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SINGLE CRYSTALS OF CUBIC TERNARY PHASES IN THE DDDAB/D2O/OCTANE SYSTEM

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Submitted on 1 Jan 1990

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SINGLE CRYSTALS OF CUBIC TERNARY PHASES IN THE DDDAB/D2O/OCTANE SYSTEM

M. Cruz, A. Vallêra, C. Toprakcioglu

To cite this version:

M. Cruz, A. Vallêra, C. Toprakcioglu. SINGLE CRYSTALS OF CUBIC TERNARY PHASES IN

THE DDDAB/D2O/OCTANE SYSTEM. Journal de Physique Colloques, 1990, 51 (C7), pp.C7-109-

C7-114. �10.1051/jphyscol:1990710�. �jpa-00231109�

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SINGLE CRYSTALS OF CUBIC TERNARY PHASES IN THE DDDAB/DZO/OCTANE SYSTEM

M.M. CRUZ, A.M. VALL%RA and C. TOPRAKCIOGLU'

Dep. de Fisica, Univ. d e Lisboa/CFMC, Campo Grande, Ed. Cl, F-1700 Lisboa, Portugal

Cavendish Lab., Univ. of Cambzidge. Madingley Road, GB-Cambridge CB3 OHE, Great-Britain

-

La c o n n a i s s a n c e d e s s t r u c t u r e s c u b i q u e s q u i a p p a r a i s s e n t d a n s l e s s y s t e m e s t e r n a i r e s t e n s i o a c t i f / e a u / h u i l e p o u r r a i t d t r e b i e n p l u s p r e c i s e s i l ' o n d i s p o s a i t d e m o n o c r i s t a u x . La p o s s i b i l i t e d ' e n c r o y t r e e s t demontree d a n s c e t e t u d e . On p r g s e n t e d e s r e s u l t a t s de d i f f r a c t i o n de n e u t r o n s e t d e r a y o n s X a u x p e t i t s a n g l e s p a r les p r e m i e r s m o n o c r i s t a u x o b t e n u s pour l e s y s t e m e DDDAB/D20/octane.

A b s t r a c t

-

P r e c i s e knowledge of t h e c u b i c s t r u c t u r e s a p p e a r i n g i n t e r n a r y s y s t e m s s u r f a c t a n t / w a t e r / o i l can b e a c h i e v e d i f s i n g l e c r y s t a l s o f t h e s e p h a s e s c a n b e grown. I n t h i s work t h i s i s shown t o b e p o s s i b l e . Small a n g l e X-ray a n d n e u t r o n s c a t t e r i n g r e s u l t s a r e p r e s e n t e d f o r t h e f i r s t s i n g l e c r y s t a l s o f t h i s t y p e , grown f o r t h e s y s t e m DDDAB/D20/octane.

Microemulsions a r e d i s p e r s i o n s o f o i l a n d w a t e r , s t a b i l i z e d by t h e p r e s e n c e of a m p h i p h i l i c m o l e c u l e s ( s u r f a c t a n t t h a t i n some c a s e s n e e d s a l s o t h e a d d i t i o n of a C O - s u r f a c t a n t ) . I n t h e s e t e r n a r y s y s t e m s o r d e r e d p h a s e s c a n b e found1r2.

Numerous i n v e s t i g a t i o n s , i n c l u d i n g s e l f - d i f f u s i o n a n d c o n d u c t i v i t y measurements3t4, showed t h a t some o f t h e o r d e r e d s t r u c t u r e s a r e c o n t i n u o u s b o t h i n t h e o i l a n d t h e w a t e r p h a s e s . I n s u c h b i c o n t i n u o u s s t r u c t u r e s , nowadays w e l l e s t a b l i s h e d , s e v e r a l w e r e f o u n d t o h a v e c u b i c ~ y r n r n e t r y ~ . ~ . A p o s s i b l e d e s c r i p t i o n o f t h e s e 3 - d i m e n s i o n a l l y o r d e r e d s y s t e m s i s b a s e d t h e n on a p e r i o d i c s u r f a c e s e p a r a t i n g a w a t e r l a b y r i n t h from a n i n t e r p e n e t r a t i n g o i l l a b y r i n t h . We c a n t h i n k o f a s i m p l e s u r f a c e

