Support and magnet coil KEK Hiroshi Yamaoka Nov. 10, ‘04.

Slides:



Advertisements
Similar presentations
Q1 for JLAB’s 12 Gev/c Super High Momentum Spectrometer S.R. Lassiter, P.B. Brindza, M. J. Fowler, S.R. Milward, P. Penfold, R. Locke Q1 SHMS HMS Q2 Q3.
Advertisements

Mechanical Analysis of Dipole with Partial Keystone Cable for the SIS300 A finite element analysis has been performed to optimize the stresses in the dipole.
Zian Zhu Superconducting Solenoid Magnet BESIII Workshop Zian Zhu Beijing, Oct.13,2001.
Challenges in High Field Solenoids A. Hervé / ETHZ CLIC09-Workshop,13 October 2009.
IR Magnets for SuperKEKB KEK, Norihito Ohuchi 1.IR Magnets (ES, QCS, QC1) 2.Interference between Magnet-Cryostats and Belle 3.Summary SuperB.WS05.Hawaii.
Spectrometer Solenoid Design and Procurement Review Steve Virostek Mike Green Mike Zisman Lawrence Berkeley National Lab MICE Collaboration Meeting October.
Tracker Solenoid Module Design Update Steve VirostekStephanie Yang Mike GreenWing Lau Lawrence Berkeley National LabOxford Physics MICE Collaboration Meeting.
Preliminary Analysis of the Target System Magnets 1.Version with a 6-T copper magnet insert 2.Version with a 6-T high-temperature superconductor insert.
Talk outline 1 st talk: –Magnetic forces –Quench in the absorber cryostat 2 nd talk: –Shielding of magnetic fringe fields.
“GLD” Detector Concept Study 21. Mar. Y. Sugimoto KEK.
Twin Solenoid Twin Solenoid - conceptual design for FCC-hh detector magnet - Matthias GT Mentink Alexey Dudarev Helder Pais Da Silva Leonardo Erik Gerritse.
Superconducting Large Bore Sextupole for ILC
MCTF Alexander Zlobin MUTAC Meeting 8-10 April MCTF Magnet and HTS Conductor R&D.
1 超伝導電磁石/鉄ヨーク/実験室について 高エネルギー加速器研究機構 山岡 広 田中 賢一 目 次 ・概 要 ・ 超伝導電磁石について ・ 鉄ヨークについて ・ 実験室について ・まとめ Jun. 28, ‘06.
1 Design of Solenoid and iron yoke for GLD KEK Hiroshi Yamaoka Ken-ichi Tanaka July 13, ‘05.
Zhiwen Zhao (UVa), Paul Reimer (ANL) SoLID Collboration Meeting 2013/03.
CD meeting R.Yamada1 Thoughts on 4CD (4 th Concept Detector) Solenoid System based on Alex Mikhailchenko’s Basic Design Ryuji Yamada October 20,
Status of CEPC Detector magnet
Joint Institute for Nuclear Research Further optimization of the solenoid design A.Efremov, E.Koshurnikov, Yu.Lobanov, A.Makarov, A.Vodopianov GSI, Darmstadt,
SC magnet developments at CEA/Saclay Maria Durante Hélène Felice CEA Saclay DSM/DAPNIA/SACM/LEAS.
CERN Accelerator School, Erice 2013 Tiepida-2 case-study 3: High field – large aperture magnet for a cable facility TiEpIdA2 design team: I. Mondino: Project.
KEK Hiroshi Yamaoka Task list for Magnet/Iron yoke Solenoid magnet Iron yoke Experimental hall and other facilities May 11, ’05.
Focusing Lens for the SSR1 Section of PXIE Preliminary analysis of main options 3/13/2012I. Terechkine1.
Zian Zhu Magnet parameters Coil/Cryostat/Support design Magnetic field analysis Cryogenics Iron yoke structure Mechanical Integration Superconducting Magnet.
1 Detector magnet and Structure for the GLD Detector KEK Hiroshi Yamaoka Mar. 03, ‘05.
February 13, 2012 Mu2e Production Solenoid Design V.V. Kashikhin Workshop on Radiation Effects in Superconducting Magnet Materials (RESMM'12)
CEA DSM Irfu - F. KIRCHER - [Seoul Workshop, Feb 16-18, 2009] 1 ILD detector magnet: LoI version F. Kircher, O. Delferrière CEA Saclay, DSM/Irfu/SACM.
Magnets and Supports Bob Wands October 20, 2006 PPD/MD/Engineering Analysis Group Fermilab 4 th Concept Detector at Fermilab October, 2006.
