Activation Issues for ANU Peter Kasper 17-Sep-2007.

Slides:



Advertisements
Similar presentations
Thule Smart RV™ Pod Kit Installation For Smooth-Sided Fiberglass RVs
Advertisements

Ceramic Tile Installation Step 5 – Install Tile TNC EDUCATION SERVICES, INC Instructional Design and Learning Management.
Worth 25% of your overall GCSE mark. The title for your CA is “Does the centre of Salisbury have both core and frame areas?” Over the next 6-7 lessons.
Simulations des niveaux de radiations en arrêt machine M. Brugger, D. Forkel-Wirth, S. Roesler (SC/RP)
Xing Zhang Yifan Zhang Fan Yang.  A Large-scale Coal Mine locates at this area.  The problem of subsidence here is quite serious.  Use TRANSIENT.
1 Evaluation Rong Jin. 2 Evaluation  Evaluation is key to building effective and efficient search engines usually carried out in controlled experiments.
BLM Trip Limits Revisited May 28, 2004 Peter Kasper.
Neutrinos from Stored Muons STORM Target Station Conceptual Design 15-April-2013 Kris Anderson Fermilab/Accelerator Division/Mechanical Support Department.
Chapter 3 Measuring Excavation and Sitework
1 Activation problems S.Agosteo (1), M.Magistris (1,2), Th.Otto (2), M.Silari (2) (1) Politecnico di Milano; (2) CERN.
RAD309 Patient Dose.
9645 TTCSI “I AM” SECONDARY SCHOOLS COMPETITION CHALLENGE 9645.
Foundation Systems.
ENGINEERING SURVEYING & PHOTOGRAMMETRY CVE 314
Background to the current problem 1. As a result of the high stresses in the bobbin due to the magnet load, the bobbin end plate needs to be increased.
PROBLEM: Radiation Dose Rate in IR2 When IR1 is Operating (and Vice Versa) Muon Dose Rate > 1 mRem/hr for 0.1% Collimated Halo.
A U.S. Department of Energy Office of Science Laboratory Operated by The University of Chicago Argonne National Laboratory Office of Science U.S. Department.
UCN Phase 2 Design Status September 10, Design Components Bulk Shielding Target Crypt Cryogenic Insert Target Insert UCN Port Beam Window Cooling.
Preliminary studies for Muon shield modification to accommodate LCLS II Alev Ibrahimov December, 2010 BSY.
08/24/07Shutdown’07 Week 3 F.G. Garcia1 MTA beam line installation Weekly Report August 24, 2007 Period covered: August 17 th to August 24 th (Week 3)
The Tevatron Decommissioning Plans AEM 10/17/11 Paul C. Czarapata.
RADIATION PROTECTION IN DIAGNOSTIC AND INTERVENTIONAL RADIOLOGY
ANU Shutdown Status AEM meeting Cons Gattuso 6/3/2012.
NuMI NBI2006 September 9, 2006 NuMI Repairs for Hot Components Jim Hylen / FNAL Page 1 NuMI Repairs for Hot Components (1 sievert = 100 rem) Problem On.
Delivery Ring Abort B. Drendel 3/17/14. Abort Dump Location The AP2 line will stay as-is between the present IQ29 and the Debuncher. This includes all.
MCTF C. Johnstone MUTAC Meeting 8-10 April Debut of the MTA beamline Description, status and commissioning plans.
Muon Campus Projects Jerry Annala Jan 23, µ AIP Scope Recycler RF system to provide needed bunch structure to future Muon Experiments Recycler RF.
August 05, Startup 2013 Machine Status:  Proton Source Commissioning and Studies RFQ Injector Line (RIL) Linac Booster  Main Injector Startup.
1. 2 Traditional Income Statement LO1: Prepare a contribution margin income statement.
TRENTON Casing Filler Presentation
HAPL Concrete Shielding Requirements Mohamed Sawan UW Fusion Technology Inst. HAPL Project Meeting UW-Madison October 22-23, 2008.
2 IMPACT - THE FIRE PERMIT = Hot Work Permit 3 Welcome ! This course is linked to the use of IMPACT, so it is assumed that: You know how to use IMPACT.
First radiological estimates for the HIRADMAT project H. Vincke and N. Conan 1.
Radiation Protection aspects for SHIP Doris Forkel-Wirth, Stefan Roesler, Helmut Vincke, Heinz Vincke CERN Radiation Protection Group 1 st SHIP workshop,
