33 Equilibrium and Kinetic Problems in Mixed Electrolyte Solutions
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RICARDO M . PYTKOWICZ and M . R. COLE Oregon State University, Corvallis, OR 97331
Mixed aqueous electrolyte solutions such as body fluids, rivers, lakes, oceans and, at times, laboratory and industrial fluids present important problems which are not found in single electrolyte solutions. New perceptions and results are being obtained in complex media and some examples will be covered in this paper. The behavior of carbonates will be used to illustrate hetero geneous processes, with emphasis upon the formation of inorganic surface coatings and solid solutions. This is a vital topic in the study of solid-solution interactions since it is coatings rather than bulk phases which are sensed by liquid solutions. Homogeneous reactions will be studied in terms of the competition of coulombic ion pairs with true complexes for anions. An extended form of the phase rule will be used. Phase Rule The phase rule is often used in the form f = c - p + 2 to ascertain the number of degrees of freedom of a system even when the concentration units in the aqueous phase are molal im) or molar. This is not correct because the phase rule is derived in terms of mole fractions (X). Thus, an additional quantity, the total number of moles, is required to convert X into m. This is illustrated by equations below which we shall find useful later on. For t h e s y s t e m CO2-H2O w i t h two p h a s e s , v a p o r and aqueous s o l u t i o n , i f we assume f o r s i m p l i c i t y t h a t pr^O and t h e a c t i v i t y c o e f f i c i e n t s f o r a l l t h e components a r e known, t h e e q u a t i o n s a r e
Ρ = pC0 + ξ ρ .
(1)
2
[C0 ] = k 2
K
h
I =
P
C0
(2)
2
rH C0 ]/[C0 ][H 0] 2
3
2
2
0-8412-0569-8/80/47-133-643$05.00/0 © 1980 American Chemical Society
In Thermodynamics of Aqueous Systems with Industrial Applications; Newman, S., et al.; ACS Symposium Series; American Chemical Society: Washington, DC, 1980.
(3)
644
THERMODYNAMICS OF AQUEOUS SYSTEMS WITH INDUSTRIAL APPLICATIONS
^'
= a [HC0 -]/[H C0 ]
(4)
K '
= a [C0
(5)
H
2
H
K ' +
TC0
3
_
]
3
2
2
2
(6)
2
= [HC0 "]+ 2 [ C 0
+ [H 0] Downloaded by INDIANA UNIV BLOOMINGTON on May 29, 2014 | http://pubs.acs.org Publication Date: October 29, 1980 | doi: 10.1021/bk-1980-0133.ch033
3
']/[HC0
2
+
+ TH 0 = [C0 ]
2
3
2
• [Η ][0Η"]/ΓΗ 0]
w
[H ]
3
3
"] +
2
[OH"]
(7)
+ [H C0 ] + LHC0 "] + 2
+ [H ] +
3
+
3
(8)
[OH"]
T h u s , t h e r e are e i g h t e q u a t i o n s i n n i n e unknowns. The phase r u l e t e l l s us t h a t f = 2 - 2 + 2 = 2 s o t h a t , i f Ρ and Τ a r e f i x e d t h e n t h e s y s t e m i s a t e q u i l i b r i u m and i s s p e c i f i e d . T h i s i s t r u e i n t e r m s o f mole f r a c t i o n s i n s o l u t i o n b u t , f o r m o l a l i t i e s , f = f + 1 = 3 and c = f 2. The t e r m c i s the number o f c o m p o s i t i o n a l v a r i a b l e ? w h i c h must be s p e c i f i e d . Its v a l u e i s 3 - 2 = 1 i n a c c o r d w i t h t h e a n a l y s i s o f t h e above s y s t e m o f e q u a t i o n s , t h a t i s , i n a c c o r d w i t h a system o f e i g h t e q u a t i o n s i n n i n e unknowns. In t h e a b s e n c e o f a v a p o r p h a s e , f = 3 and f = 4 with c = 2. m m m
