Power System Analysis Lecture Notes Ppt Today

[ I_a1 = \fracV_fZ_1 + Z_2 + Z_0 + 3Z_f ] [ I_f = 3I_a1 ]

| Line type | R (Ω/km) | L (mH/km) | C (nF/km) | |-----------|----------|-----------|-----------| | Short (<80 km) | lumped | ignored | ignored | | Medium (80–240 km) | lumped | lumped | lumped (π model) | | Long (>240 km) | distributed parameters | | | 4. Load Flow Analysis (PPT Module 4) Goal: Determine voltage magnitude & angle at each bus for given loads/generations.

Zero-sequence current cannot flow if transformer delta or ungrounded wye on source side. 7. Power System Stability (PPT Module 7) Definition: Ability to return to synchronous operation after a disturbance.

neglected for overhead lines.

[ C = \frac2\pi \epsilon_0\ln(D/r) \ \textF/m ]

Base quantities: ( S_base ) (3-phase MVA), ( V_base ) (line-to-line kV).

Derived bases: [ I_base = \fracS_base\sqrt3 V_base, \quad Z_base = \frac(V_base)^2S_base ] power system analysis lecture notes ppt

[ Z_pu,new = Z_pu,old \times \left( \fracV_base,oldV_base,new \right)^2 \times \left( \fracS_base,newS_base,old \right) ]

Convert a 10% transformer reactance from 20 MVA, 132 kV to 100 MVA, 132 kV → ( Z_pu,new = 0.1 \times (1)^2 \times (100/20) = 0.5 ) pu. 3. Transmission Line Parameters (PPT Module 3) Resistance: ( R = \rho \fraclA ) (corrected for skin effect at 50/60 Hz).

[ L = 2\times 10^-7 \ln \left( \fracDr' \right) \ \textH/m ] where ( r' = r \cdot e^-1/4 ) (geometric mean radius, GMR). [ I_a1 = \fracV_fZ_1 + Z_2 + Z_0

Generator: 10 MVA, 11 kV, ( X_d'' = 0.12 ) pu. Transformer 10 MVA, 11/132 kV, ( X_t = 0.08 ) pu. Line impedance 20 Ω (on 132 kV). Fault at 132 kV bus. Find ( I_f ) in kA.

Slide 1: Title – Load Flow Analysis Slide 2: Bus types (Slack, PV, PQ) Slide 3: Y-bus formation example (3-bus system) Slide 4: Newton-Raphson algorithm flowchart Slide 5: Convergence criteria (|ΔP|,|ΔQ| < 0.001) Slide 6: Class exercise – 4-bus system Slide 7: Solution & interpretation (voltage profile)

[ \textpu value = \frac\textActual value\textBase value ] [ C = \frac2\pi \epsilon_0\ln(D/r) \ \textF/m ]