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Resonance Properties of Rotating Ring Circuits.
Friedrich J. Tischer authored a paper entitled "Resonance Properties of Ring circuits" in which he describes a wave guide, in the form of a ring.
If a circular waveguide is excited at a tangent, the excitation (wave) will travel away from the point of excitation (meaning it will go in two directions around the ring, clockwise and counterclockwise).
The paper describes a ring circuit which is excited at two tangents 1/4 wavelength apart. This creates quarter wave interference, meaning that the wave traveling in one direction is negated, and the wave traveling in the other direction is doubled. This is the result of interference of the waves being introduced at the two tangents.
This concept is used in a patent application by the Corum brothers, called "Parametric Power Multiplication" to accomplish the same thing in a lumped element wave guide (individual capacitors and inductors in a ring network).
This in and of itself is a really really interesting concept. A wave, traveling in one direction around a circular track. This is where optics meets electrical engineering.
Now imagine that we take this ring structure and excite it at only one tangent, we have once again a wave traveling in two directions around the structure, and this will cause an interference pattern of its own, the super position of the waves will create its own interference pattern (not quarter wave).
Now, we spin the structure. What happens?
The wave traveling in the direction of the spin will be augmented by the the velocity of the spining structure. It will have a "blue shift" to to an outside observer.
the wave traveling in the direction against the spin will be retarded by the velocity of the spining structure. It will have a "red shift" to an outside observer.
http://upload.wikimedia.org/wikipedi...eshift.svg.png
This will create a differential of perceived frequency's to the static outside observer.
The more quickly the ring spins, the greater the red and blue shift (Doppler shift) between the wave propagation going with the spin of the ring, and the one going against.
One frequency gets higher and higher, and one gets lower and lower.
And now we can see that these two frequencies will interact with the static environment through superposition of waves. This will create beat frequencies, and interference patterns with the local environment around the excited ring.
The beat frequencies created will be known from the equations (f1+f2) and (f1-f2).
as the spin of the ring is changed, the multitude of frequencies created outside the ring will will change. different patterns, and different harmonic sets will arise.
I cannot say for certain what this implies, but I can imagine....
Friedrich J. Tischer authored a paper entitled "Resonance Properties of Ring circuits" in which he describes a wave guide, in the form of a ring.
If a circular waveguide is excited at a tangent, the excitation (wave) will travel away from the point of excitation (meaning it will go in two directions around the ring, clockwise and counterclockwise).
The paper describes a ring circuit which is excited at two tangents 1/4 wavelength apart. This creates quarter wave interference, meaning that the wave traveling in one direction is negated, and the wave traveling in the other direction is doubled. This is the result of interference of the waves being introduced at the two tangents.
This concept is used in a patent application by the Corum brothers, called "Parametric Power Multiplication" to accomplish the same thing in a lumped element wave guide (individual capacitors and inductors in a ring network).
This in and of itself is a really really interesting concept. A wave, traveling in one direction around a circular track. This is where optics meets electrical engineering.
Now imagine that we take this ring structure and excite it at only one tangent, we have once again a wave traveling in two directions around the structure, and this will cause an interference pattern of its own, the super position of the waves will create its own interference pattern (not quarter wave).
Now, we spin the structure. What happens?
The wave traveling in the direction of the spin will be augmented by the the velocity of the spining structure. It will have a "blue shift" to to an outside observer.
the wave traveling in the direction against the spin will be retarded by the velocity of the spining structure. It will have a "red shift" to an outside observer.
http://upload.wikimedia.org/wikipedi...eshift.svg.png
This will create a differential of perceived frequency's to the static outside observer.
The more quickly the ring spins, the greater the red and blue shift (Doppler shift) between the wave propagation going with the spin of the ring, and the one going against.
One frequency gets higher and higher, and one gets lower and lower.
And now we can see that these two frequencies will interact with the static environment through superposition of waves. This will create beat frequencies, and interference patterns with the local environment around the excited ring.
The beat frequencies created will be known from the equations (f1+f2) and (f1-f2).
as the spin of the ring is changed, the multitude of frequencies created outside the ring will will change. different patterns, and different harmonic sets will arise.
I cannot say for certain what this implies, but I can imagine....
) inside would do the job...
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