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Expor ts of par ticulate car bon from the shelf

Spatial and temporal distributions of biogenic fluxes demonstrate that POC and

PIC collected from bottom traps on the slope are derived mainly from the shelf.

The lateral fluxes of POC and PIC leaving the shelf are assumed to be effectively

intercepted by traps on the slope floor. Exports of POC and PIC from the ECS

continental shelf, which are a major goal of the KEEP study, can then be estimated

by integrating the time-weighted mean fluxes from the sea floor over the distance

of slope. Data from traps [T1(T3)-T4-T5-T6] located on a transect over the slope

are used for analyses. In doing so, we first extrapolate the POC and PIC fluxes of

deployed bottom traps (> 50m above the bottom) to expected fluxes measured from

the floor. Linear extrapolation of flux with water depth is applied for each trap

because we found linear relationships between POC(PIC) fluxes and depth in T4

and T5 traps that were deployed successfully for three depths (figure 9). Before making the integration, depth-extrapolated POC flux from each trap site is

subtracted from the vertical contribution (8-34%, see discussion in the temporal

variation) to represent more rigorously for lateral flux of POC. The same factor is

used to correct PIC flux as the mean POC/PIC ratio of all data approximates 1.0.

The integrated area (g C m-1d-1) represents the lateral flux through 1m- wide slope

extending 8 x 104 m from the shelf break to the lower slope. The integrated area

is calculated to be 2.506 x 104 and 4.536 x 104 g C m-1d-1, respectively, for POC

and PIC exports from the southern ECS continental shelf (figure 10).

In order to estimate total exports of POC and PIC from the ECS continental

shelf, the modeled export values on a basis of one meter width from southern ECS

slope are normalized to the latitudinal distance (1000 km) of the whole slope

estimated from the Cheju Island to the northern tip of Taiwan (figure 1). This estimate may introduce a large uncertainty because southern ECS canyon-slope

appears to be a major conduit of particle transport. However, to a first

approximation, total exports of POC and PIC can be estimated as followings:

POCexport = 2.506x104 g C m-1 d-1 x 106 m x 365 d yr-1 =9.15 x 1012 g C yr-1 (1)

PICexport = 4.536x104 g C m-1 d-1 x 106 m x 365 d yr-1 = 16.6 x 1012 g C yr-1 (2)

The calculated values may be regarded as upper bounds of exports from the

ECS shelf, as POC and PIC fluxes measured from the MHC are higher than those

from general slope and NMHC. The POC flux of T5 trap at 960m (water depth

1060m) is also about two times the flux (38±27 mg C m-2 d-1) found by Oguri et al.

[38] from northern ECS slope at 1030m (water depth 1080m). Nevertheless,

Chen and Wang [9] recently reported 8.3±4.2 x 1012 and 22.2±15.0 x 1012 g C yr-1,

respectively, for modern POC and PIC exports from the ECS shelf, derived from

water and nutrient budgets through a box model. Our estimates are very close to

the ranges found by Chen and Wang [9]. These comparable values indicate that

our estimated values are reasonable and the uncertainty may be smaller than

expected.

The primary productivity is spatially and temporally variable on the ECS shelf

[17, 20, 49]. Zhang [49] and Gong et al. [17] reported an average primary

productivity of 438 and 397 mg C m-2 d-1, respectively, in the ECS shelf. Liu et al.

[28] argued that 493 mg C m-2 d-1 may be reasonable for the Kuroshio-influenced

system. If the average value (443 mg C m-2 d-1) is adopted for productivity on the

ECS shelf, then the total POC produced biologically from the whole ECS shelf

would be 146 x 1012 g C yr-1, based on the shelf area of 0.9 x 1012 m2 [9]. Thus,

the estimated annual export of POC from the ECS shelf is equivalent to 6.3% of

annual primary production occurring on the shelf. This value is somewhat

between the shelf export measured from SEEP I (<10%) and from SEEP II (<1%)

areas [3, 13, 40], but very close to the value (6.4%) measured by Falkowski et al.

[14] from the combination of SEEP I&II and to the value (5.7%) developed from

nutrient budgets by Chen and Wang [9] from the ECS shelf.

Following the same method for POC export developed from sediment trap

data, the export of particulate nitrogen from the ECS shelf is 1.15 x 1012 g N yr-1.

The annual primary production on the shelf is equivalent to 25.8 x 1012 g N yr-1 if

Redfield ratio (6.6) is applied for biological production. The exported particulate

nitrogen, therefore, represents only 4.5% of total nitrogen required for sustaining

primary production on the shelf at a steady state. This export ratio is much

smaller than the f-ratios (0.17-0.51) measured on the ECS shelf [10] and 0.15

estimated by Chen and Wang [9]. A large fraction of new production appears to

be buried on the shelf. Therefore, recycled nitrogen may be more important than

allochthonous nitrogen in maintaining relatively high production on the ECS shelf.

4. CONCLUSION

The estimate of particulate carbon exports from the ECS continental shelf is

imperative for constructing carbon budgets in the continental margin of the western

boundary current system. This study illustrates particle and biogenic fluxes in the

southern ECS slope. Particulate carbon collected by sediment traps deployed on the

slope area is derived primarily from the shelf. Exports of particulate carbon from the

ECS shelf were derived from measured particulate carbon fluxes and shelf-wide

extrapolation. Despite the possible uncertainty associated with large spatial and

temporal variations in particle and biogenic fluxes, the exports of particulate organic

and inorganic carbon are estimated to be 9.15 x 1012 g C yr-1 and 16.6 x 1012 g C yr-1,

respectively. Only about 6.3% of carbon and 4.5% of nitrogen fixed biologically on

the ECS shelf are exported to the slope. The similar extent of exports obtained both

from SEEP (6.4% primary production) and KEEP (6.3% primary production) studies

may imply the similar role of continental shelves in regulating carbon cycling and

export in both western boundary current systems.

Acknowledgments. The authors would like to thank the National Science Council, Republic of China for financial support under Contract Nos. NSC

84-2611-M110-006k2, NSC 85-2611-M110-010-k2, 86-2611-M110-002k2 and NSC

88-2611-M110-006k2. The captain, crew and research assistants aboard the R/V

Ocean Researcher I and II are appreciated for technical support and sampling assistance during deployments and recoveries of sediment traps. We are also

grateful for helpful comments from Profs. K. K. Liu, C. L. Wei and S. Lin. This

research is a contribution to the KEEP study, a recognized program of the JGOFS.

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