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© ABCC Australia 2015 new-physics.com
RESURRECTION OF THE MMX –
LENGTH CONTRACTION
© ABCC Australia 2015 new-physics.com
Community Shocked
As soon as Michelson
announced the null results, the
physicists were utterly
shocked. The scientific
community found it hard to
assimilate the failure of MMX
to get the expected results.
The first thing of the failed
MMX did was to whirl the
science world into great chaos.
© ABCC Australia 2015 new-physics.com
Salvaging the Aether
There was a rush of efforts among the scientists to look for what was actually
going wrong. Numerous attempts were made to explain the experiment so as
to salvage the endangered aether postulate.
© ABCC Australia 2015 new-physics.com
Aether Drag Proposal
Michelson himself also
proposed that the aether
near the earth might have
been affected by the earth
and move along with the
earth. This aether flow
would have carried the light
along with it and jeopardize
the results.
© ABCC Australia 2015 new-physics.com
Aether Drag – Partial & Complete
There were existing theories of
two modes by which aether
was being dragged along.
The first one was proposed by
Augustin-Jean Fresnel in 1818.
He thought that the aether is
almost stationary and is
‘partially’ entrained by matter.
This phenomenon was
‘apparently’ confirmed by the
Fizeau experiment in 1851.
Another theory was proposed
by George Stokes in 1845. He
believed that the aether is
‘completely’ entrained within
or in the vicinity of matter. This
proposal was apparently
confirmed by the Michelson–
Morley experiment in 1881
and finally in 1887.
© ABCC Australia 2015 new-physics.com
Contraction Theory
This contradictive situation
form of aether dragging was
later banished by the
contraction theory proposed
independently by George
Fitzgerald (1851-1901) in
1889 and Hendrik Lorentz
(1853-1928) in 1895.
Hendrik Lorentz-
1853-1928
George Fitzgerald
1851-1901
© ABCC Australia 2015 new-physics.com
Lorentz-Fitzgerald
contraction
Both of them try to explain the
experiment by way of length
contraction to an amount
according to their proposed
equation. So the proposals
were called Lorentz-Fitzgerald
contraction.
However it was Lorentz who
put the theory in exact
mathematical form, so the
formulation is also called
Lorentz contraction.
Lorentz-Fitzgerald contraction
© ABCC Australia 2015 new-physics.com
Encumbered Proposal
Of course there were also
others theories proposed
besides the contraction
theory. Only the Lorentz
hypothesis was quoted
because the transformation
equation contained therein
bored special relation to the
development of a
supposedly better theory
that was to come.
𝑙 = 𝑙 𝑜 1 − 𝑣2/𝑐2
𝑙 𝑜 is the length at
absolute rest
𝑙 is the shrunken
length on the move
𝑉𝑒𝑙𝑜𝑐𝑖𝑡𝑦 𝑜𝑓 𝑚𝑜𝑡𝑖𝑜𝑛 𝑆𝑝𝑒𝑒𝑑 𝑜𝑓 𝐿𝑖𝑔ℎ𝑡
© ABCC Australia 2015 new-physics.com
Hendrik Lorentz said in
1906:
“In order to explain this
absence of any effect of the
Earth's translation (in the
Michelson-Morley
experiment), I have ventured
the hypothesis, that the
dimensions of a solid body
undergo slight change, of
the order of 𝑣2
/𝑐2
, when it
moves through the ether. . .
© ABCC Australia 2015 new-physics.com
Lorentz continued: “From this
point of view it is natural to suppose
that, just like the electromagnetic
forces, the molecular attractions and
repulsions are somewhat modified by
a translation imparted to the body,
and this may very well result in a
change of dimensions. The electrons
themselves become flattened
ellipsoids. . . This would enable us to
predict that no experiment made
with a terrestrial source of light will
ever show us an influence of the
Earth's motion.”
10% the speed of light
85% the speed of light
99% the speed of light
99.99% the speed of light
© ABCC Australia 2015 new-physics.com
Beam A under focus
We go to the details first by
considering Beam A which is
aligned with the movement of
the earth and thus reversely
with the aether wind.
Beam B
Beam A
Light Source
Beam B
Beam A
Light Source
© ABCC Australia 2015 new-physics.com
Shrinkage along Motion
The setup contracted along
the direction of motion.
Lorentz considered this
length contraction as a real
physical change in the
material object that depends
on its motion relative to
absolute space.
Beam A
© ABCC Australia 2015 new-physics.com
BeamB
Beam A
Viewer
Light Path Geometry
Since the apparatus set-up
in the experiment contracted
in a certain amount in the
direction of the aether wind,
light would take less time to
travel along such a path
than that along the path
perpendicular to the wind.
