SIMULATION OF THREE PHASE THREE LEG TRANSFORMER BEHAVIOR UNDER DIFFERENT VOLTAGE SAG TYPES

Similar documents
Chapter 7. Systems 7.1 INTRODUCTION 7.2 MATHEMATICAL MODELING OF LIQUID LEVEL SYSTEMS. Steady State Flow. A. Bazoune

Introduction to Electronic circuits.

Conduction Heat Transfer

CHAPTER 3 ANALYSIS OF KY BOOST CONVERTER

Wp/Lmin. Wn/Lmin 2.5V

V. Electrostatics Lecture 27a: Diffuse charge at electrodes

ME2142/ME2142E Feedback Control Systems. Modelling of Physical Systems The Transfer Function

PHYSICS 536 Experiment 12: Applications of the Golden Rules for Negative Feedback

Design of Analog Integrated Circuits

Feedback Principle :-

CTN 2/23/16. EE 247B/ME 218: Introduction to MEMS Design Lecture 11m2: Mechanics of Materials. Copyright 2016 Regents of the University of California

Circuits Op-Amp. Interaction of Circuit Elements. Quick Check How does closing the switch affect V o and I o?

IGEE 401 Power Electronic Systems. Solution to Midterm Examination Fall 2004

Transient Conduction: Spatial Effects and the Role of Analytical Solutions

EE 204 Lecture 25 More Examples on Power Factor and the Reactive Power

A New Method for Solving Integer Linear. Programming Problems with Fuzzy Variables

CHAPTER 3: FEEDBACK. Dr. Wan Mahani Hafizah binti Wan Mahmud

Convoluted Arc with Flux Concentrator for Current Interruption

55:041 Electronic Circuits

Physic 231 Lecture 33

Water vapour balance in a building moisture exposure for timber structures

Lecture 12. Heat Exchangers. Heat Exchangers Chee 318 1

Chem 204A, Fall 2004, Mid-term (II)

Faculty of Engineering

Waveshapping Circuits and Data Converters. Lesson #17 Comparators and Schmitt Triggers Section BME 373 Electronics II J.

4.8 Degradation of Elastomers by Heat and/or Radiation

Week3, Chapter 4. Position and Displacement. Motion in Two Dimensions. Instantaneous Velocity. Average Velocity

Shell Stiffness for Diffe ent Modes

element k Using FEM to Solve Truss Problems

Section 3: Detailed Solutions of Word Problems Unit 1: Solving Word Problems by Modeling with Formulas

The three major operations done on biological signals using Op-Amp:

III. Operational Amplifiers

Comparison between Back-to-Back and Matrix Converters Based on Thermal Stress of the Switches

Fast Acquisition Digital Tanlock Loop with Adaptive Time Delay

_J _J J J J J J J J _. 7 particles in the blue state; 3 particles in the red state: 720 configurations _J J J _J J J J J J J J _

State-Space Model Based Generalized Predictive Control for Networked Control Systems

Chapter 3, Solution 1C.

Study Group Report: Plate-fin Heat Exchangers: AEA Technology

SELECTION OF MODEL PARAMETERS OF BIOGAS IC ENGINE. Karol Cupiał, Grzegorz Katolik

Novel current mode AC/AC converters with high frequency ac link *

Copyright Paul Tobin 63

CHAPTER 3 QUASI-RESONANT BUCK CONVERTER

EE 221 Practice Problems for the Final Exam

OTHER USES OF THE ICRH COUPL ING CO IL. November 1975

Exercises H /OOA> f Wo AJoTHS l^»-l S. m^ttrt /A/ ?C,0&L6M5 INFERENCE FOR DISTRIBUTIONS OF CATEGORICAL DATA. tts^e&n tai-ns 5 2%-cas-hews^, 27%

Voltage Sag and Swell Mitigation Using Matrix Converter with Reduced Number of Switches

Chapter 6 : Gibbs Free Energy

PT326 PROCESS TRAINER

A Proposal of Heating Load Calculation considering Stack Effect in High-rise Buildings

2 Analysis of the non-linear aerodynamic loads of hypersonic flow. 1 General Introduction

A method of constructing rock-analysis diagrams a statistical basks.

