Soil Science Society of America Journal 63:800-806 (1999)
© 1999 Soil Science Society of America
DIVISION S-1-SOIL PHYSICS
Comparing Field Methods that Estimate MobileImmobile Model Parameters
F.X.M. Caseya,
D.B. Jaynesb,
R. Hortona and
S.D. Logsdonb
a Dep. of Agronomy, Iowa State Univ., Ames, IA 50011 USA
b USDA-ARS, National Soil Tilth Lab., 2150 Pammel Dr., Ames, IA 50011 USA
fxcasey{at}iastate.edu
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ABSTRACT
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Recent studies have used field techniques that estimate soil hydraulic and solute transport parameters. These methods utilize a tension infiltrometer to infiltrate either a single tracer or a series of tracers in order to estimate immobile water content (
im) and mass exchange coefficient (
) of the mobileimmobile solute transport model. The objective of this study was to compare two single tracer methods (basic and variance) with one multiple tracer method for estimating
im and
from data obtained on the same field soil location. Hydraulic conductivity (K(h0)) was also estimated using these methods. Research was done at five interrow sites in a ridge-tilled corn (Zea mays L.) field, and the soil was mapped as a Nicollet series (fine-loamy, mixed, superactive, mesic, Aquic Hapludoll). The values of
im and
estimated by the multiple tracer method compared well with previously measured values using the same technique on the same field. The
im values for the multiple tracer technique were larger than values derived from the basic single tracer technique. The basic single tracer technique did not take into consideration a mass exchange between
im and the mobile water domain (
m). The
values were less variable for the multiple tracer method than for the single tracer-variance method. Values of immobile water fraction (
im/
) for the multiple and basic single tracer techniques ranged from 0.30 to 0.52 and from 0.24 to 0.35, respectively. The values of
for the multiple and single tracer-variance techniques ranged from 0.06 to 0.9 d-1 and from 0.03 to 60 d-1, respectively. The volumetric water content (
) changed considerably over the course of the experiment for the estimation of
using the single tracer-variance method; thus, the assumptions of this technique were compromised. The measured values of K(h0) at the five sites ranged from 0.47 to 1.66 µm s-1. There was evidence that the basic single tracer method underestimated
im and overestimated
m, because this method considers
= 0 during the tracer application.
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INTRODUCTION
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MANY AGRICULTURAL PROBLEMS involve the reactivity and transport of dissolved chemicals in the soil. Chemicals such as fertilizer and pesticide are deliberately added to the soil but may result in significant contamination of the groundwater (Pye et al., 1983). These chemicals can be managed to maximize their effectiveness within the root zone and minimize their transport below the root zone. Chemicals often move preferentially through soil, resulting in a high risk of groundwater contamination. Preferential flow is exemplified by the early breakthrough and long tailing in laboratory column experiments and in field lysimeter experiments (Beven and Germann, 1982; Ressler et al., 1998). The mobileimmobile solute transport model (Coats and Smith, 1964), developed within the field of petroleum engineering, includes preferential flow. This model has been expanded and applied to soil columns (van Genuchten and Wierenga, 1976, 1977; van Genuchten et al., 1977). The mobileimmobile model was also applied to field-scale solute transport by Toride and Leij (1996), who used a stochastic stream tube model.
The mobileimmobile solute transport model separates
into
m and
im. The soil solution is stagnant in
im, and advection and dispersion occur in
m. For one-dimensional transport of a noninteracting, conservative solute, the mobileimmobile model can be written as follows:
 | (1) |
where Cm and Cim are the solute concentrations in the mobile and immobile domains, t is time, Dm is the dispersion coefficient for
m, x is distance, and q is Darcy flux. The two domains are connected by a diffusive transfer of chemical at the boundary of
im and
m:
 | (2) |
The diffusive mass transfer is characterized by
. The mobileimmobile model can account for more rapid solute transport because flow only occurs in a fraction of total
. It can also account for tailing because of the solute exchange between the domains (Eq. [2]).
