Materials for Advanced Fission and Fusion Reactors · 1 Managed by UT-Battelle for the U.S....

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1 Managed by UT-Battelle for the U.S. Department of Energy Materials for Advanced Fission and Fusion Reactors Steve Zinkle Nuclear Science & Engineering Directorate Oak Ridge National Laboratory NE50: Symposium on the Future of Nuclear Energy School of Nuclear & Radiological Engineering & Medical Physics Georgia Tech, Atlanta, GA November 1, 2012

Transcript of Materials for Advanced Fission and Fusion Reactors · 1 Managed by UT-Battelle for the U.S....

1 Managed by UT-Battelle for the U.S. Department of Energy

Materials for Advanced Fission and Fusion Reactors

Steve Zinkle Nuclear Science & Engineering Directorate

Oak Ridge National Laboratory

NE50: Symposium on the Future of Nuclear Energy

School of Nuclear & Radiological Engineering & Medical Physics

Georgia Tech, Atlanta, GA

November 1, 2012

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Timeline of some key events for nuclear energy and materials and computational science

1940 1950 1960 1970 1980 1990 2000 2010

CP-1 Graphite

Shippingport

Development of Mat. Sci.

as an academic discipline

reactor JET: Q=0.65, 0.5s

1 Gflops achieved;

high performance

computing centers

established

1 Tflops 1 Pflops

Nuclear >10%

US electricity

ENIAC

Tokamak era begins

ITER

NIF

1st stellarator

& Tokamak

1st MD simulation of radiation damage

(500 atoms, 1 min. time step)

multimillion atom MD simulations

(~1 fs time step)

TFTR: Q=0.27 JT-60:

Qeq=1.25

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US Reactor Fuel Performance: Higher burnup with fewer failures

Zinkle & Was, Acta Mater., in press

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Materials performance is key for economic and safe fission reactor operation in current LWRs

• Heat generation in UO2-based fuel pellets to high burnup

• Heat transfer across Zr alloy cladding; fission product containment under normal and design-basis transient conditions

• Numerous core internal structures to securely position core

• Reactor pressure vessel for containment of fission products

• Piping and steam generator equipment for heat conversion to electricity

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ARIES-AT Magnetic Fusion Energy concept

F. Najmabadi et al. Fus. Eng. Des. 80 (2006) 3

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New technology, New requirements

Gen-III

Pressurized

Water Reactor

Gen-IV

Fast Reactor

Very High

Temperature

Reactor

Coolant Water Sodium Helium

Power Density (MW/m3) 100 350 5

Coolant Temp. (C) 330 550 1000

Net Plant Efficiency (%) 34 40 50

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Comparison of Gen IV and Fusion Structural Materials Environments

fusion SiC

V alloy, ODS steel

F/M steel

All Gen IV and Fusion concepts pose

severe materials challenges

S.J. Zinkle & J.T. Busby, Mater. Today 12 (2009) 12

S.J. Zinkle ,OECD NEA Workshop on Structural

Materials for Innovative Nuclear Energy Systems,

Karlsruhe, Germany, June 2007

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Radiation Damage can Produce Large Changes in Structural Materials

• Radiation hardening and embrittlement (<0.4 TM, >0.1 dpa)

• Phase instabilities from radiation-induced precipitation (0.3-0.6 TM, >10 dpa)

• Irradiation creep (<0.45 TM, >10 dpa)

• Volumetric swelling from void formation (0.3-0.6 TM, >10 dpa)

• High temperature He embrittlement (>0.5 TM, >10 dpa)

100 nm

50 nm

100 nm S.J. Zinkle, Phys. Plasmas 12 (2005) 058101; Zinkle & Busby, Mater. Today 12 (2009) 12

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Examples of radiation damage degradation

Zinkle & Was, Acta Mater., in press

Contributor to SCC in LWR internals Stainless steels are not attractive options

for high dose Gen IV reactor applications

Tirr=420-580oC

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There are many approaches for radiation resistance

high density of nanoscale precipitates or particles (e.g., ODS steel or Ti-modified austenitic stainless steel)

L.K. Mansur & E.H. Lee, J. Nucl. Mater. 179-181 (1991) 105

Fe-13Cr-15Ni CW (P,Si,Ti,C)-modified High mag of “b”

Operation at temperatures where vacancies are immobile (e.g., SiC composites)

Current LWR core internals

Gen IV SFR core internal structures

after S.J. Zinkle, Chpt. 3 in Comprehensive Nuclear Materials (Elsevier, 2012)

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Heat to Heat Variability has been a Common Feature of Structural Alloys

Heat 1

Heat 2

Heat 3

13.5 N-mm-2

helium

Time (hrs)

Heat 1

Heat 2

Heat 3

5000 10000 15000 20000

Cre

ep s

train

(%

)

13.5 N-mm-2

helium

P.J. Ennis et al. 1984

Alloy 617 Thermal Creep

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New steels designed with computational

thermodynamics exhibit superior mechanical

properties compared to conventional steel

• Three experimental RAFM heats (1537, 1538, and 1539), together with an optimized-Gr.92 heat (C3=mod-NF616), were investigated

• Tensile strength of new TMT steels were much higher than conventional steels

• Dramatic improvement in thermal creep strength also observed

0 100 200 300 400 500 600 700 800

200

400

600

800

NF616

1537

1538

1539

Mod-NF616

Yie

ld S

trength

(M

Pa)

Temperature (oC)

PM2000

F82H

0 100 200 300 400 500 600 700 8000

5

10

15

20

25

30

35

40

1537

1538

1539

Mod-NF616

Tota

l E

long

atio

n (

%)

Temperature (oC)

