Much of this information has been taken from:
Sellers, P. J., and Y. Mintz, Y. C. Sud, A. Dalcher, 1986:
A simple biosphere model (SiB)
for use within general circulation models.
Journal of the Atmospheric Sciences, 43, 505-531.
Prior attempts to link these two groups took the form of meteorologists using fixed vegetation conditions and plant physiologists using fixed climate conditions.
Former modeling strategies:
Surface water balance: bucket method.
Surface energy balance: prescribed albedos and roughness.
SiB allows for plant atmosphere interactions
a) Atmospheric boundary conditions for SiB
* variables represent grid-averaged values
* temperature, Tr
* water-vapor pressure, er
* wind speed ur
* Visible or PAR (< 0.72 microns, direct beam) Fs,b(0)
* Visible or PAR (, 0.72 microns, diffuse) Fs,d(0)
* Near infrared (0.72 - 4.0 microns, direct beam) ) Fn,b(0)
* Near infrared (0.72 - 4.0 microns, diffuse) Fn,d(0)
* Thermal infrared (> 4.0 microns, diffuse) Ft,d(0)
Fs is absorbed for photosynthesis by the leaves, and Fn is primarily scattered. Some light arrives at the leaves, not directly from the solar beam but reflected (sometimes with multiple reflections) of other leaves or higher levels of the canopy.
GCMs or regional climate models calculate precipitation accumulated at the surface over the time step of the model ( a few minutes to a few hours).
* Trees and shrubs
* Ground cover
Roots are different for each type of vegetation
* Layer 1: upper thin layer which allows direct soil evaporation
* Layer 2: has roots of annual plants that may grow down to the bottom of this layer with
time; has tree and shrub roots at the bottom of this layer
* Layer 3: this layer collects water that percolates through
SVATs are constructed to give proper representation of the flow of mass, momentum, energy, and trace gases (e.g., water vapor, CO2) between the surface and the atmosphere. The flow of these quantities in a unit of time is called flux. The definitions of heat, mass, and momentum fluxes are given in Figure 2. The fluxes are related to measurable variables (like temperature or relative humidity) by use of a simple electrical resistance analog (Figure 3): V = I x R, where V is voltage (sometimes called the potential difference), I is electrical current, and R is resistance. The flux is analogous to the current, I = V/R. Table 2c of Figure 3 gives the method for calculating, say, the heat flux out of the plant canopy in terms of the potential difference (essentially the difference between the temperatures of the air and canopy) and the "resistance" of the atmosphere. Similar expressions are given for other heat fluxes and also the fluxes of water vapor from the plants and the soil surface.
A schematic depicting the various resistances for the atmosphere, plant canopy, ground cover plants, and soil is given in Figure 4. A detailed depiction of the plant stomates in Figure 5 shows that when the stomates open to allow carbon dioxide to flow in, they also allow water vapor to flow out. The plant thereby uses the size of the stomatal opening to regulate its uptake of CO2 and also to keep it cool by allowing water to evaporate within the stomate and escape to the atmosphere.
From these definitions, as shown in Figure 6 for the conservation of energy (equations 1 and 2) and conservation of water substance (equations 3 and 4). In a similar way, equations describing soil wetness in each of the three soil layers can be assembled from the conservation of water as shown by equations 5, 6, and 7 of Figure 7. The various classes of vegetation are given in Table 2 of Figure 8. When a SVAT is used in conjunction with a global or regional climate model, each grid cell of the climate model must have a "land-use" class given in Table 2 of Figure 8.