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Brookhaven Science Asso ciates U. S. Department o f Energy GENERATION IV NUCLEAR ENERGY SYSTEMS HOW THEY GOT HERE AND WHERE THEY ARE GOING GENERATION IV NUCLEAR ENERGY SYSTEMS GENERATION IV NUCLEAR ENERGY SYSTEMS HOW THEY GOT HERE AND WHERE THEY ARE GOING HOW THEY GOT HERE AND WHERE THEY ARE GOING Da vid J. Diamo nd Broo khaven National L aboratory Energ y Sciences and Technology Department Nuclear Energy and Infrastructure Systems Division P resented a t t he U ni versi ty of Tennessee Apr i l 30, 2003 

Gen IV U-Tenn Presentation

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Page 1: Gen IV U-Tenn Presentation

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Brookhaven Science AssociatesU.S. Department o f Energy

GENERATION IV NUCLEAR ENERGY SYSTEMSHOW THEY GOT HERE AND WHERE THEY ARE GOING 

GENERATION IV NUCLEAR ENERGY SYSTEMSGENERATION IV NUCLEAR ENERGY SYSTEMSHOW THEY GOT HERE AND WHERE THEY ARE GOING HOW THEY GOT HERE AND WHERE THEY ARE GOING 

David J. Diamond

Brookhaven National Laboratory

Energy Sciences and Technology Department

Nuclear Energy and Infrastructure Systems Division

Presented at the University of Tennessee April 30, 2003 

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Slide 2

OUTLINE OF PRESENTATIONOUTLINE OF PRESENTATION

n Introduction to the Gen IV (long-term) Nuclear Energy Systems

n The Roadmap - how we got to the Gen IV concepts

n The Not-Gen IV Nuclear Energy Systemsaka the international near-term deployment concepts

n What do the Gen IV concepts look like; what are some of their R&D needs

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Slide 3

GENERATION IV NUCLEAR ENERGY SYSTEMSGENERATION IV NUCLEAR ENERGY SYSTEMS

Sodium Fast Reactor (SFR)

Gas-Cooled Fast Reactor (GFR)

Molten Salt Reactor (MSR)

Supercritical 

Water Reactor (SCWR)

Very High Temp.Gas Reactor (VHTR)

Lead-alloy Fast Reactor (LFR)

R&D Applications 

Size Fuel Cycle 

Neutron Spectrum 

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Slide 4

GENERATION IV NUCLEAR ENERGY SYSTEMSGENERATION IV NUCLEAR ENERGY SYSTEMS

ClosedFastSodium Fast Reactor (SFR)

ClosedFastGas-Cooled Fast Reactor (GFR)

ClosedThermalMolten Salt Reactor (MSR)

Open,

Closed

Thermal,

Fast

Supercritical 

Water Reactor (SCWR)

OpenThermalVery High Temp.Gas Reactor (VHTR)

ClosedFastLead-alloy Fast Reactor (LFR)

R&D Applications 

Size Fuel Cycle 

Neutron Spectrum 

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Slide 5

GENERATION IV NUCLEAR ENERGY SYSTEMSGENERATION IV NUCLEAR ENERGY SYSTEMS

 AdvancedRecycle

Electricity, Actinide Mgmt.

Med toLarge

ClosedFastSodium Fast Reactor (SFR)

Fuels, Materials,Safety

Electricity, ActinideMgmt., Hydrogen

MedClosedFastGas-Cooled Fast Reactor (GFR)

Fuel, Fueltreatment,Materials, Safetyand Reliability

Electricity, ActinideMgmt., Hydrogen

LargeClosedThermalMolten Salt Reactor (MSR)

Materials, SafetyElectricityLargeOpen,

Closed

Thermal,

Fast

Supercritical 

Water Reactor (SCWR)

Fuels, Materials,H2 production

Electricit y, Hydrogen,Process Heat

MedOpenThermalVery High Temp.Gas Reactor (VHTR)

Fuels, Materialscompatibility

Electricity, ActinideMgmt., Hydrogen

Small toLarge

ClosedFastLead-alloy Fast Reactor (LFR)