Solid-Solution
Interactions
A t t h i s p o i n t I s h a l l f o c u s upon t h e e f f e c t o f t h e f o r m a t i o n o f Ca Mg-|. C03 s o l u t i o n s , e i t h e r i n b u l k phases o r i n s u r f a c e c o a t i n g s , upon t h e k i n e t i c and t h e e q u i l i b r i u m b e h a v i o r of carbonates. My t h o u g h t s have r e s u l t e d i n p a r t from t h e e x t e n s i v e l i t e r a t u r e i n t h i s f i e l d , w i t h s p e c i a l r e f e r e n c e to the p a p e r s by Plummer and M a c k e n z i e (1_) and by W o l l a s t and R e i n h a r d Derie (2). C o n s i d e r an aqueous s o l u t i o n c o n t a i n i n g Ca , Mg and CI i o n s t o w h i c h enough Na2CÛ3 i s added t o i n d u c e s u p e r s a t u r a t i o n o f CaC0 . I t has been w e l l e s t a b l i s h e d t h a t , f o r ( M g ) / ( C a ) < 4 , m a g n e s i a n c a l c i t e s o f f o r m u l a CaxMg-j_ C03 p r e c i p i t a t e w h i l e f o r r a t i o s above f o u r a r a g o n i t e s e t t l e s down (3_, £ ) · S e a w a t e r f a l l s i n the l a t t e r c a t e g o r y . The r e a s o n f o r t h e a r a g o n i t e p r e c i p i t a t i o n i s n o t i t s i n t r i n sic stability. The s o l u b i l i t i e s o f c a l c i u m c a r b o n a t e s i n c r e a s e f r o m p u r e c a l c i t e t o m a g n e s i a n c a l c i t e s c o n t a i n i n g up t o a b o u t 10 m o l e p e r c e n t MgC03, t o a r a g o n i t e , and t h e n on t o h i g h m a g n e s i a n calcites. T h u s , a r a g o n i t e i s l e s s s t a b l e than low-magnesian c a l c i t e s [5). I s u s p e c t t h a t a r a g o n i t e comes down b e c a u s e , a t h i g h v a l u e s o f [ M g ] , t h e c a l c i t e n u c l e i a r e q u i t e s o l u b l e due t o t h e i r h i g h magnesium c o n t e n t s and t h e f o r m a t i o n o f c r i t i c a l n u c l e i i s i m p r o b a b l e . T h i s type o f r a t e c o n t r o l o f the polymorph formed i s one a s p e c t o f t y p i c a l s o l i d - m i x e d e l e c t r o l y t e s o l u t i o n systems. L e t us f o c u s upon t h e l o w [Mg ] / [ C a ] c a s e as i t y i e l d s x
x
s
o
l
l
d
2 +
2 +
3
2 +
x
2 +
2
2 +
In Thermodynamics of Aqueous Systems with Industrial Applications; Newman, S., et al.; ACS Symposium Series; American Chemical Society: Washington, DC, 1980.
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33.
PYTKOWICZ A N D COLE
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Mixed Electrolyte Solutions
