CAS 2004 – 4Q Power Converters Technologies Switched Mode Converters (4 Quadrants) Yves THUREL CERN CAS2004 / Warrington / 12-18 May 2004 Y. Thurel 1 / xx CAS 2004 – 4Q Power Converters Technologies 4 Quadrant basic background 4Q. Conventions 4Q. Working area / loads 4Q. Basic schematics 4 Quadrant topologies Review Principle schematics (main ones presented) Advantages / Drawbacks Some realizations 4 Quadrant practical realization & example LHC Specifications LHC Topology choice explained LHC Converter principles Technical points highlighted (loops, circulating current,…) Realizations CAS2004 / Warrington / 12-18 May 2004 Y. Thurel 2 / xx CAS 2004 – 4Q Power Converters Technologies 4 Quadrant basic background 4Q. Conventions 4Q. Working area / loads 4Q. Basic schematics 4 Quadrant topologies Review Principle schematics (main ones presented) Advantages / Drawbacks Some realizations 4 Quadrant practical realization & example LHC Specifications LHC Topology choice explained LHC Converter principles Technical points highlighted (loops, circulating current,…) Realizations CAS2004 / Warrington / 12-18 May 2004 Y. Thurel 3 / xx 4Q. Conventions CAS 2004 – 4Q Power Converters Technologies 4 Quadrant Operation: Definition (applied to R-L circuit) 1 Quadrant mode + I [A] V [V] 0 20 40 60 80 2 Quadrant mode + - + 100 I [A] V [V] 0 20 40 60 80 100 V 4 1 3 2 Control of the decreasing current is still possible within drastic conditions and limits. (RCIRCUIT acts as discharger.) Current is controlled (being always in the same sense), when increasing or decreasing. 4 Quadrant mode + - + CAS2004 / Warrington / 12-18 May 2004 I [A] V [V] 0 20 40 Y. Thurel 60 80 100 II No theoretical operation limitation. 4 / xx 4Q. Work. Area CAS 2004 – 4Q Power Converters Technologies 4 Quadrant Operation: Loads Typical Cycle (R-L) PGENE-PEAK VCIRCUIT=R.I+L.dI/dt dI/dtLOW 800 [A] CIRCUIT LCIRCUIT (CABLE) LCIRCUIT (MAGNET) I [A] 600 400 200 dI/dt MAX 0 -200 0 200 400 600 800 [t]1000 L = 1H R = 7mOhms dI/dtMAX= 5A.s-1 IMAX = 600A -400 -600 -800 10 8 4QAREA PRECEP-PEAK [V] V [V] 6 L.dI/dt 4 2 0 -2 0 200 400 600 800 [t] 1000 KEY FEATURES L.dI/dt = 5V R.IMAX = 4.2V VMAX = 9.2V -4 -6 -8 -10 CAS2004 / Warrington / 12-18 May 2004 Y. Thurel 5 / xx 4Q. Work. Area CAS 2004 – 4Q Power Converters Technologies 4 Quadrant Operation: Load Influence on topology “Pulsed” Machine [V] [A] Cycle Period High Power to be absorbed / Often Î High Energy “Slow” Machine: LHC Type / Magnet or orbit Correctors 12h or more run Power to be absorbed / sometimes Î Low Energy CAS2004 / Warrington / 12-18 May 2004 Y. Thurel [V] [A] Operation close to 0V / 0A 6 / xx 4 Quadrant Operation: Load Impact on cost & design parameters Circuit Characteristics Circuit Key Features • L = 1H LHC Machine • dI/dt = 10A.s-1 LHC Machine • I = [-600A;+600A] LHC Machine • PCable < 15kW LHC Tunnel •L•di/dt = 10V •10mOhms < Rcable < 21mOhms 6V < Rcable•IMAX < 12V 20 mOhms 10 mOhms (V: Output Voltage Power converter) (P: Output power Power converter) 30 30 13.2 kW [V] 22 VMAX 20 [V] 9.6 kW 20 16 VMAX 10 10 I[A] I[A] 0 0 -800 -600 -400 -200 0 200 400 600 800 -800 -600 -400 -200 -20 -1.25kW 0 200 V [V] P [kW] -30 -20 600 800 -2.5kW V [V] P [kW] -30 PMAX 13.2kW 100% PMAX 9.6kW 73% PABSORBED 1.25kW 100% PABSORBED 2.5kW 200% Cable Losses 14.4kW 100% Cable