POWERING LAYOUT OF THE SSS CORRECTION SCHEME (Optics version 6.4)

Similar documents
LHC MAGNET POLARITIES

RESISTIVE SOLDERING OF LINE N 6 ka BUS BARS IN THE DISPERSION SUPRESSOR ZONE

THE ELECTRICAL CIRCUITS IN THE LHC REFERENCE DATABASE

APAC 2007, Raja Ramanna Centre for Advanced Technology(RRCAT), Indore, India LHC STATUS. Lyndon Evans, CERN, Geneva, Switzerland

2008 JINST 3 S Powering and protection. Chapter Overview. 6.2 Powering circuits

LHC: CONSTRUCTION AND COMMISSIONING STATUS

2008 JINST 3 S Magnets. Chapter Overview. 3.2 Superconducting cable

INTERLOCK AND PROTECTION SYSTEMS FOR SUPERCONDUCTING ACCELERATORS: MACHINE PROTECTION SYSTEM FOR THE LHC

Usage of DSP and in large scale power converter installations (LHC)*

Emilia Cruz. September 21, 2015

Hardware Commissioning

ELECTRONIC SYSTEMS FOR THE PROTECTION OF SUPERCONDUCTING ELEMENTS IN THE LHC

Powering the High-Luminosity Triplets *

INDUSTRIAL CONTROLS FOR TEST SYSTEMS FROM SUPERCONDUCTING STRANDS TILL MAGNET FIDUCIALISATION IN THE TUNNEL FOR THE LHC PROJECT

THE HARDWARE INTERFACES BETWEEN WARM MAGNET INTERLOCK SYSTEM, NORMAL CONDUCTING MAGNETS, POWER CONVERTERS AND BEAM INTERLOCK SYSTEM FOR THE LHC RING

Basics of Accelerator Science and Technology at CERN. Power supplies for Particle accelerators. Jean-Paul Burnet

A new hybrid protection system for high-field superconducting magnets

Residual Resistivity Ratio (RRR) Measurements of LHC Superconducting NbTi Cable Strands

ALIGNMENT METHODS APPLIED TO THE LEP MAGNET MEASUREMENTS. J. Billan, G. Brun, K. N. Henrichsen, P. Legrand, 0. Pagano, P. Rohmig and L. Walckiers.

EUROPEAN ORGANIZATION FOR NUCLEAR RESEARCH European Laboratory for Particle Physics

CERN (The European Laboratory for Particle Physics)

AUTOMATION OF 3D MEASUREMENTS FOR THE FINAL ASSEMBLY STEPS OF THE LHC DIPOLE MAGNETS

DRAWING PROCESS EXTERNAL DRAWINGS

Cryogenic Testing of Superconducting Corrector Magnets for the LHC Main Dipole

Brett Parker, representing the

MD Amplitude Detuning Studies at 6.5 TeV with Various Configurations of the Crossing Scheme

KEYWORDS: LHC, helium cryogenics, superconductor, electrical feedbox, HTS current leads, busbar, magnet

Accelerator Controls CAS Hermann Schmickler

NAMING CONVENTIONS FOR BUILDINGS AND CIVIL ENGINEERING WORKS

Standard ELQA measurements, ELQA for splice and proximity equipment consolidation

NAMING CONVENTIONS FOR BUILDINGS AND CIVIL ENGINEERING WORKS

Design of beam optics for FCC-ee

LHC ARC DIPOLE STATUS REPORT

CONSTRUCTION AND TESTING OF ARC DIPOLES AND QUADRUPOLES FOR THE RELATIVISTIC HEAVY ION COLLIDER (RHIC) AT BNL *

WIEN Software for Design of Columns Containing Wien Filters and Multipole Lenses

STORING OF CONTRACTOR DRAWINGS IN EDMS/CDD

Herwig Schopper CERN 1211 Geneva 23, Switzerland. Introduction

Experience with Insertion Device Photon Beam Position Monitors at the APS

LHC BEAM ENERGY IN 2012

CERN EUROPEAN ORGANIZATION FOR NUCLEAR RESEARCH INVESTIGATION OF A RIDGE-LOADED WAVEGUIDE STRUCTURE FOR CLIC X-BAND CRAB CAVITY

Conceptual Design of the LHC Interaction Region Upgrade Phase-I

LHC COMMISSIONING AT HIGHER ENERGY

Series manufacture of the LHC main. dipole magnets. Notes about the CERN. approach to industrial. production. C.Wyss & L.

