Research in Nuclear Engineering at Penn State University
Transcrição
Research in Nuclear Engineering at Penn State University
Research in Nuclear Engineering at Penn State University Arthur T. Motta Chair of Nuclear Engineering Program Department of Mechanical and Nuclear Engineering and Materials Science and Engineering The Pennsylvania State University [email protected] 1 [email protected] Minha trajetoria pessoal • UFRJ Engenharia Mecanica – opcao nuclear • Mestrado na COPPE Engenharia Nuclear, tese em Termohidraulica • Doutorado University of California, Berkeley, Materials • Pos doutorado na Franca, Centro de Estudos Nucleares de Grenoble • Pos doutorado no Canada, Chalk River Laboratories • Professor at Penn State, Nuclear Engineering desde 1992, chefe de programa 2010. Outline • Review of Penn State University • Research in Nuclear Engineering at Penn State • Why graduate study? How to get there Review of Penn State Penn State University • Located in State College, PA • About 45,000 students on campus, 80,000 overall, research university • College of Engineering has almost 300 professors, 13 + programs • Population about 80,000 6 Views of Campus and Town 7 Some numbers • Undergraduate Program in Nuclear Engineering enrollment has been increasing dramatically (highest number in US). Currently about over 200 students in program, 75 graduated last year • Nuclear Engineering Graduate Program has 50 + resident students (about 60% PhD) and over 100 distance education students (M.Eng.) • Research funding de $500,000/ per faculty member/year on the average Nuclear B.S. Degrees Granted Comparison with peers (UG graduation) Mechanical and Nuclear Engineering at Penn State • • • Department of Mechanical and Nuclear Engineering offers PhD programs in ME and NucE. Nuclear Engineering research areas – Reactor Physics and Fuel Management (Profs. Ivanov, Watson and Avramova) – Reactor Thermal Hydraulics (Profs. Kim and Cheung) – Nuclear Materials (Profs. Motta and Catchen) – Nuclear Science Applications (Profs. Jovanovic and Brenizer) – Neutron Beam Analysis (Prof. Unlu) – Reactor Controls (Prof. Ray) – Nuclear Fuel Cycle (Prof. Fratoni) – Radiochemistry (Dr. Johnsen) 12 professors, 50 + graduate students MNE had more than 25 million dollars of research expenditures while Penn state overall had 780 million dollars 2009-2010 13 THE ADVANCED MULTI-PHASE FLOW LABORATORY (AMFL) Prof. Seungjin Kim Design and perform experiments and theoretical and computational analysis on various multi-phase flow phenomena found in nuclear reactor systems. http://www2.mne.psu.edu/amfl/ . The Advanced Multi-phase Flow Laboratory, Department of Mechanical and Nuclear Engineering Tel: (814) 867-0282 Email: [email protected] FLOW VISUALIZATION Bubbly flow: jf = 5.00, jg,atm = 0.10 m/s Slug flow: jf = 1.00, jg,atm = 1.64 m/s Plug Flow: jf = 1.00, jg,atm = 0.16 m/s TWO-PHASE FLOW TRANSPORT IN COMBINATORIAL CHANNELS Sponsored by U.S. DOE - NEER Program; Continued by U.S. NRC To study two-phase flow transport under the effects of geometric restrictions and orientations L/D=177 L/D=1.5 L/D=93 L/D=15 L/D=3 L/D=61.5 L/D=66 49.5 L/D=3 L/D=34.5 • 5.08 cm ID acrylic test section 25.5 L/D=87 L/D=7.5 1.5 L/D=165 • Glass elbows • Development length Vertical: ~ 60D or ~3 m Horizontal: ~180 or ~9 m • Two inlet conditions P4; (L/D)H = 3 P5; (L/D)H = 30 P7; (L/D)H = 93 P10; (L/D)H = 177 P3; (L/D)V = 62 P11; (L/D)V = 1.5 P12; (L/D)V = 15 P3; (L/D)V = 60 P11; (L/D)V = 1.5 Measured Void Fraction Profiles jf=3.0 m/s & jg=0.35 m/s P12; (L/D)V = 16.5 TRACE CODE DEVLEOPMNET USING INTERFACIAL AREA TRANSPORT EQUATION Sponsored by