Electrical reactance 2026-10-14
Electrical reactance is the signed imaginary part of electrical impedance , measured in ohms. It describes the part of the terminal electric potential difference in phase quadrature with the electric current in a sinusoidal steady state. In the convention, an ideal inductor has and an ideal capacitor has for . A large reduces electric current at fixed applied voltage, but an ideal purely reactive component returns the energy it receives over each cycle. This is why electrical reactance and electrical resistance have the same units yet describe different physical behavior. [ref].
Figure 1. . Calculated ideal curves, not measured data: inductance , capacitance , total electrical resistance , and applied root mean square voltage . The is the sensing resistor in electrical reactance bench measurement. Top: , signed , and their sum. Bottom: electric current and voltage-minus-current phase difference. At the sum vanishes, the electric current peaks, and terminal voltage and electric current are in phase. Details.
In a series RLC circuit, electrical impedances add because the same electric current passes through every component. For ideal positive inductance , capacitance , and total electrical resistance ,
Here is voltage wave phase minus current wave phase. Below , and electric current leads terminal voltage; above it, and electric current lags. At , the two signed electrical reactances cancel, leaving and the maximum electric current at fixed terminal voltage. This is the resonant series RLC response. Electrical resistance does not cancel: the toy circuit gives and there. These numbers follow directly from the stipulated component values. [ref].
Cancellation concerns terminal voltage, not the disappearance of stored energy. In the toy circuit at resonance, the individual inductor and capacitor voltages are each in root mean square magnitude, with opposite wave phases, while their sum is zero. Their peak stored magnetic energy and capacitor energy are each , attained at different times. With smaller positive , either component voltage can exceed the applied voltage. This ability to select a frequency while sustaining internal energy exchange connects electrical reactance to tuning and frequency response.
For an ideal inductor or capacitor, the absorbed instantaneous power equals the rate of change of stored energy:
Positive power stores energy; negative power returns it. Over a periodic steady state, each stored energy returns to its initial value, so its cycle-averaged absorbed power is zero. An ideal resistor instead has , transferring energy into Joule heating. More generally, the average terminal power of this series RLC circuit is
Zero average power in an ideal reactive component does not imply zero instantaneous power, zero electric current, or zero stored energy. Real coils and capacitors have losses, so zero ideal reactive loss is a model assumption rather than a claim about every component. [ref].