Target & Horns Fluxes were distributed. W/ J-PARC type 2.5 o, 2 o, 3 o. Target cooling evaluation and test Target stress analysis Serious stress analysis.

Slides:



Advertisements
Similar presentations
New Plate Baffle Water Flow. Quick Simulation Use triangular prism as rough estimate of a vane Uniform heat flux on each surface –600 kWm -2 on end face.
Advertisements

Radiopharmaceutical Production Target Foil Characteristics STOP.
Michael Butzek, Jörg Wolters, Bernhard Laatsch Mitglied der Helmholtz-Gemeinschaft Proton beam window for High Power Target Application 4th.
BARTOSZEK ENGINEERING 1 Review of the Stress Analysis of the MiniBooNE Horn MH1 Larry Bartoszek, P.E. 1/20/00 BARTOSZEK ENGINEERING.
for a neutrinos factory
R.Valbuena NBI March 2002 CNGS Decay Pipe Entrance Window Structural and Thermal Analysis A.Benechet, P.Cupial, R.Valbuena CERN-EST-ME.
Target & Capture for PRISM Koji Yoshimura On behalf of PRISM Target Group Institute of Particle and Nuclear Science High Energy Accelerator Research Organization.
Analysis of PC Chip Heat Sink Design Royce Tatton ME 340 Dr. Solovjov Fall 2006.
Status of T2K Target 2 nd Oxford-Princeton High-Power Target Workshop 6-7 th November 2008 Mike Fitton RAL.
The JPARC Neutrino Target
Modeling Direct Chill Casting of Aluminum Alloys Cathryn Karashin Advisor: Dr. Krane.
M. Yoda, S. I. Abdel-Khalik, D. L. Sadowski and M. D. Hageman Woodruff School of Mechanical Engineering Extrapolating Experimental Results for Model Divertor.
Target & Horns A.K.Ichikawa Fluxes were distributed. W/ BNL-type and J-PARC type. Target cooling test Comparison of various carbons Energy deposit on 1.
FETS-HIPSTER (Front End Test Stand – High Intensity Proton Source for Testing Effects of Radiation) Proposal for a new high-intensity proton irradiation.
RF-Accelerating Structure: Cooling Circuit Modeling Riku Raatikainen
Engineering Department ENEN 16/08/2013 LR - BBC Pre-Study 1 STATUS of BBC DESIGN and ENGINEERING : PRELIMINARY RESULTS G. MAITREJEAN, L. GENTINI.
JHF2K neutrino beam line A. K. Ichikawa KEK 2002/7/2 Overview Primary Proton beamline Target Decay Volume Strategy to change peak energy.
1 Design of Solenoid and iron yoke for GLD KEK Hiroshi Yamaoka Ken-ichi Tanaka July 13, ‘05.
Kanwalpreet Kaur Communication subsystem & Integration subsystem.
1 cm diameter tungsten target Goran Skoro University of Sheffield.
1 EUROnu design System target + horn First thermal calculations on the target made of aluminium G. Gaudiot 02/06/2010 Strasbourg.
Study of a new high power spallation target concept
Thermal stress & cooling of J-Parc neutrino target S. Ueda JHF target monitor R&D group Introduction neutrino target requirement for target Thermal stress.
Horn design for the CERN to Fréjus neutrino Super Beam Nikolas Vassilopoulos IPHC/CNRS.
Micro-Resistor Beam.
Stress and Cool-down Analysis Yun HE MLC Internal Review 9/5/2012Yun HE, MLC Internal Review1.
Felix Dietrich | AWLC14 | | Stress simulation in the ILC positron target with ANSYS Felix Dietrich (TH-Wildau), Sabine Riemann, Friedrich Staufenbiel.
Application of QuickField Software to Heat Transfer Problems i j k By Dr. Evgeni Volpov.
Current Status and Possible Items around ‘neutrino beam’ Horn Target Remote maintenance tools Decay volume window and collimator muon monitor Many items.
JCOV, 25 OCT 2001Thermal screens in ATLAS Inner Detector J.Godlewski EP/ATI  ATLAS Inner Detector layout  Specifications for thermal screens  ANSYS.
Consideration of Baffle cooling scheme
Support and magnet coil KEK Hiroshi Yamaoka Nov. 10, ‘04.
Feb 3, 2009Thermal aspects of Advanced Virgo cryostat design, Eric Hennes, UvA1 Advanced Virgo : cryostat designs Some thermal aspects Eric Hennes, University.
CLIC Prototype Test Module 0 Super Accelerating Structure Thermal Simulation Introduction Theoretical background on water and air cooling FEA Model Conclusions.
Beam MC activity A.K.Ichikawa for beam group For more details,
Heat load of the radiation cooled Ti target of the undulator based e+ source Felix Dietrich (DESY, TH-Wildau),Sabine Riemann(DESY), Andriy Ushakov(U- Hamburg),
Felix Dietrich | LCWS 2014 | | Target stress Analysis at DESY Felix Dietrich (TH-Wildau), James Howarth, Sabine Riemann (DESY), Friedrich Staufenbiel.
1 Mechanical calculations of the CDC end-plates KEK H. Yamaoka July 8 th, '09 KEK H. Yamaoka.
The CNGS Target Station By L.Bruno, S.Péraire, P.Sala SL/BT Targets & Dumps Section.
Presentation at BBC, Linac 4 Commissioning Dump at 50 and 100MeV 1 Øyvind Dahle Lauten, EN-STI.
SPL-SB and NF Beam Window Studies Stress Analysis Matt Rooney, Tristan Davenne, Chris Densham March 2010.
J-PARC neutrino experiment Target Specification Graphite or Carbon-Carbon composite cylindrical bar : length 900mm, diameter 25~30mm The bar may be divided.
High Intensity Beam Test of Beryllium for Target and Beam Window Applications Presented by: Brian Hartsell Contributors: Kavin Ammigan, Patrick Hurh NBI.
F.Staufenbiel / EuCARD 2 / Heat load and stress studies of the ILC collimator G. Moortgat-Pick 1;2 S. Riemann 2, F. Staufenbiel 2, A. Ushakov.
Cooling of GEM detector CFD _GEM 2012/03/06 E. Da RivaCFD _GEM1.
S1 global: thermal analysis TILC09, April 19th, 2009 Serena Barbanotti Paolo Pierini.
Horns, Hadron production etc. (from hadron production to neutrino beam) A.K.Ichikawa KEK 200/9/26 Study on horns Changing -beam energy Hadron.
Simulation of heat load at JHF decay pipe and beam dump KEK Yoshinari Hayato.
TEM3P Simulation of Be Wall Cavity Tianhuan Luo. Cavity Model Pillbox cavity with Be wall R=0.36 m, f0~319 MHz, L=0.25m (not exactly 325 MHz, but not.
Target R&D for the J-PARC neutrino experiment (II) Yoshinari Hayato (KEK/IPNS) for the J-PARC target R&D group.
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.
Horn and Solenoid options in Neutrino Factory M. Yoshida, Osaka Univ. NuFact08, Valencia June 30th, A brief review of pion capture scheme in NuFact,
Institute of Applied Mechanics
Axion Relics Thermal – mechanical simulation for a flange UHV 114/63 1D with copper gasket
Estimation of Wake Field, Heating in Modified Beam Pipe
SILICON PIXELS DETECTOR
Peter Loveridge High Power Targets Group
Beam Window Studies for Superbeams
Target and Horn status report
Thermo-mechanical simulations jaws + tank
First thermal calculations on the target made of aluminium
STUDIES TOWARDS TARGET-HORN INTEGRATION Institute of Applied Mechanics
Modified Design of Aries T-Tube Divertor Concept
Target R&D for JHF neutrino
Thermo-mechanical Analysis
EUROnu Beam Window Studies Stress and Cooling Analysis
Tutorial in Mechanical Properties
Beam dump for J-Parc neutrino facility
ANALYSIS OF THE HORN UNDER THERMAL SHOCK – FIRST RESULTS
SPL-SB and NF Beam Window Studies Stress Analysis
Presentation transcript:

Target & Horns Fluxes were distributed. W/ J-PARC type 2.5 o, 2 o, 3 o. Target cooling evaluation and test Target stress analysis Serious stress analysis started for 1 st horn consistent w/ simple calculation Optimization of the horns Load test was done w/ mini-1 st horn.

Fluxes w/ J-PARC type 2.5 o, 2 o, 3 o.

Progress by S.Ueda and Target&Monitor group Required heat convection coefficient btw. water and graphite was evaluated. T surf < 100 o Both  T surf and T water were evaluated. Actual heat convection coefficient was measured. Target cooling Q : ~60kJ/3.3sec. T water T surf water target Q

T surf Max. α=6α=6  T surf Required Heat Convection coefficient Q Z=0cm Z=90cm beam ターゲット 水 Result >6.5[kW/Km 2 >5.8[kW/Km 2 Heat deposit onto the water is not yet taken account. These are based on simple calculations. FEM analysis is being carried out. S.Ueda

horn target 90 cm One of cooling schems

electrode Cooling water Cooling Test water DC Current

Thermal stress estimation (ANSYS) Condition: Simulate the hottest part (z=100mm ~ 200mm) : The edges (z=100 & 200mm) are fixed in z direction. just after the spill (after 5  s) Equivalent stress (Because both of the edges were fixed) z (mm) maximum r=0, z=200mm maximum temperature ~8.8MPa. (r=0,z~170mm) r (mm) 0 15 slightly larger but consistent with the analytical calculations (analytical calc.: 6.0MPa) (due to the approximation of the temperature distribution) Hayato, Minakawa

Further optimization –Horn1- Parameters default Current I320kA Inner conductor radius r in 26 mm Horn1 Length L1 1.5 m Distance to Horn2 D2 0.5 m Horn2 shape parameter a Horn3 shape parameter a Fixed Parameters Horn2 Length L2 2 m Horn3 Length L3 2.5 m Total Length 11.5 m L1 D2 L2 D3 L3

Rin = 28 mm L1 = 140cm D2 = 50cm

Heat load by radiation to 1 st horn Ver4.8 Rin=23mm, Total : 70kJ/pulse 26mm, Total : 37kJ/pulse 28mm, Total : 35kJ/pulse

Time evolution of temperature at inner-condcutor r in =26mm, L1=150cm, w pulse =0.4ms 最高温度部 Asuming  from K2K (Yamanoi et al.)

Stress analysis using ANSYS beam 1 st horn Cylindrical model Only stress from Lorenz force is considered. Stress from heat load should be considered. 3mm thick aluminum  eq < 20 MPa Deformation < 60  m

I=320kA 3mm thick aluminum  eq < 20 MPa Deformation < 60  m Only stress from Lorenz force  eq < 23 MPa Deformation < 100  m Previous version Rin=26mm Rin=28mm

Load Test FSW w/ Yamanoi