Power Converters for Accelerators. CERN Course on Power Converters, Baden (CH)

The HL-LHC Machine *

Recommended Locations of Beam Loss Monitors for the ATLAS Roman Pots

Design of the magnets for the MAX IV project. Martin Johansson, Beam Dynamics meets Magnets-II workshop, Bad Zurzach, Dec.

CEBAF Overview June 4, 2010

MEASUREMENT OF BEAM LOSSES USING OPTICAL FIBRES AT THE AUSTRALIAN SYNCHROTRON

ACQUISITION SYSTEM FOR DETECTING IMPACTS OF HIGH ENERGY PROTON BEAMS ON THE LHC COLLIMATOR

Circumference 187 m (bending radius = 8.66 m)

I. INTRODUCTION. and the quality assurance have been improved, with new measurement

EFFECTS OF FRINGE FIELDS AND INSERTION DEVICES REVEALED THROUGH EXPERIMENTAL FREQUENCY MAP ANALYSIS*

Market Survey. Technical Description. Supply of Medium Voltage Pulse Forming System for Klystron Modulators

The Superconducting Strand for the CMS Solenoid Conductor

Title Coil Wound by Surface Winding Techn.

High-Speed Mobile Communications in Hostile Environments

Magnetic measurement system for superconducting final focus quadrupoles for SuperKEKB

28/11/2016 Juan Carlos Perez TE-MSC-MDT Jose Ferradas TE-MSC-MDT

Chapter 6. Cold Powering. 6 Cold powering. A. Ballarino 1, J.P. Burnet 1, D. Ramos 1, U. Wagner 1, S. Weisz 1 and Y. Yang 2

Philippe Lebrun & Laurent Tavian, CERN

FAST RF KICKER DESIGN

DQW HOM Coupler for LHC

HIGH MAGNETIC FIELD SUPERCONDUCTING MAGNETS FABRICATED IN BUDKER INP FOR SR GENERATION

Miljardkonferensen Procurement at CERN

Production Measurements of Magnets for the NSLS-II Storage Ring*

3 General layout of the XFEL Facility

CHAPTER 7 MAIN MAGNETS IN THE ARCS

A few results [2,3] obtained with the individual cavities inside their horizontal cryostats are summarized in Table I and a typical Q o

CERN LIBRARIES, GENEVA P O. Cryogenics in CERN Accelerators. Ph. Lebrun on behalf of the CERN Cryogenics Group

EMG4066:Antennas and Propagation Exp 1:ANTENNAS MMU:FOE. To study the radiation pattern characteristics of various types of antennas.

Detector for LHC collisions

LHCb Preshower(PS) and Scintillating Pad Detector (SPD): commissioning, calibration, and monitoring

THE CRYOGENIC SYSTEM OF TESLA

MEASUREMENT OF THE BEAM POSITION IN THE LHC MAIN RINGS

Activities on Beam Orbit Stabilization at BESSY II

OVERVIEW OF SIRIUS POWER SUPPLIES

Status SIS100. Peter Spiller 1. Pre-Collaboration Meeting Peter Spiller, 1. Pre-Collaboration Meeting,

Design Solutions for Compact High Current Pulse Transformers for Particle Accelerators Magnets Powering

Chapter 9. Magnet System. 9.1 Magnets in the Arc and Straight Sections

The High Luminosity LHC Project

Integrated CMOS sensor technologies for the CLIC tracker

Development of a Displacement sensor for the CERN-LHC Superconducting cryo-dipoles

Physics Requirements Document Document Title: SCRF 1.3 GHz Cryomodule Document Number: LCLSII-4.1-PR-0146-R0 Page 1 of 7

Rotating Coil Measurement Errors*

Crab Cavities for FCC

The Compact Muon Solenoid Experiment. Conference Report. Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland

HOM COUPLER ALTERATIONS FOR THE LHC DQW CRAB CAVITY

System Integration of the TPS. J.R. Chen NSRRC, Hsinchu

Protection of Hardware: Powering Systems (Power Converter, Normal Conducting, and Superconducting Magnets)