Injection Energy Review D. Schulte. Introduction Will review the injection energy So could answer the following questions: Which injection energy can.
1 Al Moretti, APC, Fermilab MAP- Winter Meeting February 28 - March 4, 2011 TJNAF Newport News, VA.
City of Winnipeg SOUTHWESTERN RAPID TRANSIT CORRIDOR Bidder Meeting October 16 th, 2009.
Lesson 7 Learning About Careers. Objectives After studying this chapter you will be able to  list factors to consider when choosing a career.  describe.
House 18 ft 20 ft Sidewalk is 36 inches wide and 4 inches thick. Driveway is 15 feet wide, 60 feet long, and 6 inches thick. DRIVEWAYDRIVEWAY.
Activation around dump shielding, and design of beam line mask Mathieu Baudin, RP Genevieve Steele, EN-STI Helmut Vincke, RP.
Mu2e Mu2e CD-2 Review Template Eric Prebys Extinction October 21-24, 2014.
Detector alignment Stefania and Bepo Martellotti 20/12/10.
SNuMI 1 Outline Action Items PP2 Progress [Nancy/Elaine] –Org Chart Update –FY07 Budget/Plans Discussion –FY08 Summer Shutdown –Overall cost Reduction.
Measurements Measurements and errors : - Here, the goal is to have some understanding of the operation and behavior of electrical test instruments. Also,
Radiation Protection studies for the Linac4 / Linac2 interface Joachim Vollaire, DGS-RP 28/09/2015 Linac4 Coordination Meeting.
Radiation Protection Considerations for the CDR Helmut Vincke DGS-RP.
Characterization of the nTOF Radioactive Waste M. Brugger, P. Cennini, A. Ferrari, V. Vlachoudis CERN AB/ATB/EET.
BOOSTER COLLIMATION AND SHIELDING Proton Source Workshop Fermilab December 7-8, 2010 Nikolai Mokhov Fermilab Accelerator Physics Center.
Conductive glue tests. J.Wickens 12/7/04 Used small pieces of HV kapton cut from redundant (old) stock, glued to silicon test structures from Karlsruhe.
Solenoid Status Paul Brindza Dec. 12, Status of work at IUCF Solenoid R&R is based on a MOU between JLAB and IUCF The MOU divides the work into.
August 12, Machine Status: 2013  Proton Source Commissioning and Studies RFQ Injector Line (RIL) Linac : Roof hatch installed Booster : Magnet.
Proton Source Meeting, August 8, 2003 – E. Prebys 1 Major Projects in Linac/Booster  New Linac Lambertson  (4) New EDWA magnets in MI-8 line  (3) New.
1 FORMER COS COB POWER PLANT From Characterization to Redevelopment Brownfields2006 November 14, 2006.
 All civil engineering projects like dams, reservoirs etc. constructed on earth crust and constructed by material obtained from the crust.  So it is.
Muon Long Term Schedule August 15, µ Points to discuss What is the schedule What is the schedule Shutdown schedules Shutdown schedules How do we.
Maximum Credible Beam Loss in the Main Injector D. Capista January 26, 2012.
Shielding the turbomolecular pump and the vacuum gauge 11 June 2013 Kiril Marinov ASTeC, MaRS, DL 1.
Radiation Protection Standards for Prompt Radiation Don Cossairt, Radiation Protection Manager, ESH&Q Section October 1, 2013.
Evolution of Field Emission Characteristics Selected C100 Cryomodules Michael Drury.
Queen Anne Academic Center Prince George’s Community College 301 Largo Road Largo, Maryland By: Austin Heidelbaugh.
STUDY OF NEUBAUER’S CHAMBER Fahareen-Binta-Mosharraf MNS.
Primary Design Parameters July 13,2001 S. Childress Page 1 NuMI Besides design specifications driven by physics and Main Injector beam parameters, significant.
IRC/SAC status Venelin Kozhuharov for the SAC/IRC working group NA62 Meeting
Forward Tagger Simulations
Final Focus Synchrotron Radiation
Simulation-Based Approach for Comparing Two Means
RICH detector for CLAS12 … continue to explore feasibility of proximity focusing RICH in LTCC sector(s) INFN-Rome and ISS CLAS12-RICH Working Group Meeting.
TRENTON Casing Filler Presentation
Strathclyde gun bead-pull results
Radiation Safety Considerations
Presentation transcript:

Activation Issues for ANU Peter Kasper 17-Sep-2007

Investigating the impact of tunnel activation at MI-14 and MI-39 on the ANU work Penetrations are planned to be installed during the 2008 shutdown The locations correspond to “hot spots” in the tunnel How do we deal with this? – Lead blankets: Low impact but limited efficacy – Removing magnets: High impact on cost, time, and operations

First Step: Find out what we are dealing with – Weekly radiation measurements in order to characterize cool down rates How much can we gain by waiting for things to cool down? Answer: Very little. – Map the radiation fields in the relevant areas How local are the hotspots? Can lead blankets be usefully deployed? What is the average dose rate that a laborer might expect?

Cooldown Measurements: – Measurements taken with LSM at upstream end of all elements … From to From to All readings are at 1 ft. – Work areas are concentrated between and and These are the hottest parts of the tunnel Activated ion pump magnet RR gave – 0.18 mr from Mn 54 (312 days) and Co 58 (71 days)

After 35 days most elements measured had cooled by ~2/3 (consistent with measurements on ion pump magnets) Larger reductions observed downstream of LAM-2 (downstream of the work area

Mapping the radiation: – Measurements taken on a 1 ft-sq. grid 70 ft long section of tunnel at each work site 6 measurements between the inner wall and the beamline elements Measurements take ~2.5 hours (where is Tomlin’s robot when you need it?) – Average dose rates obtained by averaging over all points within ~5 ft. of the major penetrations MI-14: 16.4 mrem/hr MI-39: 7.6 mrem/hr

MI-14 MI-39 Location of big penetrations Max. 100 mr/hr Max. 69 mr/hr

Work Steps: – Excavation and installation of grillage – Drill pilot holes – Cut penetration holes – Install PVC penetrations – Construct forms – Pour and cure concrete – Remove forms – Clean up tunnel – Backfill etc. Work Days 12 3* 8 (2*) 1 (1*) 2 (1*) 1 2* 40 *In tunnel

Tunnel occupancy:- – 9 days spread over 18 work days ( = 3.6 weeks ) Assume 1 tunnel day = 5 hours Assume time is evenly divided between the two sites Total dose – 539 mrem(Quarterly limit: 300 mrem) – 150 mrem/week(Weekly limit: 100 mrem) – 60 mrem/day(Daily limit: 40 mrem)

Repeat measurements in MI-10 with Pb blankets on and 104-2, including gap between them

New measurements :- – Used the same 1 ft grid as the original – Incomplete coverage ft for new measurements ( ft for original) Plots fill missing 15 ft with old measurements – Taken ~10 days after the original New measurements scaled by 1/0.87 to account for extra cool down Factor chosen to obtain agreement over the last 5 ft Consistent with measured cool down rate – Thin point in the Pb coverage at the gap center

Before After Cool down corrected Location of big penetrations Max. 100 mr/hr 35 mr/hr Max. 44 mr/hr Not remeasured

Before - after Location of big penetrations Max. 65 mr/hr Not remeasured Before / after

Tunnel occupancy:- – 9 days spread over 18 work days ( = 3.6 weeks ) Assume 1 tunnel day = 5 hours Assume time is evenly divided between the two sites Total dose with Pb as installed – 357 mrem(Quarterly limit: 300 mrem) – 99 mrem/week(Weekly limit: 100 mrem) – 40 mrem/day(Daily limit: 40 mrem)

Comments Pb blankets gave significant dose reductions Implies that magnets are the dominant source A more extensive installation would easily provide the necessary dose reduction Already close to acceptable as installed Eliminate thin point at gap Cover the entire work area in both enclosures Increasing thickness gives marginal improvement

Caveats Cool down correction Measurements were done after 35 days cool down Rates go up by 20% for a 12 day cool down Have assumed the same workers throughout Dividing the tasks among different individuals will reduce the totals even further Must not allow the tunnels to get significantly hotter