i n t e r e s t i n g s o l i d s and i s r e l e v a n t t o many f r e s h w a t e r s y s t e m s . A s t e a d y s t a t e i s e v e n t u a l l y r e a c h e d when a s o l i d i s e x p o s e d t o a s o l u t i o n and t h i s s t a t e may be t h e r e s u l t o f r a t e f a c t o r s o r o f thermodynamic o n e s . We s h a l l s e e t h e t h e r m o d y n a m i c c a s e w h i c h o c c u r s i s n o t t h e c o n v e n t i o n a l one a l o n e . 2+ I t i s known t h a t c a l c i t e s formed i n t h e p r e s e n c e o f Mg ions t u r n o u t t o be m a g n e s i a n c a l c i t e s w i t h 0.70 < χ < 1 (1_, 6). The c a l c i t e s may be b u l k p r e c i p i t a t e s a s , f o r e x a m p l e , i n m a r i n e cements o r , i n t h e c a s e o f seeded r u n s , may form c o a t i n g s o f a d i f f e r e n t c o m p o s i t i o n from t h a t o f t h e b u l k p h a s e . Under s p e c i a l c i r c u m s t a n c e s d o l o m i t e may r e s u l t ( 6 ) . D i f f e r e n t r a t e s o f p r e c i p i t a t i o n c a n c a u s e d i f f e r e n t amounts of Mg t o be i n c o r p o r a t e d i n t o t h e s o l i d . One may e x p e c t t h a t a h i g h r a t e , a c h i e v e d by a l a r g e r i n i t i a l a d d i t i o n o f ^ C O s , s h o u l d c a u s e a l a r g e r u p t a k e o f MgC03 and an i n c r e a s e i n t h e solubility of calcite. T h i s w o u l d o c c u r due t o c o l l i s i o n s o f Mg w i t h t h e g r o w i n g c a l c i t e c r y s t a l s w i t h o u t a s much o f a c h a n c e f o r e q u i l i b r a t i o n as i n slower r u n s . T h i s i s i n d e e d shown t o be t h e c a s e i n T a b l e I i n w h i c h t h e r u n s were seeded w i t h c a l c i t e so t h a t we a r e o b s e r v i n g t h e e f f e c t o f c o a t i n g s a n d t o w h i c h d i f f e r e n t amounts o f Na£C0 were a d d e d . The p r i n c i p l e i s t h e same f o r b u l k p h a s e s formed i n unseeded r u n s , n a m e l y , t h a t m e t a s t a b l e s o l i d s c a n be f o r m e d and may p e r s i s t f o r l o n g t i m e s . The p a r t i c u l a r importance o f s u r f a c e c o a t i n g s i s t h a t t h e y , r a t h e r than t h e i n t e r n a l b u l k p h a s e s , g o v e r n t h e i n t e r a c t i o n s w i t h aqueous solutions. The i n c r e a s e i n t h e f i n a l pH r e s u l t s f r o m an enhanced s o l u b i l i t y o f t h e magnesium c a l c i t e s a s t h e pH i n c r e a s e s w i t h a 2 h i g h e r [CO3 -] o f t h e magnesium c a l c i t e s . The i n c r e a s e s o l u b i l i t y r e s u l t s from a h i g h e r magnesium c o n t e n t . 2 +
2 +
3
K^
C a )
= [Ca
K'(M9) = [ M g X
CaC0
3
+
K
2 +
2 +
][C0
][C0
MgC0
3
=
3
2
3
2
"]
(9)
-]
(10)
1
where t h e K values p e r t a i n t o the presence o f a s o l i d s o l u t i o n . These a r e t h r e e e q u a t i o n s i n f o u r unknowns so t h a t t h e r e i s an a d d i t i o n a l degree o f c o m p o s i t i o n a l freedom. I n t e r m s o f t h e phase r u l e t h e s y s t e m w i t h t h e components C a ^ - M g ^ - C O ^ - r ^ O and w i t h s p
(Ca2+) (molal) 0.01 0.01 0.01
Table I Seeded r u n s a t s e v e r a l i n i t i a l s u p e r s a t u r a t i o n s C a l c i t e added (Mg' ) Na C0 (g/kq-SW) (molal) (m moles/kg-SW) O.ul 0.§2 1.1 0.01 2.3 0.82 3.5 0.01 U.82 +
2
3
a
d
d
e
d
pH
f
7779 7.83 7.90
In Thermodynamics of Aqueous Systems with Industrial Applications; Newman, S., et al.; ACS Symposium Series; American Chemical Society: Washington, DC, 1980.
