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Analyzing Complex RC Circuits Using Thevenin’s Theorem

Analyzing Complex RC Circuits Using Thevenin’s Theorem

When a circuit features resistors in both series and parallel arrangements around a reactive component, the standard time‑constant formulas (τ=RC for RC, τ=L/R for RL) no longer apply directly. The solution lies in reducing the network to a simple equivalent that preserves the voltage across the reactive element.

Consider the following example:

Analyzing Complex RC Circuits Using Thevenin’s Theorem

Step 1 – Identify the Load

In this network the capacitor (C1 = 100 µF) is the load. We temporarily remove it to determine the Thevenin equivalent seen from its terminals.

Step 2 – Compute the Thevenin Voltage (Vth)

With the switch closed and no load present, the voltage at the capacitor terminals (node 2–node 3) equals the voltage across resistor R2. Calculations give:

Vth = 1.8182 V

Because a fully charged capacitor behaves as an open circuit (zero current), this is also the final steady‑state voltage the capacitor will reach.

Step 3 – Compute the Thevenin Resistance (Rth)

All independent sources are turned off (voltage sources shorted, current sources opened). The resulting resistance seen from the capacitor terminals is:

Rth = 454.545 Ω

Step 4 – Calculate the Time Constant

With C1 = 100 µF, the circuit’s time constant is:

τ = Rth · C1 = 454.545 Ω × 100 µF = 0.0454545 s (45.45 ms)

Step 5 – Determine the Transient Response

Assuming the capacitor starts uncharged (V0=0 V), the voltage at any time t is:

V(t) = Vth · (1 – e–t/τ)

At t = 60 ms:

V(60 ms) = 1.8182 V × (1 – e–0.06/0.0454545) ≈ 1.3325 V

Verification with SPICE Simulation

The following netlist was used to confirm the analytical result. The transient analysis samples every 5 ms over 370 ms.

* Original circuit
v1 1 0 dc 20
r1 1 2 2k
r2 2 3 500
r3 3 0 3k
c1 2 3 100u ic=0

* Thevenin equivalent
v2 4 0 dc 1.818182
r4 4 5 454.545
c2 5 0 100u ic=0

.tran 0.005 0.37 uic
.print tran v(2,3) v(5,0)
.end

The output shows identical capacitor voltages in both networks at every sampled instant, confirming the equivalence of the Thevenin reduction.

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