Status and Upgrade. P. Elleaume. XVIII ESLS Workshop, November P. Elleaume, ESRF. Slide: 1

The LUCID-2 Detector RICHARD SOLUK, UNIVERSITY OF ALBERTA FOR THE ATLAS- LUCID GROUP

ONLINE COUPLING MEASUREMENT AND CORRECTION THROUGHOUT THE LHC CYCLE

Preparing for the Future: Upgrades of the CMS Pixel Detector

Maurizio Vretenar Linac4 Project Leader EuCARD-2 Coordinator

ARotating Coil Array in Mono Bloc Printed Circuit Technology for Small Scale Harmonic Measurements

Power Supplies in Accelerators

Present and future beams for SHE research at GSI W. Barth, GSI - Darmstadt

Draft of Conceptual Phase 2 Collimation System Design. Phase 2 Specification and Implementation Meeting R. Assmann

Test Procedure for Nanometric Discriminator Cards for Wire Chambers. James Clarke

Transcription:

CERN CH-1211 Geneva 23 Switzerland the Large Hadron Collider project LHC Project ocument No. LHC-CC-ES-0003.00 rev. 3.0 CERN iv./group or Supplier/Contractor ocument No. LHC-CRI/PB/cl EMS ocument No. 104157 ate: 2002-10-07 unctional Specification POWERING LAYOUT O THE SSS CORRECTION SCHEME (Optics version 6.4) Abstract This unctional Specification defines the approach used to power the corrector magnets in the Short Straight Sections of the LHC machine with beam-optics version 6.4. Some criteria involved in the setting-up of the correction scheme are given and the position of the magnets is shown on the attached drawings. The powering layout has been designed to minimise the number of superconductor wires installed in the auxiliary bus bar tube (N Line). In the attached drawings, all the cell numbers contained in the continuous cryostat in each sector of the machine are displayed. Thus, the position and the function of every single corrector or corrector family can be outlined. The powering and the location of the corresponding power converter are shown as well. Prepared by: Checked by: Approved by: Paolo Burla LHC-CRI paolo.burla@cern.ch Karl-Hubert Mess rancesco Ruggiero Oliver Bruning Ranko Ostojic Approval List:. Bordry, O. Bruning, P. Burla, K. ahlerup-pertersen, L. Evans, P. augeras, G. ernqvist, C. Hauviller, A. Ijspeert, P. Lebrun, K-H. Mess, Ph. Orlandi, R. Ostojic, J-L. Périnet-Marquet, M. Peyrot, A. Poncet, P. Proudlock, J-M. Rifflet,. Rodriguez-Mateos, P. Rohmig, L. Rossi,. Ruggiero, R. Saban, R. Schmidt, N. Siegel, B. Skoczen, L. Tavian, T. Tortschanoff, J. Vlogaert, L. Walckiers.

LHC Project ocument No. LHC-CC-ES-0003.00 rev. 3.0 Page 2 of 8 History of Changes Rev. No. ate Pages escription of Changes 0.1 - draft 30-Aug-1999 1 st draft prepared by Paolo Burla. 0.2 - draft 24-Sep-1999 Checked by P. Proudlock and J-P. Koutchouk, P. Lefèvre, R. Ostojic and sent for approval. 0.3 - draft 27-Sep-1999 Sent for approval. 1.0 08-Nov-1999 Modification of the paragraph 2. CORRECTORS AMILIES + Table 1 in 2.3. Approved by the above list and released. 1.1 24-Jan-2000 Annex 7 - Correction of the sequence of chromaticity sextupoles for beam 2 in sector 78 ocument released 1.2 16-May-00 6 Minor modifications on Table 1: IP2 L&R, IP8 L&R: Q12, Q13 = MQ + MQT. ocument released 2.0 21-July-00 Abstract: Optics version 6.2. Section 2.4, Skew Quadrupoles Section 3.5, Skew Quadrupoles setting up criteria Annexes 1 to 8: Skew Quadrupoles position and powering. ocument released 2.1 24-Aug-00 6 Modification (pattern) on Table 1. ocument released 2.2 draft 2002-08-13 4 6 New version 2.2 draft: Section 2.1 List Point 2: Q6 = MQM + MQML Table 1: IP2 and IP8 left and right: Q6 = MQM + MQML ocument sent for check and approval to the defined list. eadline: 30 August 2002. 3.0 2002-10-07 All Modifications of New Optics Version: 6.4 (instead of 6.2) + section 2.1 + Table 1 adapted to Optics version 6.4. ocument released.

