Power quality · Illustrated guide

Capacitance, Inductance & Reactive Components

A practical introduction to capacitor-bank and reactor measurements, line-to-line equivalents, star/delta connections and kvar calculations.

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You find a 29 kvar, 400 V capacitor bank on site. A meter reads capacitance between L1 and L2. Is that the actual capacitance of one internal capacitor? Not necessarily.

This guide explains what the meter sees, how to calculate kvar from capacitance or inductance, and when those shortcuts stop being reliable.

Try the calculator →Both C and L modes are included.
01 · Fundamentals

What are capacitance (C) and inductance (L)?

C

Capacitance

Farad (F), often µF

A capacitor stores energy in an electric field. In AC, ideal capacitor current leads voltage.

L

Inductance

Henry (H), often mH

An inductor stores energy in a magnetic field. In AC, ideal inductor current lags voltage.

Z

Impedance

Ohms (Ω)

Impedance includes resistance and reactance. It is not another name for inductance.

Think of C and L as physical properties. Their effect on AC is described by reactance X. Total impedance Z also includes resistive losses.

02 · AC behavior

Why frequency changes the result

At higher frequency, an ideal capacitor lets more current flow while an ideal inductor opposes more current. This is why a 50 Hz capacitor-bank calculation cannot automatically be used at 60 Hz without recalculating.

XC=12πfCX_C=\frac{1}{2\pi fC}
XL=2πfLX_L=2\pi fL

For a real reactor, the total impedance includes winding resistance and may depend on magnetic saturation or coupling between phases.

Z=R+jX(simple series model)Z=R+jX\quad\text{(simple series model)}
03 · Three-phase connection

How delta and star differ

For a balanced three-phase bank, each delta branch sits across the full line-to-line voltage. Each star branch sees the phase voltage when its center is floating and all three branches are balanced.

Delta (Δ) — three branchesOne phase-to-phase branch per side
L1L2L3BranchBranchBranch
Between L1 and L2, the meter sees the direct branch in parallel with the other two branches in series, with L3 left floating.
Star (Y) — isolated neutralOne branch from each line to the center
L1L2L3N (floating)
Between L1 and L2, two branches appear in series when the star center is not connected to an external neutral.
Delta branch voltageULLStar branch voltageULL / √3
04 · Field measurement

Why measured L-L capacitance is different

When measuring between two terminals of a disconnected, isolated three-phase capacitor network, the third terminal is left floating. The meter sees combinations of the internal branches—not just one capacitor.

CLL=32CΔC_{LL}=\frac32 C_\Delta
CLL=CY2C_{LL}=\frac{C_Y}{2}

With three ideal uncoupled inductors, the corresponding terminal inductance follows the inverse network-equivalent relationships:

LLL=23LΔL_{LL}=\frac23L_\Delta
LLL=2LYL_{LL}=2L_Y
Critical distinction: the inductive relationships above assume three independent ideal inductors without magnetic coupling. They are not generally valid for a three-phase iron-core reactor measured with a handheld LCR meter.
05 · Power

How to estimate kvar from terminal measurements

For a balanced ideal three-phase capacitor-only bank, the same kvar expression works for delta and isolated star when you use the measured L-L equivalent capacitance:

QC≈2 (2πf) ULL2 CLLQ_C\approx2\,(2\pi f)\,U_{LL}^{2}\,C_{LL}

Here Q is in var, voltage in V and C in farads. For ideal, uncoupled inductors, the corresponding magnitude is:

QL≈2ULL2(2πf)LLLQ_L\approx\frac{2U_{LL}^{2}}{(2\pi f)L_{LL}}

A three-phase reactive-power magnitude corresponds to approximate balanced line current:

I=Q3 ULLI=\frac{Q}{\sqrt3\,U_{LL}}

Use var rather than kvar inside these unscaled formulas.

06 · Worked example

29 kvar capacitor bank, 400 V, 50 Hz, delta

For an isolated, balanced capacitor-only bank, the expected line-to-line capacitance is:

CLL=29 0002×2π×50×4002C_{LL}=\frac{29\,000}{2\times2\pi\times50\times400^2}
CLL≈288.47 μFC_{LL}\approx288.47\ \mu\mathrm F

Because the bank is delta-connected, the capacitance of each equivalent branch is smaller:

CΔ=23×288.47≈192.31 μFC_\Delta=\frac23\times288.47\approx192.31\ \mu\mathrm F

Now imagine you read 285 µF, 289 µF and 288 µF between the three line-terminal pairs. Take their average and estimate the actual kvar with the calculator. Compare the result with the manufacturer's permitted tolerance—not an arbitrary fixed pass/fail threshold.

The rated kvar belongs to the capacitor's nameplate voltage. Actual output varies approximately with the square of the operating voltage for an unchanged pure capacitance.
07 · Limits

Does the same calculation work for reactors?

For simple uncoupled ideal inductors, yes: star/delta series-parallel algebra gives the terminal equivalent and an ideal inductive kvar magnitude. That is why KiloVolt offers an Inductive (L) tab.

But a real reactor may have winding resistance, magnetic coupling between phases, iron-core saturation, varying inductance with excitation and external capacitor/inductor networks. In those cases, a single L-L inductance reading is not enough to determine operating kvar accurately.

To assess a detuned capacitor bank or actual reactor, consult the manufacturer's rated voltage/frequency, test method and instrument measurement conditions.

08 · Before measuring

Work safely with capacitor banks and reactors

Do not take capacitance or inductance measurements on energized equipment. Follow the applicable isolation and lockout procedure, account for stored capacitor energy and verify safe discharge with an appropriate instrument before handling terminals.

Disconnect external reactors, discharge circuits and other components as required by the equipment manufacturer's test procedure. Measurement at the assembled bank terminals may otherwise produce misleading values.

Never use this calculator as a live testing procedure. It estimates ideal component behavior from values measured using a separately approved safe method.
09 · Common mistakes

Common mistakes to avoid

Confusing branch capacitance with L-L capacitance

The meter sees a network equivalent. On an isolated delta bank, the L-L measurement is 1.5 times the equal branch capacitance.

Using 400 V when the nameplate is rated 440 V

For the same capacitance, kvar changes with the square of voltage. Compare at the specified rating.

Assuming every bank has equal phases

Unbalanced readings indicate a need for closer investigation; the average provides only a preliminary kvar estimate.

Treating inductance (L) as impedance (Z)

Real impedance includes resistance and other effects; frequency also matters.

Testing with a reactor or external network still connected

A detuned bank does not behave like an isolated three-capacitor network.

Further reading: ABB — Power Factor Correction and Harmonic Filtering and LIFASA — Capacitor Measurement Technical Note.

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Calculate C, L, kvar and terminal equivalents

Switch between capacitive and inductive components, three-phase star/delta and L-L measurement modes.

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