A way to measure OWLS...and verify the constancy of the one way speed of light
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C.J. Luke - 20 Jul 2005 06:07 GMT We build an instrument that consists of the following: It has a master oscillator that is tuned to 300 megahertz and has an accuracy of +- one pulse per second. It has two counters that are capable of accurately counting the output of the master oscillator to an accuracy of +- one pulse per second. It has one pulse per second trigger circuit that generates a trigger in the first counter and triggers a laser with the same pulse. The first counter compares it's count to a preset value and when they are the same, it generates a signal to the second counter that will let it begin counting pulses from the master oscillator. The output of the laser is connected to a length of fiber optic cable. There is a 'receiving' lens on the device that such that when a laser signal is received it generates a pulse that will stop the count on the second counter. The second counter has a display that will enable us to read the count.
We calibrate the device by turning it on, connecting the 'free' end of the fiber optic cable to the receiving lens and adjusting the preset count in the first counter such that the count on the second counter displays zero count. This delay exactly accounts for the transmission time (the time it takes for the laser signal to travel the length of the fiber optic cable) and trigger the second counter to stop counting.
Theory of operation: When running, the first oscillator will delay the firing of the second counter by the length of time the laser takes to travel the length of cable. Upon separating the 'free' end of the cable from the device but still aiming the output of the cable at the receiving lens, we now get a count on the display of the second counter that is reflective of the number of pulses on the master oscillator that it took for the laser to travel from the 'free' end of the fiber optic cable to the receiving lens.
This device could be used for two purposes: 1. If we had an accurate enough distance measuring device, and we performed this experiment in an evacuated space, and we sufficiently controlled the temperature of the test equipment and environment, we could 'accurately' (within the range of accuracy of all equipment involved) measure the one way speed of light. 2. If we added an accurate time keeping device, encased the device in an evacuated pipe that was submerged in an underground pool, and fed the counts and time and control measurements (temperature and vibration monitors) to a database, we could then verify, or not, the constancy of the one way speed of light.
"The lack of reason is overcome by the passion of belief" < cj@totcon.com >
N:dlzc D:aol T:com (dlzc) - 20 Jul 2005 06:14 GMT Dear C.J. Luke:
...
> 1. If we had an accurate enough distance measuring device, and > we [quoted text clipped - 5 lines] > equipment > involved) measure the one way speed of light. DOA. Length is a TWLS measurement, or more accurately a remote synchronized [clock]. So you will measure OWLS to be c (or less if you actually use a fiber), with no big surprises.
David A. Smith
Bill Hobba - 20 Jul 2005 10:02 GMT > Dear C.J. Luke: > [quoted text clipped - 12 lines] > synchronized [clock]. So you will measure OWLS to be c (or less > if you actually use a fiber), with no big surprises. You are of course correct - so without going into the detail we know it will not measure what it is purported to measure. Nevertheless it will be interesting to see the precise error that some of the experimental guys who post here may point out.
Thanks Bill
> David A. Smith C.J. Luke - 21 Jul 2005 05:25 GMT >> Dear C.J. Luke: >> [quoted text clipped - 22 lines] > >> David A. Smith So far you have only made an assertion. I see no reason given for why the device won't work, other than the assertion that distance is a two way light speed measurement....which has little, if not nothing to do with my post. thanks
"The lack of reason is overcome by the passion of belief" < cj@totcon.com >
Bill Hobba - 21 Jul 2005 09:13 GMT > >> Dear C.J. Luke: > >> [quoted text clipped - 28 lines] > with my post. > thanks It is well known that it is not possible to show that OWLS is always the same http://math.ucr.edu/home/baez/physics/Relativity/SR/experiments.html
'Note that while these experiments clearly use a one-way light path and find isotropy, they are inherently unable to rule out a large class of theories in which the one-way speed of light is anisotropic. These theories share the property that the round-trip speed of light is isotropic in any inertial frame, but the one-way speed is isotropic only in an ether frame. In all of these theories the effects of slow clock transport exactly offset the effects of the anisotropic one-way speed of light (in any inertial frame), and all are experimentally indistinguishable from SR. All of these theories predict null results for these experiments'
However experimental physics is not my bag so I will leave the details up to those better qualified.
Bill
> "The lack of reason is overcome by the passion of belief" > < cj@totcon.com > C.J. Luke - 22 Jul 2005 04:37 GMT >> >> Dear C.J. Luke: >> >> [quoted text clipped - 52 lines] >> "The lack of reason is overcome by the passion of belief" >> < cj@totcon.com > I don't think that this device is encumbered with the 'slow' clock transport problem, and I beleive that within the accuracy of the equipment as built...it has the possibility of doing what I stated in my original post.
"The lack of reason is overcome by the passion of belief" < cj@totcon.com >
C.J. Luke - 21 Jul 2005 05:21 GMT "N:dlzc D:aol T:com \(dlzc\)" <N: dlzc1 D:cox T:net@nospam.com> wrote:
>Dear C.J. Luke: > [quoted text clipped - 14 lines] > >David A. Smith I am not sure that you even read my post. Firstly...length used to be, and always should be, a physical measurement. For some time is has been a calculated value based on an unproven premis. My device only has one clock and depends on the value of c to be constant in a medium...i.e. the fiber optic cable.
thanks for the reply
"The lack of reason is overcome by the passion of belief" < cj@totcon.com >
N:dlzc D:aol T:com (dlzc) - 21 Jul 2005 14:23 GMT Dear C.J. Luke:
> "N:dlzc D:aol T:com \(dlzc\)" <N: dlzc1 D:cox T:net@nospam.com> > wrote: [quoted text clipped - 17 lines] >>you will measure OWLS to be c (or less if you >> actually use a fiber), with no big surprises.
> I am not sure that you even read my post. I did.
> Firstly...length used to > be, and always should be, a physical measurement. Sorry, won't happen. The meter is supported by metrology, metrology is supported by standards, and the standard is distance = c * time. Since *any* measurement of c is automatically TWLS, c works over the entire path. And time is a "physical measurement", and long as counting is considered physical.
> For some time is > has been a calculated value based on an unproven > premis. It has been proven to 11 sig figs. And if you think about an attempt to measure OWLS, you'll find that it is in fact TWLS.
> My device > only has one clock and depends on the value of c > to be constant in a medium...i.e. the fiber optic cable. Your device has an implicit clock in the "defined distance". Which could easily simply be a mirror at the defined distance, "reflecting the reading".
Your intentions don't count. It is not physically possible to measure OWLS, without instantaneous communication over a finite distance.
David A. Smith
C.J. Luke - 22 Jul 2005 04:46 GMT "N:dlzc D:aol T:com \(dlzc\)" <N: dlzc1 D:cox T:net@nospam.com> wrote:
>Dear C.J. Luke: > [quoted text clipped - 32 lines] >c works over the entire path. And time is a "physical >measurement", and long as counting is considered physical. Given that you are seemingly stuck on the current measure....the second experiment that I mentioned in my original post can still be run. It matters not that the initial measurments are light based...because the exact length of the device is not critical...
>> For some time is >> has been a calculated value based on an unproven >> premis. > >It has been proven to 11 sig figs. And if you think about an >attempt to measure OWLS, you'll find that it is in fact TWLS. The unproven premis is the anisitropy of the OWLS. Read the definition of the speed of light...no where in it is a description of a two way light path.
>> My device >> only has one clock and depends on the value of c [quoted text clipped - 3 lines] >Which could easily simply be a mirror at the defined distance, >"reflecting the reading". I really don't think that you read the original post very carefully. You should probably do that. There is only one clock and that is all ... implicit or otherwise...the *flight time* of light in the cable is canceled exactly so the only flight time measured is the flight time from the end of the cable to the receiving lens. There is no slow transport involved. It is a relatively simple device that can do exactly what I said.
>Your intentions don't count. It is not physically possible to >measure OWLS, without instantaneous communication over a finite >distance. Your stubborn belief doesn't count for much either. It does not require instant communication to make the measurement.
