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MÖSSBAUER SPECTRA OF IRON CONTAINING NAFION MEMBRANES
E. Bauminger, A. Levy, F. Labenski de Kanter, S. Ofer, C. Heintner-Wirguin
To cite this version:
E. Bauminger, A. Levy, F. Labenski de Kanter, S. Ofer, C. Heintner-Wirguin. MÖSSBAUER SPEC-
TRA OF IRON CONTAINING NAFION MEMBRANES. Journal de Physique Colloques, 1980, 41
(C1), pp.C1-329-C1-330. �10.1051/jphyscol:19801122�. �jpa-00219605�
JOURNAL DE PHYSIQUE
Colloque
C1,suppldment au n
O 1 ,Tome
41,janvier
1980,page
C1-329M~SSBAUER SPECTRA OF
I
RON CONTAIN1 NG NAFION MEMBRANESE.R. Bauminger, A. Levy, F. Labenski de Kanter, S . Ofer and C . Heitner-Wirquin
+
Racah I n s t i t u t e of Physics, the Hebrew University, Jemsalem, Israel.
*
Department of Inorganic and Analytical Chemistry, the Hebrew University, Jemsalem, Israel.Ion containing polymers have been i n t e n s i v e l y s t u d i e d i n r e c e n t years i n s o l u t i o n a s well a s i n t h e s o l i d s t a t e . The common property o f t h i s c l a s s of compounds i s t h e aggregation of t h e i o n s togeth- e r with t h e p o l a r solvent (water) i n t o c l u s t e r s o f various s i z e s i n t h e polymeric. matrix 111. Among t h e i o n containing polymers a r e a l s o t h e i o n ex- change membranes whose i n d u s t r i a l uses have r e c e n t - l y increased due t o improvement i n t h e i r proper- t i e s . One of t h e compn used membranes is Nafion
(perf luorosulfonic acid)
M6ssbauer experiments on Naf ion membranes co- ordinated w i t h f e r r i c c h l o r i d e have been performed i n o r d e r t o d i s t i n g u i s h between t h e d i f f e r e n t kinds of i r o n complexes, t o s t u d y t h e i r s t r u c t u r e and magnetic p r o p e r t i e s and t o estimate t h e s i z e o f t h e c l u s t e r s . For t h e s e measurements t h e hydrogen i o n s of t h e membranes were replaced by t e r v a l e n t i r o n
ions.
We r e p o r t h e r e t h e r e s u l t s o f measurements on t h r e e Nafion samples [provided by t h e courtesy of t h e P l a s t i c Department, Du Pont & Co.). One sample of equivalent weight 1100 (sample 1) was e q u i l i - b r a t e d i n a methanol s o l u t i o n and two samples o f equivalent weights of 1100 (sample 2) and of 1500
(sample 3) were e q u i l i b r a t e d i n aqueous s o l u t i o n s . The d e t a i l e d p r e p a r a t i o n s o f t h e s e membranes were previously described 121. S i m i l a r measurements have been c a r r i e d out on v i n y l p y r i d i n e copolymers by Meyer [31.
~ G s s b a u e r s p e c t r a o f sample 1 were measured between 0.05K and 80K and o f samples 2 and 3, be- tween 1.5K and 200K. Some of t h e s p e c t r a obtained with sample 1 a r e shown i n Fig. 1 , A t 85K t h e spectrum i s composed o f 2 doublets, one w i t h a quadrupole s p l i t t i n g o f 0.44t0.01 m / s and an i s o - n e r s h i f t o f 0.51+0.01 m/s, (isomer s h i f t s a r e
r e l a t i v e t o m e t a l l i c i r o n ) w i t h r e l a t i v e i n t e n s i t y of G O % , t h e o t h e r with a quadrupole s p l i t t i n g o f 1.68+-0.02 mm?s and an isomer s h i f t o f 0.56+0,02 m/s with r e l a t i v e i n t e n s i t y of %20%. A t 4,lK and
lower temperatures t h e r e l a t i v e i n t e n s i t y of t h e f i r s t doublet (subspectrum A) decreases and a mag- n e t i c a l l y s p l i t spectrum (subspectrum B) appears
i n s t e a d . Fig. 2 shows t h e d i s t r i b u t i o n i n t h e values o f t h e hyperfine f i e l d s i n subspectrum B.
I
VELOCITY (mm/sec)
Fig. 1.
