The jackbot has a very short memory.
dt=t1 - t2 = 2θoωo(R22 - R12)/c2It cannot have two speeds.
And a negative term.
This is what the jackbot put forth before its readers.
Thus dt=2*omega*alpha*R22/c2-2*omega*alpha*R1^2/c2
=2*omega*alpha*(R22-R12)/c2v = ωR
v
2 = ωR
2v
1 = ωR
1s = Rφ (s = arclength)
dt = 2φωR
22/c
2 - 2φωR
12/c
2 dt = 2v2s2/c2 - 2v1s1/c2BUT THIS IS WRONG!
The Sagnac shift is made up of one term, not two.
You cannot have TWO SPEEDS, only one.
There is no negative term in the Sagnac.
dto/dtr=[4*wo*Ao/c2]/[4*wr*Ar/c2]
=wo/wrONE NEEDS TWO SETS OF RADII.
The radii (along with angle subtended) eliminated to produce the area.But you cannot eliminate the radii.
dt=2*omega*alpha*R22/c2-2*omega*alpha*R1^2/c2
=2*omega*alpha*(R22-R12)/c2[/i]
v = ωR
v
2 = ωR
2v
1 = ωR
1s = Rφ (s = arclength)
dt = 2φωR
22/c
2 - 2φωR
12/c
2 dt = 2v2s2/c2 - 2v1s1/c2BUT THIS IS WRONG!
The Sagnac shift is made up of one term, not two.
You cannot have TWO SPEEDS, only one.
There is no negative term in the Sagnac.
Let us proceed along your line of thought, and see where it will get you.
θo = angle subtended by the two radii, R2 and R1 = orbital angle
s2 = R2 x θo
s1 = R1 x θo
θr = angle subtended by the two radii, r2 and r1 = rotational angle
s2 = r2 x θr
s1 = r1 x θr
R2 - R1 = r2 - r1
r2 x θr = R2 x θo
r1 x θr = R1 x θo
r2/r1 = R2/R1
(r2 x R1) = (r1 x R2)
Since the two areas must be equal,
r1/R1 = (r2 + r1)/(R2 + R1)
Right away, one runs into huge problems with this scenario.
R2 = r2 - r1 + R1
(r2 x R1) = r1r2 - r12 + (R1 x r1)
r2(R1 - r1) = r1(R1 - r1)
So we end up with: r2 = r1, which is impossible
The entire set up doesn't make any sense.
IF YOU BLINDLY SUBSTITUTE THE AREA FOR THE ANGULAR VELOCITY X RADIUS FACTOR, YOU END UP WITH R2=R1 AND r2=r1.
REMEMBER, the original message allowed for NO MINUTE DIFFERENCES AT ALL.
The jackbot's original derivation meant: A = A and R2 - R1 = r2 - r1.
That's all.
From now on, I will not allow any departure from the data set in the original piece of analysis, where no minute differences were implied at all, or even conjectured: jackbot's data simply stated that A = A and R2 - R1 = r2 - r1.
With this data, we reach a direct contradiction in no time at all: r2 = r1.
Here are the jackbot's own words:
That's right. For a given loop, A=A.
For the rotation we have wr, for the orbit we have wo.
∆t=4*A*w/c^2
Thus ∆to=4A*wo/c^2
and ∆tr=4A*wr/c^2.
Comparing the 2:
∆to/∆tr=(4A*wo/c^2)/(4A*wr/c^2)=wo/wr.
Thus it is quite simple to see that the orbital Sagnac is much less than the rotational one due to the much lower angular velocity.
Once again, if you use different loops, your comparison is meaningless.He is telling his readers that THE SAME INTERFEROMETER HAS TO BE USED TO COMPARE THE TWO SAGNAC EFFECTS.
Obviously, it had no idea what the entire contraption entailed at that time.
But now, it is too late to change things.
The jackbot's derivation leads to the situation where r2 = r1, a total nonsense.
Now, it takes A SINGLE COUNTEREXAMPLE TO DEFEAT A CERTAIN HYPOTHESIS.
You can no longer avoid this very simple proof.
Why is the physics illiterate jackbot avoiding the exact Sagnac formula for the rotating linear segment?
Truly pathetic.
As I have already said, the use the phase-conjugate mirrors changes everything.
Now, we can derive the exact Sagnac formula for a rotating linear segment.
It makes this entire thread superfluous.
There is no need to address any further questions: the use of nonlinear optics, mainly the phase-conjugate mirror has been the most extraordinary breakthrough for the Sagnac effect.
Here is the Sagnac formula for A ROTATING LINEAR SEGMENT.
SAGNAC EFFECT WITHOUT AN AREA OR A LOOPThe biggest breakthrough in the physics of the Sagnac effect has been the use of PHASE-CONJUGATE MIRRORS.
In fact, had this technology been available to G. Sagnac and A. Michelson it would have saved them a lot of time and energy in constructing experiments and deriving formulas.
https://arxiv.org/ftp/physics/papers/0609/0609202.pdfTest of the one-way speed of light and the first-order experiment of
Special Relativity using phase-conjugate interferometers
Professor Ruyong Wang
The equation which expresses the relationship between interference fringes and time differences is F=dt[c/λ].
This experiment shows us two important points. First, it confirms the phase reversal of a PCM and
demonstrates the Sagnac effect in an arc segment AB, not a closed path. Second, it gives us important implications: The result, φ = 4πRΩL/cλ, can be re-written as φ = 4πvL/cλ where v is the speed of the moving arc segment AB (where R is the radius of the circular motion, Ω is the rotational rate).
If we increase the radius of the circular motion as shown in Fig. 6,
the arc segment AB will approach a linear segment AB, the circular motion will approach the linear motion, the phase-conjugate Sagnac experiment will approach the phase-conjugate first-order experiment as shown in Fig. 4, and the phase shift is always
φ = 4πvL/cλ.
The Sagnac formula for a straight line path which is rotating becomes:
φ = 4πvL/c2where v = RΩ
That is, the formula for a rotating linear segment is:
φ = 4πvL/c2where v = RΩ
Using the values for v for both the orbital Sagnac and the rotational Sagnac we can see immediately that v
o/v
r = 60.
A total refutation of the "analysis" signed the jackbot.