KT McDonald Target Studies Meeting June 14, 2011 1 Mechanical Issues for the Target System K. McDonald Princeton U. (June 14, 2011) Target Studies Meeting.

Slides:



Advertisements
Similar presentations
Mercury Chamber Update V. Graves NF-IDS Meeting October 4, 2011.
Advertisements

Zian Zhu Superconducting Solenoid Magnet BESIII Workshop Zian Zhu Beijing, Oct.13,2001.
MICE Superconducting Solenoids: Status and Update RAL: T W Bradshaw M Courthold J Rochford M Hills D Baynham Oxford: J Cobb W Lau S Yang MICE.
A Neutrino Factory Target Station Design based on Solid Targets J. R. J. Bennett STFC, Rutherford Appleton Laboratory, Harwell Science.
Managed by UT-Battelle for the Department of Energy Neutrino Factory Mercury Containment Concepts V.B. Graves 2 nd Oxford-Princeton High- Powered Target.
Neutrino Factory Target Cryostat Review Van Graves Cale Caldwell IDS-NF Phone Meeting August 10, 2010.
Neutrino Factory Mercury Flow Loop V. Graves C. Caldwell IDS-NF Videoconference March 9, 2010.
Particle Production of a Carbon/Mercury Target System for the Intensity Frontier X. Ding, UCLA H.G. Kirk, BNL K.T. McDonald, Princeton Univ MAP Spring.
K.T. McDonald March 18, 2010 LArTPC BNL 1 Magnetizing a Large Liquid Argon Detector Kirk T. McDonald Princeton University (March 18, 2010)
1Managed by UT-Battelle for the U.S. Department of Energy MERIT Videoconference 11 Mar 2009 Neutrino Factory Cryostat 1 Concept V.B. Graves MERIT Videoconference.
Operated by Brookhaven Science Associates for the U.S. Department of Energy A Pion Production and Capture System for a 4 MW Target Station X. Ding, D.
1Managed by UT-Battelle for the U.S. Department of Energy NF/IDS Hg Vessel Layout 30 Jun 09 Cryostat 2 Front Drain Mercury Vessel Concept Matthew F. Glisson.
Progress on the MICE Cooling Channel Solenoid Magnet System
Global Design Effort Detector concept # Plenary introductory talk IRENG07 Name September 17, 2007.
SHIELDING STUDIES FOR THE MUON COLLIDER TARGET NICHOLAS SOUCHLAS BNL Nov 30, 2010 ‏ 1.
NUMI NuMI Hot Handling Jim Hylen (FNAL) NBI02 March 13, 2002 Page 1 NuMI Target Hall Radioactive Component Handling NuMI Target Hall Utilizes Three Basic.
KT McDonald Muon Collider 2011 June 28, The Target System Baseline K. McDonald Princeton U. (June 28, 2011) Muon Collider 2011 Telluride, CO More.
Above: Energy deposition in the superconducting magnet and the tungsten-carbide shield inside them. Approximately 2.4 MW must be dissipated in the shield.
May 17-19, 2000 Catalina Island, CA Neutrino Factory and Muon Collider Collaboration Meeting 1 Target Support Facility for a Solid Target Neutrino Production.
Harold G. Kirk Brookhaven National Laboratory Target System Update IDS-NF Plenary Meeting Arlington, VA October 18, 2011.
Harold G. Kirk Brookhaven National Laboratory Target Baseline IDS-NF Plenary CERN March 23-24, 2009.
1Managed by UT-Battelle for the U.S. Department of Energy NMFCC Friday Meeting 10 Apr 2009 Neutrino Factory Nozzle Layouts V.B. Graves NFMCC Friday Meeting.
IDS-NF Target Studies H. Kirk (BNL) July 8, 2009.
TAGGER MAGNET DESIGN Presented by Tim Whitlatch Hall D Tagger Magnet Design Review July 10,
Above: Power deposition in the superconducting magnets and the tungsten-carbide + water shield inside them, according to a FLUKA simulation Approximately.
Above: On-axis field profiles of resistive, superconducting and all magnets, and bore-tube radius r = 7.5 (B/20T) −½ cm. Above: Hoop strain ε θ in resistive.
Managed by UT-Battelle for the Department of Energy Review of NFMCC Studies 1 and 2: Target Support Facilities V.B. Graves Meeting on High Power Targets.
Mercury Chamber Considerations V. Graves IDS-NF Target Studies July 2011.
Solid Target Options NuFACT’00 S. Childress Solid Target Options The choice of a primary beam target for the neutrino factory, with beam power of
Front End Technologies Harold Kirk Brookhaven National Laboratory February 19, 2014.
IDS-NF Mercury System Overview Van Graves IDS-NF 5 th Plenary Meeting April 9, 2010.
Target and Absorbers L2 Manager: K McDonald, Princeton U March xx, 2013 Presenter’s Name | DOE Mini-Review of MAP (FNAL, March 4-6, 2013)1 Mission Target:
Progress on the MuCool and MICE Coupling Coils * L. Wang a, X. K Liu a, F. Y. Xu a, A. B. Chen a, H. Pan a, H. Wu a, X. L. Guo a, S. X Zheng a, D. Summers.
KT McDonald MAP Spring Meeting May 30, Target System Concept for a Muon Collider/Neutrino Factory K.T. McDonald Princeton University (May 28, 2014)
