Determination of the Sampling Period Required for a Fast Dynamic Response of DC-Motors

Size: px
Start display at page:

Download "Determination of the Sampling Period Required for a Fast Dynamic Response of DC-Motors"

Transcription

1 Deerminaion of he Sampling Period Required for a Fas Dynamic Response of DC-Moors J. A. GA'EB, Deparmen of Elecrical and Compuer Eng, The Hashemie Universiy, P.O.Box 15459, Posal code 13115, Zerka, JORDAN Absrac: DC moors provide a high saring orque and play a significan role in modern indusrial drives. The speed of a dc-moor is responding o he change in load orque, armaure volage and field flux. For a sudden change in applied orque, here is a change in he moor speed. This speed change goes in ransien period for some ime before seling o he new value. To keep a consan moor speed for a sudden change in applied orque, a proporional conrol of armaure volage can be used. In his work, o have an opimum and faser speed response for he orque change a sampled- daa conroller is applied. The coninuous response of he moor speed is sampled and he acion for proporional conrol of armaure volage is aken a discree manner. A proper value of sampling frequency is deermined for a saisfacory speed response of he dc- moor. The paper discussed he resuls of dynamic response for off- ime and real ime conrols. Keywords: DC-machines, Dynamic Response, Digial Conrol, Transien Response, Real- ime Conrol, Sampled- daa Conrol, Opimum Conrol, Proporional Conrol. 1 Inroducion Boh series and separaely excied dc moors are normally used in variable- speed drives [1]. Wih he help of heir variable characerisics, i is possible o obain speed conrol over a wide range. The mos flexible conrol is obained by means of a separaely excied dc moor in which he armaure and field circuis are provided wih separae sources. This arrangemen produces speed- orque characerisics approximaely close o he ideal characerisics. For armaure volage, a conrolled recifier or a chopper is required [2]. The field curren can be also conrolled by he same provisions. Conrolled recifiers provide a variable dc oupu volage form a fixed ac volage, whereas choppers can provide a variable dc oupu volage from a dc volage. In his work, he coninuous dynamic response of he dc moor for a sudden change in load orque is sampled. The speed is measured a each sampling insan and he acion for proporional conrol of armaure volage is aken a discree manner. The mehod ha was suggesed in his work for deermining he sampling period gives a faser and opimum speed response for he dc moor. 2 DC Moor-speed conrol The seady- sae speed of a dc- moor reacs o he change in load orque, armaure volage and field flux. A separaely excied moor wih consan values of armaure volage and field curren develops a speed ha is decreased as he load orque is increased. During he ransien period for a sudden change in load orque, he addiion load orque demand is me iniially by a sudden reardaion of he roaing masses which conribue o he momen of ineria of he moor shaf. Some sudies ignore he mechanical sysem ransien by considering roor speed o be consan over he shor ime, or ignoring machine field and armaure winding inducance [3]. The dc/dc converer or chopper and phase conrolled ac/dc converer are using exclusively on he conrol of he armaure volage supply [4]. The chopper is involving semiconducor swiches o chop he consan supply volage a a fairly high repeiion rae, enabling he average value of armaure volage o be variable beween zero and he supply volage. In he essenial circuis of he chopper, he consan volage source is feeding o he hyrisor swich. This hyrisor swich chops he volage source before applied o he armaure circui. As he conducing period of he hyrisor

2 swich is changed, he average value of armaure volage is varied which resul in speed conrol. 3 DC Moor- Model for Transien Operaion The equivalen circui of a separaely excied dcmoor is shown in Fig.1. The field curren is assumed consan. The conrol is applied on erminal volage (V a ) which equals: V a = R a i a L a di a / d e a vol (1) and: e a = KΦω vol (2) where: e a : armaure e.m.f (vol). Φ : flux per pole (web). ω : moor speed (r/s). The air-gap or elecromechanical orque (T e ) equals: T e = J dω /d Bω T w N.m (3) Also; T e = KΦi a N.m (4) Where: J: Ineria of boh moor and driven mechanism (kg.m 2 ). B: Viscous fricion of boh moor and driven mechanism (N.m.s/r). T w : loading orque (N.m). Transien behavior of dc moor can be analyzed by ransforming he above equaions o s- domain. By aking he Laplace ransform of (1) and afer some arrangemens becomes : τ a = L a / R a (sec), is he armaure- circui ime consan. Also by aking he Laplace ransform of (3) and (4) we ge : T e(s) - T w(s) Ω (S) = (6) B (1 τ m.s) And: T e(s) = KΦI a(s) (7) τ m = J / B (sec), is he mechanical ime consan. 4 Transien Response Wih Discree Conrol The moor- mechanism model is deermined from (5), (6) and (7) and given in Fig.2. For a sudden change in applied orque (T w ), here is a change in he moor speed. This speed akes some ime before seling o new value. To keep a consan moor speed for a sudden change in applied orque, a proporional volage conrol is added. In his work, he response ime is sampled wih sampling period of (T-sec), and he acion of proporional conrol is aken a each insan of he discree period. This discree manipulaion will show a fas speed response wih less oscillaion. Va(s) 1 R a (sτ a 1) I a (s) kφ kφ T w (s) T e (s) 1 B(sτ m 1) Ω(s) V a(s) - KΦΩ (S) I a(s) = (5) R a (1 τ a.s) V a i a R a L a e a T e T w M R f Fig.1 A separaely excied dc- moor. i f V f Fig.2 DC- moor block diagram. 4.1 Off- ime Conrol The ransien response of moor speed o an unisep change in load orque wih no conrol of armaure volage is deermined and given in Fig.3. The final value of speed is changed and seled on new low value because here is no acion of armaure conrol. The conrol of armaure volage can be acivaed using discree manner. This is done by sampling he ime response of he speed a a sampling ime

