What if the EMF is affecting the medium in which the photon is passing
through; the vacuum (aka the Higgs field). .


On Sun, Nov 17, 2013 at 1:47 AM, David Roberson <[email protected]> wrote:

>  Is this phenomena accepted by the physics community?  This is the first
> time that I have heard of it and find it very interesting.
>
>  The first question that comes to mind is why does it behave in a
> transient manner?   The interference pattern would not return to a stable
> display if the actual frequency of the photons was permanently modified.
>
>  Dave
>
>
> -----Original Message-----
> From: Axil Axil <[email protected]>
> To: vortex-l <[email protected]>
> Sent: Sat, Nov 16, 2013 6:12 pm
> Subject: Re: [Vo]:Local Calculated Velocity of Space Ship
>
>  The round trip time of light is always constant because that is how a
> clock ticks and is the definition of time itself.
>
> To the Photon Acceleration Effect
> Moon, 
> Russell<http://adsabs.harvard.edu/cgi-bin/author_form?author=Moon,+R&fullauthor=Moon,%20Russell&charset=UTF-8&db_key=AST>
> American Physical Society, Texas Section APS/AAPT/SPS Joint Spring
> Meeting, March 23-25, 2006, abstract #POS.008
>
> Using the principles of the Vortex Theory, it was theorized that when a
> photon encounters an electromagnetic field, both the velocity and the
> frequency of the photon will increase. To prove this revolutionary idea an
> experiment was devised using a laser interferometer and two electromagnets.
> The electromagnets were arranged so that when the beam splitter divided the
> initial beam of laser light into two secondary beams; one of the two
> secondary beams passed back and forth between the two magnets. With the DC
> current to the electromagnets turned off, the two beams formed an
> interference pattern on the target screen. When the current to the
> electromagnets was suddenly turned on, the pattern fluctuated wildly until
> the two beams again reached a quiescent state creating a stable pattern on
> the screen; when the current to the electromagnets was suddenly turned off,
> again the pattern fluctuated wildly until it reached a quiescent state
> forming the initial stable pattern on the screen. It was determined that
> this new effect was a phenomenon created by the increasing frequency of the
> laser light whose velocity is increasing as it passes between the expanding
> electromagnetic field of the magnets. Because it is a new phenomenon in
> science revealing that the speed of light is not a constant but indeed can
> be varied, it possesses great historical significance. It is called the
> Photon Acceleration Effect. Although much more detailed work needs to be
> done investigating this new and revolutionary phenomenon in nature, it is
> reasonable to conclude that it was created by an increase in the frequency
> of the photons passing through the electromagnetic. Also, it must be stated
> that the discovery of this effect was predicted and discovered using the
> principles of the Vortex Theory. 1. . Konstantin A. Gridnev, Russell G.
> Moon, Victor V. Vasiliev. Experiment that discovered the Photon
> Acceleration Effect, Book of abstracts International Symposium on Origin of
> Matter and Evolution of Galaxies (OMEG05), New Horizon of Nuclear
> Astrophysics and Cosmology, November 8-11, 2005, University of Tokyo,
> Tokyo, Japan, p. 77. 2. Russell Moon, Fabian Calvo, Victor Vasiliev. About
> of the Conservation of Lepton Number, Bulletin of the American Physical
> Society http://www.phys.ufl.edu/sesaps05.html72nd Annual Meeting of the
> Southeastern Section of the APS November 10-12, 2005. Gainesville, Fla,
> USA, p. 8, BC.00008 3. R.G. Moon, V.V. Vasiliev. Explanation of the
> Conservation of Lepton Number, Book of abstracts 55 National Conference on
> Nuclear Physics, Frontiers in the Physics of Nucleus, June 28-July 1, 2005,
> St.-Petersburg, Russia, 2005, p. 347
>
>
>
> On Fri, Nov 15, 2013 at 9:57 PM, <[email protected]> wrote:
>
>>  On 16/11/2013 6:04 AM, David Roberson wrote:
>>
>>  jwinter says:
>>
>>
>>
>>
>> *"That is correct.  However for us to measure how fast our signal leaves
>> our ship, we need 2 clocks - Say one at the back of the ship where the
>> signal is launched from and one at the front of our ship to time how long
>> it takes to travel the length of the ship.  The signal *only* leaves our
>> ship at the speed of light *if* we have taken care to re-synchronise our
>> clocks (using the so-called Einstein method) after reaching a steady
>> speed.  If instead we kept the same synchronisation that we had before we
>> started to accelerate, then we would measure the same speed that any
>> previously stationary observer (remote or otherwise) measures (ie the light
>> pulse would travel *much* slower than c travelling from the back of our
>> ship towards the front, and *much* faster than c in the reverse direction!
