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1772<br />

Notes<br />

J<br />

1.0<br />

2<br />

E 0.9<br />

L<br />

2 0.6<br />

P<br />

< 0.7<br />

t 0.6<br />

0.010<br />

1 10 100<br />

Velocity, cm s-1<br />

Fig. 3. Plot ofclod card weight loss vs. velocity through<br />

32o/oo seawater for data from Glenn and Doty (1992) used<br />

in the form of Eq. 3 (their data extend to higher velocities<br />

than our work). The slope of the regression line is<br />

0.838kO.042.<br />

0.5<br />

0.4 r I<br />

0 5 10 15 20 25 30<br />

Temperature, "C<br />

Fig. 4. Correction factor for clod card data with T,, =<br />

298°K and pref = viscosity of pure water at 25°C. The four<br />

lines correspond to salinities of 0, 10, 20, and 40%~ from<br />

top to bottom. Calculated with viscosity data from Riley<br />

and Skit-row (1975).<br />

(e.g., Cussler 1984; Sherwood et al. 1975; Skelland<br />

1974). For solids of sample geometries<br />

which dissolve uniformly, the area and weight<br />

relationship can be approximated as<br />

A (2)<br />

Ai and Wi represent the initial area (exposed)<br />

and weight of the solid. For clod cards, this<br />

approximation is useful until > 50% of the clod<br />

has dissolved or longer, depending on the velocity<br />

of the fluid.<br />

The mass transfer coefficient is also influenced<br />

by the change in clod dimensions; however,<br />

the effect is usually minor until well into<br />

the dissolution process. Equations 1 and 2 can<br />

be combined and integrated to give<br />

1 - (?r = ;k($A,. (3)<br />

Wr is the final weight of the clod after time 8<br />

has elapsed. Equations 3 is useful for data analysis;<br />

the mass transfer coefficient usually varies<br />

with the fluid velocity raised to a power (P),<br />

so a log-log plot of [l - (WJ/ Wi)“] against<br />

velocity should yield a straight line. This is<br />

illustrated in Fig. 3 with the data of Glenn and<br />

Doty (1992). Equation 3 can be rearranged to<br />

give an expression for the overall fraction of<br />

weight 10~s (A W/ Wi):<br />

Assuming that AC remained constant during<br />

dissolution, experimental data at a given temperature<br />

and salinity were correlated with the<br />

model<br />

( )<br />

l/3<br />

Wf = aVm.<br />

I- j7<br />

I<br />

The constants a and m can be determined experimentally<br />

by means of the rotating arm, and<br />

weight loss data from clod cards exposed in<br />

the field can then be used in Eq. 5 to determine<br />

water motion.<br />

The effect of temperature at a given salinity<br />

and CaSO, concentration was corrected by using<br />

the group (T/T,,) (p,.,&) to normalize data<br />

to a reference temperature, where Tis absolute<br />

temperature, and p is viscosity. This group (Fig.<br />

4) is typically used to estimate the changes in<br />

diffusion coefficients (Reid and Sherwood<br />

1966) with varying solution strength.<br />

From Eq. 1 and 3, the dissolution rates are<br />

also dependent on the concentration of CaSO,<br />

in the bulk water and factors influencing the<br />

concentration, such as the ionic strength of the<br />

bulk water. To determine the concentration<br />

difference, we assume the solution at the gypsum-water<br />

interface is saturated with CaSO,<br />

and determine AC with the solubility product<br />

as<br />

Ksp = [Ca2+]i[S042-]i<br />

g= 1 - 11 - ;k($)ACO13. (4)<br />

or<br />

= ([Ca’+], + AC)([S042-]b + AC) (6)

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