• Keine Ergebnisse gefunden

RAFM Steels: Status and Enhancement for High-Temperature Performance

N/A
N/A
Protected

Academic year: 2022

Aktie "RAFM Steels: Status and Enhancement for High-Temperature Performance"

Copied!
30
0
0

Wird geladen.... (Jetzt Volltext ansehen)

Volltext

(1)

ORNL is managed by UT-Battelle for the US Department of Energy

RAFM Steels: Status and Enhancement for High-Temperature

Performance

L. Tan and Y. Katoh

Oak Ridge National Laboratory, USA

A.-A.F. Tavassoli

DMN/Dir, DEN, CEA, France

M. Rieth

Karlsruhe Institute of Technology, Germany

H. Tanigawa

Japan Atomic Energy Agency, Japan

Q. Huang

Institute of Nuclear Energy Safety Technology, China

ICFRM-17 | Aachen, Germany | 12-16 October 2015 Acknowledge all the persons who involved and contributed

to the tests and ideas during the R&D activities and the financial support by the respective funding sources in each county.

(2)

2

Outline

U   Introduction to Reduced Activation Ferritic- Martensitic (RAFM) Steels

U   Status of RAFM Research

U   Enhancement of RAFM Steels U   Summary

For Fe-based steels and alloys, many talks on ODS/NFA are given at this conference. There are also a few talks on some new types of alloys for potential use in fusion reactors, such as

Bainitic steels (O41 Wed.) and FeCrAl alloys.

This talk focuses on RAFM steels.

Po4-05 on Thursday

(3)

3

Development of RAFM Steels

U   USA, Japan, and European Union initiated development of RAFM steels in 1980s, and came up with respective alloys such as 9Cr-2WVTa, F82H, and Eurofer97 (adopted in 1997). China, India, Korea, etc. started

relevant R&D activities afterwards.

U   Despite comparable tensile properties as compared with the ASME

codified Grade 91, RAFM steels have significantly lower creep strength at temperatures above ~500°C.

0"

100"

200"

300"

400"

500"

600"

0" 200" 400" 600" 800"

Yield&Stress&(MPa)&

Temperature&(oC)&

Eurofer97"

F82H"

P91"

Eurofer97:"Rieth,"FZKA"6911"(2003)"

F82H:"Tavassoli,"et."al."FED"(2002)"

P91:"NIMS"Creep"Data"Sheet"

(4)

4

Typical Compositions of Representative RAFM Steels as Compared to T91

Element (1) T91 9Cr-2WVTa (2) F82H-BA07 (3) Eurofer97-2 (4) CLAM (5) CNAs (6)

C 0.09 0.11 0.09 0.11 0.10 0.08-0.12

N 0.044 0.021 0.017 0.038 0.04 <0.06

Cr 8.70 8.90 8.00 8.95 8.76 8.3-8.8

Mn 0.35 0.44 0.46 0.55 0.42 <1.0

V 0.22 0.23 0.19 0.20 0.22 0.10-0.25

W 2.01 1.88 1.04 1.40 1.0-1.5

Ta 0.06 0.04 0.14 0.16 0.05-0.15

Si 0.29 0.21 0.17 0.05 <0.2

Ti <0.003 <0.15

Nb 0.072 <0.01 <0.005 0.004 <0.01

Mo 0.90 0.01 <0.01 0.005 <0.01

Ni 0.28 <0.01 <0.01 0.03 <0.01

(1) All the elements have specific ranges for different steels. Other elements set to minimal, e.g., P/S/O/B/Al/Cu/Co/Zr/As/Sn/Sb.

(2) USA ORNL heat 3791.

(3)  F82H-BA07 has ~2X of Ta and N as compared with the ITER-grade.

(4) Eurofer97-2 version (heat 993402) has ~2X of N in Eurofer97 (0.02).

(5)  China Low-Activation Martensitic (CLAM), heat 1105.

(6)  Cast nanostructured alloys (CNAs) – advanced RAFM steels developed at ORNL.

U  L. Malerba: Why is radiation embrittlement minimum at 9Cr in FM steels (O14 at 15:00 on Monday)

U  Q. Huang: Overall progress and strategy of the CLAM project for ITER- TBM procurement (O16 at 15:40 on Monday)

(5)

5

Limits on Alloying Elements and Impurities

U   Restriction by disposal and recycle limits:

–  Mo, Ag, and Nb

proved to be the most important of the

restricted elements.

