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Rc Time Constant⚠ unverified

Electrical / Basic · Compute the time constant of a resistor-capacitor (RC) circuit

Parameters

InputSymbolUnitDefaultDescription
resistanceresistance1.0Resistance of the circuit
capacitancecapacitanceF1.0Capacitance of the circuit
OutputSymbolUnitDescription
resultτsTime constant, in seconds (s)

The science & history

Understanding the Parameters

Derivation (Approaching a Proof)

Consider a capacitor charging from a source $V$ through a series resistor $R$. Kirchhoff's voltage law gives $V = iR + v_C$, and the capacitor relation is $i = C\,\dfrac{dv_C}{dt}$. Substituting:

$$RC\,\frac{dv_C}{dt} + v_C = V.$$

This first‑order linear ODE has the solution (with $v_C(0)=0$)

$$v_C(t) = V\left(1 - e^{-t/RC}\right),$$

so the natural time scale of the exponential is $\tau = RC$. At $t = \tau$, $v_C = V(1 - e^{-1}) = 0.632\,V$; discharging follows the dual $v_C(t) = V_0\,e^{-t/RC}$.

Units. $\Omega \cdot \text{F} = \dfrac{\text{V}}{\text{A}} \cdot \dfrac{\text{C}}{\text{V}} = \dfrac{\text{C}}{\text{A}} = \text{s}$ — the product is genuinely seconds. (Note: the live calculator currently marks the resistance input "dimensionless"; it should be ohms — flagged for calculator verification.)

History

The exponential charging/discharging of an RC circuit is the archetypal first‑order transient, arising directly from Ohm's and Kirchhoff's laws combined with the capacitor's definition. It became a workhorse of timing, filtering, and pulse circuits through the 20th century (e.g. the ubiquitous 555 timer sets delays from $R$ and $C$).

Related Concepts: Rl Time Constant, Capacitive Reactance, Capacitor Energy, Ohm's Law solve for current

Notes: Registry calculator rc-time-constant (unverified). First‑order, single‑R single‑C model; networks with multiple energy‑storage elements have several time constants.

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