Impedance Magnitude Calculator – Series RLC |Z| and Phase

Impedance Magnitude Calculator

Combine resistance R with inductive reactance XL and capacitive reactance Xc into the total series impedance. This tool returns the net reactance X = XL - Xc, the impedance magnitude |Z| = sqrt(R^2 + X^2), the phase angle in degrees, the power factor, and the current I = V / |Z| when you supply an applied voltage.

Choose an Input Mode

🎯Real Circuit Presets

🔌Circuit Inputs

Total series resistance; may be 0 for an ideal reactance.

Reactance of the inductor at the operating frequency.

Reactance of the capacitor at the operating frequency.

Used with frequency to compute XL = 2 pi f L.

Applies to the inductance field above.

Used with frequency to compute Xc = 1 / (2 pi f C).

Applies to the capacitance field above.

Operating frequency for the reactance calculations.

Applies to the frequency field above.

RMS volts across the branch; leave 0 to skip current.

Controls rounding on every result card.

Impedance magnitude |Z| 0 ohm sqrt(R^2 + X^2)
Net reactance X 0 ohm X = XL - Xc
Phase angle theta 0 deg atan2(X, R)
Power factor and current 0 PF = cos theta

🔢Formula Snapshot

|Z|sqrt(R^2 + X^2)
XXL - Xc
thetaatan(X / R)
PFcos theta

📏How R and X Combine into |Z|

Resistance RNet Reactance X|Z| = sqrt(R^2+X^2)Phase atan(X/R)
3 ohm4 ohm5 ohm53.13 deg
6 ohm8 ohm10 ohm53.13 deg
10 ohm0 ohm10 ohm0 deg
0 ohm12 ohm12 ohm90 deg
5 ohm5 ohm7.07 ohm45 deg
8 ohm6 ohm10 ohm36.87 deg
12 ohm5 ohm13 ohm22.62 deg
7 ohm-24 ohm25 ohm-73.74 deg

📈Phase Angle and Power Factor

Phase Angle thetaPower Factor cos thetaCircuit BehaviorCurrent vs Voltage
0 deg1.000Purely resistiveIn phase
15 deg0.966Mostly resistiveCurrent lags
30 deg0.866Weakly inductiveCurrent lags
45 deg0.707R equals XCurrent lags
60 deg0.500Strongly inductiveCurrent lags
90 deg0.000Pure inductorLags 90 deg
-45 deg0.707R equals XcCurrent leads
-90 deg0.000Pure capacitorLeads 90 deg

🔌Reactance at Common Frequencies

ComponentValueFrequencyReactanceType
Inductor10 mH60 Hz3.77 ohmXL rises with f
Inductor1 mH1 kHz6.28 ohmXL rises with f
Inductor100 uH10 kHz6.28 ohmXL rises with f
Capacitor10 uF60 Hz265.3 ohmXc falls with f
Capacitor1 uF1 kHz159.2 ohmXc falls with f
Capacitor100 nF10 kHz159.2 ohmXc falls with f
Capacitor470 uF120 Hz2.82 ohmRipple filter

🗃Series RLC Impedance Comparison Grid

R (ohm)XL (ohm)Xc (ohm)X = XL - Xc|Z| (ohm)Phase (deg)
100000100.000.00
102051518.0356.31
86608.000.00
5210-89.43-57.99
310645.0053.13
43035.0036.87
5060204064.0338.66
20015-1525.00-36.87
12167915.0036.87
68806.000.00

Formula Breakdown

Net reactance X = XL - XcSubtract capacitive reactance from inductive reactance. With XL = 7 and Xc = 3, X = 7 - 3 = 4 ohm, a net inductive result.
Magnitude |Z| = sqrt(R^2 + X^2)Add resistance and net reactance as perpendicular sides. With R = 3 and X = 4, |Z| = sqrt(9 + 16) = sqrt(25) = 5 ohm.
Phase theta = atan(X / R)The angle between current and voltage. With X = 4 and R = 3, theta = atan(4 / 3) = 53.13 deg, positive so inductive.
Power factor PF = cos thetaFraction of apparent power that does real work. cos(53.13) = 0.600, so this branch has a 0.6 lagging power factor.
Current I = V / |Z|Ohm law with impedance. At 120 V across |Z| = 5 ohm, I = 120 / 5 = 24 A of branch current.
XL = 2 pi f LInductive reactance grows with frequency and inductance. At 1 kHz with L = 10 mH, XL = 2 pi (1000)(0.01) = 62.83 ohm.
Xc = 1 / (2 pi f C)Capacitive reactance shrinks with frequency and capacitance. At 1 kHz with C = 10 uF, Xc = 1 / (2 pi (1000)(0.00001)) = 15.92 ohm.

