Capacitor Charge Calculator
Calculates the energy stored in a capacitor using all three equivalent formulas (E=½CV², E=Q²/2C, E=½QV), finds charge and voltage from capacitance, and solves RC circuit charging and discharging problems — using the energy stored in capacitor formula with full step-by-step working throughout.
Select which two values you know:
Capacitance
C
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Voltage
V
—
Charge
Q
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Energy Stored
E
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Find Time for Target Voltage (optional)
| Time | Discharge V(t) | Charge V(t) | % (Dis) | Status |
|---|
Parallel Plate Capacitor Formula
C = ε₀ × εᵣ × A / d
ε₀ = 8.854×10⁻¹² F/m | εᵣ = dielectric constant
| Formula | When to Use | Derivation |
|---|---|---|
| E = ½CV² | C and V known — most common form | E = ∫₀Q (Q'/C)dQ' = Q²/2C = ½CV² |
| E = Q²/(2C) | Q and C known | Direct integration of work done |
| E = ½QV | Q and V known | Substitute Q=CV into ½CV² |
| Time | Discharge V/V₀ | Charge V/V_s | % Discharged | Note |
|---|---|---|---|---|
| t = 0 | 100% | 0% | 0% | Initial state |
| t = τ | 36.79% | 63.21% | 63.21% | 1/e = 0.3679 |
| t = 2τ | 13.53% | 86.47% | 86.47% | e⁻² |
| t = 3τ | 4.98% | 95.02% | 95.02% | e⁻³ |
| t = 4τ | 1.83% | 98.17% | 98.17% | e⁻⁴ |
| t = 5τ | 0.67% | 99.33% | 99.33% | Practical full discharge |
| Material | εᵣ | Notes |
|---|---|---|
| Vacuum / Air | 1.000 | Reference value |
| Teflon (PTFE) | 2.1 | Low-loss RF capacitors |
| Polyethylene | 2.25 | Cable insulation |
| Paper | 3.5 | Old capacitors |
| Mica | 6.0 | Precision capacitors |
| Glass | 7.0 | — |
| Alumina (Al₂O₃) | 9.8 | Ceramic capacitors |
| Water | 80 | Poor insulator, reference |
| Barium titanate | 1200 | High-C ceramic capacitors |
| Prefix | Symbol | Value (F) | Common Use |
|---|---|---|---|
| Farad | F | 1 | Supercapacitors |
| millifarad | mF | 10⁻³ | Large electrolytic |
| microfarad | μF | 10⁻⁶ | Most common! |
| nanofarad | nF | 10⁻⁹ | Signal circuits |
| picofarad | pF | 10⁻¹² | RF / high frequency |
Energy Stored in a Capacitor — Three Equivalent Formulas
The energy stored in a capacitor can be calculated using any of three mathematically equivalent expressions. Each uses a different pair of the four fundamental quantities (C, V, Q, E). The most important energy stored in capacitor formula is:
All three capacitor energy equations are derived from the fundamental definition: the energy stored in a capacitor equals the work done moving charge against the increasing voltage. As charge accumulates on the plate, the voltage rises linearly (V=Q/C), so:
E = ∫₀Q (Q'/C) dQ' = [Q'²/2C]₀Q = Q²/2C = ½CV² (substituting Q=CV). This derivation is why the capacitor energy stored formula has a ½ — the voltage starts at zero and rises to V, so the average voltage during charging is V/2.
| Formula | Variables | Example (C=100μF, V=12V) |
|---|---|---|
| E = ½CV² | C and V known | ½×10⁻⁴×144 = 7.2×10⁻³ J |
| E = Q²/(2C) | Q and C known | (1.2×10⁻³)²/(2×10⁻⁴) = 7.2×10⁻³ J |
| E = ½QV | Q and V known | ½×1.2×10⁻³×12 = 7.2×10⁻³ J |
The energy of a capacitor formula E=½CV² is the most-used form because capacitance C and supply voltage V are the most commonly specified parameters. The formula for energy stored in a capacitor in all three forms gives exactly 7.2 mJ for a 100μF capacitor charged to 12V. This capacitor stored energy formula applies to all capacitor types — electrolytic, ceramic, film, and supercapacitor.
Capacitor Charge Formula — Q = CV
The fundamental capacitor charge formula Q = CV defines the relationship between charge Q (Coulombs), capacitance C (Farads), and voltage V (Volts). Rearranging gives three forms:
Q = C × V— charge stored (Coulombs)V = Q / C— voltage from charge and capacitanceC = Q / V— capacitance from charge and voltage
The unit definition: 1 Farad = 1 Coulomb/Volt. A 1 Farad capacitor stores 1 Coulomb at 1 Volt. Why are real capacitors in μF, nF, pF? One Farad is an enormous capacitance — a parallel plate capacitor with 1mm air gap would need ~9×10¹² m² of plate area to achieve 1 Farad. In practice, most capacitors range from picofarads (pF = 10⁻¹² F) for RF circuits up to thousands of microfarads for power supplies.