Values of
im and
can be estimated from solute breakthrough curves in laboratory experiments. Matching the observed flux concentrations of tracers in column effluent with concentrations predicted from analytical solutions of the mobileimmobile model results in a set of best-fit solute transport parameters (Parker and van Genuchten, 1984; van Genuchten and Wagenet, 1989; Gamerdinger et al., 1990; Toride et al., 1995). Although the observed and calculated flux concentrations may match closely with this method, the estimated transport parameters may not be a unique set of values. Alternative methods for estimating parameter values are needed so that unique sets of solute transport values can be determined. There also exists a need to estimate these parameters without running extensive column breakthrough experiments. Methods that do not require effluent breakthrough curves to estimate solute transport properties are also useful in estimating these parameters in situ.
Tracer techniques have been proposed for estimating
im and
in the field. These methods give an alternative approach for the estimation of
im and
without the need for breakthrough curves or solute distribution profiles. These methods are a single tracer method (Clothier et al., 1992, 1995; Angulo-Jaramillo et al., 1996) and a multiple tracer method (Jaynes et al., 1995; Jaynes and Horton, 1998; Casey et al., 1997, 1998; Lee et al., 1996, 1997). The single and multiple tracer methods have been applied in the field and have received limited validation. The multiple tracer method was field tested by Casey et al. (1997) and further laboratory tested by Lee et al. (1996, 1997), the latter of whom used both the breakthrough curve method and the multiple tracer method to estimate
im and
in the same aggregated soil columns. In these studies a series of tracers were applied, after which the soil columns were sectioned and analyzed for resident tracer concentrations. The multiple tracer method was used with the resident tracer concentrations to estimate
im and
. Lee et al. (1996, 1997) were able to use these estimates to accurately predict solute breakthrough curves and resident concentration profiles in soil columns. The single tracer method has been field tested in several studies (Clothier et al., 1992, 1995; Angulo-Jaramillo et al., 1996) but no laboratory validation has been done.
Both the multiple and single tracer methods are simplifications of the full mobileimmobile model. There exist two separate single tracer methods: the basic single tracer method to estimate
im (Clothier et al., 1992) and the single tracer-variance method to estimate
(Clothier et al., 1995). The basic single tracer method used to estimate
im assumes that
and that there is no significant solute exchange between
m and
im
during the course of the experiment. The single tracer-variance method for estimating
does not assume
= 0 but that
can be measured over a long period of time. The multiple tracer method simultaneously estimates
and
im with the assumption that
is not negligible. Both single and multiple tracer methods assume that there is piston displacement of tracer within
m and that Cm behind the tracer front is approximated by the input tracer concentration. There are advantages with both of these methods. The basic single tracer method is simple to use when estimating
im and the analytical techniques are not complex; however, the single tracer-variance method is more involved when estimating
. Both techniques are capable of simultaneously determining soil hydraulic properties. To date there has not been a critical comparison of the two methods. The objective of this study is to compare the single and multiple tracer methods for estimating
and
im of a field soil.
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Materials and methods
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Research took place in a ridge-tilled corn field between 30 August and 14 September 1996 at the Agronomy and Agricultural and Biosystems Engineering Research Center west of Ames, IA. The soil was mapped as a Nicollet series derived from glacial till. Five infiltration sites were located in the interrow areas of adjacent corn rows. The infiltration sites were cleared of corn debris and weeds to ensure suitable hydraulic contact between the infiltrometer disk and the soil surface. Experiments to estimate soil hydraulic properties preceded experiments to estimate the solute transport coefficients
im and
.
Near each site a soil core was taken using a beveled brass ring with height 37 mm and diameter 73 mm. These soil cores were used to determine the antecedent
and bulk density. A large-base diameter (230 mm, Perroux and White, 1988) tension infiltrometer was filled with a 4-mmol L-1 solution of KCl and placed on the flat soil surface. Infiltration began at a pressure head of -30 mm and the early cumulative infiltration (I) volumes were automatically recorded every second for the first 100 s. These early I values were later used to calculate sorptivity (S). The infiltrometers were automated with transducers as described by Ankeny et al. (1988). After the first 100 s of cumulative infiltration, the automated recording interval was changed to read every 576 s for 16 h. These later I values were used to determine the steady state infiltration rates (i) according to White and Sully (1987).
To estimate S, early stages of I values were used with the following expression (Philip, 1957; White and Sully, 1987, 1988):
 | (3) |
where t is the infiltration time. Sorptivity was estimated from the slope of the measured I vs. t1/2, and coefficients of determination were determined for the regression.