3 of T- sec and he speed change is manipulaed a each sampling insan. The manipulaion is done a off-ime, i.e. he calculaions for new acion of armaure conrol is aken a each sample. I is imporan o selec a proper value for he sampling frequency o have a saisfacory ransien response. In his paper, he ransien response of he coninuous- daa conrol sysem is invesigaed and a proper equaion is developed for he deerminaion of sampling period (T P ). This equaion is: s T P = sec (8) (Mv - F v ) * 8 Where: T s : Seling ime of he coninuous response. M v : Maximum value of he response. F v : Final value of he response. From he coninuous uni- sep response of moor speed shown in Fig.3, he opimum sampling period is deermined and given below:.2 T P = =.6 sec. ( )* 8 Speed response o an uni- sep change of load orque using discree conrol for he armaure volage wih differen values of sampling period wih no conrol of Va Fig.3 Speed response o an uni- sep change in T W is given in Fig.4. The sampling period is calculaed from (8) which equals.6 sec and is response shown in fig.4-a. For a larger sampling period of.1 sec, he moor-speed response has a large overshoo as shown in Fig.4-b. The response in Fig.4-c is for a smaller sampling period of.6 sec which has more oscillaion and caused speed perurbaion. Fas and opimum speed response is obained a he deermined sampling period T P. 4.2 Real-ime Conrol In he previous resuls, he calculaions and acion for new speed were done simulaneously. Bu pracically, he conroller needs some ime for calculaions before aking he new acion for he armaure volage. Therefore, he firs sample afer he change is lef for calculaions, and he acion of conroller is aken in he second sample. The speed response o an uni- sep change of load orque and for sampling period equals o ha one calculaed by (8) bu wih off- on conroller is shown in Fig.5. The response for a half value of he calculaed sampling period is shown in Fig.6. Resuls show ha he firs overshoo wih T=.3 sec is less han ha wih T =.6 sec bu wih more speed perurbaion. Pracically, real- ime discree conrol of he dcmoor speed is proposed in Fig.7, using a dcchopper of a consan frequency. Using he pulsewidh- modulaion mehod, he chopping period of he chopper can be defined, which is he same sampling period (T) of he digial conroller. Figure.7-b explains he way of generaing swiching signals for he chopper. The riangular carrier signal (c) has a frequency of (1/T Hz). The ampliude (p r ) of he recangular reference signal (r) depends on he signal of he dc-moor caused by he change of he loading orque. Differen load orques give differen ampliudes of (p r ). The conducion angle ( ) of he chopper is hen deermined by comparing he carrier signal ampliude (p c ) wih he reference signal ampliude (p r ). If he difference beween he carrier signal (c) and reference signal (r) becomes zero, he chopper will sop conducing and he reference signal ses o zero. Figure.8 shows he way of generaing differen conducion angles a differen signals.

4 sped error a-wih discree conrol of T=.6 sec Fig.5 Real- ime speed response wih discree conrol of V a a T=.6 sec..5 speed erroe b-wih discree conrol of T=.1 sec Ref Fig.6 Real- ime speed response wih discree conrol of V a a T=.3 sec. Digial Conroller Supply DC Chopper DC Moor Speed, ω 4 x Digial Daa Acquisiion(T) a-block diagram of Conrol Sysem for dc-moor C, r signals pc for for conrol calculaions acion reference signal carrier signal pr T 2T 3T 4T c- Wih discree conrol of T=.6 sec Fig.4 Moor-speed response o an uni- sep change of Load orque. O/P Volage of Chopper T Chopping period b-chopper Oupu Fig.7 Pracical chopper circui

5 Carrier signal pr 3 pr 2 pr Fig.8 Differen conducion angles for chopper Conrol Sysem Technology, Vol. 5, No. 1, Jan [8] H. Melkoe, F. Khorrami, S. Jain, and M. maic Robus Adapive Conrol of Variable Relucance Sepper Moors IEEE Trans. Conrol Sysem Technology, Vol. 7, No., March [9] R. J. Wai, C. M. Lin, and C. F. Hsu Hybrid Conrol for Inducion Servomoor Drive IEE Proceeding. Conrol Theory and Applicaions, Vol. 149, Issue. 6, Nov. 22. [1] S. Di Gennaro Adapive Oupu feedback Conrol of Synchronous Moors Inernaional Journal of Conrol, Vol. 73, No. 16, Nov Conclusions A sampled- daa conrol sysem is developed for a dc- moor o improve he dynamic response of moor speed for load orque changes. An opimum value of sampling period for a bes behavior of he moor speed hrough ransien response is deermined. The ransien response of moor speed o an uni- sep change in load orque is invesigaed for boh off- ime and real- ime conrol, and a pracical model for real- ime conrol is included. References: [1] S. B. Dewan, G. R. Slemon, A. Sraughen, Power Semiconducors Drives, John Wiley & Sons, [2] M. H. Rashid, Power Elecronics ; Circuis, Devices and Applicaions, Prenice- hall Inernaional, Inc, [3] C. B. Gray, Elecric Machines and Drive Sysems, Longman Group UK Limied, [4] P.C.Sen, Principles of Elecric Machines and Power Elecronics, John Wiley & sons, [5] A. G. Ulsoy, Conrol of Machining Processes, Journal of Dynamic Sysems, ASME, June [6] G. E. Escobar, P. maavelli and A. M. Sankovic, Reacive Power and Unbalanced Compensaion Using STATCOM wih Dissipaiviy- Based Conrol IEEE Trans. Conrol Sysem Technology, Vol. 9, No. 5, Sep. 21. [7] N. Rafee, T. Chen and O. P. Malik, Opimal Digial Redesign wih Applicaion o Conrol of a Single- Machine Power Sysem IEEE Trans.

Lecture -14: Chopper fed DC Drives

Lecture -14: Chopper fed DC Drives Lecure -14: Chopper fed DC Drives Chopper fed DC drives o A chopper is a saic device ha convers fixed DC inpu volage o a variable dc oupu volage direcly o A chopper is a high speed on/off semiconducor

More information

Silicon Controlled Rectifiers UNIT-1

Silicon Controlled Rectifiers UNIT-1 Silicon Conrolled Recifiers UNIT-1 Silicon Conrolled Recifier A Silicon Conrolled Recifier (or Semiconducor Conrolled Recifier) is a four layer solid sae device ha conrols curren flow The name silicon

More information

Computation of the Effect of Space Harmonics on Starting Process of Induction Motors Using TSFEM

Computation of the Effect of Space Harmonics on Starting Process of Induction Motors Using TSFEM Journal of elecrical sysems Special Issue N 01 : November 2009 pp: 48-52 Compuaion of he Effec of Space Harmonics on Saring Process of Inducion Moors Using TSFEM Youcef Ouazir USTHB Laboraoire des sysèmes

More information

Chapter 5 Digital PID control algorithm. Hesheng Wang Department of Automation,SJTU 2016,03

Chapter 5 Digital PID control algorithm. Hesheng Wang Department of Automation,SJTU 2016,03 Chaper 5 Digial PID conrol algorihm Hesheng Wang Deparmen of Auomaion,SJTU 216,3 Ouline Absrac Quasi-coninuous PID conrol algorihm Improvemen of sandard PID algorihm Choosing parameer of PID regulaor Brief

