INGENIA

ELC-08

Capacitor stored energy

U = ½ C V² = ½ Q V.

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Energy storageMaxwell

Governing equation

U=12CV2=12QVU=\tfrac12 C V^2=\tfrac12 Q V

V∈[0.1,1000]V \in \left[0.1, 1000\right]

where

C
Capacitance (µF)
V
Voltage (V)
U
Energy (J)
Q
Charge (mC)

The figure, part by part

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ELC-08 · circuit
00:0 / 00:08
①

Governing law — red

U=12CV2=12QVU=\tfrac12 C V^2=\tfrac12 Q V

V∈[0.1,1000]V \in \left[0.1, 1000\right]

V=0.1V = 0.1U=5×10−7U = 5\times 10^{-7}

②

Domain of the variable — blue

Vmin⁡=0.1,Vmax⁡=1000V_{\min} = 0.1,\quad V_{\max} = 1000

V∈[0.1,1000]V \in \left[0.1, 1000\right]

V=0.1V = 0.1V=0.1V = 0.1

③

Response curve — green

U=12CV2=12QVU=\tfrac12 C V^2=\tfrac12 Q V

V∈[0.1,1000]V \in \left[0.1, 1000\right]

V=0.1V = 0.1U=5×10−7U = 5\times 10^{-7}

④

Rate of change — amber

dUdV\frac{\mathrm{d}U}{\mathrm{d}V}

V∈[0.1,1000]V \in \left[0.1, 1000\right]

V=6.389V = 6.389U′=6.39×10−4U^{\prime} = 6.39\times 10^{-4}

Lecture brief

Historical brief

Ohm (1827), Kirchhoff (1845) and Maxwell’s circuit reduction still run every board: RLC transients, transformers, skin effect and three-phase power. The sheets are those network laws, not a SPICE deck. This sheet (ELC-08 — Capacitor stored energy) is the form associated with Maxwell. Working symbols: CC, VV →\rightarrow UU, QQ. The work to assemble charge on a capacitor is the integral V dq = C V dV, hence ½ C V².

Purpose

Purpose: compute UU, QQ from CC, VV in Electrical via U=12CV2=12QVU=\tfrac12 C V^2=\tfrac12 Q V U = ½ C V² = ½ Q V. Use it when a real electrical question must be answered in SI before a code check.

Live realistic example

In symbols

Live case. Given C=100.000 μFC = 100.000\,\mathrm{\mu F}, V=24.000 VV = 24.000\,\mathrm{V}, the governing relation U=12CV2=12QVU=\tfrac12 C V^2=\tfrac12 Q V yields U=0.0288 JU = 0.0288\,\mathrm{J}, Q=2.4000 mCQ = 2.4000\,\mathrm{mC}. Linear capacitor, quasistatic. Move a slider: the numbers are this situation, not a canned story.

Calculator

Inputs

Outputs

  • Energy U0.0288 J
  • Charge Q2.4000 mC
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ELC-08 · circuit
00:0 / 00:08

Narration of this film

Linear capacitor, quasistatic.

The work to assemble charge on a capacitor is the integral V dq = C V dV, hence ½ C V².

Reading speed

Watch on YouTube