>David A. Smith "The lack of reason is overcome by the passion of belief" < cj@totcon.com >
N:dlzc D:aol T:com (dlzc) - 22 Jul 2005 05:52 GMT Dear C.J. Luke:
> "N:dlzc D:aol T:com \(dlzc\)" <N: dlzc1 D:cox T:net@nospam.com> > wrote: [quoted text clipped - 14 lines] >>>>> the range of accuracy of all equipment involved) measure >>>>> the one way speed of light. ...
>>Sorry, won't happen. The meter is supported by metrology, >>metrology is supported by standards, and the standard is [quoted text clipped - 3 lines] >>c works over the entire path. And time is a "physical >>measurement", and long as counting is considered physical.
> Given that you are seemingly stuck on the current > measure....the [quoted text clipped - 3 lines] > based...because the exact length of the device is not > critical... Then you have no measure of OWLS. Speed requires distance and time.
>>> For some time is >>> has been a calculated value based on an unproven >>> premis. >> >>It has been proven to 11 sig figs. And if you think about an >>attempt to measure OWLS, you'll find that it is in fact TWLS.
> The unproven premis is the anisitropy of the OWLS. Read the > definition of the speed of light...no where in it is a > description of > a two way light path. Look at any apparatus for measuring light speed (including yours), and in all circumstances it is TWLS that is being measured.
>>> My device >>> only has one clock and depends on the value of c [quoted text clipped - 3 lines] >>Which could easily simply be a mirror at the defined distance, >>"reflecting the reading".
> I really don't think that you read the original post very > carefully. I don't think you can hear any criticism whatsoever. "accurate enough distance measuring device" is light and time, and therefore makes you experiment TWLS.
> You should probably do that. Already done. Dead at step 1.
> There is only one clock and that is all > ... implicit or otherwise...the *flight time* of light in the > cable is canceled exactly so the only flight time > measured is the flight time from the end of the cable > to the receiving lens. "accurate enough distance measuring device". Dead at step 1.
> There is no slow transport involved. It is a relatively > simple > device that can do exactly what I said. And more, that you did not intend.
>>Your intentions don't count. It is not physically possible to >>measure OWLS, without instantaneous communication >>over a finite distance.
> Your stubborn belief doesn't count for much either. It does > not > require instant communication to make the measurement. Your head is too full to hear the truth. Run your experiment. If you don't screw up, you'll imagine that OWLS = c, just as all the other experimenters that couldn't see that they were measuring TWLS either. Just don't make it out of plywood.
David A. Smith
C.J. Luke - 23 Jul 2005 05:07 GMT "N:dlzc D:aol T:com \(dlzc\)" <N: dlzc1 D:cox T:net@nospam.com> wrote:
>Dear C.J. Luke: > [quoted text clipped - 35 lines] >Then you have no measure of OWLS. Speed requires distance and >time. As I thought. You did not read the original post. The second experiment was not a measure of the one way speed of light.
>>>> For some time is >>>> has been a calculated value based on an unproven [quoted text clipped - 30 lines] > >Already done. Dead at step 1. Again, I ask you to read the original post. 'Your Dead at step 1' does sound authoritative and final...but it is just so much bs.
>> There is only one clock and that is all >> ... implicit or otherwise...the *flight time* of light in the [quoted text clipped - 22 lines] >the other experimenters that couldn't see that they were >measuring TWLS either. Just don't make it out of plywood. You should read the paragraph above to yourself several times.
>David A. Smith "The lack of reason is overcome by the passion of belief" < cj@totcon.com >
N:dlzc D:aol T:com (dlzc) - 24 Jul 2005 01:35 GMT Dear C.J. Luke:
> "N:dlzc D:aol T:com \(dlzc\)" <N: dlzc1 D:cox T:net@nospam.com> > wrote: ...
>>Then you have no measure of OWLS. Speed requires >>distance and time.
> As I thought. You did not read the original post. The > second experiment was not a measure of the one way > speed of light. I had left in the first experiment. The one that related to the title of the thread.
Anisotropy detection such as you imagine you can attempt has already been tried... and failed. This has been pointed out to you, by others. But that is OK, someone can sell you more hardware.
>>> I really don't think that you read the original post very >>> carefully. [quoted text clipped - 6 lines] >> >>Already done. Dead at step 1.
> Again, I ask you to read the original post. 'Your Dead > at step 1' does sound authoritative and final...but it is > just so much bs. Then we are done. You can't hear what you won't hear.
Goodbye. <plonk>
David A. Smith
Bill Hobba - 24 Jul 2005 04:14 GMT > Dear C.J. Luke: > [quoted text clipped - 32 lines] > > Then we are done. You can't hear what you won't hear. Perfect response David. He has been posting the same stuff and having endless debates about something totally obvious and trivial for some time now. I even recall I engaged him in a series of useless posts where he simply said let us put facts he did not want to consider to one side (which was my insistence that if LET was true - and we have no way of ruling it out - then he was not measuring lights real one way speed) - which is why I am not going to do it again From over a year ago see the following detailed reply from Tom - http://groups-beta.google.com/group/sci.physics.relativity/msg/8ac2f3af700bac45?hl=en It is obvious he simply wants to argue - not learn.
Thanks Bill
> Goodbye. > <plonk> > > David A. Smith Ben Rudiak-Gould - 24 Jul 2005 12:45 GMT > My device > only has one clock and depends on the value of c to be constant in a > medium...i.e. the fiber optic cable. So you are assuming that the (one-way) speed of light in a fiber optic cable is constant, and using that to measure the (one-way) speed of light in some other medium, like air or vacuum? If so, that's a perfectly legitimate experiment. You ought to list your assumptions up front to avoid fruitless arguments. Also, your description of the experimental apparatus is very confusing. A diagram would help immensely in understanding what's connected to what.
-- Ben
Tom Roberts - 25 Jul 2005 15:09 GMT > So you are assuming that the (one-way) speed of light in a fiber optic > cable is constant, and using that to measure the (one-way) speed of > light in some other medium, like air or vacuum? The problem with this is: how does it behave as the index of refraction approaches 1? I don't think there is any sensible theory that has anisotropic propagation in vacuum but isotropic propagation in a fiber. All while keeping the round-trip speed of light isotropic in BOTH vacuum and fiber (because that's what measurements show).
The class of theories I discuss certainly has anisotropic propagation in the fiber. That's easily seen because theories in this class differ from SR only in the way clocks are synchronized. Except for the possibility of some ether theory "living in the errorbars" of current experiments, I believe this class includes every ether theory consistent with current experiments, and most non-ether theories as well. This class of theories is defined by: one inertial frame has an isotropic one-way speed of light, and the round-trip speed of light is isotropic in every inertial frame.
[It's quite difficult to formulate a theory to live the the current errorbars, as such a theory must agree with SR for terms up to (v/c)^6, where v is the earth's orbital speed. If it doesn't differ for higher-order terms, then it is in the above class and is experimentally indistinguishable from SR.]
Tom Roberts tjroberts@lucent.com
Tom Roberts - 21 Jul 2005 20:34 GMT > We build an instrument that consists of the following: [...] This does not measure the one-way speed of light, it measures the round-trip speed of light in a combination of the fiber and the free space between the end of the fiber and the "receiving lens". For different positions of the fiber end there are different proportions of fiber and free space, but it's still a round trip measurement.
Tom Roberts tjroberts@lucent.com
C.J. Luke - 22 Jul 2005 04:51 GMT >> We build an instrument that consists of the following: [...] > [quoted text clipped - 5 lines] > >Tom Roberts tjroberts@lucent.com Not even close Tom...unless you have a new definiton for round trip that you could share with us. The portion of the trip in the fiber is completely inconsequential to the end result so I have no idea what proportions you are talking about above. The flight time in the cable is exactly canceled. The only flight time measured is the flight time from the end of the cable to the receiving lens. Simple.
"The lack of reason is overcome by the passion of belief" < cj@totcon.com >
Martin Hogbin - 22 Jul 2005 17:49 GMT > Not even close Tom...unless you have a new definiton for round trip > that you could share with us. The portion of the trip in the fiber is > completely inconsequential to the end result so I have no idea what > proportions you are talking about above. The flight time in the cable > is exactly cancelled. Only if the time light takes to travel the length of the fibre optic is independent of positions of the two ends. How do you know that this is the case?