Module B3. VLoad = = V S V LN

Pull-Out Strength of a Cast-In-Place Anchor Bolt in Concrete Exposed to High Temperature

Grade 12 Physics Exam Review

modeling of equilibrium and dynamic multi-component adsorption in a two-layered fixed bed for purification of hydrogen from methane reforming products

Analysis of the induction machines sensitivity to voltage sags. F. Córcoles and J. Pedra Ll. Guasch

Synchronous Motor V-Curves

Applying Kirchoff s law on the primary circuit. V = - e1 V+ e1 = 0 V.D. e.m.f. From the secondary circuit e2 = v2. K e. Equivalent circuit :

Linearity. If kx is applied to the element, the output must be ky. kx ky. 2. additivity property. x 1 y 1, x 2 y 2

Comparison of Building Codes and Insulation in China and Iceland

Advances in Engineering Research (AER), volume 102 Second International Conference on Mechanics, Materials and Structural Engineering (ICMMSE 2017)

BME 5742 Biosystems Modeling and Control

Edexcel GCSE Physics

Phys 344 Ch 5 Lect 4 Feb 28 th,

Prediction of Thermal Conductivity of Aligned Short Fibre Composites with Different Fibre Aspect Ratios

Comparison of the DC/DC-Converters for Fuel Cell Applications

Problem Set 5 Solutions - McQuarrie Problems 3.20 MIT Dr. Anton Van Der Ven

CIRCLE YOUR DIVISION: Div. 1 (9:30 am) Div. 2 (11:30 am) Div. 3 (2:30 pm) Prof. Ruan Prof. Naik Mr. Singh

Where a licence is displayed above, please note the terms and conditions of the licence govern your use of this document.

34. YTTRIUM AND OTHER TRACE ELEMENTS IN BASALTS FROM DSDP LEG 37

COMPARISON OF SOME RELIABILITY CHARACTERISTICS BETWEEN REDUNDANT SYSTEMS REQUIRING SUPPORTING UNITS FOR THEIR OPERATIONS

Improved Bridgeless Interleaved Boost PFC Rectifier with Optimized Magnetic Utilization and Reduced Sensing Noise

Spring 2002 Lecture #17

CIRCUIT ANALYSIS II Chapter 1 Sinusoidal Alternating Waveforms and Phasor Concept. Sinusoidal Alternating Waveforms and

Analytical Modeling of Natural Convection in Horizontal Annuli

AVOLTAGE SAG is a short-duration reduction in rms

Computational modeling techniques

Chapter 30. Inductance

Bi-level Optimization Method of Air-conditioning System Based on Office Building Energy Storage Characteristics

A Note on the Linear Programming Sensitivity. Analysis of Specification Constraints. in Blending Problems

Thermodynamic Assessment of Liquid Fe Si C System by Unified Interaction Parameter Model

CAUSAL INFERENCE. Technical Track Session I. Phillippe Leite. The World Bank

Magnetic Field Around The New 400kV OH Power Transmission Lines In Libya

LOW FREQUENCY NOISE IN JUNCTION FIELD EFFECT TRANSISTORS

Improved Bridgeless Interleaved Boost PFC Rectifier with Optimized Magnetic Utilization and Reduced Sensing Noise

Fields and Waves I. Lecture 3

Concurrent Adaptive Cancellation of Quantization Noise and Harmonic Distortion in Sigma Delta Converter

Attempts at Ion Cyclotron Heating. In a Toroidal Octupole. Presented at the Los Angeles Meeting of the American Physical Society. November 12-15, 1969

Lucas Imperfect Information Model

CHAPTER Read Chapter 17, sections 1,2,3. End of Chapter problems: 25

Nomenclature: number of electrons e -1. electron charge F constant number, (columbs/moles of e -1 ) atomic number g

CONVEX COMBINATIONS OF ANALYTIC FUNCTIONS

Part III Lectures Field-Effect Transistors (FETs) and Circuits

A Hybrid Variational Iteration Method for Blasius Equation

Linear Amplifiers and OpAmps

Chapter 16. Capacitance. Capacitance, cont. Parallel-Plate Capacitor, Example 1/20/2011. Electric Energy and Capacitance

Linear Plus Linear Fractional Capacitated Transportation Problem with Restricted Flow

SIMULATION AND MODELING OF VECTOR CONTROLLED 3-PHASE MATRIX CONVERTER INDUCTION MOTOR DRIVE

READING STATECHART DIAGRAMS

Global Sensitivity. Tuesday 20 th February, 2018

Transcription:

