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Inductive Reactance⚠ unverified

Electrical / Basic · Compute the reactance of an inductor at a given frequency

Parameters

InputSymbolUnitDefaultDescription
inductanceinductanceH1.0Inductance of the inductor
frequencyfrequencyHz1.0Operating frequency
OutputSymbolUnitDescription
resultXlhenry * hertzInductive reactance, in ohms (Ohm)

The science & history

Understanding the Parameters

Derivation (Approaching a Proof)

The defining relation of an inductor (from Faraday's law) is $v = L\,\dfrac{di}{dt}$. Drive it with a sinusoidal current $i(t) = I_m \sin(\omega t)$, with $\omega = 2\pi f$:

$$v(t) = L\,\frac{di}{dt} = \omega L\, I_m \cos(\omega t) = \omega L\, I_m \sin\!\big(\omega t + \tfrac{\pi}{2}\big).$$

The voltage is sinusoidal with amplitude $V_m = \omega L\, I_m$ and leads the current by $90^\circ$ (equivalently, the current lags). The reactance is the amplitude ratio:

$$X_L = \frac{V_m}{I_m} = \omega L = 2\pi f L.$$

Units. $(\text{1/s})(\text{H}) = (\text{1/s})(\text{V}\cdot\text{s/A}) = \text{V/A} = \Omega$ — genuinely ohms. (Note: the live calculator currently mislabels the output unit as "henry·hertz"; the physical unit is the ohm — flagged for calculator verification.)

History

Inductive reactance rests on Faraday's law of induction (1831) and Lenz's law, which give the inductor's voltage–current relation. As with capacitance, Steinmetz's phasor method (1893) recast it as the impedance $Z_L = j\omega L$, placing reactance on the same ohmic footing as resistance and making AC network analysis algebraic.

Related Concepts: Capacitive Reactance, Impedance, Inductor Energy, Power Factor

Notes: Registry calculator inductive-reactance (unverified). Ideal‑inductor result; real inductors add winding resistance and, at high frequency, parasitic capacitance.

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