R&D Applications 

Size Fuel Cycle 

Neutron Spectrum 

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Slide 6

THE TECHNICAL ROADMAPTHE TECHNICAL ROADMAP

n Discusses the benefits, goals and challenges, and the importance of thefuel cycle

n Describes evaluation and selection process

n Introduces the six Generation IV systems chosen by the Generation IVInternational Forum

n Surveys system-specific R&D needs for all six systems

n Collects crosscut ting R&D needs

n GIF countries will choose the systems they will work on

n Programs and projects wil l be founded on the R&D surveyed in theroadmap

n Information available at gif.inel.gov/roadmap/

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Slide 7

TECHNOLOGY GOALSTECHNOLOGY GOALS

n Sustainability1. Provide sustainable energy generation that meets clean air 

objectives and promotes long-term availability of systems andeffective fuel utilization for worldwide energy production

2. Minimize and manage their nuclear waste and notably reduce the

long term stewardship burden, thereby improving protection for 

the public health and the environment

n Safety and reliability

3. Operations will excel in safety and reliability

4. Will have a very low likelihood and degree of reactor core damage

5. Will eliminate the need for offsite emergency response

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Slide 8

TECHNOLOGY GOALSTECHNOLOGY GOALS

n Economics6. Will have a clear life-cycle cost advantage over other energy

sources

7. Will have a level of financial risk comparable to other energyprojects

n Proliferation resistance and physical protection

8. Will increase the assurance that they are a very unattractive andthe least desirable route for diversion or theft of weapons-usable

materials, and provide increased physical protection against actsof terrorism

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Slide 9

INTERNATIONAL NEAR-TERM DEPLOYMENT (1/2)INTERNATIONAL NEAR-TERM DEPLOYMENT (1/2)

n Deployment by 2015

n Industry involvement

n Improvement over current advanced LWR performance

n  Advanced Boiling Water Reactors

•  ABWR-II• ESBWR

• SWR-1000

• HC-BWR

n Modular High-Temperature Gas-Cooled Reactors• GT-MHR

• PBMR

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Slide 10

INTERNATIONAL NEAR-TERM DEPLOYMENT (2/2)INTERNATIONAL NEAR-TERM DEPLOYMENT (2/2)

n

 Advanced Pressure Tube Reactor •  ACR-700

n  Advanced Pressurized Water Reactors

•  AP-600•  AP-1000•  APR-1400

•  APWR+• EPR

n Integral Primary System Reactors

• CAREM• IMR

• IRIS• SMART

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Slide 11

GEN IV NUCLEAR ENERGY SYSTEMSGEN IV NUCLEAR ENERGY SYSTEMS

n Very High Temp. Gas Reactor (VHTR)

n Gas-Cooled Fast Reactor (GFR)

n Supercritical Water Reactor (SCWR)

n Sodium Fast Reactor (SFR)

n Lead-alloy Fast Reactor (LFR)

n Molten Salt Reactor (MSR)

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Slide 12

SEQUENCED DEVELOPMENT OF HIGH TEMPERATUREGAS COOLED NUCLEAR ENERGY SYSTEMSSEQUENCED DEVELOPMENT OF HIGH TEMPERATUREGAS COOLED NUCLEAR ENERGY SYSTEMS

PMR

GFR 

> 950°C for VHTheat process

Fast neutrons &integral fuelcycle for highsustainability

VHTR 

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Slide 13

VHTR FOR HYDROGEN PRODUCTIONVHTR FOR HYDROGEN PRODUCTION

n Hydrogen demand is already large and growing rapid ly

• Heavy-oil refining consumes 5% of natural gas for hydrogen production

n Energy securi ty and environmental quality motivate hydrogen as an alternative to oilas a transportation fuel

• Zero-emissions

• Distributed energy opportunity

n Water is the preferred hydrogen“fuel”• Electro lysis using off-peak

power • High-temperature electrolysis• High-temperature

thermochemical water split ting

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Slide 14

VERY HIGH TEMPERATURE REACTOR (VHTR)VERY HIGH TEMPERATURE REACTOR (VHTR)

Characteristics

•He coolant•1000°C outlet temperature•Reactor coupled to H2

production facility•600 MWth, nominally basedon MHTGR

•Coated particle fuel,graphite block (or pebble?)core

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Slide 15

 

Reactor CavityCooling System

Reactor Pressure

Vessel 

Control Rod Drive

Stand Pipes

Power Conversion

System Vessel

Floors Typical 

Generator 

RefuelingFloor  

Shutdown Cooling

System Piping 

Cross Vessel

(Contains Hot &

Cold Duct)

35m(115ft) 

32m(105ft) 

46m(151ft  

GT-MHR REACTOR BUILDINGGT-MHR REACTOR BUILDING

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Slide 16

 