SIMULATION OF THREE PHASE THREE LEG TRANSFORMER BEHAVIOR UNDER DIFFERENT VOLTAGE SAG TYPES Mhammadreza Dlatan Alreza Jallan Department f Electrcal Engneerng, Iran Unversty f scence & Technlgy (IUST) e-mal: mhammadreza_dlatan@yah.cm e-mal: Jallan@ust.ac.r Key wrds: Vltage Sag, Three phase three leg transfrmer, Inrush current ABSTRACT Vltage sags are usually caused by energzng heavy lads such as arc furnaces, startng f large mtrs, sngle lne t grund (SLG) faults, lad transferrng frm ne pwer surce t anther etc. Vltage sags can cause prblems n sme electrcal equpment such as transfrmers, nductn mtrs etc. Smulatn shws that transfrmer saturatn s prduced when the vltage sag s recvered. It prduces dc magnetc flux and causes transfrmer saturatn. Inrush current smlar t that f transfrmer energzng s als created. In ths paper the effects f vltage sag type, depth and duratn are nvestgated by smulatn f a three phase transfrmer n Matlab envrnment. It s shwn that the current pea has a perdcal dependence n sag duratn n symmetrcal vltage sags. The lnear nfluence f sag depth s bserved n the nrush current pea value. It s als shwn that unsymmetrcal sags can prduce current pea as hgh as thse f symmetrcal vltage sags. 1. INTRODUCTION Pwer qualty prblems have sgnfcant nfluences n dfferent equpments such as transfrmers. Vltage sag s a majr cause f mal-functn f electrcal devces and equpment n electrcal systems, ndustral prcess, etc [1. It s reprted that the ttal damages due t vltage sags are hgher than ther pwer qualty prblems [2. Recently, behavur f three phase three leg transfrmer under dfferent vltage sag cndtns s nvestgated. One mdel fr three phase three leg transfrmer n PSPICE s ntrduced n [3. The transfrmer was mdelled wth varable characterzatn f ts nnlnear magnetc behavur. Each leg was vewed as a separate magnetc crcut and a functn was prpsed t represent cre nnlnear behavur. There was a functnal relatnshp between the magnetc ptental n the leg and the flux thrugh t. The mdel was mplemented and the transfrmer behavur under dfferent sag depth, duratn and ntal pnt n wave n symmetrcal vltage sag was reprted [4. Mdellng f three phase three leg transfrmer peratng under dfferent types f vltage sag n PSPICE was mplemented and reprted n [5. Unsymmetrcal vltage sag effect n transfrmer and current pea relatn wth type f vltage sags, duratn and depth was nvestgated. In ths paper a three phase three leg transfrmer and all type f vltage sags are mdelled n MATLAB/SIMULINK envrnment fr smulatn purpses. Fr prducng dfferent types f vltage sag a blc s created n MATLAB/SIMULINK t tae the parameters f vltage sag such as sag duratn ( t), depth (h) and ntal pnt n wave. In the next step the prduced vltages are appled t the transfrmer mdel separately n rder t evaluate the transfrmer behavur. The transfrmer mdel whch was mplemented n MATLAB/SIMULINK s based n the prevusly develped mdel [3. 2. CHARACTERIZATION AND SIMULATION OF VOLTAGE SAGS There are dfferent types f vltage sags whch are characterzed by ts magntude, duratn and phase angle jump. Phase angle jump depends n X/R rat f the surce and feeder. Anther reasn fr phase angle jump s the changng f the vltage t lwer level [2. Vltage sags are dvded n t 7 grups as types A t G [3. Three phase faults cause type A whch s symmetrcal vltage sag. Unsymmetrcal vltage sags are due t sngle phase and phase t phase faults [4. T clear these faults crcut breaers usually act at zer crssng pnt f current. The number f sequences fr vltage recvery depends n the fault type and can prduce 14 sub-grups as descrbed n [3. Fg.1 shws the blc that s mplemented n MATLAB/SIMULINK fr smulatn dfferent types f vltage sag. All type f vltage sag are prduced wth changng vltage sag characterstcs (sag duratn ( t), sag duratn (h) and ntal pnt n wave ( ) ).

