Assessment of High Chromium Oxide Dispersion …

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Assessment of High Chromium Assessment of High Chromium Oxide Dispersion Strengthened Steels Oxide Dispersion Strengthened Steels for Nuclear Applications for Nuclear Applications 5 5 - - 8 September 2005 8 September 2005 Prague, Czech Republic Prague, Czech Republic J.S. Lee J.S. Lee 1) 1) , I.S. Kim , I.S. Kim 2) 2) , C.H. Jang , C.H. Jang 2) 2) , A. Kimura , A. Kimura 3) 3) [email protected] [email protected] 1) 1) Center for Advanced Reactor Research, KAIST, Center for Advanced Reactor Research, KAIST, Daejeon Daejeon , Republic of Korea , Republic of Korea 2) 2) Department of Nuclear and Quantum Engineering, KAIST, Department of Nuclear and Quantum Engineering, KAIST, Daejeon Daejeon , Republic of Korea , Republic of Korea 3) 3) Institute of Advanced Energy, Kyoto University, Institute of Advanced Energy, Kyoto University, Gokasho Gokasho , , Uji Uji , Japan , Japan EUROMAT 2005 EUROMAT 2005

Transcript of Assessment of High Chromium Oxide Dispersion …

Page 1: Assessment of High Chromium Oxide Dispersion …

Assessment of High Chromium Assessment of High Chromium Oxide Dispersion Strengthened Steels Oxide Dispersion Strengthened Steels

for Nuclear Applicationsfor Nuclear Applications

55--8 September 20058 September 2005Prague, Czech RepublicPrague, Czech Republic

J.S. LeeJ.S. Lee1)1), I.S. Kim, I.S. Kim2)2), C.H. Jang, C.H. Jang2)2), A. Kimura, A. Kimura3)3)

[email protected]@kaist.ac.kr1)1) Center for Advanced Reactor Research, KAIST, Center for Advanced Reactor Research, KAIST, DaejeonDaejeon, Republic of Korea, Republic of Korea

2)2) Department of Nuclear and Quantum Engineering, KAIST, Department of Nuclear and Quantum Engineering, KAIST, DaejeonDaejeon, Republic of Korea , Republic of Korea 3)3) Institute of Advanced Energy, Kyoto University, Institute of Advanced Energy, Kyoto University, GokashoGokasho, , UjiUji, Japan, Japan

EUROMAT 2005EUROMAT 2005

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Contents Contents

Introduction and ObjectivesIntroduction and Objectives

Experimental proceduresExperimental procedures-- ODS steelsODS steels-- Hydrogen charging and thermally aged conditionsHydrogen charging and thermally aged conditions

Results Results Hydrogen effectsHydrogen effects

-- Transition of fracture strain, changes of fracture modeTransition of fracture strain, changes of fracture mode-- Critical hydrogen concentrationCritical hydrogen concentration

Thermal Aging effectsThermal Aging effects-- SP ductile to brittle transition behaviorSP ductile to brittle transition behavior-- Hardening by thermal aging Hardening by thermal aging

SummarySummary

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IntroductionIntroduction

Oxide dispersion strengthening (ODS) steelsOxide dispersion strengthening (ODS) steels-- Candidate material for fusion reactor blanket, fuel clad in Candidate material for fusion reactor blanket, fuel clad in FBR, and high burnFBR, and high burn--up LWRup LWR

Requirements for fuel clad applicationRequirements for fuel clad application-- high resistance to irradiation embrittlement and swellinghigh resistance to irradiation embrittlement and swelling-- corrosion resistance in high temperature water environmentcorrosion resistance in high temperature water environment-- low susceptibility to hydrogenlow susceptibility to hydrogen--induced cracking and SCCinduced cracking and SCC-- lower DBTT shift by thermal aging embrittlementlower DBTT shift by thermal aging embrittlement……………………

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Corrosion propertiesCorrosion properties

Strong corrosion resistanceStrong corrosion resistance in SCWRin SCWR

H.S. Cho, A. Kimura, S. Ukai, M.Fujiwara, J. Nucl. Mater. 329-333 (2004) 387-391.

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General hydrogen and thermal aging effects in a General hydrogen and thermal aging effects in a high Cr steelhigh Cr steel-- reduction in ductility and toughnessreduction in ductility and toughness-- brittle fracture (brittle fracture (intergrannularintergrannular or or transgrannulartransgrannular))

ObjectivesObjectives-- to investigate the to investigate the effects of effects of hydrogen hydrogen and thermal and thermal aging aging on the mechanical propertieson the mechanical properties of ODS steels of ODS steels ddependependinging on the anisotropy of deformation structureon the anisotropy of deformation structure

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Experimental Experimental Test materialsTest materials--K1; 18.37CrK1; 18.37Cr--0.29W0.29W--0.28Ti0.28Ti--0.368Y0.368Y22OO33

