Journal Pre-proof Numerical modelling and performance evaluation of multi-permeable reactive barrier system for aquifer remediation susceptible to chloride contamination Rahul Singh, Sumedha Chakma, Volker Birke PII:
S2352-801X(19)30072-4
DOI:
https://doi.org/10.1016/j.gsd.2019.100317
Reference:
GSD 100317
To appear in:
Groundwater for Sustainable Development
Received Date: 1 March 2019 Revised Date:
18 October 2019
Accepted Date: 6 December 2019
Please cite this article as: Singh, R., Chakma, S., Birke, V., Numerical modelling and performance evaluation of multi-permeable reactive barrier system for aquifer remediation susceptible to chloride contamination, Groundwater for Sustainable Development (2020), doi: https://doi.org/10.1016/ j.gsd.2019.100317. This is a PDF file of an article that has undergone enhancements after acceptance, such as the addition of a cover page and metadata, and formatting for readability, but it is not yet the definitive version of record. This version will undergo additional copyediting, typesetting and review before it is published in its final form, but we are providing this version to give early visibility of the article. Please note that, during the production process, errors may be discovered which could affect the content, and all legal disclaimers that apply to the journal pertain. © 2019 Published by Elsevier B.V.
Performance evaluation of a Multi-Permeable Reactive Barrier system for contaminant plume treatment in the subsurface originating from multiple point sources using numerical modelling Contaminant Source 1
Contaminant Source 2
Residential Area
Partially treated water
Homogeneous Aquifer Continuous PRB 3
Contaminant Plume
Continuous PRB 1
Continuous PRB 2
Ground water flow
Treated water
1
Numerical Modelling and Performance Evaluation of Multi-Permeable
2
Reactive Barrier System for Aquifer Remediation Susceptible to Chloride
3
Contamination
4 5
Rahul Singh*
6
Research Scholar, Department of Civil Engineering, Indian Institute of Technology Delhi,
7
New Delhi, India: E-mail -
[email protected]
8 9
Sumedha Chakma
10
Assistant Professor, Department of Civil Engineering, Indian Institute of Technology Delhi,
11
New Delhi, India: E-mail -
[email protected]
12 13
Volker Birke
14
Professor, Mechanical Engineering / Process Engineering and Environmental Engineering
15
Hochschule Wismar, Germany: E-mail –
[email protected]
16 17
*
18
Rahul Singh
19
E-mail -
[email protected]
20
Telephone number - +49-17677896518
Corresponding author
21
1
22
Abstract Many in-situ groundwater remediation technologies have been developed, among
23
which the permeable reactive barrier (PRB) technology has emerged as an efficient, cost-
24
effective and sustainable remediation technique for the variety of contaminants. In this paper,
25
a numerical model is developed, using Visual MODFLOW, to evaluate the performance of a
26
multi-PRB system over the temporal and spatial groundwater quality variations. Model is
27
simulated for a single contaminant, i.e. Chloride (Cl-), released from multiple point sources,
28
over a hypothetical study area for a period of five years (1800 days). Initially, the model is
29
simulated without any remediation barrier and later multiple barriers, using Activated wood
30
charcoal (AWC) as a common reactive material, are introduced consecutively to contain the
31
plume to a desirable limit. Various parameters, such as the dimensions of the barriers and
32
continuous pumping, are taken into consideration for the performance evaluation of the
33
multi-PRB system. The results indicate that the performance of the multi-PRB system is more
34
efficient compared to the single PRB and natural attenuation system as the concentration in
35
all the wells could be seen drastically declined with the installation of PRBs. Thicker PRB
36
could produce better chloride removal rate due to the increase in residence time for the
37
adsorption of chloride over the reactive media. Further, the continuous pumping would also
38
increase the rate of remediation for the observation wells in its vicinity, however, up to a
39
certain limit. Furthermore, the maximum efficiency of the multi-PRB system can be achieved
40
at a lower depth compare to full study depth. Moreover, the PRBs adjacent to the
41
contaminant source treat the contaminants in the plume capture zone with high efficiency
42
than the far away PRBs. Finally, the numerical model shows that the contaminant plume,
43
containing chloride, is efficiently captured by the multi-PRB system in the proximity of the
44
point sources.
45
Keywords
46
MODFLOW; Activated wood charcoal; Continuous Pumping.
Groundwater
remediation;
Multi-Permeable
2
Reactive
Barrier;
Visual
47
1 Introduction
48
Recent years have witnessed an increasing concern over the deterioration of groundwater
49
quality due to various geogenic and anthropogenic sources like agricultural runoff, industrial
50
exertions, activated mine drainage, domestic and municipal solid wastes, etc. (Chakraborty et
51
al., 2010; Schipper et al., 2010; Wiafe et al., 2013; Rodak et al., 2014). These sources have
52
caused the emergence of numerous toxic and fatal contaminants in the groundwater like the
53
chlorinated compounds, hydrocarbons, heavy metals, etc., which have gathered worldwide
54
attention (Thiruvenkatachari et al., 2008; Obiro-Nayarko et al., 2014). More than 400,000
55
sites in the USA have been severely contaminated with toxic metals such as chlorinated
56
compounds and radioactive materials. Similarly, over Europe and Australia, there are well-
57
documented cases of groundwater pollution due to nitrates, hydrocarbons, chlorinated
58
compounds, sulfates, phosphates, etc. (Chakraborty et al., 2010; Thiruvenkatachari et al.,
59
2008; NRC, 1994). The increasing concentration of groundwater contamination has not only
60
led it unfit for drinking but also caused an adverse effect on humans, animals, and the
61
environment. (Suhag, 2016; Thiruvenkatachari et al., 2008). These severe incidents of
62
groundwater contamination create demand for the development of an efficient groundwater
63
remediation technique to eliminate the higher risk to health and the environment (Suhag,
64
2016).