0" 5" 10" 15" 20"

Nb"

V"

Mo"

Ti"

316SS"

Al"

appm$He/dpa$

Fission"Spectra"

Fusion"Spectra"

[After G.L. Kulcinski of Univ. of Wisconsin]

[R.L. Klueh, et al., JNM 280 (2000) 353]

U   Fusion spectra result

in extremely higher

appm He/dpa ratio

than fission spectra,

leading to the limit of

some elements.

(6)

6

Outline

U   Introduction to Reduced Activation Ferritic- Martensitic (RAFM) Steels

U   Status of RAFM Research

U   Enhancement of RAFM Steels

U   Summary

(7)

0 100 200 300 400 500 600 0

100 200 300 400 500 600 700

stress, MPa

Temperature (°C)

(RP0.2)min (Rm)mi n

Sm

Mechanical Properties of CLAM

q   Fabrication technology has been mature.

q   All-around mechanical property tests are in progress.

Tensile (>700 specimens)

Impact properties (>1,000, ~100 curves)

Fracture toughness (~40 specimens )

Fatigue properties (LCF/HCF) (~200 specimens)

Creep Properties (>8,000 hrs, ~150 specimens)

10 100 1000

120 140 160 180 200

应力,MPa

断裂时间,h

-200 -150 -100 -50 0

-20 0 20 40 60 80 100 120 140 160 180 200 220

Absorbed Energy, J

Temperature,

DBTT ≈ –80°C

Stress rupture results under 600°C

Tensile properties

Fatigue properties Impact properties

Fracture toughness

Rupture time, h Stress, MPa

(8)

Fatigue Properties of CLAM

1000000 1E7

230 240 250 260 270 280 290 300

310 550?

450?

Stress amplitude (MPa)

fatigue life (N)

1000 10000 100000

0.4 0.6 0.8 1.0 1.2 1.4 1.6 1.8 2.0 2.2

INEST(RT) IMR(RT) INEST(450 ) INEST(550 )

Total axial strain range (%)

Number of cycle to failure (Nf)

Low cycle fatigue (LCF) at different temperature High cycle fatigue (HCF) at different temperature

æ   With the test temperature increases, fatigue life was slightly decreased under LCF, but significantly

decreased under the HCF condition.

(9)

Creep Properties of CLAM

Creep curve at 550°C Minimum creep rate vs. Stress

at 550 and 600°C Coarse M23C6 after creep test at 550°C for 1595h

æ   The creep property of CLAM steel was similar to that of Eurofer97.

A series of creep tests were carried out at 500, 550, 600 and 650°C with stresses of 150–300 MPa (~200 specimens).

(10)

Mechanical  proper�es  of  20t-­‐F82H  Plates   with  Different  Thicknesses

Tensile  and  Charpy  impact  proper�es  of  plates  with  difference  thicknesses   from  18  to  100  mm,  which  were  made  from  F82H-­‐BA12  heat  melted  in  a   20  tons  electric  arc  furnace.    

No  significant  thickness  dependence  was  observed  in  tensile  property,   but  Charpy  impact  property  degraded  with  increasing  thickness  of  plate.  

Tensile  proper�es  (Ttest=RT)   Charpy  impact  proper�es  

H.  Sakasegwa  /JAEA,  Presented  at    ISFNT12  2015  

(11)

Thermal Aging Effect on Impact Toughness

æ   Aging-induced increase of DBTT and decrease of USE of CLAM is consistent with the F82H-IEA at 600°C, but not consistent at 650°C.

600°C

650°C

[Full-size L-T orientation F82H- IEA: K. Shiba, et al., Fus. Eng.

Des. 86 (2011) 2895.]

–63 J

+40°C –20 J

+30°C

(12)

12

Fracture Toughness of Eurofer97 at Transition Region

U  The code RCC-MRx edition 2015 for Eurofer97 validates the full materials properties (irradiated section will be included in the next edition).

0 50 100 150 200 250 300 350 400

-200 -150 -100 -50

EEuurrooffeerr 9977--11 UUnnIIrrrr ((EEPPFFLL && NNRRGG))

KJC (1T), MPam

Temperature, °C KJC(1T) = 12+88 Exp(0.019(T-To)

(To = -90 °C) 0

100 200 300 400 500

-200 -150 -100 -50

EEuurrooffeerr 9977--11

UUnnIIrrrraaddiiaatteedd CCTT SSppeecciimmeennss

CIEMAT-0.5T NRG-0.2T (8 mm) NRG-0.2T (14 mm) NRG-0.2T (25 mm) NRG-0.4T (14 mm) NRG-0.4T (25 mm) EPFL-0.35T (L-T) EPFL-0.35T (T-L) EPFL-0.87T (L-T) Master Curve 5% confidence 95% confidence

KJC (1T), MPam

Temperature, °C

KJC(1T) = 30+70 Exp(0.019(T-To)) (To = -95 °C)

5%

95%

U  The updated tests of fracture toughness indicate that the lower bound curve does not adequately cover the scatter of the data, leading to the proposal of using a lower

median curve.

