Formula & Calculator

RC Time Constant

When you charge a capacitor through a resistor, it does not fill up instantly. The time constant, tau = R x C, tells you the speed of that process. After one time constant the capacitor has reached about 63.2% of the supply voltage. After about five time constants it is over 99% full and we treat it as fully charged. A bigger resistor or a bigger capacitor means slower charging.

Circuit Analysis Transient Response
VORZEP · ELECTRONICS & CIRCUIT TOOLS

RC Time Constant Calculator

Solve τ = R · C in any direction — time constant from resistance and capacitance, or work backwards to find R or C. Includes a circuit diagram, live charge/discharge curves, step-by-step math, tolerance sensitivity, and companion metrics like cutoff frequency and rise time.

τ = R · C | VC(t) = V₀ · (1 − e−t/τ)
Solve for
Resistance (R) The series resistor's resistance, in ohms (Ω). Larger R charges the capacitor more slowly.
Resistance must be greater than zero.
Capacitance (C) The capacitor's capacitance, in farads (F). Larger C stores more charge and slows the charge/discharge cycle.
Capacitance must be greater than zero.
Time constant (τ) The time for the capacitor to reach ≈63.2% of the supply voltage while charging (or fall to 36.8% while discharging).
Time constant must be greater than zero.
Source voltage (V₀) Used only for the companion energy, charge and peak-current metrics in Advanced mode. It does not affect τ.
V
TIME CONSTANT (τ)
1 s
1 × 10⁰ s
τ = R · C
Step-by-step solution
Charge & discharge curves
Charging — V₀(1 − e−t/τ) Discharging — V₀·e−t/τ 63.2% at t = τ
Tolerance sensitivity
Companion RC Metrics
RC circuit diagram — where τ comes from
+ − V₀ switch R C VC i

Closing the switch connects V₀ across the series combination of R and C. The capacitor voltage VC climbs exponentially toward V₀, and the time it takes to cover 63.2% of that gap is exactly τ = R · C — independent of the supply voltage.

How R and C drive the time constant
τtime constant (s)
=
Rohms
×
Cfarads

R ↑ — slower charge

τ scales linearly with resistance. Doubling R doubles τ, so the capacitor takes twice as long to reach any given fraction of V₀. Current is limited more, so charge accumulates more slowly.

C ↑ — slower charge

τ also scales linearly with capacitance. A bigger capacitor holds more charge at the same voltage, so it takes proportionally longer to fill through the same resistor.

Independent of V₀

τ never depends on the supply voltage. Raising V₀ makes the capacitor charge to a higher final voltage, but the shape of the curve — and the time to reach 63.2% — stays identical.

Time-domain vs. frequency-domain

τ is the time-domain face of the same circuit whose frequency-domain face is the cutoff fc = 1/(2πRC). A large τ means a low cutoff frequency, and vice versa.

How to Use This Calculator

The RC relation links three quantities: resistance R, capacitance C, and the time constant τ = R · C. Pick which one you want the tool to solve, then fill in the other two.

1. Choose what to solve for

Pick τ (time constant from R and C), R (resistance from τ and C), or C (capacitance from τ and R) — the tool rearranges the formula automatically.

2. Pick a preset, or type your own values

Use the quick pills (100 Ω → 1 MΩ, 1 pF → 100 µF, 1 ns → 10 s) or type any custom value and choose its unit from the dropdown.

3. Read the result and steps

The result card shows the solved value with an auto-selected unit plus engineering (×10ⁿ) notation. The step-by-step panel shows exactly how the number was reached.

4. Study the charge/discharge chart

The plot shows both exponential curves normalised to V₀, with the 63.2% point at t = τ marked, so you can see the 1τ–5τ settling behaviour at a glance.

5. Switch to Advanced for more depth

Advanced mode adds a tolerance sensitivity panel, plus cutoff frequency, half-life, 10–90% rise time, energy stored and peak current companion metrics.

6. Convert τ to frequency, or copy the result

Use the τ → cutoff frequency converter further down the page to see the frequency-domain equivalent, or "Copy result" to grab the solved value.

What This Tool Offers

Built around the fundamental RC relation τ = R · C, the first-order circuit result behind every filter, debounce circuit, and timing delay in electronics.

Solve all three directions

Go from R and C to τ, from τ and C to R, or from τ and R to C — the formula is rearranged for you.