Losses 7.2kW 50% CAS2004 / Warrington / 12-18 May 2004 400 -10 -10 Y. Thurel Î Price 4Q. Work. Area CAS 2004 – 4Q Power Converters Technologies Ï Ò 7 / xx 4Q. Conventions CAS 2004 – 4Q Power Converters Technologies 4 Quadrant Operation: Receptor mode Goals: • Absorbing magnet energy No Resistance [V] [A] I [A] V [V] 600 Energy Receptor Concepts 8 6 400 4 200 2 0 0 • Still regulating magnet reverse voltage, i.e dI/dt •Solutions: Ideal Magnet 800 -200 0 50 100 150 -2 -400 -4 -600 -6 -800 -8 • Variable resistor (active) • Voltage source added for 0 A transition: No voltage can be obtained when 0 Amp in the magnet. V I>0 • Converter magnet-mains, giving back energy to mains. • Converter magnet-capacitor, storing the magnet energy. V>0 • This capacitor is charged by the magnet and the needed generator converter •Alternative (not very used) solutions could be: rotative machine, or (supraconductor) inductor…not treated here. CAS2004 / Warrington / 12-18 May 2004 Y. Thurel 8 / xx 4Q. Basics Sch. CAS 2004 – 4Q Power Converters Technologies 4 Q Stage: Main topologies 2x Thyristor bridge in anti// Very well known Power returned to mains Bip. / Mos. Transistor Linear dissipative Stage Basic background known, (push-pull stage) 4Q operation to be explained later Dissipation in the transistors, acting as programmable resistor LL RL Switching Stage Conventional H bridge (L-C Filter) Power returned to capacitor or dissipated in brake chopper. CAS2004 / Warrington / 12-18 May 2004 Y. Thurel 9 / xx 4Q. Basics Sch. CAS 2004 – 4Q Power Converters Technologies (* The 2 voltages are always the same) 4Q Stage: Linear basic principle …Combined with double* DC fixed voltage output 0A..100A 100A 12V 2V 10V 12V LL RL 0A 12V 10V 2V 0.. 100A 22V 100..0A 12V LL RL 0A Efficiency!!! 10V 100A 12V 20V -8V 100A 14V 0A 12V LL RL 20V 12V -8V 100A ..0A 0A 20Vx100A in Q1!!! 4V 0.. -100A LL RL 12V 4V 0A..100A 100A 0A 0A 2V GENERATOR CAS2004 / Warrington / 12-18 May 2004 Y. Thurel -100A -8V -8V RECEPTOR GENERATOR 10 / xx 4Q. Basics Sch. CAS 2004 – 4Q Power Converters Technologies (* The 2 voltages are always the same) 4Q Stage: Linear basic principle …combined with double* DC variable voltage output for better efficiency an losses reduced in receptor mode 0A..100A 100A 12V 2V 10V 12V LL RL 0A 4V 2V 2V 0.. 100A 22V 100..0A 4V 6V 0A Efficiency better 10V 100A 0V 8V -8V 100A LL RL 0A 0V LL RL 0A 8Vx100A in Q1 10V 14V -8V 100A ..0A -8V 0.. -100A LL RL 10V 2V 0A..100A 100A 0A 0A 2V GENERATOR CAS2004 / Warrington / 12-18 May 2004 Y. Thurel -100A -8V -8V RECEPTOR GENERATOR 11 / xx 4Q. Basics Sch. CAS 2004 – 4Q Power Converters Technologies 4Q Stage: Linear basic principle (variation “linear” H bridge) …combined with single DC variable voltage output VE+ VE+ VL LL RL VL VE IL LL RL IL Remark: This solution is easier, from the inverter side, but leads to polarity new transitions which can be source of distortion, and finally lead to a complex 4 quadrant stage CAS2004 / Warrington / 12-18 May 2004 Y. Thurel Polarity Switches Single output inverter 12 / xx 4Q. Basics Sch. CAS 2004 – 4Q Power Converters Technologies 4Q Stage: Switching basic principle H Bridge: 2 modes T1 VE It is possible to work in Buck Mode so that both IL T3 VL Vs - ∆ I is reduced (HF output voltage ripple) - Losses are reduced T2 T4 T1=T4=T2=T3 T VE α 1-α Note: transition between these 2 possible modes can be source of distortions. VMEAN IMEAN VMEAN=(2.