Electrical Theory and Principles
This domain tests the physical math behind code rules: Ohm's law, power, series and parallel circuits, AC reactance and impedance, power factor, three-phase relationships, transformers, and voltage drop. Expect calculation items and concept items that ask why a conductor, overcurrent device, or neutral behaves as it does.
Core relationships
- Ohm's law: E = I × R; I = E/R; R = E/I.
- DC power: P = E × I; P = I²R; P = E²/R. Keep units consistent: volts, amperes, ohms, watts.
- Series: one path; current is the same; voltages add; R_total = R1 + R2 + ...
- Parallel: voltage is the same; branch currents add; 1/R_total = 1/R1 + 1/R2 + ...
- AC: 60 Hz sine wave; RMS values are used for power and code calculations; peak = RMS × √2.
- Inductive reactance X_L = 2πfL; capacitive reactance X_C = 1/(2πfC); impedance Z = √(R² + (X_L − X_C)²).
- Power factor = P/S = cos θ. True power is in watts; apparent power is in volt-amperes; reactive power is in VAR.
- Voltage drop: single-phase VD = 2KID/CM; three-phase VD = √3KID/CM, where K is the conductor constant, I is amperes, D is one-way distance, and CM is circular mils.
Three-phase and transformers
For a balanced three-phase load, P = √3 × V_L × I_L × PF. In a wye, line voltage = √3 × phase voltage and line current = phase current. In a delta, line voltage = phase voltage and line current = √3 × phase current. Transformer turns ratio: V_p/V_s = N_p/N_s; current ratio is inverse; the kVA rating does not change with voltage ratio.
Worked example
A 240-volt single-phase load draws 30 amperes at 0.80 power factor. True power = 240 × 30 × 0.80 = 5,760 W. Apparent power = 240 × 30 = 7,200 VA. Reactive power = √(7,200² − 5,760²) = 4,320 VAR. If the same 5,760 W load were balanced three-phase at 240 V and 0.80 PF, line current would be I = P/(√3 × V × PF) = 5,760/(1.732 × 240 × 0.80) ≈ 17.3 A.
Traps
- Mixing RMS and peak values.
- Using the single-phase formula on a three-phase load.
- Forgetting power factor when converting watts to amperes.
- Adding resistances directly in parallel.
- Treating transformer kVA as fixed current at every voltage.
- Ignoring the return path in voltage-drop calculations.