OK so scaling the blue measurement by the inverse of fuchsia measurement, yields this plot of Crosstalk factor vs. Frequency attached below. As you can see, this time the measurements are made well and the influence of LC circuit's frequency response at the primary winding (pancakes) is cancelled completely (i.e. no peaks around 4MHz). Up to 2.5MHz the crosstalk is much smaller than at higher frequencies, which suggests capacitive coupling. From 6MHz to 7.5MHz the slight downward slope could be taken for inductive coupling but I think this is caused by the intrawinding capacitance of the pancake coils stealing current from their windings at higher frequencies (IOW: current flowing between the windings, instead through the windings). If it was not for the frequency selectivity of the secondary LC circuit, I would expect this downward trend to continue. The large peak at 8.5MHz is most likely an artifact of the frequency selectivity of the secondary LC circuit, which "amplifies" the crosstalk. This should be verified by watching the smaller 8.5MHz peak during the same blue measurement in real time while tweaking the trimmer cap connected to the secondary toroidal coil. IMO the remedy for the undesirable coupling is the E-field symmetrization of the system like Smudge has suggested originally. Also, I would suggest grounded electric shielding*, which does not attenuate HF H-fields strongly. This shielding should be placed between the pancake coils and the toroidal coil (or just wrapped around the toroidal coil). Last, but not least, the H-field symmetrization of all coils and liberal use of Litz wire in their construction, per my earlier suggestions, will also minimize the I/O crosstalk and increase the quality of the signals. * Such shelding is regularly used even in low-frequency power transformers and shielded loop antennas. See here and here
« Last Edit: 2020-07-08, 01:42:59 by verpies »
|