α-1).VE -VE CAS2004 / Warrington / 12-18 May 2004 Y. Thurel 13 / xx CAS 2004 – 4Q Power Converters Technologies 4 Quadrant basic background 4Q. Conventions 4Q. Working area / loads 4Q. Basic schematics 4 Quadrant topologies Review Principle schematics (main ones presented) Advantages / Drawbacks Some realizations 4 Quadrant practical realization & example LHC Specifications LHC Topology choice explained LHC Converter principles Technical points highlighted (loops, circulating current,…) Realizations CAS2004 / Warrington / 12-18 May 2004 Y. Thurel 14 / xx CAS 2004 – 4Q Power Converters Technologies Topologies: Key points, (how to classify them, how to select them?) SIZE, SIZE,WEIGHT, WEIGHT, COST COST POWER POWERRANGE, RANGE, DISSIPATIVE DISSIPATIVEOR ORNOT, NOT, EFFICIENCY EFFICIENCY AC ACMAINS MAINSPERT. PERT.REJ., REJ., EMC, BF & HF RIPPLE EMC, BF & HF RIPPLE TOPOLOGY CHOICE ???? NUMBER NUMBEROF OFCPTS, CPTS,DESIGN DESIGN COMPLEXITY, MTBF, COMPLEXITY, MTBF,USE USEOF OF COMMERCIAL PART COMMERCIAL PART DISTORTION DISTORTION BANDWIDTH BANDWIDTH CAS2004 / Warrington / 12-18 May 2004 Y. Thurel 15 / xx CAS 2004 – 4Q Power Converters Technologies Mains Rectifier bridge 4Q. AC-DC Converter Filter Filter DC-AC Converter 4Q. DC-AC Converter LF Transfo. (Volt. Adapt.) HF Transfo. (Volt. Adapt.) 4Q. Thyristor bridge Rectifier bridge Filter Filter 4Q. Linear Stage Storage Energy or B. Chopper 4Q. AC-DC Converter 4Q. DC-DC H Bridge Filter Filter Load CAS2004 / Warrington / 12-18 May 2004 Y. Thurel 16 / xx CAS 2004 – 4Q Power Converters Technologies Topologies: Thyristor (Principle) V V 1 4 I 3 2 I I I I LF Thyristor bridge Thyristor bridge I ILOAD VLOAD 50 Hz transfo. Optimal voltage output (Galvanic Isolation) LF LF LF Low freq. Output Filter CAS2004 / Warrington / 12-18 May 2004 Y. Thurel 17 / xx CAS 2004 – 4Q Power Converters Technologies Topologies: Thyristor (schematics Example) Basic schematic • [0,0] & [V] axis required circulating current between the 2 bridges . . 7.5m B6C 7.5m 2.16m Rmag . . 540u 4.7 . . alpha-refcircu 7.5m . . . . . . 2.16m 540u Lmag 4.7 7.5m B6C • Active Filter increase dynamic performance (low amplitude bandwidth, low frequency ripple, perturbation…) Adding a circulating current between the 2 thyristor bridges helps!!! CAS2004 / Warrington / 12-18 May 2004 Y. Thurel 18 / xx CAS 2004 – 4Q Power Converters Technologies Topologies: Thyristor (Discussion) Advantages • Huge power possible • Not Dissipative: power returned to mains • High Efficiency • Very well known topology • Rather simple design • No High frequency signal (low frequency operation): EMC easy to handle Drawbacks • Low Bandwidth (addition of active filter can help a bit in small signal) • Poor AC mains perturbation rejection (speed loop limited by L-C filter) • Distortion (crossing axes, and point [0,0]) requires some additional circuit for high precision converter: Circulating current • Size, weight of transformer and filtering elements CAS2004 / Warrington / 12-18 May 2004 Y. Thurel 19 / xx CAS 2004 – 4Q Power Converters Technologies Topologies: 50Hz + Linear (Principle) DC Fixed LF LF ILOAD VLOAD LF L I N E A R DC Fixed LF 50 Hz transfo. Optimal voltage output (Galvanic