65
Many conventional groundwater remediation techniques have been developed, over the past
66
few decades, among which the pump and treat (P&T) technology has been widely adopted
67
for the active remediation of contaminated groundwater above the ground surface (Phillips
68
and Atlas, 2005). The P&T technique is simple in application, however, it has low
69
remediation efficiency and is less cost-effective due to requirements of exhaustive energy and
70
input resources (USEPA, 2002). The drawbacks of the P&T technology have ushered the
71
evolution of many other ex-situ groundwater remediation technologies like steam stripping,
72
bioremediation, etc. (Thiruvenkatachari et al., 2008, ITRC, 2011).
73
technologies are also unable to restore the contaminated groundwater sites completely or
74
within the prescribed limit (USEPA, 1998). Further, many in-situ groundwater remediation
75
technologies have been developed, among which the Permeable Reactive Barrier (PRB) has
76
emerged as a promising alternative for the in-situ treatment of a variety of the groundwater
77
contaminants such as heavy metals, organics radionuclides, volatile organic carbons (VOCs),
3
However, these
78
chlorinated compounds, etc. (Thiruvenkatachari et al., 2008; Phillips, 2009; Xu et al., 2012;
79
Obiri-Nyarko et al., 2014; Faisal and Ali, 2017).
80
The PRB system primarily consists of a barrier filled with the reactive material which is
81
placed in the path of the contaminant plume at the subsurface to provide treated water
82
downstream from the barrier (Naidu and Birke 2014). The reactive materials, used in the PRB
83
system, play a very significant role to determine the performance efficiency of the entire
84
remediation process. The widely used reactive materials in PRB are Zero-valent iron (ZVI),
85
activated carbon (AC), limestone, activated alumina, sawdust, pea gravel, etc. The most
86
common reactive material among them is ZVI, which has been installed in more than 60% of
87
the PRBs in worldwide (ITRC, 2005). However, the treatment efficiency of ZVI is very
88
insignificant in many cases due to critical issues of precipitation and clogging at certain sites.
89
Therefore, AC has been applied widely for the removal of contaminants such as
90
hydrocarbons and chlorinated compounds (USEPA, 1998; Obiri-Nyarko et al., 2014). In
91
particular, for the treatment of chlorinated compounds, variety of AC have been used such as
92
commercial activated charcoal (CAC), activated coconut charcoal (ACC), heat-activated
93
bone charcoal (HABC) and activated wood charcoal (AWC) (Mukherjee et al., 2007;
94
Mohammed et al., 2012; Trubetskaya et al., 2019). AC and its different varieties provide
95
higher adsorption sites on their surface for the chloride and other contaminants, therefore,
96
many studies have shown AC as an effective and efficient adsorption material for various
97
organic pollutants (Webber and Morris, 1963; Mukherjee et al., 2007; Faust and Aly, 2013).
98
Adsorption of various pollutants over activated carbon is considered as the best available
99
technology (BAT), recommended by USEPA, among all the available technologies (Adams
100
and Watson, 1987). However, it is found that the CACs are very costly in nature and they
101
cannot use to treat a large range of chlorinated and other contaminants very efficiently for a
102
longer time period (Akl et al., 2014). Therefore, locally available material, i.e. AWC, as
103
steam activated biomass soot and tire carbon black, are more sustainable options for the
104
treatment of a large number of contaminants at a lower cost (Kennedy et al., 2004;
105
Mohammed et al., 2012; Trubetskaya et al., 2019).
106
The suitable design of the reactive barrier depends on many factors in which hydraulic
107
conductivities of the surrounding aquifer (Kaquifer) as well as the barrier (Kbarrier) are the most
108
significant. Kbarrier of the barrier must be higher than that of the Kaquifer to maximize the
109
remediation efficiency by allowing the contaminated groundwater plume to pass through the 4
110
barrier under a natural hydraulic gradient (Kacimov et al., 2011; Bortone et al., 2013).
111
Various studies have investigated the performance of the PRB system for the treatment of
112
different contaminants, on lab-scale experiments or large scale field assessment, (Blowes et
113
al., 1998; Vogan et al., 1999; Puls et al., 1999; Wilkin et al., 2003; Genç-Fuhrman et al.,
114
2007). However, prior to on-site PRB installation, the modelling of the PRB design would aid
115
in analyzing the performance of the PRB system for longer time periods and simulate its
116
behaviour under various plausible scenarios by varying factors such as the configuration of
117
PRB, location, and orientation of barrier, contaminant properties, etc.
118
Zeng and Wang (1999) and Konikow (2011) have used the numerical groundwater modelling
119
tools - MODFLOW and MT3DMS - for the flow and solute transport modelling respectively
120
to analyze the spreading of the contaminant plume in the aquifer system for a longer duration.
121
The MODFLOW and the MT3DMS tools work on finite difference techniques such as
122
explicit, implicit and Crank Nicolson finite difference methods. MODFLOW has been widely
123
used to quantitatively estimate the aquifer response concerning different input parameters
124
(McDonald and Harbaugh, 1988; Scott and Folkes, 2000; Zhan et al., 2009; Xu et al., 2012).
125
Scoot and Folkes (2000), Mayer et al. (2001) and Pandey and Mathur (2015) have introduced
126
reactive barriers in their groundwater models to analyze the behaviour of plume migration
127
through the PRB system. Further, few studies are carried out towards multiple reactive barrier
128
(multi-PRB) systems instead of a single barrier system for efficient groundwater remediation
129
(Birke et al., 2007, Lee et al., 2010; Xu et al., 2012).