To estimate K(h0), the White and Sully (1987) method was used. White and Sully (1987) derived the following expression for the matrix flux potential (
):
 | (4) |
where b is a shape factor between 1
2 and
/4, and 
is the change in
during the entire infiltration period. Taking a reasonable approximation for b of 0.55 (Smettem and Clothier, 1989) and substituting Eq. [4] into Wooding's (1968) solution for unconfined steady state infiltration from a disk results in the following expression:
 | (5) |
where R is the base radius of the infiltrometer (115 mm) and h0 is the pressure head (-30 mm).
After the 4-mmol L-1 KCl solution had reached steady state infiltration rate, a series of four benzoic acid tracer solutions was applied to each site. The tracer solutions were mixed in the same manner as described by Jaynes et al. (1995) and Casey et al. (1997, 1998). The tracers used were o-trifluoromethylbenzoate; 2,6-difluorobenzoate; pentafluorobenzoate; and 2,3,6-trifluorobenzoate. Tracer application order was randomized to minimize any error caused by nonidentical transport, recovery, and analysis. Each tracer solution was applied using a separate infiltrometer; detailed laboratory experiments have shown that infiltration rates quickly return to steady state after brief removal of a tension infiltrometer (Clothier et al., 1992). The final tracer solution was applied for approximately 1 to 2.5 h so that the tracer front was well beyond the soil sampling depth of 15 mm. Clothier et al. (1995) determined that infiltrating 25 to 30 mm of tracer was sufficient to sample soil 10 to 15 mm deep while well avoiding the tracer front. We used the same criteria as the Clothier et al. (1995) study for tracer application and sampling depth.
Within seconds after the final tracer application the infiltrometer was removed, and the soil was sampled from the area that had been beneath the tension infiltrometer. The infiltration area was sectioned into four equal parts, and eight cylindrical samples (15 mm deep and 10.6 mm diameter) were taken from one of the quarters (Fig. 1)
at the same time. The infiltration area was sectioned into four quarters so that sampling disturbance was localized to a single quarter and minimized at the other quarters. The infiltration sites were then covered with plastic and loose soil was spread over the plastic. This was done to prevent water loss by evaporation and infiltration from precipitation. During the course of the experiment there was no precipitation. Approximately 2 d after the start of the tracer application, the soil and plastic sheets were taken off the infiltration sites and eight more soil samples were taken from another quarter of the infiltration site. The soil was then covered again with the plastic and loose soil. This procedure was repeated at approximately 7 d and 15 d after the start of the tracer application. Figure 1 shows the sampling scheme. All soil samples were weighed and placed in plastic zip-lock bags and refrigerated to prevent any loss of tracer or change in
.

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Fig. 1 A diagram of the soil sampling scheme beneath the tension infiltrometer. The soil sampled immediately after the tracer application was used to estimate im and with the Jaynes et al. (1995) method, and to estimate im with the Clothier et al. (1992) method. All sampling dates were used to estimate with the Clothier et al. (1995) method. The sampling dates immediately after the final tracer application, 0, 2, 7, and 15 d, correspond to the numerals, 0, 2, 7, and 15 within the white circles, respectively
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The soil samples were taken to the laboratory for tracer extraction and
measurements. Tracer extractions of the soil samples were done in 150-mL Erlenmeyer flasks using
1:1 soil/0.0005 M CaSO4 solution. The extraction mixture was shaken for 5 min on a wrist shaker and allowed to settle for 5 min. The solution was then decanted through no. 40 filter paper and stored at 2°C until analysis. Approximately 10 mL of filtered solution was needed for tracer solution determination. The remaining decant and soil retained on the filter paper were oven dried at 105°C to compute
.
Analysis for the fluorobenzoate tracers was done on a Dionex Series 4500i ion chromatograph (Dionex, Sunnyvale, CA) as described by Bowman and Gibbens (1992). For the fluorobenzoates, a SAX column (Regis Chemical Co., Morton Grove, IL)1 was used with 230 mM KH2PO4, adjusted to a pH of 2.65 with H3PO4 and 20 mL L-1 acetonitrile as the eluting solution. The flow rate was 1 mL min-1 and the detection wavelength was set to 205 nm.