Isolation) CAS2004 / Warrington / 12-18 May 2004 LF Rectifier + Double Output High Freq. Filter Y. Thurel Linear Stage (Dissipate Magnet Energy) 20 / xx CAS 2004 – 4Q Power Converters Technologies Topologies: 50Hz + Linear (Principle variation) LF 50 Hz transfo. Optimal voltage output (Galvanic Isolation) LF Diode bridge C H A . LF Low freq. Output Filter L I N E A R ILOAD VLOAD DC Fixed P O L . H Bridge Linear Stage (Polarity Changer / Dissipate Magnet Energy) CAS2004 / Warrington / 12-18 May 2004 Y. Thurel 21 / xx CAS 2004 – 4Q Power Converters Technologies Topologies: 50Hz + Linear (Discussion) Advantages • Schematics and topologies are very well known • Simple schematics • Adding circulation current helps • Bandwidth (10 kHz) Drawbacks • Dissipative • Efficiency very low in generator mode • Size, weight of transformer and filtering elements • Often realized with several transistors in // (MTBF and avalanche failure) CAS2004 / Warrington / 12-18 May 2004 Y. Thurel 22 / xx CAS 2004 – 4Q Power Converters Technologies Topologies: 50Hz + Switching (Principle) ILOAD LF LF Diode 50 Hz transfo. Optimal voltage bridge output (Galvanic Isolation) VLOAD DC Fixed LF HF Add. Low freq. PWM Brake Chopper Output Filter Converter (Optional) (Magnet Energy Hard Î1/2.C.V²) (Dissipate Magnet Commutation CAS2004 / Warrington / 12-18 May 2004 HF High freq. Output Filter Energy) Y. Thurel 23 / xx CAS 2004 – 4Q Power Converters Technologies Topologies: 50Hz + Switching (Schematics Example) Basic schematic High Frequency Hard commutation Bridge 50Hz Transfo + L –C Filter Commercial part possible Brake chopper: absorb magnet energy if Vcap. too high CAS2004 / Warrington / 12-18 May 2004 Y. Thurel High Frequency LC Filter (2 cells) 24 / xx CAS 2004 – 4Q Power Converters Technologies Topologies: 50Hz + Switching (Discussion) ±150A ±200V Advantages • Huge power possible • Part of magnet energy re-used • Very well known topology– possible to use commercial standard elements • High bandwidth (10 kHz) • Good AC mains perturbation rejection • No distortion of the signal (if H bridge not changing mode) Drawbacks • H bridge hard commutation @ high current • 50Hz LC-Filter can be un-damped by H bridge negative equivalent resistor • Size, weight of transformer and filtering elements • Hard commutation EMC to cope with • Low voltage high current not ideal (loss of the switching H bridge, fswitching limited) • HF filtering Ripple difficult (if buck mode not used), at “only fswitching” CAS2004 / Warrington / 12-18 May 2004 Y. Thurel 25 / xx CAS 2004 – 4Q Power Converters Technologies Topologies: Switching + Linear (Principle) LF 3Ph Diode Bridge LF Low freq. Output Filter HF HF High Freq. Soft Commutation Inverter CAS2004 / Warrington / 12-18 May 2004 HF HF HF HF High Freq. Transfo. Rectifier + Double Output High Freq. Filter Y. Thurel ILOAD VLOAD HF L I N E A R Linear Stage 26 / xx CAS 2004 – 4Q Power Converters Technologies Topologies: Switching + Linear (Principle variation) LF LF 3Ph Diode Bridge Low freq. Output Filter HF HF High Freq. Soft Commutation Inverter CAS2004 / Warrington / 12-18 May 2004 HF High Freq. Transfo. HF HF Rectifier + Single Output High Freq. Filter Y. Thurel ILOAD VLOAD P O L L I . N E C A H R A . H Bridge Linear Stage (Polarity Changer) 27 / xx CAS 2004 – 4Q Power Converters Technologies Topologies: Switching + Linear (Schematics Example) Basic schematic Input Module, Bd: 70Hz Phase shifted Inverter Rectifer + Filter 4 Quadrant Linear Stage VOUT EMI FILTER HF Transfo. 