12 July 2007IRENG07 WG-A M. Breidenbach1 SiD Concept SiD is relatively modest in scale compared to the LHC detectors, and comparable to SLD: Tracker Radius.

Slides:



Advertisements
Similar presentations
BARTOSZEK ENGINEERING 1 The Design of the Booster Collimators Larry Bartoszek BARTOSZEK ENGINEERING 3/10/03.
Advertisements

STAR Detector Main Support System1 Lateral Tracking of the STAR Detector during Translation. November 23, 2005 Ralph L. Brown STAR Operations Group.
Mu2e Production Target Remote Handling By: Michael R. Campbell, Fermi National Accelerator Laboratory, , System Layout Basic.
Zian Zhu Superconducting Solenoid Magnet BESIII Workshop Zian Zhu Beijing, Oct.13,2001.
Assembly Hall in Hybrid-A’ and ILD 2014/9/6 Yasuhiro Sugimoto 1.
SiD assembly Marco Oriunno (SLAC), May. 14, 2014 ALCW 2014, Fermilab Infrastructures & Timeline for Hybrid Access.
Global Design Effort Detector concept # Plenary introductory talk IRENG07 Name September 17, 2007.
NLC - The Next Linear Collider Project IR Layout Tom Markiewicz SLAC LCWS Cornell 15 July 2003.
1 Installation of Delphi Frame  ITS Installation.
Tagger and Vacuum Chamber Design. Outline. Design considerations. Stresses and deformations. Mechanical assembly.
1 Status of infrastructure MICE Video Conference, August 17, 2005 Yury Ivanyushenkov Applied Science Division, Engineering and Instrumentation Department.
October 22, 2003H.J. Krebs1 LST Mechanical Design Review Mechanical Installation Preparation H. James Krebs October 21, 2003.
DH in Hybrid-A and ILD 2014/9/5 Yasuhiro Sugimoto 1.
Experimental hall in Japanese mountain site Y. Sugimoto ILD MDI/Integration 1.
Loading Considerations © 2000 Dr. B. C. Paul revisions 2009 Note These slides include screen shots from the Caterpillar Performance Manual Edition 29.
Push Pull Considerations
Global Design Effort Detector concept Plenary introductory talk IRENG07 Kurt Krempetz September 17, 2007.
3 March 2009M. Breidenbach1 SiD LoI Costs M. Breidenbach.
1 Design of Solenoid and iron yoke for GLD KEK Hiroshi Yamaoka Ken-ichi Tanaka July 13, ‘05.
1 ILD/CMS Engineering Meeting M. Joré – ILD integration philosophy Integration philosophy of ILD Matthieu Joré – January 21st Integration of the subdetectors.
Experimental hall in Japanese mountain site Y. Sugimoto 1.
CLIC main detector solenoid and anti-solenoid impact B. Dalena, A. Bartalesi, R. Appleby, H. Gerwig, D. Swoboda, M. Modena, D. Schulte, R. Tomás.
Hcal Geometry and Assembly CLIC Meeting - LAPP December 2008, 15th.
1 Discussion for basic options — engineering video conference July 12, 2006 Outline Water pool — advantages — issues, problems, engineering options Aquarium.
1 ILC Push-Pull : Platform Marco Oriunno, SLAC ILD Workshop, Paris May 24, 2011.
ASTeC Report for CLIC-UK Jim Clarke on behalf of all ASTeC & Technology Department staff contributing to CLIC-UK STFC Daresbury Laboratory, UK CERN-UK.
Philip Burrows SiD Meeting, Paris 11/02/081 Machine Detector Interface Issues Philip Burrows John Adams Institute Oxford University Thanks to: Tom Markiewicz.
September 18, 2007H. J. Krebs1 SiD Collaboration One Piece End Door Design Concept plus Forward Equipment Interfaces H. James Krebs SLAC September 18,
SiD IR & MDI Engineering Progress Prelude to a Discussion of Integration with ILD and Based on Marco Oriunno’s Jan 2008 Talk at SiD CM Tom Markiewicz/SLAC.
Detector design optimization for push-pull IR and for surface assembly and corresponding IR requirements Tom Markiewicz/SLAC SLAC BDS Kick-Off-Meeting.
SiD MDI Marco Oriunno, SLAC ALCPG11 Eugene- Oregon, March 2011.
CLIC Permanent Magnet Quadrupole Engineering Development of second family member Norbert Collomb, STFC Daresbury Laboratory 1N. Collomb 07/11/2012.
1 SiD Push-pull Plans Marco Oriunno, SLAC International Workshop on Linear Colliders 2010 Geneva, October 2010 M.Oriunno, IWLC10 – Geneva, Oct.2010.
Date Event Global Design Effort 1 Platform Moved on Hillman Rollers, Deformations John W. Amann ILC – Mechanical Engineering 9/12/07 IREng07.
G.Barber Mice Tracker Mechanical Progress Tracker Mechanical Progress Contents:- Station Space Frame Station Layout Light Guide Map Connectors Patch.
SiD Collaboration Meeting Highlights Tom Markiewicz/SLAC ILC BDS Meeting 08 May 2007.
Presentation by ANAS AHMAD ME1 B1 batch Submited to
FD Movers and Alignment Methods Superconducting Magnet Division, BNL IRENG07 Workshop: September 19, 2007.
SiD MDI Issues Tom Markiewicz/SLAC Beijing ACFA/GDE Meeting 05 February 2007.
BY B.JITHENDRA KUMAR Shaper Machine. Introduction The shaping machine is used to machine flat metal surfaces especially where a large amount of metal.
SHAPER MACHINE Name: Jaypalsinh Jadeja Roll no.: 13ME517 Division: Mech- Q.
MEA Machine and Experiment Assembly Norbert Meyners, MEA 12. July 2007ILC IRENG07 WG-A1 LDC Engineering Design (Status) Introduction General Design Detector.
Joint Institute for Nuclear Research Deformations and stresses in the flux return yoke A.Efremov, Yu.Lobanov, A.Makarov Darmstadt,
Page 1 GSI, Hydraulic Actuators for PANDA Target Spectrometer Jost Lühning, GSI Darmstadt Functional Specifications for moving the TS: Two synchronous.
Status of the Yoke Interfaces Presented by Evgeny Koshurnikov February 2013.
ROLLING Rolling is a process of reduction of the cross-sectional area or shaping a metal piece through the deformation caused by a pair of metal rolls.
Status of the PANDA Magnet Yoke Presented by E. Koshurnikov GSI, June 26, 2013.
M.Oriunno, SLAC 1 SiD installation with horizontal access shafts Marco Oriunno, SLAC SiD/ILD Engineering Meeting SLAC, December 2011.
Miscellaneous MEC Topics Mainz, CM September 2016, MEC Session J
Roller/rail - System for PANDA
SiD Collaboration Meeting SLAC, December 2011
CBM magnet overview of the BINP work
Platform for moving and positioning Target Spectrometer on the floor
Platform Design for the Target Spectrometer using Heavy-Weight Rollers J. Lühning, GSI Darmstadt, Three design goals for Platform: Low construction.
Solenoid Yoke Door-Barrel Connection
Present status of the flux return yoke design
Layout of Detectors for CLIC
Platform for Target Spectrometer using linear montion drive Rexroth
SiD Muon Yoke Structure - Deformation Studies -
Design Concept Update – Platform Moved on Hillman Rollers
SiD LoI Costs M. Breidenbach 29 July 2010 M. Breidenbach.
Detector hall in mountain regions
Integration and IR Hall
SiD IR Layout M. Breidenbach, P. Burrows, T. Markiewicz
Detector hall in mountain regions
ILC Detector Technology
SiD IR Layout M. Breidenbach, P. Burrows, T. Markiewicz
CLEO II Magnet in Hall A for SoLID
as a prototype for Super c-tau factory
Some of the Points Raised During my JLAB Visit
Presentation transcript:

12 July 2007IRENG07 WG-A M. Breidenbach1 SiD Concept SiD is relatively modest in scale compared to the LHC detectors, and comparable to SLD: Tracker Radius Inner Coil Radius Outer Iron Radius Half Length to pole face Total Mass (Ktonne) SLD ~4 SiD ~9

12 July 2007IRENG07 WG-A M. Breidenbach2 SLD

12 July 2007IRENG07 WG-A M. Breidenbach3 SiD

12 July 2007IRENG07 WG-A M. Breidenbach4 Comments Overall mechanical approach to SiD similar to SLD – but must emphasize very little engineering done so far. Iron yoke supported from “exoskeleton” frame at each end. –End frames tied together by return yoke. –End frames carry doors when detector is traveling. –Return yoke take magnetic compressive force of doors. Doors are not split. Motivation for split door appears to be that components of forward calorimetry could have larger radius than door opening. SiD has avoided this. –No “seams” in endcap tracking or calorimetry or muon tracking. –Stronger structure to take magnetic forces. –Fewer pieces to move.

12 July 2007IRENG07 WG-A M. Breidenbach5 Comments Doors retract along Z axis. –Simple 1-D motion. –Works well with beamline shielding (Pacmen) –Sliding support for final lens (needs active compensation as door retracts). –~2m motion for people access. This approach worked well for SLD: –Designed for (and tested in!) major earthquake. –Measured transverse motion of SLC lens package ~50 nm (spec was 0.5 micrometer – SLC achieved much smaller beams vertically than expected, so extra stability was nice!) –Door opening or closing ~2 hours (including everything, but with practice). Cryogenic systems (LArgon calorimeters, superconducting quads undisturbed (but quads run down). –Simple alignment system put final quads within 1 mm of beamline. Beam based alignment and tuning to full luminosity < 8 hours. –Doors moved on Hilman Rollers on flat rails, with pitch, roll, and elevation adjustment from computer controlled hydraulic jacks. (Jacks ~never used after initial alignment). Drive was hydraulic motors to ball screws.

12 July 2007IRENG07 WG-A M. Breidenbach6 Is a platform needed for Push-Pull? A platform may be motivated by the basic detector architecture – e.g. a legless structure might need a platform. A stiff platform might be useful if the detector is floppy – but a stiff platform needs some height – which is likely to increase the beamline elevation in the IR Hall – which is probably expensive. A stiff platform might be useful if the floor is uneven – but see above. It seems relatively easy to adjust detector leg length hydraulically. (A 560 ton hydraulic jack with a follow nut costs ~$9K) The floor may move when loaded and unloaded on a scale that must be corrected. A platform doesn’t directly address this. A platform could carry auxiliary equipment, such as the solenoid power supply, dump resistors, etc. It seems plausible that this kind of equipment could be on platforms on top and on the sides of the detector, which would not raise the beamline.

12 July 2007IRENG07 WG-A M. Breidenbach7 Comments A platform provides a transversely stiff support for the detector so it can be pushed or pulled without distorting the structure. True- but this would appear to need some analysis to compare the costs of a platform to the costs of struts between the legs to get the necessary stiffness. SLD moved on ton Hilman Rollers supporting 500 ton jacks, pushed by long stroke jacks. Worked well, but would not copy for SiD. Would suggest looking at roller system on a guide track, and moved by a ball screw(s). Whatever the motion system is, it should be a detector responsibility and cost!