ECE 476 Power System Analysis

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Presentation transcript:

ECE 476 Power System Analysis Lecture 12: Power Flow Prof. Tom Overbye Dept. of Electrical and Computer Engineering University of Illinois at Urbana-Champaign overbye@illinois.edu Special Guest Lecturer: TA Iyke Idehen

Announcements Please read Chapter 2.4, Chapter 6 up to 6.6 HW 5 is 5.31, 5.43, 3.4, 3.10, 3.14, 3.19, 3.23, 3.60, 6.30 should be done before exam 1 Exam 1 is Thursday Oct 6 in class Closed book, closed notes, but you may bring one 8.5 by 11 inch note sheet and standard calculators Last name A-M here, N to Z in ECEB 1013

Power Flow Analysis When analyzing power systems we know neither the complex bus voltages nor the complex current injections Rather, we know the complex power being consumed by the load, and the power being injected by the generators plus their voltage magnitudes Therefore we can not directly use the Ybus equations, but rather must use the power balance equations

Power Balance Equations

Power Balance Equations, cont’d

Real Power Balance Equations

Power Flow Requires Iterative Solution

Gauss Iteration

Gauss Iteration Example

Stopping Criteria

Gauss Power Flow

Gauss Two Bus Power Flow Example A 100 MW, 50 Mvar load is connected to a generator through a line with z = 0.02 + j0.06 p.u. and line charging of 5 Mvar on each end (100 MVA base). Also, there is a 25 Mvar capacitor at bus 2. If the generator voltage is 1.0 p.u., what is V2? SLoad = 1.0 + j0.5 p.u.

Gauss Two Bus Example, cont’d

Gauss Two Bus Example, cont’d

Gauss Two Bus Example, cont’d

Slack Bus In previous example we specified S2 and V1 and then solved for S1 and V2. We can not arbitrarily specify S at all buses because total generation must equal total load + total losses We also need an angle reference bus. To solve these problems we define one bus as the "slack" bus. This bus has a fixed voltage magnitude and angle, and a varying real/reactive power injection.

Stated Another Way From exam problem 4.c we had This Ybus is actually singular! So we cannot solve This means (as you might expect), we cannot independently specify all the current injections I

Gauss with Many Bus Systems

Gauss-Seidel Iteration

Three Types of Power Flow Buses There are three main types of power flow buses Load (PQ) at which P/Q are fixed; iteration solves for voltage magnitude and angle. Slack at which the voltage magnitude and angle are fixed; iteration solves for P/Q injections Generator (PV) at which P and |V| are fixed; iteration solves for voltage angle and Q injection special coding is needed to include PV buses in the Gauss-Seidel iteration (covered in book, but not in slides since Gauss-Seidel is no longer commonly used)

Accelerated G-S Convergence

Accelerated Convergence, cont’d

Gauss-Seidel Advantages/Disadvantages Each iteration is relatively fast (computational order is proportional to number of branches + number of buses in the system Relatively easy to program Disadvantages Tends to converge relatively slowly, although this can be improved with acceleration Has tendency to miss solutions, particularly on large systems Tends to diverge on cases with negative branch reactances (common with compensated lines) Need to program using complex numbers

Newton-Raphson Algorithm The second major power flow solution method is the Newton-Raphson algorithm Key idea behind Newton-Raphson is to use sequential linearization

Newton-Raphson Method (scalar)

Newton-Raphson Method, cont’d

Newton-Raphson Example

Newton-Raphson Example, cont’d

Sequential Linear Approximations At each iteration the N-R method uses a linear approximation to determine the next value for x Function is f(x) = x2 - 2 = 0. Solutions are points where f(x) intersects f(x) = 0 axis

Newton-Raphson Comments When close to the solution the error decreases quite quickly -- method has quadratic convergence f(x(v)) is known as the mismatch, which we would like to drive to zero Stopping criteria is when f(x(v))  <  Results are dependent upon the initial guess. What if we had guessed x(0) = 0, or x (0) = -1? A solution’s region of attraction (ROA) is the set of initial guesses that converge to the particular solution. The ROA is often hard to determine