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UNSATURATED
FLOW IN FRACTURES WITH ANISOTROPIC VARIABLE APERTURES
CNR- National Research Council - Water Research Institute,
Via F. De Blasio 5, 70123 -
Bari, Italy
ABSTRACT
Vertical movement of water in a fracture plane
under unsaturated condition has been investigated by means of a computational
code. The relevant conceptual model is based on a 2D approximation of the
generalized Darcy law. Portion of the fracture is occupied by wetting and
non-wetting phases, respectively, according to the capillary pressure and
global accessibility criteria. The finite difference method was used in the
computational code to solve the nonlinear set of equations. An internal
iteration method was used at every time step to evaluate the nodal value of the
pressure head, in agreement with the mass-balance equation and the
characteristic functional relationships of the coefficients. The variable
apertures were calculated by means a spatial correlation matrix which can be
considered also anisotropic. The code results were tested with results known in
the literatures for isotropic correlation of fracture apertures. A fingering
effect in the pressure head distribution within the fracture plane was noted.
The application of the code to a fracture with anisotropic aperture variability
showed a reduction of the fingering due to larger values of apertures selected,
in the x direction.
Keywords: Fractured media; Unsaturated flow; Numerical model.
INTRODUCTION
Unsaturated
flow is very important to understand the vertical movement of pollutants. An
example is the estimation of the effects on deeper aquifers of potential
releases of leachate by no-controlled waste landfills. In the Apulia Region (South Italy) this
aspect received particular attention because in the carbonatic platform is
inserted a fractured aquifer interested by heavy withdrawals for drinking uses.
Obviously, the behavior of leachate infiltration derived by landfills depends
upon the medium characteristics, which govern fluid flow, fluid interactions
with the rock matrix and fracture aperture variability. Moreover, unsaturated
hydraulic conductivity is highly dependent upon the moisture content in the
system. Capillary theory of moisture retention suggests that since fractures
are region at relatively large voids, they will drain under smaller suction
head than the surrounding rock matrix. Therefore in steady unsaturated flow
through fractured media the moisture will preferentially move through the
matrix pore system. Nevertheless the existence of a low permeability
mineralized layer or coating at the interface fracture-rock matrix may
substantially reduce matrix imbibition and the water flow can be considered fracture
dominated. Fractures in the Apulia aquifer are often open and partly filled
with calcspar or terra rossa, which
is a coating material that include iron (15%) and aluminum oxides (30%), silica
(33%) and other minor compounds (Dell'Anna et al., 1985).
Pruess and
Tsang (1990) developed a conceptual and numerical model as a two-dimensional
heterogeneous porous medium to study unsaturated flow in fractures. Their
illustrative examples indicated that relative permeability depend sensitively
on the nature and range of spatial correlation between apertures. Studies of
individual fractures conducted in the field (Abelin et al., 1994; Shapiro and
Nicholas, 1989) and with numerical models (Moreno et al. 1988; Masciopinto et
al., 1999), have shown that within a fracture the aperture variability can
significantly affect the movement of water and solutes by forming preferential
channels. Kwicklis and Healy (1993) used the Pruess and Tsang (1990) approach
to study unsaturated flow in a discrete horizontal fracture network with
impermeable rock matrix. Abdel-Salam and Chrysikopoulos (1996) demonstrated in
their simulations that, for the case of no-moisture exchange with the rock
matrix, the moisture follows preferential pathways within fracture and exhibits
pronounced fingering effects. Following this latter approach, in this study a
comprehensive mathematical model describing moisture flow within a fracture
with anisotropic variable aperture is presented. Two stochastic fields based
upon exponential variogram models generated the apertures. The finite
difference method was used to evaluate the pressure head and potential field at
each time. Moreover an impermeable rock matrix has been considered in this
first step of the work.
MODEL DEVELOPMENT
The mathematical model presented
here was proposed to study vertical movement of moisture in a sub-vertical
fracture. This study has been carried out under the following hypotheses:
-
validity
of the generalized Darcy law;
-
fracture
with incompressible rock matrix;
-
variable
apertures and hydraulic fracture conductivity based upon incompressible fluid.
Under 2D approximation with
vertical axis upward and horizontal one in the direction of groundwater flow,
the components of water velocities are
(1)
where b is the nodal
fracture aperture. The mass-balance equation is given by
(2)
where the suction head is
(3)
Q takes
into account sink or source terms able to describe cross-flow due to drains and
pumping or recharge wells. The specific moisture capacity Γ=¶qw/¶y in the
equation (2) refers to the fracture water content.