Control Rod

Drive Assembly

RefuelingStand Pipe

Control RodGuide tubes

Cold leg Core

Coolant Upper

Plenum

Central ReflectorGraphite

Annular shaped

Active Core

Outer Side ReflectorGraphite

Core Exit Hot Gas

Plenum

Graphite Core

Support Columns

Reactor Vessel

Upper PlenumShroud

Shutdown CoolingSystem ModuleHot Duct

Insulation

Module

Cross Vessel

Nipple

Hot Duct

StructuralElement

Metallic Core

Support Structure

Core Inlet Flow

CoreOutletFlow

Insulation Layer for Metallic

Core Support Plate

Upper Core Restraint

Structure

Control Rods

7m(23 ft)

23.7m(78ft)

2.2m(7ft)

8.2m(27ft) Dia

Vessel Flange

Upper plenum - hot plume 

mixing - “LOF” 

Core - depressurized cooldown 

Flow between hotter/ cooler 

channels - “LOF” 

Lower plenum - hot 

 jet mixing 

Natural convection and thermal radiation 

Core flow - normal operation 

GT-MHRGT-MHR

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Slide 17

CORE FLOW ISSUES DURING NORMAL OPERATIONCORE FLOW ISSUES DURING NORMAL OPERATION

n Calculation of the coolant channel temperatures during normal operation

• Significant local variations in power occur across the core due the non-uniformlocation of the reflectors, control rods, and burnable poison assemblies and due tothe fuel loading

• Power variations are amplified in the hot channels due to the buoyancy resistance

• Therefore the coolant temperatures can vary by more than + or - 200°C from theaverage

n Calculation of the core lower plenum flow mixing and pressure drop

• Hot jet mixing, complex 3-dimensional flow around the core suppor ts, and the flowacceleration near the hot duct need to be calculated

n Calculation of the hot duct coo lant mixing and insulation effectiveness• Permeation o f the hot gas into the insulation is a concern

• The entrance condit ions are somewhat uncertain, but the flow must be well mixed bythe time it reaches the turbine

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Slide 18

Thermal-hydraulic Issues

n Mixing of the gases during bypassevents

n Flow distributions among therecuperators and recuperator efficiency

n Hot streaks at the turbine inlet

 

Generator 

Thrust Bearing  

Turbine 

High Pressure

Compressor

Recouperator 

Recouperator 

Low Pressure

Compressor

Precooler/ Intercooler 

Cold Gas to Reactor

Hot Gas from Reactor

PCS Vessel 

34m(112ft)  

8.2m(27ft) Dia.

Vessel Flange  

POWER CONVERSION UNITPOWER CONVERSION UNIT

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Slide 19

THERMAL-HYDRAULIC ISSUES - ACCIDENT CONDITIONSTHERMAL-HYDRAULIC ISSUES -

 ACCIDENT CONDITIONS

n

Rejection of the heat by natural convection and thermal radiation from the reactor pressure vessel outer wall to the passive cooling system

• Local effects around the hot duct need to be cons idered

• Some separate effects proof testing may be needed

n Reliability , robustness, and effectiveness of the Reactor Cavity Cooling System

n Flow through the core during a loss of circulation accident

• Up flow in the hot channels and down flow in the cool channels results in hotplumes in the upper plenum

• The hot and cold channel flow dist ribution and the upper plenum mixing areuncertain

• Low Reynolds number flow with turbulent, transitional, and/or laminar flow,

buoyancy effects, and gas property variations

n Core cool down during a LOCA

n  Air or water ingress during a LOCA

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Slide 20

GAS-COOLED FAST REACTOR (GFR)GAS-COOLED FAST REACTOR (GFR)

Characteristics

• He (or SC CO2) coolant, direct

cycle energy conversion

• 850°C outlet temperature

• 600 MWth /288 MWe

• U-TRU ceramic fuel in coated

particle, dispersion, or 

homogeneous form

• Block, pebble, plate or pin core

geometry

• Combined use of passive and

active safety systems

• Closed fuel cycle system with fullTRU recyc le

• Direct Brayton cycle energy

conversion

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Slide 21

 ADVANTAGES OF GFR ADVANTAGES OF GFR

n

GFRs share the sustainability attributes of fast reactors• Effective fissioning of Pu and minor actinides

•  Ability to operate on wide range of fuel compositions (“ dirty fuel” )

• Capacity for breeding excess fissile material

n  Advantages offered by use of He coolant• Ease of in-service inspection

• Chemical inertness

• Very small coolant void reactivi ty (<ßeff )

