Current transformer
Ratio, currents, burden voltage and the lead the magnetising current gives, plus what wiring inductance in the sense loop costs you, which becomes critical once the burden is small.
N = N₁·N₂ I₂ = I_pri/N U = I₂·R L₂ = A_L·N₂² φ_mag ≈ arctan( R / (ω·L₂) ) (falls as 1/N₂²) anything in series in the measured loop ADDS to L1
The CT's own leakage is negligible, settled. This page used to carry an open question here, with one model putting the leakage at 13° and another at almost nothing. It is resolved by where the signal is sensed: across L1 + R, which it must be, or there would be no lead at all. That puts the leakage inside the magnetising term, where 920 µH of L_m swamps it. Moving the leakage from 0 to 1 µH shifts the total lead by 0.000085°. The old 13° belonged to a topology that is not on the board.
Wiring inductance is a different animal and still bites. Whatever sits between the sense point and the burden adds straight to L1. At 51 Ω that was a couple of per cent; at 3.9 Ω, 0.3 µH is 28 % of the target angle. Never set L1 by its nominal value, only on the scope, and keep the burden and CT leads extremely short.
The "optimum turns count" stays removed. It rested on the stray phase going as N², which the same model that closed the question above disproves.
The lead from magnetising printed above is the same quantity the CT timing page reports, and it enters the phase-lead budget with a minus.