Imagine replacing the fibre optic with a collection of mirrors.
Martin Hogbin
bz - 23 Jul 2005 00:47 GMT >> Not even close Tom...unless you have a new definiton for round trip >> that you could share with us. The portion of the trip in the fiber is [quoted text clipped - 9 lines] > > Martin Hogbin If you keep the total distance traveled between mirrors constant{exclusive of the point where the fiber /mirror bath is to end} [as the fiber does] then mirrors should work too.
Also, you have the potential of testing the c'=c+/-v theory with your apparatus.
You just have to have the end of your fiber tangential to the edge of a spinning disk [you do need a coupling to keep the spin from breaking your fiber]
 Signature bz
please pardon my infinite ignorance, the set-of-things-I-do-not-know is an infinite set.
bz+sp@ch100-5.chem.lsu.edu remove ch100-5 to avoid spam trap
Martin Hogbin - 23 Jul 2005 09:16 GMT > If you keep the total distance traveled between mirrors constant{exclusive > of the point where the fiber /mirror bath is to end} [as the fiber does] > then mirrors should work too. Yes, but it is then easy to see that you are measuring the round trip (two-way, one-clock) speed of light.
> Also, you have the potential of testing the c'=c+/-v theory with your > apparatus. > > You just have to have the end of your fiber tangential to the edge of a > spinning disk [you do need a coupling to keep the spin from breaking your > fiber] Once you introduce rotation, which is non-inertial motion, you are no longer measuring the speed of light in an inertial frame.
Martin Hogbin
Tom Roberts - 24 Jul 2005 05:25 GMT >>>We build an instrument that consists of the following: [...] >> [quoted text clipped - 6 lines] > Not even close Tom...unless you have a new definiton for round trip > that you could share with us. Your signal goes out and back -- that makes it a round-trip measurement.
NOTE: I assume the source and detector are co-located, so intitially the fiber loops out and back to its origin. I can no longer see the original post and don't recall if that was stipulated there or not. This makes the discussion simpler, but the conclusion is unchanged even if detector and source are not co-located....
> The portion of the trip in the fiber is > completely inconsequential to the end result NOT TRUE! To claim that you must ASSUME that the one-way speed of light inside the fiber is isotropic. But that is directly related to what you are trying to measure.
> so I have no idea what > proportions you are talking about above. Consider the initial situation in which the end of the fiber is right next to the detector. Then the signal goes out and back entirely in the fiber, and its east->west and west->east distances are identical (as are its north->south and south->north distances, which I'll ignore). Now move the end of the fiber some distance to the west -- now the east->west distance in the fiber exceeds the west->east distance in the fiber by EXACTLY the same amount as the west->east distance in air. But still, the total west->east distance equals the total east->west distance. The proportion of the total trip that is in the fiber varies as you move its end: 100%fiber/0%air when the end is next to detector, 50%fiber/50%air when the fiber is fully extended.
My "air" might be vacuum in your original (which I cannot see).
> The flight time in the cable > is exactly canceled. ONLY if you assume isotropy in the propagation in the fiber, which defeats the whole point of the measurement.
> The only flight time measured is the flight time > from the end of the cable to the receiving lens. Not true. You cannot rule out the possibility that light propagates anisotropically in the fiber. In fact, there is an entire class of aether theories in which the one-way speed of light is not isotropic, but the round-trip speed of light is isotropically c in any inertial frame. These theories are all experimentally indistinguishable from SR. They ALL predict anisotropic propagation in the fiber, and that "just so happens" to exactly cancel out the effect you seek (after all, they are experimentally indistinguishable from SR).
NOTE: there is no point in considering theories in which the round-trip speed of light is not isotropic (in the inertial frame of the apparatus), as any such theory is soundly refuted experimentally.
Simple example: Consider the case for which the west->east speed of light is > c (so east->west speed < c, in order to retain an isotropic round-trip speed). As you move the end of the fiber a distance L to the west, the light end->detector travels faster than c and you would expect the time delay to be less than L/c. But you are forgetting that you have also increased the (east->west - west->east) distance the light must travel in the fiber, and it travels more slowly east->west in the fiber than west->east in the fiber. This goes in the opposite direction of the effect you expect; and in fact it cancels it exactly in the class of theories I mentioned above.
bz wrote:
> "Martin Hogbin" <goatREMOVETHIS123@hogbin.org> wrote in > news:dbr83b$a4u$1@nwrdmz02.dmz.ncs.ea.ibs-infra.bt.com: [quoted text clipped - 3 lines] > of the point where the fiber /mirror bath is to end} [as the fiber does] > then mirrors should work too. Again, ONLY if you assume that the propagation among the mirrors is isotropic. But Martin's point was that in this case you clearly cannot assume that, as the region among the mirrors is no different from your "measurement region".
Bottom line: one way or another this is a round-trip measurement. For the simple reason that the singal goes out and back. And there are zillions of experiments that show the round-trip speed of light is isotropically c in any inertial frame we have access to.
Tom Roberts tjroberts@lucent.com
C.J. Luke - 24 Jul 2005 13:47 GMT >>>>We build an instrument that consists of the following: [...] >>> [quoted text clipped - 94 lines] > >Tom Roberts tjroberts@lucent.com For Bill, David, and Tom, I give you this opportunity to demonstrate you prowess with math. I ask you to show me the calculation you would need to make to predict the reading on my device under the following conditions.
I will include part of the original post for you and add a few things.
We build an instrument that consists of the following: It has a master oscillator that is tuned to 300 megahertz and has an accuracy of +- one pulse per second. It has two counters that are capable of accurately counting the output of the master oscillator to an accuracy of +- one pulse per second. It has one pulse per second trigger circuit that generates a trigger in the first counter and triggers a laser with the same pulse. The first counter compares it's count to a preset value and when they are the same, it generates a signal to the second counter that will let it begin counting pulses from the master oscillator. The output of the laser is connected to a length of fiber optic cable. There is a 'receiving' lens on the device that such that when a laser signal is received it generates a pulse that will stop the count on the second counter. The second counter has a display that will enable us to read the count.
We calibrate the device by turning it on, connecting the 'free' end of the fiber optic cable to the receiving lens and adjusting the preset count in the first counter such that the count on the second counter displays zero count. This delay exactly accounts for the transmission time (the time it takes for the laser signal to travel the length of the fiber optic cable) and trigger the second counter to stop counting.
Theory of operation: When running, the first oscillator will delay the firing of the second counter by the length of time the laser takes to travel the length of cable. Upon separating the 'free' end of the cable from the device but still aiming the output of the cable at the receiving lens, we now get a count on the display of the second counter that is reflective of the number of pulses on the master oscillator that it took for the laser to travel from the 'free' end of the fiber optic cable to the receiving lens.
The additions that I make are adding a dimension for the length of cable. It is 1000 meters long. And for you David, you can measure it with a meter stick or a DME laser...your choice.
Now for your turn...show me the calculation that you will use to find out what the display on the second counter will read when the free end of the fiber optic cable is a distance of 300 meters from the receiving window....and Tom....I am especially interested to see the 1000 meter cable length in your calculation.
"The lack of reason is overcome by the passion of belief" < cj@totcon.com >
rotchm@gmail.com - 24 Jul 2005 18:15 GMT Could you restate your experiment for me, removing all superflouus devices. Make it a thought/ideal experiment. Is the fibre cable necesary, the lens? I dont need to know the +- 1 pulse accuracy either etc.
I ask you this bcause I would like to take a shot at it but I want to make sure I understand correctly the whole situation. So removing unnecesary concepts will minimize misunderstandings.
Thanks.
C.J. Luke - 25 Jul 2005 05:04 GMT >Could you restate your experiment for me, removing all superflouus >devices. Make it a thought/ideal experiment. [quoted text clipped - 6 lines] > >Thanks. The concept is easy. Use one clock, two counter circuits, a laser, optical receiver, and a one second trigger circuit all co-located in a single box. One counter has a preset count that is adjustable that once that count has been reached, it will send a *start counting* pulse to the second counter. The second counter will start counting when it gets that pulse and stop counting when the laser beam is *received* at the optical receiver circuit. The length of fiber optic cabel is initally attached to the receiving lens for calibration.