KT McDonald MAP Winter Meeting (SLAC) December 5, Solid Target Options for an Intense Muon Source K. McDonald Princeton U. (December 5, 2014) MAP.
Spectrometer Solenoid Test Plan Workshop: Spectrometer Solenoid Overview Steve Virostek - LBNL February 17, 2012.
Review of Recent IDS120 Target Concepts Van Graves October 31, 2013.
20to2T5m100cm Images Van Graves February 13, 2014.
K. McDonald Target Studies Meeting June 29, Materials for the Target System Internal Shield K. McDonald Princeton U. (June 27, 2010) Iron Plug Proton.
SHIELDING STUDIES FOR THE MUON COLLIDER TARGET. (From STUDY II to IDS120f geometries) NICHOLAS SOUCHLAS (BNL)‏ ‏ 1.
KT McDonald MAP Tech Board Meeting Oct 20, The MAP Targetry Program in FY11 and FY12 K. McDonald Princeton U. (Oct 20, 2011) MAP Technical Board.
NuMI NuMI Target Hall Air System Review Introduction July 30, 2003 Jim Hylen / FNAL Page 1 NuMI Target Hall Air System Review Introduction Air system for.
Focusing Lens for the SSR1 Section of PXIE Preliminary analysis of main options 3/13/2012I. Terechkine1.
K. McDonald NFMCC Collaboration Meeting Jan 14, The Capture Solenoid as an Emittance-Reducing Element K. McDonald Princeton U. (Jan. 14, 2010)
KT McDonald MAP Front End Meeting March 3, Finalizing the C- and Hg-Target Configurations for 6.75-GeV Proton Beams Present studies are for a carbon.
J. Pasternak First Ideas on the Design of the Beam Transport and the Final Focus for the NF Target J. Pasternak, Imperial College London / RAL STFC ,
1 Target Station Design Dan Wilcox High Power Targets Group, Rutherford Appleton Laboratory EuroNu Annual Meeting 2012.
IDS120j WITHOUT RESISTIVE MAGNETS: NEW Hg MODULE mars1510 ( DESKTOP ) vs. mars1512 ( PRINCETON CLUSTER ) Nicholas Souchlas, PBL (3/28/2012) 1.
1 Target Station Design for Neutrino Superbeams Dan Wilcox High Power Targets Group, Rutherford Appleton Laboratory NBI 2012, CERN.
RSVP AGS Upgrade Projects MECO RSVP Preliminary Baseline Review Brookhaven National Lab April 6-8, 2005 D. Phillips.
A. Leveling - Fermilab Recent Operating Experience at the Antiproton Source Target Hall 3 rd High Power Targetry Workshop September 12, 2007 Fermilab Accelerator.
RSVP AGS Upgrade Projects MECO RSVP Preliminary Baseline Review Brookhaven National Lab April 6-8, 2005 D. Phillips.
Kinetic Energy Spectra of pi +, pi -, mu +, mu - and sum of all from the 20to4T5m Configuration X. Ding Front End Meeting June 23,
IDS120j WITHOUT RESISTIVE MAGNETS ( 20 cm GAPS AND 15.8 g/cc W BEADS ) AZIMUTHAL DPD DISTRIBUTION STUDIES FOR: BP#1, SH#1, SHVS#1/LFL, SC#1+SC#2, BeWind.
MICE Prototype Coupling Coil Fabrication Update Allan DeMello Lawrence Berkeley National Laboratory MICE CM38 - Napa California February 25, 2014 February.
IDS120j WITHOUT RESISTIVE MAGNETS MODIFYING Hg MODULE Nicholas Souchlas, PBL (11/1/2012) 1.
Proton Driver – Target Station Interfaces Keith Gollwitzer Fermilab Wednesday May 28, 2014 MAP 2014 Spring Meeting.
IDS120j WITH AND WITHOUT RESISTIVE MAGNETS PION AND MUON STUDIES WITHIN TAPER REGION, III ( 20 cm GAPS BETWEEN CRYOSTATS ) Nicholas Souchlas, PBL (9/4/2012)
IDS120j WITHOUT RESISTIVE MAGNETS SEMGENTATION STUDIES FOR BEAM PIPE BEYOND FIRST CRYOSTAT ( 20 cm GAPS AND 15.8 g/cc W BEADS ) Nicholas Souchlas, PBL.
IDS120j WITHOUT RESISTIVE MAGNETS SEMGENTATION STUDIES FOR BP#2 WITHIN FIRST CRYOSTAT AND RIGHT FLANGE OF Hg POOL INNER VESSEL ( 20 cm GAPS AND 15.8 g/cc.
Neutrino Factory Target Vessel Concept Update V. Graves Target Studies EVO June 12, 2012.
Neutrino Factory Target Cryostat Review (Update Aug 12) Van Graves Cale Caldwell IDS-NF Phone Meeting August 10, 2010.
CW Cryomodules for Project X Yuriy Orlov, Tom Nicol, and Tom Peterson Cryomodules for Project X, 14 June 2013Page 1.
Target Proposal Feb. 15, 2000 S. Childress Target Proposal Considerations: –For low z target, much less power is deposited in the target for the same pion.
MICE Coupling Coil Vacuum Vessel Fabrication Update Allan DeMello Lawrence Berkeley National Laboratory Coupling Coil Working Group January 28, 2014 January.
Ids120h_side. ids120h_top ids120h_iso ids120h_end.
Target On axis field [scale /20 T] Target Magnets Decay-Channel Triplets Taper magnets.
KT McDonald MAP Spring Meeting May 30, Target System Concept for a Muon Collider/Neutrino Factory K.T. McDonald Princeton University (May 28, 2014)
ENERGY FLOW AND DEPOSITION IN A 4-MW MUON-COLLIDER TARGET SYSTEM
IR Beam Transport Status
Presentation transcript:

KT McDonald Target Studies Meeting June 14, Mechanical Issues for the Target System K. McDonald Princeton U. (June 14, 2011) Target Studies Meeting

KT McDonald Target Studies Meeting June 14, Baseline Concept Present baseline concept is described in Figures related to the baseline configuration are at Figures by Phil Spampinato from Study 2 are at Present Target Concept

KT McDonald Target Studies Meeting June 14, Overview of Mechanical Issues 1.Layout of final-focus (quads, x-y correctors, beam pipe/window). 2.Layout of superconducting magnets and their cryostats (+ quench-protection circuit). 3.Layout of tungsten-carbide (WC) shielding (+ cooling water). 4.Layout of the 6-T copper magnets (+ cooling water and electrical feeds). 5.Layout of the mercury system (nozzle, containment vessel, downstream window, mercury flow return, …. How do these items fit together? How can they be removed for repair? (Remote handling mandatory.) No lubricants viable in high-radiation area!

KT McDonald Target Studies Meeting June 14, Final Focus Basic specs of final focus: Proton beam energy = 8 GeV. Transverse, geometric emittance = 5  m (rms) =  2 /   (p. 224) Spot size,  = 1.2 mm (rms).   = 30 cm. Beam divergence,   =  /   = 4 mrad Air gap(?) in proton beam between end of final-focus system and target system. Can the radioactive air-handling system deal with the resulting activation of air? Can this gap be long enough that the target system could be (dis)assembled with the final-focus system in place? Example: if want last quad at z = - 10 m, beam  = 4 cm, so a 5-  clearance requires the bore of the quad to be 40 cm. Is this large bore practical? [Could use a solenoid lens rather than a quad.]

KT McDonald Target Studies Meeting June 14, Superconducting Magnets How are the coils arranged inside cryostats? Braces against the strong intermagnet forces are simpler if at 4K,  Many coils per cryostat, but then must replace many coils if one fails. Where will the substantial quench protection system be located? Will radiation compromise the superinsulation/magnet vacuum? WC Shields The WC shields are very massive, and their containment vessels must be reinforced to minimize deformations. The shields must be assembled inside the magnet cryostat by some kind of sliding support system. However, lubricants must be avoided in the high-radiation environment of the target system. The cooling-water flow paths must be defined.

KT McDonald Target Studies Meeting June 14, T Copper Magnet Can all services (electrical leads and cooling water connections) be on the upstream face of the coils (layer wound)? How little shielding can there be inside the inner radius of the copper magnets? N. Mokhov quotes limit of Gy = 100 mW/g for 10 “years” of 10 7 s each. How are the copper coils supported? Mercury System Needs both primary and secondary containment vessel. Can the secondary containment vessel be the inner surface of the WC shield? Need gas between primary and secondary vessel to permit monitor of possible Hg leak  No water cooling of the primary vessel,  Need substantial He gas flow! What is the configuration of the Hg pool, including splash mitigation? What is the Hg exit flow path? What is the layout of entrance and exit beam windows?

KT McDonald Target Studies Meeting June 14, Removable Target Module Present thinking is that the mercury vessel must be removable replacement if necessary. The tapered primary containment vessel is trapped by the copper magnet and WC shield.  Must be able to remove the mercury vessel, copper magnets, and some/all of the upstream WC shield as a unit, which I call the target module. Could/should the upstream WC shield consist of concentric subunits, with only the inner subunit being part of the target module? Could the target module be removed directly upstream, without interference with the final-focus system (which might be removed first)? Or, should some substantial portion of the target system be first movable transversely, followed by axial disassembly? Should the target module include the entire mercury recirculation system (as at JPARC) or have mercury disconnects (as at SNS)?