matheinste
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Saying the spaceship is in motion is meaningless.
Matheinste.
Matheinste.
matheinste said:Isn't this reasonong back to front. Clocks in a common inertial reference frame are synchronized to make them show the same time,not to make light speed isotropic. The standard synchronization process depends on the average of the two way directional speed of light being constant which it assumed to be. If clocks are not first synchronized how can you measure speed.
Matheinste
Hmm... it's about synchronizing clocks?I would like to know what you believe the whole purpose of clock (re-)synchronisation in each reference frame is, if it is not to get c isotropic?
You will tell us. Sooner or later.Please tell me what ATM theory is about.
vin300 said:If you use this formula, you get the velocity of light as c in all frames
Whatever be the velocity of the ship, velocity of light in the ship remains c.
In the frame of reference of the observer on the earth, the length of the ship contracts, he sees the length of the ship to be L/(gamma)
The time for the light from the back to reach the front is
t =L/c+v(gamma)
The time to reach the back is L/c-v(gamma)
I think I remember this discussion.--------Assuming that the world lines of the two clocks and the world line of this observer guy all look the same in the original rest frame (except for their starting position), the answer is definitely yes. This is an immediate consequence of the definition of proper time and the postulate that clocks measure proper time.
eekf said:There will be no Doppler shift between two objects moving at the same velocity whether you are using sound in a medium propagating sound or a medium (or non-medium) propagating light.
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Apart from the distance increase of the path in the moving frame, you will therefore also have a Doppler shift in the 90 degree arm which will increase in relation to your velocity
eekf said:I have not checked these calculations, but have been lead to believe that you get a Null result for all velocities.
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I am not trying to start a new belief or theory.
A.T. said:You are contradicting yourself.
The MM-setup doesn't rely on clock synchronization or exact distance measurement, and would not give a null result in water with sound. I cannot follow your argument about the Doppler shift in the 90°-arm, that miraculously cancels out the expected phase shift. If I move trough a sound medium parallel to a wall and make a loud sound, I receive the echo without any Doppler shift. It doesn't even matter if the wall also moves with me or rests in the medium. This sound travels exactly the same way, it would in the 90°-arm of a sound-MM-setup.
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If you send out a sound wave at exactly 90 deg to the reflecting plane you get it back at exactly 90 deg, that is the law of reflectioneekf said:Secondly let me handle the 90°-arm. If I send out a sound wave at exactly 90° when moving through the water, I can not get the reflection back, as it will come back behind me.
Maybe, and maybe there still are. But scientists didn't believe it. It's been known for centuries that celestial objects had great speeds relative to the speed of sound.eekf said:May I just note that there was a time when people believed it impossible to move faster than sound.
First line deleted, second line is wrong, replaced with sound is a pressure wave, it's velocity varies with framesvin300 said:Sound does not bend as light to make up transformations.It follows the same path in every frame
This is correct and furthermore, if the other object just reflects the wave back, the sender will receive the same frequency he produced. None of them measures a changed frequency, and since the ends of the arm in the MM-setup are also at rest to each other, there will be no frequency shift as well. So I'm still puzzled how you come up with a Doppler shift in the 90° arm.eekf said:When you are moving through the water, the sound you emit into the water will have a Doppler shift depending on your velocity with respect to the water. Another object moving at the same velocity, will not detect this Doppler shift, as it will have the inverse shift when receiving.
Oh really? But this works fine with light. It always comes back if you shine it at a reflector facing you. So you admit, that light and sound do not behave in the same way, as you originally claimed in this thread.eekf said:Secondly let me handle the 90°-arm. If I send out a sound wave at exactly 90° when moving through the water, I can not get the reflection back, as it will come back behind me.
You don't have to (and cannot easily) aim the sound. Just send it out at a broad angle, and some of it will return reflected by the wall at the end of the arm, with the same frequency you sent outeekf said:The sound reflection I get back can only one that I have aimed slightly in front of me.
This is again contradicting what you correctly stated in the first quoted part. Namely that regardless their movement in the medium, two observers at rest to each other will not measure any frequency change of their signals. But an observer at rest to the medium of course will observe a different frequency.eekf said:To presume no Doppler shift in either the arm or straight, you have to assume the "medium" traveling at the same speed as your system
It works fine with sound too, the difference being lesser measured time in case of light and velocity decrease in case of sound(velocity will not decrease as much because of lesser measured time at rel speeds)A.T. said:Oh really? But this works fine with light. It always comes back if you shine it at a reflector facing you. So you admit, that light and sound do not behave in the same way, as you originally claimed in this thread.