Let's say the fiber optic cable is 1000 meters long and the main oscillator is running at 300 mhz, and the speed of light is 300 million meters per second.
The trigger fires the laser and the first counter. Light speeds down the 1000 meters of cable, while the first counter ticks away. Light reaches the receiver in 1000 ticks of the first counter. You adjust the preset so that the first counter will *tell* the second counter to start counting as soon as the first counter counts up to 1000. With this calibration, the second counter won't get to count, be cause as soon as it gets the signal to start counting, the receiver circuit will disable it's ability to count.
Now seperate the end of the fiber optic cable from the receiver ... say a distance of 300 meters. The first counter starts counting, when the light reaches the end of the cable, the first counter has reached 1000, and sends the signal to the second counter to begin counting. Light travels from the end of the fiber optic cable to the receiving lens, a distance of 300 meters = 300 counts on the second counter. The light hits the receiver and stops the count on the second counter which now displays a count of 300.
Move the cable end to a distance of 600 meters and the second counter will display 600, move it to 1000 (less an inch so we can aim it back to the receiver) and it will read ~1000.
Simple OWLS measuring device....to get higher accuracy, you can increace the frequency of the oscillator and/or the length of the cable. A couple of problems with accuracy though....distance measuring...creating a temperature and vibration stable vacuume environment for accurate measurments.
"The lack of reason is overcome by the passion of belief" < cj@totcon.com >
rotchm@gmail.com - 25 Jul 2005 21:07 GMT Thanks for the restatement... I think I understand your experiment now (you can greatly simplify it still...).
Ok, I think I understood your experiment. To me it seems to be a TWLS experiment.
Ok. Let the cable be of length 1000m. Do the calibration: The time it takes for the signal to leave the device and come back (or to travel within the cable) is T1=1000/c, where c is 299792458 (an arbitrairy value...). (you call it 1000 ticks).
Now, as I understand it, you rearange the cable to be elongated out of the device to, say, 1000 meters away (minus an inch ok...ok...): One end of the cable is at the device, the other end 1000 meters away.
As the first clock (clock 1, counter if u wish) indicates T1=1000/c it triggers the locally other clock (clock 2) to start counting: At this instant, clock 1 indicates T1 and clock 2 indicates 0 and the laser light signal is at the end of the cable, 1000m away.
The light emmenates out of the cable (1000 away), being sent towards clock 2 (the device). The time elapsed on clock 2 uppon reception of this laser signal is thus (according to SR) 1000/c, which = T1.
So, my conclusion is that clock 2 will indicate T1=1000/c on reception of the laser signal.
I used SR to do this.
Now, If you are using Prefered frame theories (PFT) where OWLS is not isotropic (but a TWLS measurement will always give c), PFT will conclude the same thing as above: Upon reception of the laser signal, clock 2 will indicate T1.
This experiment will not be able to distinguish between OWLS and TWLS.
That problem I have tackeled in the past and many similar other ones.
And btw, the calibration is a TWLS also.
L8r.
C.J. Luke - 26 Jul 2005 02:09 GMT >Thanks for the restatement... I think I understand your experiment now >(you can greatly simplify it still...). [quoted text clipped - 6 lines] >within the cable) is T1=1000/c, where c is 299792458 (an arbitrairy >value...). (you call it 1000 ticks). Actually, for the purposes of making the math simple I arbitraily defined the speed of light to be 300,000,000 meters per second. The 1000 ticks that you mention above is not arbitrary. I also defined that the master oscillator had a frequency of 300,000,000 cycles per second. That number was chosen to make a single *tick* of the oscillator to equate to light traveling the distance of 1 meter.
>Now, as I understand it, you rearange the cable to be elongated out of >the device to, say, 1000 meters away (minus an inch ok...ok...): One >end of the cable is at the device, the other end 1000 meters away. It is important to understand that the ONLY significance of the LENGTH of the fiber optic cable is the distance that it will allow you to get between the end of the cable and the receiving lens. For the experiment I described for you, the cable could be 5000 meters long. As long as you follow the described calibration procedure and move the end of the cable 1000 meters from the receiving lens the results will be exactly the same.
>As the first clock (clock 1, counter if u wish) indicates T1=1000/c it >triggers the locally other clock (clock 2) to start counting: At this >instant, clock 1 indicates T1 and clock 2 indicates 0 and the laser >light signal is at the end of the cable, 1000m away. It is important to understand that there is only ONE *clock* in the device. It is the only timing element. The two counters only count the output pulses of the oscillator.
>The light emmenates out of the cable (1000 away), being sent towards >clock 2 (the device). The time elapsed on clock 2 uppon reception of >this laser signal is thus (according to SR) 1000/c, which = T1. > >So, my conclusion is that clock 2 will indicate T1=1000/c on reception >of the laser signal. You should probably read my replys and re-read the setup. Your conclusion is in error.
>I used SR to do this. > [quoted text clipped - 8 lines] > >And btw, the calibration is a TWLS also. Well, at least you are consistant in your misunderstanding.
>L8r. "The lack of reason is overcome by the passion of belief" < cj@totcon.com >
rotchm@gmail.com - 26 Jul 2005 04:09 GMT Actually, for the purposes of making the math simple I arbitraily defined the speed of light to be 300,000,000 meters per second. The 1000 ticks that you mention above is not arbitrary. I also defined that the master oscillator had a frequency of 300,000,000 cycles per second. That number was chosen to make a single *tick* of the oscillator to equate to light traveling the distance of 1 meter.
Understood, but irrelevan as a thought experiment.
It is important to understand that the ONLY significance of the LENGTH of the fiber optic cable is the distance that it will allow you to get between the end of the cable and the receiving lens. For the experiment I described for you, the cable could be 5000 meters long. As long as you follow the described calibration procedure and move the end of the cable 1000 meters from the receiving lens the results will be exactly the same.
Understood.
It is important to understand that there is only ONE *clock* in the device. It is the only timing element. The two counters only count the output pulses of the oscillator.
Understood. But that not what you wrote previously. I quote: " Light speeds down the 1000 meters of cable, while the first counter ticks away". Now, according to what u r saying, the counter does not tick; it reads or counts the "pulses" from the oscillator (main clock). "ticking" refers to an object that keep time, a clock. "counter" refers to an object that reads or counts or notes whant is indicated on a clock. But the two counters can be considered as clocks too, that tick at the same rate as the main oscillator, which is a clock also. But this is also irrelevent. Only one clock is needed as you say, and the counters are superflous here.
You should probably read my replys and re-read the setup. Your conclusion is in error. Well, at least you are consistant in your misunderstanding.
I will look at the other posts.
Now, here is the experiment simplified. Tell me if this is equivalent to the experiment u have in mind:
At location X we have a clock and two counters that notes time from the clock. To the clock is attached both ends of a 1000 m (fibre,empty space) cable. (this cable can be looped around or just flat on the ground or whatever).
The calibration: The clock sends out a light pulse in the "first" end of the cable. This pulse travels within the cable to reach the other end where it rejoins the clock. This clock (or even the counter if you wish), notes the total time of travel, wich is, according to SR, T1 = 1000/c. (this is what both clock and counter indicate...if the counters are cosidered as clocks too).
The experiment: Detach the second end of the cable from the clock and set this end 1000m away from the clock. Fire a pulse of light in the attached end of the cable and "start" the clock and first counter. As the light pulse reaches the free end, the clock (and the first counter) thus indicate T1. At this instant, counter 1 signals to counter 2 to start counting the time elapsed on the clock. Also at this instant, the light pulse emmenating from the free end of the fiber is reflected back towards the clock. It takes a time of T2=1000/c for the pulse to reach back to the clock, the instant when counter 2 stops. Hence the clock indicates 1000/c + 1000/c and counter 2 indicates 1000/c.
So the counclusion, using SR, is that counter 2 indicates 1000/c. The conclusion, using PFT, although the algebra is completely different, yields the same conclusion.
Is this experiment equivalent?
