Circuit fundamentals and reference directions
Choose a reference node. Resistor current from a toward b is (Va − Vb)/R. Kirchhoff's current law sums signed currents to zero. For the passive sign convention, reference current enters the positive voltage terminal; positive vi then means absorbed power.
Check yourself: Does a negative current simply reverse your chosen arrow?
Thévenin equivalents and source deactivation
For a linear resistive one-port, Vth is the open-circuit terminal voltage. Find Rth with independent voltage sources shorted and independent current sources opened. Retain dependent sources and use a test source when needed. Superpose voltages or currents, not powers, because power is generally quadratic.
Check yourself: Is the load excluded, and did each source receive the correct zero-value replacement?
Transient versus DC equilibrium
At finite DC equilibrium, ideal capacitors are open and inductors short. These substitutions fail during switching. Without impulsive excitation, capacitor voltage and inductor current are continuous. A first-order RC response uses initial and final values and τ = Rseen C.
Check yourself: Have you found the post-switch resistance seen by the capacitor?
Sinusoidal steady state and phasors
Phasors describe single-frequency sinusoidal steady state, excluding startup. Use ZL = jωL and ZC = 1/(jωC), with ω = 2πf in rad/s and f in Hz. Sinusoidal RMS equals peak/√2. With RMS phasors, average power is Re(VI*), where I* conjugates I.
Check yourself: Are both voltage and current phasors RMS, at the same frequency?
Two-port networks
With both port currents entering the network, z parameters satisfy V1 = z11 I1 + z12 I2 and V2 = z21 I1 + z22 I2. Setting I2 = 0 specifies an open output port, not a short.
Check yourself: Which port variable must vanish for your parameter measurement?