LHC Project ocument No. LHC-CC-ES-0003.00 rev. 3.0 Page 3 of 8 Table of Contents 1. INTROUCTION...4 2. CORRECTOR AMILIES...4 2.1 MATCHING SECTIONS (Q4 - Q7)...4 2.2 ISPERSION SUPPRESSOR (Q8 - Q11)...5 2.2.1 EXCEPTION O IP3 AN IP7... 5 2.3 ISPERSION SUPPRESSOR EXTENSION (Q12-Q13)...5 2.4 ARC SHORT STRAIGHT SECTIONS...7 3. CORRECTION SCHEME AN POWERING LAYOUT...7 3.1 TUNING QUARUPOLES...7 3.2 SKEW QUARUPOLES...7 3.3 CHROMATICITY SEXTUPOLE...8 3.4 SKEW SEXTUPOLES...8 3.5 OCTUPOLES...8 4. SSS CORRECTION SCHEME RAWINGS...8 5. REERENCES...8

LHC Project ocument No. LHC-CC-ES-0003.00 rev. 3.0 Page 4 of 8 1. INTROUCTION The SSS correction scheme for the LHC beam-optics version 6.1 was discussed at the 51st meeting of the Parameters & Layout Committee held on May 19th 1999. It was also presented and approved at the July 6th 1999 meeting of the Technical Committee. The powering philosophy proposals presented at the 52nd meeting of the Parameters & Layout Committee held on June 16th 1999 are taken into account. An optimised version of the powering layout for the correction magnets is included in this document. In particular the left/right feeding of the corrector families has been reviewed to minimise the size and the number of superconducting wires of the cable in line N and hence its size. This unctional specification was undertaken in view to make the powering layout of the correction scheme easily readable. It should specially serve as a basis to the definition of the auxiliary superconducting cables, and to the mechanical layout of the housing of line N. 2. CORRECTOR AMILIES This unctional Specification only applies to the corrector magnets installed in the long continuous cryostat near the main quadrupoles and powered through the auxiliary superconducting bus bar housed in line N of the 8 sectors of the LHC. The spool piece correctors in the arc Main ipoles and the arc orbit corrector dipoles are not powered through the auxiliary superconducting bus bar, even if installed in the long continuous cryostat. The powering scheme of these magnets is outside the scope of this document and is, therefore, not considered here. 2.1 MATCHING SECTIONS (Q4 - Q7) Except left and right of IP3 and IP7, most of the Matching Sections are built with MQM or MQY type individually powered quadrupoles. No additional correctors are required when this type of magnets is used. The connections between the power converters and the individually powered MQM's or MQY s are made in line with the cabling layout approved at the 42nd P&LC meeting held on September 16th 1998. The magnets on the two beams are connected with the corresponding power converters by means of a three-conductor bus bar. The central conductor of this arrangement carries only the difference of currents flowing in the two magnets, provided that the two magnets are connected with reversed polarities. The Matching Sections configuration depends on IP's special features. The existing configurations are described in the list below. 1. Except for left and right of IP3 and IP7, the matching sections are composed of the following individually powered quadrupoles with no additional correctors: Q4 MQY in IP1, IP5 and IP6 2xMQY in IP2 and IP8 Q5 MQML in IP1 and IP5 2xMQY in IP2L and IP8R MQY in IP4 and IP6 2xMQM in IP2R and IP8L Q6 MQML in IP1 and IP5 MQH+MQML in IP2 and IP8 MQY in IP4 Q7 2xMQM in IP1, IP2, IP5, IP8 MQM in IP4. rom Q4 to Q6, the above magnets are fitted in individual cryostats whereas Q7 in located at the end of the long continuous arc cryostat beside the electrical feed box BA.