More information

Dual Current-Mode Control for Single-Switch Two-Output Switching Power Converters

Dual Current-Mode Control for Single-Switch Two-Output Switching Power Converters Dual Curren-Mode Conrol for Single-Swich Two-Oupu Swiching Power Converers S. C. Wong, C. K. Tse and K. C. Tang Deparmen of Elecronic and Informaion Engineering Hong Kong Polyechnic Universiy, Hunghom,

More information

8. Basic RL and RC Circuits

8. Basic RL and RC Circuits 8. Basic L and C Circuis This chaper deals wih he soluions of he responses of L and C circuis The analysis of C and L circuis leads o a linear differenial equaion This chaper covers he following opics

More information

Chapter 7 Response of First-order RL and RC Circuits

Chapter 7 Response of First-order RL and RC Circuits Chaper 7 Response of Firs-order RL and RC Circuis 7.- The Naural Response of RL and RC Circuis 7.3 The Sep Response of RL and RC Circuis 7.4 A General Soluion for Sep and Naural Responses 7.5 Sequenial

More information

RC, RL and RLC circuits

RC, RL and RLC circuits Name Dae Time o Complee h m Parner Course/ Secion / Grade RC, RL and RLC circuis Inroducion In his experimen we will invesigae he behavior of circuis conaining combinaions of resisors, capaciors, and inducors.

More information

Module 4: Time Response of discrete time systems Lecture Note 2

Module 4: Time Response of discrete time systems Lecture Note 2 Module 4: Time Response of discree ime sysems Lecure Noe 2 1 Prooype second order sysem The sudy of a second order sysem is imporan because many higher order sysem can be approimaed by a second order model

More information

Speed Control of Brushless DC Motor Using Proportional Integral Controller

Speed Control of Brushless DC Motor Using Proportional Integral Controller www.ijrase.com Volume 3 Issue XII, December 2015 Inernaional Journal for Research in Applied Science & Engineering Speed Conrol of Brushless DC Moor Using Proporional Inegral Conroller Vikramarajan Jambulingam

More information

Principle and Analysis of a Novel Linear Synchronous Motor with Half-Wave Rectified Self Excitation

Principle and Analysis of a Novel Linear Synchronous Motor with Half-Wave Rectified Self Excitation Principle and Analysis of a Novel Linear Synchronous Moor wih Half-Wave Recified Self Exciaion Jun OYAMA, Tsuyoshi HIGUCHI, Takashi ABE, Shoaro KUBOTA and Tadashi HIRAYAMA Deparmen of Elecrical and Elecronic

More information

L1, L2, N1 N2. + Vout. C out. Figure 2.1.1: Flyback converter

L1, L2, N1 N2. + Vout. C out. Figure 2.1.1: Flyback converter page 11 Flyback converer The Flyback converer belongs o he primary swiched converer family, which means here is isolaion beween in and oupu. Flyback converers are used in nearly all mains supplied elecronic

More information

Comparative study between two models of a linear oscillating tubular motor

Comparative study between two models of a linear oscillating tubular motor IOSR Journal of Elecrical and Elecronics Engineering (IOSR-JEEE) e-issn: 78-676,p-ISSN: 3-333, Volume 9, Issue Ver. IV (Feb. 4), PP 77-83 Comparaive sudy beween wo models of a linear oscillaing ubular

More information

Dynamic Effects of Feedback Control!

Dynamic Effects of Feedback Control! Dynamic Effecs of Feedback Conrol! Rober Sengel! Roboics and Inelligen Sysems MAE 345, Princeon Universiy, 2017 Inner, Middle, and Ouer Feedback Conrol Loops Sep Response of Linear, Time- Invarian (LTI)

More information

ECE 2100 Circuit Analysis

ECE 2100 Circuit Analysis ECE 1 Circui Analysis Lesson 35 Chaper 8: Second Order Circuis Daniel M. Liynski, Ph.D. ECE 1 Circui Analysis Lesson 3-34 Chaper 7: Firs Order Circuis (Naural response RC & RL circuis, Singulariy funcions,

More information

Lab 10: RC, RL, and RLC Circuits

Lab 10: RC, RL, and RLC Circuits Lab 10: RC, RL, and RLC Circuis In his experimen, we will invesigae he behavior of circuis conaining combinaions of resisors, capaciors, and inducors. We will sudy he way volages and currens change in

More information

First Order RC and RL Transient Circuits

First Order RC and RL Transient Circuits Firs Order R and RL Transien ircuis Objecives To inroduce he ransiens phenomena. To analyze sep and naural responses of firs order R circuis. To analyze sep and naural responses of firs order RL circuis.

More information

R.#W.#Erickson# Department#of#Electrical,#Computer,#and#Energy#Engineering# University#of#Colorado,#Boulder#

R.#W.#Erickson# Department#of#Electrical,#Computer,#and#Energy#Engineering# University#of#Colorado,#Boulder# .#W.#Erickson# Deparmen#of#Elecrical,#Compuer,#and#Energy#Engineering# Universiy#of#Colorado,#Boulder# Chaper 2 Principles of Seady-Sae Converer Analysis 2.1. Inroducion 2.2. Inducor vol-second balance,

More information

Università degli Studi di Roma Tor Vergata Dipartimento di Ingegneria Elettronica. Analogue Electronics. Paolo Colantonio A.A.

Università degli Studi di Roma Tor Vergata Dipartimento di Ingegneria Elettronica. Analogue Electronics. Paolo Colantonio A.A. Universià degli Sudi di Roma Tor Vergaa Diparimeno di Ingegneria Eleronica Analogue Elecronics Paolo Colanonio A.A. 2015-16 Diode circui analysis The non linearbehaviorofdiodesmakesanalysisdifficul consider

More information

dv 7. Voltage-current relationship can be obtained by integrating both sides of i = C :

dv 7. Voltage-current relationship can be obtained by integrating both sides of i = C : EECE202 NETWORK ANALYSIS I Dr. Charles J. Kim Class Noe 22: Capaciors, Inducors, and Op Amp Circuis A. Capaciors. A capacior is a passive elemen designed o sored energy in is elecric field. 2. A capacior

More information

i L = VT L (16.34) 918a i D v OUT i L v C V - S 1 FIGURE A switched power supply circuit with diode and a switch.

