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ORIGINAL ARTICLE
Two in one leachate plume in a karstic aquifer
Roger Gonzalez-Herrera • Rodolfo Gomez-Lopez
Received: 9 September 2011 / Accepted: 28 July 2012 / Published online: 14 August 2012
� Springer-Verlag 2012
Abstract Some sites formerly used for waste disposal
purposes, even if they are closed, continue generating
leachate that seeps into the ground and contaminates
groundwater in the area where they are located. It is
believed that the rainfall being in contact with waste
becomes a source of leachate. This fluid seeps into the
aquifer and may identify sources of pollution. A modeling
work which determined the migration times of solutes in
the karstic aquifer of Merida, Yucatan, Mexico, is pre-
sented. Both existing and generated information was ana-
lyzed; a leachate plume was identified. The methodology
used in the study is described, the application of which
allowed concluding that this plume was generated from
two sources: a waste disposal site and the oxidation
lagoons located next to it. The procedure consisted of
performing simulations considering the sources that con-
tribute to the development of the pollution plume and
forecasting their behavior. With the developed methodol-
ogy, similar cases can be analyzed to avoid locating
catchment zones of drinking water in inappropriate places
and/or develop projects to place waste disposal sites that
could affect existing catchment areas and to preserve this
resource, essential for life.
Keywords Groundwater � Leachate � Pollution �Karstic aquifer � Simulation
Introduction
The Yucatan Peninsula is geographically distinctive by its
shape and size; it is bounded by the Gulf of Mexico to the
north and west, and by the Caribbean Sea to the east
(Fig. 1).
Northern Yucatan, where Merida is located, is the best-
known part of the peninsula, because most of its human
population has been concentrated there for the past 1,000
years. During the recent period of accelerated diversifica-
tion, Merida, with a population of about 830,000 inhabit-
ants, has emerged as the major urban center for the
southeast, and as such, Yucatan’s capital has become the
focal point of the region’s industrial, commercial and
professional services (INEGI 2011).
In Merida, one of the permanent problems is the dis-
posal of domestic and industrial wastes that are carried out,
dumping the solids and injecting the liquids on and into the
ground.
A landfill was opened in November 1997; however, an
old municipal solid waste disposal site existed which
started operations in 1979. This dump site was situated
on the northern outskirts of the city of Merida (Fig. 2)
and was operated by the municipality. The site had a
long history of uncontrolled dumping and waste burning
including commercial, industrial and domestic wastes.
From 1993 to 1998, an attempt was made to place the
waste into a compacted raise with a soil cover. This
methodology reduced the risk of the waste catching fire
and also nuisance from air-borne pollution and smells.
Toxic materials were burned in another plant dedicated
exclusively to this practice; however, the resulting
ashes were sent to the old municipal solid waste disposal
site. There is also a composting plant located west of the
city.
R. Gonzalez-Herrera (&) � R. Gomez-Lopez
Facultad de Ingenierıa de la UADY,
Avenida Industrias no Contaminantes por Periferico Norte,
Tablaje Catastral, 12685 Merida, Yucatan, Mexico
e-mail: [email protected]
123
Environ Earth Sci (2013) 68:1945–1953
DOI 10.1007/s12665-012-1882-x
The Merida dump site was emplaced directly onto a
karstic, Tertiary, marine limestone of Miocene–Pliocene
age (DGGTN 1984), with a thin (\1 m; DGGTN 1985) to
non-existent soil cover. The following hydraulic data cor-
respond to the local unconfined aquifer: (1) the hydraulic
conductivity is very high due to the fissured nature of the
rock. Mendez (1993) indicates values of the order of 10-3–
10-4 ms-1, while Sanchez (1992) quotes values ranging
from 3.7 9 10-5 for calcarenites to 3.38 9 10-8 ms-1 for
recrystallized limestone; (2) both matrix and fissure
porosity are high, the former ranging between 40 and 50 %
(Sanchez 1992; Brewerton 1993); (3) the water table is
about 5 m below the ground level; (4) the hydraulic gra-
dient is low at 7.5 9 10-5 ms-1 with flow in a north-
westerly and westerly direction toward the coast; (5) most
of the recharge occurs in August and September. Rapid
bypass flow can be assumed during rainfall events and a
high percentage of rainfall is estimated to go to recharge,
i.e., 150 mma-1.