• Potential for very high temperature and direct cycle conversion

n High temperature potential opens possibil ities for new applications,including hydrogen production

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Slide 22

GFR R&D NEEDSGFR R&D NEEDS

n Safety case difficult wi th low thermal inertia and poor heat transfer 

properties of coolant

• Reliance on active and “ semi-passive” systems for decay heat removal• Passive reactivity shutdown is also targeted

n High actinide-density fuels capable of withstanding high temperature and

fast fluence

• Modified coated particle or dispersion type fuels, e.g., – (U,TRU)C/SiC – (U,TRU)N/TiN

• Fuel pins with high-temperature cladding, e.g., infiltrated kernel particle

n Core structural materials for high temperature and fast-neutron fluenceconditions (ceramics, composites, refractory alloys)

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Slide 23

FUEL / CORE CONFIGURATIONSFUEL / CORE CONFIGURATIONS

n GFR

• Metal or ceramic matrix (similar to prismatic)

• Pin, plate types (ceramic, metallic)

• Pebble/particle

C o m p o s i t e C e r a m i c s

F u e l E l e m e n t C o r e L a y - o u t

Co r e V e s s e l

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Slide 24

SCWR: GENERAL CHARACTERISTICSSCWR: GENERAL CHARACTERISTICS

n

LWR operating at higher pressure (>22.1 MPa) and temperature (280-550°C)• Operating condi tions with fossil plant experience

n Higher thermal efficiency (44% vs. 33%)

n No change of phase

• Larger enthalpy rise in core• Lower flow rate (~10% of BWR)

• Lower pumping power (smaller pumps)

n Simplified direct cycle system• No recirculation

• Smaller reactor pressure vessel/containment

n Thermal or fast spectrum possible• Fuel cycle flexibili ty

Improved Economics 

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Slide 25

SCWR: OPTIMIZATION OF LWR TECHNOLOGYSCWR: OPTIMIZATION OF LWR TECHNOLOGY

Reactor

Turbine/Generator

Reactor

Turbine/Generator

ReactorSteam-waterseparation system

Recirculationsystem

Turbine/Generator

ReactorSteam-waterseparation system

Recirculationsystem

Turbine/Generator

Reactor

Steam generatorPressurizer

Turbine/Generator

Reactor

Steam generatorPressurizer

Turbine/Generator

Reactor

Turbine/Generator

Reactor

Turbine/Generator

ReactorSteam-waterseparation system

Recirculationsystem

Turbine/Generator

ReactorSteam-waterseparation system

Recirculationsystem

Turbine/Generator

Reactor

Steam generatorPressurizer

Turbine/Generator

Reactor

Steam generatorPressurizer

Turbine/Generator

Reactor

Turbine/Generator

Reactor

Turbine/Generator

ReactorSteam-waterseparation system

Recirculationsystem

Turbine/Generator

ReactorSteam-waterseparation system

Recirculationsystem

Turbine/Generator

Reactor

Steam generatorPressurizer

Turbine/Generator

Reactor

Steam generatorPressurizer

Turbine/Generator

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Slide 26

SCWR: EFFECT OF SIMPLIFICATIONSCWR: EFFECT OF SIMPLIFICATION

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Slide 27

Fuel assembly 

SCWR NEUTRONIC DESIGNSCWR NEUTRONIC DESIGN

n Considerations with core design

• Large change in density axially

•  Average coolant density higher thanin BWR

• Downward flow in water rods

• Other moderators (BeO, ZrH2

)

• Square or hexagonal geometry

Water rod

nSafety consideration

•Rod ejection accident•Negative moderator reactivi ty coefficient

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Slide 28

BASIC DATA - HEAT TRANSFERBASIC DATA - HEAT TRANSFER

Heat-transfer data at prototypical

SCWR condi tions (i.e.,

supercritical water, complex

bundle geometry, high heat flux)

are needed.

 

Single-phase heat transfer: Data exist for either simpleround tubes and/or surrogatefluids. Existing SCW heat-transfer database and

correlations are inconsistent.

Existing correlations and models for SCW heat transfer exhibi t large

discrepancies and diverging trends

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Slide 29

CODES - NUMERICAL INSTABILITIESCODES - NUMERICAL INSTABILITIES

Large (albeit continuous) variation of the thermo-physical properties…

… may result in code execution failures.

