The attached simulation is for a VLF detector with a concentric (Tesoro) coil. With this setup, all targets give a phase-shift left, non-ferrous targets increase in amplitude, and ferrous give a decrease. There are three simulation runs comprising "no target", a "100us TC non-ferrous (eddy) target", and a "100us TC ferrous (magnetic) target". In order for the ferrous target to give the correct results, the coupling between the target and the RX loop is decreased by 25%, and the coupling coefficient between the nulling and RX loop is increased from 0.71 to 0.7135. As you can readily see, it only takes a small adjustment to account for the distortion of the magnetic field (due to absorption) and produce the necessary amplitude decrease below that of the no target response.
Having tested various targets with a 9" diameter concentric coil connected to a Raptor circuit, I can see that the simulation results are a reasonably close match with reality. I would have expected that the phase-shift in the RX loop would increase with higher TC targets, but this is not the case. In fact, the phase-shift seems to be unrelated to the TC, and is more affected by the distance of the target from the coil. Also, it is important not to confuse the RX phase-shift with the phase angle calculated by sampling the in-phase and quadrature components of the RX signal. In this case, the phase angle
You also have to remember that the double-differentiating architecture of Tesoro-like analog detectors are processing the rate-of-change of the rate-of-change of the RX signal. When a VDI circuit is attached to the outputs of the GEB and DISC channels, the GEB channel will always go positive when any metal target passes over the coil. On the other hand the DISC channel goes positive for non-ferrous and negative for ferrous. In this latter case the value of R is negated, which shifts the calculated value of
If you want to run the same simulation for a DD coil, it is necessary to adjust the TX-RX coupling coefficient to account for absorption with the ferrous target, instead of the nulling coil, which (of course) is no longer there. The target to RX loop coupling coefficient will also need to be adjusted accordingly.
In the attached simulation:
Green = no target
Blue = 100us TC non-ferrous (eddy) target
Red = 100us TC ferrous (magnetic) target
Even without running a similar simulation for a PI detector with a mono coil, it should be fairly obvious that the PI will be unable to distinguish between the ferrous and non-ferrous targets, as only changes in amplitude are available. Without a balanced loop system, there is no way to detect the effects of absorption produced by the ferrous target. All you see is an increase is RX signal for all targets.
Anyway, more food for thought...
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