130
A multi-PRB system, as shown in Fig. 1, is broadly defined as a sequence of PRBs placed
131
one-after-another and each PRB is either filled with the same or different reactive materials
132
based on the target contaminants (Birke et al., 2007). It can also be defined as a single barrier
133
filled with two or more reactive materials for the simultaneous removal of contaminants (Xu
134
et al., 2012; Obiri-Nyarko et al., 2014). Lee et al. (2010) recommended the use of numerical
135
modelling coupled with the multi-PRB system for the efficient remediation of a wide variety
136
and higher ranges of contaminants. Xu et al. (2012) have developed a model for a three-
137
dimensional flow and contaminant transport in an aquifer system subject to multi-PRB
138
remediation considering different forms of a single contaminant developed in various stages
139
of a chain reaction. However, they modelled the plume under the impact of a single
140
contaminant point source in a very small area and for a short time period. Birke et al. (2007)
141
have explained that treating a mixture of pollutants, without many difficulties, is easy with 5
142
the single reactive material in the multi-PRB system. Contrary, the situation is very difficult,
143
arises many problems such as clogging, uncertain interruption of fluid flow, etc., when
144
several reactive materials used sequentially in a multi-PRB system. Nevertheless, for the
145
higher range of single contaminant, it is very difficult to design and manage the hydraulics of
146
the system and its reactive behaviour with a large thickness of the barrier. The analysis of
147
these factors and their impact on the performance of the PRB system for a large area are rare
148
to find in the earlier studies. Moreover, the role of the location of the multiple reactive
149
barriers was unexplored in the modelling for the PRB system over a longer timeframe.
150
This paper aims to develop a multi-PRB numerical model using a modified MODFLOW
151
engine for the flow model followed by the MT3DMS engine for the contaminant transport
152
model. This numerical model aims to analyze the reactive efficiency of activated wood
153
charcoal (AWC), as a reactive barrier material, for the treatment of a single contaminant at
154
different stages, released from multiple point sources, in an artificially drawn study area. The
155
study is based on the advection-dispersion-reaction (ADR) equation considering the
156
adsorption as the reaction process for the groundwater remediation from all the PRBs in a
157
sequential manner. The three reactive barriers, in continuous configuration, are placed at
158
three different locations from the point sources. The VMOD is used as a numerical modelling
159
tool for the development of a flow and solute transport model for a multi-PRB system. The
160
MODFLOW-2000 and MT3DMSV5.2 are used as a flow and solute transport engine
161
respectively in VMOD. The three major aims of this paper are: a) to simulate the three
162
dimensional flow and solute transport model for the remediation of a homogeneous aquifer;
163
b) to analyse the removal efficiency of all the reactive barriers, under the impact of various
164
factors, over space and time for the treatment of contaminants released from multiple source;
165
c) to analyze the effect of continuous pumping on the removal efficiency of the PRB system.
166
2 Study Area
167
A hypothetical study area, as shown in Fig. 2, is considered for the development of the multi-
168
PRB numerical model to analyze the management of the contaminated plume. Mahar and
169
Data (2000) have introduced this study area for the identification of groundwater pollution
170
sources under transient conditions. Later, various researchers like Borah and Bhattacharjya
171
(2013, 2014), Singh et al. (2004), Srivastava and Singh (2015), Chaubey and Kashyap (2017)
6
172
have adopted the same study area for dealing with different aspects of groundwater
173
modelling.
174
The hypothetical study area covers a confined aquifer with an area of 1.04 km2 (1.3 km × 0.8
175
km) and a depth of up to 30 m. The details of the aquifer characteristics are shown in Table 1.
176
A continuous pumping well (P) is located at the center of the study area. The pumping rates
177
of the P, as shown in Table 2, are varied at an interval of 90 days (constant time step) with the
178
maximum and minimum pumping rates (m3/day) being 381.024 and 163.296 respectively.
179
The boundary conditions of the aquifer are considered to be time-invariant. The north and the
180
south boundaries are modelled as no-flow boundaries. The east and the west boundaries are
181
regarded as the constant head boundaries with the hydraulic head (m) varied from 100.00 to
182
99.58 and 88.00 to 87.72, respectively. Two potentially active contaminant sources (S1, S2)
183
are placed at the upgradient of the study area. The S1 and S2 sources are active for the first
184
360 days, with varying flux after every 90 days (as shown in Table 3). It is assumed that
185
Chloride (Cl-) is the only contaminant produced from all the active contaminant sources. The
186
eight observation wells, C1, C2, C3, C4, C5, C6, C7, and C8, are spread throughout the
187
aquifer. Aquifer parameters
Symbol
Hydraulic Conductivity in all three
Kxx
=
Kyy
=
Values Kzz
0.000191 m/s
dimensions
Effective Porosity
ᶯ
0.25
Longitudinal Dispersivity
DL
40.0 m
Transverse Dispersivity
DT
9.6 m
Specific Storage
S
0.002
188 189
Table 1. Aquifer characteristics for the study area.
190
Time step (90 days)
Pumping 3
rate (m /day)
Time step (90 days)
Pumping rate 3
(m /day)
7
Time step
Pumping rate
(90 days)
(m3/day)
1
273.024
8
273.024
15
381.024
2
163.296
9
381.024
16
217.728
3
327.456
10
217.728
17
273.024
4
163.296
11
163.296
18
163.296
5
273.024
12
327.456
19
327.456
6
327.456
13
273.024
20
217.728
7
163.296
14
163.296
-
191
Table 2. Pumping rate of water at pumping locations for different time steps (Borah and
192
Bhattacharjya, 2014).
193
Duration
Source flux (g/day)
(days)
S1
S2
S3
0-90
4,060,800
2,592,000
0
91-180
1,296,000
5,080,320
0
181-270
3,196,800
0
0
271-360
0
3,024,000
0
194 195
Table 3. Source Flux at different locations (Borah and Bhattacharjya, 2014).