R. Bonomi R. Kleindienst J. Munilla Lopez M. Chaibi E. Rogez CERN Accelerator School, Erice 2013 CASE STUDY 1: Group 1C Nb 3 Sn Quadrupole Magnet.
CERN Accelerator School Superconductivity for Accelerators Case study 1 Paolo Ferracin ( ) European Organization for Nuclear Research.
Mechanical Designs of The Central Detector Jinyu Fu
1 Mechanical calculations of the CDC end-plates KEK H. Yamaoka July 8 th, '09 KEK H. Yamaoka.
56 MHz SRF Cavity Cryostat support system and Shielding C. Pai
New options for the new D1 magnet Qingjin Xu
Muon Cooling Channel Superconducting Magnet Systems Muon Collider Task Force Meeting on July 31, 2006 V.S. Kashikhin.
CERN Accelerator School Superconductivity for Accelerators Case study 3 Paolo Ferracin ( ) European Organization for Nuclear Research.
1. Introduction 2. Magnetic field design Optimization of yoke configuration in several conf. Boundary conditions -
Design of wide aperture/thin septa of extraction system for J-PARC-50GeV ring 1. The outline of septa system for 50GeVring 2. Designing of thin septa and.
Super Fragment Separator (Super-FRS) Machine and Magnets H. Leibrock, GSI Darmstadt Review on Cryogenics, February 27th, 2012, GSI Darmstadt.
MICE CC Magnet Cryostat Design Overview Derun Li Center for Beam Physics Lawrence Berkeley National Laboratory MICE CC Cryostat Design Review LBNL, February.
Joint Institute for Nuclear Research Deformations and stresses in the flux return yoke A.Efremov, Yu.Lobanov, A.Makarov Darmstadt,
Thermal screen of the cryostat Presented by Evgeny Koshurnikov, GSI, Darmstadt September 8, 2015 Joint Institute for Nuclear Research (Dubna)
QXF magnet integration Paolo Ferracin Joint LARP/CM20 HiLumi meeting Napa Valley, CA, USA 8-10 April, 2013.
FNAL Workshop, July 19, 2007 ILC Main Linac Superconducting Quadrupole V.Kashikhin 1 ILC Main Linac Superconducting Quadrupole (ILC HGQ1) V. Kashikhin.
F. Kircher CLIC concept meeting 12/15/08 1 Some points about the superconducting magnet for a CLIC detector F. Kircher (CEA Saclay/DSM/Irfu/SACM) December.
Preliminary analysis of a 16 T sc dipole with cos-theta lay-out INFN team October 2015.
Update on PANDA solenoid design and analysis Gabriella Rolando Helder Pais Da Silva Herman ten Kate Alexey Dudarev 3 November
Design ideas for a cos(2q) magnet
Present status of the flux return yoke design
PANDA Yoke of the Magnet
The CMS magnet superconducting coil
Development of the Canted Cosine Theta Superconducting Magnet
Status of Detector Solenoid and Anti-DID
Vibration studies for the QD0-support system
SiD Solenoid Status and Plans
EuroCirCol: 16T dipole based on common coils
Analytical Cost Model (16 T dipole)
CDC Structure S. Uno KEK
SoLID Magnet - Engineering and Cost
BESIII Collaboration Meeting, June 5~6, 2002, Zian Zhu
11T Dipole for the LHC Collimation upgrade
MQXF coil cross-section status
CERN Accelerator School Superconductivity for Accelerators Case study 2 Paolo Ferracin European Organization for Nuclear Research.
Design of Nb3Sn IR quadrupoles with apertures larger than 120 mm
The superconducting solenoids for the Super Charm-Tau Factory detector
CDC structure Shoji Uno (KEK)    July-8, 2009.
Design of Nb3Sn IR quadrupoles with apertures larger than 120 mm
Budker Institute of Nuclear Physics,
Qingjin XU Institute of High Energy Physics (IHEP),
Cross-section of the 150 mm aperture case
Presentation transcript:

Support and magnet coil KEK Hiroshi Yamaoka Nov. 10, ‘04

Initial configuration of the iron yoke Further amount of iron is necessary. → Too large!! Iron Yoke configuration is optimized! 3T

Material for return yoke S10C(JIS) Carbon= 0.1wt%  t =310MPa  e =205MPa  allow =120MPa Permeability These dimensions are fixed, Coil length, yoke dimensions are changed. Belle

Calculations dz Coil-L 4.25m

R2.05m R1.8m R0.4m R1.0m 0 2 1

Fringe/Leakage field Flux line Magnetic field distribution

Max. 1.8mm Max. 90MPa<120MPa 18000tons Fixed Stress/deformation of End Yoke

Max. 7mm Max. 65MPa<120MPa Stress/deformation of Barrel Yoke 13300tons Fixed

4.2mm 30mm 4.3mm Aluminum stabilized superconductor NbTi:Cu:Al= 1:0.9:15.6 Strand diameter: 1.23mm Filament diameter: 20  m Jc in NbTi at 5T, 4.2K: > 2750A/mm 2 Ic at 5T, 4.2K: > 20300A (For ATLAS) Superconducting Solenoid

Circum. direction Axial direction Compression Stress level in the coil Development of High-strength Al 4.93m(Half) R4.0m Support cylinder (t=50mm) Conductor (h=30mm) 8mm 4mm Deformation of the coil Solenoid center By Makida

- Outer vac. vessel 40mm thick p: Buckling pressure 0.1MPa x 2(safety factor) 2000tons Fixed Thickness of ・ Inner vacuum vessel ・ End plates were optimized. Load condition Weight of the calorimeter: 2000tons Weight of the solenoid : ~ 140tons Vacuum : 0.1MPa Cryostat design SUS304  t =530MPa  y =210MPa  allow =140MPa 2000tons Fixed Model-1 Model-2 Oct. 29, ’04 KEK H. Yamaoka

118MPa<140MPa 9mm t=40mm t=60mm t=100mm 274MPa>140MPa 15mm 2000tons Fixed 2000tons Fixed t=40mm t=60mm t=100mm 2000tons x 0.3G Fixed 9mm 125MPa Stiffness: D E: Young’s modulus I: Moment of Inertia Model-1Model-2 Material: SUS304

Requests to calorimeter structure; - Calorimeter is divided to several pieces in the axial direction. - One piece of calorimeter is stiff enough. 5250(Half) 4930(Half) R4000 R3720 R4400 t=50mm t30mm, 2 layers *Detail design is not yet done. *Coil support system is not designed yet.

Feb. 14, ’02 H. Y Cost estimation of Return Yoke ○ Law material \180/kg x 11000e3kg = \19.8 oku +  (10%) 19.8x1.1=21.8 oku ○ Machining Total area for machining of Barrel yoke 340m 2 End Yoke: 501m 2 Machining cost per 1m 2 \200000/m 2 Total: ( )m2x20 万 =16.8 oku +  (10%) 、 16.8x1.1=18.5 oku ○ Design cost 1 oku ○ Cost for QC 0.5 oku ○ 利益率 20 %とすると、 41.8x0.2=8.4 oku Total 50.2 okux1.05= 52.7 oku Cost estimation of Solenoid

The way for improving field uniformity Solenoid magnet Z2 R2 R1 Z1 ・ Plenty of amount of iron ・ Minimize Z1,R1 ・ Optimize Z2,R2 3T Saturation