Lecture II Objective: Representation of sequence components

Slides:



Advertisements
Similar presentations
Lecture #12 EGR 272 – Circuit Theory II
Advertisements

Lecture 1. Balanced Three-phase Systems From Network to Single-phase Equivalent Circuit Power plant TransformerSwitching station LineLoad Three-phase.
Lesson 8 Symmetrical Components
Announcements Be reading Chapters 8 and 9
Chapter 12 Three Phase Circuits
SYMMETRICAL COMPONENETS OF POWER SYSTEM
Chapter 12 Three-Phase Circuits
ARRDEKTA INSTITUTE OF TECHNOLOGY ♦ GUIDED BY ♦ Prof. D.R.PATE Asst.prof in electrical Department PREPARED BY PREPARED BY RATHOD VISHANU. RATHOD VISHANU.
EE 369 POWER SYSTEM ANALYSIS
Lecture 6. Chapter 3 Microwave Network Analysis 3.1 Impedance and Equivalent Voltages and Currents 3.2 Impedance and Admittance Matrices 3.3 The Scattering.
Electromagnetic Oscillations and Alternating Current
Power I, VI, V I max  V max  I, VI, V I max AC Circuits use a similar definition of power as DC circuits. The one detail that need to be included.
Physics for Scientists and Engineers II, Summer Semester Lecture 19: July 8 th 2009 Physics for Scientists and Engineers II.
Transformer Professor Mohamed A. El-Sharkawi. 2 Why do we need transformers? Increase voltage of generator output –Transmit power and low current –Reduce.
Problem #2-8 A 480 – 120 V, 60 Hz transformer has its high voltage winding connected to a 460 V system, and its low voltage winding connected to a 24/32.8°Ω.
1 AC Nodal and Mesh Analysis Discussion D11.1 Chapter 4 4/10/2006.
ECE 4411 Introduction to Three-Phase Power. ECE 4412 Typical Transformer Yard.
Lesson 35 Per Phase Analysis
Lecture 101 EEE 302 Electrical Networks II Dr. Keith E. Holbert Summer 2001.
Universal College of Engineering & Technology
Announcements Be reading Chapter 3
Lecture No. 11 By. Sajid Hussain Qazi
Generator Protection. Amount of Protection Rated power of the generator Ratio of its capacity to the total capacity of the system Configuration of the.
Unit 27 Three-Phase Circuits
Chapter 7 Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
POLY PHASE A.C.CIRCUITS CHAPTER 7.
Balanced 3-phase systems Unbalanced 3-phase systems
Balanced poly phase circuits. Two and four phase systems  A two phase system is an electrical system in which the voltages of the phases are 90 degree.
Circuits II EE221 Unit 12 Instructor: Kevin D. Donohue
Three – Phase Power System. Three-Phase Power Definitions 4 wires –3 “active” phases, A, B, C –1 “ground”, or “neutral” Color Code –Phase ARed –Phase.
Lecture 28Electro Mechanical System1  Consider a circuit with a source, a load, & appropriate meters.  P and Q are positive, so the load absorbs both.
1 Chapter 3 Harmonic Modeling of Networks Contributors: T. Ortmyer, C. Hatziadoniu, and P. Ribeiro Organized by Task Force on Harmonics Modeling & Simulation.
ECE 530 – Analysis Techniques for Large-Scale Electrical Systems
EE212 Passive AC Circuits Lecture Notes 2a EE 212.
Dept of Aeronautical Enggineering S.M.M. Rahman MIST Direct Current Limitations: Transmission Loss No Amplification Power Distribution Lim.
Fundamentals of Electric Circuits Chapter 13 Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
Announcements For lectures 9 and 10 please be reading Chapter 3
P.VIJAYALAKSHMI M.E(power electronics &drives) Assistant Professor EEE Department.
Announcements Read Chapters 8 and 9 HW 9 quiz today
THREE PHASE POWER Generation Transportation Consumption.
CIRCUITS and SYSTEMS – part I Prof. dr hab. Stanisław Osowski Electrical Engineering (B.Sc.) Projekt współfinansowany przez Unię Europejską w ramach Europejskiego.
LITAR ELEKTRIK II EET 102/4. SILIBUS LITAR ELEKTRIK II  Mutual Inductance  Two port Network Pengenalan Jelmaan Laplace Pengenalan Jelmaan Laplace Kaedah.
Balanced poly phase circuits. Two and four phase systems  A two phase system is an electrical system in which the voltages of the phases are 90 degree.
Lecture 19 Fault Analysis, Grounding, Symmetrical Components Professor Tom Overbye Department of Electrical and Computer Engineering ECE 476 POWER SYSTEM.
Grounded Wye-Delta Transformer Bank Backfeed Short-Circuit Currents W. H. Kersting & Wayne Carr Milsoft Utility Solutions.
ELEN 3441 Fundamentals of Power Engineering Spring Instructor: Dr. Gleb V. Tcheslavski Contact: Office Hours:
NEUTRAL CURRENT IS NOT ZERO
Chapter 9 Sinusoids and Phasors
Power System Protective Relaying-Part Two
Hao Zhu Dept. of Electrical & Computer Engineering University of Illinois, Urbana-Champaign ECE 498HZ: Power Distribution System Analysis.
ECE 476 POWER SYSTEM ANALYSIS
B4.2 Power System One-Line Diagrams
DC MACHINE AND tRANSFORMER
SWAMI VIVEKANAND COLLEGE OF ENGINEERING,INDORE(M.P)
K. J. I. T institute of engineering 3-PHASE TRANSFORMER. PREPARD BY:-
Energy Conversion and Transport George G. Karady & Keith Holbert
Single Phase Transformers ELE 2103 Electrical Machinery1
3-Phase Transformer Construction, Principal, Working, Operation Advantages Over 1-Phase Transformer Introduction Advatages Construction Principal Working.
Energy Conversion and Transport George G. Karady & Keith Holbert
Ch. 13 – Ideal Transformers
Transformer Impedance
ELL100: INTRODUCTION TO ELECTRICAL ENGG.
Three Phase Circuits Chapter Objectives:
TRANSFORMERS.
Lecture 10 - Transformers/Three-Phase Circuits
Source Transformation
C H A P T E R 23 Symmetrical Components.
Three Phase Transformers
Prepared by: Ismael K. Saeed
Exercise 9 Power systems.
Presentation transcript:

Lecture II Objective: Representation of sequence components Equation to find unbalanced vectors from symmetrical components and vice versa. Definition: Sequence Impedance and sequence Network Sequence Networks for Power system Components Zero sequence network for transformer connections.

Classification of Symmetrical Components for 3Φ System Three Types – Positive Sequence , Negative Sequence and Zero Sequence - Magnitude, Displacement and Phase Sequence Positive Sequence 3 vectors equal magnitude 120° displaced Phase sequence similar to Original Vectors Negative Sequence 3 Vectors Phase sequence Opposite to Original Vectors Zero Sequence equal in magnitude No phase Difference

Representation of Positive Sequence Components Vc1 Va1 120° Vc1= a Va1 120° Va1 Vb1=a2Va1 120° Vb1

Representation of Negative Sequence Components Vb2 Va2 Vb2= a Va2 Vc2=a2Va2 120° 120° Va2 120° Vc2

Representation of Zero Sequence Components Va0 Va0 = Vb0 = Vc0 Vb0 Vc0

Equation for Phase Voltage from Symmetrical Components Positive Sequence Va1 Vc1= a Va1 Vb1=a2Va1 Negative Sequence Va2 Vb2= a Va2 Vc2=a2Va2 Zero Sequence Va0 = Vb0 = Vc0 Phase Voltage in terms of Symmetrical Components Va= Va1 + Va2 + Va0 ………………………………. 1 Vb= Vb1 + Vb2 + Vb0 Vb= a2Va1 + a Va2 + Va0 ……………………………. 2 Vc= Vc1 + Vc2 + Vc0 Vc= a Va1 + a2Va2 + Va0 ………………………………. 3

Cond… Equation in Matrix Form for phase Voltage and phase current in terms of symmetrical components of voltage and current is, Vph= T Vsym where T is Symmetrical Component Transformation Matrix, ----------------------- 4 ----------------------- 5

Equation for Symmetrical Components from Phase Voltage Symmetrical components of Voltage and currents from phase Voltages and phase currents ----------------- 6 ----------------- 7 ----------------- 8

Sequence Impedance Definition: The impedance offered by the circuit elements for sequence current is called as sequence Impedance. Positive sequence Impedance Negative Sequence Impedance Zero sequence Impedance

Definition sequence Impedances 1.Positive sequence Impedance: The impedance offered by circuit elements for positive sequence currents is called as positive sequence impedance. 2. Negative Sequence Impedance: The impedance offered by circuit elements for negative sequence currents is called as negative sequence impedance. 3. Zero Sequence Impedance: The impedance offered by circuit elements for zero sequence currents is called as zero sequence impedance.

Sequence Networks Definition: The single phase equivalent circuit of power system formed using the impedance of any one sequence only is called as sequence network. Positive sequence Network (or) Per unit reactance Negative sequence Network Zero sequence Network

Positive, Negative and Zero Sequence Networks for Power System Components Generator Transmission Line Transformer Load

Positive, Negative Sequence Networks for Generator with neutral is not Grounded Positive Sequence Network Ia1 Va1=Ea-Ia1Z1 Ref. bus Negative Sequence Network Va0= -Ia0Z0 Va2= -Ia2Z2 Ref. bus Zero Sequence Network Ref. bus

Zero Sequence Network for Generator with Neutral is Grounded Va0= -Ia0Z0 Zn Ref. bus Zero Sequence Network

Transmission Line Positive Sequence Network Ia2 Z2 Va2 Ref. bus Negative Sequence Network Ia1 Z1 Va1 Ref. bus Ia0 Z0 Va0 Ref. bus Zero Sequence Network

Transformer Positive Sequence Network Negative Sequence Network Z2 Z1 Ia2 Z2 Va2 Ref. bus Negative Sequence Network Ia1 Z1 Va1 Ref. bus

Zero sequence Network of Transformer D1 D2 Ref. bus S – Indicates Star Connection D – Indicates Delta Connection 1 – Indicates Primary Side 2 – Indicates Secondary Side For Delta connections in primary and secondary side, switches D1 and D2 will be closed otherwise in open condition. For Star connection with neutral grounded, switches S1 and S2 will be closed otherwise in open condition.

Zero sequence Network of Transformer Y – Y Y – Δ Δ - Δ Ref. bus Z0 S1 S2 D2 Z0 S1 S2 D2 D1