THERMODYNAMICS
646
OF
AQUEOUS
SYSTEMS
WITH
INDUSTRIAL
APPLICATIONS
one s o l i d , one l i q u i d , and one v a p o r phase has f = 3 , f = 4 , and c« = 2 . T h i s a g r e e s w i t h what e q u a t i o n s (1) t h r o u g h (11) t e l l u s . The v a r i a b l e s t o be f i x e d may b e , f o r e x a m p l e , and χ = XçaC0 T h i s t e l l s us t h a t , f o r e a c h s o l i d c o m p o s i t i o n , t h e r e i s o n l y one e q u i l i b r i u m aqueous s o l u t i o n o f a g i v e n c o m p o s i t i o n y = [Ca ]/{[Ca ] + [Mg ]}. T h i s i s shown i n F i g . 1 by X Y and f2 f2« i is i n i t i a l s u p e r s a t u r a t e d s o l u t i o n w h i l e X ^ and X f 2 a r e t h e aqueous s o l u t i o n s i n e q u i l i b r i u m w i t h t h e s o l i d s Y f | and Y f 2 - We s h a l l see n e x t why t h e i n i t i a l aqueous c o m p o s i t i o n Χ · i s shown t o y i e l d two ( a c t u a l l y many) e q u i l i b r i u m s y s t e m s . C o n v e n t i o n a l t h e r m o d y n a m i c s shows t h a t f o r each X - t h e r e i s one and o n l y one b u t does n o t t e l l us a n y t h i n g a b o u t t h e r e l a t i o n s h i p between i n i t i a l s o l i d s and aqueous s o l u t i o n s and t h e f i n a l e q u i l i b r i u m s y s t e m . T h i s i s where t h e a p p r o a c h o f W o l l a s t and R e i n h a r d - D e r i e (2j), upon w h i c h I have e l a b o r a t e d somewhat, comes i n . These a u t h o r s (2) p r e s e n t e d t h e i r argument f o r d i s s o l u t i o n . In t h e c a s e o f p r e c i p i t a t i o n , w h i c h I t r e a t , i t s t a r t s w i t h m
3
2 +
x
2 +
Y
2 +
x
t
h
f l
f l
e
η
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fl
D. = Ρ + D
(12)
where ϋ · i s t h e amount o f i n i t i a l s o l u t e s and Ρ and D a r e t h e amounts o f t h e p r e c i p i t a t e and o f D«j l a t e r o n . The r a t i o s o l i d / s o l u t i o n i m p l i e s the s o l i d s u r f a c e / t o t a l s o l u t e s r a t i o . Let χ be t h e mole f r a c t i o n o f C a C 0 i n t h e s o l i d and y be m / ( m + m g). Then, f o r calcium Ί
3
C a
C a
M
y D 1
1
= xP + yD
Through the m a n i p u l a t i o n o f Eqns. y D.
(12)
D. - D
(13) and (13)
one a r r i v e s
at
T h i s i s t h e c o n d i t i o n f o r c o n s e r v a t i o n o f mass shown i n F i g . 2 . Note t h a t 1 s e t χ = X w h i l e W o l l a s t and R e i n h a r d - D e r i e u s e t h e symbol χ = X . The e q u i l i b r i u m c o n d i t i o n i s o b t a i n e d i n a . s t r a i g h t f o r w a r d manner f r o m t h e r a t i o o f * n ' = Y+CaC03 s p / caC03 CaCy3 * s i m i l a r e x p r e s s i o n f o r K^tjg). T h i s f i g u r e shows t h a t t h e e q u i l i b r i u m v a l u e s x-f, y f depend upon t h e s o l i d / w a t e r r a t i o . T h e r e i s no thermodynamic i n c o n s i s t e n c y i n t h i s b e c a u s e , i n terms o f F i g . 1 a l l t h a t F i g . 2 i m p l i e s i s t h a t Χ · f o r two s o l i d / w a t e r r a t i o s w i l l y i e l d two v a l u e s o f X^, e a c h w i t h i t s t h e r m o d y n a m i c a l l y c o r r e s p o n d i n g Y f ( s e e F i g u r e C a
M g
K
x
x
a
n
d
0T
a
K
a
η
T h u s , l a r g e r s o l i d / w a t e r r a t i o s s u c h as a r e e n c o u n t e r e d i n p o r e w a t e r s o f s e d i m e n t s l e a d t o s m a l l e r MgC0 c o n t e n t s i n t h e e q u i l i b r i u m m a g n e s i a n c a l c i t e s a l t h o u g h i n e i t h e r c a s e t h e mag nesium c o n t e n t o f t h e s o l i d i n c r e a s e s . W o l l a s t and R e i n h a r d - D e r i e p r e s e n t e d data t o s u p p o r t the t h e o r y from the s t a n d p o i n t o f d i s s o l u t i o n and some o f o u r r e s u l t s f o r t h e p r e c i p i t a t i o n c a s e 3
In Thermodynamics of Aqueous Systems with Industrial Applications; Newman, S., et al.; ACS Symposium Series; American Chemical Society: Washington, DC, 1980.
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PYTKOWICZ AND COLE
Figure 1.
647
Mixed Electrolyte Solutions
Triangular solid solution-aqueous solution equilibria
Increasing water/ solid ratio
l-x Figure 2. Equilibrium Curve A and conservation of mass Curve B. The equilibrium point D corresponds to a very large solid/water ratio and the reverse is true for E.
