RBSK/EEE/PE 8/21/2015 SNS COLLEGE OF ENGINEERING SNS KALVI NAGAR, SATHY MAIN ROAD, COIMBATORE – 641 107 DEPARTMENT OF ELECTRICAL AND ELECTRONICS ENGINEERING THYRISTOR EE 6503 POWER ELECTRONICS Mr.R.B.SELVAKUMAR CHOPPERS ASSISTANT PROFESSOR DEPARTMENT OF ELECTRICAL AND ELECTRONICS ENGINEERING SNS COLLEGE OF ENGINEERING, COIMBATORE rbsk.snsce@gmail.com Mobile : 9942483127 8/21/2015 RBSK/SNSCE/EEE/PE 1 8/21/2015 RBSK/SNSCE/EEE/PE 2 THYRISTOR CHOPPER CIRCUITS THYRISTOR CHOPPER CIRCUITS • SCR IS USED AS SWITCH FOR HIGH • SCR IS USED AS SWITCH FOR HIGH POWER LEVEL POWER LEVEL • SEPARATE COMMUTATION CIRCUIT IS • SEPARATE COMMUTATION CIRCUIT IS ESSENTIAL ESSENTIAL • COMMUTATION – PROCESS OF TURNING- • COMMUTATION ? OFF, A CONDUCTING THYRISTOR 8/21/2015 RBSK/SNSCE/EEE/PE 3 8/21/2015 RBSK/SNSCE/EEE/PE 4 1 RBSK/EEE/PE 8/21/2015 THYRISTOR CHOPPER CIRCUITS TURNING-OFF A THYRISTOR • SCR IS USED AS SWITCH FOR HIGH • REDUCING IA < IH POWER LEVEL • APPLYING REVERSE VOLTAGE ACROSS IT • SEPARATE COMMUTATION CIRCUIT IS • SO, IT REGAIN ITS FORWARD BLOKING ESSENTIAL CAPABILITY • COMMUTATION – PROCESS OF TURNINGOFF, A CONDUCTING THYRISTOR • HOW TO TURN-OFF A THYRISTOR? 8/21/2015 RBSK/SNSCE/EEE/PE 5 CLASSIFICATION OF COMMUTATION 8/21/2015 RBSK/SNSCE/EEE/PE 6 1. FORCED COMMUTATION • External Elements L & C are used 1. FORCED COMMUTATION • Achieved in two ways a) Voltage Commutation a) Voltage Commutation b) Current Commutation - Application of pulse of large reverse voltage 2. LOAD COMMUTATION - Applied by previously charged capacitor - Reduces IA to zero 8/21/2015 RBSK/SNSCE/EEE/PE 7 8/21/2015 RBSK/SNSCE/EEE/PE 8 2 RBSK/EEE/PE 8/21/2015 1. FORCED COMMUTATION 2. LOAD COMMUTATION b) Current Commutation - Application of pulse of current > load current IL in reverse direction - When pulse current = IL ; IA reduces to zero - Diode is connected in antiparallel with main SCR - Voltage drop across diode reverse biases SCR - Commutation time is greater than in Voltage commutation 8/21/2015 RBSK/SNSCE/EEE/PE 9 THYRISTOR CHOPPER CIRCUITS • Achieved by either a) The IL = 0 due to the nature of load circuit parameters b) IL is transferred to another device from conducting SCR 8/21/2015 RBSK/SNSCE/EEE/PE 10 VOLTAGE COMMUTATED CHOPPER • Used in high power circuits where load • VOLTAGE COMMUTATED CHOPPER fluctuation is not large • CURRENT COMMUTATED CHOPPER • Other names • LOAD COMMUTATED CHOPPER Parallel-capacitor turn-off chopper Impulse-commutated chopper Classical chopper 8/21/2015 RBSK/SNSCE/EEE/PE 11 8/21/2015 RBSK/SNSCE/EEE/PE 12 3 RBSK/EEE/PE 8/21/2015 TYPE –A CHOPPER TYPE –A CHOPPER MAIN POWER SWITCH 8/21/2015 RBSK/SNSCE/EEE/PE 13 8/21/2015 RBSK/SNSCE/EEE/PE TYPE –A CHOPPER TYPE –A CHOPPER CAPACITOR AUXILIARY THYRISTOR 8/21/2015 RBSK/SNSCE/EEE/PE 14 15 8/21/2015 RBSK/SNSCE/EEE/PE 16 4 RBSK/EEE/PE 8/21/2015 TYPE –A CHOPPER TYPE –A CHOPPER DIODE 8/21/2015 INDUCTOR RBSK/SNSCE/EEE/PE 17 8/21/2015 RBSK/SNSCE/EEE/PE TYPE –A