LHC Project ocument No. LHC-CC-ES-0003.00 rev. 3.0 Page 5 of 8 2. Left and right of IP3 and IP7 (cleaning insertions), between the IP s and Q6, no individually powered quadrupoles are installed in LSS. The Q6 quadrupoles of these IP s are composed with 6 low current (600 A) MQTL type magnets in series housed in individual cryostats. The Q7 quadrupoles are of the same type and are powered in series with arc quadrupoles. They are fitted at the end of the arc continuous cryostat. or each Q7 quadrupole an MQTL type corrector magnet is required in this case. Q6 6xMQTL In series with arc MQ's Q7 MQ + MQTL. 2.2 ISPERSION SUPPRESSOR (Q8 - Q11) In all sectors, except left and right of IP3 and IP7, most of the ispersion Suppressor short straight sections are built around MQM type individually powered quadrupoles. No additional quadrupole correctors are required when individually powered quadrupoles are used. The same cabling layout as described in 2.1 will be applied. Q8 MQML Q9 MQMC+MQM Q10 MQML. However, in all sectors, Q11 is of the same type and is powered in series in the same way as the arc quadrupoles. In this case, the quadrupoles of the two beams are fitted with individually powered MQTL type corrector magnets. In series with arc MQ's Q11 MQ + MQTL. 2.2.1 EXCEPTION O IP3 AN IP7 Left and right of IP3 and IP7 the quadrupoles in the short straight sections are of the same type and are powered in series in the same way as those in the arc. The quadrupoles of the two beams are fitted with individually powered corrector circuits. In series with arc MQ's Q8 MQ + MQTL Q9 MQ + 2xMQTL Q10 MQ + MQTL. 2.3 ISPERSION SUPPRESSOR EXTENSION (Q12-Q13) In all sectors, the quadrupoles of the two beams are fitted with individually powered MQT type corrector magnets. In series with arc MQ's Q12 MQ + MQT Q13 MQ + MQT

LHC Project ocument No. LHC-CC-ES-0003.00 rev. 3.0 Page 6 of 8 Table 1: ispersion suppressor quadrupole magnets in the long continuous cryostat Q4 Q5 Q6 Q7 Q8 Q9 Q10 Q11 Q12 Q13 IP1 left MQY MQML MQML 2xMQM MQML MQMC + MQM MQML MQ +MQTL MQ + MQT MQ + MQT IP1 right MQY MQML MQML 2xMQM MQML MQMC + MQM MQML MQ + MQTL MQ + MQT MQ + MQT IP2 left 2xMQY 2xMQY MQM + MQML 2xMQM MQML MQMC + MQM MQML MQ + MQTL MQ + MQT MQ + MQT IP2 right 2xMQY 2xMQM MQM + MQML 2xMQM MQML MQMC + MQM MQML MQ + MQTL MQ + MQT MQ + MQT IP3 left MQ + MQTL MQ + MQTL MQ + 2xMQTL MQ + MQTL MQ + MQTL MQ + MQT MQ + MQT IP3 right MQ + MQTL MQ + MQTL MQ + 2xMQTL MQ + MQTL MQ + MQTL MQ + MQT MQ + MQT IP4 left MQY MQY MQM MQML MQMC + MQM MQML MQ + MQTL MQ + MQT MQ + MQT IP4 right MQY MQY MQM MQML MQMC + MQM MQML MQ + MQTL MQ + MQT MQ + MQT IP5 left MQY MQML MQML 2xMQM MQML MQMC + MQM MQML MQ + MQTL MQ + MQT MQ + MQT IP5 right MQY MQML MQML 2xMQM MQML MQMC + MQM MQML MQ + MQTL MQ + MQT MQ + MQT IP6 left MQY MQY MQML MQMC + MQM MQML MQ + MQTL MQ + MQT MQ + MQT IP6 right MQY MQY MQML MQMC + MQM MQML MQ + MQTL MQ + MQT MQ + MQT IP7 left MQ + MQTL MQ + MQTL MQ + 2xMQTL MQ + MQTL MQ + MQTL MQ + MQT MQ + MQT IP7 right MQ + MQTL MQ + MQTL MQ + 2xMQTL MQ + MQTL MQ + MQTL MQ + MQT MQ + MQT IP8 left 2xMQY 2xMQM MQM + MQML 2xMQM MQML MQMC + MQM MQML MQ + MQTL MQ + MQT MQ + MQT IP8 right 2xMQY 2xMQY MQM + MQML 2xMQM MQML MQMC + MQM MQML MQ + MQTL MQ + MQT MQ + MQT Matching ispersion Suppressor (S) S Extension Local individual cryostats Long continuous cryostats