American Chemical Society Library 1155 16th St. N. W. In Thermodynamics of Aqueous Systems with Industrial Washington, D. C.Applications; 20036 Newman, S., et al.; ACS Symposium Series; American Chemical Society: Washington, DC, 1980.
T H E R M O D Y N A M I C S OF AQUEOUS SYSTEMS W I T H INDUSTRIAL
648
APPLICATIONS
a r e shown i n T a b l e I I . A k i n e t i c c o n t r o l would l e a d t o a f a s t e r p r e c i p i t a t i o n a n d , c o n s e q u e n t l y , t o a h i g h e r MgC0 c o n t e n t and s o l u b i l i t y f o r a l a r g e r a d d i t i o n o f c a l c i t e as more s u r f a c e f o r n u c l e a t i o n would be a v a i l a b l e . 3
Table II The e q u i l i b r i u m pH i n t h e m u l t i s t a t e e q u i l i b r i u m as a f u n c t i o n o f t h e s o l i d / w a t e r r a t i o ( C o l e and P y t k o w i c z , i n p r e p a r a t i o n ) f o r a r t i f i c i a l seawaters w i t h m o d i f i e d (Mg ). The l a s t two columns f o r c a l c i t e r e f e r t o successive additions of s o l i d . (Ca* ) l M g ^ ) N a C 0 x added C a l c i t e added S t e a d y C a l c i t e Steady ( m o l a l ) ( m o l a l ) ( m o l / k g SW) (g/kgSW) S t a t e pH added s t a t e pH 0.01 0.01 3.27 0.62 0.62 7.88 0.01 0.01 1.61 0.20 7.95 0.20 7.89 0.01 0.01 1.31 0.07 8.01 0.07 8.01
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2 +
+
+
2
We o b s e r v e t h e o p p o s i t e t r e n d , e x p e c t e d f r o m t h e m u l t i p h a s e h y p o t h e s i s as a h i g h e r s o l i d / s o l u t i o n r a t i o l e a d s t o a s m a l l e r mole f r a c t i o n o f MgCOq a n d , c o n s e q u e n t l y , t o a l o w e r s o l u b i l i t y (and pH) o f t h e s o l u t i o n . In t h e f i r s t r u n t h e h i g h N a C 0 3 added i s o f f s e t by t n e l a r g e amount o f c a l c i t e a d d e d . In t h e d i s s o l u t i o n p r o c e s s t h e magnesium c o n t e n t o f t h e s o l i d d e c r e a s e s and does so t o a g r e a t e r e x t e n t f o r s m a l l e r s o l i d / s o l u t i o n r a t i o s . For f a b l e m t h e s o l u b i l i t y p r o d u c t s o f CaC03 and M g C 0 were p l a c e d i n t h e form , 2
3
2
X
K
sp
ι
λ was c a l c u l a t e d f o r known v a l u e s o f γ and K i n s e a w a t e r and from assumed v a l u e s o f X . Then y ^ w a s ~ c a l c u l a t e d from t h e e q u i l i b r i u m e q u a t i o n and compared t o y * = 0 . 0 1 / ( 0 . 0 1 + 0 . 0 5 ) = 0 . 1 6 7 f o r seawater. I t c a n be seen t h a t t n e most s t a b l e c a l c i t e i n s e a w a t e r must c o n t a i n r o u g h l y l e s s t h a n one mole p e r c e n t MgC03« The t i m e b e h a v i o r s f o r t h e v a r i o u s t y p e s o f p r o c e s s e s a r e shown i n F i g u r e 3 . The t h r e e u p p e r c u r v e s c o r r e s p o n d t o a k i n e t i c c o n t r o l w h i l e t h e t h r e e l o w e r ones r e s u l t from thermodynamic c o n trol. I t s h o u l d be n o t e d t h a t a t i n t e r m e d i a t e r a t e s o f p r e c i p i t a t i o n t h e two t y p e s o f mechanisms may a c t a t t h e same t i m e i n t e r m s o f t h e d i f f e r e n c e between t h e i o n p r o d u c t and Κ ' . The i m p o r t a n t c o n c l u s i o n i s t h a t c o m p l e x c o n t r o l l i n g p r o c e s s e s c a n o c c u r i n s o l u b i l i t y phenomena i n m i x e d e l e c t r o l y t e solutions. T h i s i s e s p e c i a l l y t r u e o f s u r f a c e c o a t i n g s formed k i n e t i c a l l y o r by m u l t i s t a t e t h e r m o d y n a m i c s and w h i c h p r e v e n t t h e aqueous s o l u t i o n f r o m i n t e r a c t i o n w i t h i n t e r n a l b u l k p h a s e s . One s h o u l d remember o f c o u r s e t h a t , when t h e d e g r e e o f s u p e r s a t u r a t i o n i s l a r g e enough f o r b u l k p r e c i p i t a t i o n t o o c c u r , t h e k i n e t i c and m u l t i p h a s e thermodynamic p r o c e s s e s s t u d i e d above w i l l a p p l y t o the a c t u a l bulk phases. +
S £ )
In Thermodynamics of Aqueous Systems with Industrial Applications; Newman, S., et al.; ACS Symposium Series; American Chemical Society: Washington, DC, 1980.
