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Capacitors Energy Power

Reference data and engineering information about capacitors energy power for electrical applications.

capacitorsenergypowerCalculator

Overview

Capacitors store energy in an electric field between their plates. The stored energy and the power available during discharge are fundamental to designing timing circuits, power supplies, and energy storage systems. This page covers the core formulas for energy storage, instantaneous power delivery, and discharge time under constant-power loading.

Key Formulas

Energy Stored in a Capacitor

W=12CV2W = \frac{1}{2} C V^2

Where W is the energy stored (joules), C is capacitance (farads), and V is the voltage across the capacitor (volts).

Average Power During Discharge

P=Wt=CV22tP = \frac{W}{t} = \frac{C V^2}{2\,t}

This gives the average power over a discharge pulse of duration t. In practice, discharge starts at a peak and decays, so this is a rough engineering estimate rather than a constant instantaneous value.

Discharge Time at Constant Power Load

t=WP=CV22Pt = \frac{W}{P} = \frac{C V^2}{2\,P}

Rearranging the power equation gives the time required to fully discharge a capacitor into a load that consumes power P at a constant rate.

Variables

SymbolDescriptionUnit
WWEnergy stored (work done)J
CCCapacitanceF
VVVoltage across capacitorV
PPPowerW
ttDischarge times

Example Calculation

A 10 µF capacitor is charged to 230 V.

Stored energy:

W=12×10×106×2302=0.265 JW = \frac{1}{2} \times 10 \times 10^{-6} \times 230^2 = 0.265 \text{ J}

Average power if discharged in 5 µs:

P=0.2655×106=52900 W53 kWP = \frac{0.265}{5 \times 10^{-6}} = 52\,900 \text{ W} \approx 53 \text{ kW}

Capacitor Energy and Power

Capacitor Discharge Time at Constant Power

Unit Converter

Capacitance, Energy, and Power Unit Converter

Original Source Images

The following original source images are preserved to avoid losing visual reference material. When an image contains chart or tabular data, its extracted values are represented in the page tables, calculators, or interactive charts; remaining images are retained as visual source references.

capacitor Capacitor

Source Table Coverage

The cached source includes Engineering ToolBox layout/search rows around the calculator area. The substantive migrated content is preserved as the capacitor energy calculator, dielectric breakdown table, original capacitor image, and the unit converter above.

2 rows
Original source layout/search table preserved for completeness; it is not engineering calculation data.
Source cell 1
Source cell 2
Source cell 3
Source cell 4
Source cell 5
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Source: engineeringtoolbox.com

Engineering Notes

  • Exponential decay: In a resistive-load circuit, voltage (and therefore instantaneous power) decays exponentially — not linearly. The P=W/tP = W/t formula yields a rough average over the pulse duration, not the peak.
  • Peak power is higher: At the start of discharge the instantaneous power is Ppeak=V2/RP_{\text{peak}} = V^2 / R (for a resistive load), which can far exceed the average value.
  • ESR limits: Real capacitors have equivalent series resistance (ESR) that limits peak current and converts some energy to heat inside the component rather than the load.
  • Safe design margin: Always derate the working voltage well below the dielectric breakdown value, accounting for temperature, aging, and transient overvoltage.

Breakdown Voltage by Dielectric

Puncture voltage measured at 1 MHz. Values in V per mil (1 mil = 0.001 inch ≈ 25.4 µm).

This dielectric breakdown table is retained as source-related capacitor design reference material needed for completeness of the migrated capacitor page; it supports the voltage derating and safe working-voltage notes above.

16 rows
Approximate dielectric puncture voltage at 1 MHz.
Material
Breakdown(V/mil)
Air240
Alsimag240
Bakelite300
Bakelite, mica-filled325 – 375
Cellulose acetate250 – 600
Formica450
Glass, window200 – 250
Glass, Pyrex335
Mica, ruby3800 – 5600
Plexiglas990
Polyethylene1200
Polystyrene500 – 700
Porcelain40 – 100
Quartz, fused1000
Steatite, low-loss150 – 315
Teflon1000 – 2000

Source: engineeringtoolbox.com

Actual breakdown depends on temperature, frequency, dielectric thickness, and electrode geometry. Consult manufacturer datasheets for rated working voltages.

References