LHC Project ocument No. LHC-CC-ES-0003.00 rev. 3.0 Page 7 of 8 2.4 ARC SHORT STRAIGHT SECTIONS 1. 2. 3. 4. 5. Tuning Quadrupoles: 2 families/arc MQT [1] QT, QT Skew Quadrupoles: In even sectors, beam 1 & in odd sectors beam 2: 2 families/arc MQS [1] QS In odd sectors, beam 1 & in even sectors beam 2: 1 family/arc MQS [1] QS Chromaticity Sextupoles: 4 families/arc MS [1] S1, S2, S1, S2 or Skew Sextupoles: (=tilted MS) 1 family/arc MSS [1] SS Octupoles: 2 families/arc MO [1] O, O 3. CORRECTION SCHEME AN POWERING LAYOUT 3.1 TUNING QUARUPOLES The four circuits formed by the two families per beam are independent in terms of powering. The power converters are always installed in the even IP end of the sector. In all sectors, the Tuning Quadrupoles are installed in cells 14 to 21, left and right. 3.2 SKEW QUARUPOLES In all sectors, skew quadrupoles are installed in cells 23 and 27 (left and right). In the even sectors (12, 34, 56, 78). On beam 2; One single family/beam of 4 magnets, forming a single circuit powered as a whole. The power converter feeding this circuit is installed in the odd IP at one end of the sector. On beam 1; 2 families/beam of 2 magnets (right of the odd IP & left of the even IP), forming 2 individually powered circuits. The power converters feeding these circuits are installed in the corresponding IP at both ends of the sector. In the odd sectors (23, 45, 67, 81). On beam 1; One single family/beam of 4 magnets, forming a single circuit powered as a whole. The power converter feeding this circuit is installed in the odd IP at one end of the sector. On beam 2; 2 families/beam of 2 magnets (right of the even IP & left of the odd IP), forming 2 individually powered circuits. The power converters feeding these circuits are installed in the corresponding IP at both ends of the sector.

LHC Project ocument No. LHC-CC-ES-0003.00 rev. 3.0 Page 8 of 8 3.3 CHROMATICITY SEXTUPOLE The eight circuits formed by the four families per beam are independent in terms of powering. The power converters are always installed in the even IP at one end of the sector. Beam 1 enters on the right of an IP at Q11 fitted with S1 or S1 depending on sector, and exits on the left of the next IP at Q11 equipped with S2 or S2 respectively. Beam 1 starts with a focusing Sextupole (S1) in arc 12. The sequence is always: S1, S1, S2, S2 or S1, S1, S2, S2 If one sextupole is "ocusing" on one beam, it is "efocusing" on the other. 3.4 SKEW SEXTUPOLES The two circuits formed by the Skew Sextupoles single family/beam are independent in terms of powering. The power converters feeding these circuits are always installed in the odd IP at one end of the sector. In the cells containing a Skew Sextupole, the latter will take the place of a normal Sextupole. A Skew Sextupole always replaces a focusing Sextupole. Whenever possible the Skew Sextupoles are centred around Q34; otherwise they are shifted one half-cell clockwise. 3.5 OCTUPOLES The four circuits formed by the two families per beam are independent in terms of powering. The power converter feeding each family is always installed in the odd IP at one end of the sector. In all sectors, the Octupoles are installed in cells 22 to 34, left and right, with the exception of 23 and 27 (Skew Quadrupoles rules above 3.2). 4. SSS CORRECTION SCHEME RAWINGS Each of the attached drawings, in Annexes 1 to 8, is dedicated to one particular sector of the LHC machine. Colour was employed to build the original version of these drawings so that more information can be displayed on the document, and in addition, the reading is made easier. The following information can be found in these drawings: Number, position (internal, external) and direction of beams. Position of the arc BA for the sector. Position and function of corrector magnets in the sector. IP number in which the power converter feeding a magnet or magnet family is installed. Number of wires or bus bars entering a sector and connected to a BA. The number of wires for each location can be easily deducted. 5. REERENCES [1] Hallgeir KLETTE Equipment codes, EMS No. 107834: Magnet System.