300Hz L –C Filter High Frequency Soft commutation H Bridge CAS2004 / Warrington / 12-18 May 2004 Y. Thurel 4Q Linear Stage HF Filter + Rectifier 28 / xx CAS 2004 – 4Q Power Converters Technologies Topologies: Switching + Linear (Discussion) Advantages • Medium power possible • Addition of 2 distinct well known topologies • High bandwidth • Good AC mains perturbation rejection • No distortion of the signal (if circulating current used) • HF filtering Ripple at 2x fswitching possible • Efficiency OK, (no switching Loss at secondary side) • EMC OK, since Soft commutation possible Drawbacks • Dealing with Inverter Loop & Circulation current Loop can lead to some complexity • Double output voltage requires additional power components (L-C Filtering + Rectifiers) • Dissipative (No energy back to anywhere, except Output transistors!!!) CAS2004 / Warrington / 12-18 May 2004 Y. Thurel 29 / xx CAS 2004 – 4Q Power Converters Technologies Topologies: Switching + Switching Type 1 (Principle) VLOAD ILOAD LF LF HF 50 Hz transformer Optimal voltage output Galvanic isolation CAS2004 / Warrington / 12-18 May 2004 HF Diode bridge HF HF Low freq. Output Filter Y. Thurel HF HF HF PWM Converter Add. Crowbar Hard Commutation 30 / xx CAS 2004 – 4Q Power Converters Technologies Topologies: Switching + Switching Type 1 (Discussion) Advantages • High power possible • Part of magnet energy re-used • Very well known topology • High bandwidth • Good AC mains perturbation rejection • No distortion of the signal (if H bridge not changing mode) Drawbacks • Secondary H bridge hard commutation @ high current (Losses EMC to cope with ) • Low voltage high current not ideal (loss of the switching H bridge, fswitching limited) • 2 HF filtering levels • Complexity (2 inverters, Gate drives) & Cost • Efficiency low • HF filtering Ripple difficult (if buck mode not used), at “only fswitching” CAS2004 / Warrington / 12-18 May 2004 Y. Thurel 31 / xx CAS 2004 – 4Q Power Converters Technologies Topologies: Switching + Switching Type 2 (Principle) LF LF LF VLOAD ILOAD LF LF Diode Low freq. Add. bridge Output Filter Crowbar CAS2004 / Warrington / 12-18 May 2004 HF HF High Freq. Soft Commutation Inverter Y. Thurel HF HF HF HF 4Q Converter High Freq. Soft Commutation Transfo. 32 / xx CAS 2004 – 4Q Power Converters Technologies Topologies: Switching + Switching Type 2 (Schematic Example) θr’ γ Vdc + TH1 on Vin TD1 TD3 off off • TD2 TD4 off off Vdc - IL See Paper from CERN & LEEI for detailed explanation. TH3 Iout • LOAD • on θr TH3 on TH4 on TH2 TH1 •……. Out - TH2 •…… •…… TH4 Out + THbis3 Iout1 iout2 THbis1 THbis2 THbis4 CAS2004 / Warrington / 12-18 May 2004 Y. Thurel 33 / xx CAS 2004 – 4Q Power Converters Technologies Topologies: Switching + Switching Type 2 (Discussion) Advantages • Fully reversible with energy sent back to mains (thyristor bridge to be added) • High frequency power converter (low volume and high dynamic performance) • High bandwidth • Good AC mains perturbation rejection • No distortion of the signal (if H bridge not changing mode) • Soft commutation possible on the 2 H-Bridges • High