265.927131
Ω
-67.911217
°
18.849556
Ω
265.258238
Ω
-246.408683
Ω
0.376043
0.003760429
S
265.927131
Ω
-67.911217
°
18.849556
Ω
265.258238
Ω
-246.408683
Ω
0.376043
0.003760429
S
The impedance calculator computes the total AC impedance of a series RLC circuit, along with phase angle, individual reactances, and power factor. Impedance (Z) is the complete opposition to alternating current in a circuit, combining resistive (energy-dissipating) and reactive (energy-storing) components into a single complex quantity: Z = R + j(XL - XC).
Unlike DC circuits where only resistance matters, AC circuit analysis requires impedance because inductors and capacitors introduce frequency-dependent effects. The impedance magnitude |Z| = √(R² + (XL - XC)²) determines how much current flows for a given voltage (I = V/|Z|), while the phase angle θ = arctan((XL - XC)/R) indicates whether current leads or lags the voltage.
In a purely resistive circuit, Z = R and θ = 0° — voltage and current are in phase. When inductive reactance dominates (XL > XC), θ > 0° and current lags voltage — the circuit draws lagging reactive power. When capacitive reactance dominates (XC > XL), θ < 0° and current leads voltage — the circuit draws leading reactive power. At resonance (XL = XC), the circuit is purely resistive with minimum impedance.
Power factor, defined as cos(θ) = R/|Z|, is critical in electrical power systems. A power factor of 1.0 (purely resistive) means all power is useful work. A lagging power factor from inductive loads wastes apparent power (VA) on reactive energy exchange. Utilities often charge industrial customers for low power factor. Capacitor banks are added to correct lagging power factor.
Impedance matching is essential in RF engineering and audio systems. Maximum power transfer from a source to a load occurs when the load impedance is the complex conjugate of the source impedance (ZL = ZS*). Transformer turns ratios and L-networks are used to transform impedances.
This calculator is designed for series RLC circuits. Enter resistance in ohms, inductance in millihenries, capacitance in microfarads, and frequency in hertz to obtain impedance, phase angle, and power factor.
Inductive reactance: XL = 2πfL. Capacitive reactance: XC = 1/(2πfC). Net reactance: X = XL - XC. Impedance magnitude: |Z| = √(R² + X²). Phase angle: θ = arctan(X/R) in degrees. Power factor: PF = cos(θ) = R/|Z|. All component values are converted to SI units (H and F) internally.
If |Z| ≈ R (phase angle near 0°), the circuit is near resonance. A large positive phase angle means high inductive reactance — reduce inductance or increase capacitance. A large negative angle means high capacitive reactance — increase inductance or reduce capacitance. Power factor near 1.0 indicates efficient energy transfer.
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Results
At resonance with R = 10 Ω, |Z| = 10 Ω, θ = 0°, and PF = 1.0 — the circuit is purely resistive.
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Results
An inductive motor load with R = 50 Ω and L = 132.6 mH has |Z| ≈ 86.6 Ω, θ ≈ 54.7° lagging, PF ≈ 0.577 — would need power factor correction.
Impedance Z = R + jX (ohms) is the total opposition to AC current, combining resistance R and reactance X. The magnitude |Z| = √(R² + X²) gives the ratio of voltage to current amplitude (|V|/|I|).
The phase angle θ = arctan(X/R) indicates the time difference between voltage and current. Positive θ means inductive (current lags voltage); negative θ means capacitive (current leads voltage).
For AC circuits, Ohm's law generalizes to V = I × Z (using complex phasors). The magnitude is |V| = |I| × |Z|, and the phase of V is the phase of I plus θ.
Maximum power transfer occurs when the load impedance ZL equals the complex conjugate of the source impedance ZS* (i.e., same magnitude, opposite phase angle). This is critical in RF, audio, and power systems.
Admittance Y = 1/Z (in siemens) is the reciprocal of impedance. Y = G + jB where G = conductance and B = susceptance. Admittance is more convenient for analyzing parallel circuits.
Power factor PF = cos(θ) = R/|Z| determines what fraction of apparent power (VA) is converted to real power (W). Low PF means more current for the same real power — causing higher cable losses and utility penalties.
This calculator is designed for series RLC circuits. For parallel RLC, use admittances: Y = 1/R + 1/(jωL) + jωC, then Z = 1/Y. The resonant frequency is the same, but the impedance behavior is inverted.
At series resonance, XL = XC, so net reactance X = 0 and |Z| = R (minimum). Current is maximum and in phase with voltage. In a parallel LC circuit, resonance creates maximum impedance.
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