U.S. NRC To develop TRACE code capable of dynamic modeling of two-phase flow using the interfacial area transport equation • Dynamic prediction throughout regime transition Vertical Downward Air-Water Pipe Size: 2.54 cm ID jg,loc,1= 0.453 m/s, jf= 3.110 m/s • Eliminates bifurcation / numerical oscillation • Significant improvements in code prediction results Error bars shown: ±20% HORIZONTAL TWO-PHASE FLOW Sponsored by Bettis Atomic Laboratory To establish database for CMFD code development at Bettis Atomic Power Laboratory • 38.1 mm ID acrylic test section • Adiabatic air-water • L/D ~ 250 or 9.5 m • Capable of comprehensive twophase flow regimes The Advanced Multi-phase Flow Laboratory, Department of Mechanical and Nuclear Engineering Tel: (814) 867-0282 Email: [email protected] Igor Jovanovic Associate Professor of Nuclear Engineering Current projects: •laser particle acceleration in plasma waveguides and dielectric photonic bandgap structures •laser-induced breakdown spectroscopy for nuclear forensics •quantum sensors for super-resolution in imaging •graphene-based radiation detectors •coherent neutrino-nucleus scattering •directional neutron detection •expect to hire 1-2 Ph.D-track students next year See http://www.mne.psu.edu/IJ for more info Department of Mechanical and Nuclear Engineering & Radiation Science and Engineering Center Radiation Science and Engineering Center Breazeale Nuclear Research Reactor 1 MW TRIGA 3x1013 n/cm2 sec thermal neutron flux at core center Gamma Irradiation Facilities In-Pool irradiators Gamma Cell 220 Dry Irradiator (12,000 Curie Co-60, 1.5 MRads/hour) Hot Cells Radiation Detection and Measurement Labs Neutron Beam Laboratory Radionuclear Applications Laboratory Radiochemistry Laboratory Department of Mechanical and Nuclear Engineering & Radiation Science and Engineering Center Measurements of signature trace elements in dated tree ring samples to make correlations with environmental effects Using Neutron Activation Analysis and Compton Suppression System at RSEC Dendrochemistry measurements are being performed for thousands of dated tree ring samples for identifications of volcanic eruptions and climate effects in history. Department of Mechanical and Nuclear Engineering & Radiation Science and Engineering Center Analysis of spent fuel samples with Compton Suppression System at RSEC Gamma spectroscopy spent fuel samples to determine isotopic content Department of Mechanical and Nuclear Engineering & Radiation Science and Engineering Center Development of innovative radioactive isotope production techniques at RSEC Radioisotope production 41Ar, 56Mn, 82Br and 24Na is being explored at RSEC. Production of 67Cu and by extension 64Cu to alleviate the national shortage of needed isotopes. Department of Mechanical and Nuclear Engineering & Radiation Science and Engineering Center New Radiochemistry Teaching Laboratory Current Research Bill Cheung – Professor of Mechanical & Nuclear Engineering Project #1: Study the effects of spacer grids on heat transfer. Sponsors: US Nuclear Regulatory Commission, Purdue Univ. Thermal Hydraulics Institute Project #2: Conceptual design of core catcher in case of core accident for severe accident mitigation for Eu-APR1400 Sponsors: Korean Atomic Energy Research Institute SPACER-GRID THERMAL-HYDRAULICS (SGTH) Sponsored by U.S. NRC To study spacer-grid effects on the cooling of PWR fuel assemblies, including the oscillating reflood conditions • Reference System: 17x17 Westinghouse PWR steam separator • 7x7 full length heated rod bundle assembly Pressure oscillation damping tank exhaust muffler upper plenum Clad