--K2; 13.64CrK2; 13.64Cr--1.65W1.65W--4.12Al4.12Al--0.28Ti0.28Ti--0.381Y0.381Y22OO33

--K3; 16CrK3; 16Cr--1.82W1.82W--4.59Al4.59Al--0.28Ti0.28Ti--0.368Y0.368Y22OO33

--K4; 18.85CrK4; 18.85Cr--1.83W1.83W--0.28Ti0.28Ti--4.61Al4.61Al--0.368Y0.368Y22OO33

--K5; 22.05CrK5; 22.05Cr--1.8W1.8W--4.55Al4.55Al--0.27Ti0.27Ti--0.356Y0.356Y22OO33

--RMS; 9CrRMS; 9Cr--2W2W--0.03Al0.03Al

T-direction

L-direction

Extrusion directionFe-xCr-yW-zAl / Argon gas atomized powder

Y2O3, Ti Powders

Mechanically alloyed by ball mill

Canning and degassing

Hot extrusion

(1423 K, 67 mm dia. to 25 mm dia.)

Heat treatment

(1423K x 1h+ air cooling)

Machining

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Microstructural characteristics of ODS SteelsMicrostructural characteristics of ODS Steels

K1 ODS K2 ODS K4 ODS K5 ODS

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Size & number density of oxide particlesSize & number density of oxide particles

K1 ODS K2 K3 K4 K5

1181.3×10227.3K5 (22Cr-4Al)

1121.6×10226.7K4 (19Cr-4Al)

1181.4×10226.8K3 (16Cr-4Al)

952.3×10226.3K2 (13Cr-4Al)

651.4×10232.4K1 (19Cr)

Average spacing (nm)Density (m-3)Size (nm)

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Hydrogen EffectsHydrogen Effects

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Hydrogen charging during tensile testHydrogen charging during tensile test

Hydrogen charging conditionsHydrogen charging conditions-- cathodiccathodic charging charging -- solution; 1N Hsolution; 1N H22SOSO44 + 10 mg/l As+ 10 mg/l As22OO33-- prepre-- (30 min.) + (30 min.) + inin--situsitu chargingcharging-- current density; 100 ~ current density; 100 ~ --520 A/m520 A/m22

Test TemperatureTest Temperature-- 297 K297 K

Strain rateStrain rate-- 9x109x10--55 /s/s

Hydrogen contentsHydrogen contents-- measured by TDS measured by TDS

Tensile Testing system

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K2 ODS (13Cr-4Al)L-direction T-direction

Tensile stressTensile stress--strain curvesstrain curves

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K4 ODS (19Cr-4Al)

L-direction T-direction

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Transition of fracture strain (Transition of fracture strain (εεpfpf) ) by hydrogen by hydrogen chargingcharging

L-direction T-direction

The critical current density of K2-L, K4-L and a 9Cr2W was approximately -42.5, -23.0 and -4.0 A/m2, respectively.

The critical current density of T-direction was almost 0 A/m2, irrespective of the materials.

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Changes of fracture modeChanges of fracture mode

Brittle

(IG+TG type)

Ductile

(MVC type)

-519 A/m2 -30 A/m2 -514 A/m2

Afte

rcha

rgin

g

K2-L K2-T 9Cr2W

Bef

ore

char

ging

Change in fracture mode from ductile shear rupture to brittle inter + transgrannular fracture by H charging

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Critical hydrogen concentrationof K2 ODS and 9Cr-2W steel is in the range of 10∼12 and 1∼2wppm, respectively.

Critical hydrogen concentration

17 2 16.( / ) 1.3106 10 ( / ) 4.9645 10L InC Hatoms gFe I mA cm= × + ×

H concentration in NISL and input current density in Fe iron [5].

[5] J.L Lee, J.Y. Lee, Scripta METALL. 19 (1985) 341.

9Cr2

W

K2

OD

S

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Thermal Aging EffectsThermal Aging Effects

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Thermal aging treatment and SP testsThermal aging treatment and SP tests

Thermal aging treatmentThermal aging treatment-- from 430 to 475 C up to 1000 h from 430 to 475 C up to 1000 h

Small Punch testSmall Punch testTEM disk type ( TEM disk type ( φφ=3, t=0.25~0.27)=3, t=0.25~0.27)Cross head Speed: 0.2 mm/minCross head Speed: 0.2 mm/minTest Temperature: from RT to 77KTest Temperature: from RT to 77K1 mm diameter steel ball1 mm diameter steel ball

Steel Ball(φ 1.0mm)

PuncherClamping Screws

Specimen(φ 3.0mm)

Die

SP jig

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Changes in SPChanges in SP--energyenergy((437 C + 322 hrs)

80 120 160 200 240 280 3200.0

0.3

0.6

0.9

1.2

1.5

1.8

SP e

nerg

y, J

/mm

Temperature, K

As-received Aged (437oC + 322 hrs)K2 (13Cr-4Al) K3 (16Cr-4Al) K4 (19Cr-4Al)

