Download presentation
Presentation is loading. Please wait.
Published byAndres Eyre Modified over 9 years ago
1
EAR2 simulation update Collaboration board meeting 06.10.2011 Christina Weiss & Vasilis Vlachoudis
2
Outlook 1.Introduction 2.Results Neutron Fluence Resolution Charged Particle Fluence & γ Background Collimation Implemented Beam Dump Neutron Fluence for Irradiation (@ 1.5 m) 6 October 2011FLUKA Simulation for EAR22
3
INTRODUCTION 6 October 2011FLUKA Simulation for EAR23
4
Latest simulations Geometry in the simulations match the design of the CE plans EAR2 @ 18.4 m Implemented Collimator: 1.2m Fe: conical shape 2.1m PE borated: straight with 8 cm diameter Simulations have been performed for a setup: 1.Without additional moderator at the bottom of the neutron tube (97e+6 primaries) 2.With Moderator at the bottom of the tube (52e+6 primaries) : Polyethylene (d min = 1 cm) 6 October 20114FLUKA Simulation for EAR2
5
RESULTS Neutron Fluence 6 October 2011FLUKA Simulation for EAR25
6
Neutron Fluence 6 October 20116FLUKA Simulation for EAR2 In total the neutron fluence is reduced by about 32 % when using an additional moderator for EAR2
7
Neutron Fluence Comparison to EAR1 6 October 2011FLUKA Simulation for EAR27 Energy Interval EAR1EAR2 Without Moderator Gain [ n / cm 2 / pulse ] Error [%] [ n / cm 2 / pulse ] Error [%] 0.1 – 10 eV5.11e40.38.01e52.615.7 0.01 – 1 keV4.07e40.31.09e61.826.8 1 – 100 keV5.03e40.21.39e61.727.6 0.1 – 10 MeV1.77e50.12.95e61.116.7 10 – 100 MeV2.64e40.34.03e52.715.2 > 100 MeV4.71e40.38.76e45.9 1.9 Total Energy Range 4.68e50.087.82e60.916.7 Reference for EAR1 : FLUKA Simulations with fission collimator (d = 8 cm)
8
RESULTS Resolution 6 October 2011FLUKA Simulation for EAR28
9
Time – Energy Relation 6 October 2011FLUKA Simulation for EAR29
10
Time – Energy Relation 6 October 2011FLUKA Simulation for EAR210
11
Resolution in comparison with EAR1 6 October 2011FLUKA Simulation for EAR211 Neutron EnergyEAR1EAR2 No Moderator EAR2 With Moderator FWHM [cm] 1 eV342 1 keV5.187 1 MeV34.13836 Neutron Fluence is reduced by about 32 % if a Moderator in this form is used Neutron EnergyEAR1: 187.5 mEAR2: 18.9 m No Moderator EAR2: 18.9 m With Moderator ΔE / E 1 eV3.0e-44.3e-32.2e-3 1 keV5.4e-48.5e-37.5e-3 1 MeV3.6e-34.1e-23.9e-2
12
RESULTS Charged Particle Fluence 6 October 2011FLUKA Simulation for EAR212
13
Charged Particle Fluence 6 October 2011FLUKA Simulation for EAR213
14
Magnet 6 October 2011FLUKA Simulation for EAR214 p max = 1.205 [GeV/c] protons B = 0.2 [Tm] Collimator h = 4.60 [m] Possible Position for a magnet: Assumed magnet length: l = 1 [m]
15
Photon Fluence EAR2EAR1 6 October 2011FLUKA Simulation for EAR215
16
Arrival Time EAR2EAR1 6 October 2011FLUKA Simulation for EAR216
17
RESULTS Collimation 6 October 2011FLUKA Simulation for EAR217
18
Neutron Beam Profile 6 October 2011FLUKA Simulation for EAR218 Collimator: 1.2m Fe: conical shape 2.1m PE borated: straight with 8 cm diameter
19
RESULTS Beam Dump – Backscattered Neutrons 6 October 2011FLUKA Simulation for EAR219
20
Beam Dump Backscattered Neutrons 6 October 2011FLUKA Simulation for EAR220 1.5 m of Fe surrounded by 40 cm of borated PE 1 mm of Cd at the entrance
21
RESULTS Neutron Fluence at 1.5 m from the target center – Material Irradiation 6 October 2011FLUKA Simulation for EAR221
22
Neutron Tube has 32 cm diameter at 1.5 m from the target center Neutron Fluence for Irradiation 6 October 2011FLUKA Simulation for EAR222 Total: 2.5e10 n / cm^2 / 7e12 ppp
23
Thank you for your attention! 6 October 2011FLUKA Simulation for EAR223 Energy IntervalEAR1EAR2 Without Moderator Gain [ n / cm 2 / pulse ] Error [%] [ n / cm 2 / pulse ] Error [%] 0.1 – 10 eV5.11e40.38.01e52.615.7 0.01 – 1 keV4.07e40.31.09e61.826.8 1 – 100 keV5.03e40.21.39e61.727.6 0.1 – 10 MeV1.77e50.12.95e61.116.7 10 – 100 MeV2.64e40.34.03e52.715.2 > 100 MeV4.71e40.38.76e45.9 1.9 Total Energy Range 4.68e50.087.82e60.916.7 Reference for EAR1 : FLUKA Simulations with fission collimator (d = 8 cm) Neutron Fluence Comparison
Similar presentations
© 2025 SlidePlayer.com. Inc.
All rights reserved.