• Aucun résultat trouvé

THE EFFECT OF HYDROGEN DURING STRESS CORROSION CRACKING AND CORROSION FATIGUE OF Al-Li-Cu ALLOYS IN 3.5 % NaCl SOLUTIONS

N/A
N/A
Protected

Academic year: 2021

Partager "THE EFFECT OF HYDROGEN DURING STRESS CORROSION CRACKING AND CORROSION FATIGUE OF Al-Li-Cu ALLOYS IN 3.5 % NaCl SOLUTIONS"

Copied!
8
0
0

Texte intégral

(1)

HAL Id: jpa-00226630

https://hal.archives-ouvertes.fr/jpa-00226630

Submitted on 1 Jan 1987

HAL is a multi-disciplinary open access archive for the deposit and dissemination of sci- entific research documents, whether they are pub- lished or not. The documents may come from teaching and research institutions in France or abroad, or from public or private research centers.

L’archive ouverte pluridisciplinaire HAL, est destinée au dépôt et à la diffusion de documents scientifiques de niveau recherche, publiés ou non, émanant des établissements d’enseignement et de recherche français ou étrangers, des laboratoires publics ou privés.

THE EFFECT OF HYDROGEN DURING STRESS CORROSION CRACKING AND CORROSION FATIGUE OF Al-Li-Cu ALLOYS IN 3.5 % NaCl

SOLUTIONS

T. Magnin, M. Rebière

To cite this version:

T. Magnin, M. Rebière. THE EFFECT OF HYDROGEN DURING STRESS CORROSION CRACK-

ING AND CORROSION FATIGUE OF Al-Li-Cu ALLOYS IN 3.5 % NaCl SOLUTIONS. Journal de

Physique Colloques, 1987, 48 (C3), pp.C3-835-C3-841. �10.1051/jphyscol:1987398�. �jpa-00226630�

(2)

JOURNAL DE PHYSIQUE

Colloque C3, supplgment au n09, Tome 48, septembre 1987

THE EFFECT OF HYDROGEN DURING STRESS CORROSION CRACKING AND CORROSION FATIGUE OF Al-Li-Cu ALLOYS IN 3.5 % NaCl SOLUTIONS

T. MAGNIN and M. R E B I ~ R E

E c o l e des M i n e s , 158, C o u r s F a u r i e l , F-42023 S a i n t - E t i e m e C e d e x , France

SYNOPSIS

S t r e s s c o r r o s i o n c r a c k i n g and c o r r o s i o n f a t i g u e t e s t s a t imposed s t r a i n r a t e a r e conducted on a n i n d u s t r i a l Al-Li-Cu a l l o y i n a 3 . 5 % NaCl s o l u i i o n a t imposed poten- t i a l . I n t h e c o n d i t i o n o f t h e t e s t s and f o r s h o r t f a t i g u e l i f e t i m e s , t h e a n o d i c d i s - s o l u t i o n i s shown t o p l a y t h e predominant r o l e d u r i n g c o r r o s i o n - f a t i g u e a t f r e e c o r - r o s i o n p o t e n t i a l . N e v e r t h e l e s s a marked hydrogen e m b r i t t l e m e n t i s o b s e r v e d a t c a t h o - d i c p o t e n t i a l s d u r i n g c o r r o s i o n f a t i g u e of specimens c o n t a i n i n g s u p e r f i c i a l micro- c r a c k s . These o b s e r v a t i o n s a r e d i s c u s s e d t o compare t h e s u s c e p t i b i l i t y t o hydrogen e m b r i t t l e m e n t . o f t h e Al-Li-Cu a l l o y s and o f c o n v e n t i o n a l Al-Zn-Mg a l l o y s d u r i n g s t r e s s c o r r o s i o n and c o r r o s i o n - f a t i g u e t e s t s .