Diagram
showing over
emphasized
contraction
Shorter
path thus
less time
© ABCC Australia 2015 new-physics.com
The Data from Michelson
𝐵𝑒𝑎𝑚 𝐴 𝑃𝑟𝑒𝑠𝑒𝑡 𝑃𝑎𝑡ℎ 𝑙𝑒𝑛𝑔𝑡ℎ
2𝑙 𝑜
𝐵𝑒𝑎𝑚 𝐴 𝑇𝑖𝑚𝑖𝑛𝑔
=
2𝑙 𝑜
𝑐 1 − 𝑣2/𝑐2
* 1 − 𝑣2
/𝑐2
𝐵𝑒𝑎𝑚 𝐵 𝑃𝑟𝑒𝑠𝑒𝑡 𝑃𝑎𝑡ℎ 𝐿𝑒𝑛𝑔𝑡ℎ
2𝑙 𝑜
𝐵𝑒𝑎𝑚 𝐵 𝑇𝑖𝑚𝑖𝑛𝑔
=
2𝑙 𝑜
𝑐 1 − 𝑣2/𝑐2
** 1 − 𝑣2/𝑐2
© ABCC Australia 2015 new-physics.com
Transformation
Applying the equation to Beam A:
𝐵𝑒𝑎𝑚 𝐴 𝑇𝑖𝑚𝑖𝑛𝑔
=
2𝑙 𝑜
𝑐 1 − 𝑣2/𝑐2
× 1 − 𝑣2/𝑐2
=
2𝑙 𝑜
𝑐 1 − 𝑣2/𝑐2
𝐵𝑒𝑎𝑚 𝐵 𝑇𝑖𝑚𝑖𝑛𝑔
=
2𝑙 𝑜
𝑐 1 − 𝑣2/𝑐2
Then the two timings are the
same
© ABCC Australia 2015 new-physics.com
Length Contraction
Lorentz has two choices: either
there is a dilation in time or a
contraction in length. Time in
classical physics is a ratio and
has nothing to be changed. So
it may be length because it is
made up of the solid chunk of
stone material. So he assigned
the change to the length
instead of to time as a whole.
Beam A Timing
Shrinkage applied to timing:
=
2𝑙 𝑜
𝑐 1 − 𝑣2/𝑐2
× 1 − 𝑣2/𝑐2
Shrinkage applied to length:
=
2𝑙 𝑜 × 1 − 𝑣2/𝑐2
𝑐 1 − 𝑣2/𝑐2
© ABCC Australia 2015 new-physics.com
Shrinkage Explained MMX
The shortening in path thus
permitted the beam to catch
up with the other beam and
arrive at the viewer at the
same time. In other words,
the contraction was there just
enough to make light to
retain its constancy without
being affected by the way the
apparatus is orientated.
BeamB
Beam A
Viewer
Diagram
showing over
emphasized
contraction
Shorter
path thus
less time
© ABCC Australia 2015 new-physics.com
Application to MMX
By doing the length
contraction, the two timings in
MMX matched perfectly.
𝐵𝑒𝑎𝑚 𝐴 𝑇𝑖𝑚𝑖𝑛𝑔
=
2𝑙 𝑜 × 1 − 𝑣2/𝑐2
𝑐 1 − 𝑣2/𝑐2
=
2𝑙 𝑜
𝑐 1 − 𝑣2/𝑐2
𝐵𝑒𝑎𝑚 𝐵 𝑇𝑖𝑚𝑖𝑛𝑔
=
2𝑙 𝑜
𝑐 1 − 𝑣2/𝑐2
© ABCC Australia 2015 new-physics.com
The Mysterious Factor
The most wonderful thing
is that a very unusual
factor sprung up.
Although Lorentz and
Fitzgerald used it to
explain MMX, they did not
derived the equation. In
fact, you simply have no
explanation to it because it
had come from a basically
wrong concept.
1 − 𝑣2/𝑐2
© ABCC Australia 2015 new-physics.com
Contraction theory
not acceptable
The contraction of material
bodies by itself puzzled the
physicists. It seemed to them
that the phenomenon is out
of this world and did not
appeal to their senses.
?
*
*
© ABCC Australia 2015 new-physics.com
Shrinking - Unfathomable
Phenomenon
It appeared to the scientists
of the day that this way of
thinking about nature is
unfathomable. They
wondered if it was worth to
go to such an extraordinary
length just to prevent the
aether from being detected.
So the contraction theory
was finally not favoured.
© ABCC Australia 2015 new-physics.com
Return of the Dead
We saw the deaths of two
theories:
1. The MMX aether theory by
Maxwell and Michelson.
2. The proposed Length
Contraction postulate by
Fitzgerald and Lorentz.
