The fundamental voltage across a capacitor formula depends on whether you are analyzing a static charge or a dynamic charging circuit. For a static electrostatic charge, the formula is V = Q / C. For a capacitor charging through a resistor in a DC circuit (transient response), the formula is V(t) = Vs × (1 - e-t / (R × C)). These two equations govern everything from timing delays in 555 timer circuits to bulk hold-up capacitance in power supplies.
Below, we break down every symbol, track units through real-world solved problems, and provide a concrete decision path to select the exact physical component for your next build.
The Core Formulas and Symbol Definitions
To use these formulas reliably on the bench, you must distinguish between the electrostatic state (how much voltage is currently stored) and the transient state (how the voltage changes over time). Both are critical for circuit design.
| Symbol | Parameter | Standard SI Unit | Common Sub-units |
|---|---|---|---|
| V or V(t) | Voltage across the capacitor at time t | Volts (V) | mV, kV |
| Q | Electric charge stored on the plates | Coulombs (C) | mC, μC |
| C | Capacitance | Farads (F) | μF, nF, pF |
| Vs | Source (supply) voltage | Volts (V) | - |
| R | Series resistance | Ohms (Ω) | kΩ, MΩ |
| t | Time elapsed since charging began | Seconds (s) | ms, μs |
| e | Euler's number (mathematical constant) | ~2.71828 | - |
The transient formula relies on the time constant, τ (tau) = R × C. At t = 1τ, the capacitor reaches 63.2% of the source voltage. At t = 5τ, it is considered fully charged (99.3% of Vs), a standard rule of thumb in analog design.
Rearranged Forms and Critical Unit Traps
On the bench, you rarely solve for V directly. You are usually sizing a component or calculating a timing delay. Here are the algebraically rearranged forms for both equations:
Static Equation (V = Q / C) Rearrangements
- Solving for Charge: Q = V × C
- Solving for Capacitance: C = Q / V
Transient Equation (V(t) = Vs × (1 - e-t/RC)) Rearrangements
- Solving for Time (t): t = -R × C × ln(1 - (V(t) / Vs))
- Solving for Resistance (R): R = -t / (C × ln(1 - (V(t) / Vs)))
- Solving for Capacitance (C): C = -t / (R × ln(1 - (V(t) / Vs)))
The Fix: Always convert to base units first.
• 100 μF = 100 × 10-6 F = 0.0001 F
• 4.7 kΩ = 4700 Ω
• 20 ms = 0.020 s
If you plug '100' into the C variable instead of '0.0001', your calculated time constant will be off by a factor of one million.
Worked Examples with Strict Unit Tracking
Let us walk through two practical scenarios, tracking every unit to ensure the math holds up to physical reality.
Problem 1: Static Charge in a Camera Flash Circuit
Scenario: A camera flash circuit uses a 470 μF electrolytic capacitor. The charging circuit pumps 0.00564 Coulombs of charge into the capacitor before the flash triggers. What is the voltage across the capacitor at the moment of triggering?
Step 1: Identify knowns and convert to SI base units.
- Q = 0.00564 C (already in base units)
- C = 470 μF = 470 × 10-6 F = 0.00047 F
Step 2: Apply the static formula.
- V = Q / C
- V = 0.00564 [C] / 0.00047 [F]
Step 3: Calculate and verify magnitude.
- V = 12 Volts
Sanity Check: A 12V result is highly realistic for a standard 12V-rated or 16V-rated camera flash capacitor. If we had forgotten to convert μF to F, we would have calculated 0.000012V, which is physically impossible for a flash circuit.
Problem 2: RC Transient Timing for a Microcontroller Reset
Scenario: You are designing a delayed-enable circuit for an ESP32. You use a 10 kΩ resistor and a 100 μF capacitor in series connected to a 5V USB supply. What is the voltage across the capacitor exactly 0.5 seconds after power is applied?
Step 1: Identify knowns and convert to SI base units.
- Vs = 5 V
- R = 10 kΩ = 10,000 Ω
- C = 100 μF = 0.0001 F
- t = 0.5 s
Step 2: Calculate the time constant (τ).
- τ = R × C
- τ = 10,000 [Ω] × 0.0001 [F] = 1.0 [s]
Step 3: Apply the transient formula.
