As Skippy said above, an ideal inductor has a current that is the integral of the applied voltage. In an RX coil, the applied voltage is the result of Faraday's Law, and is the (negative) derivative of the applied magnetic field. Ergo, the RX coil current waveform represents the magnetic field waveform. The RX voltage is the derivative.
You can certainly filter this back to a fundamental sinusoid and look at it as if it were a normal VLF. Several multifrequency designs do this -- CZ's, DFX, V3. But you can also leave it in the time domain and look at the raw target tau. BBS/FBS does it this way.
You can certainly filter this back to a fundamental sinusoid and look at it as if it were a normal VLF. Several multifrequency designs do this -- CZ's, DFX, V3. But you can also leave it in the time domain and look at the raw target tau. BBS/FBS does it this way.
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