IP 1 Auxiliary bus-bars and connections for Short straight section correction scheme Sector 12 ( IP1 to IP2 ) Right of 1 Left of 2 IP2 Chromaticity Sext. S1,S1,S2,S2 1 1 1 1 2 2 2 2 2 2 2 2 2 2 2 2 1 1 2 2 2 2 2 1 1 1 1 2 2 2 2 1 2 2 2 2 2 2 1 1 1 2 2 2 2 1 1 2 2 2 2 2 2 2 1 2 1 1 1 2 2 2 Skew Sextupoles Octupoles, Skew Quads x 600A circuits 28 wires 14 19 x 600A circuits 38 wires Tuning Quads, Q11 to Q13 Trims, individually powered S Quad, individually powered BL 9 x 6 ka b.b. 12 x 6 ka b.b. 12 b.b. BM BM IP 1 LHC Project ocument No 8 x 6 ka circuits 12 bus-bars BA BA IP2 Version 6.4 optics LHC-CC-ES-0003 rev 3.0 / Annex N o 1 10 x 6 ka circuits 15 bus-bars P. Burla 10/09/2002

IP 2 Auxiliary bus-bars and connections for Short straight section correction scheme Sector 23 ( IP2 to IP3 ) Right of 2 Left of 3 IP3 Chromaticity Sext. S1,S1,S2,S2 1 1 1 1 2 2 2 2 2 2 2 2 2 2 2 2 1 1 2 2 2 2 2 1 1 1 1 2 2 2 2 1 2 2 2 2 2 2 1 1 1 2 2 2 2 1 1 2 2 2 2 2 2 2 1 2 1 1 1 2 2 2 Skew Sextupoles Octupoles, Skew Quads 19 x 600A circuits 38 wires x 600A circuits 28 wires 14 Tuning Quads, Q11 to Q13 Trims, individually powered S Quad, individually powered BM BM 12 b.b. BM 8 x 600A circuits 16 wires LHC Project ocument No LHC-CC-ES-0003 rev 3.0 / Annex N o 10 x 6 ka circuits BA 15 bus-bars IP 2 IP 3 Version 6.4 optics 2 BA P. Burla 10/09/2002

IP 3 Auxiliary bus-bars and connections for Short straight section correction scheme Sector 34 ( IP3 to IP4 ) Right of 3 Left of 4 IP4 Chromaticity Sext. S1,S1,S2,S2 1 2 2 2 2 2 2 1 1 1 2 2 2 2 1 1 2 2 2 2 2 2 2 1 2 1 1 1 2 2 2 1 1 1 1 2 2 2 2 2 2 2 2 2 2 2 2 1 1 2 2 2 2 2 1 1 1 1 2 2 2 2 Skew Sextupoles Octupoles, Skew Quads 14 x 600A circuits 28 wires 19 x 600A circuits 38 wires Tuning Quads, Q11 to Q13 Trims, individually powered S Quad, individually powered 8 x 600A circuits 16 wires LHC Project ocument No LHC-CC-ES-0003 rev 3.0 / Annex N o BM BL IP3 IP 4 BA 3 Version 6.4 optics 6 x 6 ka b.b. 12 x 6 ka b.b. BM's 8 x 6 ka circuits 12 bus-bars BA P. Burla 10/09/2002

IP 4 Auxiliary bus-bars and connections for Short straight section correction scheme Sector 45 ( IP4 to IP5 ) Right of 4 Left of 5 IP5 Chromaticity Sext. S1,S1,S2,S2 1 2 2 1 1 1 1 1 1 1 1 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 1 1 1 1 2 2 2 2 2 2 2 2 2 2 2 1 1 1 1 1 1 2 2 2 2 Skew Sextupoles Octupoles, Skew Quads 19 x 600A circuits 38 wires 14 x 600A circuits 28 wires Tuning Quads, Q11 to Q13 Trims, individually powered S Quad, individually powered BM's 6 x 6kA b.b. LHC Project ocument No 12x 6 ka b.b. 12 x 6 ka b.b. 8 x 6 ka circuits 12 bus-bars BA IP4 IP 5 Version 6.4 optics LHC-CC-ES-0003 rev 3.0 / Annex N o 4 8 x 6 ka circuits 12 bus-bars BA 9 x 6 ka b.b. BL P. Burla 10/09/2002

