HPT & M/D I WG DISCUSSION SLIDES PASI 2012 Hurh et al.

Slides:



Advertisements
Similar presentations
WP2: Targets Proposed Outline Work Programme Chris Densham.
Advertisements

Matt Rooney RAL The T2K Beam Window Matt Rooney Rutherford Appleton Laboratory BENE November 2006.
WG1: High Power Targets PASI 2013 Working Group Sessions Introduction Convened by: Dr. C. Densham (STFC/RAL), Mr. P. Hurh (FNAL)
PASI WP1 PASI meeting April 2013 WP1 progress report D.M.Jenkins.
A Neutrino Factory Target Station Design based on Solid Targets J. R. J. Bennett STFC, Rutherford Appleton Laboratory, Harwell Science.
2nd High-Power Targetry Workshop MATERIAL IRRADIATION STUDIES FOR HIGH-INTENSITY PROTON BEAM TARGETS Current & Future Activities N. Simos and H. Kirk,
Solid Targets for the Neutrino Factory J R J Bennett Rutherford Appleton Laboratory, Chilton, Didcot, Oxon, OX11 0QX, UK
NuMu Collaboration - March 2006 Solid Targets for Neutrino Factory REPORT to the Collaboration On what have we been doing since we last reported! (amazing.
Primary Target Systems for a Muon Collider / Neutrino Factory. What has the experimental effort taught us thus far. N. Simos, H. Kirk, S. Kahn, P. Thieberger,
May 17-19, 2000 Catalina Island, CA Neutrino Factory and Muon Collider Collaboration Meeting 1 Target Support Facility for a Solid Target Neutrino Production.
NuFact2004, Osaka, Japan MATERIAL R&D FOR HIGH-INTENSITY PROTON BEAM TARGETS Nicholas Simos, H. Kirk, W-T. Weng, P. Thieberger, (BNL) K. McDonald, Princeton.
Simulations of Pressure Waves induced by Proton Pulses In search of the answer to the fundamental question: are materials indeed stronger than what we.
1 BROOKHAVEN SCIENCE ASSOCIATES N. Simos Brookhaven National Lab May 1-2, Oxford U., UK High Power Target R&D Simulations.
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.
MuTAC Review - March Solid Target Studies N. Simos Brookhaven National Laboratory.
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
OVERVIEW Material Irradiation Damage Studies at BNL BLIP N. Simos and H. Kirk, BNL K. McDonald, Princeton U N. Mokhov, FNAL (Oct. 20, 2009) (BLIP = Brookhaven.
FNAL Target Related Capabilities PASI 2013 Working Group 1 P. Hurh (FNAL)
1Managed by UT-Battelle for the U.S. Department of Energy PASI_2012_Flowing_Target_Challenges Challenges for Flowing Targets Bernie Riemer (ORNL) (Jan.
Proton Accelerators for Science and Innovation Workshop at Fermilab
KT McDonald MAP Spring Meeting May 30, Target System Concept for a Muon Collider/Neutrino Factory K.T. McDonald Princeton University (May 28, 2014)
Next generation of ν beams Challenges Ahead I. Efthymiopoulos - CERN LAGUNA Workshp Aussois, France, September 8,2010 what it takes to design and construct.
temperature heat conduction radiation Particles in Motion convection vaporization thermal conductor thermal insulator.
BNL Neutrino Long Baseline Neutrino Initiative N. Simos, BNL NWG Baseline = 2540 Km Homestake.
Initiatives in the Target Sector J. R. J. Bennett CCLRC, Rutherford Appleton Laboratory, Chilton, Didcot, Oxon. OX11 0QX, UK.
NuFact 2005 US Solid Target Program Neutrino Factory/Neutrino Super Beam N. Simos, BNL H. Kirk, H. Ludewig, PT. Trung (BNL) K. McDonald, Princeton U. J.
KT McDonald MAP Winter Meeting (SLAC) December 5, Solid Target Options for an Intense Muon Source K. McDonald Princeton U. (December 5, 2014) MAP.
Lessons learnt at 5 th High-Power Targetry Workshop Fermilab, May 2015 Federico Carra EN-MME ColUSM
Harold G. Kirk Brookhaven National Laboratory Targetry Concept for a Neutrino Factory Muon Meeting BNL January 26, 2004.
Possible irradiation needs from CERN and requirements (a partial and selected view) M. Calviani (EN/STI)
BL1U at TRIUMF UCN Beamline Spallation Target & Remote-Handling System (Aug/2010) L.Lee.