INTRODUCTION

The damaging e f f e c t o f hydrogen i s known t o h e o f p r i o r i m p o r t a n c e t o e x p l a i n t h e s t r e s s c o r r o s i o n c r a c k i n g (SCC) and t h e c o r r o s i o n f a t i g u e (CF) p r o p e r t i e s o f conven- t i o n a l Al-Zn-Mg a l l o y s u s e d i n t h e a e r o s p a c e i n d u s t r i e s C1,2,33. N e v e r t h e l e s s t h e r e i s l i m i t e d knowledge a v a i l a b l e on t h e e n v i r o n m e n t a l e f f e c t s on t h e mechanical ro- p e r t i e s o f t h e v e r y p r o m i s i n g A1-Li a l l o y s [ 4 , 5 , 6 , 7 1 . Up t o d a t e , a n o d i c d i s s o f u t i o n i s e x p e c t e d t o b e t h e main damaging mechanism d u r i n g SCC i n A1-Li a l l o y r 7 1 . I n f a c t , n o t h i n g i s known a b o u t t h e i n f l u e n c e o f hydrogen d u r i n g SCC and CF of t h e s e a l l o y s , even i f hydrogen e m b r i t t l e m e n t h a s b e e n r e c e n t l y s u g g e s t e d t o b e a p o s s i b l e SCC f r a c - t u r e mechanism C61. Moreover l i t t l e a t t e n t i o n h a s b e e n p a i d , a s y e t , t o t h e i n t e r - f a c i a l r e g i o n between CF and SCC, and t o t h e r e s p e c t i v e p a r t s of t h e m e c h a n i c a l dama- ge on t h e SCC and CF p r o p e r t i e s of A1-Li a l l o y s .

Thus t h e aim of t h i s p a p e r i s t o a n a l y s e and compare t h e s t r e s s c o r r o s i o n c r a c k i n g and t h e c o r r o s i o n f a t i g u e b e h a v i o u r o f smooth specimens o f an i n d u s t r i a l Al-Li-Cu a l l o y (CP271) deformed a t imposed s t r a i n r a t e i n a 3 . 5 % NaCl s o l u t i o n , p a y i n g a par- t i c u l a r a t t e n t i o n t o t h e r e s p e c t i v e p a r t of the a n o d i c d i s s o l u t i o n and t h e hydrogen e m b r i t t l e m e n t on t h e damaging p r o c e s s e s .

EXPERIMENTAL PETHOD

Experiments were conducted on an i n d u s t r i a l Al-Li-Cu CP271 a l l o y ( s u p p l i e d b y P e c h i n e y ) c o n t a i n i n g ( i n w e i g h t p e r c e n t ) 2.5 L i , 1 . 3 Cu, 1.0 Mg, 0.09 Z r , 0 . 0 2 Fe and (C 0.25) Zn. The e x t r u d e d p l a t e s have been s o l u t i o n t r e a t e d a t 53S°C, t h e n quen- ched i n c o l d w a t e r , s t r e t c h e d by 2 % and a r t i f i c i a l l y aged f o r 12h a t 190°C. T h i s c o r r e s p o n d s t o t h e peak aged c o n d i t i o n s (T651).

The c o r r e s p o n d i n g m i c r o s t r u c t u r e s have been d e s c r i b e d e l s e w h e r e ( t h i s c o n f e r e n c e CBI). Smooth specimens (15 m gauge l e n g t h , 5 mm d i a m e t e r ) were machined from t h e e x t r u d e d p l a t e s on two d i r e c t i o n s : t h e L and TL d i r e c t i o n s a s d e s c r i b e d i n d e t a i l s i n C81.

The o b s e r v e d p r e c i p i t a t e s f o r t h e T651 h e a t t r e a t m e n t a r e t h e 6 ' (A13Li) p r e c i - p i t a t e s i n t h e m a t r i x , t h e 6 ( ~ l L i ) p r e c i p i t a t e s a t g r a i n b o u n d a r i e s , t h e S' (AlzCuMg) and 6' (Al3Zr) p r e c i p i t a t e s i n t h e m a t r i x . The T I (AlnCuLi) p r e c i p i t a t e s seem t o b e v e r y r a r e . They have been shown t o ~ r e c i p i t a t e a t g r a i n b o u n d a r i e s C71.

SCC

te

t s l w e r e performed u s i n g t h e s l o w s t r a i n r a t e method i n the s t r a i n r a t e range 10 's- < b < 1 0 - ~ s - ' a s d e s c r i b e d e l s e w h e r e r f l . CF t e s t s were c o n d u c t e d i n t e n s i o n - c o m p r e s s i o n under s y m m e t r i c a l p l a s t i c s t r a i n c o n t r o l (AE / 2 ) , a t c o n s t a n t

P

Article published online by EDP Sciences and available at http://dx.doi.org/10.1051/jphyscol:1987398

(3)

C3-836 J O U R N A L D E PHYSIQUE

s t r a i n r a t e E , u s i n g a s e r v o h y d r a u l i c machine [ 3 1 .