© ABCC Australia 2015 new-physics.com
𝜸 =
𝟏
𝟏−
𝒗 𝟐
𝒄 𝟐
WAS BORN
But in such a way
© ABCC Australia 2015 new-physics.com
THE REBIRTH OF 𝜸 IN RELATIVITY
To be continued in Episode 3.01

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Length Contraction Theory Resurrected by Einstein's Relativity

  • 1. © ABCC Australia 2015 new-physics.com RESURRECTION OF THE MMX – LENGTH CONTRACTION
  • 2. © ABCC Australia 2015 new-physics.com Community Shocked As soon as Michelson announced the null results, the physicists were utterly shocked. The scientific community found it hard to assimilate the failure of MMX to get the expected results. The first thing of the failed MMX did was to whirl the science world into great chaos.
  • 3. © ABCC Australia 2015 new-physics.com Salvaging the Aether There was a rush of efforts among the scientists to look for what was actually going wrong. Numerous attempts were made to explain the experiment so as to salvage the endangered aether postulate.
  • 4. © ABCC Australia 2015 new-physics.com Aether Drag Proposal Michelson himself also proposed that the aether near the earth might have been affected by the earth and move along with the earth. This aether flow would have carried the light along with it and jeopardize the results.
  • 5. © ABCC Australia 2015 new-physics.com Aether Drag – Partial & Complete There were existing theories of two modes by which aether was being dragged along. The first one was proposed by Augustin-Jean Fresnel in 1818. He thought that the aether is almost stationary and is ‘partially’ entrained by matter. This phenomenon was ‘apparently’ confirmed by the Fizeau experiment in 1851. Another theory was proposed by George Stokes in 1845. He believed that the aether is ‘completely’ entrained within or in the vicinity of matter. This proposal was apparently confirmed by the Michelson– Morley experiment in 1881 and finally in 1887.
  • 6. © ABCC Australia 2015 new-physics.com Contraction Theory This contradictive situation form of aether dragging was later banished by the contraction theory proposed independently by George Fitzgerald (1851-1901) in 1889 and Hendrik Lorentz (1853-1928) in 1895. Hendrik Lorentz- 1853-1928 George Fitzgerald 1851-1901
  • 7. © ABCC Australia 2015 new-physics.com Lorentz-Fitzgerald contraction Both of them try to explain the experiment by way of length contraction to an amount according to their proposed equation. So the proposals were called Lorentz-Fitzgerald contraction. However it was Lorentz who put the theory in exact mathematical form, so the formulation is also called Lorentz contraction. Lorentz-Fitzgerald contraction
  • 8. © ABCC Australia 2015 new-physics.com Encumbered Proposal Of course there were also others theories proposed besides the contraction theory. Only the Lorentz hypothesis was quoted because the transformation equation contained therein bored special relation to the development of a supposedly better theory that was to come. 𝑙 = 𝑙 𝑜 1 − 𝑣2/𝑐2 𝑙 𝑜 is the length at absolute rest 𝑙 is the shrunken length on the move 𝑉𝑒𝑙𝑜𝑐𝑖𝑡𝑦 𝑜𝑓 𝑚𝑜𝑡𝑖𝑜𝑛 𝑆𝑝𝑒𝑒𝑑 𝑜𝑓 𝐿𝑖𝑔ℎ𝑡
  • 9. © ABCC Australia 2015 new-physics.com Hendrik Lorentz said in 1906: “In order to explain this absence of any effect of the Earth's translation (in the Michelson-Morley experiment), I have ventured the hypothesis, that the dimensions of a solid body undergo slight change, of the order of 𝑣2 /𝑐2 , when it moves through the ether. . .
