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THE BAINITE FORMATION UNDER STRESS IN Cu-Zn-Al ALLOYS

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Submitted on 1 Jan 1982

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THE BAINITE FORMATION UNDER STRESS IN Cu-Zn-Al ALLOYS

K. Takezawa, H. Imamura, K. Tanizaki, S. Sato

To cite this version:

K. Takezawa, H. Imamura, K. Tanizaki, S. Sato. THE BAINITE FORMATION UNDER STRESS IN Cu-Zn-Al ALLOYS. Journal de Physique Colloques, 1982, 43 (C4), pp.C4-741-C4-746.

�10.1051/jphyscol:19824121�. �jpa-00221972�

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JOURNAL DE PHYSIQUE

CoZ2oqv.e C4, suppZ4ment au n o 12, Tome 43, ddcembre 1982 page C4-741

THE BAINITE FORMATION UNDER STRESS IN

Cu-Zn-A1

ALLOYS

K . Takezawa, H . Imamura, K. T a n i z a k i and S . S a t o

Department o f Applied Physics, FaeuZty o f Engineering, Hokkaido University, Sapporo, 060, Japan

( R e v i s e d t e x t a c c e p t e d 29 September 1982)

A b s t r a c t . - B1 s i n g l e c r y s t a l s o f Cu-29.8at%Zn-6.lat%Al a l l o y w i t h d i f f e r - e n t o r i e n t a t i o n were h e a t e d a t t e m p e r a t u r e s h i g h e r t h a n 4 2 0 O ~ u n d e r a t e n - s i l e s t r e s s . Two v a r i a n t c r y _ s t ~ l s of b a i e e h a v i n g d i f f e r e n t h a b i t p l a n e s , f o r example ( 1 2 1 1 2 ) and (12 2 1 1 ) J o r [ I 0 6 5 1 t e n s i l e d i r e c t i o n , from t h a t o f s t r e s s - i n d u c e d m a r t e n s i t e , ( 1 2 2 1 1 ) , were o b s e r v e d a f t e r a c e r t a i n p e r i o d of i n c u b a t i o n . The v a r i a n t c r y s t a l h a v i n g a maximum Schmid f a c t o r w i t h r e s p e c t t o t h e s h e a r on t h e h a b i t p l a n e was p r e f e r a b l y formed i n t h e marten- s i t e c a s e . The c l o s e - p a c k e d p l a n e of m a r t e n s i t e i s t o be t r a n s f o r m e d from

(110) p l a n e o f m a t r i x c r y s t a l by t h e s h e a r o f ( l i 2 ) [ l i i ] . On t h c z h e r hand, i t i s found t h a t t h e v a r i a n t c r y s t a l o f b a i n i t e h a v i n g (12-2-11)-habit p l a n e h a s a l a r g e r Schmid f a c t o r w i t h r e s p e c t t o t h e s h e a r o f ( 1 1 2 ) [ 1 1 1 ] , which would a l s o t r a n s f o r m (110) m a t r i x p l a n e t o t h e c l o s e - p a c k e d p l a n e . The o t h e r v a r i a n t h a v i n g ( 1 2 1 1 2) h a b i t p l a n e h a s a n o r i e n t a t i o n s u c h t h a t t h e f c c s t r u c t u r e c a n be formed by c r o s s i n g w i t h t h e f i r s t one i n p a i r . The c r o s s e d r e g i o n o f t h e s e two b a i n i t e c r y s t a l s was o b s e r v e d a s a p i n k - c o l o r e d a r e a . E l e c t r o n d i f f r a c t i o n p a t t e r n s i n d i c a t e t h a t t h e b a i n i t e h a s a d i s - o r d e r e d 9R s t r u c t u r e . I t i s supposed t h a t t h e i n t r i n s i c t r a n s f o r m a t i o n s h e a r p r o d u c i n g t h e c l o s e - p a c k e d s t r u c t u r e o p e r a t e s p r e f e r a b l y i n t h e b a i n i t e c a s e , whereas t h e m i n i m i z a t i o n o f s t r a i n e n e r g y i n t h e t r a n s f o r m a t i o n i s dominant i n t h e m a r t e n s i t e c a s e . A mechanism o f t h e s h a p e change a s s o c i a t e d w i t h t h e s t r e s s - i n d u c e d b a i n i t i c t r a n s f o r m a t i o n i s a l s o d i s c u s s e d .