A l l t h e e x p e r i m e n t s a r e made i n r e p l e n i s h e d 3.5 % NaCl s o l u t i o n s a t pH 6 ( a e r a t e d o r d e s a e r a t e d ) and u n d e r p o t e n t i o s t a t i c c o n t r o l . T e s t s a r e performed e i t h e r a t f r e e c o r r o s i o n p o t e n t i a l o r a t imposed c a t h o d i c p o t e n t i a l . The b e h a v i o u r i n t h e c o r r o s i v e s o l u t i o n s i s compared t o t h e b e h a v i o u r i n a i r ( w i t h 60 % h u m i d i t y ) and u n d e r vacuum ( 2 . T o r r )

.

The s e n s i t i v i t y t o SCC and t o CF i s q u a n t i t a t i v e l y d e f i n e d by t h e r a t i o s A(NaCl)/

A ( a i r ) and N.(NaC1)/Ni(air) r e s p e c t i v e l y . A i s t h e e l o n g a t i o n t o f r a c t u r e and N . t h e number o f c y i l e s t o c r a c k i n i t i a t i o n ( c o r r e s p o n d i n g t o a 1 % r a p i d d e c r e a s e of *he s a t u r a t i o n peak s t r e s s ) . N. h a s been shown t o b e a q u i t e r e l e v a n t p a r a m e t e r t o cha- r a c t e r i s e t h e i n i t i a t i o n o!C c r a c k s l e a d i n g t o p r o p a g a t i o n i n volume ( f o r more d e t a i l s , s e e C91).

EXPERIMENTAL RESULTS T e n s i l e p r o p e r t i e s i n a i r

The y i e l d s t r e n g t h (Y.S.), u l t i m a t e t e n s i l e s t r e n g t h (U.T.S.) and t h e e l o n g a t i o n t o f r a c t u r e (A ) o f t h e CP271 T651 a l l o y a r e shown on t a b l e 1 . A comparison i s e s t a - b l i s h e d w i t h c o n v e n t i o n a l Al-Zn-Mg a l l o y s .

E l e c t r o c h e m i c a l b e h a v i o u r

The p o l a r i z a t i o n c u r v e s o f t h e Al-Li-Cu CP271 a l l o y i n t h e a e r a t e d and d e s a e r a t e d 3.5 % NaCl s o l u t i o n a t pH 6 a r e g i v e n on F i g . 1. The f r e e c o r r o s i o n p o t e n t i a l s ( i n r e f e r e n c e w i t h t h e s a t u r a t e d c a l o m e l e l e c t r o d e (SCE)) a r e i n f a c t Eo =

-

740 ~ V / S C E f o r t h e a e r a t e d s o l u t i o n and

-

950 4 Eo <

-

900 mV/SCE f o r t h e d e s a e r a t e d s o l u t i o n . The f r e e c o r r o s i o n p o t e n t i a l s a r e c l o s e d t o t h e p i t t i n g p o t e n t i a l . A c c o r d i n g t o t h e b e h a v i o u r i n t h e c a t h o d i c r e g i o n , t e s t s a t imposed c a t h o d i c p o t e n t i a l n e e d a v e r y r e p r o d u c t i b l e method b e f o r e SCC o r CF e x p e r i m e n t s : t h e p o t e n t i a l i s s l o w l y d e c r e a s e d from E = E t o E = - 1400 mV and t h e n s l o w l y p u t t o t h e a p p r o p r i a t e v a l u e

-

1400 mV

< E < Eo. gelow E =

-

1400 mV, a d a r k l a y e r a p p e a r s o n t h e CP271 s p e c i m e n s . No t e s t s have b e e n made below - 1400 mV/SCE. F i n a l l y , b e f o r e SCC o r CF e x p e r i m e n t s t h e s y s t e m i s s t a b i l i z e d d u r i n g 12h.

