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www.inl.gov Nuclear Graphite Research Needs Will Windes Idaho National Laboratory DOE-NE NEET Cross-cut Coordination Meeting August 15-16, 2016 Department of Energy (DOE) Advanced Reactor Technologies (ART) R&D Program

Department of Energy (DOE) Advanced Reactor ......and Property Changes due to Fast Neutron Irradiation”, Juel-4183, 2005 10 Main Material Properties of Interest Irradiation Dimensional

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  • ww

    w.in

    l.gov

    Nuclear Graphite Research Needs

    Will WindesIdaho National Laboratory

    DOE-NE NEET Cross-cut Coordination Meeting August 15-16, 2016

    Department of Energy (DOE)Advanced Reactor Technologies (ART) R&D Program

  • Why Research Graphite? Lessons we’ve learned from other graphite core reactor programs

    – After Reactor Start-up…• Interestingly - fuel is not considered life limiting component after start-up• Graphite is life limiting component of reactor

    – Degradation issues of graphite – normal and accident operations– Changes resulting from irradiation – structural integrity, cracks (irradiation creep)

    – NRC will require understanding of the primary structural core material• Material properties needed for license approval before reactor start-up, and • Predicting core behavior during normal and off-normal operation

    Primary objectives of graphite components– Must keep the fuel safe

    • Must keep temperature “low” – thermal conductivity• Must maintain structural integrity – strength and irradiation behavior

    – Creep behavior → Reduces cracks resulting from irradiation stresses– Provides core structure

    • Cooling channel integrity, control rod insertion, and stable fuel configuration

    − After Reactor Start-up…• Interestingly - fuel is not considered life limiting component after start-up• Graphite is life limiting component of reactor

    • Degradation issues of graphite – normal and accident operations• Changes resulting from irradiation – structural integrity, cracks (irradiation creep), fracture

    − NRC will require understanding of the primary structural core material• Material properties needed for license approval before reactor start-up, and • Predicting core behavior during normal and off-normal operation

  • Primary function of Graphite R&D activities Defines the safe working envelope for nuclear graphite

    − Current and future nuclear graphite components− Applicable for multiple DOE reactor designs (cross-cutting):

    • HTR (both PB and Prismatic) and MSR designs

    Data/analysis will be codified− Data will be used in new ASME Code− Code requires use of irradiation data and high

    temperature behavior

  • Graphite Core Components

    ComponentMax.

    Normal Operation

    Off-Normal DPA

    Graphite fuel block 900-1200ºC ~1400ºC ~ 0.8/yr

    Reflector blocks 600-900ºC ~1200ºC ~ 0.5/yr

    Core support columns 1000-1200ºC ~1200ºC ~0.001/yr

    Other components 250 - 350ºC ~300-600ºC Varies

  • Material Issues

    Degradation

    -4

    -2

    0

    2

    4

    6

    8

    10

    12

    14

    0 5 10 15 20 25

    ∆L/L

    [%]

    dose, dpa

    1100 C900 C700 C500 C300 C

    0.40.50.60.70.80.9

    11.11.21.31.4

    -5 5 15 25C

    TE/C

    TEo

    dose, dpa

    300 C

    500 C

    700 C

    900 C

    1100 C

    0

    0.5

    1

    1.5

    2

    2.5

    0 10 20

    Tens

    ile s

    tren

    gth,

    σ/σ

    o

    dose, dpa

    400 C

    500 C

    700 C

    900 C

    1100 C

    Property changes from irradiation and environment

    O id ti i iti

    Fission product transport/retention

  • Main Material Properties of Interest

    6

    Irradiation Dimensional

    Change

  • Main Material Properties of Interest

    7

    Irradiation Dimensional

    Change

  • 8

    Main Material Properties of Interest

    Irradiation Dimensional

    Change

  • 9

    Main Material Properties of Interest

    Irradiation Dimensional

    Change

    G. Haag,” Properties of ATR-2E Graphite and Property Changes due to Fast Neutron Irradiation”, Juel-4183, 2005

  • 10

    Main Material Properties of Interest

    Irradiation Dimensional

    Change

  • Irradiation creep

    (Residual stress remover)

