Some considerations about design and technology AE IS DT Science-Techno Tea meeting Diego Perini 29.04.09.

Slides:



Advertisements
Similar presentations
Results Conclusion Methods Samples Characterization of large size co-extruded Al-Ni stabilized Nb-Ti superconducting cable Objectives Background Stefanie.
Advertisements

Positrons for a New Measurement of the Positron Magnetic Moment Shannon Fogwell Hoogerheide Lepton Moments 2014 July 21, 2014.
Chapter 17 Current and Resistance 1. Electric current 2. Drift speed 3. Current and voltage measurement 4. Ohm’s law 5. Resistivity 6. Superconductivity.
HEL pre-design Diego Perini Superconducting solenoid Operation temperature: 4.2 K, current:about 250A, magnetic field: 5 Tesla Cooled by liquid.
1 Update on Focus Coil Design and Configuration M. A. Green, G. Barr, W. Lau, R. S. Senanayake, and S. Q. Yang University of Oxford Department of Physics.
1 The Genoa Tracker Solenoids and their Contribution toward a New Design Michael A. Green Lawrence Berkeley National Laboratory and Pasquale Fabbricatore.
1 Superconducting Magnets for the MICE Channel Michael A. Green Oxford University Physics Department Oxford OX1-3RH, UK.
Superconducting Solenoids for COMET KEK Cryogenics Center, Osaka Univ. Kuno-san’s Team, J-PARC MLF Muon Group.
CM-18 June Magnet Conductor Parameters and How They affect Conductor Selection for MICE Magnets Michael Green Lawrence Berkeley Laboratory Berkeley.
Twin Solenoid Twin Solenoid - conceptual design for FCC-hh detector magnet - Matthias GT Mentink Alexey Dudarev Helder Pais Da Silva Leonardo Erik Gerritse.
Status of the Polarized 3He Target
Development of Superconducting Magnets for Particle Accelerators and Detectors in High Energy Physics Takakazu Shintomi and Akira Yamamoto On behalf of.
TRANSFORMERS?. Effects of electric current An electric current that flows in a conductor has a number of effects: 1. HEATING The friction caused by the.
Superconducting Magnet R&D for COMET Makoto Yoshida (KEK) NuFact Aug, 2011.
A basic property of the tiny particles that make up matter; it can be positive or negative: Some particles of matter have an electric charge. Electric.
Construction of Wendelstein 7-X Max-Planck-Institut für Plasmaphysik
16th Crystal Ball Meeting October, 11-13, 2010, Dubrovnik Grigory Gurevich, Yuri Usov Dubna-Mainz Dilution Cryostat of the New Frozen-Spin Target.
Martin Wilson Lecture 1 slide 1 JUAS February 2012 NbTi manufacture vacuum melting of NbTi billets hot extrusion of the copper NbTi composite sequence.
1 A Joint Proposal for US-Japan Cooperation Program Proposal to JSPS US-Japan collaboration fund R&D of superconducting magnet technology for high intensity.
Possible HTS wire implementation Amalia Ballarino Care HHH Working Meeting LHC beam-beam effects and beam-beam interaction CERN, 28 th August 2008.
Status of CEPC Detector magnet
Ultra-Compact Electrical Machines for Wind Energy DE-FOA : Demo Machine C. L. Goodzeit and M. J. Ball May 1, 2014 Part 1: Design and Construction.
M. Modena, A. Aloev CERN, Geneva, CH “An alternative Super-ferric design for ILC QD0” “LCWS14, 6-10 October 2014 Belgrade.
Study of Pion Capture Solenoids for PRISM H.Ohnishi AB M. Aoki C, Y. Ajima A, N. Fukasawa AD, K. Ishibashi B, Y. Kuno C, T. Miura A, K. Nakahara C, T.
KEK Hiroshi Yamaoka Task list for Magnet/Iron yoke Solenoid magnet Iron yoke Experimental hall and other facilities May 11, ’05.
Zian Zhu Magnet parameters Coil/Cryostat/Support design Magnetic field analysis Cryogenics Iron yoke structure Mechanical Integration Superconducting Magnet.
UCRL-PRES Magnet Design Considerations & Efficiency Advantages of Magnetic Diversion Concept W. Meier & N. Martovetsky LLNL HAPL Program Meeting.
February 13, 2012 Mu2e Production Solenoid Design V.V. Kashikhin Workshop on Radiation Effects in Superconducting Magnet Materials (RESMM'12)
Review-LHC Interaction Regions - Upgrade Phase I Amalia Ballarino, 31 st July 2008 Cold Powering Options Conceptual Design Review of the LHC Interaction.