Writing the equation (2) on the
computational cell we have
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(4) |
(5)
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where n and n-1 stand for
present and previously time step, respectively, while the relaxation parameter wt should
be 0
£ wt £ 1. The
superscript k and k1 denote that every time step n, the coefficients K of equation (4), as a function of nodal y values, are evaluated by using
which allows
the y and K=K(y) evaluation, at each time step, according to the
continuity equation (4) to be developed. Obviously also this relaxation
parameter should be selected as 0 £ wit £ 1 and a tolerance,
(6)
should be fixed. Particular attention is required to fix the time step
size (Masciopinto et al. 1994). Every time steps the van Genuchten retention curve was used to update the water content
and Γ=¶qw/¶y values.

Fig. 1. Suction
head at wetting front as a function of fracture aperture.

Fig. 2. Temporal distribution of pressure head
averaged across the fracture width, at 2 and 3 m downstream from the top of
column: a comparison between Abdel-Salam and Chrysikopoulos (1996) (****, ++++) and this work (solid lines).
Applying this equation in each
grid nodes of a discretized domain a system of equation can be obtained. The
system solution can be found after imposing suitable boundary and initial
conditions. In particular the boundary conditions can be imposed in form of
water content or suction head. The latter is a function of the surface tension
between air and water s and the fracture
aperture b
(7)
A simplified description of vertical water movement
in the fracture is given by Green-Ampt equation (Bear, 1972) with z'=-z,
(8)
valid for a one-dimensional water movement and
assuming the suction head at wetting front to be constant. This equation
suggests that for a surface tension equal to 0.0074 kg/m for water a 20 °C, hf can be expressed by
equation (5) as a function of fracture aperture. Figure 1 shows that in
fracture with aperture larger than 50 mm the
suction head cannot affect water movement, which can be considered dominated by
gravitational forces.
IDEALIZED FRACTURE
The
hypothetical fracture used here is 8 m long and 4 m wide. The fracture aperture
is assumed to be a stationary stochastic variable supposed correlated in
anisotropic fashion, over some distance in fracture plane. To generate aperture
distributions two exponential covariance models were used. A known aperture
generation code (Wiliams and El-Kadi, 1986) was modified for anisotropic
covariance matrix. Input parameters for aperture generation were the average
aperture, the standard deviation, the sill, the range and the nugget,
respectively in x and z direction.
The fracture
plane was discretized by using Dx=Dz=0.5 (153 nodes)
while the parameters of characteristics functional relationships for the
equation coefficients (i.e., van Genuchten equation parameters) were derived by
the work of Abdel-Salam and Chrysikopoulos (1996).
COMPUTATIONAL CODE
VALIDATION
To test the
model results the computational code was applied to a fracture plane described
by Abdel-Salam and Chrysikopoulos (1996). In order to investigate the effect of
variable aperture on unsaturated flow in fracture these authors examined a
first column 8 m x 4 m, where there is no moisture exchange with the rock
matrix. In Figure 2 are compared the temporal distribution of mean pressure
head given by model and results derived by Abdel-Salam and Chrysikopoulos
(1996). Obviously the same parameters, boundary and initial conditions were
imposed. Although the trends of temporal distribution of pressure heads can be considered
very similar, there are some differences on the local

a) b)
Fig. 3. Spatial distribution of the pressure head in
the vertical fracture after 1 day (isotropic aperture correlation): a) contour
map - b) two-dimensional snapshot.

a) b)
Fig. 4: Contour map and spatial distribution of
pressure head in the fracture after 4 days for isotropic (a) and anisotropic
(b) spatial correlation of the apertures.
values of the
pressure. These differences of pressure head are due to the larger grid size of
the domain applied in the current simulation (153 nodes instead of 328).
Also the
spatial distribution of the pressure heads in the fracture plane for
unsaturated flow after 1-day (Fig. 3) is quite similar to that obtained by the
above mentioned authors, when no moisture exchange with the rock matrix is
considered. The code results show that at low pressure heads, areas with large
apertures do not hold as much moisture as areas with small apertures. That is
areas with small aperture dominate the flow causing localized buildup of
potential suction heads. Inside of column an area with small aperture
completely surrounded by areas with large aperture might be noted. These areas
may remain at a high suction head for a long time.