I n t r o d u c t i o n . - The b a i n i t i c t r a n s f o r m a t i o n t a k e s p l a c e a t t e m p e r a t u r e h i g h e r t h a n 420°K i n t h e s h a p e memory Cu-Zn a l l o y s [ I ] . T h i s t r a n s f o r m a t i o n accompanying t h e d i f f u s i o n o f Zn atoms o f t e n p r o d u c e s a m a c r o s c o p i c s h a p e change s o - c a l l e d " r e v e r s e s h a p e memory" [ 2 ] and m o d i f i e s t h e c h a r a c t e r i s t i c s o f t h e u s u a l s h a p e memory e f f e c t . The c r y s t a l l o g r a p h i c n a t u r e o f t h e b a i n i t e and m a r t e n s i t e a r e v e r y s i m i l a r and i t i s c o n s i d e r e d t h a t t h e t r a n s f o r m a t i o n s t r a i n s p r o d u c i n g b o t h p r o d u c t s a r e n o t much d i f - f e r e n t [3-51. I n t h i s s t u d y t h e b a i n i t e c r y s t a l s produced u n d e r s t r e s s i n s i n g l e c r y s t a l s o f a Cu-Zn-A1 a l l o y were c r y s t a l l o g r a p h i c a l l y examined comparing w i t h t h e s t r e s s - i n d u c e d m a r t e n s i t e s and d i s c u s s t h e mechanism o f s h a p e change due t o t h e s t r e s s - i n d u c e d b a i n i t i c t r a n s f o r m a t i o n .

E x p e r i m e n t a l p r o c e d u r e . - S i n g l e c r y s t a l s of Cu-Zn-Al a l l o y s c o n t a i n i n g 29.8at%Zn and 6 . l a t % A l were grown i n a n a r g o n - f i l l e d q u a r t z c a p s u l e by t h e m o d i f i e d Bridgman method. Homogenized B1 s i n g l e c r y s t a l s were c u t by a s p a r k machine t o a form o f t e n s i l e specimen. The specimen was p u l l e d a t 423O-523OK under a l o a d o f 100-250 MPa, f o l l o w e d by h e a t i n g f o r 10-30 min. on k e e p i n g t h e l o a d and t e m p e r a t u r e unchang- e d . Then, t h e specimen was unloaded and e t c h e d e l e c t r o l y t i c a l l y t o r e v e a l t h e f o r - mation o f b a i n i t e c r y s t a l s . The specimen w i t h t h e e t c h e d s u r f a c e was a g a i n p u l l e d i n t h e same d i r e c t i o n a t room t e m p e r a t u r e t o o b s e r v e t h e r e l i e f o f s t r e s s - i n d u c e d m a r t e n s i t e . A s i m i l a r m n r p h o l o g i c a l e x a m i n a t i o n on t h e two k i n d s o f t r a n s f o r m a t i o n was made o f p o l y c r y s t a l l i n e s p e c i m e n s by u s i n g o p t i c a l a s w e l l a s e l e c t r o n micro- scopy. The e l e c t r o n d i f f r a c t i o n p a t t e r n s t a k e n from t h i n b a i n i t e p l a t e s were ana- l y s e d t o i d e n t i f y t h e c r y s t a l s t r u c t u r e .

Article published online by EDP Sciences and available at http://dx.doi.org/10.1051/jphyscol:19824121

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C4-742 JOUI<NAL DE PHYSIQUE

Fig&

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D e c r e a s e i n s t r e s s due t o t h e forma- t i o n o f b a i n i t e i n Cu-29.8at%Zn-6.1 a t % N a l l o y on i s o t h e r m a l h e a t i n g a t 473°K. The a r r o w i n d i c a t e s t h e p o i n t where t h e s t r e s s was a r t i f i - c i a l l y r e t u r n e d t o t h e o r i g i n a l v a l u e , 1 0 0 ?Pa.