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33.
PYTKOWICZ AND COLE
Mixed Electrolyte Solutions
649
Figure 3. Controls of precipitation (idealized curves) A, B, C result from the addition of different amounts of Na CO, . At D and Ε Ig of calcite was added per kg of seawater for Curve DEF, at D 2g were added for curve DF, and 3g for DG. 2
{
In Thermodynamics of Aqueous Systems with Industrial Applications; Newman, S., et al.; ACS Symposium Series; American Chemical Society: Washington, DC, 1980.
THERMODYNAMICS OF
650
AQUEOUS SYSTEMS W I T H INDUSTRIAL
APPLICATIONS
Table III C a l c i t e mole f r a c t i o n X , s o l i d s t a t e a c t i v i t y c o e f f i c i e n t s λ , and Y p , t h e s o l u t e m o l e f r a c t i o n s of calcium at e q u i l i b r i u m i n seawater. X
A
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0.99 0.98 0.97 0.88
CaC0
A
3
MgC0
3
166 83.0 55.3 13.8
1 .13 1.14 1.15 1.27
0.174 0.178 0.179 0.218
Ion P a i r - C o m p l e x C o m p e t i t i o n The c o n c e p t s o f i o n i c m e d i a , f r e e and t o t a l a c t i v i t y c o e f f i c i e n t s , p r o p e r t i e s o f e q u i l i b r i u m c o n s t a n t s , and e f f e c t i v e i o n i c s t r e n g t h t o be u s e d h e r e were examined i n an e a r l i e r p a p e r i n t h i s volume. T h i s s e c t i o n i s based upon t h e p a p e r s o f J o h n s o n and P y t k o w i c z {]) and o f S i p o s et_ a l _ . ( 8 ) . The c o n c e p t s used a r e t h e f o r m a t i o n o f c o u l o m b i c i o n - p a i r s between t h e m a j o r i o n s o f s e a w a t e r ( N a C i o , N a H C 0 ° , N a C 0 " , N a S O ^ , and s i m i l a r p a i r s f o r C a and M g ) and t h e f o r m a t i o n o f t r u e c o m p l e x e s s u c h as P b C l , P b C l ° , C d C l , P b O H , PbC0 , e t c . The c o e x i s t e n c e o f t h e s e two t y p e s o f e n t i t i e s i m p l i e s c o m p e t i t i o n , e . g . , f o r C T i o n s , one has NaClo and P b C l , and y i e l d s t r a c e m e t a l s p e c i a t i o n q u i t e d i f f e r e n t from those o b t a i n e d i n the absence o f i o n p a i r s . In T a b l e IV a r e shown t h e f r a c t i o n s o f t h e m a j o r i o n s w h i c h a r e f r e e and i o n paired. 3
2 +
3
2 +
2
+
+
+
3
+
Table
Na K+ Mg Ca2+ etc. +
2 +
IV
% Free
M-Cl
M-SO4
84.0 78.5 50.9 45.8
T2T2 17.2 39.1 43.8
3.8 4.3 9.7 10.0
a =
YT(T)
100% change i n C 0 (ïC0 )T 3
= (YC0 )F/n
3
+
sp" K* = K * ( t ) K
=
K
K
F
3
M-C0
3
0.0 0.0 0.0 0.1
Y (F) F
NaC0
sp/(YCa)T ( ) ( Y C a
0.0 0.0 0.2 0.3
-»• 1% change i n
2 _
3
-
M-HC0
Y C 0 3
(18
)
(d")p
and
2
(M
2 +
)
F
(Cl')p
