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COMPOSITION DEPENDENT HIGH

TEMPERATURE INTERNAL FRICTION IN MgO

(Al2O3)n SPINELS

J. Woirgard, P. Mazot, M. Halbwacks

To cite this version:

(2)

JOURNAL DE PHYSIQUE

Colloque C10, supplement au n012, Tome 46, decembre 1985 page C10-553

COMPOSITION DEPENDENT HIGH TEMPERATURE INTERNAL FRICTION IN MgO

( A l , 0, ), SPINELS

J. WOIRGARD,P. MAZOT AND M. HALBWACKSf

Laboratoire de Mecanique et Physique des Materiaux, U A CNRS 863, ENSMA, 86034 Poitiers Cedex, France

'Universitk de Savoie, BP 1104, 73011 Chambery Cedex, France

ABSTRACT

Isothermal damping spectra obtained between 800 K and 1100 K i n non s t o i c h i o m e t r i c s p i n e l specimens revealed an important r e l a x a t i o n peak f o r t o r s i o n a l v i b r a t i o n frequencies ranging between 10-4 Hz and 10 Hz.

The corresponding a c t i v a t j o n energy (H = 3.84 eV) i s i n good agreement w i t h c a t i o n i c d i f f u s i o n , i n d i c a t i n g t h a t t h e r e l a x a t i o n probably a r i s e s from s t r e s s induced r e o r i e n t a t i o n o f e l a s t i c d i p o l e s formed by t h e a s s o c i a t i o n o f M~~~ c a t i o n s and s t r u c t u r a l c a t i o n i c vacancies. I n s i n g l e c r y s t a l s t h e o r i e n t a t i o n dependence o f t h e r e l a x a t i o n s t r e n g t h has been i n v e s t i g a t e d leading t o a <110> p o s s i b l e o r i e n t a t i o n f o r t h e e l a s t i c d i p o l e s .

The composition dependence o f t h e r e l a x a t i o n s t r e n g t h has a l s o been i n v e s t i g a t e d i n b o t h p o l y and s i n g l e c r y s t a l s f o r n ranging between 1 and 10. The maximum r e l a x a t i o n s t r e n g t h corresponds t o n values between 2 and 3. I

-

INTRODUCTION

Spinels s t r u c t u r e s can be c h a r a c t e r i z e d by t h e formula :

M2+ M3+ 0 M ~ + and M3+ being r e s p e c t i v e l y d i v a l e n t and t r i v a l e n t c a t i o n s . The u n i t c e l l i s &scribed as an almost p e r f e c t close-packed oxygen s t r u c t u r e w i t h 64 t e t r a h e d r a l s i t e s and 32 octahedrp+l o n e ~ . ~ $ r o m theses s i t e s 8 t e t r a h e d r a l and 16 o$fa;$$ral ones can be occupied by M and M cations, g i v i n g f o r t h e u n i t c e l l .

M '32.

This paper deals w i t h s y n t h e t i c n o n s t o i c h i o m e t r i c s p i n e l s z

MgO(A1203)ncorresponding

t o a s o l i d s o l u t i o n o f alumina A1203 i n t h e Mg2A1204 s t o c h i o m e t r i c compound.

Some d i s o r d e r i n t h e c a t i o n i c d i r e c t d i s t r i b u t i o n a r i s e s from an i n v e r s i o n phenomenon, t h e t r i v a l e n t c a t i o n s normally l y i n g i n octahedral s i t e s , being interchanged w i t h d i v a l e n t ones normally l y i n g i n t e t r a h e d r a l s i t e s . The degree o f i n v e r s i o n amounts between 10 t o 15 % (1,2,3).

A d d i t i o n a l d i s o r d e r a r i s e s from t h e presence o f a l a r g e amount o f s t r u c t u r a l vacancies introduced t o preserve e l e c t r o n e u t r a l i t y :

3 2 A I ~ +

+ o

F o u r i e r a n a l y s i s o f sharp X-ray i n t e n s i t i e s have shown t h a t t h e s t r u c t u r a l vacancies occur i n octahedral s i t e s ( 4 ) . Furthermore Jodgatzinski and Haefner (5)

suggested t h a t t h e most probable arrangement f o r vacancies i s p a i r s formation i n octahedral s i t e s , along <I 10) d i r e c t i o n s i n dense (1 11) planes.

Such defects are s u s c e p t i b l e t o g i v e r i s e t o t h e l a r g e a n e l a s t i c r e l a x a t i o n phenomenon p r e v i o u s l y r e p o r t e d /6,7,8/, b u t o t h e r d e f e c t s a r e p o s s i b l e :

Mg 2t-~g2tor M ~ ~p a i r s , a l s o l y i n g along (1 10) ~ - d i r e c t i o n s .

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C10-554 JOURNAL

DE

PHYSIQUE

Therefore t h e aim o f t h i s paper i s t o study more p r e c i s e l y t h e composition dependence o f t h e r e l a x a t i o n s t r e n g t h i n order t o o b t a i n more p r e c i s e i n f o r m a t i o n about t h e n a t u r e o f t h e d e f e c t r e s p o n s i b l e f o r t h e r e l a x a t i o n .

111- EXPERIMENTAL PROCEDURE

The i n t e r n a l t r i c t i o n pendul um used i n these experiments has been p r e v i o u s l y described (9.10). We s h a l l o n l y r e c a l l t h a t isothermal measurements can be ~ e r f o r m e d i n a wide frequency range, between room temperature and up t o 2000 K.

Specimens were e l a b o r a t e d from powders s u p p l i e d by Baikowsky. For n r a t i o between 1 and 3.5 s i n g l e c r y s t a l s were grown by t h e Verneuil method.

