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Engineering Guide

Capacitor Networks, Reactance, Impedance, and AC Behavior

Equivalent capacitance is only the start of a network design. Frequency, phase, voltage sharing, ripple current, ESR, ESL, leakage, derating, and layout determine whether the real bank behaves like the ideal result.

CapacitorsIntermediate18 min readUpdated October 7, 2026

Network Analysis Workflow

StepActionEngineering Check
Define the waveformSet DC bias, RMS and peak AC voltage, frequency range, harmonics, transient energy, and duty cycle.
Choose topologyUse parallel parts for more capacitance and current sharing; use series parts only with voltage-sharing analysis.
Calculate ideal equivalentApply the correct reciprocal or additive relationship using base units.
Calculate frequency behaviorFind reactance and complex impedance at every relevant frequency, not only a nominal point.
Calculate current and energyUse RMS current for heating and peak voltage for dielectric stress and stored energy.
Add nonideal elementsInclude ESR, ESL, leakage, tolerance, bias derating, temperature, and self-resonance.
Check ratingsVerify voltage distribution, ripple current, dissipation, temperature rise, and surge or pulse limits.
ValidateMeasure capacitance, impedance, current, voltage sharing, and temperature under the real assembly conditions.

Ideal and Real Quantities

QuantityFormula or MeaningBoundary
Parallel capacitanceCeq = sum(Ci)Voltage is common; ideal current divides by branch impedance
Series capacitance1/Ceq = sum(1/Ci)Charge is common; voltage division depends on capacitance and leakage
Reactance XC1/(2 pi f C)Magnitude of ideal capacitor impedance
Ideal impedanceZC = 1/(j omega C) = -jXCIncludes the -90 degree phase relation
Real impedanceESR + j(omega ESL - 1/(omega C))Changes near self-resonance
Stored energy0.5 C V squaredUses capacitor terminal voltage
Ripple lossApproximately Irms squared x ESRESR varies with frequency and temperature

Series and Parallel Networks

Formula reference

Equivalent capacitance

Parallel: Ceq = sum(Ci)Series: 1/Ceq = sum(1/Ci)Two in series: Ceq = C1 C2/(C1 + C2)Series ideal voltage: Vi = Q/Ci

Variable definitions

Parallel branches share voltage
Ideal series parts share charge
Real DC voltage sharing depends on leakage
Recalculate tolerance corners

Use the Series & Parallel Capacitor Calculator for ideal equivalents, then check voltage and ripple-current sharing.

Reactance, Impedance, Current, and Loss

Formula reference

AC capacitor model

XC = 1/(2 pi f C)Zideal = -jXCIrms = Vrms/XCZreal approximately ESR + j(omega ESL - 1/(omega C))Ploss approximately Irms squared x ESRE = 0.5 C V squared

Variable definitions

Reactance is not real resistance
Use RMS current for heating
ESR and ESL depend on frequency and construction
Check self-resonance and bias derating

Use the Capacitive Reactance Calculator for the ideal frequency relationship. Use the existing RC design Guide when a resistor and transfer function define the circuit.

Worked Examples

Parallel pair

10 uF and 22 uF in parallel give 32 uF ideal equivalent capacitance.

Series pair

10 uF and 22 uF in series give about 6.875 uF ideal equivalent capacitance.

Equal series parts

Two equal 100 uF capacitors in series give 50 uF and ideally split applied voltage equally.

Tolerance corner

Parallel minimum and maximum values are found by summing the individual tolerance corners, not by assuming nominal.

Reactance

A 1 uF ideal capacitor at 1 kHz has XC about 159.15 ohms.

AC current

With 10 V RMS across that ideal capacitor, current magnitude is about 62.83 mA.

Frequency scaling

Doubling frequency halves ideal capacitive reactance.

Stored energy

A 100 uF capacitor at 12 V stores 7.2 mJ.

ESR heating

A 2 A RMS ripple current through 40 milliohms ESR produces about 0.16 W loss.

Self-resonance

Above self-resonant frequency, ESL dominates and the part behaves increasingly inductively rather than as an ideal capacitor.

Common Mistakes

Adding series capacitances directly.
Using the reciprocal formula for parallel parts.
Assuming series capacitors always share DC voltage equally.
Ignoring leakage-current spread and balancing resistors in high-voltage stacks.
Using reactance magnitude as though it were a positive real resistance.
Ignoring phase when combining capacitor impedance with other elements.
Using peak current where an RMS heating value is required.
Using nominal capacitance despite DC-bias and temperature derating.
Ignoring ESR ripple heating.
Ignoring ESL and self-resonant frequency.
Assuming parallel parts share current equally despite layout and ESR differences.
Treating a calculator result as a substitute for impedance curves and pulse ratings.

Related Calculators

Support reference

FAQ

How do capacitors add in parallel?

Ideal parallel capacitances add directly because every branch has the same voltage and branch charge adds.

How do capacitors add in series?

The reciprocal equivalent is the sum of reciprocal capacitances. For two parts, Ceq equals C1 times C2 divided by C1 plus C2.

Why is series capacitance smaller than either capacitor?

The same charge must develop voltage across each part, so total voltage per unit charge is larger and equivalent capacitance is smaller.

Do series capacitors share voltage equally?

Only identical ideal capacitors do. Real DC sharing depends strongly on leakage, tolerance, temperature, and balancing networks.

What is capacitive reactance?

Capacitive reactance magnitude is 1 divided by 2 pi frequency and capacitance. It decreases as frequency or capacitance increases.

Is capacitive reactance the same as resistance?

No. Ideal capacitor impedance is imaginary and produces phase shift; resistance dissipates real power.

How do I calculate capacitor AC current?

For a sinusoid in the ideal model, RMS current magnitude equals RMS voltage divided by reactance, or 2 pi f C times RMS voltage.

How is capacitor energy calculated?

Stored energy is one half capacitance times terminal voltage squared.

Why does a capacitor heat under AC ripple?

RMS ripple current dissipates power in ESR and other dielectric and conductor losses.

What is capacitor self-resonance?

Capacitance resonates with package and connection inductance. Near resonance impedance reaches a minimum; above it the part becomes increasingly inductive.

Can I parallel capacitors to increase ripple-current capability?

Often yes, but current sharing depends on ESR, ESL, value, temperature, and layout. Verify individual and bank ratings.

How should I validate a capacitor network?

Use the exact parts' impedance and derating data, inspect layout parasitics, and measure voltage sharing, ripple current, impedance, and temperature over operating corners.

Summary

Apply the correct network equation, calculate complex behavior across frequency, and close the design with voltage sharing, ripple-current, ESR, ESL, self-resonance, derating, tolerance, and thermal checks using the exact component data.