SCC p r o p e r t i e s a t f r e e c o r r o s i o n p o t e n t i a l

F i g . 2 shows t h e e f f e c t o f s t r a i n r a t e on t h e e l o n g a t i o n t o f r a c t u r e A o f t h e CP271 a l l o y i n t h e a e r a t e d NaCl s o l u t i o n a t E = E

.

A comparison 2 s e s t a b l i s h e d w i t h t h e c o n v e n t i o n a l 7020 a l l o y f o r peak aned c o g d i t i o n s T6DR ( f o r more d e t a i l s on A l l o y name

CP271 T651

-

t h i s a l l o y , s e e C33). No e f f e c t o f s t r a i n r a t e h a s b e e n e n c o u n t e r e d i n a i r f o r t h e d i f f e r e n t a l l o y s .

On F i g . 2 , i t can b e shown t h a t t h e CP271 a l l o y i n t h e L and TL d i r e c t i o n s e x h i b i t s a good SCC r e s i s t s $ c e compared t o t h e 7020 a l l o y . The c r i t i c a l s t r a i n r a t e t f o r SCC i s a b o u t 3.10 s-' f o r t h e CP271 a l l o y and I O - ~ S - ' f o r t h e 7020 a l l o y .

& = 2 . 1 0 - ~ s - ' , A i s r e d u c e d by a f a c t o r 2 f o r t h e CP271 a l l o y and h y a f a c t o r 3 f o r t h e 7020 a l l o y . I t can b e n o t i c e d t h a t A i s t w i c e h i g h e r f o r t h e L o r i e n t a t i o n t h a n f o r t h e TL o r i e n t a t i o n w h a t e v e r 6 .

0.2% Y.S. ( m a ) 47 1 413 S e c t i o n

l o n g i t u d i n a l L l o n g t r a n s v e r s e TL

CF p r o p e r t i e s of smooth specimens a t f r e e c o r r o s i o n p o t e n t i a l

The i n f l u e n c e o f t h e e n v i r o n m e n ~ ~ o n t h e f a t i g u e b e h a v i o u r of t h e CP271 a l l o y i s shown on F i g . 3 f o r AE / 2 = 3 . 3 . 1 0 and a t h i g h s t r a i n r a t e E? = IO-~S-'. It c a n b e o b s e r v e d t h a t : ( i ) FO!? t h e CP271 L a l l o y t h e f a t i g u e l i f e i s r e d u c e d o n l y by a f a c - t o r 1 . 5 i n a i r i n comparison t o vacuum b u t by a f a c t o r 3.5 i n t h e a e r a t e d NaCl s o l u - t i o n . These r e d u c t i o n s a r e l o w e r t h a n f o r t h e 7020 a l l o y ( f a c t o r 5 f o r N a C l / a i r ) b u t f a t i g u e l i f e t i m e s a r e always l o n g e r f o r t h e 7020 a l l o y .

( i i ) The CP271 TL a l l o y i s n o t s e n s i t i v e t o t h e NaCl s o l u t i o n b e c a u s e o f a v e r y redu- ced f a t i g u e l i f e i n a i r .

UTS ( m a ) 535 476

A

( x )

8 4

(4)

( i i i ) The e f f e c t of t h e o r i e n t a t i o n of t h e specimen i s s e n s i t i v e : t h e peak s t r e s s Au/2 of t h e L o r i e n t a t i o n i s h i g h e r than f o r t h e TL o r i e n t a t i o n .

Moreover, no r e d u c t i o n (NaCl/air) of t h e f a t i g u e l i f e t i m e s has been observed on the CP271 L and TL a l l o y s a t AE 12 >, l o d 3 , c o g t r a r i l y t o the behaviour of the 7020 a l l o y ( r e d u c t i o n by a f a c t o r 5 g t A& /2 = 10 C31). The e f f e c t of s t r a i n r a t e on t h e CF p r o p e r t i e s t h e CP271 L a l l o y

ig

t h e a e r a t e d s o l u t i o n i s shown on F i g . 4. For AE 12 = 3.3.10

,

i t can be ~ b s e r v e c l ~ t h g t :

' ( i ) At h i g h s t r a i n r a t e s ( k 3 10 s ), t h e r e i s no e f f e c t of 6 on t h e f a t i g u e l i f e t i m e s of t h e CP271 TL a l l o y but a marked r ~ d u c t i o n f o r t h e CP271 L a l l o y .