Thus, the main characteristic of the aquifer in the
Yucatan Peninsula, Mexico, is that it is shallow and
unconfined. The hydraulic conductivity is high because the
rock formation is of the karstic type, which facilitates the
infiltration of contaminants toward the water table. No
waste has been dumped in the old disposal site since April
1998 because of a landfill opening; site remediation and
definite closure is underway. However, it is considered that
the rainfall in contact with the waste becomes a source of
leachate. This fluid seeps into the aquifer allowing the
identification of the source of pollution.
To date most of the research work conducted in the
aquifer beneath the former waste disposal site has been
mainly focused on determining: (1) the amount of leachate
generated (Ku 1998); (2) the amount of hazardous sub-
stances and health risks (Casares 2002); (3) a methodology
and the feasibility of detection of a pollution plume (Perez
2006); and (4) different types of pollutants, the hydro-
chemical reactions and their concentrations (Vazquez
2007). The spreading process of contaminants has been
ignored.
This paper reports on a research work which determined
the migration times of solutes in the Yucatan karstic
aquifer with the aim of studying the transport process of
pollutant plumes identified with the chloride ion. The field
Fig. 1 Location of the study
area
Fig. 2 The Merida old waste disposal site and monitoring well
locations
1946 Environ Earth Sci (2013) 68:1945–1953
123
work was carried out in the former waste disposal site of
the city of Merida, Mexico. Data generated from 2000 to
2005 were available. The existing information was updated
with recent data to know the status of the pollution plume.
Methodology
The former city dump in Merida, Mexico, dates back from
the early 1980s and ceased operations in 1998. During the
period 1993–1998, the site was used to dispose of solid
waste. The waste was accumulated in the place applying
the area method of disposal. Using this method, cells of
waste were built in mounds on the ground surface. During
the time of operation, the dump site did not have any liner
to protect the aquifer. Garbage was deposited directly on
the rock face devoid of soil. This led to infiltration of
leachate into the aquifer and the resulting groundwater
pollution. This contamination has been identified as a
pollution plume, unprecedented in this type of water sys-
tem (Gonzalez et al. 2004).
Groundwater monitoring
When the study area was visited, it was noted that liquids
from septic tanks and those coming from washed maize
processing were discharged into the oxidation ponds,
located next to the solid waste disposal site (Fig. 2).
Sometimes, the discharges were made even on the hill of
garbage. During the rainy season (from May to November),
the oxidation ponds overflowed spilling the liquid con-
tained in them.
The boreholes used in this work were drilled for a pre-
vious research Gonzalez (2003). They are identified as S1,
S2, S3, S4, S5 and S6 and located at a distance of 10, 25,
50, 100, 300 and 500 m from the ‘‘mountain’’ of garbage,
respectively (see Fig. 2). In 2004, the following were
drilled: S1I, S2I, S3I, S4I, S5I, S6I, S1D, S2D, S3D, S4D,
S5D and S6D, to the left (I) and right (D) of each of the six
boreholes. This makes a total of 18 wells of 8 in. in
diameter and 50 m in nominal depth along the preferential
groundwater flow line determined by Gonzalez (1996).