C.J. Luke - 26 Jul 2005 18:17 GMT >Actually, for the purposes of making the math simple I arbitraily >defined the speed of light to be 300,000,000 meters per second. The [quoted text clipped - 69 lines] > >Is this experiment equivalent? no
in calibration with the *end* of the fiber optic cable attached to the receiving lens.
a starting pulse fires the laser and triggers the first counter to start counting
the first counter keeps checking a preset count to see if it has reached that count
when it reaches the preset count it triggers the second counter to start counting
when the laser is received at the lens, it sends a signal for the second counter to stop counting
to calibrate adjust the preset to a count high enough that you begin to get a count on the second counter...then back off the preset count until the second counter stops counting.
now you have exactly canceled the time that it takes for the light to travel the length of the fiber optic cable.
any seperation induced will result in a count displayed in the second counter that will be reflective of the time (number of counts on the master clock) it took for the light to travel from the end of the cable to the receiving lens.
cj
"The lack of reason is overcome by the passion of belief" < cj@totcon.com >
rotchm@gmail.com - 26 Jul 2005 19:11 GMT >no
>in calibration with the *end* of the fiber optic cable attached to the >receiving lens. Forget about the "receiving lens". Its irrelevant to the problem. The "end" is attached to the (master) clock-oscillator-device.
>a starting pulse fires the laser and triggers the first counter to >start counting Yes, just as I said. But I use the term light pulse instead of laser.
>the first counter keeps checking a preset count to see if it has >reached that count >when it reaches the preset count it triggers the second counter to >start counting Yes, just as I said. I quote: "At this instant, counter 1 signals to counter 2 to start counting the time elapsed on the clock."
You use the term "triggers", I used "signals to..."
>when the laser is received at the lens, it sends a signal for the >second counter to stop counting Yes, just as I said. I quote: "...for the pulse to reach back to the clock, the instant when counter 2 stops."
You use the term laser, where I use pulse. U use lens where I use clock (referring to the device or master oscillator)
Btw, the "lens" and the second counter are the same location right (as a thought experiment) ? Or are you considering that they are non-negligibly separated in distance?
The way I understand your setup is that the master clock, both counters, laser and lens are all, for practical purposes , at the same location at all times, correct?
Your calibration is a TWLS: You send out a light (laser) pulse and receive it back. Thats a TWLS, no matter how the cable is placed on the ground. When you detach an end and place it 1000m away, again you send a light pulse and receive it back. Still a TWLS.
In other words, elongate to 1000m away the free end of the cable. Send a light pulse through it. We, a priori, do not know what the master clock indicates at this instant. (according to SR its 1000/c). We, a priori, do not know how much time it takes for the pulse to reach back at the lens. But we do know the total time of the out and back trip.
And, re-read the "simplified" version of your setup and tell me where/how is it different from yours. And, although it might be different, do you agree to what is claimed or how I calcutale T1 and so forth?
Martin Hogbin - 25 Jul 2005 23:46 GMT > Now seperate the end of the fiber optic cable from the receiver ... > say a distance of 300 meters. How do you know that the light takes the same time to travel the length of the fibre after you have moved the end 300 metres.
Can you answer this question? The whole of your conclusions depend on that fact.
Martin Hogbin
C.J. Luke - 26 Jul 2005 01:56 GMT >> Now seperate the end of the fiber optic cable from the receiver ... >> say a distance of 300 meters. [quoted text clipped - 6 lines] > >Martin Hogbin Astute observation Martin, and I do not *know* for a fact that my assumption is true. I base it on experimental evidence that the velocity of light is constant and relative to the *media* that it is traveling in. I don't have a citation that I can quote for you but I am sure that a Google search will turn up several. You are absolutely correct in maintaining that my experimental device is predicated on that assumption.
But I would think that the device as designed could be used to disprove that assumption. Consider, once the device has been calibrated, and if the position of the fiber optic cable has some effect on the velocity of light through it, we could make several measurements from varing distances at, say 100 meter distance increments, and through a series of comparisons and calculations, possibly discover an anomoly that could be explained by some linear deviation in the expected results caused by the end of the fiber optic cable somehow *knowing* that it was removed some distance x from the receiving lens.
It would be an interesting experiment, and though I would predict that we would not notice a difference, I would enjoy doing the experiment.
Thanks for the reply and comments.
"The lack of reason is overcome by the passion of belief" < cj@totcon.com >
Bill Hobba - 26 Jul 2005 03:37 GMT > >> Now seperate the end of the fiber optic cable from the receiver ... > >> say a distance of 300 meters. [quoted text clipped - 9 lines] > Astute observation Martin, and I do not *know* for a fact that my > assumption is true. The assumption you are making is one of spatial isotropy/homogeneity which is one of the assumptions aether theories can violate and still be in accord with observation eg in LET we have an aether wind that breaks isotropy but is never actually detectable.
> I base it on experimental evidence that the > velocity of light is constant and relative to the *media* that it is > traveling in. That is - common sense. And no one doubts from common sense it is the same speed in both directions - proving so is another matter.
> I don't have a citation that I can quote for you but I > am sure that a Google search will turn up several. I know many posters to this group would be particularly interested in any concrete experimental way to prove a frames spatial homogeneity/isotropy ie proof similar to Brownian motion proving the existence of atoms. It is the denial that such proof can in principle be found that the claim you can not show OWLS is always constant is based on. And indeed it is obvious it must be so because to measure OWLS you must have some way of syncing the clocks at each end and such syncing is purely a matter of convention - which is the basis of the claim that it is trivially obvious it is not possible to experimentally show OWLS is the same. For example if you choose light as your syncing method then of course OWLS is always constant by fiat. If you choose say firing bullets from a gun then you need to show that the time it takes for the bullet to traverse a certain distance does not depend of where or in what direction the experiment is done - for which you need synced cocks at the start and end points. Indeed to show a frame is inertial under the usual definition of free particles move at constant velocity you need synced clocks to show particles behave that way. There is simply no way to get around the clock syncing issue. Theoretically we can assume an inertial frame is isotropic is which case OWLS constancy follows immediately from TWLS constancy - but showing such a frame is isotropic/homogeneous experimentally is simply not possible.
Bill
> You are absolutely > correct in maintaining that my experimental device is predicated on [quoted text clipped - 18 lines] > "The lack of reason is overcome by the passion of belief" > < cj@totcon.com > bz - 26 Jul 2005 15:13 GMT cj@cjluke.com (C.J. Luke) wrote in news:42e45f37.55113093@news- server.cfl.rr.com:
> The concept is easy. Use one clock, two counter circuits, a laser, > optical receiver, and a one second trigger circuit all co-located in a [quoted text clipped - 4 lines] > *received* at the optical receiver circuit. The length of fiber optic > cabel is initally attached to the receiving lens for calibration. Make it simpler. Use an oscilliscope, a laser diode, a 1000 meter length of fibre cable and a photo diode.
Use a pulse generator, you might save money by using the square wave calibration signal that most scopes have built in.
You measure the time delay introduced by the fiber cable. You make sure that moving the cable around [without moving the end of the cable away from the photodiode] has no effect on the delay introduced by the cable.
You then start to move the end of the cable away from the photodiode and measure the INCREASE in delay.
That increase is the one way speed of light.
If you fasten the end of the cable to the edge of a rotating wheel, you can even determine if c'=c+/-v is valid. You will need to introduce a coupling into the cable to allow the rotation, but the delay introduced by the coupling can be tested and accounted for.
 Signature bz
please pardon my infinite ignorance, the set-of-things-I-do-not-know is an infinite set.
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Tom Roberts - 26 Jul 2005 17:31 GMT > Make it simpler. Use an oscilliscope, a laser diode, a 1000 meter length of > fibre cable and a photo diode. [quoted text clipped - 3 lines] > that moving the cable around [without moving the end of the cable away from > the photodiode] has no effect on the delay introduced by the cable. This merely establishes that the round-trip speed within the cable does not depend on its orientation. It says nothing at all about the difference between east->west propagation compared to west->east propagation in the cable, it ONLY shows that east->west->east propagation is the same as west->east->west propagation (and other orientations as well), in the cable.