For l a r g e r n values t h e plasma spraying technique was used t o r e t a i n t h e metastable n o n - s t o i c h i o m e t r i c s o l i d s o l u t i o n /11/. P o l y c r y s t a l l i n e specimens were obtained w i t h a p o r o s i t y n o t exceeding 15 %. Due t o t h e l o s s o f magnesia occuring d u r i n g t h e plasma spraying, t h e composition o f t h e f i n a l d e p o s i t was determined by atomic absorption spectrometry and X-ray u n i t c e l l parameter measurement.

I V - EXPERIMENTAL RESULTS

Some i n t e r n a l f r i c t i o n peaks obtained i n s i n g l e c r y s t a l s f o r n values r a n g i n g between 1.5 and 3.5, are shown i n F i g u r e 1. I n t h i s composition domain t h e r e l a x a t i o n s t r e n g t h i s observed t o increase w i t h t h e alumina content up t o n = 3.

For n = 1, which correspond t o t h e equimolar compound, no peak c o u l d be observed. S i m i l a r r e s u l t s were obtained i n polycrystals,. f o r n values ranging between 1 and 10. The r e s u l t s corresponding are p l o t t e d i n F i g u r e 2 ; t h e neat i n t e r n a l f r i c t i o n peaks have been obtained a f t e r removing a low frequency background probably due t o t h e r a t h e r h i g h p o r o s i t y o f t h e specimens. No peak was observed i n pure y alumina. The r e l a x a t i o n appears v e r y a n i s o t r o p i c as can be observed i n F i g u r e 3 i n which a r e p l o t t e d i n t e r n a l f r i c t i o n peaks obtained f o r t h e same composition i n < I 0 0 > < 1 1 0 >

<Ill> s i n g l e c r y s t a l s and a f i n e grained p o l y c r y s t a l i n e specimen.

It can be seen t h a t t h e r e l a x a t i o n s t r e n g t h never vanishes, i n d i c a t i n g t h a t t h e e l a s t i c d i p o l e can be an orthorhombic o r a monoclinic d e f e c t l y i n g along a <110> d i r e c t i o n /12/. I n F i g u r e 4 a r e p l o t t e d t h e peak h e i g h t obtained i n specimens w i t h various compositions. The r e l a x a t i o n s t r e n g t h i s zero i n equimolar m a t e r i a l s , goes through a maximum f o r n between 2 and 3 and tends t o vanish f o r l a r g e n values

-

no peak i s observed i n

r

alumina. The o n l y mechanism a b l e t o e x p l a i n such a behavior i s t h e r e l a x a t i o n o f Mg2+- D p a i r s . I n t h a t case t h e r e l a x a t i o n s t r e n g t h w i l l vary as t h e product o f t h e concentrations, which i s p l o t t e d on t h e same p i c t u r e :

I t can be observed t h a t t h e agreement i s b e t t e r f o r p o l y c r y s t a l s than f o r s i n g l e c r y s t a l s . The f a c t t h a t t h e r e l a x a t i o n process i n v o l v e s t h e motion o f M ~ cations, ~ +

through a vacancy mechanism, i s f u r t h e r confirmed by t h e apparent a c t i v a t i o n energy deduced from t h e frequency s h i f t o f t h e peak w i t h temperature :

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V- CONCLUSION

A c a t i o n i c m o b i l i t y mechanism has been proved t o be r e s p o n s i b l e f o r t h e l a r g e r e l a x a t i o n peak observed i n t h e 900

-

1200 K temperature range i n non s t o i c h i o m e t r i c MgO(A1 203) s p i n e l s . From t h e observed v a r i a t i o n s i n t h e r e l a x a t i o n s t r e n g t h w i t h t h e amount o f solved A1 03, i t has been e s t a b l i s h e d t h a t t h e i n v o l v e d d e f e c t s were ~ g 2 + - p a i r s l y i n g $ong <110> d i r e c t i o n s .

V I

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REFERENCES

/1/ S. HAFNER and F. LAVES, Z. KRIST., 115, 231 (1561

1.

/2/ P. FISCHER, Z. KRIST. 124, 275 (19-

/3/ U. SCHMOCKER and F. WKDNER, J. Phys. C9, L235 (1976). /4/ H. JAGOSZINSKI and H. SAALDFELD, Z. K R I T , 110, 197 (1958). /5/ H. JAGODZINSKI and K. HAEFNER, Z. KRIST, 1 2 r 1 8 8 (1967)

/6/ M. HALBWACKS, Ph. MAZOT and J. WOIRGARD, m s . S t a t . Sol. (a)76, 157 (1983) /7/ M. HALBWACKS, Ph.MAZOT and J. WOIRGARD, Phys. s t a t . Sol.

(m

157 (1983) /8/ J. WOIRGARD, Ph. MAZOT and M. HALBWACKS, Journal de Phys.C9,44, 425 (1983) /9/ J. WOIRGARD, Y. SARRAZIN and H. CHAUMET, Rev. Sci. I n s t . 48, 1322 (1977). /10/J. WOIRGARD e t Ph. MAZOT, Journ. de Phys. C5, 42, 1135 (1T81).

/11/M. VAUDELLE and J.L. BESSON, Ceram. I n t . 7, 4 8 y ( 1 9 8 1 )

/12/A.S. NOWICK and B.S. BERRY', A n e l a s t i c reTaxation i n C r y s t a l 1 ine, Sol i d s , Academic Press, New-York/ London 1972.

/13/ R. LINDER and A.Z. AKERSTROM, Phys. Chem.

-

18, 303 (1958).

F i g u r e 1

-

Relaxation peaks obtained a t 700, 750 and 800 "C i n <I00

>

s i n g l e c r y s t a l s of d i f f e r e n t compositions.

-

exp.clrves waks

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