Temperatures at Constant Reflood Rates 2.54 cm/s (Run #5092) vs. 5.08 cm/s (Run #5086) 1800 heated water supply tank T em p eratu re (˚F ) 1400 test section: 7x7 rod-bundle flow housing 1000 Exp 5092 D3 2.69 m (106") 600 Exp 5092 D3 2.80 m (110") Exp 5086 D3 2.69 m (106") lower plenum Exp 5086 D3 2.80 m (110") 200 0 100 200 300 Time (sec) 400 500 Reactor Dynamics and Fuel Management Group Reactor Dynamics and Fuel Management Group (RDFMG) – research group consisting of 18 graduate students and four faculty: – – – – Dr. K. Ivanov – Distinguished Professor of NE, Director Dr. M. Avramova – Assistant Professor of NE, Associate Director Dr. J. Watson – ARL Dr. S. Levine – Professor Emeritus of NE Established in 1999 and since then has graduated students with the following Nuclear Engineering (NE) degrees - 21 PhD, 33 MS, 19 ME, and 5 BS with Honors Advanced Coupled Neutronics and Thermal-Hydraulics Methodologies for Integrated Fuel Management and Safety Analysis www.mne.psu.edu/rdfmg Hydrogen from corrosion responds to temperature and stress gradients (=> hydride distribution not homogeneous) Radial re-distribution due to heat flux induced temperature gradient => hydride rim Oxide thickness differences; when oxide spalling occurs, hydride blisters can form Other changes due to localized corrosion or crud deposition Concentration in liner Axial profile due to corrosion differences from coolant temperature, grid spacers and inter-pellet region 200 Azimuthal profile because ofµmdifferences in flux and in cooling around the clad circumference Miyashita 2007, Tsai & Billone 2002, Pyecha 1985 November 2011 29 The project is based on the coupling of four simulation codes and a hydride model Cross-section library Off-line coupling CFD Burn-up Cobra-TF (Thermohydraulic) FRAPCON Local Power DeCART (Neutronic) Local Power [H] Local bulk T Boundary conditions Cross sections FRAPTRAN σ (r,θ,z) T (r,θ,z) [H] (r, θ,z) At a given burn up Hydride model 30 Hydride distribution(r,θ,z) Reactor Core Designs Investigate two reactor core designs representative of current PWRs and BWRs. As a BWR representative we will utilize the General Electric BWR-4 design with 24-month cycle based on Peach Bottom 2 plant. Typical PWR 18-Month Loading Pattern 2 6 3 8 5 10 7 19 18 17 16 15 14 13 12 11 10 26 23 2 2 2 2 2 2 2 2 2 2 2 2 2 2 28 25 30 27 2 2 1 1 2 2 1 1 2 2 2 1 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 1 2 2 1 1 2 2 1 1 2 2 1 1 2 2 1 1 2 2 2 1 1 2 3 1 1 3 3 1 1 3 3 1 1 3 3 1 1 2 29 31 1 2 2 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 2 2 1 2 2 2 2 2 2 2 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 2 2 2 2 2 1 2 2 1 1 3 3 1 1 3 3 1 1 3 3 1 1 3 3 1 1 3 3 1 1 2 2 2 2 1 2 3 1 1 3 3 1 1 3 3 1 1 3 3 1 1 3 3 1 1 3 3 1 1 2 2 2 2 2 2 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 2 2 2 2 2 2 2 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 2 2 2 2 2 2 1 2 3 1 1 3 3 1 1 3 3 1 1 3 3 1 1 3 3 1 1 3 3 1 1 2 1 2 2 2 1 2 3 1 1 3 3 1 1 3 3 1 1 3 3 1 1 3 3 1 1 3 3 1 1 2 2 2 2 2 2 2 3 2 2 2 2 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 2 2 2 2 2 2 1 2 3 1 1 3 3 1 1 3 3 1 1 3 3 1 1 3 3 1 1 3 3 1 1 2 1 2 2 2 1 2 3 1 1 3 3 1 1 3 3 1 1 3 3 1 1 3 3 1 1 3 3 1 1 2 1 2 2 2 2 2 3 2 2 2 2 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 2 2 2 2 2 2 1 2 3 1 1 3 3 1 1 3 3 1 1 3 3 1 1 3 3 1 1 3 3 1 1 2 1 2 2 2 1 2 3 1 1 3 3 1 1 3 3 1 1 3 3 1 1 3 3 1 1 3 3 1 1 2 1 2 2 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 2 3 2 2 2 2 2 2 2 2 3 2 2 2 2 2 2 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 2 2 2 2 2 1 2 2 2 3 3 1 1 3 3 1 1 3 3 1 1 3 3 1 1 3 2 1 1 2 2 2 2 2 2 2 2 7 6 