> You then start to move the end of the cable away from the photodiode and > measure the INCREASE in delay. > That increase is the one way speed of light. Not true. You make the same mistake that the C.J.Luke keeps making -- you forget that in moving the cable end to the west you change the amount of east->west vs west->east traveling the signal makes within the cable.
In fact, for a change dL to the west, the dime delay dt is:
dt = c1*dL + c2*dL - c3*dL
where c1 is OWLS(west->east in vacuum/air), c2 is OWLS(east->west in cable), and c3 is OWLS(west->east in cable). Only if c2=c3 can you get the answer you desire, and you have no way to establish that equality (i.e. isotropy of OWLS in the cable).
There is no possible variation of this technique that can avoid this problem. For the simple reason that this is INHERENTLY a round-trip measurement, and no round-trip measurement can establish anything about OWLS.
Note that the observed isotropy in TWLS measurements puts a constraint on any anisotropy in OWLS, but that constraint is rather loose, and certainly doesn't require OWLS to be isotropic.
Tom Roberts tjroberts@lucent.com
C.J. Luke - 26 Jul 2005 18:07 GMT >> Make it simpler. Use an oscilliscope, a laser diode, a 1000 meter length of >> fibre cable and a photo diode. [quoted text clipped - 10 lines] >propagation is the same as west->east->west propagation (and other >orientations as well), in the cable. I hate to have to be the one to point this out to you Tom, the light only travels ONE WAY in the fiber optic cable. Also, just for the record, for the orientation of the cable to have any effect on the velocity of light within the cable, would have to presume that experimental evidence showing that the velocity of light is constant and relative to the medium, not to be confused with a vacuum, is in error. If you could provide some insight as to why you believe this it would be useful in understanding your insistance that this is a two way measurement.
>> You then start to move the end of the cable away from the photodiode and >> measure the INCREASE in delay. [quoted text clipped - 24 lines] > >Tom Roberts tjroberts@lucent.com "The lack of reason is overcome by the passion of belief" < cj@totcon.com >
Tom Roberts - 27 Jul 2005 02:45 GMT > I hate to have to be the one to point this out to you Tom, the light > only travels ONE WAY in the fiber optic cable. You are using a horrible PUN on the phrase "one way". One that completely invalidates your argument and claims.
The usual meaning of one way in this context is: from west to east, or from east to west, or from any direction to its opposite. That is, after all, the only sort of COSMIC anisotropy that could possibly be of interest.
Yes, at any point along the cable the light is moving in a single direction. But during your calibration, over the entire length of the cable it necessarily travels an equal distance east->west as it does west->east. THAT is a two-way light path (in the sense used here).
> Also, just for the > record, for the orientation of the cable to have any effect on the > velocity of light within the cable, would have to presume that > experimental evidence showing that the velocity of light is constant > and relative to the medium, not to be confused with a vacuum, is in > error. You are claiming to make a one way measurement. You omitted to mention that you implicitly assume that the OWLS in your fiber optic cable is isotropic -- with such an assumption how could you possibly expect to detect any cosmically-important anisotropy in OWLS? -- you have ASSUMED it away for a major part of your apparatus! And as I have said before, I seriously doubt there is any sensible model in which OWLS in the fiber is isotropic but OWLS in air or vacuum is not.
> If you could provide some insight as to why you believe this > it would be useful in understanding your insistance that this is a two > way measurement. It is a two-way measurement because the light signal follows a round-trip path. That is, the light signal ends up where it started, and thus necessarily travels equal distance east->west as it does west->east (and ditto for all other opposite directions).
Tom Roberts tjroberts@lucent.com
bz - 27 Jul 2005 12:44 GMT Tom Roberts <tjroberts@lucent.com> wrote in news:GGBFe.1312$gt5.1099 @newssvr17.news.prodigy.com:
> It is a two-way measurement because the light signal follows a > round-trip path. But not throught the same medium. The velocity factor of the fiber is known and is slower than the velocity of light in a vacuum.
What about if he eliminates the fiber all together and moves his laser diode to the end of a 1000 foot length of coax [of known velocity factor]? Now, his 'light' is only moving one direction.
> That is, the light signal ends up where it started, and > thus necessarily travels equal distance east->west as it does west->east > (and ditto for all other opposite directions). It would appear that ANY measurement of the speed of light, other than simple 'time of flight' MUST suffer similar defect.
For example speed of light from Jupiters moon requires comparison of time for light that has traveled at least two different paths through space. This makes the measurement a 'two way speed of light' measurement.
Of course, if we are not trying to verify that space is isotropic, then we can stop splitting hares and let the race begin.
 Signature bz
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Tom Roberts - 27 Jul 2005 14:19 GMT > Tom Roberts <tjroberts@lucent.com> wrote in news:GGBFe.1312$gt5.1099 > @newssvr17.news.prodigy.com: [quoted text clipped - 3 lines] > But not throught the same medium. The velocity factor of the fiber is known > and is slower than the velocity of light in a vacuum. Sure. Does not change the fact that this is a ROUND TRIP measurement. <shrug>
> What about if he eliminates the fiber all together and moves his laser > diode to the end of a 1000 foot length of coax [of known velocity factor]? > Now, his 'light' is only moving one direction. Then you have the very same unknowns about the coax. EM signals are EM signals, be they light or electrical pulses in coax. <shrug>
Face it: the signal travels over a round trip path. There's no possible way to turn that into a one way measurement. None. To make a one way measurement the signal must travel only one way. <shrug>
> It would appear that ANY measurement of the speed of light, other than > simple 'time of flight' MUST suffer similar defect. Yes, of course. And "simple time of flight" measurements have the problem of how to synchronize the two clocks that are necessary for such a measurement. Nature, of course, does not need clocks or their synchronization, so the result must be independent of how you synchronize those clocks -- the different theories I discuss differ only in how one synchronizes clocks; and they are experimentally indistinguishable from one another (including SR).
> Of course, if we are not trying to verify that space is isotropic, then we > can stop splitting hares and let the race begin. Many experiments measuring the anisotropy in the round-trip propagation of light have been performed. Several have millions (billions? trillions?) of times more accuracy than this one. All gave null results to within their resolution. See the FAQ for references.
Tom Roberts tjroberts@lucent.com
C.J. Luke - 27 Jul 2005 18:16 GMT >> Tom Roberts <tjroberts@lucent.com> wrote in news:GGBFe.1312$gt5.1099 >> @newssvr17.news.prodigy.com: [quoted text clipped - 13 lines] >Then you have the very same unknowns about the coax. EM signals are EM >signals, be they light or electrical pulses in coax. <shrug> Your little shrugs are cute...not very significant...but cute. By the way, would you care to quote any experiment that proves that light and EM are actually the same? As far as I know, this is a widely accepted hypotheses (belief) that has not actually been proven.
>Face it: the signal travels over a round trip path. There's no possible >way to turn that into a one way measurement. None. To make a one way >measurement the signal must travel only one way. <shrug> Accept the fact that: if the speed of light in a medium is in fact constant with respect to that medium (as is the popular consensus among physicist) then the device as I described will be able to detect any anisotropic behaviour of light in a vacuume. Period. It would be interesting for you to actually reply to this specific assertion, and not attempt to generalize a response centered around some non-descript group of "ugly" theories.
>> It would appear that ANY measurement of the speed of light, other than >> simple 'time of flight' MUST suffer similar defect. [quoted text clipped - 16 lines] > >Tom Roberts tjroberts@lucent.com "The lack of reason is overcome by the passion of belief" < cj@totcon.com >
Tom Roberts - 27 Jul 2005 18:56 GMT > if the speed of light in a medium is in fact constant with respect to > that medium (as is the popular consensus among physicist) then the > device as I described will be able to detect any anisotropic behaviour > of light in a vacuume. A major part of the basis for that "popular consensus among physicists" it the oft-repeated observation that the speed of light is isotropic in vacuum. Take away the latter and you will not have the former. Your claimed support for your assertion holds ONLY in the case where there is no anisotropic behavior of light in vacuum. <shrug>
I repeat: there is no sensible theory in which OWLS is isotropic in the fiber but anisotropic in vacuum. Consider n->1 for the fiber and see why this is so.
