparing apples with oranges here. Look at the animation again:

[URL]http://home.earthlink.net/~parvey/sitebuildercontent/sitebuilderpictures/length_con2.gif[/URL]

- The "speed" (magnitude of velocity vector) is the same for all 4 photons, regardless how they where emitted.

- The individual velocity vector components of the two "vertically" emitted photons are different. But that has nothing to do with "source velocity affecting the light". It is simply a consequence of the fact that direction of a velocity vector is frame dependent (even in Newtonian mechanics).

After all, all observers must agree that the photon hit the mirror. Otherwise you get contradictions.
 
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  • #153
A.T. said:
You are comparing apples with oranges here. Look at the animation again:

[URL]http://home.earthlink.net/~parvey/sitebuildercontent/sitebuilderpictures/length_con2.gif[/URL]

- The "speed" (magnitude of velocity vector) is the same for all 4 photons, regardless how they where emitted.

- The individual velocity vector components of the two "vertically" emitted photons are different. But that has nothing to do with "source velocity affecting the light". It is simply a consequence of the fact that direction of a velocity vector is frame dependent (even in Newtonian mechanics).

After all, all observers must agree that the photon hit the mirror. Otherwise you get contradictions.

This animation is exactly what I mean, it proves my point doesn't it?
In the stationary frame you follow the photon going straight down and in the moving frame you follow the photon going in an angle, exactly like I said.

If you're suggesting that in both frames the observer would see the photons hit the mirror after exactly the same time then we disagree and your animation shows I'm right?
 
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  • #154
  • #155
harrylin said:
I don't think so; SR makes no claims about what "really is" and merely pretends that we cannot identify such an observer. Please show me wrong. :wink:

With time dilation and length contraction it seems no longer possible to see what a 3 dimensional space looks like for a "universal observer", these are real physical effects right?
 
  • #156
Ernst Jan said:
This animation is exactly what I mean, it proves my point doesn't it?
No idea what your point is. But you seemed to compare "speed"(for photons the same in every frame) and "velocity components"(can vary between frames). The velocity of the source doesn't come in here.

Ernst Jan said:
In the stationary frame you follow the photon going straight down and in the moving frame you follow the photon going in an angle, exactly like I said.
What do you mean by "follow a photon in some frame"?

Ernst Jan said:
If you're suggesting that in both frames the observer would see the photons hit the mirror after exactly the same time ...
No, I never suggested that.
 
  • #157
A.T. said:
No idea what your point is. But you seemed to compare "speed"(for photons the same in every frame) and "velocity components"(can vary between frames). The velocity of the source doesn't come in here.
I said that the animation in my original post compared 2 different photons, exactly like in your animation.

What do you mean by "follow a photon in some frame"?
I mean the photon going between two mirrors. With stationary frame I mean the mirrors that are stationary and with moving frame I mean the mirrors that are moving.

No, I never suggested that.
Good, but why do you think there are any contradiction?
To me it seems we're saying exactly the same thing.
 
  • #158
Ernst Jan said:
This animation is exactly what I mean, it proves my point doesn't it?
In the stationary frame you follow the photon going straight down and in the moving frame you follow the photon going in an angle, exactly like I said.

If you're suggesting that in both frames the observer would see the photons hit the mirror after exactly the same time then we disagree and your animation shows I'm right?

I still don't see of what you should be convinced; but you seem to mean with such jargon something else as the others! In such cases it's better to abstain from jargon and to spell everything completely out. Thus:

Let's call S1 the "stationary" system because we choose it for our reference, and S2 the "moving" system system.

Then:
- as measured with S1, we observe the one light pulse going straight down wrt our system S1.
- also as measured with S1, we observe the other light pulse going under an angle wrt our system S1, but straight down wrt S2 (the y coordinates of that light pulse and the mirror are at every time the same).
- consequently, as measured with S2, one will observe that other light pulse also to go straight down wrt S2.

- We can measure "time" with for example such oscillators; as a result, according to our perception (measurements), the clocks that are at rest with S2 run at half the speed as the ones that are at rest with our system.

Note that due to the different reference standards in which the same situation is measured with S2, observers using S2 will conclude just the opposite, that is, that clocks that are at rest with S1 run at half the speed as the ones that are at rest with S2; that's however another topic which has also been discussed many times because it's at first sight mind-boggling or even paradoxical ("mutual" or "symmetric" time dilation). It's a direct requirement of the relativity principle.
 
