Power Systems

Comprehensive guide to electrical power systems, generation, transmission, and distribution.

Three-Phase Systems

Three-phase systems are the most common method for electric power transmission and distribution. In a balanced three-phase system:

V_L = √3 × V_P

I_L = I_P (for Y-connection)

I_L = I_P / √3 (for Δ-connection)

Where:

  • V_L = line voltage (V)
  • V_P = phase voltage (V)
  • I_L = line current (A)
  • I_P = phase current (A)

The total power in a balanced three-phase system is:

P = √3 × V_L × I_L × cos(φ)

Q = √3 × V_L × I_L × sin(φ)

S = √3 × V_L × I_L

Where:

  • P = active power (W)
  • Q = reactive power (VAR)
  • S = apparent power (VA)
  • cos(φ) = power factor

Power Flow Analysis

Power flow analysis is used to determine the steady-state operating condition of a power system. The power flow equations for a bus i are:

P_i = |V_i| × ∑|V_j| × |Y_ij| × cos(θ_ij + δ_j - δ_i)

Q_i = |V_i| × ∑|V_j| × |Y_ij| × sin(θ_ij + δ_j - δ_i)

Where:

  • P_i, Q_i = active and reactive power at bus i
  • |V_i|, |V_j| = voltage magnitudes at buses i and j
  • |Y_ij| = magnitude of the (i,j) element of the bus admittance matrix
  • θ_ij = angle of the (i,j) element of the bus admittance matrix
  • δ_i, δ_j = voltage angles at buses i and j

Power flow studies typically use iterative methods such as Newton-Raphson or Gauss-Seidel to solve these nonlinear equations.

Fault Analysis

Fault analysis is used to determine the currents and voltages in a power system during fault conditions. The symmetrical components method is commonly used for analyzing unbalanced faults:

[V_0, V_1, V_2]ᵀ = [A] × [V_a, V_b, V_c]ᵀ

[I_0, I_1, I_2]ᵀ = [A] × [I_a, I_b, I_c]ᵀ

Where:

  • V_0, V_1, V_2 = zero, positive, and negative sequence voltages
  • I_0, I_1, I_2 = zero, positive, and negative sequence currents
  • V_a, V_b, V_c = phase voltages
  • I_a, I_b, I_c = phase currents
  • [A] = transformation matrix

For a three-phase balanced system, the transformation matrix is:

[A] = [1, 1, 1; 1, a, a²; 1, a², a]

Where a = e^(j2π/3) is a complex operator representing a 120° phase shift.