Dashboard PE Power Exam Prep Circuit Analysis DC circuits & network theorems DC circuits & Thevenin / Norton

DC circuits & Thevenin / Norton

Ohm + Kirchhoff + mesh/nodal methods. Thevenin equivalent (V_th, R_th) and Norton dual (I_N, R_N). Max power transfer (R_L = R_th, η = 50%). Superposition. Foundation of all linear circuit analysis.

Freshman ~11 min

Step 1 — Ohm + Kirchhoff: foundation of DC circuit analysis

0.55×
V_th R_th I_load

Reference notes

This is the foundational toolkit for any linear DC (and by extension, any sinusoidal steady-state AC) circuit. Use Next → to walk through Ohm + Kirchhoff, the two systematic methods (mesh / nodal), Thevenin and Norton equivalents, the maximum power transfer theorem, and superposition.

Three fundamental laws

Resistor combinations

Power in circuit elements

P = V · I = I2 · R = V2 / R

P > 0 when absorbed; P < 0 when supplied. Sum of supplied = sum of absorbed (conservation of energy).

Systematic methods

Thevenin's theorem

Any linear 2-terminal network → equivalent ONE voltage source V_th in series with ONE resistance R_th:

Once V_th and R_th are known, terminal behavior for ANY load R_L is:

V_load = V_th · R_L / (R_L + R_th), I_load = V_th / (R_th + R_L)

Norton's theorem

Dual of Thevenin: same network → I_N in PARALLEL with R_N.

Maximum power transfer

For fixed V_th, R_th, the R_L that absorbs maximum power equals R_th.

P_max = V_th2 / (4 · R_th), η at max-P = 50 %

Superposition

In a LINEAR circuit with multiple independent sources, the V (or I) response at any element = sum of responses caused by each source ALONE, with all other independent sources zeroed (V → short, I → open).

Take-away. Ohm + KCL + KVL → all linear DC analysis. Series-parallel reduction, voltage / current dividers, source transformations follow as derived techniques. Thevenin (V_th + R_th series) and Norton (I_N + R_N parallel) summarize any 2-terminal network for arbitrary loads. Max power transfer: R_L = R_th, max P = V_th²/(4·R_th), η = 50 %. Superposition: sum responses from each source alone — for V and I only, not for P. These tools generalize directly to phasor analysis for sinusoidal steady-state AC by replacing R with complex impedance Z.