Powering the LHC Magnets

Slides:



Advertisements
Similar presentations
LHC Machine Protection
Advertisements

Frédérick BORDRY – LHCMAC 22- 6th December 2007 Review of the experience of LHC powering: short-circuit tests and sector 7-8 and start of powering sector.
1 Powering Tests and Safety Electrical Safety Hugues Thiesen Power Converter Group.
REVIEW OF THE CRYOGENIC BY-PASS FOR THE LHC DS COLLIMATORS ELECTRICAL CIRCUIT MODIFICATION, INCLUDING OPERATIONAL CONSIDERATIONS PRESENTED BY A. SIEMKO.
Bernhard Holzer * IP5 IP1 IP2 IP8 IR 7 ”Beam Dynamics for Nb3Sn dipoles... latest news"
David Nisbet – LIUWG 17 th July 2008 LIUWG – Options for Powering Phase I David Nisbet Summary of points from LIUWG 7 Existing topology Future topology.
Chamonix Risks due to UPS malfunctioning Impact on the Superconducting Circuit Protection System Hugues Thiesen Acknowledgments:K. Dahlerup-Petersen,
1 Second LHC Splice Review Copper Stabilizer Continuity Measurement possible QC tool for consolidated splices H. Thiesen 28 November 2011 K. Brodzinski,
HC Review, May 2005 Hardware Commissioning Review Hardware Commissioning Review Quality Assurance and Documentation of Results Félix Rodríguez Mateos,
CERN Rüdiger Schmidt FCC week 2015 Long Magnet Stringpage 1 Incident September 19 th Architecture of powering and protection systems for high field.
Becoming familiar with QPS systems in the LHC (incl. EE) Presentation 02 Sept PART 1 of 3. Part 1: General layouts and principles Presentation of.
Interlock and Protection Systems for SC Accelerators: Machine Protection System for the LHC l The Risks l The Challenge l The LHC Layout l The Systems.
The Large Hadron Collider Contents: 1. The machine II. The beam III. The interaction regions IV. First LHC beam [R. Alemany] [CERN AB/OP] [Engineer In.
1 st September 2005LHC-LUMI 05 - G.Arduini – CERN/AB Optical requirements for the magnetic lattice of the high energy injectors (SSPS in the SPS tunnel)
Rüdiger Schmidt1 The LHC collider project I Rüdiger Schmidt - CERN SUSSP Sumer School St.Andrews Challenges LHC accelerator physics LHC technology Operation.
Training LHC Powering R. Denz Quench Protection System R. Denz AT-MEL.
AT-MEL-PM, R. Denz, CERN, CH-1211 Geneva 23 1 QPS system and its risks  Principal risks  General remarks  Quench heater circuits  Quench detection.
AT-MEI-PE, RD, LIUWG 31-JUL R. Denz AT-MEI-PE LHC Luminosity Upgrade Protection of the Inner Triplet, D1, Correctors and Superconducting Links/Leads.
October, 2009 Magnet Electrical Systems Bob Lambiase October, 2009 Internal Review.
LER Workshop, October 11, 2006LER & Transfer Line Lattice Design - J.A. Johnstone1 LHC Accelerator Research Program bnl-fnal-lbnl-slac Introduction The.
Power Converters and DC cablesSlide 1/.. LHC - HC review Hugues THIESEN – AB/PO Thursday, 12 May 2005 Water cooled cables warm bus bars power converter.
BCWG - 16/11/20102 Content WHY do we need a HW Commissioning campaign? WHAT are we going to do? HOW are we going to do it? ElQA QPS Powering Tests Planning.
By Verena Kain CERN BE-OP. In the next three lectures we will have a look at the different components of a synchrotron. Today: Controlling particle trajectories.
Faster ramp rates in main LHC magnets Attilio Milanese 7 Oct Thanks to M. Bajko, L. Bottura, P. Fessia, M. Modena, E. Todesco, D. Tommasini, A. Verweij,
TE-MPE -EI 23/6/2011,Antonopoulou Evangelia RQS circuit Simulation results of Quench Antonopoulou Evangelia June 2011 Thanks to E. Ravaioli.
AT-MEL Group Meeting, CERN, 1211 Geneva 23 1 ElQA activities during hardware commissioning N. Catalan Lasheras.
Machine Protection Review, R. Denz, 11-APR Introduction to Magnet Powering and Protection R. Denz, AT-MEL-PM.
LHC Machine Protection: an introduction Jörg Wenninger OP training March 2006 Acknowledgments to my colleagues of the MPWG for input and material.
MPP Meeting 07/03/2007 MPP Main Ring Magnet Performance Panel Meeting Wednesday 7th March 2007 Agenda: 1)Matters arising 2)Recommendations for the case.
The prototype test String 2 May 13, 20082Roberto Saban – Academic Training Lecture 1 – Why LHC Hardware Commissioning?
CSCM (Thermal Amplifier) Sequence and detailed planning 07/10/2011 M.Solfaroli Thanks to: K.Brodzinski, G.D’Angelo, M.Koratzinos, M.Pojer, R.Schmidt, J.Steckert,
Comparison of magnet designs from a circuit protection point of view Arjan Verweij, CERN, TE-MPE with input from M. Prioli, R. Schmidt, and A. Siemko A.
TEST FACILITY STATUS FOR TESTING CERN Marta Bajko WP10. EUCARD 2 Task 4 - HTS Magnet Tests, June 2015.
Training LHC Powering – Blanca Perea Solano From Individual System Tests to Powering to Nominal Blanca Perea on behalf of Hardware Commissioning Coordination.
Hardware Commissioning Review, R. Denz, 12-May Superconducting circuits: what remains to be done during hardware commissioning R. Denz AT-MEL-PM.
NIKHEF Annual Meeting, December 18, The LHC Project Status report to the NIKHEF annual meeting Jos Engelen Based on last week’s reports to CERN.
First evaluation of Dynamic Aperture at injection for FCC-hh
News from the LHC J. Wenninger CERN Beams Department Operation Group
HL-LHC IT STRING and Series test of SC link
BEAM LOSS MONITORING SYSTEM
Electrical insulation of magnet circuits in sector 7-8
Powering LHC magnets version 30/3/2007.
Minimum Hardware Commissioning – Disclaimer
LHC schedule.
LHC Hardware Commissionning
Superconducting Circuits, a generic view
The LHC - Status Is COLD Is almost fully commissioned
Large Booster and Collider Ring
Concepts for magnet circuit powering and protection M
Update on circuit protection simulations of the HL-LHC Inner Triplet circuit Matthias Mentink, Circuit specifics + STEAM simulations: Samer Yammine, LEDET.
Powering from short circuit tests up to nominal
Circuits description and requirements - Closed Session-
Detailed global view on protection and detection of the circuits
Status of the BLHC ….work in progress! Mike Lamont CERN/AB 18/01/2008
BEAM LOSS MONITORING SYSTEM
Rüdiger Schmidt and Karl Hubert Mess
Initial Experience with the Machine Protection System for LHC
Mike Lamont 4th HERA and the LHC workshop 26th May 2008
Machine Protection Xu Hongliang.
+ many slides from various colleagues (KH, Rudiger, Paul, …)
LHC (SSC) Byung Yunn CASA.
ILC 3.2 km DR design based on FODO lattice (DMC3)
Hilumi WP3 meeting, 1 October 2014
LHC Beam Operations Past, Present and Future
CEPC-SPPC Beihang Symposium
ILC 3.2 km DR design based on FODO lattice (DMC3)
Negative Momentum Compaction lattice options for PS2
Commissioning of the LHC superconducting magnets systems: Why an LHC Hardware Commissioning? Specificity and complexity of this machine Roberto Saban.
Negative Momentum Compaction lattice options for PS2
Presentation transcript:

Powering the LHC Magnets markus.zerlauth@cern.ch July 2015 LHC Layout, Optics and naming conventions Electrical circuits and Powering Subsectors Power Converters, Cables, QPS, Energy Extraction,… Magnet/Circuit Protection Operation of magnet powering system

How to achieve a collision energy of 7TeV in the LHC? LHC Layout eight sectors eight arcs eight long straight sections (insertions) about 700 m long Beam dump blocks IR5:CMS IR4: RF + Beam instrumentation IR6: Beam dumping system IR3: Momentum Cleaning (warm) IR7: Betatron Cleaning (warm) Main dipole magnets: making the circle IR8: LHC-B IR2:ALICE IR1: ATLAS Injection Injection 2

LHC arcs: dipoles and short straight sections 1232 superconducting dipoles magnets magnetic field 8.3T (7Tev), each magnet 15m long, operating at 1.9K Deflection of all man dipoles: 2 , in total 19 km main dipole magnets Arc length ~21 km (dipoles + short straight sections + interconnects)

Interconnection between a quadrupole and a dipole

Interconnecting busbars

Bus bar interconnections right of point 8 (19/3/2007) 600 A bus bars (Nline) 6 kA bus bars

LHC Powering in 8 Sectors 5 (+) Less energy & voltage per circuit (+) For superconducting magnets, no DC powering across IPs (+) Commissioning possible for each sector, independent of other sectors 4 6 DC Power feed (o) Main DC power feed at even points (MB, MQ) (o) Some DC power feed at odd points Octant 3 DC Power 7 arc cryostat LHC Sector 2 8 (-) Higher complexity, i.e. more powering equipment needed (converters, DFBs,…) (-) More complex circuit tracking between circuits Sector 1