PM2000

NF616

L. Tan et al. (2012)

1.6X

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Modern steels exhibit reduced hardening and less

embrittlement compared to 1960s-era RPV steel

To = 0.3

y RAFM

To = 0.7

y RPV

YIELD STRENGTH INCREASE, MPa

0 100 200 300 400 500 600T

o SHIFT, oC

0

50

100

150

200

250

F82H-IEA

F82H-HT2

9Cr-2WVTa

Eurofer97(Lucon, SCK-CEN)

Eurofer97(Rensman, NRG)

RPV Steels

(Sokolov, ASTM STP 1325)

T0 s

hif

t, o

C

Embrittlement rate of modern steels

is about 40% that of RPV steels

(normalized to same amount of

radiation hardening)

M.A. Sokolov et al., J. Nucl. Mater. 367-370 (2007) 68 J. Rensman, NRG report 20023/05.68497/P (2005);

M. Lambrecht et al., J. Nucl. Mater. 406 (2010) 84

Hardening rate of modern steels is

about 50% that of RPV steels

RPV steel

Plotted data are 8-9%Cr steels; similar results obtained for

pressure vessel-relevant steels such as modern 2-3%Cr steels

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Advanced Manufacturing Techniques offer the potential to enable rapid fabrication of complex geometries

Examples of additive manufacturing technologies

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High

temperature

during loss of

active cooling

Improved Cladding Properties to

maintain core coolability and retain

fission products

-High temperature clad strength and

fracture

-Thermal shock resistance

-Resistance to melting

-Resistance to hydrogen embrittlement

Improved Fuel Properties

-Lower operating temperatures

-Clad internal oxidation

-Fuel relocation / dispersion

-Enhanced retention of fission

products

-Fuel melting safety margin

Suppressed Reaction Kinetics with Steam

to minimize enthalpy input and hydrogen

generation

-Oxidation rate

-Heat of oxidation

There are three major potential strategies for

accident tolerance

• potential options for fuel cladding include:

– Oxidation-resistant austenitic steels

– Oxidation-resistant coatings on Zr alloy cladding

– Ceramic matrix composite cladding

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Thermal creep strength of some candidate cladding materials

• Mo alloys and steels (and SiC/SiC, not plotted) offer improved high temperature strength

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High-Pressure Steam Oxidation Tests: Comparison of the Extent of Steam Reaction Various materials exposed to pure steam for 8 hours (various flow rates and pressures):

• Zircaloy: Pawel-Cathcart and Moalem-Olander data

• 317 Stainless Steel: ORNL high-pressure tests; thickness loss data

• NITE and CVD SiC: ORNL high-pressure tests; thickness loss data

• 310 Stainless Steel: ORNL high-pressure tests; mass gain data converted to

thickness loss

• FeCrAl Ferritic Steel: ORNL high-pressure tests; mass gain data converted to

thickness loss

0.1

1

10

100

1000

750 800 850 900 950 1000 1050 1100 1150 1200 1250 1300 1350

Mate

rial

Recessio

n [

µm

]

Temperature [ C]

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Several Accident Tolerant Fuel Concepts

are Under Consideration, including:

• UO2 – Zircaloy (Base Case)

• UO2 – FeCrAl (oxidation resistant Steel)

• FCM – FeCrAl Fully Ceramic

Microencapsulated Fuel

UO2

Pellet

Zircaloy

Cladding

Conventional LWR UO2 Rod

Coated

Fuel

Particle

Cladding

(Zircaloy,

Steel, SiC)

LWR FCM Rod

FCM

Pellet

TRISO

Fuel

Particle

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There are numerous proposed fusion blanket technology options, all of which are at a relatively immature TRL

• Key issues include tritium recovery/transport, coolant compatibility, safety, waste disposal/recycling, radiation damage effects, and lifetime limits

• The 3 leading structural materials candidate systems are ferritic/ martensitic steel, V alloys, and SiC/SiC (based on safety, waste disposal, and performance considerations)

• These blanket concepts would utilize a variety of conceptually interesting (but unproven on engineering scale) tritium recovery processes

Structural

Material

Coolant/Tritium Breeding Material

Li/Li He/PbLi H2O/PbLi He/Li ceramic H2O/Li ceramic FLiBe/FLiBe

Ferritic s teel

V alloy

SiC/SiC

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Fusion energy research is approaching a transition from plasma science to fusion engineering science

Option A: IFMIF + fission reactors +ion beams + modeling

Option B: robust spallation (e.g., MTS) + fission reactors + ion beams + modeling

Option C: modest spallation (e.g.,SNS/SINQ) + fission reactors + ion beams + modeling

• An intense neutron source (in concert with enhanced theory and modeling) is proposed to improve understanding of basic fusion neutron effects and to develop & qualify fusion structural materials

New facilities would expand current

knowledge base on ferritic steels

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Detailed timeline of some key facilities for nuclear energy and materials

1942 1944 1946 1948 1950 1952 1956 1958

CP-1

Shippingport

ORR

Obninsk

AM-1

1st radiation damage paper

E.P. Wigner

J. Appl. Phys. 17 (1946) 857

1954

MTR

BSR Graphite

reactor

ETR

Calder

Hill

CP-5

BGRR

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Conclusions

• The impact of materials on the future of fission and fusion energy is pronounced

– New materials for improved accident tolerance and core structures of light water fission reactors; Several potential candidates for improved accident tolerance exist, but further R&D is needed to examine behavior under normal and potential accident scenarios

– Existing structural materials face Gen IV fission and fusion reactor design challenges due to limited operating temperature windows

– May produce technically viable design, but not with desired optimal economic attractiveness

• Substantial improvement in the performance of structural materials can be achieved in a timely manner with a science-based approach

– e.g., Design of nanoscale features in structural materials confers improved mechanical strength and radiation resistance

– Selection of accident-tolerant fuel options for light water fission reactors