Mechanistic
surface water quality models have been developed by scientists and engineers as
mathematical descriptions of hydrologic and ecologic processes. Mechanistic
modelers have tended to concentrate on the mathematical expression of theory,
probably as a consequence of: (1) scientific interest and challenge, (2) a
belief that the theory was reasonably well-understood and that this
understanding could be expressed mathematically, (3) limited available data to
fit and evaluate models, and (4) limited resources to collect additional data.
For these reasons, model coefficients and reaction rates in mechanistic models
generally are intended to characterize actual processes and are not (prior to
model “tuning”) intended to be empirically-fitted constants (which might be
considered an “effective” value for a model parameter).
Since
the parameters of mechanistic models are intended to describe real processes,
it may be assumed that an experimental study of a particular process can yield
a parameter estimate that can be directly inserted into the model. In some
cases, it is acknowledged that a reaction rate or coefficient in a model is affected by certain
conditions in a waterbody (e.g., turbulence), and thus
adjustments must be made to the experimentally-based value. However, if the
model truly is a complete mechanistic description of the system of interest,
then adjustment should be unnecessary; this is the underlying belief of modelers
who advocate development of “physically-based” models.
However,
given the relative simplicity of all simulation models in comparison to the
complexity of nature, it seems reasonable to question the legitimacy of any
"mechanistic" mathematical description of surface water quality.
Further, given data limitations and scientific knowledge limitations, it seems
reasonable to question even the goal to strive for a model that need not be
calibrated. The correctness of model structure, the knowledge of the model
user, and the availability of experimental and observational evidence all
influence parameter choice for mechanistic models. Unfortunately, too often
knowledge and data are extremely limited, making choice of parameters and
choice of important model processes guesswork to a distressingly large degree.
The example presented below is
not re-assuring with respect to these two issues: (1) scientific support for
the selection of model parameters, and (2) scientific support for the
specification of appropriate model functional relationships.
One
of the basic functions in an aquatic ecosystem model is phytoplankton settling.
An early example of its use is in the model proposed by Chen and Orlob (1972):
where:
V = segment volume (m3)
C1 = phytoplankton concentration (g/m3)
Q = flow volume (m3/t)
E = diffusion coefficient (m2/t)
A = segment surface/bottom area (m2)
µ1 = phytoplankton growth rate (t-1)
R1 = phytoplankton respiration rate (t-1)
s1 = phytoplankton settling rate (t-1)
M1 = phytoplankton mortality rate (t-1)
µ2 = zooplankton growth rate (t-1)
C2 = zooplankton concentration (g/m3)
F2,1 = fractional feeding preference
Other
examples are quite similar; a common alternative approach is that phytoplankton
settling is sometimes treated as a velocity term with an areal loss:
phytoplankton settling (mass/time) = v1AC1
To
understand some of the problems with the current approach for parameter
determination in mechanistic surface water quality models, it is useful to
examine this process further. For that purpose, "phytoplankton settling
velocity" provides a good example. Phytoplankton, or algae, are important
in aquatic ecosystems, and thus one or more phytoplankton compartments are
found in most mechanistic surface water quality models concerned with nutrient
enrichment. Phytoplankton settling is one of the key mechanisms for removal of
phytoplankton from the water column.
Stoke's
law provides the starting point for the mathematical characterization of
phytoplankton settling. Few models, however, employ Stoke's law; instead a
simple constant settling velocity (in units of length/time) expression is
commonly used. To apply a model with this settling velocity term, a modeler
must either measure phytoplankton settling directly, or select a representative
value from another study. Since field measurement of phytoplankton settling is
a difficult task, use of literature-tabulated values is standard practice.
