RC Time Constant\ and Discharging Simulation
Updated 2026-10-04 · NEXMASON ANITEX▶ Open interactive ANITEX · equations and animations
This accessible text edition preserves the document's narrative. See the interactive edition for typeset equations, diagrams and playback.
Objective
This document explains the transient response of a resistor-capacitor circuit. The central quantity is the RC time constant =RC. The animation shows capacitor voltage, circuit current, current direction, charging, discharging, and the corresponding waveforms on a common timeline.
Circuit Parameters
For the demonstration, V_S=5V, R=1k, C=100 F. Therefore =RC=(1000)(10010^-6) =0.1s.
The initial charging current is I_0=V_SR =5mA.
Charging
For an initially uncharged capacitor, V_C(t)=V_S(1-e^-t/) and i(t)=V_SRe^-t/.
At one time constant, V_C()=V_S(1-e^-1) 0.632V_S, and i()=I_0e^-1 0.368I_0.
Thus at t=, the capacitor has reached approximately 63.2\% of its final voltage.
Discharging
For a capacitor initially charged to V_0, V_C(t)=V_0e^-t/.
Using the charging-current direction as the positive reference, i(t)=-V_0Re^-t/.
The negative sign indicates that the discharge current flows in the opposite direction.
Animation
The following block is interpreted by the NEXMASON Science Viewer.
Interpretation
At the beginning of charging the capacitor behaves approximately like a short circuit, so the current is maximum. As charge accumulates, the capacitor voltage rises and the voltage across the resistor decreases. Therefore the current decreases exponentially.
The RC time constant controls the speed of this process: =RC.
A larger R or a larger C produces a slower transient response.