Impedance Calculator

Impedance Calculator
|Z| = √(R²+X²)
Xₗ = 2πfL
Xᴄ = 1/(2πfC)
θ = arctan(X/R)
Enter Component Values & Frequency
Ω Resistance (R)
Leave blank or 0 to omit
L Inductance (L)
Leave blank or 0 to omit
C Capacitance (C)
Leave blank or 0 to omit
f Frequency (f)
Optional — Power Analysis
V Source Voltage (Vs)
Enter to see current & power
Enter values and frequency to calculate
Impedance Results
Rectangular Form
Polar Form
|Z| Magnitude
Ω
Phase θ
degrees
Nature
 
Xₗ Inductive
Ω
Xᴄ Capacitive
Ω
Net X
Ω
Admittance Y
S
Q Factor
 
Resonant f₀
Hz

Series RLC circuit — components share the same current

Figure 1: Toggle between series and parallel to see how R, L and C connect.

Find Component Value for Target Impedance

Enter what you know and what impedance you need — the calculator finds the missing component.

Z Target |Z|
f Frequency
Ω Known R
Leave blank if unknown
I want to find:
Reverse Solve Result
Required Inductance
Verification

Table of Contents
Fundamentals
  1. What Is Impedance?
  2. Series and Parallel Formulas
Worked Examples
  1. Series RLC at 1 kHz
  2. Parallel RLC at 10 kHz
  3. Speaker Crossover Impedance
  4. At Resonance
Deep Dive
  1. Phase Angle and Power Factor
  2. Inductive vs Capacitive Reactance
  3. Resonance and Q Factor
  4. Complex Impedance Notation
Reference
  1. Frequently Asked Questions
  2. Related AC Circuit Calculators

What Is Impedance?

Impedance is the total opposition that a circuit presents to alternating current. Unlike pure resistance, which opposes both DC and AC equally, impedance accounts for the frequency-dependent behaviour of inductors and capacitors as well. The symbol is Z and the unit is the ohm (Ω).

In a DC circuit you only need Ohm’s law: V = IR. In an AC circuit the voltage and current may be out of phase, so you need a quantity that captures both magnitude and timing. That quantity is impedance: Z = R + jX, where R is resistance and X is reactance. The Ohm’s Law Calculator handles the DC case; this calculator extends it into the AC domain.

Series and Parallel Formulas

Series RLC

When R, L and C are connected in series they share the same current. The total impedance is the vector sum:

Zseries = R + j(XL − XC)
Where XL = 2πfL and XC = 1/(2πfC).
Magnitude: |Z| = √(R² + (XL − XC)²)
Phase: θ = arctan((XL − XC) / R)

Parallel RLC

When R, L and C are connected in parallel they share the same voltage. It is easier to work with admittance (Y = 1/Z):

Yparallel = G + j(BC − BL)
Where G = 1/R, BL = 1/XL, BC = 1/XC.
Then |Z| = 1/|Y| and θZ = −θY

Worked Example — Series RLC at 1 kHz

Given: R = 100 Ω, L = 50 mH, C = 1 µF, f = 1 kHz

Step 1 — Inductive reactance: XL = 2π × 1000 × 0.05 = 314.16 Ω

Step 2 — Capacitive reactance: XC = 1/(2π × 1000 × 1×10−6) = 159.15 Ω

Step 3 — Net reactance: X = 314.16 − 159.15 = 154.99 Ω (inductive)

Step 4 — |Z| = √(100² + 154.99²) = 184.5 Ω

Step 5 — Phase angle: θ = arctan(154.99/100) = 57.2° (voltage leads current)

The positive phase tells us the circuit is inductive at this frequency — the inductor’s reactance dominates. To explore how this phase angle affects real power delivery, see the Phase Angle Calculator.

Worked Example — Parallel RLC at 10 kHz

Given: R = 1 kΩ, L = 10 mH, C = 10 nF, f = 10 kHz

Step 1 — XL = 2π × 10000 × 0.01 = 628.3 Ω

Step 2 — XC = 1/(2π × 10000 × 10×10−9) = 1591.5 Ω

Step 3 — Admittance: G = 1/1000 = 1 mS, BL = 1/628.3 = 1.592 mS, BC = 1/1591.5 = 0.628 mS

Step 4 — Net susceptance: B = 0.628 − 1.592 = −0.964 mS

Step 5 — |Y| = √(1² + 0.964²) = 1.389 mS → |Z| = 720.0 Ω

In parallel circuits the impedance peaks at resonance rather than dipping to a minimum. If you need to find that resonant peak precisely, use the Resonant Frequency Calculator.

Worked Example — Speaker Crossover Impedance

Given: R = 8 Ω (speaker), L = 0, C = 22 µF, f = 3 kHz

Step 1 — XL = 0 (no inductor)

Step 2 — XC = 1/(2π × 3000 × 22×10−6) = 2.41 Ω

Step 3 — |Z| = √(8² + 2.41²) = 8.36 Ω

Step 4 — θ = arctan(−2.41/8) = −16.8° (capacitive)

A capacitor in series with a speaker forms a simple high-pass crossover. The impedance stays close to the nominal 8 Ω at the crossover frequency, but the capacitive phase shift means lower frequencies are attenuated. For the full crossover design with component values, check the Crossover Calculator.

