I have attached 4 images to show the different resonant modes.
mode 0: 1/4 wave spread over two coils. This seems possible, I think we all agree.
mode 2: two 1/4 wave coils in concatenated mode. This is what Eric believes to be in Tesla's dream. The problem that I am having visualizing this mode is in the forces acting between the coils. The secondary is exiting the extra by a force F-sec. The extra has some inertia (inductance) which will counteract this force with an equal and opposite force F-ine. So in order to make the swing go the other way, it would seem to me that an extra (outside?) force F-? is needed to overcome F-ine.
mode 1: this seems to me the logical outcome of two 1/4 concatenated coils.
mode 3: the solution that I am using and which is working.
The reason I asked you if you could visualize your mode of resonance (#2) is twofold:
1 - because I can not, and I want to see if I am missing something
2 - if you can, you must also be able to define the conditions for obtaining this mode of resonance, and then it would seem to me only a small step to implement it.
For example in mode 3 the conditions are:
The secondary is freely resonating, that is without capacative or inductive load, meaning at its self-resonance frequency.
The extra and the top-load form a second resonating system so it only acts as a resistive load on the secondary.
Knowing the frequency, you know the wirelength in each coil, and from this you can design both coils.
The ideal secondary will be what I have called a phi-coil since its length to diameter ratio is the golden ratio (phi). The matching extra will become a long thin coil, especially at high frequencies. (but as you know I am still working on that)
But if my interpretation of your answer is correct, you are no longer pursuing mode 2?
Ernst.
mode 0: 1/4 wave spread over two coils. This seems possible, I think we all agree.
mode 2: two 1/4 wave coils in concatenated mode. This is what Eric believes to be in Tesla's dream. The problem that I am having visualizing this mode is in the forces acting between the coils. The secondary is exiting the extra by a force F-sec. The extra has some inertia (inductance) which will counteract this force with an equal and opposite force F-ine. So in order to make the swing go the other way, it would seem to me that an extra (outside?) force F-? is needed to overcome F-ine.
mode 1: this seems to me the logical outcome of two 1/4 concatenated coils.
mode 3: the solution that I am using and which is working.
The reason I asked you if you could visualize your mode of resonance (#2) is twofold:
1 - because I can not, and I want to see if I am missing something
2 - if you can, you must also be able to define the conditions for obtaining this mode of resonance, and then it would seem to me only a small step to implement it.
For example in mode 3 the conditions are:
The secondary is freely resonating, that is without capacative or inductive load, meaning at its self-resonance frequency.
The extra and the top-load form a second resonating system so it only acts as a resistive load on the secondary.
Knowing the frequency, you know the wirelength in each coil, and from this you can design both coils.
The ideal secondary will be what I have called a phi-coil since its length to diameter ratio is the golden ratio (phi). The matching extra will become a long thin coil, especially at high frequencies. (but as you know I am still working on that)
But if my interpretation of your answer is correct, you are no longer pursuing mode 2?
Ernst.
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