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Notes 1769<br />

salinity and temperature on results. Nevertheless,<br />

the clod cards proposed by Doty are easily<br />

prepared with standard ice-cube trays as molds<br />

and are suited to marine studies because they<br />

are large enough to be left out through a tide<br />

cycle without dissolving completely. It is a<br />

convenient and inexpensive method of measuring<br />

water motion in field studies. We have<br />

attempted to define the behavior of clod cards<br />

with respect to temperature and salinity and<br />

to develop calibration methods to enhance their<br />

usefulness.<br />

In his original description, Doty (197 1) recommended<br />

expressing field results as a “diffusion<br />

increase factor” (DF), defined as the<br />

ratio of weight loss of clod cards placed in the<br />

field to the weight loss of clod cards from the<br />

same batch held under specified still-water<br />

conditions in the laboratory. DF was meant to<br />

express the multiplication factor of diffusion<br />

in the field relative to diffusion in the absence<br />

of water motion. Unfortunately, his reported<br />

still-water values sometimes varied inexplicably<br />

among batches of clod cards that had<br />

been prepared and measured the same way.<br />

This variation introduced a large potential error<br />

into the calculation of DF, since this relatively<br />

small number is used as a divisor.<br />

Doty’s laboratory calibration method consisted<br />

of placing five clod cards on the bottom<br />

of a 15-cm-diameter container to which 2 liters<br />

of test solution were added. The water (motionless)<br />

was changed every day for 4 d. The<br />

initial and final dry weights of the clod cards<br />

were used in the DF calculations. Howerton<br />

and Boyd (1992) as well as Jokiel and Morrissey<br />

(1993) have demonstrated that the calibration<br />

container must have a minimum volume<br />

of 20 liters per clod card if it is to accurately<br />

represent weight loss due to diffusion in totally<br />

calm water.<br />

An additional problem is created by stratification<br />

in the calibration container, particu-<br />

larly when the clod cards are placed on the<br />

bottom. When a solid dissolves in quiescent<br />

water, material from the solid dissolves and<br />

diffuses away from the surface, producing a<br />

solution near the solid that is denser than the<br />

water itself. This solution flows downward, and<br />

the resulting flow increases the dissolution rate.<br />

However, the dense solution may “pool” on<br />

the bottom of the container, creating a layer<br />

of solution with a higher concentration of the<br />

dissolving material than in the bulk liquid. If<br />

the dissolving solid is placed on the bottom of<br />

the container, it will generate a layer of relatively<br />

concentrated liquid that will retard the<br />

dissolution rate compared to the solid in pure<br />

bulk solution.<br />

In unpublished experiments pointing the way<br />

to an improvement in methodology, Doty attached<br />

clod cards to a rotating arm in a tank<br />

of seawater and found that the dissolution rates<br />

of the cards were proportional to the rate at<br />

which they moved through the water. He called<br />

the apparatus a “water motion simulator”<br />

(WAMOSI) because it was the clod card, not<br />

the water, that was moving. The raw data tabulation<br />

of that study (Doty et al. 1986) shows<br />

that despite differences in apparent still-water<br />

dissolution rates among different batches of<br />

clod cards, their actual dissolution rates on the<br />

rotating arm were reproducible at a given velocity.<br />

Subsequently, Glenn and Doty (1992)<br />

used the rotating-arm calibration method in<br />

combination with field measurements to show<br />

that 85-98% of the variability of growth rates<br />

of eucheumatoid red seaweeds across seasons<br />

on a reef flat in Hawaii could be explained by<br />

water motion. These experiments indicated<br />

that calibrated clod cards would be valuable<br />

tools for correlating growth rates with water<br />

motion in the marine environment.<br />

Recently, Howerton and Boyd (1992) used<br />

clod cards to measure circulation patterns in<br />

aquaculture ponds, and Jokiel and Morrissey<br />

(1993) used clod cards to study water motion<br />

on coral reefs. In both studies, the investigators<br />

improved the still-water calibration method<br />

by increasing the volume of water into which<br />

the cards dissolve, and they measured rates of<br />

still-water dissolution of the cards as functions<br />

of duration of exposure, temperature, and salinity.<br />

Both studies used a rotating arm to estimate<br />

dissolution rates as a function of water<br />

velocity at a single temperature and salinity.<br />

They concluded that clod cards were valuable<br />

in measuring relative rates of water motion<br />

but, similar to earlier investigators, cited the<br />

need for equations relating card dissolution<br />

rates to fluid velocity as influenced by temperature<br />

and salinity before they could be used<br />

to measure absolute water velocities. Deriving<br />

and validating these equations was the purpose<br />

of our study.<br />

Clod cards were prepared essentially ac-

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