196
197
3 Methodology
198
The general methodology adopted for modelling of PRB(s), is shown in Fig. 3 and briefly
199
described below. The first step is the identification of the target contaminant in the
200
considered study area. The second step is the development of flow and solute transport
201
modelling for the given aquifer system for the analysis of the contaminant plume spreading
202
throughout the area. Based on the identification of highly contaminated zones in the
203
subsequent step, the next step is the installation of a single or multiple PRBs. Further, the
204
PRB system is subjected to performance evaluation at every installation to check the
205
desirability of the PRB system for in-situ groundwater remediation from multiple
206
contaminant sources.
207
3.1 Assumptions 8
208
In this study, the following assumptions have been made: (a) the aquifer is considered to be
209
homogeneous; (b) the aquifer is considered to be isotropic (c) all contaminant sources are
210
producing one common contaminant, i.e. chloride (Cl-); (d) the initial concentration of Cl- in
211
all the wells is considered to be 100 mg/L; (e) the adsorption phenomenon is the only form of
212
remediation taken into consideration; (f) the Langmuir isotherm is adopted for the adsorption
213
phenomenon.
214
3.2 Governing Equations
215
The reactive transport of the solute in the aquifer was modelled using the advection-
216
dispersion-reaction (ADR) equation coupled with the flow equation. In tensor notation, the
217
three-dimensional transport of the solute can be represented by Equation (1) (Zheng and
218
Wang, 1999):
+ =−
±
(1)
219
Where C
solute concentration (ML-3)
t
time (T)
ui
velocity in three dimensions (LT-1)
xi
longitudinal, lateral, and vertical distance (L)
Dij
dispersion coefficient tensor (L2T-1)
rm
physical, chemical, and biological reaction rates (ML-2T-1)
m
number of reaction types that have been taken place inside the barrier
220 221
The aquifer is considered to be homogeneous with the principal components of dispersion
222
represented by Dxx, Dyy, and Dzz for longitudinal, lateral, and vertical flow. Therefore,
223
Equation (1) can be simplified to a partial differential equation in three dimensions with
224
constant coefficients as shown by Equation (2).
225
= −[ + + ] + [ + + ] ± ∑
(2)
226
The chemical interaction, specifically adsorption, of the solute with the surfaces of the porous
227
medium, in the PRB, can be defined by the following Equation (3) (Fetter, 1992):
9
228
0
229 230
+ = ! −
"# $
∑ &'() * − (+ ,- − (. ,
(3)
= () * − (+ ,
Where 12
bulk density (ML-3)
3
porosity of the porous medium (T)
()
adsorption rate coefficient
(+
desorption rate coefficient
S
sorbed concentration (ML-3)
(.
decay rate coefficient
*
a function that indicates the sorption isotherm
231 232
The *(C) function is mainly based on the best breakthrough curve which could follow either
233
the linear or the Freundlich or the Langmuir model.
234
It is assumed that adsorption was the only predominant process for the interaction of the
235
contaminant and the reactive materials inside the barrier. Therefore, Equation (3) can be
236
reduced to Equation (4) as shown below:
237
+ = ! −
"# $
∑ &() *
(4)
238 239
3.3 Numerical Simulation of PRB
240
In this study, Visual MODFLOW version 2011.1 is used for the flow and transport simulation
241
in a homogeneous aquifer system. The entire hypothetical study area (1300 m × 800 m) is
242
disintegrated into smaller rectilinear grid cells of size 100 m × 100 m. A single layer of 30 m
243
depth is considered in all the computational grids of the model. After the definition of grid
244
size, various input parameters such as the hydraulic characteristics (conductivity,
245
transmissivity, specific yield, specific storage, effective porosity, and initial head), boundary
246
conditions (location of impermeable boundaries and constant heads) are initialized to the
247
model. Pumping well is also considered in the study, which constitutes an important
248
component of the solute transport in the aquifer system. The continuous pumping effectively
249
influences the water flow as well as solute transport within the aquifer and directly affect the 10
250
management of the groundwater system. Therefore, over-drafting of water, also termed as
251
continuous pumping, from the subsurface can unenviable changes in the movement of
252
contaminant transport in the aquifer system due to uncertain variation in head losses in the
253
aquifer system. Further, due to uncertain changes in the simulation of the flow and transport
254
model, the numerical simulation efficiency of the contaminant remediation from the reactive
255
barriers is also changed effectively. The centre of the study area is selected as the location of
256
the single continuous pumping to analyze the direct effect of solute transport in the whole
257
aquifer due to the continuous drafting of water from the aquifer as well as the effect on the
258
performance efficiency of the PRB system.
259
MODFLOW 2000, a three-dimensional finite-difference based groundwater flow modelling
260
tool, was used to simulate the flow under transient conditions. The contaminant transport
261
simulation was performed using MT3DMS, which followed the flow (MODFLOW)
262
simulation in order to analyze the contaminant spreading throughout the study area. The
263
MT3DMS tool was defined using some additional properties such as initial concentration and
264
two different point sources as the boundary conditions. The central finite difference method
265
under the implicit state was used to solve the advection-dispersion transport in the model.
266
The combined flow and contaminant transport model was run using WHS solver, which
267
works on a two-tier approach for the solution at each time step. Further, the flow and
268
transport model is simulated for 20-time steps in the entire five years’ period.