(13)

High-Energy Spallation Neutron Irradiation of CLAM

æ   ~20dpa high energy spallation neutron irradiation properties of

CLAM are similar to those of the other RAFMs.

(14)

Post  irradia�on  tensile  proper�es  above  80dpa

Target  design  window  and  HFIR    irradia�on  condi�ons

ü   Con�nuous  irradia�on  hardening  was  observed  above  80  dpa  even  at  400  and   500  ˚C,  where  so�ening  was  observed  at  the  FFTF/MOTA  experiment.

RAFM  (F82H,  etc)   Irradia�on  experiment  JP-­‐28  &  29  in  HFIR   over  a  period  of  8+  years,  supported  by   the  U.S.  DOE  –  JAEA  Collabora�on  on   Fusion  Materials.    

Tensile  tests  of  F82H  at  irradia�on  temp.

500oC 400oC 300oC

Eurofer97 BOR60@330°C

U  T. Hirose/JAEA: I21 at 11:00 on Tue.  

(15)

15

Effect of He on RAFM

O56 at 15:10 on Wednesday

Po1-66 on Monday

U  Effect of He on 9Cr-2WVTa (USA) has been studied by doping 2 wt% Ni-58 and Ni-60 isotopes. They were irradiated in HFIR to >80 dpa at 300–500°C through the U.S. DOE–JAEA Collaboration.

U Richard Kurtz/PNNL: High dose He & dpa effects on

microstructure and deformation mechanisms in RAFM and NFA (P8 at 09:10 on Wednesday).

U Yong Dai/PSI: Deformation mechanisms of FM after irradiation to a wide dpa and He range in spallation neutron targets (I14 at 14:30 on Monday).

U ORNL and KIT are collaborating on investigating the effect of He on Eurofer97 and CNAs by

alloying 54Fe isotope in the two types of alloys to be irradiated in HFIR.

(16)

Long-term Corrosion Test in Flowing Pb-Li

Po2-14 on Tuesday

U Temperature: 480oC (DRAGON-I) U Flow rate : 0.10m/s

U Samples : CLAM (0408B) U  Test time : 10,000 h

U  Temperature: 550°C (PICOLO) U  Flow rate : 0.1m/s

U  Samples : CLAM and Eurofer U Test time : 12,000 h

î  Corrosion rate of ~18.5 µm/yr at 480

o

C and

~220 µm/yr at 550

o

C (0.1 m/s), a little lower than that of Eurofer.

U  Compared to the 475°C limit for DCLL blanket, preliminary study indicates FeCrAl alloy can work at 550°C and up to 800°C in Pb-Li.

CLAM: Z. Jiang – O86 at 9:10 on Friday.

(17)

§ First Wall § Cover and Cooling Plates

Fabrication Technologies for TBM

v   Fabrication of key components of blankets using the EB and HIP welding

v   Blanket Module Assembling

Cover Plates

Cooling Plates

§ Fabrication of 1/3 scale DFLL-TBM

ü Validation of the welding and assembly techniques

ü Validation of the feasibility of the assembly procedure

æ   The key technologies for TBM fabrication have been successfully tested and developed.

1/3-scale DFLL-TBM

U-type plates and tubes EB welding

Water and Gas Elimination HIP welding

U  Ji-Ming Chen: Material development for ITER TBM and beyond in China (P7 at 08:30 on Wednesday).

U  Arun Kumar Bhaduri: RAFM steel and fabrication technologies for the Indian TBM for ITER-issues and challenges (O94 at 11:20 on Friday).

(18)

Evalua�on  of  HIP  joint  in  first  wall  mockup

HIP:    1100°C  /150  MPa  

Normalizing  (PHHT)  at  960°C,  tempering  as   second  PHHT  at  750°C.

T. Hirose, et al., Fusion Eng. Des. 83 (2008) 1176

D0=5 D1

6

11 3

R0.5

   

6SQ-­‐5D  w/  hole

Unit:  mm

3mm  thick  torsion  specimens  were  machined  out  from   HIP  joints  between  cooling  channels  of  a  HIPed  First  wall   component,  and  evaluated  successfully.