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  • #159
Ernst Jan said:
Good, but why do you think there are any contradiction?
I think it is misleading to the bring movement of the light source into it, like you do here;
Ernst Jan said:
but if a light source moves sideways there suddenly is some mysterious sideways velocity of the light.
To see the the movement of the light source is irrelevant, you can change the experiment: Instead of two vertical light clocks in relative horizontal movement, you have two long parallel mirrors, with two photons jumping between them:

FRAME A (rest frame of the mirrors):
- photon A is going vertically up & down
- photon B is zig-zaging at 45° to the right

FRAME B (moving to the right relative to the mirrors):
- photon A is zig-zaging at 45° to the left
- photon B is going vertically up & down

As you see the movement of the photons it perfectly symmetrical, between the two frames, despite the fact that in one frame the mirrors are static while moving in the other frame. So the movement of the source doesn't affect how the light propagates.

This is easier to see when you consider a 360° light pulse, instead of single photon.
 
  • #160
Ernst Jan said:
With time dilation and length contraction it seems no longer possible to see what a 3 dimensional space looks like for a "universal observer", these are real physical effects right?

Perhaps you mean that if we assume the existence of an "absolute" reference, according to SR we cannot know which point of view corresponds to it? Indeed, at least not by measurements. However, I think that according to cosmology it makes sense to postulate that the centre of mass of the universe corresponds to the origin of such a frame (maybe someone else here knows of that?).

In any case, the point of Newtonian physics was that observers who use instead an inertial system will observe exactly the same laws of nature as such such an universal observer - that's the PoR, that any inertial frame is equally suited for using the laws of physics. And this is the same in SR.
 
  • #161
commenting on:
"if a light source moves sideways there suddenly is some mysterious sideways velocity of the light."
A.T. said:
I think it is misleading to the bring movement of the light source into it, like you do here;

To see the the movement of the light source is irrelevant, you can change the experiment: Instead of two vertical light clocks in relative horizontal movement, you have two long parallel mirrors, with two photons jumping between them:

FRAME A (rest frame of the mirrors):
- photon A is going vertically up & down
- photon B is zig-zaging at 45° to the right

FRAME B (moving to the right relative to the mirrors):
- photon A is zig-zaging at 45° to the left
- photon B is going vertically up & down

As you see the movement of the photons it perfectly symmetrical, between the two frames, despite the fact that in one frame the mirrors are static while moving in the other frame. So the movement of the source doesn't affect how the light propagates.

This is easier to see when you consider a 360° light pulse, instead of single photon.

Not completely correct: the motion of the source does affect the direction of light rays, even for uniform light sources (but that is nothing mysterious, it's conservation of momentum). A moving uniform light source will show a "head light" effect. I thought it was mentioned in the physics FAQ but now I can't find it back... so I'll hopefully not link to crank site by giving a link from Google here:
http://www.adamauton.com/warp/lesson5.html
 
  • #162
Ernst Jan said:
Thanks, this was the answer I was hoping for. Too bad there are a lot of experiments in the link, could you say which of them contradict my view please, or did you mean all of them?
The idea of a privileged observer violates the first postulate, which is the specific subject of the tests in sections 3.1, 3.2, 3.5, and 3.6. However, in a broader sense you recognized the incompatibility of your idea with SR, and all of the tests confirm SR.
 
  • #163
harrylin said:
I still don't see of what you should be convinced; but you seem to mean with such jargon something else as the others! In such cases it's better to abstain from jargon and to spell everything completely out. Thus:

Let's call S1 the "stationary" system because we choose it for our reference, and S2 the "moving" system system.

Then:
- as measured with S1, we observe the one light pulse going straight down wrt our system S1.
- also as measured with S1, we observe the other light pulse going under an angle wrt our system S1, but straight down wrt S2 (the y coordinates of that light pulse and the mirror are at every time the same).
- consequently, as measured with S2, one will observe that other light pulse also to go straight down wrt S2.
I think this is how everyone interprets the animation.