vltage sag characterstcs s peratn f transfrmer s cnsdered under dfferent characterstcs f vltage sags. 4. TRANSFORMER OPERATION UNDER VOLTAGE SAG Transfrmer s smulated under symmetrcal vltage sag frst. Effects f vltage sag duratn, vltage sag depth and ntal pnt n wave n transfrmer has been nvestgated where the transfrmer lad s 0.8 p.u. Fg.1. MATLAB/SIMULINK Blc fr smulatn f dfferent types f vltage sags 3. SIMULATION OF THREE PHASE THREE LEG TRANSFORMER A 60VA-380/220V-WyeG-WyeG three phase three leg transfrmer s used fr smulatn purpses n MATLAB/SIMULINK. Functn (1) s used fr presentng cre nnlnear behavr between magnetc ptental n the leg and the flux thrugh t [3. R 1 1 ( f ) + 1 2 p p f 1 + f 0 f R ( f ) φ (1) where 1, 2,p and f 0 are expermental parameters wch allw ths sngle-valued functn t be ftted t the ( φ f ) transfrmer saturatn curve. 4-1. SYMMETRICAL VOLTAGE SAG (TYPE A) Fg.3 shws ntal vltage, current and fluxes n a vltage sag wth fllwng characterstcs: v( h 0.4, 5T 0). In ths case n pea current s ccurred. Ths fgure shws that n saturatn s ccurred when ntal and fnal fluxes are equal ( φ φ f ). Fg.4 shws that saturatn s ccurred when ( φ φf ). Fg.5 shws nrush current that s ccurred n lng term vltage sag wth characterstcs v( h 0.4, 150.5T 0). The current pea has a perdcal dependence n sag duratn n symmetrcal vltage sags. It means that pea t, ) pea + nt ). Shrt term vltage sag wth fllwng characterstc v( h 0.4, 5.5T 0) s als shwn n Fg.6 whch s smlar t Fg 5. It shws that the current pea has a perdcal dependence n sag duratn. Fg.2. Internal Vew f Smulated Three-phase Three leg Transfrmer Insde vew f smulated three phase three leg transfrmer s shwn n Fg.2. Further detal abut magnetc and electrc crcut are descrbed n [4. Tw mprtant effects f vltage sag are saturatn and nrush current n transfrmers. Inrush current s depended n dfferent Fg.3. Three phase vltage, current and flux fr a sag type v( h 0.4, 5T 0)

nfluence n transfrmer s cnsdered here. Each seres has cnstant ntal pnt n wave and vltage sag depth and dfferent vltage sag duratn as: v1 ( h 0.4,, wt 0 ),...6T v2 ( h 0.4,, 90 ),...6T v3 ( h 0.4,, 180 ),...6T v4 ( h 0.4,, 270 ), [ 5T...6T Fg.7 shws clearly that maxmum nrush current s ccured when 0 r 180 and ( nt +1/ 2) when n1, 2, 3 and etc. Fg.4. Three phase vltage, current and flux fr a sag type v ( h 0.4, 5.5T 0) Fg.5. Three phase current fr a sag type v( h 0.4, 150.5T 0) Fg.7. Maxmum nrush current versus dfferent vltage sag duratn n vltage sag type A wth h0.4 4-1-2. VOLTAGE SAG DEPTH INFLUENCE İnfluence f vltage sag depth s cnsdered here wth the fllwng characterstcs : v1 5.5T 0 ), h [0...0.9 v2 5.4T 0 ), h [0...0.9 v3 5.3T 0 ), h [0...0.9 v4 5.2T 0 ), h [ 0...0.9 v (, 5.1, 0 ), [0...0.9 5 h t T h v6 5T 0 ), h [0...0.9 Fg.6. Three phase current fr a sag type v( h 0.4, 5.5T 0) 4-1-1. VOLTAGE SAG DURATION INFLUENCE 4 seres f vltage sags wth dfferent ntal pnt n wave ( 0_ 270) and vltage sag duratn Fg.8. Maxmum nrush current versus dfferent vltage sag depth (h0-0.9) Ths fgure shws that vltage sag depth nfluence n maxmum nrush current s lnear.