Trial HIP joint component

Hardening  of  the  base  metal   seemed  to  be  suppressed  by   the  presence  of  the  HIP  

joint,  causing  ~22%  

reduc�on  of  total  work   during  torsion  process.

Base metal: τyield=425MPa, τmax=565MPa HIP joint: τyield=458MPa, τmax=564MPa

T.  Nozawa  /JAEA,  Presented  at    ASTM-­‐SSTT  2014  

(19)

O

Ouuttlliinnee

U   Introduction to Reduced Activation Ferritic- Martensitic (RAFM) Steels

U   Status of RAFM Research

U   Enhancement of RAFM Steels

U   Summary

(20)

Advanced Steels

Ø   Steels for Water Cooling

u 4 new heats produced, characterisation started

Ø   Steels for High Temperature Applications

u Alternative heat treatment and TMT on EUROFER à VERY SUCCESSFUL !!!

u 14 new heats produced, characterisation started

20  

EUROfusion  –  WPMAT  Progress/Status  

O22 at 12:20 on Tuesday U  Po4-02 (J. Hoffmann, et al.):

Improvement of mechanical and microstructural properties of Eurofer through TMT

U  Po1-17 (U. Jäntsch, et al.): TEM at samples of TMT-ed RAFM steels U  O21 at 12:00 on Tue. (Y.B. Chun,

et al.): Influence of TMT on microstructure and mechanical properties of ARAA

U  Effect of non-standard heat treatments on Eurofer97

(21)

21  

Highlights

Adjustment  of  EUROFER  proper�es  by  varying  heat   treatment  temperatures  

U   Austeni�sa�on:  980  °C  –  1150  °C   U   Tempering:  700  °C  –  760  °C  

Tensile  Strength   Creep  Strength   Charpy  Proper�es  

(22)

22

Motivation of CNAs

U   The significant recovery of T91 at 600°C and 100 MPa suggests that the less amount of MX in the current RAFM steels (e.g., Eurofer97) would have worse resistance to recovery.

0"

0.01"

0.02"

400" 600" 800" 1000" 1200" 1400"

Phase&Mole&Frac-on&

Temperature&(oC)&

M23C6"

Laves"

Z" MX"

""""""""""T91"

""""""""""Eurofer97"

T91@600°C/100MPa/34,141h

[K. Kimura, et al., Key Eng. Mater.

171-174 (2000) 483]

Noticeable aging-induced softening in F82H-IEA at T > 500°C.

[K. Shiba, et al., Fus. Eng. Des.

86 (2011) 2895.]

(23)

23

U   Higher Cr

23

C

6

amount results in greater creep rate.

High Cr23C6

Low Cr23C6 [F. Abe, Nature 2003]

Tested at 650°C/140MPa

Better Performance

U   Coarse Z-phase forms by consuming fine MX during long-term services.

U   Laves phase coarsening degrades strength.

/70MPa

[K. Sawada, MST 2013]

[Q. Li, Metall Mater Trans A 2006]

637°C

Early stage (Fine Laves)

Long-term (Coarse Laves)

Fe2(Mo,W)

Stress accelerates the replacement of MX by Z-phase.

Concerns of Current 9-12Cr FM Steels

(V/Nb/Ta)N Cr(V/Nb/Ta)N

T91 T92

V, wt% 32.4 34.8

Cr 44.0 44.2

Nb 19.4 16.3

Fe 4.2 4.7

@600°C 34,141h 39,540h Size 166 nm 155 nm Fraction 0.7% 0.3%

[K. Sawada, et. al. ISIJ Inter. 46 (2006) 769.]

(24)

24

Design of Strengthening Precipitates

U   The superior stability of TaC under thermal, stress, and irradiation as

compared with TaN and VN, inspired the development of MC-strengthened in

compared with MN-strengthened CNAs.

U   The CNAs are designed to have

–  Increased MX, e.g., MN (with Z-phase) in CNA1 and MC (without Z-phase) in CNA2;

–  Reduced M23C6;

–  Comparable amount Laves phase.