0 9 10 2 0 30

Time

(

min 1

E x p e r i m e n t a l r e s u l t s . - F i g . 1 i n d i c a t e s t h e v a r i a t i o n i n t e n s i l e stress d u r i n g t h e i s o t h e r m a l t r e a t m e n t a t 473OK o f a s i n g l e c r y s t a l h a v i n g [ l o 7 4 1 s t r e s s a x i s . F o l - l o w i n g t o t h e f o r m a t i o n o f b a i n i t e i n t h e s p e c i m e n , t h e s t r e s s l e v e l d e c r e a s e d g r a d u a l l y d u r i n g t h e h e a t t r e a t m e n t t o t h e p o i n t i n d i c a t e d by a r r o w s where t h e stress l e v e l was a d j u s t e d t o k e e p 1 0 0 MPa. The b a i n i t e c r y s t a l s w e r e formed a f t e r a p e r i o d o f i n c u b a t i o n o f a b o u t 6 min. i n t h i s e x p e r i m e n t . The i n c u b a - t i o n p e r i o d was found t o be a l m o s t t h e same, i n d e p e n d e n t o f t h e amount o f l o a d , 100- 250 NPa, and t h e t e n s i l e d i r e c t i o n s i n t h i s s e r i e s o f e x p e r i m e n t s . The e t c h e d s u r - f a c e showed t h a t t h e b a i n i t e c r y s t a l s h a v i n g two v a r i a n t s o f t h e h a b i t p l a n e , ( 1 2 T

Ti)

and (12 11 2 ) , w e r e formed d u r i n g t h e h e a t t r e a t m e n t [ 3 , 61. I t i s t o be men- t i o n e d t h a t t h e s t r e s s - i n d u c e d m a r t e n s i t e s p r o d u c e d i n t h e s e c o n d e l o n g a t i o n a t room t e m p e r a t u r e h a v e d i f f e r e n t h a b i t p l a n e v a r i a n t s from t h e s e .

P h o t o . 1 i s a n e x a m p l e c l e a r l y d e m o n s t r a t i n g t h e d i f f e r e n c e i n h a b i t p l a n e s o f b a i n i t e and m a r t e n s i t e . The p h o t o g r a p h was t a k e n by a m i c r o s c o p e on t h e e t c h e d s u r f a c e a f t e r h e a t i n g t h e s p e c i m e n f o r 1 5 min. a t 493OK u n d e r a t e n s i l e l o a d o f 1 0 0 MPa i n [ 5 i i ] d i r e c t i o n . One o b s e r v e s t h e s m a l l b l a c k c o n t r a s t s w h i c h c o r r e s p o n d t o b a i n i t e v a r i a n t c r y s t a l s w i t h two o r i e n t a t i o n s g i v e n a b o v e ( P h o t o . l ( a ) ) . Upon l o a d i n g a t room t e m p e r a t u r e a d a r k c o n t r a s t i n d i c a t i n g t h e r e l i e f o f t h e stress- i n d u c e d m a r t e n s i t e a p p e a r e d and i t moved from l e f t t o r i g h t i n t h e v i e w o f m i c r o -

( a ) ( b )

P h o t o . 1 O p t i c a l m i c r o g r a p h s t a k e n i n s u c c e s s i o n , ( a ) t o ( b ) , s h o w i n g t h e f o r m a t i o n o f s t r e s s - i n d u c e d m a r t e n s i t e . The s p e c i m e n was h e a t e d u n d e r s t r e s s a t 473°K t o p r o d u c e b a i n i t e p r e c i p i - t a t e s as i n ( a ) . The h a b i t p l a n e o f s t r e s s - i n d u c e d m a r t e n - s i t e is d i f f e r e n t f r o m t h a t o f b a i n i t e .