Worked Example — At Resonance

Given: R = 47 Ω, L = 100 mH, C = 100 nF → f0 = 1/(2π√(LC))

Step 1 — f0 = 1/(2π√(0.1 × 100×10−9)) = 1591.5 Hz

Step 2 — At resonance XL = XC = 1000 Ω

Step 3 — Series: |Z| = R = 47 Ω (minimum), θ =

Step 4 — Q = XL/R = 1000/47 = 21.3

A Q factor of 21.3 means this is a sharply tuned circuit — the voltage across the inductor or capacitor at resonance is 21 times the source voltage. This principle is fundamental to RLC circuit analysis, bandpass filter design, and radio tuning.

Phase Angle and Power Factor

The phase angle θ of the impedance tells you how much the voltage leads or lags the current. When θ = 0° the circuit is purely resistive and all power is real. When θ approaches ±90° most of the power is reactive — it sloshes back and forth without doing useful work.

Power factor is simply the cosine of the phase angle: PF = cos(θ). An industrial motor with a lagging power factor of 0.7 (inductive) draws 43% more current than necessary. Power factor correction adds capacitance to cancel the inductive reactance and bring θ closer to zero. The Power Factor Calculator can size the correction capacitor for you.

Inductive vs Capacitive Reactance

Reactance is the frequency-dependent part of impedance. Inductive reactance (XL = 2πfL) increases with frequency — an inductor passes DC freely but increasingly blocks higher frequencies. Capacitive reactance (XC = 1/(2πfC)) decreases with frequency — a capacitor blocks DC but passes higher frequencies.

This complementary behaviour is what makes filters, tuned circuits, and impedance matching possible. For standalone reactance calculations, use the dedicated Inductive Reactance Calculator or the Capacitive Reactance Calculator.

Watch the units. Inductance in millihenries and capacitance in microfarads are common bench values, but the formulas require henries and farads. The calculator above handles unit conversion automatically, but if you are working by hand always convert first.

Resonance and Q Factor

Resonance occurs when XL = XC, at the frequency f0 = 1/(2π√(LC)). In a series circuit the impedance drops to its minimum (just R), and in a parallel circuit the impedance rises to its maximum.

The quality factor Q measures the sharpness of the resonance. For a series circuit Q = XL/R at resonance. Higher Q means a narrower bandwidth: BW = f0/Q. A radio tuner with Q = 50 at 1 MHz has a bandwidth of only 20 kHz — enough to select a single AM station.

The Resonant Frequency Calculator (linked above) provides detailed resonance analysis including bandwidth and damping ratio.

Complex Impedance Notation

Impedance is a complex number: Z = R + jX. The real part R is resistance, and the imaginary part X is reactance. Engineers use j (not i) for the imaginary unit to avoid confusion with current.

There are two equivalent representations. Rectangular form (R + jX) is best for adding impedances in series. Polar form (|Z| ∠ θ) is best for multiplying, dividing, and quick mental estimates. The calculator above shows both.

For circuits with multiple impedances in complex combinations, the Complex Impedance Calculator can handle arbitrary series-parallel networks.

Frequently Asked Questions

What is the difference between impedance and resistance?
Resistance is purely real and does not depend on frequency. Impedance includes resistance plus reactance, which varies with frequency due to inductors and capacitors. In a DC circuit impedance equals resistance.
Why does impedance use complex numbers?
Complex numbers capture both the magnitude and the phase shift between voltage and current. The real part represents energy that is dissipated (resistance), and the imaginary part represents energy that is stored and returned each cycle (reactance).
What happens to impedance at resonance?
At resonance the inductive and capacitive reactances cancel. In a series circuit the impedance drops to its minimum (just R). In a parallel circuit the impedance rises to its maximum. The phase angle is zero at resonance.
Can I use this calculator for a circuit with only R and C?
Yes. Leave the inductance field blank or set it to zero. The calculator will compute the RC impedance correctly. The same applies for R-L circuits — leave capacitance blank.
How is impedance measured in practice?
An LCR meter or impedance analyser applies a known AC signal across the component and measures the resulting voltage and current magnitude and phase. These instruments directly report |Z|, θ, R, X, and other parameters at the test frequency.
What is admittance and when is it useful?
Admittance (Y = 1/Z) measures how easily AC flows. It is measured in siemens (S). Admittance is more convenient for parallel circuits because admittances add directly, just as impedances add directly in series circuits.
Does impedance affect power consumption?
Only the resistive (real) part of impedance dissipates power. The reactive part stores and returns energy. The ratio of real power to apparent power is the power factor, which equals cos(θ). A purely reactive circuit (θ = 90°) draws current but consumes no net power.
How do I convert between impedance forms?
From rectangular to polar: |Z| = √(R² + X²), θ = arctan(X/R). From polar to rectangular: R = |Z|cos(θ), X = |Z|sin(θ).

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Last updated: March 2026