Reference directions and node equations
Assign a reference node and write each branch current using its chosen direction. Kirchhoff's current law enforces charge balance. Under the passive sign convention, current enters the positive voltage terminal; positive average power then means absorption rather than delivery.
Check yourself: Would reversing a branch arrow also reverse its algebraic current?
Linear network reduction
A linear two-terminal network can be represented by a Thévenin voltage and impedance. When finding impedance by source suppression, short independent ideal voltage sources and open independent ideal current sources. Keep dependent sources active and use a test source when needed.
Check yourself: Have you accidentally suppressed a source controlled by another circuit variable?
Sinusoidal impedance
With the e^(jωt) convention, resistor, inductor, and capacitor impedances are R, jωL, and 1/(jωC). Phasors describe a single-frequency steady state, not the switching transient. Combine complex impedances before taking magnitudes; phase information determines both current and power.
Check yourself: Does an inductive branch current lag its applied voltage?
Complex power with RMS phasors
For absorbed power, S = VI* = P + jQ, where the star means complex conjugation. RMS phasors need no extra factor of one-half. P is average power, Q is reactive power, and |S| is apparent power. For a consuming load with P ≥ 0 and |S| > 0, power factor is P/|S|; also state whether current leads or lags voltage.
Check yourself: Is your reactive-power sign consistent with the current phase?
Energy storage and initial conditions
Inductor current and capacitor voltage remain continuous unless an impulsive excitation changes them. For a stable first-order circuit, the response approaches its final value exponentially. Determine the resistance seen by the storage element before selecting L/R or RC as the time constant.
Check yourself: Do your initial and final values satisfy the two limiting circuits?