Superconducting Magnet Group Superconducting magnet development for ex-situ NMR LDRD 2003 Paolo Ferracin, Scott Bartlett 03/31/2003.
CONSTRUCTION AND TEST OF A TRANSVERSE SUPERCONDUCTING HOLDING MAGNET 15th CB Meeting Mainz March 8th, 2010 Henry G. Ortega Spina.
Monday, April 23, PHYS , Spring 2007 Dr. Andrew Brandt PHYS 1444 – Section 004 Lecture #19 Monday, April 23, 2007 Dr. Andrew Brandt Inductance.
EDM Engineering Issues General Mechanical Considerations EDM Cryostat Plan D ANSYS EMAG Calculations ANSYS MECH Calculations 3 June ‘03 J. Boissevain.
Status of work on the project # (VNIINM) Team leader -V.Pantsyrny June 20071INTAS-GSI Meeting, Darmstadt.
XVII SuperB Workshop and Kick Off Meeting - La Biodola (Isola d'Elba) Italy May 28 th June 2 nd 2011 P.Fabbricatore Sezione di Genova The air core magnets.
MICE CC Magnet Cryostat Design Overview Derun Li Center for Beam Physics Lawrence Berkeley National Laboratory MICE CC Cryostat Design Review LBNL, February.
FNAL Workshop, July 19, 2007 ILC Main Linac Superconducting Quadrupole V.Kashikhin 1 ILC Main Linac Superconducting Quadrupole (ILC HGQ1) V. Kashikhin.
Superconducting Cryogen Free Splittable Quadrupole for Linear Accelerators Progress Report V. Kashikhin for the FNAL Superconducting Magnet Team (presented.
CHATS-AS 2011clam1 Integrated analysis of quench propagation in a system of magnetically coupled solenoids CHATS-AS 2011 Claudio Marinucci, Luca Bottura,
HTS and LTS Magnet Design and Prototyping for RAON
Test of QD0 Riccardo Musenich INFN-Genova SuperB 2 nd Collaboration Meeting Frascati, December
Superconducting Magnet for high energy Physics Jong-Seo CHAI SKKU 成均館大學校 Japan-Korea Phenix Meeting November 27, 2012.
Studies of the Cryogenic Part with Load Lock System T. Eisel, CERN TE-CRG-CI AEgIS November 11 th, 2010 Page 1 Cryolab Cooling of electrically insulated.
Status of the QD0 design S. Bettoni on behalf of the whole team
CERN co-worker: Thomas Eisel (lecturer) Diego Perini Friedrich Haug
Organization of proposed cryolab collaboration with AEGIS
Traps for antiprotons, electrons and positrons in the 5 T and 1 T magnetic fields G. Testera & Genoa group AEGIS main magnetic field (on axis) : from Alexei.
AEGIS positron transfer line
Superconducting magnet
Quench estimations of the CBM magnet
Yury Ivanyushenkov for the UK heLiCal Collaboration
AEGIS Magnet System.
The CMS magnet superconducting coil
INTER UNIVERSITY ACCELERATOR CENTER, INDIA
ROX sensor packaging and mounting scheme for use on dilution STM sample plates Ben MacLeod Jan
PHYS 1444 – Section 02 Lecture #19
Mike Sumption, M. Majoros, C. Myers, and E.W. Collings
Cable and Strand test facility
CEA Nb3Sn quadrupole magnet : test results and future
PHYS 1444 – Section 003 Lecture #21
I. Bogdanov, S. Kozub, V. Pokrovsky, L. Shirshov,
BESIII Collaboration Meeting, June 5~6, 2002, Zian Zhu
Preliminary study of HTS option for CEPC detector magnet
11T Dipole for the LHC Collimation upgrade
Forms of Energy Unit 3 Part 2 Vocabulary.
The superconducting solenoids for the Super Charm-Tau Factory detector
Quench calculations of the CBM magnet
CEPC Final Focus Superconducting Quadrupole and Anti-solenoid Magnets
Budker Institute of Nuclear Physics,
Presentation transcript:

Some considerations about design and technology AE IS DT Science-Techno Tea meeting Diego Perini

Alexey Dudarevmagnets Johan Bremercryostats Thomas Eisel & Friedrich Haug refrigerator Tapio Niinikoski Lionel Metral DT colleagues: Bernard Cantin Francois Garnier Pierre-Ange Giudici Luc Kottelat Philippe Lenoir

What do we need for AEgIS? - Very cold region, 50 mK (dilution refrigerator) - Magnetic field to confine particles, 5T and 1T regions. Superconducting coils Cryostat - Positron accumulator - Traps, - Laser system, - Positronium target and supports, - Anti-H detector, - Deflectometer.

Very cold environment

Dilution refrigerator. The mixing chamber is inside a solenoid and in HV.

Mixing chamber and traps The need of having both electrical insulation and thermal conductivity At these temperatures Indium is superconducting.

Superconducting solenoids

Coils: Layout Precise magnetic field  main coils + correction coils Measurements after construction to understand the system 5T 1T 0T>0.7T

Coils: Homogeneity (%) 5 T region 1 T region

Böhler P506 - C 0.012, Si 0.23, Mn 12.05, P 0.005, S 0.001, Cr 19.18, Mo 0.86, Ni 10.90, Cu 0.04, Co<0.05, B<0.001, N 0.33

Superconducting coils NbTi superconductor embedded in Cu matrix At 4.2 K current passes through NbTi (superconductor, R ~ 0) In normal state (ex. In case of quench) resistivity of NbTi > Cu so the copper carries the current. Cu gives mechanical stability and is an heat sink. Thin filaments (some  m) since current flows skin-deep. Cables are produced by extrusion starting from billets. Winding is a delicate job – see Pierre–Ange’s presentation Number of filaments 42 Cu/Sc ratio 4.0 Wire dimensions (bare) 1.19 x 0.74 mm Insulated 1.25 x 0.80 mm +/ mm 5T 400 A

Cryostat

“Easy to open” structure Rails and stoppers

Services for the traps and the mixing chamber, laser system, mechanical supports, thermal screens. One have to Minimize the power dissipation at 50 mK. Detector 80K Target Mixing chamber 50 mK Coils 4.2K 200 mm The very crowded central region

Positron accumulator