In many electronic circuits, a voltage source does not immediately appear across the load because the capacitor must first charge. The delay is governed by the circuit’s time constant, τ = RC. Despite this lag, an instantaneous voltage can be calculated at any moment using the standard RC charging equation.
For this example, choose R = 40 Ω.
For this example, choose C = 12 µF.
τ = R × C = 40 Ω × 12 µF = 480 µs.
The voltage across the capacitor at time t is:
V(t) = V₀ (1 – e–t/τ)
where V₀ is the supply voltage and t is the elapsed time since the supply was applied.
Assume a supply voltage V₀ = 120 V and we want the voltage after t = 1 µs.
t/τ = 1 µs ÷ 480 µs = 0.002.
e–t/τ = e–0.002 ≈ 0.998.
V(1 µs) = 120 V (1 – 0.998) = 120 V × 0.002 ≈ 0.24 V.
Thus, at one microsecond after the supply is applied, the instantaneous voltage across the capacitor is approximately 0.24 V, despite the 480 µs time constant required for the voltage to reach its steady‑state value.