    Irradiation Dimensional

    Change

    Main Material Properties of Interest

    Dose, dpa

  • Structural failure

    Low Thermal Conduct

    Relieves stress Irradiation

    creep(Internal stress

    remover)

    Longer component

    lifetime

    Structural failure

    Turnaround

    Higher core temperature

    Main Material Properties of Interest

    12

    Internal stress build-

    up

    Cracking&

    Fracture

    Irradiation Dimensional

    Change

    Larger block gaps (lowers

    thermal transport)

    Thermal properties

    Thermal expansion

    change

    Lower Failure

    Degradation

    StrengthlossLower

    ThermalTrans KIc

    Extends turnaround

    Strengthdecrease

  • USA’s 5 different research areas

    Graphite R&D Program

    Defines the safe working envelope for nuclear graphite and

    protection of fuelBehavior models- Predicts irradiated

    material properties and potential degradation issues

    - Irradiation behavior for continued safe operation

    Mechanisms and Analysis- Data analysis and interpretation- Understanding the damage mechanisms

    is key to interpreting data

    Irradiation- Determines irradiation

    changes to material properties- Irradiation behavior for

    continued safe operation

    Virgin Properties- (Statistically) Establishes as-

    received material properties- Baseline data used to

    determine irradiation material properties

    Licensing & Code- Establishes an ASME

    approved code (for 1st time)- Develops property values

    for initial components and irradiation induced changes

  • AGC Experiments

    Irradiation Testing:• Creep Specimens• Button “piggyback”• Changes to properties• Irradiation of new materials• Fundamental irradiation damage

  • AGC Experiment : Irradiation changes

    AGC - 3

    AGC - 5

    Database for previous nuclear graphite grades

    800 ºC

    1100 ºC

    600 ºC

    1400 ºC

    AGC - 4

    AGC - 6

    Dose (dpa)1 3 4.5 6

    HTV

    AGC - 1AGC - 2

    • By comparing between test series• Property change by dose• Property change by temperature • Property change by stress

    • Three pairs of test capsules• 3 Temperatures • 3 Stress levels• Continuous dose (0.5 – 7 dpa)

    ε, σ

    , ρ, α

    , E, C

    TE

    Dose (dpa)

    Tirr = 600, 800, 1100Cσ = 14, 17, 21 MPa

    15

  • Areas of pertinent graphite research DOE-ART focusing on large program activities

    – Irradiation (AGC), Unirradiated data, Oxidation, ASME Code

    Areas of maximum interest– Fundamental (i.e., small) irradiation studies

    • Irradiated defect structures - creep mechanisms– Material property changes

    • Affect of irradiation and molten salt– Fracture and strength

    • Fracture toughness and multi-axial fracture behavior– Degradation (oxidation – salt erosion)

    • Development of oxidation/degradation models• Development of new oxidation resistant grades/components

    (dopants and coatings)– NDE flaw detection

    • Flaw prediction and evolution during irradiation or degradation

  • Fundamental irradiation studiesA real need to determine irradiated defect structures and how they affect behavior/performance.

    • Grains shrink parallel to planes and grow in perpendicular direction

    • Overall volume shrinkage

    Cracks formed during fabrication accommodate swelling – for a while

  • Creep - Dislocation climb/glide

    • Intriguing TEM images under electron beam

    – ║to Basal planes

    – Interaction of basal planes under irradiation

    – Does this show dislocation glide possibilities?