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Slide 30

SODIUM-COOLED FAST REACTOR (SFR)SODIUM-COOLED FAST REACTOR (SFR)

Characteristics•Sodium coolant, 550°C Tout

•150 to 1500 MWe•Pool or loop plantconfiguration

•Intermediate heat transportsystem

•U-TRU oxide or metal-alloyfuel

•Hexagonal assemblies of fuel pins on triangular pitch

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Slide 31

SFR SAFETY R&D NEEDSSFR SAFETY R&D NEEDS

n Demonstration of passive safety design: providing assurance that the physical

phenomena and related design features relied upon to achieve passive safety areadequately characterized

•  Axial fuel expansion and radial core expansion

 – Experimental data plus deterministic models required for accurate corerepresentation (particularly, minor-actinide-bearing fuels)

 – Reduce uncertainties in T-H quantities by using more detailed models- Multi-pin subassembly, full assembly -by-assembly, coupled neutron ics-

thermal-hydraulic calculation

-  Accurate duct -wall and load pad temperatures required for calculatingbending moments in each subassembly to characterize core restraint andexpansion

- CFD tools for benchmark calculations or routine design calculations?

• Self-activated shutdown systems

• Passive decay heat removal systems – CFD models useful for resolution of complex natural circu lation flow paths

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Slide 32

SFR SAFETY R&D NEEDS (CONT’D)SFR SAFETY R&D NEEDS (CONT’D)

n  Accommodation of extremely low probabili ty but higher consequenceaccident scenarios

• Demonstrate that passive mechanisms exist to preclude recriticality ina damaged reactor 

• Show that debris from fuel failure is coolable within the reactor vessel

n

Implication for safety analysis tools• Requires analytical and experimental investigations of mechanism s

that will ensure passively safe response to bounding events that leadto fuel damage

 – e.g., out-of-pile experiments involving reactor materials arerecommended for metal fuels

• Local feedback and material motion modeling required

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Slide 33

LEAD-COOLED FAST REACTOR (LFR)LEAD-COOLED FAST REACTOR (LFR)

Characteristics

• Pb or Pb/Bi coolant• 550°C to 800°C out let temperature

• Fast Spectrum

• Mult i-TRU recycle

• 50–1200 MWe

• 15–30 year core li feOptions

• Long-lif e (10-30 yrs), factory -fabricated

battery (50-150 MWe) for smaller grids

and developing countries

• Modular system rated at 300-400 MWe

• Large monol ith ic p lant at ~1,200 MWe• Long-term, Pb option is intended for 

hydrogen generation – outlet

temperatu re in the 750-800oC range

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Slide 34

CHARACTERISTICS OF LEAD ALLOY COOLANTCHARACTERISTICS OF LEAD ALLOY COOLANT

n Low Neutron Absorption and Slowing Down Power 

•  Allow to open the lattice, increase coolant volume fraction absent a

neutronics penalty – pumping requirements also dictate open lattice

• Facili tates natural circulation

n High Boiling Temperature at Atmospheric Pressure (~1700°C)

• Unpressurized primary (precludes loss of coolant accident initiator)• Margins are available to employ passive safety – based on

thermo/structural feedbacks

• Potential to raise core outlet temperature (~800°C suitable for H2

production and other process heat missions)

n Non-vigorous reaction with air and water 

• Potential to simplify heat transport circuits

• Potential to simplify refueling approaches

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Slide 35

MOLTEN SALT REACTOR (MSR)MOLTEN SALT REACTOR (MSR)

HeatExchanger

Reactor

Graphite

Moderator

SecondarySalt Pump

Off-gasSystem

PrimarySalt Pump

PurifiedSalt

ChemicalProcessing

Plant

Turbo-Generator

FreezePlug

Critically Safe, Passively Cooled Dump Tanks(Emergency Cooling and Shutdown)

Steam Generator

NaBF_ 

NaFCoolant Salt

4

72LiF _ Th

Fuel Salt

 _ BeF F _ UF4 4

566Co

704Co

454Co

621Co

538 Co

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Slide 36

MOLTEN SALT REACTOR (MSR)MOLTEN SALT REACTOR (MSR)

Characteristics

•Molten fluoride salt fuel•700–800°C outlet temperature• Intermediate heat transpor t

circuit•~1000 MWe or larger •Low pressure (<0.5 MPa)•Graphite core struc ture

channels flow of actinidebearing fuel

Safety analysis issues•Modeling of nuclear, thermal,

& physio-chemical processes(e.g., FP and MA solub ilit y,nob le metal FP plate-out, …)

•Lack of established analysiscapabilities

•Regulatory framework notdefined