The rate at which clams grow is dependent on the environmental variables the clam experiences (Appendix A.4.1). In the model, clams spawn at fixed times provided they are larger than a minimum size threshold. Thus, overall clam recruitment is indirectly dependent on the environmental variables. The particular criteria used included the daily rate of clam growth; time to reach sexual maturity; average clam density in the estuary; average clam biomass and the spatial variation in clam biomass.
Simulations indicated that 20 years was an adequate burn-in time for
clams and background prey
(Fig. B4). Distinct annual
cycles were present even without predation. Clam growth rates agreed
with those reported by Nichols and Thompson (1982) and are generally
0.002 (g/day) over the first 2 years following recruitment
(Fig. B5) and showed no difference with
depth. Further, model clams lost mass during winter, agreeing with Honkoop and Beukema (1997). Clams spawned at the beginning of May
reached sexual maturity (a size
cm) anywhere from November to
the following March while clams spawned at the beginning of September
reached maturity between February and March of the next year. This is
in agreement with studies done in Chesapeake
Bay (Holland et al. 1987, Fig 7).
There was no difference in the model's spring and fall recruitment
densities. For the model, average clam density without predation was
1000 clams/m
. Given the differences in the mesh-sizes of screens
used to filter sediments for clams, comparing this density to
empirical findings is difficult. Under predation, Seitz et al. (2003b) reported densities up to 500 per m
using a
1 mm mesh, while in upper Chesapeake bay, recruitment densities of
mm clams at particular sampling times were as high as 30,000 per
m
in the absence of predation and 6500 per m
with
predation (Holland et al. 1980).
In the model average clam biomass was
750 (g/m
) and
average background biomass was 240 (g/m
). In Chesapeake Bay under
predation, total biomass in mud and sand habitats was 119 and 177 (g
dry/m
) or
720 and 1100 (g wet/m
) with clams
accounting for at least 76% of the total
biomass (Hines and Comtois 1985) (i.e., clams
547 or 840 (g
wet/m
) and background biomass
173 and 254 (g
wet/m
)). The highest clam biomass density in the model occurred at
depths between 1 and 4 m, with clam biomass decreasing rapidly for
depths less than 1 m or greater than 4 m. The lower biomass in the
deeper parts of the estuary is caused by clam die-off due to hypoxia
and not limitations in recruitment since maximum clam density in the
model occurred in the deepest parts of the estuary. The movies
indicate that clam and background biomass decreased towards the mouth
of the estuary where hypoxia was generally more severe.