Extracted tracer concentrations from the soil sampled immediately after the tracer application were used to estimate
im and
with the modified Jaynes et al. (1995) method (Casey et al., 1997; Jaynes and Horton, 1998):
 | (6) |
where C is the measured tracer concentration from the extract, C0 is the tracer concentration from the input tracer solution, t is tracer application time, and
is the soil sampling depth. It is assumed that
when the soil is sampled. Plotting ln(1 - C/C0 ) as a function of t should result in a straight line with the intercept of [ln(
im/
) + 

m/(
imq)] and the slope -
/
im (Fig. 2)
. Since
im is in both the intercept and slope, a least squares optimization has to be done to estimate
and
im.
Extracted tracer concentrations from the soil sampled immediately after the tracer application were also used to estimate
im with the basic single tracer method (Clothier et al., 1992):
 | (7) |
Equation [7] is identical to Eq. [6] if
is zero. Extracted tracer concentrations that were used to estimate
im from Eq. [7] were of the longest applied tracer in the series. The basic single tracer method assumed
for the entire tracer experiment, so it should not have mattered which tracer we chose. However, to diminish concern that the assumption that
was not being violated, we chose to use to final tracer in the series. The longer the tracer was applied the higher the probability that
was true.
Clothier et al. (1995) proposed a single tracer-variance method to estimate
by measuring the variance of tracer concentration over time. First, Clothier et al. (1995) analytically expressed the decrease of Cm through time:
 | (8) |
and the simultaneous increase of Cim through time:
 | (9) |
where C* is the equilibrium tracer concentration when
as t approaches infinity. Finally, Clothier et al. (1995) developed the following expression to predict the normalized variance in tracer concentration under the infiltrometer through time:
 | (10) |
where
is the predicted normalized variance in the soil samples over time. The temporal decline in [Cm(t) - C*] and [Cim(t)] incline in [Cim(t) - C*] can be found using the analytical expressions of Eq. [8] and Eq. [9]. At the time the soil is first sampled it is assumed that the values of
and the value of
. Also, the values for
m and
im that were used in Eq. [8], [9], and [10] came from Eq. [7].
The variance of each of the tracer concentrations from each application site was determined at approximately 0, 2, 7, and 15 d after the tracer infiltration. The time at 0 d was the time the first tracer was applied, and the first sampling occurred at the completion of the last tracer infiltration. The following expression was used to determine the sample variance (s2) of the tracer concentrations (Steel and Torrie, 1980):
 | (11) |
where n is the number of the soil samples (n = 8), and
is the mean value of the n samples. The sample variance values from Eq. [11] were normalized by dividing through by the initial sample variance, s20, calculated from all of the tracers. This approach for estimating
assumed that the soil samples that were taken from the infiltration site were either sampled from
m or
im (Clothier et al., 1995).
All four tracers were used in estimating the measured
values. The tracers were assumed to move through the soil identically, and the tracers were applied at different times. Each tracer was used to estimate an
value. Figure 3
shows the observed
values (Eq. [11]) from all four tracers and corresponding model curves that were calculated from Eq. [10]. To calculate Eq. [10] it was necessary to calculate Cm(t) and Cim(t) values which were calculated using Eq. [8] and Eq. [9], respectively. The varying calculated
values from Eq. [10] were obtained by using various
values, which are reported in Fig. 3.
To evaluate the basic single tracer method's assumption that
0, calculations were made with the
values from Eq. [6] to estimate the amount of solute accumulation in
im during the time of the experiment. The program CXTFIT 2.0 (Toride et al., 1995) was used to calculate the accumulation of tracer in
im with time.
Values of
im/
and
from this study were compared with the Casey et al. (1997) study using a one-way ANOVA at a 0.05 significance level (Steel and Torrie, 1980, p. 64, 137167).