( i i ) A t i n t e r m e d i a t e s t r a i n r a t e s (5. 1 0 - ~ s - < t < 5 . 1 0 - ~ s - ' ) t h e r e i s no CF wha- t e v e r the o r i e n t a t i o n of t h e specimen.

( i i i ) A t low s t r a i n r a t e s a new r e d u c t i o n of t h e f a t i g u e l i f e can be observed.

To analyse t h i s l a s t phenomenon, t h e microcracking process h a s been observed.

CF cracks a r e t r a n s g r a n u l a r under vacuum and a i r whatever t h e s t r a i n r a t e (Fig.

5 a ) , mix ( t r a n s + i n t e r ) i n t h e NaCl s o l u t i o n a t h i g h s t r a i n r a t e s ( F i g . 5b) which emphasizes a d i s s o l u t i o n e f f e c t a t g r a i n boundaries, and i n t e r g r a n u l a r a t low s t r a i n r a t e s (Fig. 5c) i n t h e c o r r o s i v e s o l u t i o m a s f o r SCC. Moreover, only t h i s l a s t case, microcracks form a t the f i r s t 114 c y c l e . I t can be concluded t h a t CF occurs by SCC a t low s t r a i n r a t e s and t r u e CF occurs a t high s t r a i n r a t e s .

To analyse the i n f l u e n c e o f hydrogen on the CF behaviour, t e s t s have been p e r f o r - med on the CP271 L a l l o y i n t h e d e s a e r a t e d s o l u t i o n a t E = E and a t a p p l i e d c a t h o d i c p o t e n t i a l s i n the a e r a t e d s o l u t i o n . The o b t a i n e d r e s u l t s a r e O s u m a r i z e d on Fig. 6 . It can be observed t h a t :

( i ) a t high s t r a i n r a t e s ( t = 10-')s-') t h e r e i s no d i f f e r e n c e between t h e CF beha- v i o u r i n t h e a e r a t e d and i n t h e d e s a e r a t e d s o l u t i o n a t E = E

.

( i i ) a t i n t e r m e d i a t e s t r a i n r a t e s (6 = 2 . 1 0 ~ ~ s - ' ) no CF ogcurs i n t h e a e r a t e d solu- t i o n a t E = E b u t a small r e d u c t i o n ( f a c t o r 1.5) i s observed a t E = E =-1230mV/

c a t h SCE (which cogresponds t o a b a s i c c a t h o d i c c u r r e n t J = 15 1 . ~ ~ / c m 2 ) .

This small r e d u c t i o n i s n o t s i g n i f i c a n t enough tooconclude t h a t hydrogen e m b r i t t l e - ment can take p l a c e i n t h e CP27J a l l o y .

CF p r o p e r t i e s of precycled smooth specimens

It has been shown i n a previous s t u d y on the Al-Zn-Mg a l l o y s C31 t h a t hydrogen embrittlement takes p l a c e d u r i n g CF on t h e s e a l l o y s only when microcracks a r e i n i - t i a t e d mechanically o r by d i s s o l u t i o n . So, CF t e s t s have been done on CP271 L spe- cimens p r e c y c l e d i n a i r d u r i n g 50 c y c l e s a t AE / 2 = t o o b t a i n a d e n s i t y of s u r f a c e rnicroc_r$cks = 18/mm2 a t t h e beginning of thePcF experiments, CF t e s t s a t AE /2 = 3.3.10 and 6 = 2 . 1 0 ~ ~ ~ - ' a r e then conducted on t h e precycled specimens fo! d i f f e - r e n t a p p l i e d p o t e n t i a l s (E = E