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vin300 said:If you send out a sound wave at exactly 90 deg to the reflecting plane you get it back at exactly 90 deg, that is the law of reflection
I think you are missing the point completely. The actual waves interfering and observed have not traveled at 90 deg with respect to each other as assumed by MM. The angle changes depending on which direction you are pointing your equipment to with respect the fixed ether (assumed by MM calculations).A.T. said:You don't have to (and cannot easily) aim the sound. Just send it out at a broad angle, and some of it will return reflected by the wall at the end of the arm, with the same frequency you sent out.
I am actually not contradicting myself. The interference between the waves is a function of the waves in the medium (in this case water), not of the observer. The observer is observing the interference pattern.A.T. said:This is again contradicting what you correctly stated in the first quoted part. Namely that regardless their movement in the medium, two observers at rest to each other will not measure any frequency change of their signals. But an observer at rest to the medium of course will observe a different frequency.
I do not quite understand what you are trying to say here. MM does not measure pulses, but interference between continuous waves. In adddition the direction of measurement is constantly changed in a session (recalibrated every session). There will be Doppler shift in both arms, as well as a change in angle between the two light paths.A.T. said:And I think this is exactlly the root of your confusion regarding the interfering waves in the sonic-MM-setup:
- For the parallel arm you take the perspective of the moving receiver where no frequency change occurs, as you described in the first quoted part.
- For the perpendicular arm you take the perspective of the medium where a Doppler-shift occurs, because the sender is moving in the medium.
You mix up reference frames and come up with the wrong conclusion that the two interfering waves have different wavelengths. This is not the case. In the medium's frame they both have the same Doppler-shift. At the interference screen both have none (see first quote).
Sic. Are you claiming that assuming an ether drift (as MM did) you should not bring Doppler shift into account?A.T. said:As a side note. Even if two interfering waves had a changing wavelength ratio, it is hard to see how that would cancel out a change in phase shift between the two, so that the interference pattern stays the same. Not that this really matters to the MM-setup, where the interfering waves have the same wavelength.
vin300 said:If you send out a sound wave at exactly 90 deg to the reflecting plane you get it back at exactly 90 deg, that is the law of reflection
This is true if you use a sonic-laser (focused sound beam that doesn't disperse at reflection). And this behavior is very different from a laser, which always comes back to you, regardless how you and the mirror (at rest to each other) are moving relative to anything. Do you now understand the difference between light and sound?eekf said:I agree, but if I am not there anymore because I am moving with respect to the water, it will come back behind me.
AT said:Just send it out at a broad angle, and some of it will return reflected by the wall at the end of the arm, with the same frequency you sent out.
In the reference frame of the apparatus they have traveled at 90 deg with respect to each other. Your apparent contradictions arise from constantly mixing up reference frames.eekf said:The actual waves interfering and observed have not traveled at 90 deg with respect to each other as assumed by MM.
I am claiming that the interference screen will always measure the same frequency for both signals. And you have already explained very well why: The source, the receiver and all reflecting elements are at rest to each other.eekf said:If you assume an ether drift (as MM did), you have to bring the angular shift between the light paths in the arms dependent on v/c as well as the Doppler shifts into calculation, or are you claiming that to calculate assuming an ether drift you should not bring this into account?
But the Doppler-effect depends on the observer. And you claim that the Doppler-effect affects the interference.eekf said:The interference between the waves is a function of the waves in the medium (in this case water), not of the observer.
AT said:As a side note. Even if two interfering waves had a changing wavelength ratio, it is hard to see how that would cancel out a change in phase shift between the two, so that the interference pattern stays the same. Not that this really matters to the MM-setup, where the interfering waves have the same wavelength.
In the quoted text I'm just curious how you could cancel out a change in the interference pattern due to a phase shift, by adjusting the frequencies of the two waves. Because that is your explanation for the null-result of MM. But to answer you question: Yes I think there is no frequency change between the screen and source, for neither of the signals.eekf said:Are you claiming that assuming an ether drift (as MM did) you should not bring Doppler shift into account?
Sorry if this confuses you. I am trying to use sound to evaluate the calculations made by MM (provided the assumptions they claim to have made). I am trying my best to keep reference frames apart. As I said before: I am not trying anything new. I am not trying to start a new theory.A.T. said:In the reference frame of the apparatus they have traveled at 90 deg with respect to each other. Your apparent contradictions arise from constantly mixing up reference frames.
I agree they will measure the same frequency, as they get combined to the same direction again (using the mirrors). However, in the MM experiment, you are effectively using the wavelengths of the light to measure the difference in path lengths the light is travelling. As such the wavelength in the "absolute" reference frame in the various arms are crucial.A.T. said:I am claiming that the interference screen will always measure the same frequency for both signals. And you have already explained very well why: The source, the receiver and all reflecting elements are at rest to each other.
etc..