i L = VT L (16.34) 918a i D v OUT i L v C V - S 1 FIGURE A switched power supply circuit with diode and a switch. 16.4.3 A SWITHED POWER SUPPY USINGA DIODE In his example, we will analyze he behavior of he diodebased swiched power supply circui shown in Figure 16.15. Noice ha his circui is similar o ha in Figure 12.41,

More information

Inductor Energy Storage

Inductor Energy Storage School of Compuer Science and Elecrical Engineering 5/5/ nducor Energy Sorage Boh capaciors and inducors are energy sorage devices They do no dissipae energy like a resisor, bu sore and reurn i o he circui

More information

2.4 Cuk converter example

2.4 Cuk converter example 2.4 Cuk converer example C 1 Cuk converer, wih ideal swich i 1 i v 1 2 1 2 C 2 v 2 Cuk converer: pracical realizaion using MOSFET and diode C 1 i 1 i v 1 2 Q 1 D 1 C 2 v 2 28 Analysis sraegy This converer

More information

EE100 Lab 3 Experiment Guide: RC Circuits

EE100 Lab 3 Experiment Guide: RC Circuits I. Inroducion EE100 Lab 3 Experimen Guide: A. apaciors A capacior is a passive elecronic componen ha sores energy in he form of an elecrosaic field. The uni of capaciance is he farad (coulomb/vol). Pracical

More information

Basic Circuit Elements Professor J R Lucas November 2001

Basic Circuit Elements Professor J R Lucas November 2001 Basic Circui Elemens - J ucas An elecrical circui is an inerconnecion of circui elemens. These circui elemens can be caegorised ino wo ypes, namely acive and passive elemens. Some Definiions/explanaions

More information

Embedded Systems and Software. A Simple Introduction to Embedded Control Systems (PID Control)

Embedded Systems and Software. A Simple Introduction to Embedded Control Systems (PID Control) Embedded Sysems and Sofware A Simple Inroducion o Embedded Conrol Sysems (PID Conrol) Embedded Sysems and Sofware, ECE:3360. The Universiy of Iowa, 2016 Slide 1 Acknowledgemens The maerial in his lecure

More information

ES 250 Practice Final Exam

ES 250 Practice Final Exam ES 50 Pracice Final Exam. Given ha v 8 V, a Deermine he values of v o : 0 Ω, v o. V 0 Firs, v o 8. V 0 + 0 Nex, 8 40 40 0 40 0 400 400 ib i 0 40 + 40 + 40 40 40 + + ( ) 480 + 5 + 40 + 8 400 400( 0) 000

More information

Chapter 2: Principles of steady-state converter analysis

Chapter 2: Principles of steady-state converter analysis Chaper 2 Principles of Seady-Sae Converer Analysis 2.1. Inroducion 2.2. Inducor vol-second balance, capacior charge balance, and he small ripple approximaion 2.3. Boos converer example 2.4. Cuk converer

More information

Chapter 8 The Complete Response of RL and RC Circuits

Chapter 8 The Complete Response of RL and RC Circuits Chaper 8 The Complee Response of RL and RC Circuis Seoul Naional Universiy Deparmen of Elecrical and Compuer Engineering Wha is Firs Order Circuis? Circuis ha conain only one inducor or only one capacior

More information

Voltage/current relationship Stored Energy. RL / RC circuits Steady State / Transient response Natural / Step response

Voltage/current relationship Stored Energy. RL / RC circuits Steady State / Transient response Natural / Step response Review Capaciors/Inducors Volage/curren relaionship Sored Energy s Order Circuis RL / RC circuis Seady Sae / Transien response Naural / Sep response EE4 Summer 5: Lecure 5 Insrucor: Ocavian Florescu Lecure

More information

V AK (t) I T (t) I TRM. V AK( full area) (t) t t 1 Axial turn-on. Switching losses for Phase Control and Bi- Directionally Controlled Thyristors

V AK (t) I T (t) I TRM. V AK( full area) (t) t t 1 Axial turn-on. Switching losses for Phase Control and Bi- Directionally Controlled Thyristors Applicaion Noe Swiching losses for Phase Conrol and Bi- Direcionally Conrolled Thyrisors V AK () I T () Causing W on I TRM V AK( full area) () 1 Axial urn-on Plasma spread 2 Swiching losses for Phase Conrol

More information

( ) ( ) if t = t. It must satisfy the identity. So, bulkiness of the unit impulse (hyper)function is equal to 1. The defining characteristic is

( ) ( ) if t = t. It must satisfy the identity. So, bulkiness of the unit impulse (hyper)function is equal to 1. The defining characteristic is UNIT IMPULSE RESPONSE, UNIT STEP RESPONSE, STABILITY. Uni impulse funcion (Dirac dela funcion, dela funcion) rigorously defined is no sricly a funcion, bu disribuion (or measure), precise reamen requires

More information

CHAPTER 6: FIRST-ORDER CIRCUITS

CHAPTER 6: FIRST-ORDER CIRCUITS EEE5: CI CUI T THEOY CHAPTE 6: FIST-ODE CICUITS 6. Inroducion This chaper considers L and C circuis. Applying he Kirshoff s law o C and L circuis produces differenial equaions. The differenial equaions

More information

CHAPTER 12 DIRECT CURRENT CIRCUITS

CHAPTER 12 DIRECT CURRENT CIRCUITS CHAPTER 12 DIRECT CURRENT CIUITS DIRECT CURRENT CIUITS 257 12.1 RESISTORS IN SERIES AND IN PARALLEL When wo resisors are conneced ogeher as shown in Figure 12.1 we said ha hey are conneced in series. As

More information

INVERSE RESPONSE COMPENSATION BY ESTIMATING PARAMETERS OF A PROCESS COMPRISING OF TWO FIRST ORDER SYSTEMS

INVERSE RESPONSE COMPENSATION BY ESTIMATING PARAMETERS OF A PROCESS COMPRISING OF TWO FIRST ORDER SYSTEMS Inernaional Journal of Informaion Technology and nowledge Managemen July-December 0, Volume 5, No., pp. 433-438 INVERSE RESPONSE COMPENSATION BY ESTIMATING PARAMETERS OF A PROCESS COMPRISING OF TWO FIRST

More information

ECE 2100 Circuit Analysis

ECE 2100 Circuit Analysis ECE 1 Circui Analysis Lesson 37 Chaper 8: Second Order Circuis Discuss Exam Daniel M. Liynski, Ph.D. Exam CH 1-4: On Exam 1; Basis for work CH 5: Operaional Amplifiers CH 6: Capaciors and Inducor CH 7-8:

