How did Tesla create such high frequency currents?

AI Thread Summary
Tesla achieved high frequency currents through innovative designs, notably a high frequency alternator featuring a 30-inch steel disk with 384 poles and zigzag windings, which operated at 3000 rpm to produce 200 volts at frequencies between 9600 to 10,000 Hz. His later machines improved upon this, reaching frequencies of up to 30,000 Hz. The discussion highlights the significance of defining "high frequency" in relation to other physical quantities, emphasizing the need for context in such comparisons. Tesla's work also included a spark gap LC transmitter, which utilized resonant circuits to generate frequencies. Overall, Tesla's pioneering efforts laid the groundwork for advancements in high frequency electrical engineering.
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I've read his book and he talks about AC current frequencies of incredibly high magnitudes. How was this achieved? Surely he did not just spin his dynamo really, really fast.
 
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How high did he go? Does your book say?
 
Perhaps..

http://www.mentallandscape.com/Tesla1.htm

His first experiments were with a unique new high frequency alternator [5]. This was made up of a steel disk 30 inches in diameter with 384 poles like the teeth of a cog that had zigzag windings on them. This disk revolved within a fixed ring that had 384 inductor poles. When this machine was turned at 3000 rpm, it produced about 200 volts at 9600 to 10,000 Hz. Tesla was the first man to work with such a device [6]. Later machines of somewhat different design produced up to 30,000 Hz.

It continues with a description of his later work including a spark gap LC transmitter. Basically this is a resonant circuit that is hit with an impulse to make it "ring" at the resonant frequency.
 
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10 kHz is still in the acoustic domain (for sound). Why is this "such high frequency" according to you? When you say something is very large, or very small, you must tell us what physical quantity of the same kind you are comparing it with.
 
I was using the Smith chart to determine the input impedance of a transmission line that has a reflection from the load. One can do this if one knows the characteristic impedance Zo, the degree of mismatch of the load ZL and the length of the transmission line in wavelengths. However, my question is: Consider the input impedance of a wave which appears back at the source after reflection from the load and has traveled for some fraction of a wavelength. The impedance of this wave as it...
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