Initiative in the Target Sector J. R. J. Bennett CCLRC, Rutherford Appleton Laboratory, Chilton, Didcot, Oxon, OX11 0QX, UK.
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.
ITPA - Meeting, Toronto; Session 3 - High Z studies 3 - High-Z studies (Chair - A. Herrmann) 16:25 (0:10) A. Herrmann - Introduction 16:35.
RaDIATE October Technical MeetingOctober BLIP Irradiation Planning Radiation Damage In Accelerator Target Environments.
Solid Targets for Neutron Spallation Sources Eric Pitcher Los Alamos National Laboratory Presented to: AHIPA Workshop October 20, 2009.
10/9/2007 Global Design Effort 1 Optical Matching Device Jeff Gronberg / LLNL October 9, 2007 Positron source KOM - Daresbury This work performed under.
NBI CERN Experimental Assessment of Radiation Damage in Targets Considered in Neutrino Superbeam and Neutrino Factory Initiatives N. Simos, BNL.
Ch Energy Transfer Kinetic Molecular Theory “Kinetic” = moving “Molecular” = all matter is made up of atoms and molecules So all matter is made up.
BNL Irradiation Facility Use Collimator Materials for LHC Luminosity Upgrade.
1 BROOKHAVEN SCIENCE ASSOCIATES N. Simos, BNL EUROnu-IDS Target Meeting December 15-18, 2008 Superbeam Horn-Target Integration.
What is the kinetic molecular theory? In what three ways is thermal energy transferred? How are thermal conductors and insulators different? Particles.
Thermal and Chemical Energy. Thermal Energy Thermal Energy Thermal energy is kinetic energy because molecules are in motion. Temperature Temperature =
Present status of production target and Room design Takashi Hashimoto, IBS/RISP 2015, February.
HIGH POWER TARGETS AND MACHINE/DETECTOR INTERFACE WORKING GROUP SUMMARY REPORT PASI 2012 Workshop, 1/14/12 Co-conveners: C. Densham, P. Hurh, J. Thomas,
ESSnuSB Target Chris Densham, Tristan Davenne STFC Rutherford Appleton Laboratory 26 th May 2014.
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.
Standards 3: Thermal Energy How Heat Moves  How heat energy transfers through solid.  By direct contact from HOT objects to COLD objects.
ORNL is managed by UT-Battelle for the US Department of Energy High Power Targets for Accelerator Based Research Facilities Bernard Riemer Spallation Neutron.
Thermal Energy 11/1/2011. What is thermal energy? Thermal energy is also known as heat and is the kinetic energy of all the molecules in a material. If.
Project X Energy Station Spallation Target March 20, 2012 D. Wootan, D. Asner 1.
Design for a 2 MW graphite target for a neutrino beam Jim Hylen Accelerator Physics and Technology Workshop for Project X November 12-13, 2007.
HIGH POWER TARGET DEVELOPMENT AT FERMILAB Accelerator Sector Planning and Strategy Workshop P. Hurh.
T2K Target status PASI Meeting Fermilab 11 th November Chris Densham STFC Rutherford Appleton Laboratory On behalf of the T2K beam collaboration.
TARGETRY AND IRRADIATION STUDY REQUIREMENTS OF THE FERMILAB RESEARCH PROGRAM Project X Collaboration Mtg – Experimental Opportunities 4/11/12P. Hurh.
1 1 מ חויבות ל מ צוינות - ג רעין להצלחה 200 kW Liquid Lithium Neutron Source G. Shimel, A. Arenshtam, I. Eliyahu, A. Kreisel, I. Silverman 6 th High Power.
Irradiated T2K Ti alloy materials test plans
Targets Neutrino Factory J. R. J. Bennett
n_TOF Target HiRadMat Experiment Proposal (1704)
States of Matter Matter commonly occurs in one of three “states”
Tungsten Powder Test at HiRadMat Scientific Motivation
Outline: Why now ? What ? How ?
Accelerator R&D for Future Neutrino Projects
Thermal Energy and Matter
Superbeam Horn-Target Integration
Heat = Transfer of energy between objects that are at different temperatures Goes from the HIGHER temp. object to the LOWER temp. object.
Heat Transfer Vocabulary
Heat Transfer.
Presentation transcript:

HPT & M/D I WG DISCUSSION SLIDES PASI 2012 Hurh et al

Matrix Results (Preliminary)  Weighted Averages (least to greatest)  2.83 High Magnetic Field (SC radiation protection)  3.33 Liquid Metals (Pumping, Heat exchanger, etc.)  4.50 Thermal “shock” (solid)  4.67 Thermal “shock” (liquid)  5.17 Novel Target/Window Design  5.83 Monitoring & Instrumentation  6.67 Radiation Protection and Facility Design  7.17 High Heat Flux Cooling  7.67 Radiation Damage

Matrix Results – Niche Impact  High Scores for Selected Facilities  6.67 Liquid Metals Spallation (3) ADS Demo (7) NuFact/Muon Collider (10)  8.50 High Magnetic Field (SC Rad protection) Muon (LE stopping) (7) NuFact/Muon Collider (10)

Matrix Results – Niche Impact (con’t)  High Scores for Selected Facilities  9.00 Thermal “shock” (solid) Neutrino (super-beam) (8) Spallation (9) NuFact/Muon Collider (10)  9.33 Thermal “shock” (liquid, incl. cooling medium) Neutrino (super-beam) (8) Spallation (10) NuFact/Muon Collider (10)

Cross-cutting R&D Activities Identified  Radiation Damage  Correlation of radiation damage effects of LE neutron to HE proton irradiation Gas Production Dose Rate Requires dedicated Material Scientists Will require validation testing  In-beam (>100 MeV proton?) irradiation testing Program to support LE to HE damage correlation Materials picked from potential target materials Low-Zed (graphite, Be) Med-Zed (Al, Albemet, Ti alloys) High-Zed (Tungsten, Inconel, SS) Study Annealing Effect for various materials Facility?? Funding?? PIE??

Cross-cutting R&D Activities Identified (con’t)  High Heat Flux Cooling  Studies/Tests of Cooling methods applicable to targets Radiation (emissivity enhancement?) Gas Convection Spray Cooling/Boiling/Heat Pipe Micro-channel  Energy Deposition Dilution Beam sweeping/rastering Target spinning

Cross-cutting R&D Activities Identified (con’t)  Radiation Protection and Facility Design  Participate in conceptual design and review of potential facility design Operational experience informing design Cradle to Grave mentality Largest impact on “up-time” after fundamental design  Verification/Benchmarking of Simulation Codes Residual Radiation Complex “gap” geometries Tritium migration  Remote Handling Tools and Methods “Shark Cage” Cold Cell Volume Reduction Tools  Novel/Exotic Shielding Materials

Cross-cutting R&D Activities Identified (con’t)  Novel Target/Window Design  Development of alternative technologies Pebble Bed Powder (confined and jet) Waterfall Plasma? Any others?

“Niche” R&D Activities Identified  Thermal “Shock”, Liquid  Cavitation/Erosion Mitigation Bubbles Gas Wall Coatings/Treatments Magnetic Suppression? Tensile Strength Enhancement?????  Benefits: Neutrino (super-beam) (8) Spallation (10) NuFact/Muon Collider (10)

“Niche” R&D Activities Identified  Thermal “Shock”, Solid  “Single-pulse” Testing Simulation validation (elastic-plastic) Failure Criteria validation Wide parameter space Materials Temperature Load rate Irradiated state  Target Shaping/Damping Directing stress wave into compliant, damping material  Benefits: Neutrino (super-beam) (8) Spallation (10) NuFact/Muon Collider (10)

“Niche” R&D Activities Identified  High Magnetic Field (SC Rad Protection)  Irradiation Testing of SC wire/tape and insulation Limits Annealing Parameters  Novel Shielding Materials??  Benefits: Muon (LE stopping) (7) NuFact/Muon Collider (10)

“Niche” R&D Activities Identified  Liquid Metals  Pumping, Filtering, and Handling Erosion Limits Material Compatibility (LME, etc) Contamination Control Freeze-plug mitigation  Containment/Clean-up Technologies and methods Reactions and Radiochemistry (Polonium?)

“Deliverables”  Next 12 months:  Explore…  Start…  Initiate…  Contact…  Plan…  Next 5 years:  Conduct…  Perform…  Participate…  Determine…  Design…  Build…  Test…