,

E = E cath

,

corresponding t o d i f f e r e n t v a l u e s of t h e b a s i c c u r r e n t J measured g u s t b e f o r e t h e CF t e s t ) . The s e n s i t i v i t y of t h e pre- cycled specimens t o ° C ~ i s q u a n t i t a t i v e l y d e f i n e d by t h e r a t i o N . ( ~ a C l ) / N i ( a i Z , ) r where N (NaC1) i s t h e f a t i g u e l i f e t i m e i n the NaCl s o l u t i o n akP& /2 = 3.5.10 of

i p P

t h e p r e c y c l e d specimens and N . ( a i r ) t h e corresponding f a t i g u e - l i f e t i m e i n a i r . The i n f l u e n c e of t h e b a s i c L g a t h o d i c c u r r y t J on t h e r a t i o N . (NaCl)/N. ( a i r ) i s c l e a r l y shown on F i g . 7. For AE / 2 = 3.3.10 an8 k = 2 . 1 0 ' ~ s ' ~ , ~ ~ i t e x i s t i p a marked t h r e s h o l d Joc. A t J 3 Joc a marked r e d u c t i o n of t h e f a t i g u e l i f e of P t h e precycled specimens i s observgd. At J i J , no CF i s observed. These r e s u l t s emphasizes t h e r o l e of t h e hydrogen embrit?leme% which can occur i n t h e CP271 a l l o y f o r a p p l i e d c a t h o d i c p o t e n t i a l s i n t h e c o n d i t i o n s of our-tes:s. F i n a l l y i t must be n o t i c e d t h a t the same t e s t s a t h i g h e r s t r a i n r a t e (6 = 10 s ) i n d i c a t e s no CF e f f e c t whatever J

.

This r e s u l t emphasizes t h e r o l e of t h e d u r s t i o n of the t e s t t o d e t e c t CF and tRe hydrogen embrittlement

.

DISCUSSION AND CONCLUSIONS

From t h e experimental r e s u l t s r e p o r t e d i n t h e p r e s e n t paper, 1t can b e pointed o u t t h a t :

I

-

A t f r e e c o r r o s i o n p o t e n t i a l , t h e anodic d i s s o l u t i o n p l a y s t h e main r o l e i n t h e CF damage of t h e CP271 a l l o y a s ohown by t h e i n t e r g r a n u l a r a t t a c k of t h e c o r r o s i v e s o l u t i o n which promctes crack i n i t i a t i o n (Fig. 5 ) . Moreover, i n t h e s t r a i n r a t e range I O - ~ S - ~ t o 10 's-l, the lower the s t r a i n r a t e t h e longer t h e c o r r o s i o n f a t i g u e l i f e (Fig. 4 ) . This o b s e r v a t i o n confirms t h e r o l e of t h e d i s s o l u t i o n e f f e c t . A t high s t r a i n r a t e t h e d e p a s s i v a t i o n i s more important than a t i n t e r m e d i a t e s t r a i n

(5)

C3-838 JOURNAL DE PHYSIQUE

r a t e and t h e c o r r e s p o n d i n g d i s s o l u t i o n i s t h e n more pronounced.

2

-

A t f r e e c o r r o s i o n p o t e n t i a l , i t e x i s t s a s t r a i n r a t e r a n g e ( c a l l e d " i n t e r m e d i a t e s t r a i n r a t e " ,

-

IO-'s- ) f o r which no CF can o c c u r , t h e d e p a s s i v a t i o n b e i n g n o t s u f f i - c e n t . Moreover, i t h a s been n o t i c e d t h a t , whatever t h e s t r a i n r a t e , no CF o c c u r s a t s t r a i n a m p l i t u d e s A s 1 2 >, f o r t h e CP271 a l l o y , c o n t r a r i l y t o t h e b e h a v i o u r o f t h e 7020 a l l o y f o r i R s t a n c e . T h i s o b s e r v a t i o n c a n be r e l a t e d t o t h e d u r a t i o n o f t h e CF t e s t s i n t h i s c a s e which a r e t o o s h o r t e r t o a l l o w a n e f f e c t o f c o r r o s i o n . 3

-

Hydrogen e m b r i t t l e m e n t h a s been observed a t a p p l i e d c a t h o d i c p o t e n t i a l s , mainly f o r specimens c o n t a i n i n g s u p e r f i c i a l m i c r o c r a c k s formed d u r i n g f a t i g u e i n a i r . T h i s o b s e r v a t i o n emphasizes t h e i n t e r a c t i o n between t h e m i c r o c r a c k s and t h e hydrogen e m b r i t t l e m e n t a s i t was p o i n t e d o u t i n a p r e v i o u s s t u d y on Al-Zn-Mg a l l o y s C31. When m i c r o c r a c k s a r e formed ( m e c h a n i c a l l y on by d i s s o l u t i o n ) t h e l o c a l i z a t i o n of t h e hydro- gen r e d u c t i o n f a v o u r s hydrogen e m b r i t t l e m e n t . N e v e r t h e l e s s , hydrogen e m b r i t t l e m e n t d u r i n g t r u e CF of t h e CP271 a l l o y h a s been observed o n l y f o r c a t h o d i c c u r r e n t s h i g h e r t h a n a c r i t i c a l v a l u e J

.