Full SI unit handling

Enter resistance in Ω / kΩ / MΩ / GΩ, capacitance in pF → F, and time in ns → hours. The solver auto-picks the cleanest display unit.

Live exponential chart

See the capacitor charging and discharging curves plotted side by side, with the 63.2% / 1τ point marked and 1τ–5τ gridlines.

Annotated circuit diagram

A labelled series RC schematic showing the source, switch, resistor, capacitor, current direction and capacitor voltage.

Tolerance sensitivity

See exactly how a ±1% shift in R and C compounds into the time constant — practical worst-case analysis for real components.

Companion RC metrics

Advanced mode reports cutoff frequency, angular cutoff, half-life, 10–90% rise time, 5τ settling, stored energy and peak current.

Reference Tables & Conversions

A τ → cutoff-frequency converter, plus lookup tables for charge levels, common RC combinations, and time constants in other circuit types.

τ → cutoff frequency & settling estimator

—

Capacitor Charge & Discharge vs. Time

How far along the exponential curve the capacitor is at each multiple of τ. After 5τ the transient is conventionally considered finished.

TimeCharged (% of V₀)Discharged (remaining %)Typical use
0.5τ39.3%60.7%—
1τ63.2%36.8%Definition of τ
2τ86.5%13.5%—
3τ95.0%5.0%Common "settled" rule of thumb
4τ98.2%1.8%—
5τ99.3%0.7%Full settle for most designs

Common RC Combinations

Typical resistor/capacitor pairings and the time constant and cutoff frequency they produce.

RCτCutoff fc5τ settle
1 kΩ1 nF1 µs159.2 kHz5 µs
1 kΩ100 nF100 µs1.59 kHz500 µs
10 kΩ10 nF100 µs1.59 kHz500 µs
4.7 kΩ10 µF47 ms3.39 Hz235 ms
100 kΩ1 µF100 ms1.59 Hz500 ms
10 kΩ100 µF1 s159.2 mHz5 s
1 MΩ1 µF1 s159.2 mHz5 s

Time Constants Across Circuit Types

CircuitTime constantNotes
RC seriesτ = R · CFirst-order; exponential charge/discharge
RL seriesτ = L / RFirst-order; current rises exponentially
RLC series (underdamped)τ = 2L / REnvelope decay; resonant ω₀ = 1/√(LC)

What Does τ = R · C Measure?

The RC time constant τ is the characteristic time of a resistor–capacitor circuit. It answers a simple question: how long does the capacitor take to get most of the way to its final voltage? The answer is τ — the time to cover 63.2% of the remaining gap. It is the single number that describes the speed of any first-order RC network, from a simple debounce filter to an audio tone control.

The RC Time Constant Formula

The defining relationship is:

τ = R · C

Rearranged for the other two unknowns:

R = τ / C   ·   C = τ / R

The voltage across the capacitor while charging from 0 toward V₀ follows:

VC(t) = V₀ · ( 1 − e−t/τ )

and while discharging from V₀ toward 0:

VC(t) = V₀ · e−t/τ

RC Time Constant Variables

SymbolMeaningUnit
τTime constant — time to reach 63.2% (charging)seconds (s)
RSeries resistanceohms (Ω)
CCapacitancefarads (F)
V₀Supply / initial voltagevolts (V)
fcCutoff frequency, 1/(2πRC)hertz (Hz)

How R and C Affect the Time Constant

Because τ is the product R · C, it grows linearly with either component. Doubling the resistor doubles τ; doubling the capacitor doubles τ; doubling both quadruples it. Notice what is missing from the formula: the supply voltage. τ is a property of the R and C alone, which is why the same circuit responds at the same speed whether it runs on 3.3 V or 24 V.

In the frequency domain, the very same circuit is a low-pass filter with cutoff fc = 1/(2πRC). A long time constant means a low cutoff frequency, and a short time constant means a high one — two views of the identical physical behaviour.

