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1.0
Piston
flow
0.8
0.6
P = 1
2
5
10
50
0.4
0.2
0 0
1
2
3
V/V o
FIGURE 3.10
Relative concentration ( C / C o ) versus pore volume ( V / V o ) based on the Lindstrom et al. solution
for R = 1 and P = 1. (From Selim and Amacher, 1997. With permission.)
number P are shown in Figure 3.10. As P decreases, the extent of spreading
increases due to increased apparent dispersion coefficient D or decrease in
v . Moreover, as P → ∞ ( D → 0 or v → ∞) the breakthrough resembles that for
a step function at one pore volume ( V / V o = 1) and represents the condition of
piston-type flow or convection only.
3.8 Other Exact Solutions
In addition to the exact solutions presented above for the CDE, several other
exact solutions are also available. Specifically, a number of solutions are
available for the CDE having the form:
C
t
2
C
z
−−
C
z
R
=D
v
aC
a
(3.56)
1
2
2
which includes a linear (reversible) retention term as described by the retar-
dation factor R (of Equation 3.25). In addition, Equation 3.40 includes a first-
order irreversible reaction term, with a 1 the associated rate coefficient (h -1 ).
In addition, it also includes a zero-order sink source/source term having a
constant rate of loss a 2 (or gain for negative a 2 ). Subject to different sets of
boundary conditions (Equations 3.26 to 3.32) for soil columns of finite or semi-
infinite lengths, a number of exact solutions to Equation 3.40 are available
in the literature (Carslaw and Jaeger, 1959; Ozisik, 1968; Selim and Mansell,
1976; van Genuchten and Alves 1982). However, most retention mechanisms
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