The groundwater level was first measured in each bore-
hole. The monitoring was performed from the water table to
the total borehole depth. Groundwater sampling was carried
out in each monitoring borehole starting from the water table
where the first sample was collected. Samples were then
collected every 5 m, covering the whole freshwater aquifer. It
is worth noting that the coast is 30 km away from the study
area, thus the saline intrusion was located 50-m deep,
approximately, as depicted in Fig. 3 using electric conduc-
tivity profiles. A minimum of seven samples per borehole
were obtained beginning from the more distant to that closest
to the hill of the waste disposal site in order to avoid cross
contamination. Samples were then labeled and stored in the
laboratory to subsequently analyze for chloride. The titration
method was employed to determine chloride using silver
nitrate (APHA et al. 1998).
Water table contours
A commercial contouring program was used to represent
the geometry of the medium and hydraulic heads. Surfer V.
8 is a computer software developed by Golden Software,
Fig. 3 Electric conductivity
profiles
Environ Earth Sci (2013) 68:1945–1953 1947
123
Inc. It is a geostatistical tool that generates contours, based
on data located in a mesh, applying numerical methods.
The kriging method was used in this work because it
estimates the average cell-centered value of a rectangular
block in a mesh and generates contours that the program
handles to illustrate in its graphical interface. These cal-
culated values can be exported to a file with extension grd,
which can be imported to the groundwater model used.
Modeling
Groundwater flow modeling was carried out using MOD-
FLOW, a computer program developed for the U.S. Geo-
logical Survey in the form of a modular three-dimensional
groundwater flow model. MODFLOW is able to simulate a
wide range of flow through porous media with standard and
varieties of systems including groundwater flow and
transport of contamination (Harbaugh 2005). MODFLOW
solves the distribution of hydraulic head within the model
domain and from the results the velocity components of
flow are calculated. The formula used to predict flow is:
o
oxKxx
oh
ox
� �þ o
oyKyy
oh
oy
� �þ o
ozKzz
oh
oz
� �¼ Ss
oh
otð1Þ
where Ss is the specific storage; h is the hydraulic head; t is
the time and Kxx, Kyy and Kzz are the hydraulic conductivity
values in the principal directions x, y and z.
To simulate solute transport into groundwater, MT3DMS
was used. MT3DMS simulates advection, dispersion and
chemical reactions of contamination in groundwater. It uses
cell-by-cell data which are computed and output by MOD-
FLOW to establish the results (Zheng 2006). The governing
differential equation in three-dimensional form to model
contaminant transport is:
Dxo2C
ox2þ Dy
o2C
oy2þ Dz
o2C
oz2
� �� �vx
oC
oxþ �vy
oC
oyþ �vz
oC
oz
� �
¼ Rd
oC
ot
ð2Þ
where C is the concentration; v is the seepage velocity; Rd is
the retardation factor, whose value equals 1 for conservative
tracers; x, y and z are the coordinates, and t is the time.
The next part of the methodology was to simulate the
actual conditions in the study area over time. To do this, it
was necessary to collect information to faithfully reproduce
the natural conditions of the aquifer.
Results and discussion
Simulating the groundwater flow was not an easy task
because there were different values of hydraulic
conductivity (K) reported in the literature and each of these
values yielded its own set of water flow patterns and
speeds.
Sanchez (1999), Gonzalez et al. (2002) and Marın et al.
(2004) applied different techniques to model this complex
aquifer; they have shown that the best calibration is
achieved by modeling the aquifer system as homogeneous
and isotropic. The same assumption was considered to
simulate the hydrodynamic behavior of the aquifer in space
and time.
To define the boundaries of the model, the work of
Sanchez (1993) was very useful. The wells used in his
research were successfully identified. Taking those values
as a starting point to simulate the groundwater flow, the
hydraulic potentials were reproduced in the study area
using the Surfer program V 8 to serve as input to the model
(see Fig. 4). Equipotential lines were constant head
boundaries. The arrows shown in Fig. 4 are second type of
boundaries (lines representing no flow or contaminant
transport) in the model; they define the surficial domain to
the study. The freshwater part of the aquifer, which is
unconfined, is less than 40-m thick below Merida and
underlain by a brackish mixing zone at 45 m, which gives
way to saline groundwater at about 50-m depth (Villasuso
et al. 1989).