More information

Dead-time Induced Oscillations in Inverter-fed Induction Motor Drives

Dead-time Induced Oscillations in Inverter-fed Induction Motor Drives Dead-ime Induced Oscillaions in Inverer-fed Inducion Moor Drives Anirudh Guha Advisor: Prof G. Narayanan Power Elecronics Group Dep of Elecrical Engineering, Indian Insiue of Science, Bangalore, India

More information

STATE-SPACE MODELLING. A mass balance across the tank gives:

STATE-SPACE MODELLING. A mass balance across the tank gives: B. Lennox and N.F. Thornhill, 9, Sae Space Modelling, IChemE Process Managemen and Conrol Subjec Group Newsleer STE-SPACE MODELLING Inroducion: Over he pas decade or so here has been an ever increasing

More information

A FAMILY OF THREE-LEVEL DC-DC CONVERTERS

A FAMILY OF THREE-LEVEL DC-DC CONVERTERS A FAMIY OF THREE-EVE DC-DC CONVERTERS Anonio José Beno Boion, Ivo Barbi Federal Universiy of Sana Caarina - UFSC, Power Elecronics Insiue - INEP PO box 5119, ZIP code 88040-970, Florianópolis, SC, BRAZI

More information

Hall effect. Formulae :- 1) Hall coefficient RH = cm / Coulumb. 2) Magnetic induction BY 2

Hall effect. Formulae :- 1) Hall coefficient RH = cm / Coulumb. 2) Magnetic induction BY 2 Page of 6 all effec Aim :- ) To deermine he all coefficien (R ) ) To measure he unknown magneic field (B ) and o compare i wih ha measured by he Gaussmeer (B ). Apparaus :- ) Gauss meer wih probe ) Elecromagne

More information

Electrical and current self-induction

Electrical and current self-induction Elecrical and curren self-inducion F. F. Mende hp://fmnauka.narod.ru/works.hml mende_fedor@mail.ru Absrac The aricle considers he self-inducance of reacive elemens. Elecrical self-inducion To he laws of

More information

DEPARTMENT OF ELECTRICAL AND ELECTRONIC ENGINEERING EXAMINATIONS 2008

DEPARTMENT OF ELECTRICAL AND ELECTRONIC ENGINEERING EXAMINATIONS 2008 [E5] IMPERIAL COLLEGE LONDON DEPARTMENT OF ELECTRICAL AND ELECTRONIC ENGINEERING EXAMINATIONS 008 EEE/ISE PART II MEng BEng and ACGI SIGNALS AND LINEAR SYSTEMS Time allowed: :00 hours There are FOUR quesions

More information

Homework-8(1) P8.3-1, 3, 8, 10, 17, 21, 24, 28,29 P8.4-1, 2, 5

Homework-8(1) P8.3-1, 3, 8, 10, 17, 21, 24, 28,29 P8.4-1, 2, 5 Homework-8() P8.3-, 3, 8, 0, 7, 2, 24, 28,29 P8.4-, 2, 5 Secion 8.3: The Response of a Firs Order Circui o a Consan Inpu P 8.3- The circui shown in Figure P 8.3- is a seady sae before he swich closes a

More information

Reading from Young & Freedman: For this topic, read sections 25.4 & 25.5, the introduction to chapter 26 and sections 26.1 to 26.2 & 26.4.

Reading from Young & Freedman: For this topic, read sections 25.4 & 25.5, the introduction to chapter 26 and sections 26.1 to 26.2 & 26.4. PHY1 Elecriciy Topic 7 (Lecures 1 & 11) Elecric Circuis n his opic, we will cover: 1) Elecromoive Force (EMF) ) Series and parallel resisor combinaions 3) Kirchhoff s rules for circuis 4) Time dependence

More information

Chapter 10 INDUCTANCE Recommended Problems:

Chapter 10 INDUCTANCE Recommended Problems: Chaper 0 NDUCTANCE Recommended Problems: 3,5,7,9,5,6,7,8,9,,,3,6,7,9,3,35,47,48,5,5,69, 7,7. Self nducance Consider he circui shown in he Figure. When he swich is closed, he curren, and so he magneic field,

More information

Electrical Circuits. 1. Circuit Laws. Tools Used in Lab 13 Series Circuits Damped Vibrations: Energy Van der Pol Circuit

Electrical Circuits. 1. Circuit Laws. Tools Used in Lab 13 Series Circuits Damped Vibrations: Energy Van der Pol Circuit V() R L C 513 Elecrical Circuis Tools Used in Lab 13 Series Circuis Damped Vibraions: Energy Van der Pol Circui A series circui wih an inducor, resisor, and capacior can be represened by Lq + Rq + 1, a

More information

Sub Module 2.6. Measurement of transient temperature

Sub Module 2.6. Measurement of transient temperature Mechanical Measuremens Prof. S.P.Venkaeshan Sub Module 2.6 Measuremen of ransien emperaure Many processes of engineering relevance involve variaions wih respec o ime. The sysem properies like emperaure,

More information

Application Note AN Software release of SemiSel version 3.1. New semiconductor available. Temperature ripple at low inverter output frequencies

Application Note AN Software release of SemiSel version 3.1. New semiconductor available. Temperature ripple at low inverter output frequencies Applicaion Noe AN-8004 Revision: Issue Dae: Prepared by: 00 2008-05-21 Dr. Arend Winrich Ke y Words: SemiSel, Semiconducor Selecion, Loss Calculaion Sofware release of SemiSel version 3.1 New semiconducor

More information

Non Linear Op Amp Circuits.

Non Linear Op Amp Circuits. Non Linear Op Amp ircuis. omparaors wih 0 and non zero reference volage. omparaors wih hyseresis. The Schmid Trigger. Window comparaors. The inegraor. Waveform conversion. Sine o ecangular. ecangular o

More information

d 1 = c 1 b 2 - b 1 c 2 d 2 = c 1 b 3 - b 1 c 3

d 1 = c 1 b 2 - b 1 c 2 d 2 = c 1 b 3 - b 1 c 3 and d = c b - b c c d = c b - b c c This process is coninued unil he nh row has been compleed. The complee array of coefficiens is riangular. Noe ha in developing he array an enire row may be divided or

More information

Speed Control of BLDC Motor by Using Tuned Linear Quadratic Regulator

Speed Control of BLDC Motor by Using Tuned Linear Quadratic Regulator Inernaional Journal of Scienific Engineering and Research (IJSER) ISSN (Online): 347-3878, Impac Facor (4): 3.5 Speed Conrol of BLDC Moor by Using uned Linear Quadraic Regulaor Vishnu C.S., Riya Mary Francis

