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Locked Re: Mobius Shielded Loop Antenna
¿ªÔÆÌåÓýJohn and Andrew are both correct.If modeled as a voltage source in series with inductance, you will find the output voltage into a resistive load is independent of frequency above a certain threshold, just as with the parallel current source model. This is because the loop voltage source EMF increases linearly with frequency at 6 dB/octave (induced voltage is proportional to rate of change of the magnetic flux, so when you differentiate the sin(wt) the flux rate of change becomes -w*cos(wt)) and voltage divider formed by the loop's inductive reactance (which doubles per octave) in series with the amplifier input resistance decreases the signal at the amplifier input at the same 6 dB/octave if the frequency is sufficiently high such that the amplifier input impedance is much less than the inductive reactance of the loop.? In other words, the 6 dB/octave rising voltage output is canceled by the -6 dB/octave voltage divider effect and the net voltage input into the loop amplifier is constant with frequency. This series model predicts the same behavior as a parallel current source, so either may be used provided you take care to get the maths correct. The simplistic -6 dB/octave LR voltage divider assumes, as mentioned earlier,? that the loop's inductive reactance is large compared with the input impedance of the amplifier. Jack K8ZOA On 8/20/2013 6:49 AM, Andrew Ikin
wrote:
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