💡Impedance Design Tips

Resonance cancels reactance: When XL equals Xc the net reactance X is zero, so |Z| collapses to just R and the phase angle is 0 degrees. A series RLC circuit at resonance draws the largest current for a given voltage because impedance is at its minimum, equal only to the resistance. This is exactly how tuned radio front ends select one station.
Sign of the phase tells the story: A positive phase angle means XL is larger than Xc, the load is net inductive, and current lags voltage, giving a lagging power factor like a motor. A negative angle means Xc dominates, the load is capacitive, and current leads voltage. Keeping the power factor near 1 means keeping net reactance X close to zero.

When looking at an AC circuit schematic, you might feel like resistance is lying to you, but impedance is actualy the quantity that captures everything and helps you predict current and power. Sure enough: In DC circuits, resistance do act consistently; it resists current and turns energy into heat. Alternating current adds elements like capacitors and inductors. Devices that can absorbs energy from or give up energy to the driving voltage out of sync with it. That’s when we combine resistance and reactance into a single magnitude called impedance that includes everything.

The calculator on this page do the vector math needed to turn those three individual values into one number used to predict things like power factor and current. No matter what the frequency, the current is resisted by opposition that converts electricity to heat. On the other hand, an inductor resist a change in current (hence the term inductive), so it increases with frequency. A capacitor resists a change in voltage (hence the term capacitive), so it decreases with frequency. Like resistance, each is expressed in ohms; however, neither dissipates energy but instead stores and releases it.

How to Calculate Impedance in AC Circuits

Since these can’t be added arithmetically as if you were adding R, XL and Xc, you have to combine them, like the sides of a right triangle. That’s why the equation is geometrical pretending to be electronics. That’s because there are two steps to the calculation. Step one: determine net reactance. Capacitive reactance cancels out (partially or completely) inductive reactance. You just subtract the capacitive from the inductive. A circuit containing both an inductor and some capacitance will have a net reactance less than amount of the inductor, but greater than zero if the capacitance isn’t too large.

Step two is to add the net reactance and the resistance using the Pythagorean relationship. The magnitude of impedance equals the square root of R squared plus X squared. That means that a circuit with three ohms of resistance and four ohms of net reactance would have a magnitude of impedance equal to five ohms. You’ll see that familiar three-four-five triangle pop up again and again in AC circuitry precisely because of this.

You do not need to memorize component values to get your answer. Want to just plug in numbers? The calculator allows you to type in reactances if they’re known either from a previous calculation or based off the datasheet. Or perhaps you don’t even have that; maybe you just know what components are present and what frequency they’ll be running at. Toggle the mode back and forth and let the calculator calculate reactances based on standard capacitance and inductance formulas. There are unit selectors for both capacitors (picofarads, nanofarads, etc.) and inductors (millihenries, microhenries, henries). From there it’s a few more clicks to a complete impedance answer.

What’s the phase angle? The phase angle tells you how closely the voltage and current line up in terms of timing. If the angle is zero degrees then the net reactance of the circuit is zero and voltage and current go hand-in-hand perfectly in sync (together). If it’s a positive angle, then the circuit has a net inductance and the current lags the voltage (as motors do and transformers do, classic). If it’s a negative angle, then the circuit has a net capacitance and the current leads the voltage. So that’s where that angle is important; just by seeing the sign of the angle you can quickly diagnose what kind of load you have.

That’s the piece that folks who only look at magnitude tend to miss. That’s the phase angle, and its cosine is called “power factor,” or what fraction of the apparent power is doing any useful work at all. A pure resistance will have power factor of 1; a highly reactive load could be close to zero. Why do utilities care? Because if you’re a load with a lousy power factor, they have to send more current down the wire for the same amount of useful power, wasting money and heating up the wires.

The calculator also outputs the branch current if you plug in an applied voltage. Otherwise, just leave it as zero. In that case, it ignores the voltage and focuses only on the branch impedance characteristics.

There’s one exception to all these rules that we should mention. If the inductive reactance happens to equal the capacitive reactance, then the total reactance becomes zero. That means the size of the impedance reduces to only the resistance (R) and the phase angle also goes to zero. That’s what we call series resonance, the condition that creates the lowest impedance. It’s used by radio tuners and filters which are designed to pick up signals at certain frequencies but not at other ones. Here are some resonant circuits that show how the impedance collapses down to its minimall value when the two reactances cancel each other out.

The presets derived from actual circuits bridge the gap between theory and practice: for instance, you can use pure resistive loads, an inductive motor branch, or a capacitive correction branch and watch the numbers change immediately. If you’re an engineering student studying up on AC theory, a hobbyist trying to size a speaker crossover, or an engineer double-checking the load profile of some branch, this tool will turn what would of been a step-by-step computation into one solid answer. It is no replacement for understanding, but the arithmetic friction that takes the fun out of a design’s tradeoffs is gone. Even when your circuit becomes complicated, the triangle stays a right-angle.

Impedance Magnitude Calculator – Series RLC |Z| and Phase