- We can measure "time" with for example such oscillators;
According to my "universal observer" you can't do this. The reason seems obvious; the photons do not hit the mirrors at the same time.

as a result, according to our perception (measurements), the clocks that are at rest with S2 run at half the speed as the ones that are at rest with our system.
Under the premisse that you can measure "time" with for example such oscillators, you will get no argument from me.

My question I started with is why you would assume you can measure time like that.
Like I explained earlier is stating that you can, doesn't seem like much of an explanation.
 
  • #164
DaleSpam said:
The idea of a privileged observer violates the first postulate,
I know, my question is why would you think the first postulate is true.

which is the specific subject of the tests in sections 3.1, 3.2, 3.5, and 3.6.
Thanks, I hope to find my answer there then :)

However, in a broader sense you recognized the incompatibility of your idea with SR, and all of the tests confirm SR.
Yeah, we can agree to that, but I was hoping you'd tell me which of those test disagree with my view. Since my view also explains that atomic clocks will slow down with high speed.
 
  • #165
Ernst Jan said:
My question I started with is why you would assume you can measure time like that.
How would you measure time? What kind of clock would you use?

Let's say your "correct" clock is placed right next to a light clock, and synchronized so they both tick in sync in their common rest frame. Wouldn't then all observers have to agree that they tick in sync? Otherwise you could easily create paradoxes.

If the clocks stay synchronized in every frame, what difference does it make, if we use your "correct" clock or a light clock to measure time?
 
  • #166
Ernst Jan said:
Since my view also explains that atomic clocks will slow down with high speed.
I have been following this thread since you made your first post and I cannot tell what your view is. Could you express it again, one more time, with no reference to previous explanations so that hopefully, I, and possibly others will understand what you are promoting, please?

And one more question: does your view explain how slowed down atomic clocks moving at high speed will measure the stationary atomic clocks as being slowed down by the same amount? In other words, do you understand that time dilation is reciprocal?
 
  • #167
A.T. said:
How would you measure time? What kind of clock would you use?

Let's say your "correct" clock is placed right next to a light clock, and synchronized so they both tick in sync in their common rest frame. Wouldn't then all observers have to agree that they tick in sync? Otherwise you could easily create paradoxes.

If the clocks stay synchronized in every frame, what difference does it make, if we use your clock or a light clock?

A "correct" clock would be a clock that would show a "universal observer" that one second has passed when the Earth has made (1/24 * 1/60 * 1/60=) 1/86400 of a rotation.

Let's agree that I can't stop time by smashing a clock, so that a clock does not necesarrily tell the "correct" time.
 
  • #168
ghwellsjr said:
does your view explain how slowed down atomic clocks moving at high speed will measure the stationary atomic clocks as being slowed down by the same amount? In other words, do you understand that time dilation is reciprocal?

Your question is a bit strange, since measuring implies actually looking at the clock. It brings up all kinda new problems like the Doppler effect. Let's just keep looking at it as if an observer just knows what's happening.

Obviously, in my view only the clock moving at high speed will slow down. If you would bring those clocks together you could check that this is indeed the case.
 
  • #169
Ernst Jan said:
ghwellsjr said:
does your view explain how slowed down atomic clocks moving at high speed will measure the stationary atomic clocks as being slowed down by the same amount? In other words, do you understand that time dilation is reciprocal?
Your question is a bit strange, since measuring implies actually looking at the clock. It brings up all kinda new problems like the Doppler effect.
Well, yes, measuring does imply actually looking at the clock. But the Relativistic Doppler effect is a solution (not a problem) to how each clock, moving in relation to each other, sees and measures what the other clock is doing. Do you deny that Relativistic Doppler comports with reality?
Ernst Jan said:
Let's just keep looking at it as if an observer just knows what's happening.
If you believe in an absolute ether rest state in which there is a single absolute definition of time and space, you need to tell us how to identify it. Otherwise, it's your opinion against everyone else's as to what's happening.
Ernst Jan said:
Obviously, in my view only the clock moving at high speed will slow down. If you would bring those clocks together you could check that this is indeed the case.
And which is the clock that is moving at high speed? And there is more than one way to bring those two clocks together and depending on how you do it, you can determine that either one is the one that was slowed down.
 