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Results
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Soil Hydraulic Properties
The first objective of this study was to estimate the hydraulic properties of the soil at -30 mm pressure head; these values are presented in Table 1
for the five measurement sites. The coefficients of determination for the estimation of S that used the early time infiltration data ranged from 0.77 to 0.99 with a mean of 0.87. Estimations of K(h0) from the longtime steady state infiltration data using the White and Sully (1987) method were reasonable and fell within the ranges that others have found in soils near this research area (Logsdon and Jaynes, 1996; Logsdon, 1993). Under similar tillage systems and time of the season, Logsdon and Jaynes (1996) found the mean K(h0) values at
to be 4.52 µm s-1 with a plus or minus one standard deviation range of 1.81 to 10.70 µm s-1. These values are slightly higher than the values reported in the present study. Also, Logsdon (1993) found K(h0) values in similar soils to range from 0.67 to 2.2 µm s-1, which were similar to our values (Table 1).
Soil Transport Properties
Multiple Tracer Method
Figure 2 shows the graphs of ln(1 - C/C0 ) vs. t from the first sampling, where only the mean ln(1 - C/C0) values and 95% confidence intervals of the eight samples were plotted to avoid clutter. As plotted, the slopes and intercepts of the regression from the eight soil samples at the five sites were quite similar. The estimated median values of
im from the multiple tracer method for Sites 1, 2, 3, 4, and 5 were 0.17, 0.29, 0.16, 0.19, and 0.10 m3 m-3, respectively. The variances in
im values were relatively low for all sites, ranging from 5.0 x 10-4 m6 m-6 at Site 1 to 3 x 10-3 m6 m-6 at Site 5. The corresponding
im/
values were 0.52, 0.48, 0.44, 0.44, and 0.30 for the respective Sites 1, 2, 3, 4, and 5. An ANOVA comparison with the Casey et al. (1997) study showed that
im/
values in this study were not statistically different at a 0.05 significance level. The Casey et al. (1997) study was conducted two years earlier on the same research field, using the same pressure head.
The median
values for Sites 1, 2, 3, 4, and 5 were 0.6, 0.9, 0.3, 0.7, and 0.1 d-1, respectively. The variances of
values were low, ranging from 2.5 x 10-5 d-2 at Site 5 to 0.4 d-2 at Site 2. The
values from this study were not significantly different from the Casey et al. (1997) study at a 5% level.
Single Tracer Methods
The estimates of
im that used the basic single tracer method for Sites 1, 2, 3, 4, and 5 were 0.10, 0.15, 0.10, 0.14, and 0.10 m3 m-3, respectively. The variances of
im values ranged from 1.0 x 10-4 m6 m-6 at Site 1 to 2.1 x 10-5 m6 m-6 at Site 2, which was lower than the variance values estimated by the multiple tracer method. The
im/
values estimated by the basic single tracer technique were 0.24, 0.35, 0.26, 0.33, and 0.24 for the respective Sites 1, 2, 3, 4, and 5.
Although the exact same soil samples were used, the estimates of
im and
im/
from the single tracer method were lower than the estimates from the multiple tracer method. The single tracer method assumes that the tracer enters the soil surface and moves through
m exclusively. The single tracer technique assumes that
; therefore, there is no mass exchange between
im and
m and no accumulation of tracer in
im. If
, then the concentration of the tracer should not change through time, which is contrary to the negative slopes shown for the ln(1 - C/C0) vs. t function (Fig. 2). Clothier et al. (1995) expressed concern that some of their samples did not reach final concentration due to dispersion. As a result Clothier et al. (1995) recommended that a tracer should infiltrate to depths of 25 to 30 mm for soil samples taken to the 10 to 15 mm depth. This sampling criterion was exceeded in this study. Since the Clothier et al. (1995) sampling recommendation was exceeded, it is less likely the tracer concentrations changed with time because of dispersion rather than as a consequence of
. The Clothier et al. (1995) recommendation is supported by several studies showing that dispersion approaches zero close to the solute application source at the soil surface (Yates, 1992; Gimmi, 1994). Our soil samples were taken at a shallow depth so that the effect of dispersion approached zero. A likely explanation of the increase in tracer concentration through time in Fig. 2 [i.e., decrease of ln(1 - C/C0) vs. t] was diffusion of tracer into
im.
Assuming
does not appear realistic. For instance, using
of 0.5 d-1, as estimated by Clothier et al. (1995), a measurable diffusion of solute into
im occurs within a few hours (Jaynes and Horton, 1998). Ignoring this diffusion with the basic single tracer method leads to an underestimation of
im/
. As a demostration, Cim was calculated using CXTFIT 2.0 (Toride et al., 1995) with
values from the multiple tracer method (Eq. [6]). Figure 4
shows the relative Cim as a function of time and indicates appreciable accumulation of tracer in
im at the time of the first soil sampling. This gives further evidence for the underestimation of
im with the basic single tracer method.