Once the boundary conditions were established, the
properties of the medium were defined, highlighting the
values that were used in the model. Thus, the value of
hydraulic conductivity K in the area was taken from the
work of Gonzalez et al. (2002) with a value of 96,336 m/
day, which corresponds to the maximum value reported in
the numerical model of the aquifer of Yucatan. The
porosity considered is that reported by Gonzalez (1996)
with a value of 30 % (n = 0.3). A uniform recharge of
150 mm/year was assigned (Lesser and Weidie 1988) for
the Yucatan karstic aquifer. The dispersivity of 29.75 cm
was taken from the work of Graniel et al. (2003), deter-
mined in the small town of Santa Gertrudis Copo, a place
near the study area. The specific storage Ss = 1.35 9
10-6 m-1 and the specific yield Sy = 0.25 were obtained
by Casares (2006). With these properties, groundwater flow
was simulated to obtain its general direction.
The aquifer was modeled as a homogeneous and iso-
tropic system. To determine the degree of correspondence
between simulated and field values, a sensitivity analysis
was performed after calibration as follows: the ground-
water flow obtained with the model was compared with
that originally reported by Sanchez (1993). To achieve the
above, monitoring wells used by Sanchez (1993) located in
zone 16 with UTM coordinates were positioned in the same
coordinates of the model. Equipotential contours, gener-
ated applying Surfer V. 8 software, were matched with
those obtained after simulation with Visual Modflow 3.0.
1948 Environ Earth Sci (2013) 68:1945–1953
123
The best fit was obtained when the minimum difference
values were computed between both contour maps.
When the groundwater flow model was calibrated
(Fig. 5), to adequately carry out the transport modeling
exercise, pollution plumes, identified with the chloride ion,
were simulated for the above conditions. Three scenarios
were considered as the source of pollution of the aquifer:
(1) the former waste disposal zone, because of the leachate
percolating into the aquifer; (2) only pollution from liquid
spills from the oxidation ponds; and (3) both sources, the
waste disposal zone and the spills from the oxidation
ponds, were polluting the aquifer.
The natural concentration of chloride ion in groundwater
underlying the area is 19 mg/l. It was considered as the
background concentration because it was determined in a
water sample taken in a borehole located upgradient of the
site (Casares 2002). Gonzalez (1996), Ku (1998) and
Casares (2002) report leachate chloride concentrations in
Fig. 4 Hydraulic heads in the
study area
Fig. 5 Boundaries and groundwater flow calibrated model
Environ Earth Sci (2013) 68:1945–1953 1949
123
the former waste disposal site, whose data was taken as the
initial concentration in the model. Chloride concentrations
in representative leachate samples were analyzed for three
periods: (1) during the operating time of the dump site
(Gonzalez 1996); (2) in the period of closure (Ku 1998);
and (3) a couple of years after closure (Casares 2002).
It is worth mentioning that the amount of leachate per-
colating into the aquifer varied in the source of contami-
nation and with time because of the amount of waste
present in the site. Therefore, three stages were clearly
identified in the waste disposal site: operation, closure and
abandonment. During the operation time, chloride con-
centrations were between 3,065 and 6,880 mg/l. At closure,
concentrations varied between 3,695 and 5,000 mg/l.
Therefore, a wide range of concentrations could be con-
sidered as initial input to the transport model. Given the
above, it was decided to vary the initial chloride concen-
tration in the transport model to represent field values.
The assumptions are reflected in the inputs of the model,
which illustrates the boundaries (hydraulic potentials) and
point sources. The domain is divided into 80-m intervals in
the X axis and 56-m intervals in the Y axis. A finer mesh
was built, in the section where the boreholes are located, of
16 m in the X axis and 11.3 m in the Y axis (see Fig. 6).