SP-∆DBTT13 Cr (K2) ~10K

16Cr (K3) ~50 K

19Cr (K4) ~73 K

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Thermally aged ODS steelsThermally aged ODS steels((437 C + 322 hrs)

K1

K5

As-received Aged

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Formation of Formation of αα ́́

10 hours 50 hours 505 hours 1000 hours

475 C Aging (K5 ODS)

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Atomic fluctuation by thermal agingAtomic fluctuation by thermal aging

0 20 40 60 80 100 120

20

1000 hr

505 hr

50 hr

0 hr

Fe

∆C, w

/o

distance, nm0 20 40 60 80 100 120

20

1000 hr

505 hr

50 hr

0 hr

Cr

∆C, w

/o

distance, nm0 20 40 60 80 100 120

20

1000 hr

505 hr

50 hr

0 hr

Al

∆C, w

/o

distance, nm

475 C Aging (K5 ODS)

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Activation energyActivation energy

ArrheniusArrhenius type type

0.00132 0.00138 0.00144 0.0015010

100

1000

10000

log t = (Q/2.3R)(1/T)-CK1, K4 = 11224(1/T) - 13K3 = 11929(1/T) - 14K5 = 12546(1/T) - 15

log

t

1/T, /K

K1, K4 ODS K3 K5

Q/R = 25843 (K1, K4 ODS)

= 27468 (K3 ODS)

= 28889 (K5 ODS)

Q = 214 kJ/mol (K1, K4 ODS)

= 228 kJ/mol (K3 ODS)

= 240 kJ/mol (K5 ODS)

Activation energy

*The activation energy for diffusion of Fe and Cr in a Fe-26Cr alloys was 211 and 203 kJ/mol, respectively [1].

The activation energy for Cr diffusion was 229.8 kJ/mol [3][1] Browdes EA, Brook GB, editors. Smitells metals book. Seventh ed. Heinemann: Butterworth; 1992, p. 13 [3] T. Heumann and H. Böhmer, Arch. Eisenhűttenw., 1960, Vol. 31, p. 749

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Increase in MicroIncrease in Micro--hardnesshardness

1 10 100 1000300

350

400

450

500

550

As

Vic

kers

mic

ro-h

ardn

ess,

Hv

Aging time, hr

475oC aging K1 K2 K3 K4 K5

0 200 400 600 800 1000

0

50

100

150

Incr

ease

in m

icro

hard

ness

, ∆H

v

Aging time, hr

475oC aging K1 K2 K3 K4 K5

475 C Aging

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Generalized Hardening FormulaGeneralized Hardening Formula

14 15 16 17 180

20

40

60

80

100

120

140 ∆Hv=49.4xP-738 (K5) ∆Hv=41.9xP-620 (K4, K1) ∆Hv=35.1xP-533 (K3) ∆Hv=27.9xP-419 (K2)

Har

dnes

s In

crea

se, ∆

Hv

P=T(20+log t)x10-3

∆Hv = 49.4 x P – 738 (K5 ODS)

∆Hv = 41.9 x P – 620 (K1, K4)

∆Hv = 35.1 x P – 533 (K3)

∆Hv = 27.9 x P – 419 (K2)

∆Hv = (2.37Cr-3.02)xT(20+log t)x10-3 –(34.8Cr-31.5)

( 430 < T [K] < 475 C, 5 < t [hour]< 1000, 13 < Cr [w/o] < 22 )

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Relationship yield, SP energy with Relationship yield, SP energy with ∆∆HvHv

300 350 400 450 500 5500.0

0.2

0.4

0.6

0.8

1.0

1.2

1.4

K1 K2 K3 K4 K5

SP

ene

rgy,

J/m

mHardness, Hv

SP energy=2.32-0.0047xHv

300 350 400 450700

800

900

1000

1100

1200

1300

σys[MPa] = 3.41 x Hv - 290

σ ys, M

Pa

Vicker's microhardness, Hv

∆σys [MPa] = 3.41 x ∆Hv , (0 < ∆Hv <120)

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Summary Summary

Cathodic hydrogen charging considerably reduced the tensile ductility of ODS steels accompanied by the change of fracture mode from ductile shear rupture to intergrannular and quasi-cleavage fracture.

The critical hydrogen concentration required to induce brittle cracking in ODS steels is in the range of 10-12 wppm that is almost one order higher value than the 9Cr-2W RMS.

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HHigh Cr ODS steels are experienced significant thermal aging embrittlement at temperatures from 430 to 475 C caused by at temperatures from 430 to 475 C caused by the formation of Crthe formation of Cr--rich coherent ferrite phase, rich coherent ferrite phase, αα'' phase.phase.

The hardening relationship at current test conditions can be The hardening relationship at current test conditions can be obtained successfully as a function of Cr content and aging obtained successfully as a function of Cr content and aging time. time.