4-2. UNSYMMETRICAL VOLTAGE SAGS All type f vltage sags are smulated and vltage sag parameters varatn nfluence n transfrmer s nrush current s studed. Effect f tw examples f vltage sag types (A 3 & E 1 ) n transfrmer s nrush current s shwn frst. Results f thers type f vltage sag effects n nrush curent are studed n the next step. ncreases. The current peas prduced when vltage recvers fr these sag types are drawn wth bren lne n Fg.12. 4-2-1. VOLTAGE SAG TYPE A 3 Fgure 9 shws nrush currents when vltage sag type A3 wth characterstcs (h0.4, t 5. 5T ) s ccured. Vltage sag has three step fr clearng. Avearge dc flux s mved frm zer value when vltage s recvered. Inrush current s prduced when saturatn s ccured t. Fg.11. Sag duratn nfluence n the current pea fr sag type B wth h0.4 Fg.9. Three phase current fr a sag type A 3 : h0.4, 5. 5T 4-2-2. VOLTAGE SAG TYPE E 1 Fgure 10 shws the transfrmer behavur under vltage sag type E 1 wth characterstcs (h0.4, t 5. 4T ). It shws a case where ne current pea s ccured when the vltage drps and anther current pea s prduced when the vltage recveres. Fg.12. Sag duratn nfluence n the current pea fr sag type E 1 and E 2 wth h0.4 Fg.10. Three phase current fr a sag type E 1 : h0.4, 5. 4T 4-2-3. VOLTAGE SAG DURATION INFLUENCE Fg.11 shws three phase current when duratn f sag type B s vared. It shws that saturatn s ccurred when nt and n1, 2,... whle n vltage sag type A n current pea was ccurred. In ppste manner f type A maxmum current pea s ccurred when nt +1/ 4. The transfrmer behavr caused by type E sags (E1 and E2) s dfferent snce sme f the current pea values n Fg.12 are prduced when vltage drps, and the remanng current pea values are prduced when vltage Fg.13. Sag duratn nfluence n the current pea fr sag type C and F 2 wth h0.4

Current pea fr type C and D (Fg 13) are prduced when vltage recvers and ther values are lwer than thse f type A sags. 4-2-2. VOLTAGE SAG DEPTH INFLUENCE Vltage sag depth nfluence n the current peas have been cnsdered. Almst a lnear nfluence can be bserved fr all sag types (Fg.14). saturatn s ccurred when t nt and maxmum current pea s prduced when t nt + T / 2. Accrdng t the smulatn results, vltage sag depth nfluence n nrush current pea s almst lnear. REFERENCES [1 Bllen, M. H. J., Styvatas, E, "Sgnatures f Vltage Dps: Transfrmer Saturatn and Multstage Dps", IEEE Transactns n Pwer Delvery, Vl.18, N.1, Jan. 2003. [2 Bllen, M. H. J., "Vltage Recvery after Unbalanced and Balanced Vltage Dps n Three-Phase System", IEEE Transactns n Pwer Delvery, Vl.18, N.4, Oct. 2003. Fg.14. Vltage sag depth nfluence n the current pea fr unsymmetrcal sag types. 5. CONCLUSION The behavur three phase three leg transfrmers under dfferent type f vltage sag s nvestgated n ths paper. Symmetrcal and unsymmetrcal vltage sags are smulated and appled t the transfrmer mdel whch was mplemented n MATLAB_SIMULINK envrnment. In rder t prduce dfferent types f vltage sag a blc s created whch taes the vltage sag parameters related t the dfferent vltage sags. Transfrmer saturatn, dc magnetc flux varatns, nrush current pea etc are studed usng varus smulatns. It s shwn that the vltage sag depth has drect rle n ncreasng the current pea when the vltage recvers. Hwever, the current pea and saturatn are hghly depended n the ntal pnt n wave durng recvery prcess. It s shwn that n [3 Bllen, M. H. J., "Understandng Pwer Qualty Prblems: Vltage Sags and Interruptns", NewYr: IEEE Press, 2000. [4 Pedra, J., Crcles, F., Sanz, L., Lpez, R., and Salchs, M.,"PSPICE Cmputer Mdel f a Nnlnear Three-Phase Three-Legged Transfrmer", IEEE Transactns n Pwer Delvery, Vlume 19, Issue: 1, Jan. 2004, pp. 200 207. [5 Pedra, J., Crcles, F., Guasch, L., "Effects f Symmetrcal Vltage Sag n Three Phase Three- Legged Transfrmers ", IEEE Transactns n Pwer Delvery, Vlume 19, N. 2, Aprl 2004, pp. 875 883. [6 Pedra, J., Crcles, F., Sanz, L.,"Symmetrcal and Unsymmetrcal Vltage Sag Effects n Three Phase Transfrmers", IEEE Transactns n Pwer Delvery, Vlume 20, N. 2, Aprl 2005, pp. 1683 1691.