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Fig. 4 The calculated relative tracer concentration in the immobile domain as a function of time. Relative immobile tracer concentrations were calculated using CXTFIT 2.0 (Toride et al., 1995), and values were obtained from the multiple tracer method
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The normalized variance calculated from the measured tracer concentrations with time did not fit the single tracer model (Eq. [10]) very well (Fig. 3). For each of the sampling dates a separate
value can be estimated using this method, so there was not a single
value that characterized the decrease in
with time for any of the sites. Also, at any one site the estimated
values ranged from two to three orders of magnitude. The range of
values for all the sites was 0.03 to 60 d-1.
The calculated
values did not decrease with time as the assumptions of this method predict. Furthermore, the spread of
values between the tracers at each sampling date did not diminish with time (Fig. 3). Values of
even went above one for Site 2 on the second day of sampling and again at Sites 4 and 5 on the last day of sampling. The
values that were >1 were excluded when we created Fig. 3.
The single tracer-variance method requires constant
throughout the course of the experiment to estimate
(Clothier et al., 1995). Although the infiltration areas were covered by plastic and loose soil between each of the sampling periods,
values decreased either from lateral distribution, drainage, condensation on the plastic, or transpiration during the experiment (Fig. 5) . An increase in tracer concentration over time at some of the sites was measured and was consistent with the occurrence of transpiration. Corn plants may have drawn soil water from the experimental volume and concentrated the tracer. The large decrease in
during the 15-d period compromised the single tracer-variance method and probably added variability in the tracer concentration with time. During the first two sampling dates the mean
values changed the least: 20%; but there still was no consistent decrease in
values within the first 2 d. We speculate that the variation in
for the first two sampling dates was caused by the wetting properties of the soil as affected by the interface with the infiltrometer base, not by the exchange of tracer between
m and
im. Clothier et al. (1995) showed the same disagreement between the single tracer-variance model and their measured
values but attributed the disagreement to advective transport. As a rule, the multiple tracer method fit the C data better than the single tracer-variance method.
An additional coinsideration is that the single tracer-variance method assumes that soil samples taken from the infiltration site are either sampled from
m or
im (Clothier et al., 1995). This macroscopic interpretation of
m and
im is a fundamental difference between the single and multiple tracer methods. The multiple tracer method assumes that the domains of solute transport are on a small scale and not found in large pockets of the soil. The single tracer method assumes that the solute transport domains are on a large scale and can be sampled individually.
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Conclusion
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Two single tracer (basic and variance) methods and a multiple tracer method have been proposed for the estimation of the mobileimmobile model transport parameters
and
im, but they have not been used on the same site. By using these methods at one site, we estimated the hydraulic parameters along with the solute transport parameters. The multiple tracer method consistently gave
im values that were larger than those given by the basic single tracer method, and we attributed this result to an invalid assumption of
used in the basic single tracer method. The single tracer-variance method for estimating
was less practical than the multiple tracer method because it took a long time and was less consistent with the measured data. The single tracer-variance method gave biased estimates of
because of decreasing soil water during the test period.
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ACKNOWLEDGMENTS
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This material is based upon work supported by the CSREES-USDA under agreement 94-37102-01906.
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NOTES
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Journal Paper J-17829 of the Iowa Agriculture and Home Economics Exp. Stn., Ames, IA, Project no. 3287, with support by Hatch Act and state of Iowa funds.
1 Names are necessary to report factually on available data; however, the USDA neither guarantees nor warrants the standard of the product, and the use of the name by USDA implies no approval of the product to the exclusion of others that may be suitable. 
Received for publication May 8, 1998.
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J.L. Heitman, A. Gaur, R. Horton, D. B. Jaynes, and T. C. Kaspar
Field Measurement of Soil Surface Chemical Transport Properties for Comparison of Management Zones
Soil Sci. Soc. Am. J.,
March 12, 2007;
71(2):
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[Abstract]
[Full Text]
[PDF]
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