where ( c j i n d i c a t e s t h e c o r r e c t e d v a l u e s . T h i s was done a t t h e e f f e c t i v e i o n i c s t r e n g t h o f t h e s e a w a t e r o f i n t e r e s t w h i c h was roughly 0.7. U n c o r r e c t e d and c o r r e c t e d r e s u l t s f o r t h e t r a c e m e t a l s p e c i a t i o n o f l e a d a r e p r e s e n t e d i n T a b l e V . I t c a n be seen t h a t t h e c o m p e t i t i o n between t r u e c o m p l e x e s and c o u l o m b i c i o n - p a i r s m o d i f i e s c o n s i d e r a b l y the s p e c i a t i o n o f l e a d . The f r a c t i o n s do n o t add up t o 100% b e c a u s e s p e c i e s s u c h a s P b C l ° , P b c l " , e t c . , were n o t e n t e r e d i n t o t h e t a b l e . A g l o s s a r y o f s y m b o l s c a n be f o u n d i n T a b l e V I . 2
3
Table V Lead s p e c i a t i o n i n s e a w a t e r c o r r e c t e d a n d uncorrected f o r C I " i o n - p a i r s . Corrected Uncorrected [Pb2+] 0.57% 1.94% 1.57% [HbCl*] 4.48% [PbOH ] 35.89% 61.55% [PbC0 °] ϋ2.53% 44.33% +
3
In Thermodynamics of Aqueous Systems with Industrial Applications; Newman, S., et al.; ACS Symposium Series; American Chemical Society: Washington, DC, 1980.
THERMODYNAMICS OF AQUEOUS SYSTEMS WITH INDUSTRIAL APPLICATIONS
652
T a b l e VI Symbols. number o f components amount o f s o l u t e d u r i n g t h e c o u r s e o f an e x p e r i m e n t amount o f i n i t i a l s o l u t e s number o f d e g r e e s o f f r e e d o m s t o i c h i o m e t r i c s o l u b i l i t y p r o d u c t o f CaC03
c D D-j f sp K
K^Mg) m [Na ]p [Na ]j Ρ +
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+
ρ pC0 pH Τ X χ y f
2
s t o i c h i o m e t r i c s o l u b i l i t y p r o d u c t o f MgCU3 molality free ion concentration of Na total concentration of Na amount o f s o l i d d u r i n g t h e c o u r s e o f an e x p e r i m e n t ; a l s o the pressure number o f p h a s e s p a r t i a l pressure o f C0 f i n a l pH temperature mole f r a c t i o n m o l e f r a c t i o n o f component s u c h a s CaCU3 i n t h e s o l i d s o l u t e m o l e f r a c t i o n o f t h e e l e m e n t i n t h e aqueous solution mean m o l a l a c t i v i t y c o e f f i c i e n t +
+
2
Literature Cited
1. Plummer, N.L.; Mackenzie, F.T., Am. J. Sci., 274, 61-83, 1974. 2. Wollast, R.; Reinhard-Derie, D., "The Fate of Fossil Fuel CO in the Ocean", Ν. Andersen and A. Malahoff, eds., pp. 479493, Plenum, New York, 1977. 3. Kitano, Y.; Hood, U.W., J. Oceanogr. Soc. Japan, 18, 141-145, 1962. 4. Möl1er, P.; Rajagopalan, G., Z. Phys. Chem., Neve Holge, 94, 297-314, 1975. 5. Chave, K.E.; Deffeyes, K.S.; Weyl, P.K.; Garrels, R.M.; Thompson, M.E., Science, 137, 33-34, 1962. 6. Berner, R.A., "Principles of Chemical Sedimentology", Mc-Graw Hill, New Jersey, 1971. 7. Johnson, K.; Pytkowicz, R.M., Am. J. Sci., 278, 1428-1447, 1978. 8. Sipos, L.; Raspos, B.; Nurnberg, H:W.; Pytkowicz, R.M., Mar. Chem., In press.
2
RECEIVED
February 14, 1980.
In Thermodynamics of Aqueous Systems with Industrial Applications; Newman, S., et al.; ACS Symposium Series; American Chemical Society: Washington, DC, 1980.