efficiency Drawbacks ±600A ±12V • Complex control CAS2004 / Warrington / 12-18 May 2004 Y. Thurel 34 / xx CAS 2004 – 4Q Power Converters Technologies 4 Quadrant basic background 4Q. Conventions 4Q. Working area / loads 4Q. Basic schematics 4 Quadrant topologies Review Principle schematics (main ones presented) Advantages / Drawbacks Some realizations 4 Quadrant practical realization & example LHC Specifications LHC Topology choice explained LHC Converter principles Technical points highlighted (loops, circulating current,…) Realizations CAS2004 / Warrington / 12-18 May 2004 Y. Thurel 35 / xx CAS 2004 – 4Q Power Converters Technologies LHC: Specifications • Electrical Characteristics – – – – – – • Mechanical Characteristics – – – • To be installed in LHC tunnel Must be possible to change it as a plug-in module Low volume and low weight Electrical Environment – – – – • Low Output Voltage / High Output Current High Efficiency (Losses in Tunnel must be as low as possible) High bandwidth No need for returning power to mains (slow machine) Operation close to [0V-0A] Low BF ripple (magnet current precision) & Low HF Ripple (EMC) Good immunity to mains perturbation (phase loss of 100ms) Very low level of distortion tolerated (high precision) EMC behavior must be very good (IN & OUT) To be integrated in a few ppm current loop regulation Other key points – – 15 years of operation (MTBF) Principle as simple as possible (operation) CAS2004 / Warrington / 12-18 May 2004 Y. Thurel LHC Power Converters Family LHC ±600A ±40V Transtechnik Germany LHC ±600A ±10V Cirtem France LHC ±120A ±10V CERN & EFACEC Portugal LHC ±60A ±08V CERN & CEL France 36 / xx CAS 2004 – 4Q Power Converters Technologies LHC ±120A ±10V: EMC Highlighted Magnet loads are several magnets in series (hundreds of meters “load”) IEC478.3 C applied INPUT and OUTPUT side 400V ac Iref r Vref +- Vout L RST B LHC Electronic : (control + DCCTS) Power converter Iout Circuit Digital & Analog signals exchanged between Power converter & High Precision Current Controller CAS2004 / Warrington / 12-18 May 2004 Y. Thurel 37 / xx CAS 2004 – 4Q Power Converters Technologies LHC ±120A ±10V Topology Choice Minimum 50Hz Components for size & weight reduction (tunnel installation) EMC Switching based topology Linear base topology High precision environment: EMC must be as good as possible No distortion / operation [0V-0A] CAS2004 / Warrington / 12-18 May 2004 Y. Thurel 38 / xx CAS 2004 – 4Q Power Converters Technologies LHC ±120A ±10V Topology Choice Input Module, Bd: 70Hz Phase shifted Inverter Rectifer + Filter 4 Quadrant Linear Stage VOUT EMI FILTER BREAKER & INPUT FILTER & SOFT COM. INVERTER, ISOLATION & CONTACTOR SOFT-START 50kHz..100kHz RECTIFIER + FILTER CAS2004 / Warrington / 12-18 May 2004 Y. Thurel 4Q.L.S. 39 / xx CAS 2004 – 4Q Power Converters Technologies LHC ±120A ±10V Topology Choice AC-DC • 3 phases + Neutral (used for auxiliary power supply) • 1400V Rectifiers • 70Hz Input filter (damped with C-4C) to give a flat 540V DC (around -20dB on 300Hz) • Soft start based on “R + switch”. High Frequency Soft commutation Inverter • • • • • Fixed switching frequency (50..100kHz). ZVS operation with Phase Shifted command. ZCS for lagging leg IGBT Bridge “Voltage” or “current” mode possible CAS2004 / Warrington / 12-18 May 2004 