Even if the reflecting elements are stationary to the source and receiver (which I did not imply), unless sound is traveling ballistically, it will not hit the reflecting element (using the MM assumptions). Unless the sound wave is directed to have the same v component (wrt medium) as the source reflector and receiver (i.e. not 90 degrees), it will not hit the reflector, unless the reflector is behind me.A.T. said:I am claiming that the interference screen will always measure the same frequency for both signals. And you have already explained very well why: The source, the receiver and all reflecting elements are at rest to each other.
AT said:In the reference frame of the apparatus they have traveled at 90 deg with respect to each other. Your apparent contradictions arise from constantly mixing up reference frames.
You are rather confusing yourself here.eekf said:Sorry if this confuses you.
The actual path lengths are not the point here. The arms don't have exactly the same length anyway. What you measure by the phase shift is the time delay of arrival between the signals. If that changes, the waves would propagate at different speed depending on their direction in the frame of the instrument. Light waves never do this. Sound waves do, if the instrument moves in the medium.eekf said:However, in the MM experiment, you are effectively using the wavelengths of the light to measure the difference in path lengths the light is travelling.
No they are not. The wavelengths in the arms don't affect the time the signal needs to travel both ways in an arm. And only this time shift determines the phase shift in the interference wave, after reunion.eekf said:As such the wavelengths in the "absolute" reference frame in the various arms are crucial.
eekf said:Even if the reflecting elements are stationary to the source and receiver (which I did not imply), unless sound is traveling ballistically, it will not hit the reflecting element (using the MM assumptions). Unless the sound wave is directed to have the same v component (wrt medium) as the source reflector and receiver (i.e. not 90 degrees), it will not hit the reflector, unless the reflector is behind me.
As far as I understand the experiment tried to measure the changes in the path length differences as the table is rotated using a constant light signal (no instantaneous pulses). Nobody ever claimed the arms have to be the same length.A.T. said:The actual path lengths are not the point here. The arms don't have exactly the same length anyway. What you measure by the phase shift is the time delay of arrival between the signals.
etc..
eekf said:I agree, but if I am not there anymore because I am moving with respect to the water, it will come back behind me. This does not have to do with reflection, but with the fact that I am moving with respect to the water which propagates the wave at a fixed speed (not related to my velocity).
Therefore for it to reach me (when I am moving), I have to send it at a different angle.
It is not about the difference in reflection of light and sound. It is about how to aim a theoretical sonic-laser to hit a reflector at rest in your frame and at 90° to your movement trough the sound's medium. Unlike with light you cannot just aim it at the reflector, because the beam will stay behind with the medium and miss the reflector. This was correctly stated by eekf but he still fails to see the difference between light and sound here.vin300 said:There is no distinction between reflection of light and that of sound, objecting to A.T.'s cloudy point
vin300 said:http://en.wikipedia.org/wiki/File:Time-dilation-002.svg
In the image, light is sent out at 90 deg, but from the perspective of an observer through the normal to the plane, the wave goes diagonal, because the velocity of the moving observer adds vectoriallyto perpendicular velocity as seen by the traveling observer.
The latter still sees every point on the diagonal lines move perpendicular to his motion.
The same happens with sound, that is why it doesn't come behind you.
There is no distinction between reflection of light and that of sound, objecting to A.T.'s cloudy point
GoodPR said:Also note in your example of the two boats, that in order for them to not notice a doppler shift between each other, they have to be traveling with the same velocity and traveling parallel to each other.
Actually I think we have allready covered that earlier. If you change your velocity, unless you re-synchronise your clocks, you will have incorrect (improper) time measurements. Not elapsed time measurements at any point, but the synchronisation of your clocks at different positions in the ship will be out. You have to accept this as it is part and parcel of SRT.GoodPR said:As for this huge argument your having over the time it will take light to get from between the two mirrors. Relative velocity will not change any measurements you take inside the ship.
vin300 said:Anyway, there are practical problems with doing MM with sound .A sound splitter which allows vibration in two directions only is to be used which becomes a thoght. Doing it underwater while in motion is something this forum doesn't allow to write(a foul word)
If it is somehow possible, then you hear beats(or not, depending on the difference in frequencies, it gives beats or diff tones)
No it doesn't. How would you do that? Multiply the number of waves with wavelength? You have no idea how many waves there are in the arms, because you don't know the exact arm lengths anyway. And the number of waves doesn't matter. All that matters is if the signal-run-time difference between the arms (and therefore the phase shift) changes, when you change the orientation of the arms.eekf said:as the experiment actually measures the light path lengths according to wavelengths.
Noeekf said:You therefore have to take Doppler effects into account.
eekf said:Same velocity. Direction of travel is inherent in velocity, as it is a vector. Speed is something different though.
eekf said:Actually I think we have allready covered that earlier. If you change your velocity, unless you re-synchronise your clocks, you will have incorrect (improper) time measurements. Not elapsed time measurements at any point, but the synchronisation of your clocks at different positions in the ship will be out. You have to accept this as it is part and parcel of SRT.