More information

Time Domain Transfer Function of the Induction Motor

Time Domain Transfer Function of the Induction Motor Sudies in Engineering and Technology Vol., No. ; Augus 0 ISSN 008 EISSN 006 Published by Redfame Publishing URL: hp://se.redfame.com Time Domain Transfer Funcion of he Inducion Moor N N arsoum Correspondence:

More information

Problem Set #1. i z. the complex propagation constant. For the characteristic impedance:

Problem Set #1. i z. the complex propagation constant. For the characteristic impedance: Problem Se # Problem : a) Using phasor noaion, calculae he volage and curren waves on a ransmission line by solving he wave equaion Assume ha R, L,, G are all non-zero and independen of frequency From

More information

CHANGE IN THE RESISTANCE OF THE SEMICONDUCTOR IN THE VARIABLE DEFORMATION FIELD

CHANGE IN THE RESISTANCE OF THE SEMICONDUCTOR IN THE VARIABLE DEFORMATION FIELD CHANGE IN THE RESISTANCE OF THE SEMICONDUCTOR IN THE VARIABLE DEFORMATION FIELD M. AHMETOGLU (AFRAILOV) 1, G. GULYAMOV 2, S. H. SHAMIRZAEV 2, A. G. GULYAMOV 2, M. G. DADAMIRZAEV 2, N. APRAILOV 2, F. KOÇAK

More information

Optimal Control of Dc Motor Using Performance Index of Energy

Optimal Control of Dc Motor Using Performance Index of Energy American Journal of Engineering esearch AJE 06 American Journal of Engineering esearch AJE e-issn: 30-0847 p-issn : 30-0936 Volume-5, Issue-, pp-57-6 www.ajer.org esearch Paper Open Access Opimal Conrol

More information

EEEB113 CIRCUIT ANALYSIS I

EEEB113 CIRCUIT ANALYSIS I 9/14/29 1 EEEB113 CICUIT ANALYSIS I Chaper 7 Firs-Order Circuis Maerials from Fundamenals of Elecric Circuis 4e, Alexander Sadiku, McGraw-Hill Companies, Inc. 2 Firs-Order Circuis -Chaper 7 7.2 The Source-Free

More information

2.9 Modeling: Electric Circuits

2.9 Modeling: Electric Circuits SE. 2.9 Modeling: Elecric ircuis 93 2.9 Modeling: Elecric ircuis Designing good models is a ask he compuer canno do. Hence seing up models has become an imporan ask in modern applied mahemaics. The bes

More information

Join discussion of this test paper at Q.1 Q.30 carry one mark each. = + is: Z 2 i 1 i 2

Join discussion of this test paper at   Q.1 Q.30 carry one mark each. = + is: Z 2 i 1 i 2 GATE EE - 005 Q. Q.0 carry one mark each.. In Fig.Q, he value of R is.5ω 8A R 5.0Ω (c) 7.5Ω (d) 0.0Ω 00V 0Ω 0Ω. The RMS value of he volage u ( ) 4cos ( ) = is: 5V (c) 7V 7V (d) ( ) V Z i i ν Z ν. For he

More information

The problem with linear regulators

The problem with linear regulators he problem wih linear regulaors i in P in = i in V REF R a i ref i q i C v CE P o = i o i B ie P = v i o o in R 1 R 2 i o i f η = P o P in iref is small ( 0). iq (quiescen curren) is small (probably).

More information

Simulation-Solving Dynamic Models ABE 5646 Week 2, Spring 2010

Simulation-Solving Dynamic Models ABE 5646 Week 2, Spring 2010 Simulaion-Solving Dynamic Models ABE 5646 Week 2, Spring 2010 Week Descripion Reading Maerial 2 Compuer Simulaion of Dynamic Models Finie Difference, coninuous saes, discree ime Simple Mehods Euler Trapezoid

More information

Sliding Mode Controller for Unstable Systems

Sliding Mode Controller for Unstable Systems S. SIVARAMAKRISHNAN e al., Sliding Mode Conroller for Unsable Sysems, Chem. Biochem. Eng. Q. 22 (1) 41 47 (28) 41 Sliding Mode Conroller for Unsable Sysems S. Sivaramakrishnan, A. K. Tangirala, and M.

More information

University of Cyprus Biomedical Imaging and Applied Optics. Appendix. DC Circuits Capacitors and Inductors AC Circuits Operational Amplifiers

University of Cyprus Biomedical Imaging and Applied Optics. Appendix. DC Circuits Capacitors and Inductors AC Circuits Operational Amplifiers Universiy of Cyprus Biomedical Imaging and Applied Opics Appendix DC Circuis Capaciors and Inducors AC Circuis Operaional Amplifiers Circui Elemens An elecrical circui consiss of circui elemens such as

More information

Chapter 4 DC converter and DC switch

Chapter 4 DC converter and DC switch haper 4 D converer and D swich 4.1 Applicaion - Assumpion Applicaion: D swich: Replace mechanic swiches D converer: in racion drives Assumions: Ideal D sources Ideal Power emiconducor Devices 4.2 D swich

More information

(b) (a) (d) (c) (e) Figure 10-N1. (f) Solution:

(b) (a) (d) (c) (e) Figure 10-N1. (f) Solution: Example: The inpu o each of he circuis shown in Figure 10-N1 is he volage source volage. The oupu of each circui is he curren i( ). Deermine he oupu of each of he circuis. (a) (b) (c) (d) (e) Figure 10-N1

More information

04. Kinetics of a second order reaction

04. Kinetics of a second order reaction 4. Kineics of a second order reacion Imporan conceps Reacion rae, reacion exen, reacion rae equaion, order of a reacion, firs-order reacions, second-order reacions, differenial and inegraed rae laws, Arrhenius

More information

Modeling the Dynamics of an Ice Tank Carriage

Modeling the Dynamics of an Ice Tank Carriage Modeling he Dynamics of an Ice Tank Carriage The challenge: To model he dynamics of an Ice Tank Carriage and idenify a mechanism o alleviae he backlash inheren in he design of he gearbox. Maplesof, a division

More information

Some Basic Information about M-S-D Systems

Some Basic Information about M-S-D Systems Some Basic Informaion abou M-S-D Sysems 1 Inroducion We wan o give some summary of he facs concerning unforced (homogeneous) and forced (non-homogeneous) models for linear oscillaors governed by second-order,