  • #170
Ernst Jan said:
A "correct" clock would be a clock that would show a "universal observer" that one second has passed when the Earth has made (1/24 * 1/60 * 1/60=) 1/86400 of a rotation.
So you want to use the Earth's rotation as a clock. Well anything I said still applies:

Let's say your "correct" clock is placed right next to a light clock, and synchronized so they both tick in sync in their common rest frame. Wouldn't then all observers have to agree that they tick in sync? Otherwise you could easily create paradoxes. If the clocks stay synchronized in every frame, what difference does it make, if we use your clock or a light clock?

Ernst Jan said:
Let's agree that I can't stop time by smashing a clock,.
But by smashing the Earth?

Ernst Jan said:
so that a clock does not necesarrily tell the "correct" time.
So who does tell the "correct" time? How do you measure it?
 
  • #171
ghwellsjr said:
Well, yes, measuring does imply actually looking at the clock. But the Relativistic Doppler effect is a solution (not a problem) to how each clock, moving in relation to each other, sees and measures what the other clock is doing. Do you deny that Relativistic Doppler comports with reality?
No, the Doppler effect only depends on the difference in velocity, so it makes no difference if speed is relative or absolute. For a "universal observer" it will look different though, but the effect is the same.

If you believe in an absolute ether rest state in which there is a single absolute definition of time and space, you need to tell us how to identify it. Otherwise, it's your opinion against everyone else's as to what's happening.
Actually, the easiest solution should always be preferred over a more complex one.
I'm convinced my solution is not right though, but still trying to find out why it's false.

And which is the clock that is moving at high speed?
It's the clock that runs slower.

And there is more than one way to bring those two clocks together and depending on how you do it, you can determine that either one is the one that was slowed down.
That's ONLY true for SR and frankly you have a lot of trouble explaining the following with it.
You put an atomic clock on a plane and you keep one on the ground. You then let the plane circle the Earth and you bring the clock from the ground up to the plane. If you check the clocks you'll notice that the one that was in the plane first will have a time indicating it has run slower.
 
  • #172
A.T. said:
So you want to use the Earth's rotation as a clock. Well anything I said still applies:

Let's say your "correct" clock is placed right next to a light clock, and synchronized so they both tick in sync in their common rest frame. Wouldn't then all observers have to agree that they tick in sync?
Of course.

Otherwise you could easily create paradoxes.
You can proof everything with 0=1 indeed.

If the clocks stay synchronized in every frame, what difference does it make, if we use your clock or a light clock?
Obviously, it will not stay synchronized when you start to move.

So who does tell the "correct" time? How do you measure it?
Well, "correct" time can only be a question of definition. Measuring should be done by something that's the same for everyone. Like calling one rotation of the Earth a day.
(I'm aware that it means each day has a different length, but it doesn't matter as long as it's the same for everyone. Note that this is not the same as how someone observes a rotation of the earth, because for someone moving away it will seem like the Earth is rotating slower than it is.)
 
  • #173
Ernst Jan said:
I know, my question is why would you think the first postulate is true.
Two reasons. First, and most importantly, because of the experimental evidence cited above. Second, because the mathematical forms of all of the currently known fundamental laws of physics are invariant under boosts.

Ernst Jan said:
Yeah, we can agree to that, but I was hoping you'd tell me which of those test disagree with my view.
Again, all of those supporting the first postulate disagree with your view (3.1, 3.2, 3.5, 3.6).

Ernst Jan said:
Since my view also explains that atomic clocks will slow down with high speed.
No, your view does not explain that atomic clocks will slow down with high speed. The idea that clocks slow down with high speed could be added as an ad-hoc patch to your idea, but it certainly would not explain it. In other words, from the two postulates you can derive time dilation. The same is not true if you replace the first postulate with a preferred observer.
 
  • #174
DaleSpam said:
No, your view does not explain that atomic clocks will slow down with high speed. The idea that clocks slow down with high speed could be added as an ad-hoc patch to your idea, but it certainly would not explain it. In other words, from the two postulates you can derive time dilation. The same is not true if you replace the first postulate with a preferred observer.
DaleSpam, we have evidence that the clocks slow down on satellites, but they move in a gravitational field.
Do we have proof that clocks slow down in non-gravitational field?
If the energy and the mass depend on the speed, can we say that those clocks are identical with the ground clocks?

[EDIT] I started to stress from my English :D Should I say "related with" instead of "depend on"?
 