>> (this is not well known and is a surprise even to many physicists). The
>> important thing here is that once we have reset our clocks to be
>> synchronous in our new high speed inertial frame, (or once we consider
>> ourselves to be at rest), then all distances with respect to our new
>> coordinate system have changed.  In particular the 10 light year remote
>> star, has now instantly (with the synchronism or the consideration that we
>> are stationary) become only 1 light year away.  That is why it will only
>> take us one light year to reach it.  Distances in the reverse direction
>> (places behind us) are likewise increased (instead of decreased) simply by
>> the change of inertial reference frame. However if we consider ourselves
>> using our initial clock synchronisation, then we know our true accumulated
>> speed because we can see that the light pulse is only just travelling a bit
>> faster than us (it takes the pulse a very long time to travel from the back
>> of the ship to the front) and so we are travelling just a shade slower than
>> c.  Also since any clock tick rate is given by an oscillation time, if we
>> use the round trip time of a light pulse travelling from the back of the
>> ship, to the front and back again, as our oscillation tick time, then we
>> know that our time is ticking a lot slower than it was before we
>> accelerated.  If we divide the known distance (10 light years) by our speed
>> measured this way (~0.99c or thereabouts) then we know how many ticks of
>> our (slowed down) clock will happen in that distance - and it will be 1
>> years worth.  Since our clock seems to us to be ticking at its normal rate,
>> we will get there in what feels to us like a year."*
>>
>>  Why would we need two clocks to measure the speed of light leaving our
>> ship?
>>
>>  Quite simply because that is how we measure the speed of anything
>> (distance travelled / time taken).  When it is relatively slow (like a 100
>> meter dash) we can signal from end to end with light and only use a single
>> stopwatch.  But if we want to measure the one-way speed of light itself,
>> then we need 2 clocks - one at each end, and read the time near where the
>> light pulse is launched, and read the time at the other end when the pulse
>> arrives.  If we try to do it with one clock, then we can only measure the
>> round trip time.  The round trip time of light is always constant because
>> that is how a clock ticks and is the definition of time itself.
>>
>>   We were only subjected to a 10 G acceleration for the 1 year drive
>> period.  Does the problem encountered accumulate throughout the entire time
>> that the acceleration is applied?  For example, radiation emitted by our
>> drive engine at the very beginning of the trip would simply be measured by
>> all observers as having a velocity of c.  Also, those on board the ship
>> plus every clock on board would determine everything was normal except for
>> the constant 10 G acceleration due to the drive.  It is normally assumed
>> that the ship is rigidly constructed so that the front remains a constant
>> distance from the rear of the device.
>>
>>  Pretty much correct - but since it is a one-way measurement that is
>> "measured by all observers", you have assumed that they all have the
>> equivalent of two separated clocks which they have synchronised by some
>> means - and usually by assuming that they are stationary.  So observers
>> moving with respect to each other synchronise their clocks differently -
>> and that is how they can all read the same speed (when it is obviously not
>> the same if they all agreed on synchrony!).
>>
>> If the people on board ship (who are being accelerated) want to consider
>> themselves as being at rest, then they have a continually changing
>> synchrony.  From the point of view of external unaccelerated observers they
>> are slowly acquiring a time-shear from the front of the ship to the back.
>> But the effect can also be measured by the people on board ship.  Clocks
>> near the front tick slightly faster than clocks near the back.  If they
>> transport one of clocks to be next to one that has long been separated from
>> it (so that their times can be compared directly without light signalling
>> between) then the one that has spent a while further forward will be found
>> to be fast in comparison to one which was located further back.
>>
>> The same effect happens in a gravitational field (since it is the same as
>> an acceleration) and has been measured on earth.  If one clock is taken to
>> the top of the Eiffel tower (the front of the ship) then it runs slightly
>> faster than the one at ground level (the back of the ship).  With a careful
>> measurement an observer at ground level could measure that "light" from the
>> clock at the top is slightly blue-shifted (because it has fallen through a
>> gravitational field and picked up energy) and vice-versa.  An observer at
>> the back of the space ship could measure the same effect - when the "light"
>> from the clock at the front was emitted it had a particular frequency, but
>> as the back of the ship accelerates to encounter it, by the time it is
>> encountered it is blue shifted.
>>
>> This blue-shift / red-shift effect accumulates for the 1 year drive
>> period, so that at the end of it the clocks are significantly out of sync.
>> You can think of the time difference accumulation between the separated
>> clocks as simply accumulating your acceleration to provide a velocity
>> reading, which you could otherwise do electronically.  When the clock
>> separation divided by the time difference accumulation is equal to the
>> speed of light, at that point (if your time had not slowed down) you would
>> be breaking through the speed of light barrier!