269
After a successful model run for the flow and contaminant transport modelling, the
270
installation of a single and multiple PRB systems is incorporated. The results of the
271
developed numerical model, using Visual MODFLOW, have been compared with the results
272
of the previous studies of Mahar and Dutta (2000), Borah and Bhattacharjya (2013 and 2014),
273
Srivastava and Singh (2015) performed on the same study area. The results could verify the
274
solute transport model including the temporal distribution of concentration in the area
275
covering all the observation wells. Thereafter, the continuous PRB configuration system,
276
followed by the developed flow and solute transport model, is adopted for the chloride
277
remediation produced from two different point sources. Initially, the 1st PRB is installed just
278
adjacent to the contaminant source (S1 andS2) followed by multi-PRB (2nd PRB and 3rd PRB)
279
installation, as shown in Fig. 2. The thickness of the PRBs is defined as 10 meters throughout
280
the depth of the barrier, i.e., 30 meters, of the study area. The PRBs are installed at an
281
orientation of 90◦ to the contaminant plume. Activated wood charcoal (AWC) is used as the
282
reactive material in the PRB system for the adsorption of the Cl- (Mohammed et al., 2012). 11
283
The adsorption parameters for the AWC reactive materials, such as adsorption capacity
284
(3.637 g/kg) and adsorption intensity (0.804 L/g) are obtained from Mohammed et al. (2012).
285
Many researchers have defined that, for a given PRB design, the discharge through the barrier
286
increases with an increase in Kbarrier (permeability of the barrier) relative to Kaquifer
287
(permeability of the aquifer) and vice versa (e.g., Gupta and Fox, 1999). Therefore, the
288
hydraulic conductivity of the reactive barrier is defined as three times that of the aquifer
289
hydraulic conductivity with a value of 5.7e-4 m/s. The 2nd PRB is installed close to the
290
contaminant source, however, at some distance to the 1st PRB. The 3rd PRB is installed far
291
away from the contaminant sources as well as from the 1st and 2nd PRBs.
292
The numerical simulation of the model is performed in six parts: (a) no PRB installation; (b)
293
after 1st PRB installation, (c) after 2nd PRB installation, (d) after 3rd PRB installation, (e) after
294
(1st+2nd) PRB installation together, (f) after (1st+2nd+3rd) PRB installation together.
295
4 Results and Discussions
296
The results of this study are divided into five major sections: (i) concentration analysis of the
297
wells, (ii) effect of PRB thickness variations, (iii) effect of pumping variations, (iv) effect of
298
depth variations, (v) spatial variation of the contaminant plume at different time-steps, (vi)
299
contaminant removal efficiency of the multi-PRB system.
300
4.1 Concentration Analysis of the Wells
301
The variation in the concentration of Chloride with time, in all the observation wells, for all
302
the cases of PRB installation is shown in Fig. 4. In case (a) with no PRB installation, the
303
observation wells, C2, C5, and C1, show the steep increase in the contaminant concentration
304
for the initial days in the observation period due to continuous emission of the contaminant
305
from the nearby contaminant sources, S1 and S2. Thereafter, the concentration in C2, C5, and
306
C1 reaches their respective maximum values and then subsequently decreases to zero until
307
the end of the observation period (1800 days). The well C5 shows a bi-modal concentration
308
profile, i.e., having two peaks, because of its proximity to the discontinuous source S2. The
309
continuation of the source (S2) for the first 180 days leads to the gradual increment of the
310
contaminant concentration in the well until the first peak is achieved. S2 is discontinued for
311
the next 90 days, leading to a decrease in concentration. After 270 days, S2 is re-continued
312
following which the concentration rapidly increases and attains the global peak. The other
313
wells C3, C4, C6, C7, and C8, which are located far away from source S1 and S2 show a very 12
314
minimal increase in contaminant concentration with respect to time. Moreover, they achieve
315
their peak concentration very late, 900 days after the source is deactivated. At the end of the
316
observation period, i.e., 1800 days, most of the wells, except C2, C5, and C1 are not
317
completely attenuated. The continuity-discontinuity of the contaminant sources near the
318
observation wells leads to the increment-decrement pattern in the concentration profile of
319
these wells. The concentration in all the observation wells declines mostly due to no
320
continuous external recharge of contaminants from both the sources as well as continuous
321
dilution due to pumping.
322
In case (b), i.e., 1st PRB installation, the similar increment-decrement pattern of the
323
concentration in the wells is observed, as shown in Fig. 4 (b). When compared to the case (a)
324
with no PRB installation, the concentration in all the observation wells drops threefold.
325
Similarly, the rate of increase in contaminant concentration is also decreased in all the
326
observation wells. This is evident as the time to reach the peak concentration is significantly
327
delayed. Moreover, the concentration profile of well C5, which is bimodal in case (a), shows
328
a single peak, as one of the peaks gets replaced by the point of inflection. It is noteworthy
329
here that the placement of the reactive barrier, in addition to remediating the groundwater,
330
retards the contaminant plume for a longer period when compared to the case (a) of the
331
absence of a barrier. At the end of the observation period, the wells C2, C5, and C1 show
332
higher concentrations, compared to all other observation wells due to retardation of the solute
333
transport upstream of all the observation wells. Therefore, the high intensity of the plume is
334
contained in the vicinity of the contaminant sources and these three observation wells, unlike
335
other far away observation wells.
336
Further, the installation of a 2nd PRB, upstream of all the observation wells, as shown in Fig.
337
4 (c) has been incorporated adjacent to the 1st PRB location. Both the reactive barriers have
338
shown almost similar results of concentration degradation with respect to time for all the
339
observation wells. However, in the case of wells C5 and C2, concentration degradation is
340
opposite for the entire observation period, 1800 days, in both the PRBs. As in the 1st PRB, the
341
rate of concentration degradation of well C5 is faster than well C2, however, the rate of
342
concentration degradation of well C2 is faster than well C5 after the installation of the 2nd
343
PRB. This manifests the different time period of concentration recharge in both the sources
344
and different time of interaction of the contaminant plume with the reactive barrier as the
345
location of both the barriers are different. Further, the 3rd PRB is placed downstream of
346
observation wells C2, C5, and C2 but upstream of all the other observation wells, i.e. C3, C4, 13
347
C5, C6, C7, and C8, as shown in Fig (4). Wells C2, C5, and C1 show worse results, as shown
348
in Fig. 4 (d), as compared to 1st PRB and 2nd PRB, however, the remaining wells show the
349
same results for all three PRBs. This clearly identifies the importance of the PRB location for
350
the remediation of a contaminated site.