How to Calculate Energy Stored in a Capacitor — Step-by-Step
To calculate energy stored in a capacitor, follow this four-step method:
- Convert capacitance to Farads: 100μF = 100×10⁻⁶ F = 1×10⁻⁴ F (never skip this step!)
- Identify voltage: ensure V is in Volts
- Apply E=½CV²: E = 0.5 × C_in_Farads × V²
- Convert to preferred units: 7.2×10⁻³ J = 7.2 mJ = 7200 μJ = 0.002 Wh
Example 1 — Camera Flash Capacitor: C=100μF, V=300V
- C = 100×10⁻⁶ F = 1×10⁻⁴ F
- E = ½ × 1×10⁻⁴ × (300)² = ½ × 1×10⁻⁴ × 90000
- E = 4.5 J | Q = 1×10⁻⁴ × 300 = 30 mC
Example 2 — Cardiac Defibrillator: C=150μF, V=2000V
- C = 150×10⁻⁶ F
- E = ½ × 150×10⁻⁶ × (2000)² = ½ × 150×10⁻⁶ × 4×10⁶
- E = 300 J — delivered in milliseconds to restart the heart
Example 3 — Supercapacitor: C=1F, V=2.7V
- E = ½ × 1 × (2.7)² = ½ × 7.29
- E = 3.645 J | Q = 1 × 2.7 = 2.7 C
RC Circuit — Charging and Discharging
The time constant τ = RC governs how quickly a capacitor charges or discharges through a resistor. It is the fundamental parameter of any RC circuit — the time for voltage to fall to 36.8% (1/e) during discharge, or rise to 63.2% of supply during charging.
Physical interpretation of τ: it is the time it would take to fully discharge at the initial rate (the tangent at t=0 crosses zero at exactly t=τ). After exactly one time constant, 63.2% of the energy has been delivered to the load. After five time constants (5τ), the capacitor is considered fully charged or discharged for all practical purposes.
RC Discharge Example: C=470μF, R=10kΩ, V₀=9V, find V at t=4.7s
- τ = R × C = 10000 Ω × 470×10⁻⁶ F = 4.7 s
- t/τ = 4.7/4.7 = 1.000 (exactly one time constant)
- V(4.7) = 9 × e^(−1) = 9 × 0.36788 = 3.311 V
- Q(4.7) = C×V = 470×10⁻⁶ × 3.311 = 1.556 mC
- E_remaining = ½×470×10⁻⁶×(3.311)² = 2.575 mJ (86.5% dissipated)
Capacitors in Series and Parallel
Capacitors combine in the opposite way to resistors. Parallel capacitors add their capacitances (like resistors in series add resistances); series capacitors combine using reciprocals (like resistors in parallel).
| Configuration | Formula | Result vs Individual |
|---|---|---|
| Parallel | C_total = C₁ + C₂ + ... + Cₙ | Greater than largest |
| Series | 1/C_total = 1/C₁ + 1/C₂ + ... + 1/Cₙ | Less than smallest |
| Two in series | C_total = C₁C₂/(C₁+C₂) | Less than both |
Physical reason: parallel capacitors effectively add plate area (more charge at same voltage → more capacitance). Series capacitors effectively increase the plate separation (less capacitance). In series, all capacitors carry the same charge Q; voltages add up. In parallel, all have the same voltage V; charges add up.
Series: C₁=10μF, C₂=22μF → C_total=?
- 1/C_total = 1/10 + 1/22 = 0.1 + 0.04545 = 0.14545
- C_total = 1/0.14545 = 6.875 μF (less than 10μF, the smaller)
Parallel: C₁=10μF, C₂=22μF → C_total=?
- C_total = 10 + 22 = 32 μF (greater than 22μF, the larger)
What Is Capacitance? — Physical Definition and Units
A capacitor stores energy stored in a capacitor in the electric field between two conducting plates separated by a dielectric insulator. Capacitance C = Q/V is defined as the charge stored per unit voltage. The energy stored in a capacitor using the parallel plate formula:
Why dielectrics increase capacitance: the dielectric material polarizes in the electric field, partially canceling the field between the plates. This allows more charge to be stored at the same voltage — increasing capacitance by the factor εᵣ. Barium titanate (εᵣ≈1200) allows capacitors thousands of times smaller than air-gap designs.
Where is energy stored in a capacitor? In the electric field between the plates. The energy density is u = ½ε₀εᵣE² J/m³. This is analogous to magnetic energy stored in an inductor's magnetic field.
Capacitor Energy Applications — From Flash to Defibrillator
The energy stored in a capacitor finds application wherever rapid energy delivery is needed — capacitors provide high power density (fast discharge) though lower energy density than batteries.
1. Camera Flash: C=100μF, V=300V
E = ½CV² = ½×100×10⁻⁶×90000 = 4.5 J. τ with R=10Ω: τ = RC = 10×100×10⁻⁶ = 1ms. The flash fires in ~1ms — 4.5 J in 1ms = 4500 W peak power.
