(C+V) (C−V) MATHEMATICS FOR ELECTROMAGNETIC THEORY

Han Erim

January 1, 2016
Update: January 13, 2016

Electromagnetic Theory does not correctly describe electromagnetic interaction between frames moving relative to each other. (c+v)(c−v) mathematics extends the mathematics of Electromagnetic Theory so that it includes electromagnetic interaction between moving frames. When v = 0 in (c+v)(c−v) mathematics, the currently existing mathematics of Electromagnetic Theory is obtained, which corresponds to electromagnetic interaction between stationary frames. With the introduction of (c+v)(c−v) mathematics into Electromagnetic Theory, significant changes will occur throughout the theory.

“On which principle is (c+v)(c−v) mathematics based?” I can briefly answer this question as follows: (c+v)(c−v) mathematics is the **Rule of Addition of Velocities** for electromagnetic waves. An electromagnetic wave takes the reference frame of its destination as the basis and travels at speed **c** (the speed of light constant) relative to that frame. The direction and speed of motion of the reference frame it is based on do not change this rule. This behavior of electromagnetic waves is represented by (c+v)(c−v) mathematics.

“Is there any evidence for the existence of (c+v)(c−v) mathematics?” Yes, there is. (c+v)(c−v) mathematics shows itself very clearly in the **Doppler Shift** observed in electromagnetic waves.

“What is the physical and theoretical foundation behind (c+v)(c−v) mathematics?” This is a very comprehensive question. In this article, without going into theoretical explanations, I will introduce you to (c+v)(c−v) mathematics through mathematical equations and show you several important equations related to it.
WAVE SPEED = WAVE FREQUENCY × WAVELENGTH

The product of a wave’s wavelength and frequency gives the speed of the wave. Using this fundamental equation, which is also valid for electromagnetic waves, let us see how electromagnetic interaction is intertwined with (c+v)(c−v) mathematics.


Let us assume that we are using a signal transmitter. Let the transmitter’s signal frequency be f0, and its wavelength be λ0(*). An airplane moving away from us will receive the signal—due to Doppler Shift—at frequency f1 and wavelength λ1. An airplane approaching us will receive the signal at frequency f2 and wavelength λ2. (Figure 1)

(*) Now please pay attention;
According to the observer on the receding airplane, the wavelength of the signal reaching him is λ1. But we are on the side of the signal transmitter, and the frequency of our transmitter is f0. If the frequency value of the transmitter is multiplied by the wavelength of the signal detected on the airplane, the speed of the signal traveling toward the airplane is obtained.

Speed of the signal going to the receding airplane

c1 = f0 . λ1        c1 > c



Similarly, for the airplane approaching the signal source, the equation is formed as follows:

Speed of the signal going to the approaching airplane

c2 = f0 . λ2          c2 < c



Therefore, we can express the two equations above as follows:

Signal Speed = Frequency of the Transmitter × Wavelength at the Receiver


This equation is the fundamental equation of electromagnetic interaction.

All errors and deficiencies in today’s Electromagnetic Theory arise from not knowing this equation. The current theory has been built on the assumption that the speed of a signal is constant for all frames (= c), which is extremely wrong. The reason such a major mistake has been made is that the speed of a signal traveling to a moving frame has never been measured until today.


I have now revealed where the mistake in Electromagnetic Theory comes from. From this point on, I will proceed by taking the equation above as the basis.

(c+v)(c−v) Mathematics for Electromagnetic Theory



If we speak for Figure 1 above, the following equations apply for the signal speeds traveling from the transmitter to the airplanes. The “+v” value in the equations is the speed of the receding airplane, and the “−v” value is the speed of the approaching airplane. (The necessary explanation is given in the table below.)

c1 = f0 . λ1 = c + v

c2 = f0 . λ2 = c - v



(c+v)(c-v) Mathematics is the “Rule of Addition of Velocities” for electromagnetic waves.



Let us examine the signal speeds approaching the observers, considering the reference frames of the observers on the airplanes.

According to the observer on the receding airplane, the speed of the signal reaching him is as follows, because the signal and the airplane move in the same direction:
signal speed = speed of the signal traveling toward the airplane − speed of the airplane
c = (c+v) - v

According to the observer on the approaching airplane, the speed of the signal reaching him is as follows, because the signal and the airplane move toward each other:
signal speed = speed of the signal traveling toward the airplane + speed of the airplane
c = (c-v) + v

We see that, regardless of the airplane’s direction, for an observer on the airplane the speed of the signal reaching him is “c”. The two equations above, which yield the constant c, are the Rule of Addition of Velocities for electromagnetic waves.

Let us find the frequency of the signal reaching the observers on the airplanes:
We use the Wave Speed equation.
For the observer on the receding airplane:    f1 = c / λ1
For the observer on the approaching airplane:    f2 = c / λ2
As seen, we have confirmed a known situation within (c+v)(c-v) mathematics.

At this stage we can write a rule for electromagnetic interaction:

Whether a frame is in motion or not, in its own reference frame, the speed of a signal coming toward it is always “c”.



The table below summarizes what has been explained here, using example values.