3 2 5 4 3 3 3 3 4 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 1 1 3 3 1 1 3 3 1 1 3 3 1 1 2 2 1 2 2 3 3 3 3 3 3 3 3 3 3 3 3 3 3 2 2 2 2 1 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 6 5 3 2 2 2 3 2 2 2 1 1 2 2 1 1 2 2 1 1 2 2 1 1 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 1 31 24 21 2 8 1 22 19 2 2 9 20 17 2 25 21 18 15 2 24 20 16 13 2 26 23 14 11 2 29 28 27 12 9 30 22 Consider as PWR representative a typical Westinghouse 4-loop pressurized water reactor core design with a 18-month highburnup cycle 4 1 31 8 7 10 9 12 11 14 13 16 15 18 17 20 19 22 21 24 23 2 26 25 28 27 2 2 2 2 1 Assembly Type 1 2 Assembly Type 2 3 Assembly Type 3 30 29 PB-2 BWR Loading Pattern 31 Multi-Physics Analysis Core cycle calculations will be performed with CASMO-4/SIMULATE-3 Based on these results representative core and pin locations exhibiting strong azimuthal flux and temperature gradients will be identified Advanced high-fidelity multi-physics modeling capability will be utilized for “zoom-in” snapshot calculations of the identified locations Local power / linear heat rate DeCart/TORTTD Local power CTF Local bulk temperature & density Local pressure Local bulk temperature Local surface HTC Local flow area reduction Heat transfer to coolant Initial flow area reduction Local fuel temperature FRAPTRAN 32 Initial fuel state FRAPCON Multi-physics high-fidelity simulation framework Calculation Sequence Selection of Core locations for two prototypical reactors using CASMO4/SIMULATE-3 Pteparation of Multi-group PinCell CrossSection Library DeCart/TORT calculation of Φn CTF calculation of mass flow rate, T in coolant CTF sub-pin analysis capability for flexible azimuthal modeling of flux and temperature distributions Calculation of T(r,θ,z) by FRAPTRAN Flowchart of Calculation Tasks 33 Azimuthal flux distribution in a pin-cell of assembly with intra-assembly flux gradient Coupling of Core Thermal-Hydraulic Models with other Models and Phenomena Faculty Participants: Prof. Avramova Lab/Center Name: RDFMG Sponsor: AREVA NP, MHI, NECSA and GRS MCNP/NEM/CTF – Accelerated Monte Carlo Calculations with Thermal-Hydraulic Feedback Multi-Scale MultiPhysics System NEM/CTF/FRAPCON TORT-TD/CTF coupling for High-Fidelity Calculations RELAP-3D/COBRATFCoupling for LOCA Analysis Coupled 3-D Neutronics/Thermal-Hydraulic System Safety Analysis Faculty Participants: Dr. Watson, Prof. Ivanov and Prof. Avramova Lab/Center Name: RDFMG Sponsor: US NRC, GSE, Risk Engineering Ltd., ARL Fully implicit coupling of TRACE and PARCS Cross-section modeling for transient applications Real –time simulators for operator training Research interests Nuclear reactor design – Accident tolerant fuel for light water reactors – Liquid fuel thorium reactors – Critical and subcritical systems for actinides transmutation Nuclear fuel cycle and system analysis – Thermal modeling of repository – Energy return over investment Massimiliano Fratoni Assistant Professor of Nuclear Engineering [email protected] Microencapsulated Metallic Matrix (M3) fuel Scope: design light water reactors to operate with M3 fuel Motivations: M3 fuel is expected to improve fuel performance and reactor safety; M3 fuel does not require cladding and eliminates all failure mechanisms associated with cladding Sponsors and collaborators: – Oak Ridge National Laboratory Zr-Alloy Matrix Zircaloy Cladding Coated Fuel Particle UO2 Pellet Gap Conventional LWR UO2 Fuel Rod Integral LWR M3 Fuel Rod M3 fuel consists of TRISO particles dispersed in a zirconium matrix Microencapsulated Metallic Matrix (M3) fuel Challenge: heavy metal load in M3 fuel is 50% or