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s c o p e . Upon u n l o a d i n g t h e b o u n d a r y b e t w e e n d a r k and w h i t e r e g i o n moved i n t h e re- v e r s e d i r e c t i o n w i t h o u t a n y d i s t u r b a n c e a t t h e b a i n i t e p r e c i p i t a t e s . The b o u n d a r y , w h i c h i s t h e t r a c e o f h a b i t p l a n e o f t h e s t r e s s - i n d u c e d m a r t e n s i t e , c a n b e i n d e x e d a s ( 1 2 7 1 1 ) and t h e v a r i a n t c r y s t a l i s t h e most p r o b a b l e one h a v i n g a maximum Schmid f a c t o r w i t h r e s p e c t t o t h e s h e a r on t h i s h a b i t p l a n e . The above r e s u l t was c o n f i r m - e d f o r v a r i o u s s p e c i m e n s w i t h d i f f e r e n t s t r e s s a x i s . '111e s i t u a t i o n h o l d s when t h e t e n s i l e d i r e c t i o n i s i n d e x e d a s [ u ;

w] ,

where u > v > w > 0 .

I n P h o t o . 1, two b a i n i t e c r y s t a l s w i t h (12

1 n)

and (12 11 2) h a b i t p l a n e s were o b s e r v e d s e p a r a t e l y . However, t h e y grew t o form a c r o s s e d s t r u c t u r e w i t h i n c r e a s i n g t h e h e a t - t r e a t m e n t t i m e . F i g . 2 shows a v a r i a t i o n i n s t r e s s d u r i n g t h e h e a t i n g a t 473°K when a s i n g l e c r y s t a l was p u l l e d i n [ 1 1 1 0 8 ] d i r e c t i o n . The b a i n i t i c t r a n s - f o r m a t i o n s t a r t e d a f t e r a n i n c u b a t i o n o f 6 min. and a l a r g e d r o p i n s t r e s s l e v e l a p p e a r e d a f t e r h e a t i n g t h e s p e c i m e n f o r 9 min.. At t h e t i m e when t h e s t r e s s was s u d - d e n l y d e c r e a s e d , a l o c a l l y s t r e t c h e d r e g i o n a p p e a r e d i n t h e s p e c i m e n a s shown i n a s k e t c h of F i g . 2 . The h e a v i l y d e f o r m e d r e g i o n was c o l o r e d by p i n k , i n d i c a t i n g t h e f o r m a t i o n o f n p h a s e c r y s t a l s w i t h f c c s t r u c t u r e [ 7 1 . A m o r p h o l o g i c a l e x a m i n a t i o n r e v e a l e d t h a t t h e s t r e t c h e d r e g i o n was composed o f t h e c r o s s e d s t r u c t u r e s w i t h a h i g h d e n s i t y .

F i g . 2

( a ) A marked d r o p i n s t r e s s a s s o c i a t e d w i t h t h e f o r m a t i o n o f numerous c r o s s e d s t r u c t u r e s o i b a i n i t e . ( b ) The d e f o r m a t i o n i s c o n c e n t r a t e d t o

t h e r e g i o n where a l a r g e number o f c r o s s e d s t r u c t u r e s a r e formed a s

0 5 10

i n d i c a t e d b y a r r o w . The d r o p i n

Time ( m i n )

( a ) c o r r e s p o n d s t o t h e f o r m a t i o n o f t h i s r e g i o n .

P h o t o . 2 E l e c t r o n m i c r o g r a p h s h o w i n g t h e c r o s s i n g o f b a i n i t e c r y s t a l s . The h a b i t p l a n e s a r e h e n t a t t h e c r o s s e d s t r u c t u r e and t h e c o n t r a s t i s m o d i f i e d i n s i d e t h e c r o s s e d r e g i o n .

