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Raleigh R. Hood
University of Maryland Center for Environmental Science, Cambridge, Maryland
"Email" <raleigh barney hpl fred umces fred edu>
Julian P. McCreary, Jr.
International Pacific Research Center, University of Hawaii, Honolulu, Hawaii
"Email" <jay barney soest fred hawaii fred edu>
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Model description
The physical fields are obtained from the 4½-layer physical model of McCreary et al. (2000), which extends throughout the entire Indian Ocean. For our 1-D purpose, we extract the needed fields from the grid points nearest the WHOI mooring site. The model consists of 4 upper-ocean layers with velocities vi =(ui , vi), layer thicknesses hi, temperatures Ti, and salinities Si (i=1,2,3,4 is a layer index), overlying a deep inert ocean with temperature Td and salinity Sd. The layers correspond to either distinct oceanic regions or water-mass types, namely the surface mixed layer (layer 1), the diurnal thermocline (layer 2), the seasonal thermocline (layer 3), and the main thermocline (layer 4). The diurnal-thermocline layer allows the system to "remember" physical and biological variables when the mixed layer thins during the day, and thereby helps to prevent spurious vertical mixing between the mixed layer and the deeper ocean. Fluid is allowed to transfer between the layers with velocities w1, w2, and w3, and system is thermodynamically active in that Ti and Si vary horizontally in response to surface heat and buoyancy fluxes, horizontal advection, entrainment and detrainment. Finally, h1, h2, and h3 are not allowed to become thinner than minimum values h1min=10m, h2min=1m, and h3min=10m. These minima are necessary to keep the model numerically stable, solutions are not sensitive to their values provided they are sufficiently small. After an initial spin-up period of several years, the model is forced by daily-mean data from the WHOI mooring for the period from October 15, 1994, through October, 1995. These fields include wind stress, scalar wind, air temperature, specific humidity, and solar radiation Q. Diurnal forcing is included by modifying Q to have a realistic diurnal cycle. Variables The physical fields that are necessary for running a 1-D version of the McCreary et al. (2000) biological layer model are the layer thickness fields hi, the exchange velocities across the layer interfaces wi, and the surface light intensity Q. Salinity Si and temperature Ti fields are "optional," in that they are used in some, but not all, biological models. The following table provides these 1-D environmental fields for a solution to the 3-D layer model with diurnal forcing. Data is stored every half hour for the time period from October, 1994, through October, 1995.
Interpolation In order to be usable in a level model (the typical type of 1-d biological model), the environmental variables from the layer model must be interpolated onto a level grid. Our interpolation grid encompasses the depth range -400m < z < 0m with a vertical resolution of 1m. Details of the interpolation scheme are located in interpolation.pdf. The fields that are needed for a biological level model are the mixed-layer thickness h1, the vertical velocity field w(z), and Q.
Below are the program codes which can be used to obtain the physical field data on a level model interpolation grid.
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Two examples of biological models are given below: a layer model and level model. Each section provides the necessary code and data to run each of the model types.
Layer model The 1-D biological layer model is a straightforward adaption of the 3-D model described in McCreary et al. (1996). It determines nitrogen concentrations in four compartments: inorganic nitrogen N (that is, nitrate, nitrite and ammonia), phytoplankton P, zooplankton Z, and detritus D. In this model, hyperbolic saturation functions are used to describe how the autotrophic production rate is related to photosynthetically active radiation (PAR) and nutrient concentration, and how zooplankton growth rate is related to food supply. Vertical exchanges of nitrogen are specified via entrainment and detrainment from layers, background diffusion, and sinking. Details can be found in biolayermodel.pdf. The following table provides the information necessary to run the model, and to reproduce the solution shown below. It includes the model code (row 1) and the input data (row 2), as well as initial conditions for biological variables qi (row 3) and advective fields v·Ñqi for the diurnal solution (row 4)from McCreary et al. (2000). The initial conditions and advective terms are optional, but when they are used the resulting solutions are identical to the response of the 3-D model at the WHOI grid point.
The level-model formulation provided below is an offline version of 6-compartment ecosystem model described in Hood et al. (2000). It is similar to the McCreary et al. (1996) model in that it is a nitrogen-based system, includes N, P, Z and D compartments, and uses hyperbolic saturation functions to describe autotrophic growth and zooplankton grazing. However, it differs in that it includes two additional state variables, one for dissolved organic nitrogen (DON) and the diazotrophic cyanobacterium, Trichodesmium. In addition, the zooplankton compartment in this model is replaced by a "heterotroph" compartment, which is intended to represent both bacteria and microzooplankton. Vertical exchanges are specified via advection, diffusion and sinking of detritus. For details see biolevelmodel.pdf. The following table provides the information necessary to run the biological level model. It includes the model code (row 1), as well as program codes to interpolate the various fields. Note: These interpolation codes are identical to those given in the Interpolation section above. To interpolate the input data fields, download the file layercode_data.asc described in the Physical Fields-Variables section above and use it as input into the interpolation program l2l.f. Similarly, download the appropriate data files from the biological layer model section above and use the corresponding interpolation program to create data for the biological level model.
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Physical data
Biological data
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Hood, R. R., N. R. Bates, D. G. Capone, and D. B. Olson (2000) Modeling
the effect of nitrogen fixation on carbon and nitrogen fluxes at BATS.
Deep-Sea Res., 2nd Special Issue on the USJGOFS Time-Series
Stations.
In press.
Marra, J., T. D. Dickey, C. Ho, C. S. Kinkade, D. E. Sigurdson, R. A. Weller, and R. T. Barber, 1998: Variability in primary production as observed from moored sensors in the central Arabian Sea in 1995. Deep-Sea Res., 45:2253-2267. McCreary, J. P., P. K. Kundu, and R. L. Molinari, 1993: A numerical investigation of dynamics, thermodynamics and mixed-layer processes in the Indian Ocean. Prog. Oceanogr., 31: 181-244. McCreary, J. P., K. E. Kohler, R. R. Hood, and D. B. Olson, 1996: A four-component ecosystem model of biological activity in the Arabian Sea. Prog. Oceanogr., 37: 193-240. McCreary, J. P., K. E. Kohler, R. R. Hood, S. Smith, J. Kindle, A. Fischer, and R. A. Weller (2000) Influences of diurnal and interseasonal forcing on mixed-layer and biological variability in the central Arabian Sea. J. Geophys. Res.. Accepted, in revision.
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