IP 5 Auxiliary bus-bars and connections for Short straight section correction scheme Sector 56 ( IP5 to IP6 ) Right of 5 Left of 6 IP6 Chromaticity Sext. S1,S1,S2,S2 1 1 1 1 2 2 2 2 2 2 2 2 2 2 2 2 1 1 2 2 2 2 2 1 1 1 1 2 2 2 2 1 2 2 2 2 2 2 1 1 1 2 2 2 2 1 1 2 2 2 2 2 2 2 1 2 1 1 1 2 2 2 Skew Sextupoles Octupoles, Skew Quads 14 x 600A circuits 32 wires 19 x 600A circuits 38 wires Tuning Quads, Q11 to Q13 Trims, individually powered S Quad, individually powered BL 9 x 6 ka b.b. 12 x 6 ka b.b. 9 b.b. BM BM LHC Project ocument No 8 x 6 ka circuits 12 bus-bars BA IP5 IP 6 Version 6.4 optics LHC-CC-ES-0003 rev 3.0 / Annex N o 5 6 x 6 ka circuits 9 bus-bars BA P. Burla 10/09/2002

IP 6 Auxiliary bus-bars and connections for Short straight section correction scheme Sector 67 ( IP6 to IP7 ) Right of 6 Left of 7 IP7 Chromaticity Sext. S1,S1,S2,S2 1 2 2 2 2 2 2 1 1 1 2 2 2 2 1 1 2 2 2 2 2 2 2 1 2 1 1 1 2 2 2 1 1 1 1 2 2 2 2 2 2 2 2 2 2 2 2 1 1 2 2 2 2 2 1 1 1 1 2 2 2 2 Skew Sextupoles Octupoles, Skew Quads 19 x 600A circuits 38 wires 14 x 600A circuits 28 wires Tuning Quads, Q11 to Q13 Trims, individually powered S Quad, individually powered BM BM 9 b.b. BM 8 x 600A circuits 16 wires LHC Project ocument No 6 x 6 ka circuits 9 bus-bars BA IP6 IP 7 Version 6.4 optics LHC-CC-ES-0003 rev 3.0 / Annex N o 6 BA P. Burla 10/09/2002

IP 7 Auxiliary bus-bars and connections for Short straight section correction scheme Sector 78 ( IP7 to IP8 ) Right of 7 Left of 8 IP8 Chromaticity Sext. S1,S1,S2,S2 1 1 1 1 2 2 2 2 2 2 2 2 2 2 2 2 1 1 2 2 2 2 2 1 1 1 1 2 2 2 2 1 2 2 1 2 2 1 2 2 1 2 2 1 2 1 2 2 2 2 2 1 2 2 1 2 2 1 2 2 1 2 Skew Sextupoles Octupoles, Skew Quads 14 x 600A circuits 28 wires 19 x 600A circuits 38 wires Tuning Quads, Q11 to Q13 Trims, individually powered S Quad, individually powered 8 x 600A circuits 16 wires BM 12 b.b. BM BM LHC Project ocument No 15 bus-bars IP7 IP 8 BA Version 6.4 optics LHC-CC-ES-0003 rev 3.0 / Annex N o 7 10 x 6 ka circuits BA P. Burla 10/09/2002

IP 8 Auxiliary bus-bars and connections for Short straight section correction scheme Sector 81 ( IP8 to IP1 ) Right of 8 Left of 1 IP1 Chromaticity Sext. S1,S1,S2,S2 2 2 1 1 1 1 1 1 1 1 1 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 1 1 1 1 2 2 2 2 2 2 2 2 2 2 2 1 1 1 1 1 1 2 2 2 2 Skew Sextupoles Octupoles, Skew Quads 19 x 600A circuits 38 wires 14 x 600A circuits 28 wires Tuning Quads, Q11 to Q13 Trims, individually powered S Quad, individually powered BM BM 12 b.b. 12 x 6 ka b.b. 9 x 6 ka b.b. BL LHC Project ocument No LHC-CC-ES-0003 rev 3.0 / Annex N o 10 x 6 ka circuits BA 15 bus-bars IP 8 IP 1 Version 6.4 optics 8 8 x 6 ka circuits 12 bus-bars BA P. Burla 10/09/2002