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c4-744 JOURNAL D E PHYSIQUE

P h o t o . 2 i s a n e x a m p l e o f e l e c t r o n m i c r o g r a p h s t a k e n f o r a t h i n n e d p o l y c r y s t a l - l i n e s p e c i m e n which was s u b j e c t e d t o a n e n o u g h h e a t - t r e a t m e n t f o r t h e b a i n i t e f o r - m a t i o n . Two v a r i a n t b a i n i t e c r y s t a l s a s i n P h o t o . 1 grew t o form a c r o s s e d s t r u c - t u r e . As p r e v i o u s l y r e p o r t e d [&v10], t h e s t r e s s - i n d u c e d B ; m a r t e n s i t e v a r i a n t s w i t h m o d i f i e d 9R s t r u c t u r e , which h a v e a p a r t i c u l a r c r y s t a l l o g r a p h i c r e l a t i o n w i t h e a c h o t h e r , c a n o n l y c r o s s t o f o r m f c t a; m a r t e n s i t e o f 3R s t r u c t u r e . The o b s e r v e d p a i r o f b a i n i t e v a r i a n t s i n t h i s work was j u s t t h e same a s t h e m a r t e n s i t e p a i r p r e v i o u s l y r e p o r t e d [ 9 ] . I t i s t o b e n o t i c e d t h a t t h e h a b i t p l a n e t r a c e s o f two b a i n i t e v a r i - a n t s c l e a r l y bend a t t h e c r o s s e d r e g i o n and t h e c o n t r a s t i n s i d e t h e c r o s s e d r e g i o n i s d i f f e r e n t f r o m t h e f i n e s t r u c t u r e i n t h e b a i n i t e a s s e e n i n a c i r c l e o f P h o t o . 2 .

P h o t o . 3 A t y p i c a l e l e c t r o n d i f f r a c t i o n p a t t e r n o f b a i n i t e ( a ) w i t h a k e y d i a g r a m ( b ) . Th@ a n g l e y i s e x a c t l y 90".

A t y p i c a l d i f f r a c t i o n p a t t e r n o f t h e b a i n i t e c r y s t a l i s r e p r e s e n t e d i n P h o t o . 3 which a s s u r e s t h a t t h e c r y s t a l s t r u c t u r e i s 9R. Comparing w i t h t h e d i f f r a c t i o n p a t - t e r n from t h e m o d i f i e d 9R s t r u c t u r e o f 6; m a r t e n s i t e , o n e c a n n o t i c e t h a t t h e a n g l e y i n d i c a t e d i n P h o t o . 3 ( b ) is n o t 88' b u t e x a c t l y 90'. M o r e o v e r , c o n t r a r y t o t h e m a r t e n s i t e c a s e , n e i g h e r s p o t s n o r s t r e a k s d u e t o t h e s u p e r l a t t i c e s t r u c t u r e w e r e o b s e r v e d i n v a r i o u s d i f f r a c t i o n p a t t e r n s w i t h d i f f e r e n t o r i e n t a t i o n s . T h e s e r e s u l t s s u p p o r t t h a t t h e b a i n i t e c r y s t a l w i t h 9R s t r u c t u r e i s n o t o r d e r e d and t h e c r o s s e d r e g i o n h a s a l s o a d i s o r d e r e d s t r u c t u r e o f 3R, i . e . , f c c .

D i s c u s s i o n . - It m i g h t b e v e r y i m p o r t a n t t o d i s c u s s t h e r e a s o n why o n e h a s d i f f e r e n t v a r i a n t c r y s t a l s o f b a i n i t e f r o m t h o s e o f m a r t e n s i t e . It would o c c u r i f t h e s h a p e d e f o r m a t i o n s due t o t h e b o t h t r a n s f o r m a t i o n s a r e d i f f e r e n t from e a c h o t h e r . Accord- i n g l y , we f i r s t t r y t o c a l c u l a t e t h e s h a p e c h a n g e due t o t h e b a i n i t i c t r a n s f o r m a t i o n by t h e p h e n o m e n o l o g i c a l t h e o r y t o c h e c k t h i s p o i n t .