-
~ S s s b a u e r s p e c t r a o f 5 7 ~ e i n Nafion, equi- l i b r a t e d with methanol. The s o l i d l i n e s a r e l e a s t squares computer f i t s t o t h e s p e c t r a , assuming 2 quadrupole doublets and a magnetically s p l i t spec- trum with a d i s t r i b u t i o n o f hyperfine f i e l d s given by N(H) = N ~ / [ ~ + [ ( H - H ~ ) / A H ] ~ ] , where AH i s d i f f - e r e n t f o r H>Ho and H<Ho.The r e l a t i v e i n t e n s i t y of t h e second quadru- pole s p l i t subspectrum (C) i s ~ 2 0 % a t a l l tempera- t u r e s . Subspectrum C i s a t t r i b u t e d t o iron-dimers
Article published online by EDP Sciences and available at http://dx.doi.org/10.1051/jphyscol:19801122
C1-330 JOURNAL DE PHYSIQUE
w i t h a n t i f e r r o m a g n e t i c coupling and t o t a l s p i n ze- r o [4]. The temperature dependence o f s u b s p e c t r a A and B i s c h a r a c t e r i s t i c o f superparamagnetic p a r t i c l e s 151. Subspectra A and B correspond t o i r o n containing c l u s t e r s with non uniform s i z e s . A t each temperature, c l u s t e r s with s i z e s smaller than a c r i t i c a l s i z e y i e l d magnetically u n s p l i t s p e c t r a and c l u s t e r s l a r g e r than t h e c r i t i c a l s i z e , y i e l d magnetically s p l i t s p e c t r a .
o im 200 m w MO
HYPERFINE MUlETlC FIELD (KO )
Fig. 2.- D i s t r i b u t i o n o f hyperfine f i e l d s i n sam- p l e 1. The a r e a o f t h e r e c t a n g l e s r e p r e s e n t t h e i n t e n s i t i e s o f s u b s p e c t r a A.
Fig. 3 . - Ratio (%) between t h e i n t e n s i t y o f sub- spectrum A and t h e sum o f t h e i n t e n s i t i e s of sub- s p e c t r a A and B, a s a function of temperature.
The d i s t r i b u t i o n of t h e s i z e s o f t h e aggregates can be deduced from t h e d a t a i l l u s t r a t e d i n Fig. 3, using t h e formula derived by ~ e i l 161 f o r t h e r a t e a t which t h e magnetization changes d i r e c t i o n : f = f o expc-CV/kT). V is t h e volume o f t h e aggre- g a t e , f o and C a r e c o n s t a n t s c h a r a c t e r i s t i c o f t k e m a t e r i a l . Fig. 4 shows t h e d i s t r i b u t i o n o f t h e d i -
ues of f o and C a r e t h e same a s i n Fe2O3 [5], a
0
value o f ~ 2 0 A i s derived f o r d i n Fig. 4. A v a l -
0
ue of d=16A i s derived using t h e c o n s t a n t s given by Coey e t a l .
[ T I .
DIAMETER
Fig. 4 . - D i s t r i b u t i o n o f c l u s t e r diameters i n sample 1.
The s p e c t r a of samples 2 and 3 do n o t change between 4 . 1 and 1.5K and even a t 85K t h e y a r e com- posed o f t h r e e subspectra (A,B,C) w i t h t h e same parameters a s those o f sample 1, except t h a t t h e h y p e r f i n e f i e l d i s about 10% h i g h e r (58515 kOe).
The f a c t t h a t even a t 85K, p a r t o f t h e s p e c t r a is s p l i t , shows t h a t t h e s e samples contain i r o n ag-
o
gregates with d*80A. In sample 2, about 2/3 o f t h e i r o n i o n s which a r e n o t i n dimers, a r e i n ag-
o
g r e g a t e s with a diameter o f *80A and 1 / 3 of them
0
a r e smaller than 15A. In sample 3, about 50% have
0 0
diameters of %80A and %SO% a r e s m a l l e r than 15A.
Conclusions: In t h e Nafion samples examined two kinds o f i r o n s p e c i e s a r e present: (1) c l u s t e r s .
C2) dimers, In t h e sample e q u i l i b r a t e d with me- t h a n o l , t h e mean diameter o f t h e c l u s t e r s i s %20;.
I n t h e water e q u i l i b r a t e d samples, t h e r e a r e l a r g e
0 0
c l u s t e r s , (*80A) and small c l u s t e r s (115A).
REFERENCES
[ll
GIERKE, T.D., The Electrochemical Society Veeting, October 1977, A t l a n t a , Georgia.121 HEITNER-WIRGUIN, C . , Polymer
2
(1979) 371.[3] YEYER, C.T., J. de Physique,
37
(1976) C6-777.141 LECFWJ, R . , NICOLINI, C . , ABELEDO, C.R.,
FRANKEL, R.B., J. Chem. Phys.
59
(1973) 3138.[5] KUNDIG, W . , BOWEL, H., CONSTABARIS, G . , LINDnUIST, R.H., Phys. Rev. 142 (1966) 32.
16) N E ~ L , L . , Ann. Geophysique
5
(1949) 99.1 7 1 COEY, J . Y . , READMAN, P.W., Earth and Planetary Science L e t t e r s
21
(1973) 45.ameters o f t h e aggregates. Assuming t h a t t h e v a l -