Enter the capacitance and voltage into the calculator to determine the energy stored in a capacitor. This calculator can also solve for capacitance or voltage when the other two values are known.
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Capacitor Energy Formula
The energy stored in a capacitor is calculated using the following primary formula:
E = \frac{1}{2} C V^2Where E is energy in joules (J), C is capacitance in farads (F), and V is voltage in volts (V). This equation can also be expressed in two equivalent forms using the relationship Q = CV, where Q is charge in coulombs:
E = \frac{Q^2}{2C} = \frac{1}{2} Q VAll three forms are mathematically identical. The first (using C and V) is the most practical for circuit design because capacitance and voltage are typically the known quantities. The second form (using Q and C) is useful when charge is measured directly, as in coulomb-counting battery management systems. The third (using Q and V) appears frequently in physics derivations of electrostatic potential energy.
Why the 1/2 Factor Exists
The factor of 1/2 in the capacitor energy formula is not arbitrary. It arises from the physics of how charge accumulates on a capacitor. As charge builds on the plates, the voltage across the capacitor increases linearly from 0 to its final value V. The energy delivered at any instant is the product of the current voltage and the incremental charge added. Integrating this from zero to full charge gives E = (1/2)CV^2, not CV^2. In other words, the average voltage during charging is V/2, so the total energy is half of what it would be if the full voltage were present from the start.
Energy Density and the Electric Field
The energy stored in a capacitor physically resides in the electric field between its plates. The volumetric energy density of that field is u = (1/2) * permittivity * E_field^2, where u is energy per unit volume (J/m^3), E_field is the electric field strength (V/m), and permittivity is the product of vacuum permittivity (8.854 x 10^-12 F/m) and the dielectric constant. A higher dielectric constant means more energy stored in the same physical space. For a parallel-plate capacitor with plate area A and separation d, the total stored energy equals u multiplied by the volume A*d, which reduces back to (1/2)CV^2.
Capacitance and Voltage to Joules Reference Table
| Capacitance | Voltage (V) | Energy (J) |
|---|---|---|
| 10 uF | 24 | 0.003 |
| 22 uF | 24 | 0.006 |
| 47 uF | 12 | 0.003 |
| 100 uF | 12 | 0.007 |
| 220 uF | 12 | 0.016 |
| 470 uF | 12 | 0.034 |
| 1000 uF | 12 | 0.072 |
| 2200 uF | 12 | 0.158 |
| 4700 uF | 12 | 0.338 |
| 10 mF | 12 | 0.720 |
| 0.1 F | 5 | 1.250 |
| 0.5 F | 5 | 6.250 |
| 1 F | 2.7 | 3.645 |
| 1 F | 5 | 12.500 |
| 2.7 F | 2.7 | 9.842 |
| 5 F | 2.7 | 18.225 |
| 10 F | 2.7 | 36.450 |
| 10 F | 5 | 125.000 |
| 50 F | 2.7 | 182.250 |
| 100 F | 2.7 | 364.500 |
| * Rounded to 3 decimals. Energy computed using E = 0.5 * C * V^2. | ||
Real-World Capacitor Energy by Application
The energy stored in a capacitor varies enormously depending on the application. The table below shows representative values for real devices, calculated using E = (1/2)CV^2, to illustrate the practical range of capacitor energy storage.
| Application | Typical C | Typical V | Stored Energy |
|---|---|---|---|
| DRAM refresh (per cell) | 30 fF | 1 V | 15 pJ |
| MLCC bypass (digital IC) | 100 nF | 3.3 V | 0.54 uJ |
| Camera flash (disposable) | 120 uF | 330 V | 6.5 J |
| Camera flash (professional) | 1000 uF | 400 V | 80 J |
| External defibrillator | 100 uF | 5000 V | 1,250 J |
| Implantable defibrillator (ICD) | 120 uF | 750 V | 33.75 J |
| Supercapacitor (bus regen braking) | 63 F | 125 V | 492 kJ |
| UPS ride-through module | 5.5 F | 48 V | 6.3 kJ |
| Railgun pulse capacitor bank | 0.26 F | 22,000 V | 63 MJ |
| * Values are representative of commercially available devices. Actual specifications vary by manufacturer and model. | |||
Capacitors vs. Batteries: Energy Storage Comparison
Farads and joules relate to each other through the energy formula, but the resulting energy values are small compared to batteries at equivalent weight and volume. This difference reflects a fundamental tradeoff between energy density and power density.
