Understanding Impedance in Parallel RL Circuits
In alternating current (AC) physics, components interact differently compared to basic direct current (DC) systems. When a pure resistor and an inductor are connected in parallel across an AC voltage source, the voltage across both components remains identical in magnitude and phase. However, the currents passing through each branch differ significantly due to reactive opposition.
The resistor opposes current flow linearly without introducing phase shifts, maintaining branch current in phase with the applied supply voltage. In contrast, the inductor opposes changes in current through electromagnetic induction, causing current through the inductive branch to lag behind the supply voltage by exactly 90 degrees. Because these branch currents are orthogonal, total circuit impedance cannot be calculated by adding component resistances directly.
The Concept of Admittance and Reactance
To analyze parallel AC networks effectively, electrical engineers often utilize admittance ($Y$), which represents the ease with which current flows through a circuit. Admittance is the mathematical reciprocal of impedance ($Y = 1/Z$) and is measured in Siemens ($S$). In a parallel RL combination, total admittance equals the vector sum of conductance ($G = 1/R$) from the resistor and inductive susceptance ($B_L = 1/X_L$) from the coil.
As the operating signal frequency increases, inductive reactance ($X_L = 2\pi f L$) increases proportionally. High reactance restricts current through the inductor branch, pushing total equivalent circuit impedance closer to the pure resistance value $R$. Conversely, at lower signal frequencies, inductive reactance decreases, causing the inductor to act as a dominant low-impedance path that draws higher lagging current from the power supply.