DC Circuits

Lectures 7–9 · Tutorials 5–6  |  Ohm's Law, Resistance, Series/Parallel, Power, EMF

Current & Ohm's Law

Cylindrical Conductor — From Physics to Circuits

E field → I → S (cross-section) L (length) V = E·L | I = J·S | J = σE → V = I·L/(σS) = I·R

Electric Current

I = dQ/dt [A = C/s]

Current density (per unit area):

J = I/S [A/m²]
J = σ·E (conduction current)

Ohm's Law

V = I·R [V]
R = L/(σ·S) = ρ·L/S [Ω]

σ = conductivity [S/m], ρ = resistivity = 1/σ [Ω·m]

💡 Valid only for uniform cross-section conductors.

Power

P = V·I = I²R = V²/R [W]

If P > 0 → power absorbed (load).
If P < 0 → power supplied (source).

Conductivity Table

Materialσ [S/m]
Gold4.1×10⁷
Aluminum4.0×10⁷
Silicon4.4×10⁻⁴
Glass10⁻¹²
🔌 Series & Parallel Resistance

Series Resistors — same current

R₁ R₂ R₃ I → R_eq = R₁ + R₂ + R₃ Same I, voltages ADD

Parallel Resistors — same voltage

R₁ R₂ R₃ V + V − 1/R_eq = 1/R₁+1/R₂+1/R₃

Series Combination

R_eq = R₁ + R₂ + R₃ + …

Same current through all. Total V = sum of individual V drops. R_eq > any single resistor.

Parallel Combination

1/R_eq = 1/R₁ + 1/R₂ + 1/R₃

Two resistors: R_eq = R₁R₂/(R₁+R₂)

Same voltage across all. Total I = sum of branch currents. R_eq < smallest resistor.

Open & Short Circuits

Open circuit: R = ∞, I = 0
Short circuit: R = 0, V = 0
💡 If a resistor is shorted (R=0) in parallel with others, the whole parallel combination = 0. All current flows through the short.
📝 Real-world Example — Transmission Line
AWG aluminum cable: σ=4×10⁷ S/m, A=107 mm², L=100 km. System delivers 10 MW at V=200 kV, I=50 A.
R_TL = L/(A·σ) = 100×10³ / (107×10⁻⁶ × 4×10⁷) = 23.36 Ω
P_loss = I²R = 50² × 23.36 = 58,400 W ≈ 58.4 kW
Loss% = 58.4 / (10000 + 58.4) = 0.58% ← High voltage = low loss!
🔋 EMF, Batteries & Internal Resistance

Real Battery with Internal Resistance r

V_emf r (int) + R_L I → V_emf = I(R_L + r) | I = V_emf/(R_L+r) | V_terminal = V_emf − Ir

Ideal vs Real Source

Ideal: V_terminal = V_emf
Real: V_terminal = V_emf − I·r

r is the internal resistance. Higher current drawn → larger voltage drop inside → lower terminal voltage.

Power Distribution

P_total = I·V_emf
P_load = I²·R_L
P_internal = I²·r

Total power = load power + internal losses.

Special Cases

Open circuit: I = 0, V_terminal = V_emf (no drop).
Short circuit: V = 0, I = V_emf/r (maximum current).

💡 These are the two extremes of the V-I characteristic line for a source.