less than in standard fuel Approach: – High fidelity neutronics modeling using stochastic codes (Serpent, MCNP) – Single assembly and full core models Current design requirements: – High density fuel – 15% enrichment – Small rod pitch-to-diameter ratio (1.10) – Distributed neutron poison (BN) to compensate reactivity excess M3 fuel compared to standard fuel requires higher enrichment and larger fuel rods Generic repository thermal modeling Scope: Develop and implement a simplified thermal modeling tool for generic (no site and no media specific) waste repository Motivations: thermal limits determine the waste management strategy (surface storage duration, waste package size, repository capacity, etc.); necessity to analyze and compare numerous options Sponsors and collaborators: – DOE – Lawrence Livermore Nat. Lab. Generic repository thermal modeling An analytical model was developed for scoping natural or engineered barriers peak temperature Peak temperatures were compared against thermal limits Combinations of three media (granite, clay, and salt) and six fuel forms derived from three fuel cycle options (oncethrough, modified open, and closed) were analyzed Result example: large waste packages are preferred for transportation but they could require long surface storage Razoes para se fazer pos graduacao • • • • Aprofundar conhecimentos Fazer pesquisa Aumentar sua marketabilidade Mais $$$ ~$10,000/yr Source: www.asme.org 2011 salary survey Graduate Student Life • Graduate students are generally supported through their degree program as a Graduate Teaching Assistant or Graduate Research Assistant. The stipend for an incoming MS student is $1900 / month. • With an Assistantship, your tuition and health coverage are paid for through the department (for TA) or through the research grant (for RA) • The MS degree generally requires two years while the PhD degree requires a total of 4-5 years both of which depends on many factors Pos-graduacao em Eng. Nuclear PhD: doutorado, leva de 4 a 5 anos, precisa exame de candidatura (coisas basicas da nuclear), exame compreensivo (projeto de tese) e defesa final. MSc: grau de pesquisa, 2 anos, 24 creditos de cursos, e tese (financiado por projetos de pesquisa. M.Eng: grau profissional, 2 anos, baseado em cursos (financiado pelo aluno). Como chegar la? Pos graduacao • Bolsa de doutorado pleno CNPq ou CAPES • Bolsa sanduiche, dado pelos mesmos orgaos • Financiamento pela universidade americana O que e necessario? • • • • • Aplicacao: mne.engr.psu.edu (tem uma taxa) Curriculo escolar traduzido Graduate Record Examination (treinar) TOEFL (test of English as a Foreign Language) Cartas de recomendacao (2 ou 3 dadas por professores que os conhecam) • Personal essay (dizendo sua motivacao, interesse, eventualmente areas de foco, etc) Suporte americano • Bolsa mensal • Ensino pago (ensino americano nao e gratis, mas a bolsa cobre) • Seguro de saude • Pode ser research assistantship ou teaching assistantship (monitor de cursos) ou uma combinacao dos dois. • Research Assistantship ligado a um projeto especifico (suporte pedido no projeto) e dado para o projeto (ao inves de para o aluno) Como chegar la? graduacao • • • • Estamos costurando! Ciencia sem fronteiras (?) Estagio e cursos Faremos contato direto entre professores • Participacao com Penn State e Westinghouse Conclusion • Review of Penn State, world class research university and very highly rated in nuclear engineering • Review of research areas at Penn State • Discussed how one can apply for graduate study • Encourage you all to think about it, could have a major difference in your career END