Probably
the most thorough listing of suggested values for phytoplankton
settling velocity continues to be Bowie et al. (1985),
which presents a thorough table of reported values, by algal type (see the
table below). Bowie et al. note that under quiescent
conditions in the laboratory, phytoplankton settling is a function of algal
cell radius, shape, density, and special cell features such as gas vacuoles and
gelatinous sheaths. For natural water bodies, water turbulence can be quite
important. In two- or three-dimensional models with hydrodynamic simulation,
turbulence is accounted for in the model equations; in zero- or one-dimensional
models, the effect of turbulence on phytoplankton settling must usually be
incorporated into the choice of settling velocity.
That
information is typically the extent of technical guidance considered by
modelers when selecting this parameter using a reference like the table
from Bowie et al. The range of options in the table
is substantial, even within a single category (e.g., diatoms) for algal type.
The algal cell size, shape, and other features mentioned in the previous
paragraph can vary from species to species within a single type category, so
this may be responsible for some of the variability in the table.
However, even if the modeler who must choose a point estimate has data that
identify dominant species in a water body at a particular time and location,
dominance is apt to change with time and location. Further, models contain at
most only a few distinct phytoplankton compartments, so a choice must still be
made concerning species to be modeled and their characteristics.
Examination
of the original references from which the table
was created does little to enlighten the parameter selection process. Most
of the references summarized in
the table do not present observational studies of
phytoplankton; rather, they are simulation model studies, and the value for
phytoplankton settling velocity listed in the table
is the value chosen for the model. In some of the references checked, little or
no basis was provided for the choice. When a rationale for choice was given, it
was usually to adopt or adjust the few values presented in the literature from
experimental studies, or to adopt a value from another modeling study. In one
way or another, it appears that virtually all of the values presented in the table
have some dependency on the early experimental work of Smayda and Boleyn (1965)
and other work by Smayda.
Unfortunately,
evaluation studies of simulation models have provided little insight on good
point estimates for this parameter. Observational data on surface water quality
are almost always inadequate for testing functional relationships and assessing
parameter choices. Typical observational data sets are noisy, with few
measurements of each of only a few variables. In the case of phytoplankton
settling velocity, observational data are apt to consist of phytoplankton cell
densities at various dates, times, and areal locations, but probably not depths.
Since phytoplankton are also removed from the water column
through consumption by higher food chain organisms, the observational data do
not permit separate identification of the removal mechanisms.
Given
this situation, modelers have relied almost exclusively on the few experimental
studies in the laboratory and their judgment concerning adjustments to these
values. For one-dimensional models without explicit modeling of hydrodynamics,
the chosen value may be as much as an order of magnitude higher than the
laboratory values. Two- or three-dimensional models with hydrodynamics may
incorporate the unadjusted laboratory value. After early modeling studies
presented chosen values, these values were sometimes adopted in subsequent
studies without comment (in effect, "default" values were
identified). Thus, there is probably much less information in the columns of the table
than implied by the number of values reported.
In
summary, the choices for phytoplankton settling velocity appear to be based on
ad hoc adjustments to a few values measured under controlled conditions. There
is virtually no field confirmation of choices made for parameters individually
(as opposed to collectively). This situation is fairly typical of the
state-of-the-art in mechanistic surface water
quality simulation modeling.
Bowie,
G.L., Mills, W.B., Porcella, D.B., Campbell, C.L., Pagenkopf, J.R., Rupp, G.L.,
Johnson, K.M., Chan, P.W.H., Gherini, S.A., and Chamberlin, C.E., 1985. Rates,
Constants, and Kinetics Formulations in Surface Water Quality Modeling. U.S.
Environmental Protection Agency, EPA/600/3-85/040.
Chen,
C.W and Orlob, G.T., 1972. Ecologic Simulation for Aquatic Environments. Office
of Water Resources Research, US Dept. of Interior. Washington, DC.
Smayda,
T.I. and Boleyn, B.J., 1965. Experimental observations on the floatation of
marine diatoms. Part I: Thalassiosira naria, T.
rotula and Nitzschia seriata. Limnol.
and Oceanogr., 10:499-510.