The vertical dimension (Z axis) was defined in 5-m inter-
vals from the water table to the bottom of the aquifer.
To illustrate the behavior of chloride, when monitoring
was carried out, plots, like the one shown in Fig. 7, were
generated with the information collected. With the help of
graphs similar to these, results were compared with those
reported by Gonzalez (2003) who located the center of
mass of the plume at a depth of 21 m below the water table.
The graphics obtained in this research were also compared
with profiles of chloride concentrations for six monitoring
wells considered in a research carried out by Vazquez
(2007), covering the period October 2000 to September
Fig. 6 Model grid. Mesh is refined in the area of interest
Chloride Concentration at a depth of 20 m
0.0050.00
100.00150.00200.00250.00300.00350.00400.00450.00500.00
1998 2000 2002 2004 2006 2008
YEARS
S1_20M
S2_20M
S3_20MS4_20M
S5_20M
S6_20M
Fig. 7 Chloride profiles in central boreholes at a depth of 20 m
1950 Environ Earth Sci (2013) 68:1945–1953
123
2005, who identified that the contaminant plume was 25 m
below the water table. Therefore, looking at the results of
these researchers, greater attention was paid to the behavior
of the plume at 15- to 25-m depth below the water table.
No significant differences were observed between
chloride concentrations, in boreholes S5 and S6, with time
from 2003 to 2007 at a depth between 15 and 25 m;
therefore, it was thought that the plume was not in the
process of attenuation or that there was an additional
source of chloride entering the aquifer. Neither of the
boreholes S3 and S4 had a significant reduction in chloride
concentration during the same time period and depth
interval. However, boreholes S1 and S2 showed a down-
ward trend in the concentration of chloride ion from 2002;
this is consistent with the ideas expressed by Gonzalez
(2003), who mentioned that the contaminant plume gen-
erated by leachate from waste accumulated, identified in
his research, was attenuating.
On analyzing all these graphs, the pattern could not be
explained when considering the original idea that there was
only one plume generated by leachates of the old waste
disposal site (Fig. 8). In other words, the high values of
chloride in boreholes S5 and S6 were not only a contri-
bution of such a plume. The resulting behavior can be
explained if an additional source of contamination is
considered.
When the chloride in excess is attributed to the oxida-
tion ponds, given that they are located near the study area
and in the model domain, and no other source of chloride is
present, the behavior of the local groundwater contamina-
tion can be reproduced (Fig. 9). The simulation (Fig. 10)
shows that the contaminant plume emanating from the old
disposal site is currently stable and their concentrations
decrease slowly. The plume generated from the oxidation
ponds will continue growing should conditions be the same
over time.
Conclusions
Carrying out model simulations of both groundwater flow
and contaminant transport, it was possible to identify the
presence of a plume generated by the oxidation ponds
located next to the old waste disposal site of Merida,
Mexico, which had not been identified in previous inves-
tigations in the karstic aquifer below the site. The model
simulations show that the contaminant plume of the old
waste disposal area is currently stable and contaminant
Fig. 8 Plume generated, assuming the old disposal site as the only source of contamination
Environ Earth Sci (2013) 68:1945–1953 1951
123
concentrations are slowly decreasing. On the other hand,
the plume generated in the zone of the oxidation ponds will
increase over time if conditions remain similar to those of
the model. The boreholes, of the monitoring network,
located far from the old waste disposal site are more
influenced by the plume emanating from the oxidation
ponds.
Acknowledgments The authors express gratitude to: the Engi-
neering School of the Autonomous University of Yucatan, Mexico,
for the provided facilities, equipment and transportation to carry out
field and laboratory work; the National Council of Science and
Technology (CONACYT) for funding the research projects from
which this work derives and the fellowship for Rodolfo Gomez to
complete his graduate studies. This work was part of his master’s
degree thesis in environmental engineering. The authors also thank
the reviewers for their invaluable comments for improving this paper.
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