Thus, i n t h e c o n d i t i o n s o f o u r t r u e CF t e s t s , t h e hydrogen e m b r i t t l e m e n t does n o t ?$ke p l a c e a t f r e e c o r r o s i o n p o t e n t i a l f o r t h e CP271 a l l o y , a s shown on F i g . 7.-However, f o r l o n g e r CF t e s t s , i t w i l l be p a r t i c u l a r l y i n t e r e s t i n g t o s t u d y t h e e v o l u t i o n o f J a s a f u n c t i o n of t h e d u r a t i o n o f t h e t e s t s . It can b e imagined f o r i n s t a n c e a decggase o f J when t h e s t r a i n amplitude a p p l i e d on precy-

0 C

c l e d specimens d e c r e a s e s .

Thus, i t can b e s u g g e s t e d t h a t , when m i c r o c r a c k s a r e formed i n CF o f i n SCC by a n o d i c d i s s o l u t i o n f o r i n s t a n c e , hydrogen e m b r i t t l e m e n t c a n be a ~ o s s i b l e damaging mechanism when t h e t e s t s a r e l o n g enough. Hydrogen e m b r i t t l e m e n t could be o p e r a t i v e w i t h d i s s o l u t i o n d u r i n g SCC t e s t s even a t f r e e c o r r o s i o n p o t e n t i a l . I n t h e same way, when CF o c c u r s by SCC a t v e r y low s t r a i n r a t e , hydrogen e m b r i t t l e m e n t c o u l d b e a l s o o p e r a t i v e f o r CF a t f r e e c o r r o s i o n p o t e n t i a l . T h i s i s t h e s u b j e c t o f f u r t h e r s t u d i e s .

F i n a l l y , i t must b e emphasized t h a t t h e Al-Li-Cu CP271 a l l o y i n t h e NaCl s o l u t i o n seems t o be l e s s s u s c e p t i b l e t o hydrogen e m b r i t t l e m e n t t h a n t h e c o n v e n t i o n a l Al-Zn-Mg a l l o y s i n t h e peak aged c o n d i t i o n s .

REFERENCES

--

C11 M.O. S p e i d e l , Met. Trans. A . , v o l . 6A, 1975, p. 631.

r 2 1 N . J . H . Holroyd and D . H a r d i e , Environment-Sensitive F r a c t u r e , ASTM STP 821, S. Dean, E. Pugh and G. Ugiansky, E d s . , P h i l a d e l p h i a , 1984, p . 534.

1 3 1 T. Magnin, C. Dubessy and P. Rieux, Aluminum a l l o y s : t h e i r p h y s i c a l and mechani- c a l p r o p e r t i e s , E.A. S t a r k e and T.H. Sanders Eds., EMAS, 1986, p. 1177.

C41 L. C h r i s t o d o u l o u , L. S t r u b l e and J . R . P i c k e n s , Aluminium-Lithium 11, E.A. S t a r k e and T.H. Sanders E d s . , THS-AIM., 1984, p. 561.

r 5 1 P . P i z z o , R. Galvin and H. Nelson, i b i d , p . 627.

C61 N . J . Holroyd, A. Gray, G. Scamans and R. Herman, Aluminium-Lithium 111, Baker, Gregson, H a r r i s and P e e l Eds., The I n s t i t u t e o f M e t a l s , London, 1986, p. 310.

171 E . I . M e l e t i s , J . M . S a t e r and T.H. S a n d e r s , Aluminium a l l o y s : t h e l r p h y s i c a l and mechanical p r o p e r t i e s , E.A. S t a r k e and T.H. Sanders E d s . , EMAS, 1986, p . 1157.