>>
>>   ...Is there any special reason that we would synchronize our clocks by
>> taking into account our original velocity?
>>
>> If we had two clocks, and synchronised them at the start of the trip
>> (before we started to accelerate), then whatever process you choose to do
>> it by assumes our original velocity to be zero.  It doesn't matter if we
>> keep the clocks separated and signal between them through wires or with
>> light, or if we put them together to synchronise them and separate them
>> afterwards.  All presently available methods take into account our original
>> velocity and assume that it is zero.  If we signal between them with light,
>> and if we are "really" moving with respect to an absolute reference frame
>> then our signals are delayed differently in different directions and we
>> have synchronised them with a built-in time-shear.  If we synchronise them
>> when the are next to each other and then separate them, then during the
>> motion of separation one clock travels faster w.r.t the "really" moving
>> absolute reference frame and so ticks slower for the period that the
>> separation motion occurs and acquires a time-shear offset from the other.
>> It turns out (as it always does!) that these methods have the identical
>> effect and if we are "really" moving during clock synchronisation, we
>> cannot avoid synchronising them with a time-shear that matches our initial
>> velocity.
>>
>>   Since that could have been any velocity, it is not clear why it is
>> important.  Suppose we happened to be going at a velocity of c/2 relative
>> to some observer.  No one can determine that he or we are at any particular
>> velocity.  Was that not one of the rules guiding SR and GR?
>>
>>  It doesn't matter what velocity it is.  By synchronising your clocks
>> you have simply calibrated your present speed to read zero.  Comparing the
>> ongoing synchronisation of separated clocks then simply indicates to what
>> velocity, and in which direction you have accelerated with respect to that
>> initial reference frame.
>>
>>
>>  If we adjust our calculations in such a manner as to take into account
>> what other at rest observers determine, then we leave the local frame which
>> I am attempting to analyze.  Let's remain on board the ship until we can
>> milk as much knowledge as possible from this location.  We should assume
>> that we have reached a static constant velocity state once the acceleration
>> period has ended.  Then we look at the world from that point of view to
>> determine our fate.  We are aware of the distance measurement conducted
>> before our acceleration that the star was 10 light years distant.  This
>> information is important and allows us to calculate the time it should take
>> to cover it at our assumed velocity.  Any distance contraction can now be
>> measured by sending a radar probe toward the star.  The reflected beam
>> yields both velocity as shown in the Doppler shifted signal as well as
>> distance calculated by the time delayed return.  At this point the ship is
>> essentially stationary in space and the observer and star are heading
>> towards us.
>>
>>  Do you see a way that this paradox can be resolved without prior
>> knowledge of absolute velocities?
>>
>>  I don't actually see a paradox.  Unless different observers agree on a
>> what reference frame to use, then they cannot even agree on the order in
>> which two events separated in distance happened in time.  This is because
>> the time-shear effect that occurs during synchronisation of slightly
>> separated clocks, when extended to great distances produces very different
>> "now"s.  Observers on earth will consider that "now" on the 10 light year
>> distant star is ~9 years different from the "now" that observers on the
>> space ship contemplate.  After all they will be there in 1 year and so only
>> a years worth of history will pass while they are travelling.  But to
>> earthbound observers 10 years worth of history will pass while the ship
>> makes the journey.
>>
>> Supposing that according to observers on earth who are in (very slow)
>> communication with the remote world (which shares the same reference
>> frame), a nuclear holocaust occurs 5 years after the ship departs on its
>> journey.  According to the travellers who have just started their trip and
>> just reached top speed, when they arrive they will find that it happened 5
>> years ago.  So in their time-sheared frame of reference at the start of the
>> trip the holocaust had already occurred 4 years ago before they left
>> earth!  So the travellers in their travelling reference frame say that the
>> holocaust preceded their departure by 4 years, whereas the earthbound
>> observers say that the departure preceded the holocaust by 5 years.  Can
>> they both be right?  According to Einstein's relativity they are both as
>> right as each other because there is no preferred reference frame.
>>
>> Here is an interesting question.  Supposing one of the travellers had a
>> dearly beloved relative on the distant planet who dies in the holocaust.
>> And supposing, as is so often reported as happening on earth, appears in
>> the traveller's bedroom momentarily after death.  At what point before or
>> during the trip should the apparition occur?  If you want that this
>> occurrence should be almost "immediate" regardless of distance then you
>> need to have a preferred universal reference frame - such as the CMBR.
>> Then all can agree on simultaneity, and instantaneous mental telepathy and
>> suchlike over large distances become non-problematic.
>>
>>
>

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