-

a s s o c i a t e d w i t h a s u r f a c t a n t monolayer

-

s e p a r a t i n g o i l and w a t e r domains, o r assume t h a t t h e s u r f a c e i s a s s o c i a t e d w i t h a b i l a y e r t h a t s e p a r a t e s domains o f t h e same n a t u r e . The f i r s t e x a m p l e s o f t h i s t y p e o f c u b i c s t r u c t u r e s a p p e a r e d i n b i n a r y w a t e r - l i p i d s y s t e m s and were o f t h e s e c o n d t y p e 7 ; t h e f i r s t c o n v i n c i n g e v i d e n c e f o r t h e e x i s t e n c e o f s t r u c t u r e s o f t h e monolayer t y p e was r e p o r t e d o n l y r e c e n t l y 8 .

Article published online by EDP Sciences and available at http://dx.doi.org/10.1051/jphyscol:1990710

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COLLOQUE DE PHYSIQUE

G e o m e t r i c a l l y t h e s e i n t e r f a c e s a r e t e n t a t i v e l y d e s c r i b e d by i n f i n i t e p e r i o d i c c o n s t a n t c u r v a t u r e s u r f a c e s g .

The e x p e r i m e n t a l s t u d y o f t h e s e o r d e r e d s y s t e m s i s u s u a l l y done by X-ray o r n e u t r o n s m a l l a n g l e s c a t t e r i n g from p o l y c r y s t a l l i n e s a m p l e s . However, a much more d e t a i l e d a n d p r e c i s e d e s c r i p t i o n o f t h e i r s t r u c t u r e s c a n b e hoped f o r i f s i n g l e c r y s t a l s a r e a v a i l a b l e .

I n t h e p r e s e n t work w e r e p o r t s m a l l a n g l e X-ray a n d n e u t r o n s c a t t e r i n g measurements i n t h e f i r s t s i n g l e c r y s t a l s grown f o r t h e s y s t e m DDDAB(didodecy1 d i m e t h y l ammonium bromide)/D2O/octane.

DDDAB h a s t h e i m p o r t a n t p r o p e r t y o f f o r m i n g m i c r o e m u l s i o n s w i t h o u t t h e a d d i t i o n o f a n y C O - s u r f a c t a n t . Being p r a c t i c a l l y i n s o l u b l e b o t h i n o i l and w a t e r , i t s c o n c e n t r a t i o n d e t e r m i n e s t h e o i l - w a t e r i n t e r f a c i a l a r e a . The system s t u d i e d , DDDAB/DzO/octane, a p p e a r s a s a v e r y r i g i d non b i r e f r i n g e n t g e l i n a l a r g e domain which e x t e n d s f r o m 35% t o 7 7 % w a t e r c o n t e n t , t h e c u b i c zone r e p r e s e n t e d a p p r o x i m a t e l y i n t h e p h a s e d i a g r a m o f f i g . 1 . A l l t h e p h a s e s i n t h e s e r e g i o n show t h e i n t e r e s t i n g p r o p e r t y o f " r i n g i n g " : t h e y p r o d u c e a c l e a r l y a u d i b l e sound when t a p p e d . R i g i d i t y i s h i g h e r f b r t h e p h a s e s w i t h l o w e r w a t e r c o n t e n t .

F i g . l : P a r t i a l p o s i t i o n o f t h e

D20 80 60

O c t a n e ->

p h a s e d i a g r a m f o r t h e s y s t e m DDDAB/DgO/octane c u b i c p h a s e r e g i o n s .

s h o w i n g t h e

Small a n g l e X-ray d i f f r a c t i o n p a t t e r n s f o r t h e s e s y s t e m s show s p o t t y Debye- S c h e r r e r r i n g s , i n d i c a t i n g t h e e x i s t e n c e o f l a r g e o r d e r e d domains. Based on t h e s e o b s e r v a t i o n s , we c h o s e o u r s y s t e m i n t h e low w a t e r l i m i t o f t h e c u b i c r e g i o n , c o r r e s p o n d i n g t o t h e c o m p o s i t i o n 4 8 . 3 / 3 6 . 4 / 1 5 . 3 ( p e r c e n t w e i g h t r e s p e c t i v e l y f o r DDDAB/D2O/octane). A diamond s t r u c t u r e h a s b e e n a s s i g n e d t o t h i s c o m p o s i t i o n l O .

