Study on the Neutronic Characteristics of Subcritical Reactors Driven by an Accelerated Pulsed Proton Beam Ali Ahmad.

Slides:



Advertisements
Similar presentations
The UK ADSR programme Roger Barlow FFAG08 Manchester, 4 th September 2008.
Advertisements

TRANSIENT EVALUATION OF A GEN-IV LFR DEMONSTRATION PLANT THROUGH A LUMPED-PARAMETER ANALYSIS OF COUPLED KINETICS AND THERMALHYDRAULICS ANALYSIS OF COUPLED.
Stefan Roesler SC-RP/CERN on behalf of the CERN-SLAC RP Collaboration
HZDR FLUKA activities in support of the MYRRHA Project Short summary with a focus on activation problems Anna Ferrari, Stefan Müller, Jörg Konheiser.
Dynamic Response to Pulsed Beam Operation in Accelerator Driven Subcritical Reactors Ali Ahmad Supervisor: Dr Geoff Parks University Nuclear Technology.
ADSR systems and their contribution to our energy needs Roger Barlow DIUS visit Manchester, 16 th September 2008.
Design on Target and Moderator of X- band Compact Electron Linac Neutron Source for Short Pulsed Neutrons Kazuhiro Tagi.
Multi-physics coupling Application on TRIGA reactor Student Romain Henry Supervisors: Prof. Dr. IZTOK TISELJ Dr. LUKA SNOJ PhD Topic presentation 27/03/2012.
Measurements of cross-sections of neutron threshold reactions and their usage in high energy neutron measurements Ondřej Svoboda Nuclear Physics Institute,
Studies of ADS by means of JINR Nuclotron Martin Suchopár Nuclear Physics Institute, Academy of Sciences of the Czech Republic Department of Nuclear Reactors,
20 F POWER MEASUREMENT FOR GENERATION IV SODIUM FAST REACTORS R. Coulon, S. Normand, M. Michel, L. Barbot, T. Domenech, K. Boudergui, J-M Bourbotte, V.
Fundamentals of Neutronics : Reactivity Coefficients in Nuclear Reactors Paul Reuss Emeritus Professor at the Institut National des Sciences et Techniques.
Nuclear Energy Options and Project-X Shekhar Mishra Fermilab Yousry Gohar ANL June 7 th 2010.
ISIS Target studies Could a used ISIS target provide fusion relevant irradiated tungsten material properties? Tristan Davenne 20 th May nd Radiate.
Work Package 2 Giacomo Grasso ENEA UTFISSM-PRONOC LEADER Work Package 2 meeting Madrid, May 8, 2012 Current status and organization of the work.
Completion of Water-Cooled Backup Study Eric Pitcher TAC-10 November 5, 2014.
Future usage of quasi-infinite depleted uranium target (BURAN) for benchmark studies Pavel Tichý Future usage of quasi-infinite depleted uranium target.
Simulations of Accelerator Driven Systems (ADS) Aleksander Polanski Joint Institute for Nuclear Research, Dubna, Russia. The Andrzej Soltan Institute for.
ADSRs and FFAGs Roger Barlow. 7 Jan 2008Workshop on ADSRs and FFAGsSlide 2 The ADSR Accelerator Driven Subcritical Reactor Accelerator Protons ~1 GeV.
The Proposed Materials Test Station at LANSCE Eric Pitcher Los Alamos National Laboratory Presented at the Workshop on High-Power Targetry for Future.
Measurements of the (n,xn) reactions cross sections using new digital methods. Habib Karam Group GRACE.
Possible calibration methods for the final LXe calorimeter A. Papa 01/20/2004.
The Materials Test Station Eric Pitcher Los Alamos National Laboratory Presentation to: AHIPA Workshop, Fermilab October 19, 2009.
Simulations on “Energy plus Transmutation” setup, 1.5 GeV Mitja Majerle
A brief account of some topics studied under the umbrella of the ThorEA organisation and reported at their meetings: (1) Making Uranium from Thorium through.
AFCI Reactor-Accelerator Coupling Experiments (RACE) Project Prof. Denis Beller Project Director Idaho State University ( Eighth.
D J Coates, G T Parks Department of Engineering, University of Cambridge, UK Actinide Evolution and Equilibrium in Fast Thorium Reactors UNTF 2010 University.
Systematic studies of neutrons produced in the Pb/U assembly irradiated by relativistic protons and deuterons. Vladimír Wagner Nuclear physics institute.
PSB dump: proposal of a new design EN – STI technical meeting on Booster dumps Friday 11 May 2012 BE Auditorium Prevessin Alba SARRIÓ MARTÍNEZ.
AN ALTERNATIVE PROPOSAL FOR A HIBRID REACTOR (SUB-CRITICAL FACILITY COUPLED WITH AN ACCELERADOR) Sergio A. Pereira and Adimir dos Santos.
Advanced Heavy Water Reactor Amit Thakur Reactor Physics Design Division Bhabha Atomic Research Centre, INDIA.