2. Cardiac Defibrillator: C=150μF, V=2000V
E = ½×150×10⁻⁶×(2000)² = 300 J. Delivered through the chest in ~10ms. The capacitor must be charged from a battery (takes ~5 seconds) then discharged almost instantaneously.
3. Car Audio Capacitor: C=1F, V=14V
E = ½×1×(14)² = 98 J. Acts as a local energy reservoir for the amplifier during bass peaks, preventing voltage sag.
4. Supercapacitor Bank: C=500F, V=2.7V
E = ½×500×(2.7)² = 1822.5 J = 0.506 Wh. Used for regenerative braking energy recovery in hybrid vehicles.
Common Mistakes in Capacitor Energy Calculations
Mistake 1 — Not converting μF to F (the most common error)
- ❌ Wrong: E = ½ × 100 × 12² = ½ × 100 × 144 = 7200 J
- ✅ Correct: E = ½ × (100×10⁻⁶) × 144 = 7.2×10⁻³ J = 7.2 mJ
- Always convert: 100μF = 100×10⁻⁶ = 0.0001 F before using the energy stored in capacitor formula
Mistake 2 — Forgetting the ½ factor
- ❌ Wrong: E = CV² = 10⁻⁴ × 144 = 0.0144 J (twice the actual value)
- ✅ Correct: E = ½CV² = 0.5 × 10⁻⁴ × 144 = 7.2×10⁻³ J
Mistake 3 — Using E=QV instead of E=½QV
- ❌ Wrong: E = QV = 1.2×10⁻³ × 12 = 14.4×10⁻³ J
- ✅ Correct: E = ½QV = 0.5 × 1.2×10⁻³ × 12 = 7.2×10⁻³ J
Mistake 4 — Thinking τ is the time to fully discharge
- ❌ Wrong: "After τ = 4.7s the capacitor is fully discharged"
- ✅ Correct: After τ, 36.8% voltage REMAINS. After 5τ (23.5s), only 0.67% remains — that's the practical "fully discharged" threshold
Mistake 5 — Series capacitance gives MORE total capacitance
- ❌ Wrong: "Two 10μF in series give 20μF"
- ✅ Correct: Two 10μF in series give C_total = 10×10/(10+10) = 5μF — HALF of either one. Series capacitors give LESS capacitance than the smallest.
Worked Examples — 8 Complete Problems
1. C=100μF, V=12V → find Q, E
- C = 1×10⁻⁴ F
- Q = CV = 1×10⁻⁴ × 12 = 1.2×10⁻³ C = 1.2 mC
- E = ½CV² = ½×1×10⁻⁴×144 = 7.2×10⁻³ J = 7.2 mJ
2. C=470μF, V=400V → find E
- C = 470×10⁻⁶ F
- E = ½ × 470×10⁻⁶ × (400)² = ½ × 470×10⁻⁶ × 160000
- E = 37.6 J (defibrillator scale)
3. E=1J, V=100V → find C
- E = ½CV² → C = 2E/V² = 2×1/(100)² = 2/10000
- C = 2×10⁻⁴ F = 200 μF
4. Q=50μC, C=10μF → find V, E
- V = Q/C = 50×10⁻⁶ / 10×10⁻⁶ = 5 V
- E = ½QV = ½ × 50×10⁻⁶ × 5 = 125×10⁻⁶ J = 125 μJ
5. RC discharge: C=10μF, R=100kΩ, V₀=5V, find V at t=1s
- τ = RC = 100000 × 10×10⁻⁶ = 1.0 s
- V(1) = 5 × e^(−1/1) = 5 × 0.36788 = 1.839 V (36.8% of initial)
6. Series: C₁=10μF, C₂=22μF → C_total
- 1/C_total = 1/10 + 1/22 = 0.1 + 0.04545 = 0.14545
- C_total = 6.875 μF
7. Parallel: C₁=10μF, C₂=22μF → C_total
- C_total = 10 + 22 = 32 μF
8. Find τ for discharge from 9V to 1V: R=47kΩ, C=100μF
- τ = RC = 47000 × 100×10⁻⁶ = 4.7 s
- t = −τ × ln(V_target/V₀) = −4.7 × ln(1/9) = −4.7 × (−2.197)
- t = 10.33 s = 2.20τ
Frequently Asked Questions — Capacitor Energy
Related Calculators
36.8% remains (discharge)
63.2% charged (charge)
5.0% remains
95.0% charged
0.67% remains ← "fully done"
99.33% charged
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Shahid Ali
Shahid Ali is the creator and lead developer of SciSolveLab, a platform dedicated to making complex scientific and mathematical computations accessible. With a deep background in physics, thermodynamics, and wave mechanics, Shahid's work is driven by the belief that robust, accurate mathematical tools should be just a click away for students, engineers, and researchers.