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are nonlinear and time dependent in nature, and analytical solutions are not
available. As a result a number of numerical models using finite-difference
or finite-element approximations have been utilized to solve nonlinear reten-
tion problems of multiple reactions and multicomponent solute transport for
one- and two-dimensional geometries.
3.9 Estimation of
D
In a number of field and laboratory miscible displacement studies, the main
purpose of a tracer application is to estimate the apparent dispersion coef-
ficient,
D
. A commonly used technique for estimating
D
is to describe tracer
breakthrough results where tritium, chloride-36, bromide, or other tracers
are used. It is common to use one of the above exact solutions or an approxi-
mate (numerical) solution of the CDE. In addition, a least-squares optimiza-
tion scheme or curve-fitting method is often used to obtain best-fit estimates
for
D
. One commonly used curve-fitting method is the maximum neighbor-
hood method of Marquardt (1963), which is based on an optimum interpola-
tion between the Taylor series method and the method of steepest descent
(Daniel and Wood, 1973) and is documented in a computer algorithm by van
Genuchten (1981).
The goodness-of-fit of tracer BTCs is usually unacceptable when
D
is the
only fitting parameter. Thus, two parameters are fitted (usually
D
along
with the retardation factor
R
) in order to improve the goodness-of-fit of
tracer BTCs (van Genuchten, 1981). Other commonly fitted parameters
include pulse duration
t
p
and the flow velocity
v
for solute retention (Jaynes,
Bowman, and Rice, 1988; Andreini and Steenhuis, 1990). However, since
v
can be measured experimentally under steady-state flow, it may not be
appropriate to fit
v
to achieve improved fit of the BTCs. The best-fit veloc-
ity
v
is often different from that measured experimentally. Estimates for
R
values for tritium and chloride-36 tracers are often close to unity for most
soils.
R
greater than unity indicates sorption or simply retardation, whereas
R
less than one may indicate ion exclusion or negative sorption. Similar val-
ues for
R
for tritium and
36
Cl were reported by Nkedi-Kizza et al. (1983),
van Genuchten and Wierenga (1986), and Selim, Schulin, and Fluhler (1987).
Table 3.1 provides estimates for
D
obtained from tracer breakthrough results
for several soils. Selected examples of measured and best-fit prediction of
tritium breakthrough results for selected cases are shown in Figures 3.11 to
3.13 for two reference clays (kaolinite and monotorillonite) and a Sharkey
clay soil material (Gaston and Selim, 1990b, 1991). Ma and Selim (1994) pro-
posed the use of an effective path length
L
e
or a tortuosity parameter τ (
L
e
/
L
)
where
L
e
was obtained based on mean residence time measurements. They
tested the validity of fitting solute transport length (
L
e
) or tortuosity (τ)
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