Formula Value Unit
Velocities of moving frames v 700 m/s
Frequency of the signal transmitter f0 3,180,000,000 Hertz
Speed of light c 299,792,458 m/s
Wavelengths relative to the signal transmitter
Wavelength of the signal in a stationary frame λ0 = c / f0 0.094274358 m
Wavelength of the signal for a receding frame λ1 = λ0 · (c+v)/c 0.094274578 m
Wavelength of the signal for an approaching frame λ2 = λ0 · (c−v)/c 0.094274138 m
According to the signal transmitter:
1) Signal traveling to a receding frame:
Velocity of the target frame +v 700 m/s
Signal speed c1 = c + v 299,793,158 m/s
Signal speed = Signal frequency × Wavelength at the receiver c1 = f0 · λ1 299,793,158 m/s
2) Signal traveling to an approaching frame:
Velocity of the target frame −v −700 m/s
Signal speed c2 = c − v 299,791,758 m/s
Signal speed = Signal frequency × Wavelength at the receiver c2 = f0 · λ2 299,791,758 m/s
According to the receding frame
Speed of the incoming signal c = c1 − v 299,792,458 m/s
Signal frequency f1 = c / λ1 3,179,992,575 Hertz
According to the approaching frame
Speed of the incoming signal c = c2 + v 299,792,458 m/s
Signal frequency f2 = c / λ2 3,180,007,425 Hertz

DOPPLER SHIFT


The fact that the speed of a signal traveling toward a moving target differs from the value “c” causes a deformation in the wavelength of the signal at the moment of emission. This deformation—manifested as either an increase or a decrease in wavelength—is called Doppler Shift. The ratio of the signal’s emission speed (c′ = c ± v) to the speed of light determines the magnitude of the deformation. The change in wavelength occurs in direct proportion to this ratio.



The equation that forms the basis of our discussion provides this information:

Signal Speed = Frequency of the Transmitter × Wavelength at the Receiver



The figure below shows how the equations describing wavelength change can be easily derived using (c+v)(c−v) mathematics.

ALICE EQUATIONS


(c+v)(c−v) mathematics brings with it several important equations. The first of these is an equation that expresses the change in wavelength, in electromagnetic interaction between two frames moving relative to each other, by using distances.

d0 = Distance between the frames at the moment the signal is emitted.
d1 = Distance between the frames at the moment the signal arrives.
λ0 = Normal wavelength of the transmitter (λ0 = c / f0)
λ1 = Wavelength of the signal sent from the transmitter to a moving target (λ1 = (c±v) / f0)


The value "v" in (c+v)(c−v) mathematics represents the rate at which the frames move away from or toward each other, and at the same time indicates the amount by which the signal’s speed deviates from the speed of light. In our previous examples, since motion occurred only along the X-axis, the velocities of the frames were used directly as the value of "v". The equations below show how the value of "v" is calculated in electromagnetic interaction between two frames moving in any direction.


The derivation of these equations is detailed below. The signal transmitter is at point "O". The receiver is moving with velocity "u" in the direction of line "AB". When the receiver is at point "A", a signal is emitted from point "O". When the receiver reaches point "B", the signal also arrives at point "B". In the figures, the length "SB = b" is related to the value "v" through the equation "b = v · Δt", and calculations are based on this relationship. If point "B" lies outside the circle centered at "O" with radius "OA = r", the value of "v" is positive; if it lies inside, "v" is negative.

THE THEORETICAL CONSEQUENCES OF (c+v)(c−v) MATHEMATICS

If (c+v)(c−v) mathematics is experimentally confirmed, a major upheaval in the theory of physics will be inevitable. First of all, a major deficiency in the mathematics of Electromagnetic Theory will be eliminated, which would be a great achievement. Relativity Theory would no longer be needed. As a result, physics would undergo a significant simplification.

Interestingly, when the consequences of (c+v)(c−v) mathematics are examined, we see that concepts such as time dilation, length deformation, and simultaneity — which are also present in Relativity Theory — appear here as well. However, since these concepts are based on a different mathematical foundation, they carry different meanings within (c+v)(c−v) mathematics. Under the name of Alice Law, I have published many works investigating (c+v)(c−v) mathematics and its consequences. You can find these publications at www.aliceinphysics.com. I must admit that I realized quite late that instead of Alice Law, I was actually dealing with Electromagnetic Theory.

As we see here, the interesting behavior of electromagnetic waves based on (c+v)(c−v) mathematics will raise many questions. We will encounter very challenging questions for which we may not yet have answers. The foremost of these questions is undoubtedly: “How can an electromagnetic wave know its destination, and how can it take that reference frame as its basis?” I believe that correct answers can only be obtained through long and painstaking studies.

In its current form, (c+v)(c−v) mathematics only covers uniform linear motion. It is incomplete for interactions between frames undergoing accelerated motion, rotational motion, or other types of complex motion. Eliminating this deficiency will carry Electromagnetic Theory to a much more advanced level.

THE SPEED OF AN ELECTROMAGNETIC WAVE TRAVELING TOWARD A MOVING FRAME HAS NEVER BEEN MEASURED.

Dear Scientists,

The mathematics of Electromagnetic Theory is (c+v)(c−v) mathematics. The only thing this mathematics currently needs is the measurement of the speed of a signal traveling toward a moving frame. Once this is done, what is explained here will take its rightful place in science.

The BYTE SHIFT phenomenon I previously described is a good method to verify (c+v)(c−v) mathematics. Of course, another method could also be chosen.

I kindly ask you to raise your voices and support the urgent performance of an experiment that will reveal (c+v)(c−v) mathematics.

Thank you for reading.

Han Erim