More information

Mechanical Fatigue and Load-Induced Aging of Loudspeaker Suspension. Wolfgang Klippel,

Mechanical Fatigue and Load-Induced Aging of Loudspeaker Suspension. Wolfgang Klippel, Mechanical Faigue and Load-Induced Aging of Loudspeaker Suspension Wolfgang Klippel, Insiue of Acousics and Speech Communicaion Dresden Universiy of Technology presened a he ALMA Symposium 2012, Las Vegas

More information

8.022 (E&M) Lecture 16

8.022 (E&M) Lecture 16 8. (E&M) ecure 16 Topics: Inducors in circuis circuis circuis circuis as ime Our second lecure on elecromagneic inducance 3 ways of creaing emf using Faraday s law: hange area of circui S() hange angle

More information

IE1206 Embedded Electronics

IE1206 Embedded Electronics E06 Embedded Elecronics Le Le3 Le4 Le Ex Ex P-block Documenaion, Seriecom Pulse sensors,, R, P, serial and parallel K LAB Pulse sensors, Menu program Sar of programing ask Kirchhoffs laws Node analysis

More information

Phys1112: DC and RC circuits

Phys1112: DC and RC circuits Name: Group Members: Dae: TA s Name: Phys1112: DC and RC circuis Objecives: 1. To undersand curren and volage characerisics of a DC RC discharging circui. 2. To undersand he effec of he RC ime consan.

More information

Laplace Transforms. Examples. Is this equation differential? y 2 2y + 1 = 0, y 2 2y + 1 = 0, (y ) 2 2y + 1 = cos x,

Laplace Transforms. Examples. Is this equation differential? y 2 2y + 1 = 0, y 2 2y + 1 = 0, (y ) 2 2y + 1 = cos x, Laplace Transforms Definiion. An ordinary differenial equaion is an equaion ha conains one or several derivaives of an unknown funcion which we call y and which we wan o deermine from he equaion. The equaion

More information

V(z, t) t < L v. z = 0 z = vt z = L. I(z, t) z = L

V(z, t) t < L v. z = 0 z = vt z = L. I(z, t) z = L W.C.Chew ECE 35 Lecure Noes 12. Transiens on a Transmission Line. When we do no have a ime harmonic signal on a ransmission line, we have o use ransien analysis o undersand he waves on a ransmission line.

More information

Basic Principles of Sinusoidal Oscillators

Basic Principles of Sinusoidal Oscillators Basic Principles of Sinusoidal Oscillaors Linear oscillaor Linear region of circui : linear oscillaion Nonlinear region of circui : ampliudes sabilizaion Barkhausen crierion X S Amplifier A X O X f Frequency-selecive

More information

LAPLACE TRANSFORM AND TRANSFER FUNCTION

LAPLACE TRANSFORM AND TRANSFER FUNCTION CHBE320 LECTURE V LAPLACE TRANSFORM AND TRANSFER FUNCTION Professor Dae Ryook Yang Spring 2018 Dep. of Chemical and Biological Engineering 5-1 Road Map of he Lecure V Laplace Transform and Transfer funcions

More information

EECE251. Circuit Analysis I. Set 4: Capacitors, Inductors, and First-Order Linear Circuits

EECE251. Circuit Analysis I. Set 4: Capacitors, Inductors, and First-Order Linear Circuits EEE25 ircui Analysis I Se 4: apaciors, Inducors, and Firs-Order inear ircuis Shahriar Mirabbasi Deparmen of Elecrical and ompuer Engineering Universiy of Briish olumbia shahriar@ece.ubc.ca Overview Passive

More information

On the Analysis and Optimal Control Design of BLDC Drives

On the Analysis and Optimal Control Design of BLDC Drives Inernaional Journal of Elecrical Engineering. ISSN 974-58 Volume 6, Number 5 (), pp.59-5 Inernaional Research ublicaionhouse hp://www.irphouse.com On he Analysis and Opimal Conrol Design of BLDC Drives

More information

INDEX. Transient analysis 1 Initial Conditions 1

INDEX. Transient analysis 1 Initial Conditions 1 INDEX Secion Page Transien analysis 1 Iniial Condiions 1 Please inform me of your opinion of he relaive emphasis of he review maerial by simply making commens on his page and sending i o me a: Frank Mera

More information

non-linear oscillators

non-linear oscillators non-linear oscillaors The invering comparaor operaion can be summarized as When he inpu is low, he oupu is high. When he inpu is high, he oupu is low. R b V REF R a and are given by he expressions derived

More information

Detection of Tire Lateral Force Based on a Resolver Mechanism

Detection of Tire Lateral Force Based on a Resolver Mechanism 4 Special Issue Esimaion and Conrol of Vehicle Dynamics for Acive Safey Research Repor Deecion of Tire Laeral Force Based on a Resolver Mechanism Takaji Umeno To observe he fricional sae of a ire and improve

More information

di Bernardo, M. (1995). A purely adaptive controller to synchronize and control chaotic systems.

di Bernardo, M. (1995). A purely adaptive controller to synchronize and control chaotic systems. di ernardo, M. (995). A purely adapive conroller o synchronize and conrol chaoic sysems. hps://doi.org/.6/375-96(96)8-x Early version, also known as pre-prin Link o published version (if available):.6/375-96(96)8-x

More information

Converter - Brake - Inverter Module (CBI2)

Converter - Brake - Inverter Module (CBI2) Converer - Brake - Inverer Module (CBI2) 21 22 D11 D13 D15 1 2 3 7 D7 16 15 T1 D1 T3 D3 T5 D5 18 6 17 5 19 4 D12 D14 D16 T7 T2 D2 T4 D4 T6 D6 23 14 24 11 12 13 NTC 8 9 Three Phase Brake Chopper Three Phase

More information

Analysis and design of a high-efficiency zero-voltage-switching step-up DC DC converter

Analysis and design of a high-efficiency zero-voltage-switching step-up DC DC converter Sādhanā Vol. 38, Par 4, Augus 2013, pp. 653 665. c Indian Academy of Sciences Analysis and design of a high-efficiency zero-volage-swiching sep-up DC DC converer JAE-WON YANG and HYUN-LARK DO Deparmen

More information

UNIT- III DC CHOPPERS

UNIT- III DC CHOPPERS UN- D HPPES NDUN A chopper is a saic device which is used o obain a variable dc volage from a consan dc volage source. A chopper is also known as dc-o-dc converer. he hyrisor converer offers greaer efficiency,

