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Solubility of chlorargyrite (AgCl) in water vapor at elevated ...

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3822 A. A. Migdisov, A. E. Williams-Jones, and O. M. Suleimenov<br />

Fig. 5. Published experimental measurements and predicted values<br />

<strong>of</strong> P <strong>AgCl</strong> gas over <strong>chlorargyrite</strong>. The diagram omits some high temper<strong>at</strong>ure<br />

d<strong>at</strong>a (1150 to 1700 K), which appear <strong>in</strong> public<strong>at</strong>ions between<br />

1920 and 1952.<br />

logX <strong>AgCl</strong> H2O n<br />

n 1 logf H2O logK 4 (7)<br />

logX <strong>AgCl</strong> H 2O n<br />

logP<br />

<br />

T<br />

n 1 (8)<br />

Fig. 4. <strong>AgCl</strong> concentr<strong>at</strong>ions <strong>in</strong> the <strong>vapor</strong> versus the pressure <strong>in</strong> the<br />

system. Due to the low partial pressure <strong>of</strong> <strong>AgCl</strong> vap. , the total pressure<br />

<strong>in</strong> the autoclave was effectively th<strong>at</strong> <strong>of</strong> the <strong>w<strong>at</strong>er</strong>. The heavy solid l<strong>in</strong>es<br />

show the silver chloride concentr<strong>at</strong>ion calcul<strong>at</strong>ed assum<strong>in</strong>g no hydr<strong>at</strong>ion<br />

<strong>of</strong> <strong>AgCl</strong>. The calcul<strong>at</strong>ions were done us<strong>in</strong>g the d<strong>at</strong>a on <strong>AgCl</strong> gas<br />

<strong>vapor</strong> pressure over crystall<strong>in</strong>e <strong>chlorargyrite</strong> reported by Tagirov et al.<br />

(1993).<br />

The hydr<strong>at</strong>ion number (n) can be determ<strong>in</strong>ed by the slope <strong>of</strong> the<br />

trend <strong>of</strong> log X <strong>AgCl</strong> (H2 O) n <strong>in</strong> <strong>w<strong>at</strong>er</strong> <strong>vapor</strong>, versus log P H2 O<br />

(Eqs. 7 and 8). This rel<strong>at</strong>ionship is illustr<strong>at</strong>ed <strong>in</strong> Fig. 7.<br />

It is evident from Fig. 7 th<strong>at</strong> the slope is 2 for the temper<strong>at</strong>ures<br />

<strong>in</strong>vestig<strong>at</strong>ed. The rel<strong>at</strong>ively constant slope for all these<br />

temper<strong>at</strong>ures confirms, to a first approxim<strong>at</strong>ion, the assumption<br />

<strong>of</strong> constant stoichiometry <strong>of</strong> the hydr<strong>at</strong>ed complex. However,<br />

those predicted by the more complic<strong>at</strong>ed Pitzer-Palaban model<br />

(Pitzer and Palaban, 1986).<br />

Assum<strong>in</strong>g, th<strong>at</strong> the fugacity <strong>of</strong> <strong>AgCl</strong> (H 2 O) n gas can be<br />

approxim<strong>at</strong>ed as:<br />

f <strong>AgCl</strong> H2On<br />

f H2O X <strong>AgCl</strong> H2O n<br />

(5)<br />

where X <strong>AgCl</strong> (H2 O)n is the mole fraction <strong>of</strong> the hydr<strong>at</strong>ed complex<br />

and f H2 O is the <strong>w<strong>at</strong>er</strong> fugacity, the equilibrium constant <strong>of</strong><br />

reaction (4) can be written as:<br />

logK 4 logX <strong>AgCl</strong> H2O n<br />

logf H2O n logf H2O <br />

logX <strong>AgCl</strong> H2On n 1 logf H2O (6)<br />

To a first, rough approxim<strong>at</strong>ion, it can be assumed th<strong>at</strong> the<br />

fugacity coefficients <strong>of</strong> the components <strong>in</strong> a <strong>vapor</strong> solution do<br />

not differ gre<strong>at</strong>ly from unity, and the total pressure <strong>in</strong> the<br />

system is equal to the pressure <strong>of</strong> <strong>w<strong>at</strong>er</strong>. The equ<strong>at</strong>ions rel<strong>at</strong><strong>in</strong>g<br />

the mole fraction <strong>of</strong> <strong>AgCl</strong> (H 2 O) n gas , partial pressure <strong>of</strong> <strong>w<strong>at</strong>er</strong><br />

and total pressure <strong>of</strong> the system can be obta<strong>in</strong>ed from Eq. 6 as<br />

follows:<br />

Fig. 6. Isobaric solubility trends obta<strong>in</strong>ed from polynomial fits <strong>of</strong> the<br />

experimental d<strong>at</strong>a. The heavy solid l<strong>in</strong>e represents liquid<strong>vapor</strong> s<strong>at</strong>ur<strong>at</strong>ion.

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