C81 T. Magnin, P. Rieux, C. L e s p i n a s s e and C . B a t h i a s , 1987, T h i s c o n f e r e n c e . [9] T . Magnin, L. Coudreuse and J . M . Lardon, S c r i p t a Met., v o l . 1 9 , 1985, p. 1487.

(6)

FIG. I.. P o l a r i z a t i o n curves of t h e Al-Li-Cu CP271 (T651) a l l o y i n t h e a e r a t e d and d e s a e r a t e d 3 . 5 % NaCl s o l u t i o n s a t pH 6 .

FIG. 2. SCC s u s c e p t i b i l i t y of t h e CP271 (L and TL) and t h e 7020 L a l l o y s a t f r e e corro- s i o n p o t e n t i a l f o r peak aged c o n d i t i o n s

.

FIG. 3 . I n f l u e n c e of t h e environment on t h e e v o l u t i o n with the number of c y c l e s N of t h e peak s t r e s s Ao/2 a t AE /2=3.3.10-'

- 3 - 1 P

and t = 18 s

.

Comparison with t h e 7020 a l l o y i n peak aged condi- t i o n s .

(7)

JOURNAL DE PHYSIQUE

FIG. 4. E f f e c t of the s t r a i n r a t e k c on t h e CF s u s c e p t i b i l i t y of t h e CP271 L and TL a l l o y s a t A& / 2 = 3.3.10 i n t h e a e r a t e d s o l u t i o n .

P

( a ) h i g h s t r a i n r a t e i n vacuum ( L = I O - ~ S - ~ )

( b ) h i g h s t r a i n r a t e i n t h e NaCl s o l u t i o n ( t = I O - ~ S - ~ )

FIG. 5 . Crack i n i t i a t i o n modes i n t h e CP271 L a l l o y a t AE / 2 = 3 . 3 . 1 0 ~ ' .

P

( c ) Low s t r a i n r a t e i n t h e NaCl

- 7 -1

s o l u t i o n (t = 2.10 s ) a f t e r 1 / 4 c y c l e .

(8)

FIG. 6. I n f l u e n c e of t h e a p p l i e d p o t e n t i a l on t h e CF b e h a v i o u r of t h e CP271 L a l l o y a t AE / 2 = 3.3.10-' i n t h e a e r a t e d and d e s a e r a t e d s o l u t i o n . (Ecath = - 7260 mV/SCE c o r r e s p o n d i n g t o a b a s i c c a t h o d i c c u r r e n t Jo = 15 p ~ / c m ~ ) .

FIG. 7 . I n f l u e n c e of a p p l i e d c a t h o d i c p o t e n t i a l s and c o r r e s p o n $ i n f b a s i c c a t h o d i c c u r r e n t J on t h e f a t i g u e l i f e t i m e s a t AE / 2 = 3.3.10 and E = Z . I O - ~ ~ - '

P i n t h e 3.5 % NaCl s o l u t i o n o f p r e c y c l e d specimens.

Références

Documents relatifs

increasing the applied stress in a relatively low stress level (approximately the yield stress). This may be due to an increase of piled-up dislocations at the boundary. Namely,

EFFECT OF GRAIN-BOUNDARY STRUC- TURE ON STRESS CORROSION CRACKING IN αCu-Al ALLOY BICRYSTALS... EFFECT OF GRAIN-BOUNDARY STRUCTURE ON STRESS CORROSION CRACKING IN aCu-A1

Constant strain and constant load tests characterized the investigated plate material in the LT-direction being not susceptible to stress corrosion cracking.. In

lntergranular corrosion and exfoliation corrosion (EXCO 48H) only occur in copper containing alloys, regardless of the corrosion test.. We will compare these

L’archive ouverte pluridisciplinaire HAL, est destinée au dépôt et à la diffusion de documents scientifiques de niveau recherche, publiés ou non, émanant des

A specially designed cast mold, which had surface layers composed of inserts of treated sand in the form of biscuit was used in comparing the relative interac- tion

L’archive ouverte pluridisciplinaire HAL, est destinée au dépôt et à la diffusion de documents scientifiques de niveau recherche, publiés ou non, émanant des

This last assumption could explain the low value of the dielectric constant and the behavior observed in thick ceramics layers based on TiCl 3 , where the grain size ranges between