S i n c e n o d a t a a r e a v a i l a b l e a s s o c i a t e d w i t h t h e c o m p o s i t i o n a l c h a n g e o r t h e c h a n g e i n l a t t i c e p a r a m e t e r , d u r i n g t h e b a i n i t i c t r a n s f o r m a t i o n i n Cu-Zn-Kt t e r n a r y a l l o y s , we u t i l i z e t h e e x p e r i m e n t a l r e s u l t s i n Cu-Zn b i n a r y a l l o y s . The a u t h o r s h a v e m e a s u r e d t h e c h a n g e i n l a t t i c e p a r a m e t e r s b y X-ray d i f f r a c t i o n d u r i n g t h e b a i n i t i c t r a n s f o r m a t i o n i n Cu-40.5wtXZn a l l o y s [ 6 ] . The r e s u l t s h a v e b e e n a n a l y s e d by u s i n g t h e e q u i l i b r i u m v a l u e s r e p o r t e d by Beck and S m i t h [ l l ] and i t h a s b e e n con- c l u d e d t h a t t h e c o n c e n t r a t i o n o f Zn a t o m s i n b a i n i t e c r y s t a l , c b , i s n e a r l y a con- s t a n t , i . e . 3 5 a t % , w h e r e a s t h a t i n B 1 m a t r i x c r y s t a l , Co, i s changed f r o m 40 t o 4 8 a t ZZn [ 6 ] . I f we u s e t h e s e v a l u e s and set t h e d i l a t a t i o n p a r a m e t e r 6 = 1 , t h e h a b i t p l a n e n o r m a l p and s h e a r d i r e c t i o n dl c a n b e o b t a i n e d a s shown i n t h e t o p t h r e e rows i n T a b l e 1, t h e v a l u e s o f p b e i n g d i f f e r e n t f r o m I 1 2 11 2 ) . I f we u s e 6 s 3 d -

(6)

instead o f 1 , where V and V are t h e corresponding volume o f b a i n i t e and m a r t e n s i t e

b m

c r y s t a l s , r e s p e c t i v e l y [ 1 2 ] , t h e value o f p, i s obtained independent o f Cn and C h as

-

shown i n t h e f o u r t h row i n Table 1 , which i s c l o s e t o { 1 2 1 1 2 } and a l s o c l o s e t o t h e value o f m a r t e n s i t e calculated as shown i n t h e bottom row. The value o f shear d i - r e c t i o n d f o r t h e b a i n i t e i s a l s o derived t o be almost t h e same as t h a t f o r t h e m a r t e n s i t e . T h e r e f o r e , t h e shear deformation should be almost t h e same i n b o t h t r a n s f o r m a t i o n s . From t h e above c a l c u l a t i o n , we conclude t h a t t h e variant c r y s t a l s should be t h e same as t h a t o f m a r t e n s i t e . Consequently, t h e present experimental r e s u l t s support t h a t t h e f a c t o r determining the preferred v a r i a n t s o f " s t r e s s - i n d u c - ed b a i n i t e " i s not t h e o v e r a l l macroscopic shear deformation o f b a i n i t e which could r e l a x t h e applied s t r e s s .

0.40 0.35

Bainite 0.44 0.35

0.48 0.35

Table 1 Calculated h a b i t planes and shear d i r e c t i o n s o f b a i n i t e and m a r t e n s i t e . C and C are t h e c o n c e n t r a t i o n i n matrix and

b

b a i n i t e , r e s p e c t i v e l y . p, dl and 6 and the habit plane normal, shear d i r e c t i o n , and d i l a t a t i o n parameter, r e s p e c t i v e l y .