- V(t) = Vs × (1 - e-t / τ)
- V(0.5) = 5 × (1 - e-0.5 / 1.0)
- V(0.5) = 5 × (1 - e-0.5)
Step 4: Calculate the exponential term and final voltage.
- e-0.5 ≈ 0.60653
- V(0.5) = 5 × (1 - 0.60653)
- V(0.5) = 5 × 0.39347
- V(0.5) = 1.967 Volts
Sanity Check: At 0.5 seconds, we are at exactly 0.5τ. The voltage should be roughly 39.3% of the source voltage. 39.3% of 5V is 1.965V. Our calculated 1.967V matches perfectly.
Decision Path: Sizing a Capacitor for Voltage Hold-Up
When designing power supply hold-up circuits (keeping a microcontroller alive during a brief brownout), the standard RC charging formula is less useful than the constant-current discharge approximation: C = (I × Δt) / ΔV. Use this decision tree to select your physical component.
| Design Condition | Action / Calculation | Resulting Specification |
|---|---|---|
| 1. Define Load Current (I) | Measure or calculate max steady-state draw of the 3.3V rail. | I = 150 mA (0.15 A) |
| 2. Define Hold-up Time (Δt) | Determine how long the MCU needs to execute a safe shutdown sequence. | Δt = 20 ms (0.02 s) |
| 3. Define Allowable Droop (ΔV) | Subtract the MCU's minimum brownout voltage from the nominal rail voltage. | ΔV = 3.3V - 2.8V = 0.5 V |
| 4. Calculate Base Capacitance | C = (0.15 A × 0.02 s) / 0.5 V = 0.003 / 0.5 | C = 0.006 F (6000 μF) |
| 5. Apply Derating Margin | Add 20% margin for capacitor aging and ESR voltage drop. | Target ≥ 7200 μF |
| 6. Concrete Component Pick | Select a low-ESR radial electrolytic rated above the max rail voltage (e.g., 16V or 25V for a 5V input). | Panasonic EEU-FR1V682 (6800 μF, 35V, Low ESR FR Series) |
Assumptions, Parasitics, and Realistic Magnitudes
The formulas V = Q/C and V(t) = Vs(1 - e-t/RC) assume an ideal capacitor. In physical reality, every component has parasitics that alter the voltage profile, especially at high frequencies or high currents.
When the Ideal Formula Applies
The ideal formulas are highly accurate for:
- DC and low-frequency analog circuits (below 10 kHz).
- Timing circuits where the charge/discharge current is relatively low (< 100 mA).
- Initial theoretical sizing before prototyping.
When Parasitics Break the Math
You must account for Equivalent Series Resistance (ESR) and Equivalent Series Inductance (ESL) when:
- High Ripple Current: In switching power supplies, the ESR creates an instantaneous voltage drop (V = I × ESR) that adds to the capacitive voltage. If your math says the ripple should be 50mV, but the capacitor has a 0.5Ω ESR and sees 1A of ripple, your actual voltage ripple will be 550mV.
- Fast Transients: In high-speed digital decoupling (e.g., bypassing an FPGA), ESL dominates. The voltage across the capacitor cannot change instantly because the inductance resists rapid current changes (V = L × di/dt). This is why we place 0.1 μF (low ESL) ceramic capacitors physically adjacent to IC power pins, alongside bulk electrolytics.
Realistic Answer Magnitudes
If your calculation yields a physically impossible magnitude, you have a unit error or a flawed assumption. Use this reference to ground your expectations:
- Standard Ceramic (MLCC): 1 pF to 100 μF. Voltages: 6.3V to 1000V. (If you calculate needing 1 Farad of ceramic capacitance, you must switch to an electrolytic or supercapacitor topology).
- Aluminum Electrolytic: 1 μF to 10,000+ μF. Voltages: 6.3V to 450V.
- Supercapacitors (EDLC): 0.1 F to 3000 F. Voltages: strictly limited to 2.5V - 2.7V per cell. (If your formula demands 5V across a single supercap, it will violently vent or explode; you must use a series string with a balancing BMS).
By strictly tracking your units, applying the correct transient or static formula, and derating for real-world ESR, you can transition from theoretical math to reliable, physical circuit design. For further reading on capacitor dielectrics and transient response modeling, refer to the All About Circuits DC textbook chapter on capacitors and the Electronics Tutorials DC capacitor guide.