AERB Safety Research Institute 1 TIC Benchmark Analysis Subrata Bera Safety Research Institute (SRI) Atomic Energy Regulatory Board (AERB) Kalpakkam –
Kayla J. Sax MPhil Candidate in Engineering Department of Engineering, University of Cambridge Supervised by Dr. Geoff T. Parks Investigating the Scope.
ThEC13, Geneva, 28th-31st Oct., 2013 C. H. Pyeon, Kyoto Univ. 1 Cheolho Pyeon Research Reactor Institute, Kyoto University, Japan
Beam test possibilities at JINR and Fermilab V. Pronskikh Fermilab 02/15/2012.
Experimental Studies of Spatial Distributions of Neutrons Produced by Set-ups with Thick Lead Target Irradiated by Relativistic Protons Vladimír Wagner.
Cristian Bungau ThorEA Meeting - Oxford - April 2010.
Ondřej Svoboda Nuclear Physics Institute, Academy of Sciences of Czech Republic Department of Nuclear Reactors, Faculty of Nuclear Sciences and Physical.
Double Chooz Near Detector Guillaume MENTION CEA Saclay, DAPNIA/SPP Workshop AAP 2007 Friday, December 14 th, 2007
Mitja Majerle for the “Energy Plus Transmutation” collaboration.
M. Štefánik *), P. Bém, M. Honusek, K. Katovský, M. Majerle, J. Novák, and E. Šimečková AER Working Group F – „Spent Fuel Transmutation“ and INPRO IAEA.
Neutron production in Pb/U assembly irradiated by deuterons at 1.6 and 2.52 GeV Ondřej Svoboda Nuclear Physics Institute, Academy of Sciences of Czech.
1 Neutron Effective Dose calculation behind Concrete Shielding of Charge Particle Accelerators with Energy up to 100 MeV V. E Aleinikov, L. G. Beskrovnaja,
Simulations on “Energy plus Transmutation” setup, 1.5 GeV Mitja Majerle, V Wagner, A Krása, F Křížek This document can be downloaded.
Neutron production in Pb/U assembly irradiated by 1.26 AGeV deuterons. First experimental results Ondřej Svoboda Neutron production in Pb/U assembly irradiated.
D J Coates, G T Parks Department of Engineering, University of Cambridge, UK 3 rd Year PhD student Actinide Breeding and Reactivity Variation in a Thermal.
COMPARATIVE ANALYSIS OF DIFFERENT METHODS OF MODELING OF MOST LOADED FUEL PIN IN TRANSIENTS Y.Ovdiyenko, V.Khalimonchuk, M. Ieremenko State Scientific.
4th International Summer School « Nuclear Physics Methods and Accelerators in Biology and Medicine » Monte-Carlo simulations : FLUKA vs. MCNPX Maxime ODEN.
F D F November 8, 2006Alessandro G. Ruggiero1 of GeV 10-MWatt Proton Driver Target 200-MeV DTL 1.0-GeV FFAG H – Stripping Foil Injection Energy,
A Low Power ADS Demonstrator Hywel Owen School of Physics and Astronomy University of Manchester.
Bob Cywinski International Institute for Accelerator Applications Why thorium? Why Accelerators? PASI 13 January 2012.
NEAR-COMPLETE TRANSURANIC WASTE INCINERATION IN THORIUM-FUELLED LIGHT WATER REACTORS Ben Lindley.
ADS Activities at Argonne National Laboratory Yousry Gohar Argonne National Laboratory Proton Accelerators for Science and Innovation Workshop FERMILAB,
Physics Department Lancaster University Physics Department Lancaster University Reliability Rebecca Seviour Cockcroft Institute Dept Physics Lancaster.
Neutron production and iodide transmutation studies using intensive beam of Dubna Phasotron Mitja Majerle Nuclear Physics Institute of CAS Řež, Czech republic.
ADSR Workshop, May ‘08 ADSR Systems for Power Generation: some practical considerations Bob Cywinski 7 May 2008, Daresbury.
Ali Ahmad FLUKA code validation of nuclear data required for the spallation target design in Accelerator Driven Subcritical Reactors ThorEA Meeting – Daresbury.
ADSR08 Thorium Fuel Rods Bob Cywinski School of Applied Sciences University of Huddersfield ThorEA ADSR Workshop Cambridge 13 January 2009.
Reactor anti-neutrinos and neutrinos
Study on Neutronics of plutonium and Minor Actinides Transmutation in Accelerator Driven System Reactor By Amer Ahmed Abdullah Al-Qaaod Ph.D student Physics.
ADS reliability requirements
Analyses to Support Waste Disposition of SNS Inner Reflector Plug
the s process: messages from stellar He burning
D J Coates, G T Parks Department of Engineering, University of Cambridge, UK Safety Considerations for the Design of Thorium Fueled ADS Reactors ThorEA.
for collaboration “Energy plus transmutation”
David Sangcheol Lee Prof R.Cywinski, Dr C.Bungau and Prof R.Seviour
JOINT INSTITUTE FOR NUCLEAR RESEARCH
Performed experiments Nuclotron – set up ENERGY PLUS TRANSMUTATION
Egyptian Atomic Energy Authority (EAEA), Egypt
Presentation transcript:

Study on the Neutronic Characteristics of Subcritical Reactors Driven by an Accelerated Pulsed Proton Beam Ali Ahmad

Outline Motivation The Simulation Set-up Results & Analysis Conclusions

ADSR in question? Three main components: – Accelerator – Spallation target – Subcritical core Possible deployment of thorium fuel cycle

Motivation : Why pulsed beam operation? LINAC is expensive Classic cyclotron technology is mature and approaching its power limit FFAG has the potential to be both affordable and technologically capable of doing the job (Takahishi. 2001) FFAG is a pulsed accelerator

Motivation : cont. Why is neutronic analysis required? Pulsed proton beam means pulsed production of spallation neutrons Oscillations in the power profile are inevitable Frequent and rapid temperature transients Thermal cyclic fatigue Modeling of flux variation with time is needed

The Simulation Set-up Simulations performed using the MCNPX neutron transport code. En < 20 MeV : Nuclear data tables (ENDF/B-VI) En > 20 MeV : Nuclear models – Bertini Model (Bertini 1969) Delayed neutrons and thermal treatment are included

The Simulation Setup…cont Reactor Materials: - Target: Pb Fuel: Th-Pu MOX - Clad: Stainless steel - Coolant: Pb-208 / Water - Radiation shield: Lead Core arrangement: - Core geometry: hexagonal - Bundle geometry: hexagonal - Number of bundles: Number of fuel pins: 96 - Fuel active height = 202 cm

Results & Analysis (1) : Neutron spectrum evolution

Very fast neutrons (En > 20 MeV) decay in less than 30 ns This means that primary neutrons aren’t of interest to the core neutronics study Hypothesis: Neutron generators can be used instead of a proton beam to study neutrons’ kinetic characteristics

Results & Analysis (1) …cont 14 MeV DT-n-source and beam-operated n-source have very similar core neutronic characteristics A 14 MeV n-source can potentially replace the proton accelerator in an ADSR for research purposes Similar results have been obtained by Yamamoto & Shiroya (2003)

Results & Analysis (2) : Spatial variations and diffusion The diffusion of neutrons in a thermal ADSR is characterised by: - The spallation neutrons are dominant for a period τ  10 µs - After that time, the fission neutrons become dominant

Results & Analysis (2) :... cont A pulsed beam of frequency 1 kHz almost allows four orders of magnitude reduction in the neutron flux level in a fast ADSR The sharp decrease in the neutron flux in a fast ADSR is instantaneous in all assemblies The perturbation in the neutron flux due to a 1 kHz beam in a thermal ADSR is observed only in the assemblies close to the target After a few pulses, the fission neutrons become dominant elsewhere ThermalFast

Results & Analysis (3) : Monitoring of ADSR reactivity The ideal monitoring of core reactivity should be: – On-line – Accurate – Simple and robust measurement technique Experiments done to measure the subcritical reactivity: – MUSE (Billeboud et al. 2003) – YALINA (Fernandez-Ordonez et al. 2003) None of the experimental techniques meet all of the requirements

Results & Analysis (3) : Cont. All of the proposed techniques rely on deliberate gaps in the beam to measure the subcritical reactivity The diffusion equation in a thermal ADSR: Using At a certain spatial position in the reactor (detector position):

Results & Analysis (3) : Cont. For the case when the beam is off the last equation has the solution: Using the definition of neutron life time: Then, Define α can be estimated from the flux decrease rate when the beam is off

Results & Analysis (3) : Cont. Once the neutron life time of a certain core configuration is known, a reactivity measurement will be straightforward To perform on-line measurement of Keff in a thermal ADSR, the separation time between pulses should be more than several tens of microseconds

Conclusions Experimental investigations of the neutronic transients in an ADSR can be done through a relatively cheap neutron source In a thermal ADSR the diffusion time of spallation neutrons is around 10 microseconds, while it is much quicker in a fast ADSR The flux fluctuations due to pulsed operation are almost independent of the spatial position in a fast ADSR The reactivity of a thermal ADSR can be measured on-line if the beam frequency is less than 10 kHz The next step in my research is to study the thermal issues related to pulsed operation and their consequences Thank you