We now consider t h e p o s s i b i l i t y o f having d i f f e r e n t shear systems t o n u c l e a t e a small b a i n i t e c r y s t a l . R e f e r r i n g t o t h e previous study on t h e pre-martensitic pro- d u c t s i n B 1 m a t r i x i n Cu-Zn a l l o y s [ 1 3 ]

,

we propose a model o f double shears producing t h e b a i n i t e nucleus as shown i n F i g . 3. T h i s model i s s i m i l a r t o Burger's model f o r t h e bcc-hcp t r a n s f o r m a t i o n [ 1 4 ] but a second shear o f {110}<110>

i s added t o get t h e 9 R s t a c k i n g sequence. For t h e v a r i a n t c r y s t a l having ( 1 2 2 1 1 ) h a b i t plane as i n Table 1 , t h e f i r s t shear i n F i g . 3 ( a ) b r i n g s ( 1 1 0 ) matrix plane t o t h e close-packed plane b y ( 1 i 2 ) [ 1 x i ] shears and-she

2 R

s t a c k i n g i s attained by t h e second shear o f ( 1 1 0 ) [ 1 1 0 ] i n F i g . 3 ( b ) . I f ( 1 1 2 ) [ 1 1 1 ] shear i s operated on ( 1 1 0 ) plane instead o f ( l i 2 ) [l'ii] s h e a r , t h e b a i n i t e product has t h e same l a t t i c e corre- spondence as t h e f i r s t one b u t diff_e_rent h a b i t plane, i . e . , ( 1 2 1 n ) . The Schmid f a c t o r s f o r (112) [ l i i ] shear and (112) [ l i l ] shear w i t h respect t o [ u v w] _tensile-- d i r e c t i o n , S(112) and S ( 1 1 2 ) , r e s p e c t i v e l y , have a r e l a t i o n such t h a t S(112)-S(112)=

-($w/3)(u+v)<0. Consequently, i f we assume the shear producing t h e close-packed plane predominates i n t h e process forming b a i n i t e n u c l e u s , t h e experimental f a c t t h a t t h e v a r i a n t c r y s t a l s having (12?=) appear instead o f those having ( 1 2 1 1 1 ) can be understood without d i f f i c u l t y .

The growth o f b a i n i t e w i l l be c o n t r o l l e d by t h e d i f f u s i o n o f Zn atoms from t h e product t o t h e matrix [ 1 4 ] and the experimental r e s u l t s t h a t t h e incubation period appeared t o be independent o f the d i r e c t i o n and amount o f t h e applied s t r e s s can be i n t e r p r e t e d by t h i s mechanism. Moreover, as f a r a s t h e process which produces t h e

" r e v e r s e shape memory" i s concerned, one could i n t e r p r e t e t h a t t h e b a i n i t i c t r a n s - formation proceeds by t h e d i f f u s i o n controlled growth o f t h e stress-induced v a r i a n t c r y s t a l s having ( 1 2 1

n)

h a b i t plane w i t h a s i m i l a r s t r a i n f i e l d as t h a t o f marten- s i t e .

(7)

JOUKSAL DE PHYSIQUE

1 s t s h e a r :

[ l i i ] s h e a r / ~ , = ( 1 / 1 2 ) [ l i i b ,

~ @ ' O l o ,

o n,matrix bainite

2nd s h e a r :

( 1 1 0 ) [ l i 0 ] s h e a r lA2=(1/6) [ I T o ~ , F i g . 3 A d o u b l e s h e a r model p r o d u c i n g t h e b a i n i t e n u c l e u s .

15

h a s b e e n r e p o r t e d s o f a r t h a t two v a r i a n t s o f m a r t e n s i t e h a v i n g ( 1 2 1 1 1 ) and ( 1 2 1 1 2 ) h a b i t p l a n e s a r e s t r e s s - i n d u c e d i n p a i r by p u l l i n g s i n g l e c r y s t a l s p e c i m e n s i n a d i r e c t i o n n e a r [ l o o ] , and a l s o t h a t t h e v a r i a n t s i n p a i r c a n e a s i l y c r o s s t o form a n u; m a r t e n s i t e h a v i n g f c t s t r u c t u r e , which p l a y s a v e r y i m p o r t a n t r o l e t o p r o d u c e t h e r e v e r s i b l e s h a p e memory [7-91. Tn t h e p r e s e n t work, i n a d d i t i o n t o t h e v a r i a n t h a v i n g ( 1 2 2 1 1 ) h a b i t p l a n e , which i s p r e f e r a b l y formed by t h e r e q u i r e m e n t o f c l o s e - p a c k e d s t r u c t u r e , t h e o t h e r o n e h a v i n g ( 1 2 1 1 2 ) h a b i t p l a n e was t r a n s f o r m e d i n p a i r w i t h t h e f i r s t o n e .