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  • #175
sisoev said:
DaleSpam, we have evidence that the clocks slow down on satellites, but they move in a gravitational field.
Do we have proof that clocks slow down in non-gravitational field?
If the energy and the mass depend on the speed, can we say that those clocks are identical with the ground clocks?

[EDIT] I started to stress from my English :D Should I say "related with" instead of "depend on"?

Ah, so you're perfectly happy with General Relativity, just not special relativity? GPS, satellite experiments, even aiplane experiments on Earth must take account of general relativity (which includes special relativity as an exact special case: exact on the tangent plan to any spacetime point; asymptotically true in any small region of spacetime). The demand for testing special relativity without any (even very small) gravitational corrections would require doing only experiments in an empty universe with mass-less equipment. Have fun with that.

Note that current generation of most accurate clocks must use GR+SR corrections to account for differences when they are raised from the floor to a table top.
 
  • #176
PAllen said:
Ah, so you're perfectly happy with General Relativity, just not special relativity? GPS, satellite experiments, even aiplane experiments on Earth must take account of general relativity (which includes special relativity as an exact special case: exact on the tangent plan to any spacetime point; asymptotically true in any small region of spacetime). The demand for testing special relativity without any (even very small) gravitational corrections would require doing only experiments in an empty universe with mass-less equipment. Have fun with that.

Note that current generation of most accurate clocks must use GR+SR corrections to account for differences when they are raised from the floor to a table top.
Ha-ha :biggrin:
I wouldn't say "perfectly happy", but definitely happier with GR.
And no, we don't need mass-less equipment in an empty universe; just identical equipment and relatively empty region of space.
Then we can compare the difference in the time between those two spacecraft s and the difference we get between our satellite and ground clocks.
 
  • #177
sisoev said:
Ha-ha :biggrin:
I wouldn't say "perfectly happy", but definitely happier with GR.
And no, we don't need mass-less equipment in an empty universe; just identical equipment and relatively empty region of space.
Then we can compare the difference in the time between those two spacecraft s and the difference we get between our satellite and ground clocks.

Do you understand that every aspect of SR is included in GR? And the GPS tests both?
 
  • #178
A.T. said:
Let's say your "correct" clock is placed right next to a light clock, and synchronized so they both tick in sync in their common rest frame. Wouldn't then all observers have to agree that they tick in sync?
Ernst Jan said:
Of course.
So here you a agree that a light clock at rest to your Earth clock will always be observed in sync with the Earth clock, reagrdless how the observer moves relative to them.
Ernst Jan said:
A.T. said:
If the clocks stay synchronized in every frame,
Obviously, it will not stay synchronized when you start to move.
And now you say the opposite of what you agreed to above.

Ernst Jan said:
Note that this is not the same as how someone observes a rotation of the earth,
So now we cannot use the observation of the Earth to measure the "correct" time anymore? Well then again: How do you measure it?
 
  • #179
A.T. said:
So here you a agree that a light clock at rest to your Earth clock will always be observed in sync with the Earth clock, reagrdless how the observer moves relative to them.
This is correct.

And now you say the opposite of what you agreed to above.
No, I'm saying there is a difference between the clock moving away from the observer and the observer moving away from the clock. Only the Doppler effect will be the same in both cases.

So now we cannot use the observation of the Earth to measure the "correct" time anymore?
We've only been discussing the animation in a way that all observers know what the situation is, not how they would actually see the clocks.

Well then again: How do you measure it?
Obviously we can use any clock to measure time. For it to make sense they should all run the same for a "universal observer". Just like the atomic clocks in our GPS satelites, if the satelite moves to a higher or lower orbit they'd have to be adjusted again.
 
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  • #180
DaleSpam said:
Two reasons. First, and most importantly, because of the experimental evidence cited above. Second, because the mathematical forms of all of the currently known fundamental laws of physics are invariant under boosts.
Sorry, I thought you meant this postulate:
The speed of light in vacuum has the same constant value c in all inertial systems.
since it was the one I was questioning.

No, your view does not explain that atomic clocks will slow down with high speed. The idea that clocks slow down with high speed could be added as an ad-hoc patch to your idea, but it certainly would not explain it.
This is strange, because according to me the ONLY thing different is the reason why clocks slow down. Other than that I'm using the axact same numbers.

