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Parallel Resistor–Capacitor AC Circuits: Analysis, Impedance, and Ohm’s Law

Building on the series example, we now connect the same resistor and capacitor in parallel to observe how AC behavior changes.

Parallel Resistor–Capacitor AC Circuits: Analysis, Impedance, and Ohm’s Law

Parallel R‑C circuit.

Resistor and Capacitor in Parallel

With the power source operating at the same frequency as in the series case, the resistor (R) and capacitor (C) retain identical resistance and capacitance values. Consequently, their individual impedances (Z) are also identical. We begin our analysis with the following table of given values:

Parallel Resistor–Capacitor AC Circuits: Analysis, Impedance, and Ohm’s Law

In a parallel topology, the voltage across each branch is equal, so the total source voltage (10 V∠0°) appears in every column:

Parallel Resistor–Capacitor AC Circuits: Analysis, Impedance, and Ohm’s Law

Calculation Using Ohm’s Law

Applying Ohm’s Law (I = E/Z) vertically, we compute the branch currents for the resistor and capacitor:

Parallel Resistor–Capacitor AC Circuits: Analysis, Impedance, and Ohm’s Law

Just as in DC circuits, the branch currents in a parallel AC network sum to the total current, in accordance with Kirchhoff’s Current Law:

Parallel Resistor–Capacitor AC Circuits: Analysis, Impedance, and Ohm’s Law

We can determine the total impedance by applying Ohm’s Law again (Z = E/I) to the “Total” column. The same reciprocal formula used for parallel resistances also applies to any parallel impedance configuration:

Parallel Resistor–Capacitor AC Circuits: Analysis, Impedance, and Ohm’s Law

This relationship holds for all types of impedances—whether purely resistive, inductive, capacitive, or a mixture—because impedance behaves as a complex quantity in AC analysis.

While the reciprocal method may appear laborious without a calculator capable of handling complex arithmetic, both approaches—direct application of Ohm’s Law or the reciprocal formula—yield the same total impedance.

Key Takeaways

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