Proton Driver Magnet Power Supply System Cezary Jach BD/EE Support April 19, 2000.

Slides:



Advertisements
Similar presentations
Alternating Current Circuits and Electromagnetic Waves
Advertisements

ISIS Electrical Engineering Group
DC Choppers 1 Prof. T.K. Anantha Kumar, E&E Dept., MSRIT
EMMA Upgrade: Slow Acceleration with Low-Frequency Cavity J. Scott Berg Brookhaven National Laboratory 12 March 2010.
Proton Beam Measurements in the Recycler Duncan Scott On Behalf of the Main Injector Group.
Proton / Muon Bunch Numbers, Repetition Rate, RF and Kicker Systems and Inductive Wall Fields for the Rings of a Neutrino Factory G H Rees, RAL.
DC Choppers 1 Prof. T.K. Anantha Kumar, E&E Dept., MSRIT
Power I, VI, V I max  V max  I, VI, V I max AC Circuits use a similar definition of power as DC circuits. The one detail that need to be included.
Alternating Current Circuits
Chapter 20 Quasi-Resonant Converters
9/29/2004EE 42 fall 2004 lecture 131 Lecture #13 Power supplies, dependent sources, summary of ideal components Reading: Malvino chapter 3, Next:
Lecture 20-1 Alternating Current (AC) = Electric current that changes direction periodically ac generator is a device which creates an ac emf/current.
Fundamentals of Power Electronics 1 Chapter 20: Quasi-Resonant Converters Chapter 20 Quasi-Resonant Converters Introduction 20.1The zero-current-switching.
Presented By: Er. Ram Singh (Asstt. Prof.) Deptt. Of EE
Copyright by UNIT III DC Choppers 4/17/2017 Copyright by
Chapter 20 Quasi-Resonant Converters
Copyright © 2009 Pearson Education, Inc. Lecture 10 – AC Circuits.
Fall 2008 Physics 121 Practice Problem Solutions 13 Electromagnetic Oscillations AC Circuits Contents: 121P13 - 2P, 3P, 9P, 33P, 34P, 36P, 49P, 51P, 60P,
1 BROOKHAVEN SCIENCE ASSOCIATES NSLS-II Stability Workshop April , 2007 NSLS-II Electrical Systems G. Ganetis NSLS-II Electrical Systems NSLS-II.
Chapter 22 Alternating-Current Circuits and Machines.
Options for a 50Hz, 10 MW, Short Pulse Spallation Neutron Source G H Rees, ASTeC, CCLRC, RAL, UK.
Alternating-Current Circuits Chapter 22. Section 22.2 AC Circuit Notation.
Power Electronics and Drives (Version ) Dr. Zainal Salam, UTM-JB 1 Chapter 3 DC to DC CONVERTER (CHOPPER) General Buck converter Boost converter.
ECE Electric Drives Topic 10: Cycloconverters Spring 2004.
Alternating Current Circuits
Alternating Current Circuits
9/27/2004EE 42 fall 2004 lecture 121 Lecture #12 Circuit models for Diodes, Power supplies Reading: Malvino chapter 3, Next: 4.10, 5.1, 5.8 Then.
Fundamentals of Electric Circuits Chapter 11
Yichao Jing 11/11/2010. Outline Introduction Linear lattice design and basic parameters Combined function magnets study and feasibility Nonlinear dynamics.
Electrical Principles 1 1 G5 - ELECTRICAL PRINCIPLES [3 exam questions - 3 groups] G5A - Reactance; inductance; capacitance; impedance; impedance matching.
3 GeV,1.2 MW, Booster for Proton Driver G H Rees, RAL.
Performance Improvement of APS Booster Ring Dipole Magnet Power Supplies Ju Wang The 3 rd Workshop on Power Converters for Particle.
110/16/2015 Applied Physics Lecture 19  Electricity and Magnetism Induced voltages and induction Energy AC circuits and EM waves Resistors in an AC circuits.