CHOPPER TYPE –A CHOPPER RLE LOAD FREE WHEELING DIODE 8/21/2015 RBSK/SNSCE/EEE/PE 18 19 8/21/2015 RBSK/SNSCE/EEE/PE 20 5 RBSK/EEE/PE 8/21/2015 WORKING HOW TO CHARGE C? • Working of this chopper starts only if the C charged with marked polarities WAY - 1 • Close Switch S • How to achieve this? • So C charged to VS through VS ,C,S & RC CHARGING RESISTOR 8/21/2015 RBSK/SNSCE/EEE/PE 21 8/21/2015 RBSK/SNSCE/EEE/PE 22 HOW TO CHARGE C? WAY - 2 • Auxiliary Thyristor TA is Now Chopper is ready for operation with marked polarities as positive triggered • C gets charged through VS ,C,TA & load • Charging current through C decays & as it reaches zero, vc = VS ; TA turned-off 8/21/2015 RBSK/SNSCE/EEE/PE 23 8/21/2015 RBSK/SNSCE/EEE/PE 24 6 RBSK/EEE/PE 8/21/2015 MODE - I ASSUMPTIONS T1 Triggered at t = 0 Two currents it1= ic + io Commutation Current • Load Current is Constant • Thyristor and Diodes are Ideal Load Current 8/21/2015 RBSK/SNSCE/EEE/PE 25 8/21/2015 RBSK/SNSCE/EEE/PE 26 MODE - II MODE -I • ic changes sinusoidally • vc changes cosinusoidally • vTA changes cosinusoidally Main SCR T1 only conducting • At t = t1 • ic = 0 • it1= io • vc = -VS • vTA = VS • vo = VS 8/21/2015 RBSK/SNSCE/EEE/PE 27 8/21/2015 RBSK/SNSCE/EEE/PE 28 7 RBSK/EEE/PE 8/21/2015 MODE - III To turn off T1, TA is Triggered at t = t2 MODE -II For t1 < t < t2 ic = 0 it1= io vc = -VS vTA = VS vo = VS id = 0 8/21/2015 RBSK/SNSCE/EEE/PE Commutation Current Load Current 29 8/21/2015 RBSK/SNSCE/EEE/PE vc = -VS appears across T1 Reverse Biases it it1= 0 vo = VS + vc = 2 VS 30 MODE - IV MODE – III At t = t3 ic = 0 iTA= 0 vc = vT1 = VS vo = 0 For t2 < t < t3 C discharges through load vc & VT1 Changes linearly from –VS to zero at t2 + tc vo starts falling towards zero ic = -io iTA = io TA turned-off naturally 8/21/2015 RBSK/SNSCE/EEE/PE 31 8/21/2015 RBSK/SNSCE/EEE/PE 32 8 RBSK/EEE/PE 8/21/2015 MODE – IV DISADVANTAGES For t3 < t < T • A starting circuit is required FD forward biased Load current free wheels ic = 0 iT1 = 0 ifd = io iTA = 0 vT1 = VS 8/21/2015 RBSK/SNSCE/EEE/PE • At the instant of commutation vo = 2 VS , so FD is subjected to twice the supply voltage • It can’t work at no load 33 8/21/2015 RBSK/SNSCE/EEE/PE 34 CURRENT COMMUTATED CHOPPER ASSUMPTIONS TYPE –A CHOPPER • Load Current is Constant • Thyristor and Diodes are Ideal • RC is so large, treated as open circuit during the commutation interval 8/21/2015 RBSK/SNSCE/EEE/PE 35 8/21/2015 RBSK/SNSCE/EEE/PE 36 9 RBSK/EEE/PE 8/21/2015 FOR 0 < t < t1 WORKING • Working of this chopper starts only if the C charged with marked polarities • vo = VS • The energy for current commutation comes from capacitor 8/21/2015 RBSK/SNSCE/EEE/PE • T1 fired at t = 0 • io = IO 37 8/21/2015 RBSK/SNSCE/EEE/PE MODE - I 38 MODE -I To turn off T1, TA Triggered at t = t1 • T1 remains uneffected • Ic & vc varies sinusoidally ic = (Vs / woL) Sin wo t • vo = VS • io = IO OSCILATTORY CURRENT 8/21/2015 