[L. Tan, et al. J. Nucl. Mater. 445 (2014) 104; Acta Mater. 71 (2014) 11]

(c) VN (b) TaN

(a) TaC 20 dpa 20 dpa 20 dpa

0"

0.01"

0.02"

400" 600" 800" 1000" 1200" 1400"

Phase&Mole&Frac-on&

Temperature&(oC)&

M23C6"

Laves"

Z"

MX"

""""""""""CNA1"

""""""""""CNA2"

""""""""""Eurofer97"

Po3-11 on Wednesday

(25)

25

Tensile and Creep Resistance of CNAs

U   CNAs exhibited ~100–300 MPa increases in yield strength compensated by some reductions in ductility as compared with the FM/RAFM steels.

U   Creep at 650°C showed superior creep resistance of CNAs as compared with Eurofer97 and F82H.

0"

10"

20"

30"

40"

50"

60"

70"

80"

90"

100"

0"

100"

200"

300"

400"

500"

600"

700"

800"

0" 200" 400" 600" 800"

Total&Elonga*on&(%)&

Yield&Stress&(MPa)&

Temperature&(oC)&

Eurofer97"

CNA2"

F82H"

CNA1"

P91"

CNA3"

SS-3 (this work) Eurofer97 (FZKA6911) Gauge Cross-Section

0"

20"

40"

60"

80"

100"

120"

140"

160"

180"

10" 100" 1000" 10000"

Stress&(MPa)&

Creep&Life&(h)&

this work SS-3 Eurofer97

Gauge Cross-Section

650oC"

600oC"

F82H"

CNA"

(26)

26

Microstructure of CNAs

U  Lath boundary width (λsgb: 200–

500 nm) is comparable to or less than conventional FM/RAFM steels (350–500 nm).

U  MX nanoprecipitate (di: ~5 nm) density (ni: 1022 m-3) in CNA2 is two orders of magnitude higher than that in Eurofer97 (≥~20 nm;

1020 m–3).

U  Free dislocation density (ρd: 1014 m–2) is comparable to that in FM/

RAFM steels.

MX#(DF)(CNA2# Disloca3ons#(WBDF)#

12x12µm

[Klimenkov et al., Prog. Nucl. Ener. (2012)]

Eurofer97

σsgb ≈≈10Gb / λsgb

σi ≈≈ aMGb dini

σd ≈≈ 0.5MGb ρd

>2X

>1X

~1X

~700 vs. ~500 MPa

~200 vs. ~80 MPa

~300 vs. ~300 MPa

~780 vs. ~580 MPa ~200MPa

(27)

27

Charpy Impact Toughness of CNAs

U   CNA1 (primarily MN) exhibited USE and DBTT comparable to Grade 91.

U   CNA2 and CNA3 (primarily MC) showed significantly increased USE with comparable or lower DBTT as compared with Grade 91.

U   The CNAs and FM steel have remarkably higher USE as compared to the general value of 12-14Cr ODS/NFA.

0"

10"

20"

30"

40"

50"

60"

70"

80"

+150" +100" +50" 0" 50" 100" 150" 200"

Energy,"J"

Temperature,"oC"

G91"

CNA3"

CNA2"

ODS/NFA"

CNA1"

5"mm"

5"mm" 4"mm"

(28)

28

Radiation Hardening and Softening of CNA1

U   HFIR irradiation of CNA1, primarily strengthened by (V,Ta)N, exhibited

–  Slight hardening at 300°C with negligible changes in total elongation.

–  Significant softening with increased total elongations at 500 and 650°C.

U   The behavior is generally consistent with the modified Grade 92 FM steels under the same irradiation conditions, as well as CLAM (HFETR irradiation) at 300°C.

[Courtesy of T.S. Byun of PNNL]

(29)
(30)

Referenzen

ÄHNLICHE DOKUMENTE

Figure 3: Calculated accumulated strain of different steel grades along the solidified steel shell The different phase transformation sequences of type A, B and C steel grades and

Figure Annex H-6 Comparing of response functions of mean (lower) and maximum (upper) cutting forces

The results show that after the microwave treatment on a specific material, the forces applied to the bucket wheel are reduced, due to the decrease of the cutting

To influence the transformation, these precipitates have to be small-sized (nm range) and homogenously distributed. In carbon steels the γ-α transformation is

Allerdings wird verschiedentlich auch darauf verwiesen, dass beim Zugang zu einem Forschungsfeld weder eine fixe Grenze überschritten werde noch sich das Feld nach Überschreiten

In this study, the Taylor-Quinney coefficient β is shown as a function of strain and being influenced by the test specific strain rate and stress state.. The tested material is

Partially Oxidised Products of Magnus Green Salt and Similar Conducting

The calcium cations are shown as large grey spheres, oxygen atoms as white spheres, and boron atoms as black