I've taken a look at the experiments in your link and I think they are all about frequencies. Is this correct?
 
  • #181
Ernst Jan said:
Sorry, I thought you meant this postulate:
The speed of light in vacuum has the same constant value c in all inertial systems.
since it was the one I was questioning.
The idea of a universal observer directly contradicts the principle of relativity, and would only indirectly impact the postulate of the invariance of c if at all. However, that postulate is also tested in the list I sent.

Ernst Jan said:
This is strange, because according to me the ONLY thing different is the reason why clocks slow down. Other than that I'm using the axact same numbers.
Exactly, and that reason must be added as an ad-hoc assumption if you are using a preferred observer.

Ernst Jan said:
I've taken a look at the experiments in your link and I think they are all about frequencies. Is this correct?
Not all of them, no. The interferometer ones are about length or phase. The speed tests are generally about either speed or mass. There are also many that are about decay times, including ones that decay based on the weak and based on the strong interaction.

One of the reasons that the evidence is so overwhelming is that there is such a wide variety of different mechanisms that are tested.
 
  • #182
sisoev said:
DaleSpam, we have evidence that the clocks slow down on satellites, but they move in a gravitational field.
Do we have proof that clocks slow down in non-gravitational field?
If the energy and the mass depend on the speed, can we say that those clocks are identical with the ground clocks?

[EDIT] I started to stress from my English :D Should I say "related with" instead of "depend on"?
I am not interested in discussing GR with you at this time. IMO, it doesn't make any sense to try to tackle GR when you still don't understand SR since SR is the simplest possible case of GR. In fact, since you struggle with Newtonian mechanics even discussing SR is challenging.
 
  • #183
Ernst Jan said:
I'm saying there is a difference between the clock moving away from the observer and the observer moving away from the clock.
What difference?
Ernst Jan said:
Obviously we can use any clock to measure time. For it to make sense they should all run the same for a "universal observer".
Define "make sense".
 
  • #184
And define "universal observer"!
 
  • #185
DaleSpam said:
The idea of a universal observer directly contradicts the principle of relativity, and would only indirectly impact the postulate of the invariance of c if at all. However, that postulate is also tested in the list I sent.
Again... just saying that the principle of relativity is TRUE doesn't make it so.

Exactly, and that reason must be added as an ad-hoc assumption if you are using a preferred observer.
I'm not sure what you mean. I'm simply exploring 2 possible ways of looking at the animation. In order to find out which is the right one I'm asking questions.

Let me describe the difference between SR and my view.

Suppose we have an observer in rest in a train.
This is an observer in any FoR in SR, and in my view it's an observer who's in rest for the "universal observer". Let's say the observer is in a FoR where both views apply.

Now the observer points a laserpen at a spot on the wall.
The train starts to accelerate to 0.8c and holds this speed.
Now SR predicts that the observer is still pointing at the same spot on the wall without having to adjust his aim, where in my view he would have to adjust his aim.

Let's say this train accelerates further to c.
Now SR predicts time stops and in my view there no longer is an angle that will allow the observer to point towards the spot on the wall.
With time stopped it seems difficult to move, but in my view nothing changes.

Since both views differ a lot, I'll be pretty easilly convinced SR is the right view. All I need is one experiment or reason that my view is false. Until then my view seems the most logical.

Not all of them, no. The interferometer ones are about length or phase. The speed tests are generally about either speed or mass. There are also many that are about decay times, including ones that decay based on the weak and based on the strong interaction.

One of the reasons that the evidence is so overwhelming is that there is such a wide variety of different mechanisms that are tested.

Thanks, it seems you're not able or willing to give me one experiment that will certainly proof my view is false, so I'll just try The Michelson-Morley Experiment. I'll start a new thread if it won't convince me.
 
  • #186
A.T. said:
What difference?
In my view all velocities are absolute, in SR they are relative.
In my view the change of velocity is absolute in SR it's absolute too.

[/QUOTE]
Define "make sense". [/QUOTE]
If someone says "it took me a day to do something", it would make sense if the one listening knows how long it took without having to ask at what relative speed to how we're moving now.

HallsofIvy said:
And define "universal observer"!
GOD (if you believe such an entity is all knowing and sees everything)
 
  • #187
Ernst Jan said:
In my view all velocities are absolute,
How do you measure the absolute velocity of something?