ANISOTROPIC SIMULATION
To test its
capability the code was applied to unsaturated flow in a fracture with aperture
generated with an anisotropic matrix of spatial correlation. To produce
significant changes in the stochastic generation, the apertures were calculated
by means of different parameters (table 1) in x and z direction.
|
Parameter |
X |
Z |
|
Mean of aperture (Log(mm)) Standard deviation of
Log aperture Nugget Sill Spatial
correlation length (m) |
3.0 0.33 0.01 0.10 2 |
1.44 0.33 0.01 0.10 8 |
Table 1. Parameters for Lognormal distribution of
apertures.
The results of
code application show different behaviors (Fig. 4). A two-dimensional snapshot
of the pressure head in the fracture plane after 4 days of simulation time
shows that in the anisotropic case there is no significant fingering. This is
due to higher conductance in x direction and to the boundary conditions imposed
(i.e., constant pressure head at the top of column).
CONCLUSIONS
In this study
unsaturated flow in a vertical fracture plane with no sorbing rock matrix is
investigated. The fracture aperture is considered as a stochastic variable
generated by an isotropic and anisotropic covariance matrix. Also the mean of
apertures was considered variable with the direction in the fracture plane. The
resulting set of coupled nonlinear equations, with pressure head as dependent
variable, have been solved by means of finite difference methods. An internal
iteration method was used to reduce nonlinear equations. Temporal distributions
of pressure heads in the isotropic simulations were positively tested with
results of similar model applied by other authors. A good agreement of results
was noted also if a reduced discretization cell size was adopted (0.5 m x 0.5 m
instead of 0.2 m X 0.2 m). The spatial distribution of pressure head is
dominated by smaller apertures.
The code was
applied also to study the effect of anisotropic generation of fracture
apertures on unsaturated vertical movement of water in fractures. The
computational code results show a minor fingering of the isotropic case, due to
larger aperture generated in the x direction.
REFERENCES
Abelin, H., Birgerson, L., Widén, H., Agren, T., Moreno, L. e
Neretnieks, I. (1994). Channelling experiments in crystalline fractured rocks. Journal of Contaminant Hydrology. 15, pp. 129-158.
Abdel-Salam, A. and Chrysikopoulos, V. C. (1996). Unsaturated flow in a quasi
three-dimensional fractured medium with spatially variable aperture. Water Resource Research, vol. 32, no. 6,
pp. 1531-1540.
Bear,
J. (1972). Dynamics of fluids in porous
media. American Elsevier publishing Company, INC. New York, pp. 119-360.
Dell'Anna, L., Fiore, S., Laviano, R.
(1985). The mineralogical, chemical and grain-size features of some clay
deposits from terra rossa d'Otranto (Puglia, Southern Italy), Geologia Applicata e Idrogeologia, vol.
XX, 1, pp. 110-123.
Kwicklis, M. E. and Healy, R., (1993).
Numerical investigation of steady liquid water flow in a variably saturated
fracture network. Water Resource Research, vol. 29, no. 12, pp. 4091-4102.
Masciopinto, C., Passarella, G., Vurro, M.
& Castellano, L. (1994). Numerical simulation for the evaluation of the
free surface history in porous media. Comparison between two different
approaches. Advance in Engineering
Software, 21, pp. 149-157.
Masciopinto,
C. (1999). Particles' transport in a single fracture under variable flow
regimes. Advance in Engineering
Software, in press.
Moreno,
L., Tsang, Y. W., Tsang, C. F., Hale, V. and Neretnieks, I. (1988). Flow and
Tracer Transport in a Single Fracture: A Stochastic Model and Its Relation to
Some Field Observations. Water Resources
Research, 24, pp. 2033-2048.
Pruess, K. And Tsang, Y. W., (1990). On
two-phase relative permeability and capillary pressure of rough-walled rock
fractures. Water Resource Research,
vol. 26, no 9, pp. 195-1926.
Shapiro, A. M., and Nicholas, J. R. (1989). Assessing the Validity of
the Channel Model of Fracture Aperture Under Field Conditions. Water Resources Research, 25, pp. 817-828.
Williams, S. A. and El Kadi, A. I. COVAR.
(1986). A Computer Program for
Generating Two-dimensional Fields of Autocorrelated Parameters by Matrix
Decomposition. IGWMC -International groundwater modelling center, c/o tno
Institute of Applied Geoscience, Deft, Netherlands.