I repeat: there are many theories in which OWLS is not isotropic, but your experiment cannot observe the anisotropy (in fact, no experiment can do so). <shrug>
Tom Roberts tjroberts@lucent.com
bz - 27 Jul 2005 19:48 GMT Tom Roberts <tjroberts@lucent.com> wrote in news:dc8hrr $5ft@netnews.net.lucent.com:
> I repeat: there are many theories in which OWLS is not isotropic, but > your experiment cannot observe the anisotropy (in fact, no experiment > can do so). <shrug> I don't understand why the anisotropy would not be dependent upon the velocity factor of light in the media.
Of course if the anisotropy is independent of the velocity factor, then it is clear that the proposed test can not be relied upon. Is there a theoretical reason to expect anisotropy to be independent of media?
 Signature bz
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Tom Roberts - 27 Jul 2005 21:46 GMT > Tom Roberts <tjroberts@lucent.com> wrote in news:dc8hrr > $5ft@netnews.net.lucent.com: [quoted text clipped - 4 lines] > I don't understand why the anisotropy would not be dependent upon the > velocity factor of light in the media. The effect in the fiber is different from the effect in vacuum, and is related to the index of refration of the fiber. The result is that it exactly cancels the anisotropy in the vacuum, for any distance in vacuum for this setup. Basically it is the time delay that is the same (but opposite in sign), not any "ansiotropy factor".
> Of course if the anisotropy is independent of the velocity factor, then it > is clear that the proposed test can not be relied upon. Is there a > theoretical reason to expect anisotropy to be independent of media? No. The anisotropy in a medium MUST depend on the index of refration of the medium. If not, then a) the theory is probably self-inconsistent, and b) many existing measurements refute the theory.
Tom Roberts tjroberts@lucent.com
bz - 28 Jul 2005 14:01 GMT >> Tom Roberts <tjroberts@lucent.com> wrote in news:dc8hrr >> $5ft@netnews.net.lucent.com: [quoted text clipped - 10 lines] > for this setup. Basically it is the time delay that is the same (but > opposite in sign), not any "ansiotropy factor". Is there a mathematical justification for 'the result is that it exactly cancels the ansitropy in the vacuum for any distance in vacuum' or is it just handwaving?
>> Of course if the anisotropy is independent of the velocity factor, then >> it is clear that the proposed test can not be relied upon. Is there a [quoted text clipped - 3 lines] > the medium. If not, then a) the theory is probably self-inconsistent, > and b) many existing measurements refute the theory. That is what I thought but that seems contradictory to 'the result is that it exactly cancels the ansitropy in the vacuum for any distance in vacuum'.
 Signature bz
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Tom Roberts - 29 Jul 2005 14:19 GMT >>The effect in the fiber is different from the effect in vacuum, and is >>related to the index of refration of the fiber. The result is that it [quoted text clipped - 5 lines] > cancels the ansitropy in the vacuum for any distance in vacuum' or is it > just handwaving? For the class of theories I mentioned, it is mathematical.
The theories in that class differ from SR in that clocks are synchronized differently; that is the ONLY difference from SR. In SR, of course, propagation in vacuum is isotropic in any inertial frame, and the propagation of light in any optical medium is isotropic in the inertial frame of the medium. Here everything is at rest in the inertial frame of the fiber (and source+detector).
Imagine a configuration with fiber extended from source+detector to the west, and a return path west->east in vacuum back to source+detector. Imagine placing clocks at both the source+detector and at the fiber/vacuum interface -- in SR clearly the readings of these clocks when the light ray reaches them will reflect the isotropic propagation. Pick any other theory in the class, and it will require adding some fixed offset to the clock at the fiber end relative to the clock at source+detector. So using the new clock setting neither propagation in fiber or in vacuum will be isotropic. But resetting that clock cannot possibly affect the light signal itself, so the measurement at source+detector is unaffected. So clearly the anisotropy in the cable must cancel EXACTLY any anisotropy in vacuum.
>>No. The anisotropy in a medium MUST depend on the index of refration of >>the medium. If not, then a) the theory is probably self-inconsistent, >>and b) many existing measurements refute the theory. > > That is what I thought but that seems contradictory to 'the result is that > it exactly cancels the ansitropy in the vacuum for any distance in vacuum'. The description above did not use the index of refraction of the cable, and is thus independent of the speed of light in the cable. So the anisotropy in the cable must depend on the index of refraction in the cable -- the time change due to anisotropy is fixed (must cancel the vacuum anisotropy), but the time delay in the cable depends on that index of refraction, so the ratio (which characterizes the anisotropy) depends on the index.
Tom Roberts tjroberts@lucent.com
Bilge - 28 Jul 2005 12:10 GMT C.J. Luke:
>>> What about if he eliminates the fiber all together and moves his laser >>> diode to the end of a 1000 foot length of coax [of known velocity factor]? [quoted text clipped - 6 lines] >light and EM are actually the same? As far as I know, this is a >widely accepted hypotheses (belief) that has not actually been proven. Be serious. Light is produced by accelerated charges. That makes it an electromagnetic effect by definition. If light was not electro- magnetic, you couldn't produce it using charged particles.
bz - 26 Jul 2005 19:05 GMT >> Make it simpler. Use an oscilliscope, a laser diode, a 1000 meter >> length of fibre cable and a photo diode. [quoted text clipped - 20 lines] > amount of east->west vs west->east traveling the signal makes within the > cable. We are comparing the speed of light in two very different media. It is unlikely that something will effect BOTH speeds by the same amount.
> In fact, for a change dL to the west, the time delay dt is: > > dt = c1*dL + c2*dL - c3*dL > > where c1 is OWLS(west->east in vacuum/air), c2 is OWLS(east->west in > cable), and c3 is OWLS(west->east in cable). scope laser--------fiber---------------------------------\ diode.............................................-/ East West length fiber is constant. distance diode-fiber is variable. deltat = c1 * delta distance - (cw * lw + ce * le) but lc (length of cable) = lw (length to the west + le (length to the east)
deltat = c1 * delta distance - ce le + cw(le -lc) if ce = cw deltat = c1 * delta distance - cw lc if cw is constant deltat = c1 * delta distance - a constant.
> Only if c2=c3 can you get > the answer you desire, and you have no way to establish that equality > (i.e. isotropy of OWLS in the cable). I don't really care very much. If it appears to be constant, I will be happy.
> There is no possible variation of this technique that can avoid this > problem. For the simple reason that this is INHERENTLY a round-trip > measurement, and no round-trip measurement can establish anything about > OWLS. You perform the test with your cable moved outward in many different directions.
If you find that the delta delay is only dependent on distance between photo diode and the end of the cable, then it doesn't matter that part of your apparatus is has the signal traveling two ways, the ONLY part where the testing of light [in a vacuum] is taking place is between the end of the fiber and the photo diode. Everything else remains 'constant' and drops out of any calculations.
> Note that the observed isotropy in TWLS measurements puts a constraint > on any anisotropy in OWLS, but that constraint is rather loose, and > certainly doesn't require OWLS to be isotropic.
 Signature bz
please pardon my infinite ignorance, the set-of-things-I-do-not-know is an infinite set.
bz+sp@ch100-5.chem.lsu.edu remove ch100-5 to avoid spam trap
Tom Roberts - 26 Jul 2005 22:59 GMT >>Not true. You make the same mistake that the C.J.Luke keeps making -- >>you forget that in moving the cable end to the west you change the [quoted text clipped - 3 lines] > We are comparing the speed of light in two very different media. It is > unlikely that something will effect BOTH speeds by the same amount. Your "unlikely" is not good enough. Not nearly. In fact, for the class of theories I discuss, this is GUARANTEED to happen. But it's not really "affecting both speeds by the same amount", it is actually a cancellation of any anisotropy in the vacuum/air path by the necessary changes in the fiber path.
>>There is no possible variation of this technique that can avoid this >>problem. For the simple reason that this is INHERENTLY a round-trip [quoted text clipped - 3 lines] > You perform the test with your cable moved outward in many different > directions. That does not help in determining any anisotropy of OWLS within the cable.