1 Status of EMMA Shinji Machida CCLRC/RAL/ASTeC 23 April, ffag/machida_ ppt & pdf.
Enrollment no.: Abhi P. Choksi Anuj Watal Esha N. Patel Guidied by: M. K. Joshi, P.R.Modha A.D.PATEL.INSTITUTE.
Inductance and AC Circuits. Mutual Inductance Self-Inductance Energy Stored in a Magnetic Field LR Circuits LC Circuits and Electromagnetic Oscillations.
Simulation of direct space charge in Booster by using MAD program Y.Alexahin, A.Drozhdin, N.Kazarinov.
Copyright © 2009 Pearson Education, Inc. Chapter 33 Inductance, Electromagnetic Oscillations, and AC Circuits Part II.
Design of an Isochronous FFAG Ring for Acceleration of Muons G.H. Rees RAL, UK.
Electron Model for a 3-10 GeV, NFFAG Proton Driver G H Rees, RAL.
The ISIS Dual Harmonic Upgrade The Council for the Central Laboratory of the Research Councils Andy Seville Joint Accelerator WorkshopMarch 28th, 2006.
Slide 1Fig 33-CO, p Slide 2Fig 33-1, p the basic principle of the ac generator is a direct consequence of Faraday’s law of induction. When.
Physics 212 Lecture 21, Slide 1 Physics 212 Lecture 21.
Fundamentals of Power Electronics 1 Chapter 19: Resonant Conversion Solution of converter voltage conversion ratio M = V/V g Eliminate R e :
Chapter 31 Lecture 33: Alternating Current Circuits: II HW 11 (problems): 30.58, 30.65, 30.76, 31.12, 31.26, 31.46, 31.56, Due Friday, Dec 11. Final.
Chapter 8 Alternating Current Circuits. AC Circuit An AC circuit consists of a combination of circuit elements and an AC generator or source An AC circuit.
Chinese Academy of Sciences Institute of High Energy Physics Accelerator Center Power Supply Group Status of BEPCII and CSNS Power Supply System Qi Xin.
FFAG Studies at RAL G H Rees. FFAG Designs at RAL Hz, 4 MW, 3-10 GeV, Proton Driver (NFFAGI) Hz,1 MW, GeV, ISIS Upgrade (NFFAG) 3.
UNIT-VII Static Series Compensators
The Introduction to CSNS Accelerators Oct. 5, 2010 Sheng Wang AP group, Accelerator Centre,IHEP, CAS.
TECHNICAL PAPER ON SIMULTANEOUS AC-DC POWER TRANSMISSION
Chapter 3 – Diode Circuits – Part 3
ICFA mini-Workshop on Beam Commissioning for High Intensity Accelerators Yasuhiro Watanabe (J-PARC / JAEA) Tracking between bending and quadrupole families.
High Power RF Systems for 2-8 GeV Fast Cycling Synchrotron PROJECT X (ICD-2) John Reid September 11, 2009.
Electronics Technology Fundamentals Chapter 10 Inductors.
TRANSFORMERS  A power station produces an AC pd of ~25 kV  This AC pd is stepped up to ~132 kV so that it can transport through cables without losing.
Effects of Harmonics on Capacitors Electrical System
The ISIS Dual Harmonic Upgrade
Islamic University of Gaza
Coupling Correction at the Australian Synchrotron
Development of new power supplies for J-PARC MR upgrade
Electromechanical Systems
Klystron Power Supplies for ILC
OCR 21st Century Science Unit P5 a and b Revision
Reading: Malvino chapter 3, Next: 4.10, 5.1, 5.8
PSB magnetic cycle 160 MeV to 2 GeV with 2.5E13 protons per ring
Negative Momentum Compaction lattice options for PS2
INDUCTORS, CAPACITORS AND ALTERNATING CURRENT
POWER ELECTRONICS DC-DC CONVERTERS (CHOPPERS) PART 2
Presentation transcript:

Proton Driver Magnet Power Supply System Cezary Jach BD/EE Support April 19, 2000

Cezary Jach - BD/EE Support2 System Top Level Parameters Frequency - 15 Hz Dipole peak stored energy MJ (Main Injector dipole GeV) Dipole peak field T B max /B min = 17.7 Quad. peak stored energy MJ Quadrupole peak gradient T/m G max /G min = 17.7

April 19, 2000Cezary Jach - BD/EE Support3 Design Choices SCR power supply system (similar to Main Injector) –Dipole power supply system S = 550 MVA peak –Quadrupole power supply system S = 50 MVA peak –Combined S = 600 MVA peak (Main Ring 300 MVA 500 GeV), mostly reactive power approximately 4 times existing site peak power returns reactive power to the grid with 15 Hz frequency difficult & costly reactive power compensation IGBT power supply system (S. Fang) Resonant power supply system (similar to Booster)

April 19, 2000Cezary Jach - BD/EE Support4 Resonant Power Supply Systems Single frequency. Current is in the form of biased sinusoid Dual frequency. Current is in the form of 15 Hz biased sinusoid with superimposed 30 Hz component- chosen design Switched. Current is in the form of biased 10 Hz sinusoid when rising, and 30 Hz when falling

April 19, 2000Cezary Jach - BD/EE Support5 Switched System Magnet Current Ripple at injection = 270 ppm p-p

April 19, 2000Cezary Jach - BD/EE Support6 Dual Frequency Resonant Power Supply System LCR network with single resonant frequency at 15 Hz, driven by a source containing 15 Hz and 30 Hz frequencies (30 Hz needs 15 MVA peak) LCR network with two resonant frequencies at 15 Hz and 30 Hz, driven by a source containing 15 Hz and 30 Hz frequencies - chosen design

April 19, 2000Cezary Jach - BD/EE Support7 Adding 2nd Harmonic to Magnet Current

April 19, 2000Cezary Jach - BD/EE Support8 Resonant Power Supply Systems

April 19, 2000Cezary Jach - BD/EE Support9 Power Supply System Parameters System design based on lattice version 1, dated Jan. 1, 2000 Total induced voltage = 167 kV, number of res. cells = 27 System Voltage –Voltage across cell, peak = 6,200 V (Booster 940 V) –Voltage to ground, peak = 3,100 V (Booster 470 V) Magnet Current –Peak Current = 7,500 A –Minimum Current = 420 A –DC Current = 3,700 A –AC Current, fundamental, peak = 3,500 A –AC Current, 2nd harmonic = 440 A

April 19, 2000Cezary Jach - BD/EE Support10 Proton Driver Magnet Power Supply Diagram

April 19, 2000Cezary Jach - BD/EE Support11 Resonant Cell Elements

April 19, 2000Cezary Jach - BD/EE Support12 Resonant Cell Frequency Response

April 19, 2000Cezary Jach - BD/EE Support13 Power Supply System 3.6 MVA of DC power - special cell for DC power supply insertion. Power supply rating MVA 14.5 MVA peak at 15 Hz, either “injected” through secondary windings of dc bypass choke or in series with magnets. Power supply rating MVA 0.8 MVA peak at 30 Hz, either “injected” or in series with magnets. Power supply rating MVA 27 chokes, 100 t, 425 kJ, 3m x 4m x 4m

April 19, 2000Cezary Jach - BD/EE Support14 Power Supply System Parameters

April 19, 2000Cezary Jach - BD/EE Support15 Quadrupole Tracking Error Tolerance Study ISIS experience,   0.01 To avoid space charge tune spread edge to touch a 4th order resonant line (space charge = 0.06)

April 19, 2000Cezary Jach - BD/EE Support16 Quadrupole Tracking Power Supply Choices Independent power supply circuits Quadrupole main coils in series with dipoles –bucking chokes to produce opposing induced voltage –quadrupole trim coils connected in series with secondary of bucking choke –IGBT power supplies (Main Injector sextupole power supply style), will meet required current, voltage and bandwidth

April 19, 2000Cezary Jach - BD/EE Support17 Quadrupole Tracking System Diagram - 1/3 of the Ring

April 19, 2000Cezary Jach - BD/EE Support18 Quadrupole Tracking

April 19, 2000Cezary Jach - BD/EE Support19 Quadrupole Compensation

April 19, 2000Cezary Jach - BD/EE Support20 Quadrupole Tracking |  | max  0.01% if compensation current includes up to 7th harmonic

April 19, 2000Cezary Jach - BD/EE Support21 Quadrupole Tracking and Tune Control Power supply peak current rating at given frequency is set by required tune compensation or tracking, whichever is higher

April 19, 2000Cezary Jach - BD/EE Support22 Quadrupole Tracking Calculations Assume bucking choke’s main inductance Calculate trim circuit input impedance at each frequency Assume calculated previously required peak currents for each frequency Calculate required peak voltages for each frequency Vary quad turns ratio to arrive at reasonable power supply current/voltage ratings Calculate bucking choke turns ratio

April 19, 2000Cezary Jach - BD/EE Support23 Quadruple Tracking Circuit Calculation Results Bucking choke requirements: –L1 = 2 mH, L2 = 4.31 mH, k = 0.98 –N1 = 32, N2 = 47,  = 0.03% –74 kJ Quadrupole turns ratio 4:1 Power supply requirements: –210 Hz minimum bandwidth –860 A peak, 608 V peak –6 power supplies, 608 kVA peak each –Capable of 4 quadrant operation

April 19, 2000Cezary Jach - BD/EE Support24 Conclusions Well proven technology Very large components More detailed design and complete system simulations will be done after lattice design is stabilized. Challenges –3,100 V magnets –Quadrupole tracking –Regulation (DC, 15 Hz, 30 Hz)