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o b t a i n e d was r e m e l t e d by h e a t i n g t o a t e m p e r a t u r e a few d e g r e e s above i t s m e l t i n g p o i n t (45OC) a n d i n t r o d u c e d t o X-ray c a p i l l a r y t u b e s of lmm d i a m e t e r . These were s e a l e d i m m e d i a t e l y a f t e r w a r d s .

S i n g l e c r y s t a l s were t h e n grown u s i n g a molten zone t e c h n i q u e , w i t h a growth v e l o c i t y of l e s s t h a n 3mm/h.

F i g . 2 : O p t i c a l m i c r o s c o p e p h o t o g r a p h s o f two s a m p l e s : ( a ) a s f i l l e d i n t o t h e c a p i l l a r y t u b e ; ( b ) s u b m i t t e d t o ' o n e growth c y c l e .

F i g . 2 shows o p t i c a l m i c r o s c o p e p h o t o g r a p h s of two s a m p l e s : one s u b m i t t e d t o no t r e a t m e n t , t h e o t h e r a f t e r one m o l t e n zone g r o w t h c y c l e . W e c a n c o n c l u d e t h a t t h e t u b e f i l l i n g i n d u c e d some p h a s e s e p a r a t i o n b u t , a f t e r o n e g r o w t h c y c l e , t h e t r e a t e d zone h a s a n homogeneous a p p e a r a n c e w i t h o u t p h a s e s e p a r a t i o n .

X-ray s c a t t e r i n g m e a s u r e m e n t s t o o k p l a c e a t t h e M.R.C. L a b o r a t o r y of M o l e c u l a r B i o l o g y , Cambridge, and n e u t r o n s c a t t e r i n g e x p e r i m e n t s i n t h e C . E . A . L a b o r a t o i r e Leon B r i l l o u i n , S a c l a y .

P

-.-

single c r y s t a l

6 p o l w s t a l

F i g . 3 : Comparison between n e u t r o n d i f f r a c t i o n p a t t e r n s o b t a i n e d f o r one s i n g l e c r y s t a l , i n t e g r a t e d i n a n g l e , and t h e p o l y c r y s t a l l i n e i n i t i a l m a t e r i a l .

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COLLOQUE DE PHYSIQUE

To c h e c k f o r c o m p o s i t i o n c h a n g e s d u r i n g c r y s t a l g r o w t h , w e compared t h e n e u t r o n d i f f r a c t i o n p a t t e r n o b t a i n e d w i t h a s i n g l e c r y s t a l , i n t e g r a t e d f o r a s m a l l r e g i o n i n a n g l e , w i t h t h a t o f t h e p o l y c r y s t a l l i n e i n i t i a l m a t e r i a l ( f i g . 3 ) . T h e r e i s o n l y a s l i g h t d e v i a t i o n o f t h e p o s i t i o n of t h e f i r s t r e f l e c t i o n , i n d i c a t i n g t h a t t h e r e i s no i m p o r t a n t c o m p o s i t i o n c h a n g e .

iie show i n f i g s . 4 a n d 5 e x a m p l e s o f t h e s m a l l a n g l e X-ray s c a t t e r i n g r e s u l t s f o r r e c r y s t a l l i z e d g e l s , o b t a i n e d by r o t a t i o n of t h e samples a b o u t an

a x i s p e r p e n d i c u l a r t o t h e d i r e c t i o n o f t h e i n c i d e n t beam. By s c a n n i n g t h e c a p i l l a r y t u b e s l o n g i t u d i n a l l y , and from t h e i n v a r i a n c e o f t h e X-ray p a t t e r n , we c o u l d c o n c l u d e t h a t c r y s t a l s w i t h volumes o f t h e o r d e r o f t h r e e c u b i c m i l l i m e t e r s a r e p r e s e n t .

2400

File 21 1, 90<1-<97

i J

;h 1600

U -+

;?

