Current-transformer excitation admittance represents the secondary-referred magnetic-core response as a complex ratio between current-transformer excitation current and the induced secondary electric potential difference at a stated frequency:For a passive parallel loss-and-magnetization model, is the in-phase conductance and the inductive susceptance magnitude. NIST's equivalent circuit separates this excitation response from leakage and external current-transformer burden.[ref]
In an original linear model with parallel core-loss electrical resistance and magnetizing inductance ,Thus and when those parameters are positive. For stipulated , and , the corresponding values are and .
At RMS, the excitation phasor is , with magnitude about . Mean power in the modeled loss branch is . The quadrature current also has physical significance even though it supplies no mean power in this ideal sinusoidal branch.
The admittance can be inferred from a measured complex transfer if the circuit assumptions are known. Let , with consistent secondary polarity, and let be winding-plus-burden impedance. The current balance givesWith the current-transformer ratio correction factor and secondary-leading phase , , so the same inversion isMagnitude-only ratio data cannot determine both and without additional information.
A real core is nonlinear, so the effective fundamental ratio can change with excitation amplitude, frequency, waveform and magnetic history. A parameter inferred from a small perturbation about one operating state need not equal the full-signal ratio at another. NIST explicitly notes nonlinear magnetizing impedance and current/burden dependence.[ref]
A Calibration Service for Current Transformers by John D. Ramboz and Oskars Petersons. §1.2, printed pp.4–5
A proposed check measures ratio and phase at several known burdens, compares the inferred admittance values, and tests whether one local model describes them before applying it outside that range. Articles by others on the same topic
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