More information

Advanced Power Electronics For Automotive and Utility Applications

Advanced Power Electronics For Automotive and Utility Applications Advanced Power Elecronics For Auomoive and Uiliy Applicaions Fang Z. Peng Dep. of Elecrical and Compuer Engineering Michigan Sae Universiy Phone: 517-336-4687, Fax: 517-353-1980 Email: fzpeng@egr.msu.edu

More information

Module 10 SCR. 2. To understand two Transistor Static and Transient Models. 3. To learn the SCR Turn-on and Turn-off methods

Module 10 SCR. 2. To understand two Transistor Static and Transient Models. 3. To learn the SCR Turn-on and Turn-off methods 1 Module 1 SR 1. Inroducion 2. SR characerisics 3. Two ransisor saic and ransien models 4. SR urnon mehods 5. SR urnoff mehods 6. SR proecion and Triggering circuis 7. ae proecion circuis 8. Summary Learning

More information

I. Define the Situation

I. Define the Situation I. efine he Siuaion This exam explores he relaionship beween he applied volage o a permanen magne C moond he linear velociy (speed) of he elecric vehicle (EV) he moor drives. The moor oupu is fed ino a

More information

Designing Information Devices and Systems I Spring 2019 Lecture Notes Note 17

Designing Information Devices and Systems I Spring 2019 Lecture Notes Note 17 EES 16A Designing Informaion Devices and Sysems I Spring 019 Lecure Noes Noe 17 17.1 apaciive ouchscreen In he las noe, we saw ha a capacior consiss of wo pieces on conducive maerial separaed by a nonconducive

More information

Active Harmonic Filtering and Reactive Power Control

Active Harmonic Filtering and Reactive Power Control Session 3, Page /34 Acive Harmonic Filering and Reacive Power Conrol Imiaion Measured Currens: Define array of ime and define angular frequency: Δ Δ.3 4 s 86Hz 6 secδ ω 6Hz π6hz ω() ω Load curren as a

More information

Analysis of a PM DC Motor Model for Application in Feedback Design for Electric Powered Mobility Vehicles

Analysis of a PM DC Motor Model for Application in Feedback Design for Electric Powered Mobility Vehicles Analysis of a PM DC Moor Model for Applicaion in Feedback Design for Elecric Powered Mobiliy Vehicles P. Wolm 1, X.Q. Chen 1, J.G. Chase 1, W. Peigrew 2, C.E. Hann 1 1 Deparmen of Mechanical Engineering,

More information

V L. DT s D T s t. Figure 1: Buck-boost converter: inductor current i(t) in the continuous conduction mode.

V L. DT s D T s t. Figure 1: Buck-boost converter: inductor current i(t) in the continuous conduction mode. ECE 445 Analysis and Design of Power Elecronic Circuis Problem Se 7 Soluions Problem PS7.1 Erickson, Problem 5.1 Soluion (a) Firs, recall he operaion of he buck-boos converer in he coninuous conducion

More information

Converter - Brake - Inverter Module (CBI2)

Converter - Brake - Inverter Module (CBI2) Converer - Brake - Inverer Module (CBI2) 21 22 D11 D13 D1 1 2 3 7 D7 16 1 T1 D1 T3 D3 T D 18 2 6 17 19 4 D12 D14 D16 T7 T2 D2 T4 D4 T6 D6 23 14 24 11 1 12 13 NTC 8 9 Three Phase Brake Chopper Three Phase

More information

Problemas das Aulas Práticas

Problemas das Aulas Práticas Mesrado Inegrado em Engenharia Elecroécnica e de Compuadores Conrolo em Espaço de Esados Problemas das Aulas Práicas J. Miranda Lemos Fevereiro de 3 Translaed o English by José Gaspar, 6 J. M. Lemos, IST

More information

Converter - Brake - Inverter Module (CBI2)

Converter - Brake - Inverter Module (CBI2) MUBW 5-6 7 Converer - Brake - Inverer Module (CBI2) 2 22 D D3 D5 2 3 7 D7 6 5 T D T3 D3 T5 D5 8 2 6 7 5 9 4 D2 D4 D6 T7 T2 D2 T4 D4 T6 D6 23 4 24 2 3 NTC 8 9 Three Phase Brake Chopper Three Phase Recifier

More information

Physical Limitations of Logic Gates Week 10a

Physical Limitations of Logic Gates Week 10a Physical Limiaions of Logic Gaes Week 10a In a compuer we ll have circuis of logic gaes o perform specific funcions Compuer Daapah: Boolean algebraic funcions using binary variables Symbolic represenaion

More information

Linear Time-invariant systems, Convolution, and Cross-correlation

Linear Time-invariant systems, Convolution, and Cross-correlation Linear Time-invarian sysems, Convoluion, and Cross-correlaion (1) Linear Time-invarian (LTI) sysem A sysem akes in an inpu funcion and reurns an oupu funcion. x() T y() Inpu Sysem Oupu y() = T[x()] An

More information

6.2 Transforms of Derivatives and Integrals.

6.2 Transforms of Derivatives and Integrals. SEC. 6.2 Transforms of Derivaives and Inegrals. ODEs 2 3 33 39 23. Change of scale. If l( f ()) F(s) and c is any 33 45 APPLICATION OF s-shifting posiive consan, show ha l( f (c)) F(s>c)>c (Hin: In Probs.

More information

Controlled Switching Based on the Injection Method

Controlled Switching Based on the Injection Method Conrolled Swiching Based on he Injecion Mehod C.D. Tsirekis, N.D. Haziargyriou, B.C. Papadias Elecric Energy Sysems Laboraory Deparmen of Elecrical and Compuer Engineering Naional Technical Universiy of

More information

Chapter 5: Discontinuous conduction mode. Introduction to Discontinuous Conduction Mode (DCM)

Chapter 5: Discontinuous conduction mode. Introduction to Discontinuous Conduction Mode (DCM) haper 5. The isconinuous onducion Mode 5.. Origin of he disconinuous conducion mode, and mode boundary 5.. Analysis of he conversion raio M(,K) 5.3. Boos converer example 5.4. Summary of resuls and key

More information

An Adaptive Control of Static Var Compensator on Power Systems

An Adaptive Control of Static Var Compensator on Power Systems An Adapive Conrol of Saic Var Compensaor on Power Sysems N.F.DJAGAROV Zh.G.GROZDEV M.B.BONEV G.D.GEORGIEV Elecrical Deparmen Technical Universiy, Sudenska sr, Varna BULGARIA Absrac: The sysem means of

More information