Standard aluminum electrolytic capacitors store roughly 0.01 to 0.3 Wh/kg. Commercial supercapacitors (also called ultracapacitors or EDLCs) reach 0.5 to 15 Wh/kg. By contrast, lithium-ion batteries store 100 to 265 Wh/kg, roughly 10 to 500 times more energy per kilogram. However, supercapacitors deliver power at rates 10 to 100 times higher than batteries, fully charging in seconds rather than hours. This makes them suited for applications requiring short, intense energy bursts (regenerative braking, grid frequency regulation, backup power bridging) while batteries handle sustained energy delivery over longer periods.
Dielectric Materials and Stored Energy
The dielectric material between a capacitor’s plates directly affects how many joules it can store. Inserting a dielectric with relative permittivity (dielectric constant) of value k multiplies the capacitance by k while maintaining the same plate geometry. Since E = (1/2)CV^2, a higher dielectric constant at the same voltage means proportionally more stored energy.
Air has a dielectric constant of approximately 1.0006. Common capacitor dielectrics include polyester film (k = 3.2 to 3.3), ceramic Class II X7R (k = 2,000 to 4,000), and barium titanate-based ceramics (k up to 15,000). However, higher-k materials typically have lower breakdown voltages per unit thickness, which limits the maximum voltage and therefore the V^2 term in the energy formula. Capacitor designers balance dielectric constant against breakdown field strength, temperature stability, and loss tangent to maximize energy storage for each application.
Practical Considerations for Capacitor Energy
The formula E = (1/2)CV^2 gives the ideal stored energy under perfect conditions. Several real-world factors reduce the usable energy available from a charged capacitor.
Equivalent series resistance (ESR) converts a portion of stored energy into heat during discharge, reducing efficiency. Electrolytic capacitors have ESR values ranging from tens of milliohms to several ohms, while ceramic MLCCs typically have ESR below 10 milliohms. Leakage current causes a charged capacitor to slowly self-discharge over time; electrolytic capacitors lose a measurable fraction of their charge within hours, while film capacitors can hold charge for weeks. Voltage derating is another factor: manufacturers recommend operating capacitors at 50% to 80% of their rated voltage for reliability, which reduces the effective stored energy to 25% to 64% of the theoretical maximum at rated voltage. Temperature also plays a role, particularly for ceramic capacitors whose capacitance can drop by 30% to 80% from the nominal value at temperature extremes, directly reducing stored energy.
Farads to Joules FAQ
Can you convert farads directly to joules?
No. Farads measure capacitance (charge stored per volt) and joules measure energy. They are different physical quantities. To convert between them, you need a third variable: voltage. The relationship is E = (1/2)CV^2. Without knowing the voltage, a capacitance value in farads cannot be expressed in joules.
How much energy does a 1 farad capacitor store?
It depends entirely on the voltage. A 1 F capacitor charged to 2.7 V (a common supercapacitor rating) stores 3.645 J. The same capacitor charged to 5 V would store 12.5 J. At 12 V, it stores 72 J.
Why does doubling the voltage quadruple the energy?
Energy depends on V squared. Doubling voltage from V to 2V means the energy becomes (1/2)C(2V)^2 = (1/2)C*4V^2 = 4 times the original energy. This is why high-voltage capacitors store disproportionately more energy than low-voltage ones of the same capacitance, and why voltage rating is often the more important specification for energy storage applications.
What happens to the energy when a capacitor discharges?
The stored electrostatic energy converts to other forms depending on the discharge circuit. In a resistive load, it becomes heat. In an LC oscillator, it cycles between electric field energy (in the capacitor) and magnetic field energy (in the inductor). In a camera flash, it becomes light and heat. In a defibrillator, it becomes the electrical pulse delivered to the patient’s heart. Some energy is always lost to ESR heating and conductor resistance during discharge.