RBSK/SNSCE/EEE/PE 39 8/21/2015 RBSK/SNSCE/EEE/PE 40 10 RBSK/EEE/PE 8/21/2015 MODE - II MODE - II For t2 < t < t3 TA turned-off at t2 8/21/2015 EXCESS CURRENT RBSK/SNSCE/EEE/PE TA turned-off at t2 Oscillatory current flow through T1 At t3, iT1 = 0 ; T1 turned-off 41 8/21/2015 RBSK/SNSCE/EEE/PE MODE - III 42 MODE -III Ic > Io D1 Conducts Ic is at its peak value 8/21/2015 RBSK/SNSCE/EEE/PE 43 8/21/2015 RBSK/SNSCE/EEE/PE 44 11 RBSK/EEE/PE 8/21/2015 MODE - IV MODE - V Ic = Io , D1 off FD forward biased Load current free wheels During the time 8/21/2015 RBSK/SNSCE/EEE/PE 45 8/21/2015 RBSK/SNSCE/EEE/PE 46 LOAD COMMUTATED CHOPPER MERITS TYPE –A CHOPPER • Commutation is reliable • Capacitor is always charged with correct polarity • TA is naturally commutated 8/21/2015 RBSK/SNSCE/EEE/PE 47 8/21/2015 RBSK/SNSCE/EEE/PE 48 12 RBSK/EEE/PE 8/21/2015 THYRISTORS – T1 to T4 CAPACITOR 8/21/2015 RBSK/SNSCE/EEE/PE 49 8/21/2015 RBSK/SNSCE/EEE/PE 50 FREE WHEELING DIODE • If T1,T2 – Main Thyristors, then T3,T4 & C forms commutating elements • If T3,T4 – Main Thyristors , then T1,T2 & C forms commutating elements 8/21/2015 RBSK/SNSCE/EEE/PE 51 8/21/2015 RBSK/SNSCE/EEE/PE 52 13 RBSK/EEE/PE 8/21/2015 ASSUMPTIONS WORKING • Working of this chopper starts only if the C charged with marked polarities • Load Current is Constant • Thyristor and Diodes are Ideal 8/21/2015 RBSK/SNSCE/EEE/PE 53 8/21/2015 RBSK/SNSCE/EEE/PE 54 MODE - I vc charges from VS to -VS At t = 0 T1, T2 Triggered T3,T4 Reverse biased vT3 = vT4 = - VS vo = VS + Vc = 2 VS 8/21/2015 RBSK/SNSCE/EEE/PE 55 Load voltage falls to zero. At t = t1 T3,T4 Forward biased vT3 = vT4 = VS 8/21/2015 RBSK/SNSCE/EEE/PE 56 14 RBSK/EEE/PE 8/21/2015 MODE - II During (t2-t1) vc = -VS vo = 0 ic = 0 ifd = io iT1 = iT2 = 0 vT3 = vT4 = VS vT1 = vT2 = -ΔVS At t = t1 C slightly overcharged by ΔVS FD Forward biased Load current Freewheels 8/21/2015 RBSK/SNSCE/EEE/PE 57 8/21/2015 RBSK/SNSCE/EEE/PE 58 MODE - III During (t3-t2) vc = VS ic = -io iT3 = iT4 = io At t = t3 vT1 = vT2 = VS T1,T2 Forward biased At t = t2 T3, T4 Triggered T1,T2 Reverse biased & turned-off vo = VS + Vc = 2 VS Capacitor charges to VS vT1 = vT2 = -VS 8/21/2015 RBSK/SNSCE/EEE/PE 59 8/21/2015 RBSK/SNSCE/EEE/PE 60 15 RBSK/EEE/PE 8/21/2015 MERITS After t3 FD Forward biased • Capable of commutating any amount of load Load current Freewheels upto t4 current • No commutating inductor is required At t = t4 T1,T2 Triggered Mode I repeats 8/21/2015 RBSK/SNSCE/EEE/PE • As it can work in high frequencies (KHz), Filtering requirements are minimal 61 8/21/2015 RBSK/SNSCE/EEE/PE 62 DEMERITS • Peak load voltage is twice the supply voltage • For high power applications – higher switching losses at high operating frequencies – efficiency may low • FD is subjected to twice the supply voltage • Capacitor current which is alternating to be sensed to turn on one pair of SCRs when the other pair is commutated 8/21/2015 RBSK/SNSCE/EEE/PE 63 16