  • 10. © ABCC Australia 2015 new-physics.com Lorentz continued: “From this point of view it is natural to suppose that, just like the electromagnetic forces, the molecular attractions and repulsions are somewhat modified by a translation imparted to the body, and this may very well result in a change of dimensions. The electrons themselves become flattened ellipsoids. . . This would enable us to predict that no experiment made with a terrestrial source of light will ever show us an influence of the Earth's motion.” 10% the speed of light 85% the speed of light 99% the speed of light 99.99% the speed of light
  • 11. © ABCC Australia 2015 new-physics.com Beam A under focus We go to the details first by considering Beam A which is aligned with the movement of the earth and thus reversely with the aether wind. Beam B Beam A Light Source Beam B Beam A Light Source
  • 12. © ABCC Australia 2015 new-physics.com Shrinkage along Motion The setup contracted along the direction of motion. Lorentz considered this length contraction as a real physical change in the material object that depends on its motion relative to absolute space. Beam A
  • 13. © ABCC Australia 2015 new-physics.com BeamB Beam A Viewer Light Path Geometry Since the apparatus set-up in the experiment contracted in a certain amount in the direction of the aether wind, light would take less time to travel along such a path than that along the path perpendicular to the wind. Diagram showing over emphasized contraction Shorter path thus less time
  • 14. © ABCC Australia 2015 new-physics.com The Data from Michelson 𝐵𝑒𝑎𝑚 𝐴 𝑃𝑟𝑒𝑠𝑒𝑡 𝑃𝑎𝑡ℎ 𝑙𝑒𝑛𝑔𝑡ℎ 2𝑙 𝑜 𝐵𝑒𝑎𝑚 𝐴 𝑇𝑖𝑚𝑖𝑛𝑔 = 2𝑙 𝑜 𝑐 1 − 𝑣2/𝑐2 * 1 − 𝑣2 /𝑐2 𝐵𝑒𝑎𝑚 𝐵 𝑃𝑟𝑒𝑠𝑒𝑡 𝑃𝑎𝑡ℎ 𝐿𝑒𝑛𝑔𝑡ℎ 2𝑙 𝑜 𝐵𝑒𝑎𝑚 𝐵 𝑇𝑖𝑚𝑖𝑛𝑔 = 2𝑙 𝑜 𝑐 1 − 𝑣2/𝑐2 ** 1 − 𝑣2/𝑐2
  • 15. © ABCC Australia 2015 new-physics.com Transformation Applying the equation to Beam A: 𝐵𝑒𝑎𝑚 𝐴 𝑇𝑖𝑚𝑖𝑛𝑔 = 2𝑙 𝑜 𝑐 1 − 𝑣2/𝑐2 × 1 − 𝑣2/𝑐2 = 2𝑙 𝑜 𝑐 1 − 𝑣2/𝑐2 𝐵𝑒𝑎𝑚 𝐵 𝑇𝑖𝑚𝑖𝑛𝑔 = 2𝑙 𝑜 𝑐 1 − 𝑣2/𝑐2 Then the two timings are the same
  • 16. © ABCC Australia 2015 new-physics.com Length Contraction Lorentz has two choices: either there is a dilation in time or a contraction in length. Time in classical physics is a ratio and has nothing to be changed. So it may be length because it is made up of the solid chunk of stone material. So he assigned the change to the length instead of to time as a whole. Beam A Timing Shrinkage applied to timing: = 2𝑙 𝑜 𝑐 1 − 𝑣2/𝑐2 × 1 − 𝑣2/𝑐2 Shrinkage applied to length: = 2𝑙 𝑜 × 1 − 𝑣2/𝑐2 𝑐 1 − 𝑣2/𝑐2
  • 17. © ABCC Australia 2015 new-physics.com Shrinkage Explained MMX The shortening in path thus permitted the beam to catch up with the other beam and arrive at the viewer at the same time. In other words, the contraction was there just enough to make light to retain its constancy without being affected by the way the apparatus is orientated. BeamB Beam A Viewer Diagram showing over emphasized contraction Shorter path thus less time
  • 18. © ABCC Australia 2015 new-physics.com Application to MMX By doing the length contraction, the two timings in MMX matched perfectly. 𝐵𝑒𝑎𝑚 𝐴 𝑇𝑖𝑚𝑖𝑛𝑔 = 2𝑙 𝑜 × 1 − 𝑣2/𝑐2 𝑐 1 − 𝑣2/𝑐2 = 2𝑙 𝑜 𝑐 1 − 𝑣2/𝑐2 𝐵𝑒𝑎𝑚 𝐵 𝑇𝑖𝑚𝑖𝑛𝑔 = 2𝑙 𝑜 𝑐 1 − 𝑣2/𝑐2
  • 19. © ABCC Australia 2015 new-physics.com The Mysterious Factor The most wonderful thing is that a very unusual factor sprung up. Although Lorentz and Fitzgerald used it to explain MMX, they did not derived the equation. In fact, you simply have no explanation to it because it had come from a basically wrong concept. 1 − 𝑣2/𝑐2
  • 20. © ABCC Australia 2015 new-physics.com Contraction theory not acceptable The contraction of material bodies by itself puzzled the physicists. It seemed to them that the phenomenon is out of this world and did not appeal to their senses. ? * *
  • 21. © ABCC Australia 2015 new-physics.com Shrinking - Unfathomable Phenomenon It appeared to the scientists of the day that this way of thinking about nature is unfathomable. They wondered if it was worth to go to such an extraordinary length just to prevent the aether from being detected. So the contraction theory was finally not favoured.
  • 22. © ABCC Australia 2015 new-physics.com Return of the Dead We saw the deaths of two theories: 1. The MMX aether theory by Maxwell and Michelson. 2. The proposed Length Contraction postulate by Fitzgerald and Lorentz.
  • 23. © ABCC Australia 2015 new-physics.com 𝜸 = 𝟏 𝟏− 𝒗 𝟐 𝒄 𝟐 WAS BORN But in such a way
  • 24. © ABCC Australia 2015 new-physics.com THE REBIRTH OF 𝜸 IN RELATIVITY To be continued in Episode 3.01