Ernst Jan said:
If someone says "it took me a day to do something", it would make sense if the one listening knows how long it took without having to ask at what relative speed to how we're moving now.
Define "knowing how long it took".

Ernst Jan said:
GOD
That's quite an exclusive measurement device. If that is the only thing that can measure your "correct time" and "absolute velocities", than those concepts are pretty useless to us humans. But maybe you can get GOD interested in them, next time you both have a chat.
 
  • #188
Ernst Jan said:
Again... just saying that the principle of relativity is TRUE doesn't make it so.
Obviously not. The mountain of evidence does.

Ernst Jan said:
All I need is one experiment or reason that my view is false. ...
Thanks, it seems you're not able or willing to give me one experiment that will certainly proof my view is false
I gave you dozens of experiments. Your view is incompatible with a mountain of evidence.

If you think that your view is also compatible with the same evidence, then it is up to you to not only explain one experiment, but all of them. It is not our job to prove your theory wrong, but your job to prove your theory right. But not here, the proper place for that is a peer reviewed mainstream scientific journal. This forum is for learning relativity, not debunking alternatives.
 
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  • #189
Ernst Jan said:
Define "make sense".
If someone says "it took me a day to do something", it would make sense if the one listening knows how long it took without having to ask at what relative speed to how we're moving now.

I don't know if the intent Ernst Jan put into this sentence is the understanding i got from it, but this is actually a very good example of why SR is weird. Because at the end of the day, even if you are moving at 80% the speed of light and then a buddy is in rest, and you are having a conversation, when that above sentence is said it will not need clarification, because one day for a moving object is still measured the same way as one day for a stationary object.
 
  • #190
Denius1704 said:
this is actually a very good example of why SR is weird.
Sure, SR is weird. But it is the way the universe works. Weird stuff happens.
 
  • #191
Denius1704 said:
I don't know if the intent Ernst Jan put into this sentence is the understanding i got from it, but this is actually a very good example of why SR is weird. Because at the end of the day, even if you are moving at 80% the speed of light and then a buddy is in rest, and you are having a conversation, when that above sentence is said it will not need clarification, because one day for a moving object is still measured the same way as one day for a stationary object.

This is getting interesting. Now if we live on one of the poles of a spinning planet and take the spinning planet to be our local clock. We also have an atomic clock. They are synchronized at some time. Let us imagine that the planet has a very elliptic orbit, sometimes the planet is very close to the sun and sometimes it is very far away. Would our spinning planet clock and our atomic clock stay synchronized at all times? We let the planet be so small that we can ignore tidal effects.
 
  • #192
DaleSpam said:
g is the gravitational field, or more precisely, the proper acceleration.

I don't get your point. You could smash it with a hammer too. Once it is broken it is no longer an identically constructed clock.
That was never the point trying to be made it was purely the effect of G.
I imagined that the dependence on gravity and acceleration was made quite clear with regards atomic clocks.
Ok. the event horizon of a black hole is an extreme example but your formulated reply that there is no dependence with regards gravity or acceleration is false.
I insist that all clocks are effected by gravity and acceleration it is not possible to discriminate between relativistic, gravitational, or those caused by accelerational effects.
 
  • #193
DaleSpam said:
I am not interested in discussing GR with you at this time. IMO, it doesn't make any sense to try to tackle GR when you still don't understand SR since SR is the simplest possible case of GR. In fact, since you struggle with Newtonian mechanics even discussing SR is challenging.

You could at least answer the question for those who understand GR and SR more than me :)
 
  • #194
Ernst Jan said:
Let me describe the difference between SR and my view.

Suppose we have an observer in rest in a train.
This is an observer in any FoR in SR, and in my view it's an observer who's in rest for the "universal observer". Let's say the observer is in a FoR where both views apply.

