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Ill keep this short sweet and succinct as I have little time with internet access in the wilderness these days. Usually I try to illustrate as well as possible a concept in several ways to really convey the information from several angles, but no time today!
How does one go about creating high Q resonant devices which operate on levels close to the Schumann resonance frequencies? The benefits can be manifold if such a device could be created both in the health and alternative energy field, but many problems plague the inventor.
The recipe for high Q is low ohmic resistance, high inductance, low capacitance.
The recipe for low frequency resonant circuits is high inductance + high capacitance.
Therefore in order to secure a low frequency resonator with high quality factor, one needs to have a VERY high inductance, reasonable capacitance, and very low ohmic resistance. This equates to a REALLY REALLY big coil, many turns, with lots of copper for low resistance, very difficult and expensive to create.
Here is the solution.
Obtain a large ceramic magnet. Give it a ring (tap it with a sharp mechanical impulse and find its resonant frequency in terms of sound). note this resonant peak.
Now excite the magnet at its "acoustic resonant point" and mechanically vibrate it. This vibration in turn creates a changing magnetic field within the space surrounding the magnet at the frequency of the acoustic resonant point. This changing field will impinge back upon the exciting inductor, and it will reach a state of high impedance, little power draw, and large resonant magnetic field (in turn inducing electric fields).
This state acts much like a parallel tank (LC) circuit in that it has a very high impedance point. You now have a resonator in the audible frequency range which uses very little copper windings, and has low resistance internally (ohmic resistance of the winding).
Now you may use TWO of these devices to create Beat frequencies (if you need an explanation "google" it.) The sum and difference of the two frequencies creates your needed Schumann resonance points.
You have now merged sound, with electrical. You have used the large B field of the magnet, and its mechanical properties to create a very efficient tank circuit for low frequency experimentation. You really have no idea how important this technique is.
Please consider these techniques when working with the papers of Frank Znidarsic.
Thank you for your time.
Andrew Manrique.
How does one go about creating high Q resonant devices which operate on levels close to the Schumann resonance frequencies? The benefits can be manifold if such a device could be created both in the health and alternative energy field, but many problems plague the inventor.
The recipe for high Q is low ohmic resistance, high inductance, low capacitance.
The recipe for low frequency resonant circuits is high inductance + high capacitance.
Therefore in order to secure a low frequency resonator with high quality factor, one needs to have a VERY high inductance, reasonable capacitance, and very low ohmic resistance. This equates to a REALLY REALLY big coil, many turns, with lots of copper for low resistance, very difficult and expensive to create.
Here is the solution.
Obtain a large ceramic magnet. Give it a ring (tap it with a sharp mechanical impulse and find its resonant frequency in terms of sound). note this resonant peak.
Now excite the magnet at its "acoustic resonant point" and mechanically vibrate it. This vibration in turn creates a changing magnetic field within the space surrounding the magnet at the frequency of the acoustic resonant point. This changing field will impinge back upon the exciting inductor, and it will reach a state of high impedance, little power draw, and large resonant magnetic field (in turn inducing electric fields).
This state acts much like a parallel tank (LC) circuit in that it has a very high impedance point. You now have a resonator in the audible frequency range which uses very little copper windings, and has low resistance internally (ohmic resistance of the winding).
Now you may use TWO of these devices to create Beat frequencies (if you need an explanation "google" it.) The sum and difference of the two frequencies creates your needed Schumann resonance points.
You have now merged sound, with electrical. You have used the large B field of the magnet, and its mechanical properties to create a very efficient tank circuit for low frequency experimentation. You really have no idea how important this technique is.
Please consider these techniques when working with the papers of Frank Znidarsic.
Thank you for your time.
Andrew Manrique.
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