1200

P) U

c

800 400

-180 -120 0 -60 0 60 120 180 T h e t a (degrees)

(a) (b)

F i g . 4 : X-ray s m a l l a n g l e s c a t t e r i n g i n t e n s i t y f r o m o n e of t h e s a m p l e s i n t e g r a t e d f o r a c o m p l e t e r o t a t i o n a b o u t a v e r t i c a l a x i s : ( a ) 2-dimensional X- r a y d i f f r a c t i o n p a t t e r n ; ( b ) i n t e n s i t y i n t h e "Debye-Scherrer r i n g " shown i n

( a ) a s a f u n c t i o n o f i n - p l a n e a n g l e ( O0 c o r r e s p o n d s t h e d i r e c t i o n o f t h e r o t a t i o n a x i s ) .

0 100 200

-180 -120 -60 0 60 120 180 Theta (degrees)

3 0 0 7 . - ; - - - - -

200

too

(a) (b)

F i g . 5 : Same a s f i g u r e 4 f o r a n o t h e r s a m p l e . The v e r t i c a l l i n e s mark t h e p o s i t i o n o f t h e c a l c u l a t e d ( n n 0) s p o t s f o r two d i f f e r e n t s i n g l e c r y s t a l s

( d a s h e d and f u l l l i n e s ) .

250

-

-

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. ** .

d

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t -

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-

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* ..

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Pile 204, 90<~<97 i

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100 200

(6)

The vertical lines in figs. 4b and 5b mark the positions of the (n n 0 ) planes calculated from two of the known diffraction spots: agreement with experimental results is good. As can be seen from the XY pattern in figs. 4a and 5a, no intense second order could be detected in the range of these spectra.

The experimental conditions were not ideal. These first experiments were not yet aimed at structure solving, but rather at simply testing the possibility of single crystal growth. One major drawback with the X-ray experiment was that we have no information on the sample rotation angle $ at which each of the Bragg reflections occurred (another difficulty was that long exposure to the X-ray beam progressively destroyed the crystalline structure; the reason for this is still unknown). Information on the angle I$ was already available in a similar SANS (Small Angle Neutron Scattering) experiment, but too large a beam area was used and so more than one crystal was always illuminated by the beam. Both these limitations will be overcome in future experiments.

The results presented here are not sufficient for definitive conclusions on the crystal structure. We only demonstrate that the first Bragg reflection is due to (n n 0) type planes and that no intense second order was detected in the range of the experiment, for the composition studied.

The main conclusion is that it is possible to grow macroscopic single crystals of the cubic phases appearing in the ternary system DDDAB/D20/octane.

The mosaic spread was not carefully measured but it is of the order of one degree only.

Acknowledaments

We would like to thank A.R.Faruqi from M.R.C. for making possible the X-ray experiments and the Lab. Leon Brillouin for providing neutron beam facilities.

One of us (M.M.C.) would like to thank L.Auvray from L.L.B. for help during the neutron experiments.

This work was partially funded by a NATO grant.

References

/I/ A.de Geyer and J.Tabony, in "Physics of Amphiphilic Layers", eds.

J.Meunier, D.Langevin and N.Boccara, Springer Verlag, Berlin

/2/ F.D.Blum, S.Pickup, B.Ninham, S.J.Chen and D.F.Evans, J.Phys.Chem.89 (1985) 711

/3/ B.Lindman, N.Kamenka, T.M.Kathopoulis, B.Brun and P.G.Nilsson, J.Phys.Chem.84 (1980) 2485

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COLLOQUE DE PHYSIQUE

/4/ M.Clausse, P.Peyerlasse, J.Hei.1, C.Bonod and B.Lagourette, Nature 293 (1981) 636

/5/ S.Radiman, Ph.D. thesis, Univ. of Cambridge 1989

/6/ P.Barois, S-Hyde, B.Ninham and T.Dowling, Langmuir 6 (1990) 1136

/ 7 / V.Luzatti, H-Mustacchim, A.E.Skoulios and F.Husson, Acta.Cryst.14 (1960)

660

/8/ J.O.Rddler, S.Radiman, A.de Valldra and C.Toprakcioglu, Physica 156&157 (1989) 398

/9/ D.M.Anderson, H.T.Davis, L.E.Scriven and J.C.C.Nitsche in "Advances in Chemical Physics" 77, eds. 1.Prigogine and S.Rice, 1990

/10/ S.Radiman, C.Toprakcioglu and A.R.Faruqi, J.de Physique 51 (1990) 1501

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