Now the observer points a laserpen at a spot on the wall.
The train starts to accelerate to 0.8c and holds this speed.
Now SR predicts that the observer is still pointing at the same spot on the wall without having to adjust his aim, where in my view he would have to adjust his aim.
While the train is accelerating, the spot of laser light on the wall will move to a different place but after the train holds its speed, it will move back to its original location and everything in the train will be the same as it was before the train started moving. The train could repeat this sequence any number of times with the same result. The train will never get any closer to the speed of light than it was before it started.
Ernst Jan said:
Let's say this train accelerates further to c.
Now SR predicts time stops and in my view there no longer is an angle that will allow the observer to point towards the spot on the wall.
With time stopped it seems difficult to move, but in my view nothing changes.
No train can ever accelerate to c, so the rest of your comments are meaningless.
Ernst Jan said:
Since both views differ a lot, I'll be pretty easilly convinced SR is the right view. All I need is one experiment or reason that my view is false. Until then my view seems the most logical.
Is the fact that your view of SR is incorrect enough to convince you that your comparisons are invalid and maybe you should learn what SR really means?
 
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  • #195
sisoev said:
You could at least answer the question for those who understand GR and SR more than me :)
If one of them asks I will.
 
  • #196
Buckleymanor said:
That was never the point trying to be made it was purely the effect of G.
Did you mean to make that a capital G (the universal gravitational constant) or did you mean lower case g (the local gravitational field). Either way it doesn't have an effect to my knowledge, unless you have such strong tidal forces (changes in g) that the atoms are spaghettified.

Buckleymanor said:
I insist that all clocks are effected by gravity and acceleration it is not possible to discriminate between relativistic, gravitational, or those caused by accelerational effects.
It should be pretty easy to discriminate. Simply attach an accelerometer to your clock. Then you can tell if the acceleration is entirely due to gravity (accelerometer reads 0) or not.
 
  • #197
Buckleymanor said:
I insist that all clocks are effected by gravity and acceleration it is not possible to discriminate between relativistic, gravitational, or those caused by accelerational effects.

Except that it has been shown experimentally that acceleration has no effect on time measurement.

The set up is fairly simple" you put radioactive samples on a centrifuge, spin it up to high speed and then see how fast they decay.

Now here's the trick. By varying the angular velocity and length of the centrifuge arm, you can set the experiment up so that the sample travels at different speeds but experiences the same acceleration or travels at the same speed but experiences different accelerations.

Such experiments have shown that the resulting time dilation depends only on the speed at which the sample moves and is independent of the acceleration it undergoes.
 
  • #198
ghwellsjr said:
While the train is accelerating, the spot of laser light on the wall will move to a different place but after the train holds its speed, it will move back to its original location and everything in the train will be the same as it was before the train started moving. The train could repeat this sequence any number of times with the same result. The train will never get any closer to the speed of light than it was before it started.
That's indeed what I said where SR and my view disagree.

No train can ever accelerate to c, so the rest of your comments are meaningless.
Even though I also said this is where SR and my view disagree. Light goes with the speed of light in SR, so the "problem" of movement stays. (In GR you get the same problem at the event horizon of a black hole.)

Is the fact that your view of SR is incorrect enough to convince you that your comparisons are invalid and maybe you should learn what SR really means?
I'm unaware my view of SR is incorrect. Please explain.
 
  • #199
Janus said:
Except that it has been shown experimentally that acceleration has no effect on time measurement.

The set up is fairly simple" you put radioactive samples on a centrifuge, spin it up to high speed and then see how fast they decay.

Now here's the trick. By varying the angular velocity and length of the centrifuge arm, you can set the experiment up so that the sample travels at different speeds but experiences the same acceleration or travels at the same speed but experiences different accelerations.

Such experiments have shown that the resulting time dilation depends only on the speed at which the sample moves and is independent of the acceleration it undergoes.

I completely agree. However, the FAQ in this forum refers to a web site:
http://www.edu-observatory.org/physics-faq/Relativity/SR/experiments.html#Twin_paradox
which states that:

"The so-called “twin paradox” occurs when two clocks are synchronized, separated, and rejoined. If one clock remains in an inertial frame, then the other must be accelerated sometime during its journey, and it displays less elapsed proper time than the inertial clock. This is a “paradox” only in that it appears to be inconsistent but is not. "

Now if people keep saying acceleration has anything to do with the elapsed time, it will confuse people... I do not know if this is the case this time... The link is actually referencing to jour example:

"“Measurements of relativistic time dilation for positive and negative muons in a circular orbit,” "
 
  • #200
The acceleration does not directly affect time dilation. It only breaks the symmetry between the twins. There is nothing wrong with mentioning acceleration, because the broken symmetry is important (even though by itself it does not affect time dilation).
 

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