Y. Thurel 40 / xx CAS 2004 – 4Q Power Converters Technologies LHC ±120A ±10V Topology Choice Rectifer + Filter Rectifier + DC Filter • HF Ripple at 2x inverter Fswitching • Schottky rectifiers. • Double LC cell at 5..10 kHz. 4 Quadrant Linear Stage • Linear Regulation based on Mosfets. • Mosfet used as - polarity switch in generator mode - programmable resistor to dissipate Magnet energy. • Use of 4QLS as an active filter • Use of 4QLS to pre-load inverter (continuous mode) • Circulating current always present but value depending from load current (no mode change transition, both DCDC outputs always minimum loaded CAS2004 / Warrington / 12-18 May 2004 Y. Thurel 4 Quadrant Linear Stage VOUT 41 / xx CAS 2004 – 4Q Power Converters Technologies IHIGH LHC ±120A ±10V Topology Choice Highlights on 4QLS VE • A double power source programmable via inverter (VE) • 2 MOSFETS, Q1 & Q2, used as switch and programmable resistor. (high level of power possible) • A command which works according to : VGS HIGH VOUT IOUT LL RL VE VGS LOW ILOW VOUT = +(VE − R HIGH ⋅ I HIGH ) VOUT = −(VE − R LOW ⋅ I LOW ) RHIGH & RLOW are equivalent MOSFET resistance CAS2004 / Warrington / 12-18 May 2004 Y. Thurel 42 / xx CAS 2004 – 4Q Power Converters Technologies LHC: 4QLS without circulation current • Remember a limitation of the linear stage… • Main Loop (VOUT linear regulation loop) cannot provide needed step for biasing MOSFET (-3V to + 3V) • Playing with fixed bias is a bad idea!!! Discrepancies on VGS ON ±1V !!! LHC ±120A ±10V Measurements IHIGH VE VGS HIGH VDS HIGH VOUT IOUT LL Without Circulating Current RL VE VDS LOW VGS LOW ILOW 1 VREF + - VGS HIGH PID VOUT Without Circulating Current -1 VGS LOW CAS2004 / Warrington / 12-18 May 2004 Y. Thurel 43 / xx CAS 2004 – 4Q Power Converters Technologies LHC: 4QLS with circulation current • Adding 2x circulation current loop • To avoid 0A distortion crossing , a circulating can help, biasing MOSFET gates. • These additional loops (one per MOSFET) must not perturb main loop. (must be slower) LHC ±120A ±10V Measurements IHIGH VGS HIGH VE VDS HIGH VOUT IOUT LL With Circulating Current RL VE VDS LOW VGS LOW • ICirculation can vary ILOW IHIGH IREF + - PID’ + +1 VREF + - + VGS HIGH PID With Circulating Current -1 VOUT + + VGS LOW CAS2004 / Warrington / 12-18 May 2004 Y. Thurel 44 / xx CAS 2004 – 4Q Power Converters Technologies LHC: 4QLS with circulation current different approaches: •Circulating current always present, changing its value depending on output current • Its control is easy (reference is only smoothly changing with IOUT) • Inverter reference must always be set so that this circulating current is possible leading to higher losses in receptor mode. • No changing mode (Gate of each side MOSFET always biased) Q1 Q1 & Q2 Q2 •Circulating current only present when close to a potential transition • This solution saves a lot of energy when recovering, since inverter doesn’t inject power in MOSFET when absorbing power. • dI/dt Limitation exists, since if too fast, circulating current doesn’t have time to appear and MOSFET Gate are not well biased. CAS2004 / Warrington / 12-18 May 2004 Y. Thurel ICC REF Fr. Icc loop VGS Q2 Fr. Main loop [t] 45 / xx CAS 2004 – 4Q Power Converters Technologies LHC: 4QLS / Inverter Reference LHC ±120A ±10V Measurements • Inverter REF is built according to – VBIAS MIN. not to saturate MOSFET (i.e saturate Loop) – VBIAS OPT. For 4Q Linear stage acting as active filter (better rejection of mains disturbances and 300 Hz) – VMIN coupled to I circulation MIN to always minimum load inverter (Conduction mode un-changed) – Inverter Loop must be faster / transparent than 4Q stage loop VBIAS VBIAS |VREF| + VMIN + + VMIN PID’ - INVERTER VE IHIGH IREF + - PID’ + +1 VREF + - PID VOUT + VGS HIGH -1 + + VGS LOW CAS2004 / Warrington / 12-18 May 2004 Y. Thurel 46 / xx CAS 2004 – 4Q Power Converters Technologies LHC: 4QLS MOS working Area (Example) Practical case of Circulation current always ON, at the same value: 5A. VOUT 5A 11 V -120 A RDSON variations 11 V limited by circulating current. 10 V 1 V, 5 W 200 mΩ 11 V 21 V, 2.6 kW 168 mΩ 11 V 125 A 120 A 10 V 125 A 1 V, 125 W 8.00 mΩ 21 V, 105 W 4.20 Ω 5A 5A Dissipate Power is: 1V 0A •21V x 120A in recovering MOSFET instead of 10V x 120A required by the load. •Only valid if not often the case. 1V -120 A 11 V -10 V 125 A 21 V, 105W 4.20 Ω 11 V 1 V, 125W 8.00 mΩ 11 V 125 A CAS2004 / Warrington / 12-18 May 2004 IOUT 1 V, 5 W 200 mΩ 5A 5A 11 V 0V 1 V, 5 W 200 mΩ Y. Thurel 120 A -10 V 21 V, 2.6 kW 168 mΩ 1 V, 5 W 200 mΩ 5A 47 / xx CAS 2004 – 4Q Power Converters Technologies LHC: 4QLS MOS Model (FB180SA10 I.R.) 10.0 Settings like: - Circulating current value - Difference voltage issued from the inverter output voltage - Number of MOSFET in // are the key to maintain a stable efficient analog loop. Rdson at VDS= 5 V 9.0 Rdson [Ohms] MOSFET is difficult to control directly from the main loop to the gate. Indeed gain is from virtually 0 if saturated to thousands when almost OFF. Rdson at VDS= 2 V 8.0 Rdson at VDS= 1 V 7.0 Rdson at VDS= 0.6 V 6.0 Rdson at VDS= 10 V Rdson at VDS= 20 V 5.0 4.0 3.0 2.0 1.0 VGS [V] 0.0 3.7 CAS2004 / Warrington / 12-18 May 2004 3.9 Y. Thurel 4.1 4.3 4.5 4.7 4.9 48 / xx CAS 2004 – 4Q Power Converters Technologies LHC ±120A ±10V Measurements LHC: Practical Results DISTORTION ?: Crossing axis is OK. No distortion, achieved thanks to circulating current. CONTROL: Bandwidth in generator & receptor quadrant Crossing 0A is OK, being unchanged. CAS2004 / Warrington / 12-18 May 2004 Y. Thurel 49 / xx CAS 2004 – 4Q Power Converters Technologies LHC: Realizations LHC ±120A ±10V • 330 Converters • Correctors • CERN Internal Design LHC ±60A ±8V • 800 Converters • Orbit Correctors • Below Dipoles, in a radiation zone • CERN Internal Design CAS2004 / Warrington / 12-18 May 2004 Y. Thurel 50 / xx CAS 2004 – 4Q Power Converters Technologies LHC ±600A ±10V • 440 Converters • 1x 6U Module LHC ±600A ±40V • 50 Converters • 2x 6U module CAS2004 / Warrington / 12-18 May 2004 Y. Thurel 51 / xx CAS 2004 – 4Q Power Converters Technologies Thank you for your attention. AND?…END. CAS2004 / Warrington / 12-18 May 2004 Y. Thurel 52 / xx CAS 2004 – 4Q Power Converters Technologies + - IHIGH VE VGS HIGH VDS HIGH VOUT IOUT LL RL VE VDS LOW VGS LOW ILOW CAS2004 / Warrington / 12-18 May 2004 Y. Thurel 53 / xx CAS 2004 – 4Q Power Converters Technologies Reference Care with test invisble so that alignment is ok LF LF LF LF LF LF LF VLOAD ILOAD HF P O L . C H A . HF L I N E A R HF HF HF HF HF HF L I N E A R CAS2004 / Warrington / 12-18 May 2004 Y. Thurel 54 / xx