RC Time Constant Calculation Examples

Given: R = 10 kΩ, C = 100 µF — solve for τ
R = 10,000 Ω  ·  C = 1 × 10⁻⁴ F
τ = 10,000 × 1 × 10⁻⁴
τ = 1 s
Given: τ = 100 µs, C = 10 nF — solve for R
C = 1 × 10⁻⁸ F
R = 1 × 10⁻⁴ / 1 × 10⁻⁸
R = 10,000 Ω = 10 kΩ
Given: τ = 47 ms, R = 4.7 kΩ — solve for C
R = 4,700 Ω  ·  τ = 0.047 s
C = 0.047 / 4,700
C = 1 × 10⁻⁵ F = 10 µF

Frequently Asked Questions

It is the time required for the capacitor voltage to change by 63.2% of the total change it is heading toward. While charging, that means reaching 63.2% of V₀; while discharging, that means falling to 36.8% of the starting voltage. It is the natural timescale of the circuit.

Because the response is exponential, not linear. Substituting t = τ into V₀(1 − e−t/τ) gives V₀(1 − e⁻¹) = V₀(1 − 0.3679) = 0.6321 · V₀. The number falls out of the mathematics of the exponential, not from an arbitrary choice. If you want 50%, that happens at t = τ · ln 2 ≈ 0.693τ.

Technically never — an exponential only approaches its final value asymptotically. In practice, 5τ brings the capacitor to 99.3% of V₀, which is close enough that engineers treat the transient as finished. That is why "5τ" appears as the settling time throughout this tool.

No. τ = R · C contains no voltage term at all. Raising V₀ raises the final voltage the capacitor charges to, but the percentage-versus-time curve — and therefore the time to reach 63.2% — is completely unchanged. This is a distinctive property of linear RC circuits.

By fc = 1 / (2πτ), which is the same as fc = 1/(2πRC). The time constant and the −3 dB cutoff frequency carry identical information about the circuit, just expressed in the time domain versus the frequency domain. Use the converter above to move between them.

Very many. Switch debounce circuits, RC low-pass and high-pass filters, 555 timer timing networks, power-on reset delays, audio tone controls, integrators and differentiators, camera flash charging, and sample-and-hold circuits all have τ = RC at their core.

Because τ is a product, relative errors add. A +1% resistor combined with a +1% capacitor gives ≈ +2.01% in τ; −1% in both gives ≈ −1.99%. Electrolytic capacitors in particular are often specified at ±20%, which dominates the total error budget — see the tolerance sensitivity panel in Advanced mode.

Variables

Symbol Quantity Unit
τ Time constant s
R Resistance Ω
C Capacitance F

What it means

The time constant τ (tau) of an RC circuit is the product of resistance R and capacitance C: τ = R*C, measured in seconds. It is the time required for the capacitor voltage to reach approximately 63.2% of its final value during charging (or to fall to 36.8% during discharging) when subjected to a step input. After 5 time constants (5τ), the transient is considered essentially complete (over 99%). This parameter is fundamental for understanding the speed of response of RC circuits, which are used in filters, timing circuits, and signal shaping. The time constant determines the cut‑off frequency of a low‑pass filter (f_c = 1/(2πτ)). In digital circuits, the RC time constant affects the rise and fall times of signals and the propagation delay. Example: With R=1kΩ and C=100µF, τ = 1000 * 100e-6 = 0.1 seconds. The capacitor charges to 6.32V (assuming 10V supply) in 0.1s and reaches 9.9V in 0.5s (5τ).

Worked example

RC Time Constant – Practical Example

Real‑World
Scenario: You have a 1 kΩ resistor and a 100 µF capacitor. Calculate the time constant τ = RC, which determines how fast the capacitor charges.
ParameterValue
R1 kΩ = 1000 Ω
C100 µF = 100×10⁻⁶ F
Formulaτ = R · C
1Substitute:τ = 1000 Ω × 100×10⁻⁶ F
2Calculate:τ = 0.1 s = 100 ms
Final Design τ = 100 ms ✓ 5τ = 500 ms to fully charge
Why: After one time constant, the capacitor reaches 63.2% of the final voltage – useful for timing circuits.

Common mistakes

Applications

The RC time constant τ = R·C is the time required for a capacitor to charge to approximately 63.2% of the final voltage (or discharge to 36.8%) when a step voltage is applied. This parameter is fundamental to timing circuits, filters, and transient analysis. Engineers use it to design timing delays, to set the cutoff frequency of RC filters, and to control the rise and fall times of signals. In power supplies, it determines the ripple voltage. In digital circuits, it affects the propagation delay of CMOS gates. By understanding the RC time constant, professionals can design circuits with predictable timing and frequency response. This formula is a cornerstone of analog and mixed‑signal design.

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  • Published July 10, 2026
  • Last updated July 30, 2026