351
After (1st+2nd) PRB (case (e)) and (1st+2nd+3rd) PRB (case (f)), simultaneous installation, the
352
concentration in most of the wells is further reduced, as compared to the individual
353
installation, as shown in Fig. 4 (e-f). However, due to the increased containment of the
354
contaminant plume by the (1st+2nd) and (1st+2nd+3rd) PRB, the rate of concentration decrease
355
in wells after discontinuity of all sources is significantly lowered. With the installation of
356
(1st+2nd+3rd) PRB, a concentration reduction in wells C3, C4, C6, C7, and C8 is observed
357
when compared to their concentrations during the (1st+2nd) PRB installation. However, no
358
such reduction in the concentration is observed for the observation wells lying upstream of
359
the 3rd PRB, i.e., C2, C5, and C1.
360
The installation of the (1st+2nd+3rd) PRB does not show a significant reduction in the peak
361
concentration of the contaminant. The concentration in C2, C5, and C1 is still higher than the
362
permissible limit of Cl-. Since the third PRB is placed far away from the source and therefore,
363
it lies in the downstream of the observation wells C2, C5, and C1, it plays no role in reducing
364
their contamination. This raises a critical point that the location of PRB plays a vital role in
365
increasing the remediation efficiency of the entire aquifer system. The PRBs which placed
366
nearby the pollution sources are more likely to remediate the aquifer compared to PRBs
367
which are far away from the source.
368
The peak contaminant concentration in all the wells, for all the four cases of the PRB system,
369
is shown in Fig. 5. The installation of the multi-PRB system sequentially reduces the
370
contaminant concentration in all the wells. In case (a) with no PRB installation, the maximum
371
peak concentration of the contaminant is observed in C2 followed by C5 and C1 due to their
372
proximity to the contaminant source. However, the other wells, i.e., C6, C3, and C7 show
373
relatively lower concentration. The minimum peak concentration of the contaminant is
374
observed in C8 and C4. These results reveal that the natural attenuation system of the aquifer
375
is not sufficient to remediate the contaminant up to the required plausible limit (permissible
376
limit of chloride in drinking water). Thereafter, the installation of the 1st PRB led to a
377
decrease in concentration at C2 and C5 along with other observation wells. Further, with the
378
installation of the (1st+2nd) and (1st+2nd+3rd) PRB, together, the concentration in C2, C5, and
14
379
C1 decreases more compared to individual installations of 1st PRB, 2nd PRB, and 3rd PRB.
380
However, the concentration in C5 drops down drastically when compared to C1 and C2
381
because C5 is closer to the continuous pumping location (P) than to C1 and C2. Further, the
382
concentration in C3, C4, C6, C7, and C8 observation wells drops below the required plausible
383
limit.
384
4.2 Effect of PRB Thickness Variations
385
The effect of various thicknesses of reactive barrier in a single PRB system for chloride
386
degradation, releasing from the multiple contaminant sources, is represented in Fig. 6. The
387
barrier thickness has been varied from 1 meter to 10 meters. It is clearly shown that the
388
thicker PRB shows better chloride degradation results than the thinner reactive barrier. The
389
thickest PRB, i.e., 10 meters, manifests the highest drop in chloride concentration for the
390
nearest observation wells C2 and C5 from the source (below 1000 mg/l), as shown in Fig. 6
391
(f). However, the thinnest PRB, i.e., 1 meter, manifests a small decline in chloride
392
concentration but the concentration is found more than 2000 mg/l, as shown in Fig. 6 (a), for
393
the same observation wells. The other cases of barrier thickness show the chloride
394
degradation results in between thickest, i.e., 10 meters, and thinnest PRB, i.e., 1 meter. It can
395
be clearly observed that the more residence time has been provided to the contaminant plume
396
for the thick barrier, which leads the contaminant plume for better adsorption process over
397
the barrier’s reactive media, compared to the thin PRB.
398
4.3 Effect of Continuous Pumping Variations
399
Three different cases of pumping variations have been observed when (a) the rate of
400
continuous pumping is P, as mentioned in Table 2., (b) the rate of continuous pumping is five
401
times more than the current pumping i.e., 5P, and (c) the rate of continuous pumping is ten
402
times more than the current pumping i.e., 10P. The effect of continuous pumping variations
403
has been observed for four different installations of PRBs i.e. without PRB, 1st PRB, (1st+2nd)
404
PRB and (1st+2nd+3rd) PRB as shown in Fig. 7. It has been observed that the increase in
405
continuous pumping rate from P to 5P leads to dilution of contaminant concentration in all
406
the observation wells. The high rate of dilution has been observed in the without PRB case,
407
Fig. 7 (a & e), however in all other PRB cases, Fig. 7 (b & f) – 1st PRB, Fig. 7 (c & g) -
408
(1st+2nd) PRB, and Fig. 7 (d & h) (1st+2nd+3rd) PRB, the rate of dilution of concentration is
409
lower due to contaminant retardation within the reactive barriers. Further, the rate of pumping
410
has been increased to 10P which also displays almost similar results, Fig. 7 - (i), (j), (k) & (l), 15
411
or the same rate of dilution in contaminant concentration as in the case of 5P. This exhibits
412
the saturation of dilution rate of contaminant concentration at 5P pumping rate and thereafter
413
the changes in the concentration are very low for all the observation wells.
