Vasik,
OK, attached is a pix of the basic transformer used in my aforementioned bench experiments. The cores are EC-52 with a center leg gap and the circuit configuration is that the outside coils are the primaries and are connected in a buck mode to drive the center coil secondary. The secondary Ls is biased by a constant current inductor Lcc with Lcc>>Ls. The voltage polarity on Ls is such that when the primaries are being charged, the current in Lcc increases and is clamped at the peak of the primary current. The device gain comes from the differential current in Lcc.
However, if one examines the layout, the MVP of the primaries is in phase with the Ls MVP resulting in a current gain increase in Lcc that is greater than the applied voltage across Lcc using di=E*t/L. In the pix, the transformer on the right will exhibit a current increase of ~10% while the transformer on the left will exhibit an increase of ~15% or greater and also produces a larger COP. Therefore my logic says that the additional coil heighth of the primaries and secondaries provides a greater area for the aiding MVP field between the adjacent winds of the primaries and secondary. I could be wrong of course!
The two core transformer arrangement has reached a COP~1.25 as the best at the moment but I'm sure this can be improved upon over time.
Regards, Pm
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