> If you find that the delta delay is only dependent on distance between photo > diode and the end of the cable, then it doesn't matter that part of your > apparatus is has the signal traveling two ways, the ONLY part where the > testing of light [in a vacuum] is taking place is between the end of the > fiber and the photo diode. Everything else remains 'constant' and drops out > of any calculations. Yes, if the result is isotropy, then your other assumptions cancel away. But that is not what you set out to measure -- it is still the case that OWLS could be anisotropic, but because of cancellations within the fiber the result APPEARS to be isotropic. And in fact, for the class of theories I mentioned, this is GUARANTEED to happen. <shrug>
Tom Roberts tjroberts@lucent.com
C.J. Luke - 27 Jul 2005 01:27 GMT >>>Not true. You make the same mistake that the C.J.Luke keeps making -- >>>you forget that in moving the cable end to the west you change the [quoted text clipped - 32 lines] >the result APPEARS to be isotropic. And in fact, for the class of >theories I mentioned, this is GUARANTEED to happen. <shrug> Answer me this Tom. Do you agree or disagree that the speed of light in the fiber optic cable is constant with respect to the fiber optic cable?
Because this experiment boils down to that. If the speed is constant in the fiber optic cable and not affected by it's motion with respect to anything else, then the device can measure the one way speed of light.
If the speed of light through the cable is not constant wrt the cable, then the device will be able to measure an anomoly....i.e. a difference in the expected speed verses the recorded speed.
In either case it offers some interesting possibilities.
>Tom Roberts tjroberts@lucent.com "The lack of reason is overcome by the passion of belief" < cj@totcon.com >
Tom Roberts - 27 Jul 2005 03:01 GMT > Answer me this Tom. Do you agree or disagree that the speed of light > in the fiber optic cable is constant with respect to the fiber optic > cable? The answer depends on what theory/model you are using. If you use SR then indeed this is so. But there are an infinite number of theories that are experimentally indistinguishable from SR, in which the speed of light relative to the fiber depends on both its orientation and its velocity relative to an ether frame. Note every one of those theories is JUST AS WELL ESTABLISHED as is SR, because every experiment supporting SR also supports all of them, and because no experiment has refuted any of them.
These theories are not well known because a) they are ugly, b) they are complicated, and c) there is no compelling basis for their postulates (as there is for SR's, which are symmetry principles). AFAIK these theories are the only ones consistent with the experimental record (within this domain of locally-inertial measurments).
> If the speed is constant > in the fiber optic cable and not affected by it's motion with respect > to anything else, then the device can measure the one way speed of > light. If the speed is constant in the cable then there is no sensible model or theory in which OWLS is anisotropic, and you have a silly measurement.
I repeat: by assuming OWLS isotropy in the cable you have assumed away the very effect you set out to measure! as I said before: consider the limit as n->1 in the cable -- how could your claims possibly make sense -- for a cable with n=1 how could OWLS be isotropic in the "cable" but anisotropic outside it???
> If the speed of light through the cable is not constant wrt the cable, > then the device will be able to measure an anomoly....i.e. a > difference in the expected speed verses the recorded speed. No, it cannot do so for ANY of those theories mentioned above. The anisotropy in the cable EXACTLY cancels the anisotropy outside the cable. <shrug>
> In either case it offers some interesting possibilities. No, it's both useless and boring: there is no useful information to obtain from it that is not already known from myriad experiments testing SR. The point of performing experiments is to TEST THEORIES, and this experiment has no power to test any theory in any way different from the myriad experiments already performed. This is equivalent to measurements of TWLS using interferometers, but this one has millions (billions? trillions?) of times less accuracy.... So it's boring. And useless.
Tom Roberts tjroberts@lucent.com
rotchm@gmail.com - 27 Jul 2005 04:44 GMT Right on !!!
I hope he understands this time !
C.J. Luke - 27 Jul 2005 18:23 GMT >> Answer me this Tom. Do you agree or disagree that the speed of light >> in the fiber optic cable is constant with respect to the fiber optic [quoted text clipped - 8 lines] >SR also supports all of them, and because no experiment has refuted any >of them. Nice hedge Tom. I asked you (Tom Roberts) if you (Tom Roberts) believe that the speed of light in a medium is constant with respect to that medium. Would you care to answer that question?
>These theories are not well known because a) they are ugly, b) they are >complicated, and c) there is no compelling basis for their postulates [quoted text clipped - 9 lines] >If the speed is constant in the cable then there is no sensible model or >theory in which OWLS is anisotropic, and you have a silly measurement. So you are saying that you don't believe that the speed of light is constant with respect to the medium? And just for clarity....when I use the term *medium* I am refering specifically to a *detectable* *physical* medium, not the vacuum of space or some undetectable *aether*.
>I repeat: by assuming OWLS isotropy in the cable you have assumed away >the very effect you set out to measure! as I said before: consider the [quoted text clipped - 19 lines] >of TWLS using interferometers, but this one has millions (billions? >trillions?) of times less accuracy.... So it's boring. And useless. I hate to just be argumentative, so I will suggest that you have somehow mis-understood this whole series of post. This experiment is nothing like the interferometer experiments that you refer to.
>Tom Roberts tjroberts@lucent.com "The lack of reason is overcome by the passion of belief" < cj@totcon.com >
Bill Hobba - 28 Jul 2005 06:42 GMT > >> Answer me this Tom. Do you agree or disagree that the speed of light > >> in the fiber optic cable is constant with respect to the fiber optic [quoted text clipped - 12 lines] > believe that the speed of light in a medium is constant with respect > to that medium. Would you care to answer that question? What has Toms beliefs got to do with it? It is what we know for sure - not what he what or may not believe. For what it is worth I believe OWLS is constant - proving so is another matter.
Bill
> >These theories are not well known because a) they are ugly, b) they are > >complicated, and c) there is no compelling basis for their postulates [quoted text clipped - 46 lines] > "The lack of reason is overcome by the passion of belief" > < cj@totcon.com > Tom Roberts - 28 Jul 2005 20:40 GMT >>>Answer me this Tom. Do you agree or disagree that the speed of light >>>in the fiber optic cable is constant with respect to the fiber optic [quoted text clipped - 10 lines] > > Nice hedge Tom. It's not a "hedge" at all, it is an EXPLANATION.
> I asked you (Tom Roberts) if you (Tom Roberts) > believe that the speed of light in a medium is constant with respect > to that medium. Would you care to answer that question? The question does not make sense in the abstract -- to make sense of it one must have a theory that defines the concepts used in the question. As I explained above there are an infinite number of equivalent choices and they give different answers.
But among all those theories, SR is BY FAR the simplest to use and the only one with symmetry principles as postulates. So it is convenient to select SR, and in SR OWLS is of course isotropic in any inertial frame, and the speed of light in a medium is constant with respect to the medium.
> So you are saying that you don't believe that the speed of light is > constant with respect to the medium? No, I never said anything like that. You need to READ what I write.
>>No, it's both useless and boring: there is no useful information to >>obtain from it that is not already known from myriad experiments testing [quoted text clipped - 7 lines] > somehow mis-understood this whole series of post. This experiment is > nothing like the interferometer experiments that you refer to. I repeat: you have to READ what I write. Certainly this experiment is different from those interferometer measurements; but from the standpoint of testing theories it is EQUIVALENT to them. And as it is far less accurate, it is boring and useless. <shrug>
Tom Roberts tjroberts@lucent.com
kenseto@erinet.com - 22 Jul 2005 15:37 GMT The experiments described in the following link are capble of measuring OWLS and TWLS. Also they will confirm if OWLS is equal to TWLS as claimed by the SRians <http://www.geocities.com/kn_seto/2005Experiments>
Ken Seto
kenseto@erinet.com - 22 Jul 2005 19:42 GMT Oops sorry...wrong link. Should be: <http://www.geocities.com.kn_seto/2005Experiment.pdf>
Ken Seto
Henri Wilson - 24 Jul 2005 13:16 GMT >We build an instrument that consists of the following: >It has a maste |
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