Arc cryostat with string of dipole magnets LHC powered in eight sectors, each with 154 dipole magnets Time for the energy ramp is about 20-30 min (Energy from the grid) Time for discharge is about the same (Energy back to the grid) DFB DFB Magnet 2 Magnet 4 Magnet 152 Magnet 154 Magnet 1 Magnet i Magnet 153 Magnet 3 Energy Extraction: switch closed Energy Extraction: switch closed Power Converter

Main dipoles: quench of a magnet Quench in one magnet: Resistance and voltage drop across quenches zone Quench is detected: Voltage across magnet exceeds 100 mV DFB DFB Magnet 2 Magnet 4 Magnet 152 Magnet 154 Magnet 1 Magnet i Magnet 153 Magnet 3 Energy Extraction: switch closed Energy Extraction: switch closed Quench Detector Power Converter

Main dipoles: magnet protection Quench heaters warm up the entire magnet coil: energy stored in magnet dissipated inside the magnet (time constant of 200 ms) Diode in parallel becomes inductive: current of other magnets goes through diode Resistance is switched into the circuit: energy of 153 magnets is dissipated into the resistance (time constant of 100 s for main dipole magnets) DFB DFB Magnet 2 Magnet 4 Magnet 152 Magnet 154 Magnet 1 Magnet i Magnet 153 Magnet 3 Energy Extraction: switch open Energy Extraction: switch open Quench Detector Quench Heater PS Power Converter

Magnet current after a quench Current in a dipole magnets after a quench, when heaters are fired (7 TeV / 8.3 Tesla) - 7 MJ within 200 ms into magnet Current after quench Gaussian approximation

Circuit Protection Protection of superconducting circuits is a function of stored energy (and complexity) of the circuit Main concern is with fast extraction of energy from circuit and avoidance of quenches (mechanical stress, downtime to recover,..) Quench Protection system to detect quenches, mitigation through Quench heaters (spread out energy dissipation in whole volume) Parallel protection through diode or resistor (bypass the quenching magnet) Energy Extraction system and crow-bars (forced extraction of energy from magnet chain)

QPS Installations II MB protection rack Protection unit Q4.L8 & D2.L8 Quench heater power supplies Q4.L8 Quench heater connection Q5.L8

QPS Installations III 13 kA EE systems 13 kA protection diode 13 kA EE extraction resistors RB 600 A EE systems

LHC Hardware Commissioning EE, @ nominal Free-wheel @ 6kA EE, @ 4kA EE, free-wheel + cycle @ 2kA EE, free-wheel + cycle @ Injection level Splice Measurements Splice Measurements Power Converter Setup Interlock tests Splice Measurements Splice Measurements

Putting it all together: The LHC operational cycle beam dump energy ramp (30mn) Physic run (10 to 12h) coast 2000 4000 6000 8000 10000 12000 -4000 -2000 time from start of injection (s) dipole current (A) 7 TeV start of the ramp injection phase preparation and access 450 GeV

CERN - Eine Einführung

Superconducting Magnet Units

Standard FODO cell = 2 electrical ‘half’-cell

Circuit Types defined for HWC and operation 60A (752 orbit corrector circuits) 80-120A (~ 284 LSS and DS orbit correctors) 600A EE (202 x 600A correctors with Energy Extraction System) 600A no EE (72 x 600A correctors without Energy Extraction) 600A no EE crowbar (136 x 600A correctors without EE, but crowbar) IPQ (~ 6kA) (78 x Individually powered quads, Q4-Q10) IPD (~ 6kA) (16 x Separation and re-combination dipoles) IT (~ 8kA) (8x Main Inner Triplet Circuits) Main Dipole and Quadrupoles (~ 12kA) x 24 WARM x40 Total of 1612 electrical circuits

Electrical half-cells - Electrical Circuits & connections Line N Majority of magnets in the arc of a given family connected in SERIES …why not in the whole machine…? Main Busbars + Spool-pieces

Magnet inventory 1232 main dipole magnets powered in series with the same strength to make it around the LHC 752 orbit corrector magnets powered individually to ensure that the beam follows the design orbit (within about 0.5 mm), 392 Focusing and defocusing quadrupole magnets powered in series to keep beam size limited Lattice sextupole magnets powered in series to correct the trajectories for off-energy particles, Multipole-corrector magnets (sextupoles, decapoles, octupoles, ...) to correct field imperfections, to suppress instabilities, etc., powered in series Corrector magnets to adjust essential beam parameters (quadrupoles) Insertion dipole and quadrupole magnets to ensure beam crossing / increase the interbeam distance / focus beams for experiments etc. Total of more than 10.000 superconducting magnets in the LHC http://edms.cern.ch/cedar/plsql/navigation.tree?top=1459088716 23