The s e c o n d v a r i a n t c r y s t a l h a s a n o r i e n t a t i o n s u c h t h a t i t c a n e a s i l y c r o s s w i t h t h e f i r s t o n e t o form f c c c r y s t a l . The 6! m a t r i x c r y s t a l i n t h e p r e s e n t a l l o y i s u n s t a b l z a t h i g h e r t e m p e r a t u r e and f i n a l l y t r a n s f o r m t o t h e e q u i l i b r i u m t c c s t r u c t u r e , i . e . , n p h a s e . T h e r e f o r e , i t i s q u i t e r e a s o n a b l e t h a t two b a i n i t e c r y s - t a l s h a v i n g p a r t i c u l a r o r i e n t a t i o n s which c o u l d e a s i l y p r o d u c e t h e a c r y s t a l b y c r o s s i n g a p p e a r e d i n p a i r i n t h e p r e s e n t e x p e r i m e n t .

R e f e r e n c e s

.-

[ I ] F l e w i t t ( P . E . ) and Towner(J.W.), J . T n s t . M e t a l s , 1 9 6 7 ,

95,

273.

[ 2 ] P o p s ( H . ) , Shape Memory E f f e c t s i n A l l o y s Ed. P e r k i n s ( J . ) , Plenum P r e s s , New York and London, 1 9 7 5 .

[ 3 ] Garwood(R.D.), J . I n s t . Y e t a l s , 1 9 5 4 ,

83,

6 4 .

[ 4 ] Hornbogen(E.) and k ' a r l i m o n t ( H . ) , A c t a Met., 1 9 6 7 , 15., 943.

[ S ] C o r n e l i s ( 1 . ) and k'ayman(C.M.), A c t a ? l e t . , 1 9 7 4 ,

22,

291.

[ 6 ] Takezawa (K.) and S a t o ( S . ) , J . J a p a n I n s t . M e t a l s , 1 9 7 1 ,

35,

469. (Tn J a p a n e s e ) [ 7 ] S c h r o e d e r ( T . A . ) and k'ayman(C.M.), S c r i p t a Met., 1 9 7 6 ,

10,

241.

[ 8 ] Takezawa(K.) and S a t o ( S . ) , B u l l . Fac. Eng. Hokkaido U n i v . , 1 9 7 4 , No.74, 1 2 5 . ( I n J a p a n e s e )

[ 9 ] Takezawa(K.) and S a t o ( S . ) , P r o c . I n t e r n . Conf. o n N a r t e n s i t l c T r a n s f o r m a t i o n , ICOPlAT-79, 1 9 7 9 , 655.

[ l o ] S a t o ( H . ) , Takezawa(K.) and S a t o ( S . ) , P r o c . J o i n t J . S . / J a p a n S e m i n a r , T r o y , A.Y., U.S.A., 1 9 7 9 , 9 2 .

[ l l ] Deck(L.H.) and S m i t h ( C . S . ) , J . M e t a l s , 1 9 5 2 ,

5 ,

1 0 7 9 .

[ 1 2 ] S r i n i v a s a n ( G . R . ) and Hepworth(M.T.), A c t a Y e t . , 1 9 7 1 ,

19,

1 1 2 1 .

[13! Takezawa(K.) and S a t o ( S . ) , 1 . J a p a n I n s t . M e t a l s , 1 9 7 3 ,

2,

793. ( I n ~ a p a n e s e ) [ 1 4 ] C o r n e l i s ( 1 . ) and Wayvsn(C.M.), S c r i p t a H e t . , 1 9 7 3 ,

L,

5 7 9 .

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