    • Not supposed to happen in current model

    C. Karthik et al. J. Nuc Mat 412 (2011) 321–326

  • 2 IL bonds

    3 IL bonds

    Dislocation climb/glide

    2 IL bonds3 IL bonds

    T. Trevethan et al, U of Sussex & U of Leeds, INGSM-13, Sept 2012

  • Evidence of irradiation damage in graphite

    A. Asthana et al, J. Appl. Cryst., (2005) 38, 361-367

    • Tirr = 333 K (60°C)

    • φlow 0.004 dpa

    • φhigh 0.24dpa

    Unirr

    γlow

    γhigh

    No indication of sub-plane formation Different from current model

  • Questions• What /Which defect structure affects material properties

    – What are real creep mechanisms? Defect structures– What defect structures affect strength/modulus?

    – How does this affect fracture behavior?– How is thermal diffusivity/conductivity affected?– Thermal expansion doesn’t match up with current explanation of

    microstructure/defect changes. Why?• How does defect structure behave/interact

    – Microstructure evolution• How does the defect microstructure change over increased dose

    and temperature?• Defect accumulation

    – How is porosity affected?• Pore generation in tertiary creep – but how/why?

    • Irradiated specimens - at National Labs (INL/ORNL)– Collaborations and sharing of irradiated specimens is a priority– Independent (small) studies with university reactors is needed, too

  • Material Property Changes

    -4

    -2

    0

    2

    4

    6

    8

    10

    12

    14

    0 5 10 15 20 25

    ∆L/L

    [%]

    dose, dpa

    1100 C

    900 C

    700 C

    500 C

    300 C

    0.4

    0.5

    0.6

    0.7

    0.8

    0.9

    1

    1.1

    1.2

    1.3

    1.4

    0 5 10 15 20 25

    CTE

    /CTE

    o

    dose, dpa

    300 C

    500 C

    700 C

    900 C

    1100 C

    0

    0.5

    1

    1.5

    2

    2.5

    0 5 10 15 20 25

    Tens

    ile s

    tren

    gth,

    σ/σ

    o

    dose, dpa

    400 C

    500 C

    700 C

    900 C

    1100 C

    Irradiation shown to affect graphite properties− Dimensional changes, internal stress− Increased stiffness and strength− Dramatic decrease in thermal diff.

    What about Molten Salt?− If salt infiltrates graphite pores− Are basic properties the same?− Combination effects from irradiation and salt?

  • Fracture and Strength Irradiation shown to affect graphite

    strength− Initial strength due to dislocation pinning

    from point defects− But what about pore structure?

    − Microstructure evolution over dose?

    − Increased flaw population must change fracture behavior

    How does molten salt penetration into pores affect fracture behavior?− Solidification of salt inside pores will create high

    internal tensile stresses− Pore/crack growth will result.− Exacerbates fracture?

    G. Haag,” Properties of ATR-2E Graphite and Property Changes due to Fast Neutron Irradiation”, Juel-4183, 2005

  • Degradation - oxidation

    0123456789

    1011

    0 0.5 1 1.5 2 2.5 3

    PCEA

    IG-110

    NBG-18

    Pure PCEA NBG-17

    Wei

    ght l

    oss,

    %

    PCEA

    NBG-18

    • Lots of data and studies on graphite oxidation

    • Need to develop improved models based on new data

  • Radioactivity – tritium and fp build-up• Build-up of tritium

    − Especially important for dissolved fuel

    • Does graphite retain it? Diffusion rate?− Any build-up?

    • Important for HTR design as well− Source term for accident calculations.

    − Waste disposal issues− How does temperature affect release rates (accident)?− Diffusion rate at accident temperatures?

  • Nondestructive Evaluation of Graphite• Desperately need development of NDE Technologies for large components

    and In-Service Inspection (ISI)• Conventional NDE Inspection technologies applicable to Graphite

    – Eddy Currents, X-Ray Radiography, and Ultrasonics

    Ultrasonics

    Laser Based UT

    Contact UT

    X-Ray Source

    X-Ray Radiography

    Induction CoilAC Magnetic Field

    Eddy Currents

    Test Piece

    Eddy Currents

  • 27

    Will Windes Idaho National [email protected] (208) 526-6985