414
4.4 Effect of Depth Variations
415
The multiple PRBs performances have been analyzed for four different depth variations
416
between 0-30 meters. Three different PRB cases, i.e., 1st PRB, (1st PRB+2nd PRB) and (1st
417
PRB+2nd PRB+3rd PRB), have been taken for performance analysis for four different depths,
418
5 meters, 10 meters, 20 meters, and 30 meters. In this study, all the scenarios have been
419
analyzed at a depth of 30 meters. However, in three-dimensional modelling, it is significant
420
to analyze the reactive barrier performance at different depths in the porous media. Therefore,
421
the comprehensive analysis for all the observation wells has been shown in Fig. 8 as
422
concentration vs time graph. The degradation of contaminant concentration is very low at 5
423
meters and 10 meters depths for all the multi PRB installation as shown in Fig. 8 (a-f).
424
However, the pattern of rising and fall of concentration vs time graph for all the observation
425
wells is similar to the without PRB installation case as shown in Fig. 4 (a). This clearly
426
displays the very small rate of contaminant degradation at these depths, therefore, for high
427
degradation rates PRB must be installed at higher depth at this particular study area.
428
Further, the installation of the PRB at 20 meters’ depth has significantly changed the rate of
429
contaminant degradation compared to the lower depth as shown in Fig. 8 (g-i). The
430
contaminant concentration has come down below the required plausible limit except at
431
observation wells C2, C5 and C1, however, these wells also show a significant drop in the
432
concertation at this depth as shown in Fig. 8 (g) for 1st PRB case. At the same depth, the rate
433
of degradation has increased after the installation of multi PRBs (1st PRB+2nd PRB) together,
434
as shown in Fig 8 (h). The same concentration drop has been displayed by (1st PRB+2nd
435
PRB+3rd PRB) installation simultaneously, as shown in Fig. 8 (i).
436
However, wells downstream of 3rd PRB have shown more significant changes after the
437
installation of three PRBs together compared to upstream wells. This is because the
438
contaminant plume is treated thrice before reaching downstream wells compared twice for the
439
upstream wells. The rate of contaminant degradation, for all the observation wells, at a depth
440
of 30 meters is similar to the rate of degradation at 20 meters, as shown in Fig. 8 (j-l), for all
441
the PRB installations. It is evident from this depth variation study that the maximum removal
442
efficiency is achieved at a depth of 20 meters. Therefore, this study reveals that instead of 16
443
going for the full depth of 30 meters, the maximum efficiency of a multi reactive barrier
444
system for this hypothetical example can be achieved at a lower depth of 20 meters.
445
4.5 Spatial Variation of Contaminant Plume at Different Time-steps
446
The spatial variation of the contaminant plume in the entire aquifer is analyzed at four
447
different time steps - 90 days, 450 days, 900 days and 1800 days for each PRB installation
448
case, as shown in Fig. 9-12.
449
Fig. 9 shows the spatial distribution of contaminant plume in the case of no PRB installation.
450
It is observed that with the passage of time, the plume spreads and moves away from the
451
point source. The concentration intensity of the plume is at a maximum near the source and
452
radially decreases while moving away from the source. At the end of 450 days, the plume
453
spread almost reaches the center of the aquifer (as shown in Fig. 9 (b)). The plume spreads in
454
an oval shape which indicates that the longitudinal dispersivity (X direction) is higher than
455
transverse dispersivity (Y direction) within the aquifer. At the end of 900 days, the plume
456
spread increases significantly, however, the strength of the plume is reduced. Due to lower
457
dispersivity in the transverse direction, the plumes from sources S1 and S2 overlap as shown
458
in Fig. 9 (c) and their cumulative spread encompasses all the observation wells. It is also
459
observed that after the discontinuity of source S1 and S2, the contaminant plume moves away
460
from their source profoundly in the downstream direction. At the end of the simulation
461
period, i.e., 1800 days the overlapped plume has entirely left the contaminant source and
462
moved to the downgradient half of the aquifer. Moreover, the maximum concentration
463
intensity of the plume is significantly reduced to 750 mg/L as shown in Fig. 9 (d).
464
The installation of the 1st PRB significantly decreases the contaminant intensity of the plume
465
at all the time steps as shown in Fig. 10. However, the plume spread of plume is reduced at
466
the initial time-steps only. Due to the placement of the 1st barrier just adjacent to the sources,
467
the management of plume near the source takes place; as a result, the plume is unable to leave
468
its originating point sources even after many days of discontinuity of the source. Therefore,
469
when compared to the case of no PRB installation, the longitudinal plume spread is higher
470
within the considered section of the aquifer. Nevertheless, the 1st PRB is highly effective in
471
minimizing the overall spread and intensity of contamination in the considered aquifer
472
system.
473
The spreading of the plume and the contaminant intensity further reduces by installing the
474
(1st+ 2nd) PRB, at a small distance away from the sources (as shown in Fig. 11). Similar to the 17
475
previous case, the plume does not leave the discontinuous source until the end of the
476
observation period. The PRBs not only act as barriers that treat the water passing through it
477
but also contain the contaminant for a longer time upstream of the barrier. The installation of
478
the (1st+2nd+3rd) PRB where 3rd PRB has been installed away from the contaminant source
479
further reduces the spread and the intensity of contamination in the aquifer as shown in Fig.
480
12. The concentration of contaminant decreases below the required permissible limit of Cl-
481
within the entire aquifer during the observation period of 1800 days. Moreover, the plume is
482
completely contained between the source and the third barrier, thus reducing the spread of the
483
contaminated plume significantly at the end of 1800 days. This shows that the water passing
484
through the third barrier is completely remediated.
485
4.6 Contaminant Removal Efficiency of the Multi-PRB System
486
The contaminant removal efficiency of the multi-PRB system has been defined by its
487
percentage of contaminant concentration degradation in all the observation wells after every
488
PRB installation in the aquifer. The removal efficiency is defined by equation (5). % 56789 =
489
::;< = ;>
;<
(5)
490
Where, ? is the concentration of the ith well in mg/l without any PRB installation
491
throughout the aquifer; is the concentration of the ith well in mg/L after jth PRB
492
installation.
493
The removal efficiency of the multi-PRB system is evaluated with reference to the no PRB
494
installation case. Fig. 13 shows the percentage removal of the contaminant in each
495
observation well after the installation of the 1st PRB, 2nd PRB, 3rd PRB, (1st+2nd) PRB and
496
(1st+2nd+3rd) PRB. The contaminant removal starts early in wells C2, C5 and C1 as compared
497
to other observation wells (as shown in Fig 13 (b, e, a)) as the treated plume from the 1st and
498
2nd PRB reach them early when compared to the other observation wells. However, the
499
percentage removal curve of the 3rd PRB is shown to be the lowest removal efficiency for
500
these observation wells. This is because the 1st PRB and 2nd PRB have been installed at the
501
upstream of all the observation wells but the 3rd PRB has been installed downstream of C2,
502
C5 and C2 and upstream of the other wells. Therefore, the contaminant retardation has not
503
occurred in these upstream wells due to the 3rd PRB installation. Nevertheless, the percentage
504
removal curves of the (1st+2nd) and (1st+2nd+3rd) PRB is overlapped for these wells
505
throughout the observation period because these wells are located in the downstream of 1st 18
506
and 2nd PRB but upstream of the 3rd PRB, therefore, no major changes have occurred in these
507
wells after the installation of 3rd PRB. However, in the case of the other wells (C3, C4, C6,
508
C7, and C8), situated downstream from the 3rd PRB, the overlap of the removal curves takes
509
place for the first half of the simulation period, i.e., 900 days. However, wells C3 and C7
510
show the incomplete contaminant remediation after all the three PRB installation, at the end
511
of the observation time (1800 days). Due to the lower dispersivity of the aquifer in the
512
transverse direction and the nonalignment of these wells with the contaminant source, the
513
treated plume reaches these wells very late.
514
It is observed that the percentage removal of the contaminants sequentially increased with the
515
installation of multiple numbers of PRBs. The contaminated plume initially gets treated with
516
the first PRB, followed by the second PRB and third PRB sequentially. Therefore, the
517
efficiency of the (1st+2nd+3rd)
518
PRB. These results indicate the higher efficiency of the multi-PRB compared to single PRB
519
in remediating the aquifer efficiently.
PRB is higher than the (1st+2nd) PRB followed by the 1st
520 521
5 Conclusions
522
This paper has investigated the in-situ remediation of a homogeneous aquifer system with a
523
single contaminant by numerical modelling of a multi-PRB system. A hypothetical study
524
area, having two active point sources of contamination and continuous pumping, is modelled.
525
MODFLOW is used to simulate the flow model followed by MT3DMS for the solute
526
transport model. Three PRBs, continuously configured are installed at three different
527
locations from the source. The performance of the multi-PRB system is evaluated for a time
528
period of five years (1800 days).
529
It is observed that the performance of multiple PRBs is superior to a single PRB system and
530
natural attenuation in the aquifer processes. In the case of no PRB system, the maximum
531
intensity of contaminant plume is significantly higher than the permissible limit as the
532
concentration in all the observation wells are many folds higher than the desired standard
533
limits. Therefore, with the installation of the 1st PRB, adjacent to the contaminant sources, the
534
plume concentration intensity dropped down remarkably so as the concentration in all the
535
observation wells. However, the 1st PRB installation is still unable to achieve the reduction up
536
to the permissible contaminant limit. Consequently, the second and third PRBs are installed 19
537
simultaneously to remediate the aquifer to achieve the essential limit of the contaminant in
538
the groundwater. Since, the concentration in all, near and far away, wells are dropped to a
539
required value.
540
The thickness of the PRB is a guiding factor in determining the efficiency of PRB in the
541
remediation of the contaminant plume. The thick barriers can be provided more residence
542
time to the contaminant plume for better reactivity with the reactive material compare to the
543
thin PRB. Multiple PRBs, with the limited barrier thickness, also drop down the chances of
544
frequent hydraulic loss and help to manage the reactive behaviour between the contaminant
545
and reactive material, when installed on the field. In addition, the continuous pumping also
546
increases the remediation rate of the multi-PRB system for the area in its vicinity. Further, it
547
is observed that the depth of reactive barrier installation is also important to analyze, before
548
field installation, to achieve the optimum depth of the barrier for obtaining maximum
549
removal efficiency. The depth variation in this study showed that the maximum contaminant
550
degradation can be achieved at a depth less than the full depth possible for the study.
551
Therefore, on the field study, the installation of reactive barriers at the right depth should lead
552
to a cost-saving by minimizing the size and number of required reactive barriers. Further, it is
553
also observed that the PRBs which are in the proximity of contaminant source contain the
554
plume more significantly than the far away PRBs.
555
Furthermore, it is observed that dispersion plays an important role in governing the treatment
556
rate of the contaminant plume for a long period of time. The low transverse dispersion
557
coefficient results in a lower treatment rate of the plume that reaches the observation wells
558
are not aligned with the point source. On the other hand, the high longitudinal dispersion
559
leads to a higher rate of plume treatment to the observation wells aligned with the
560
contaminant source. Moreover, the results suggest that the performance evaluation of multi-
561
PRB systems is very significant through numerical modelling for a longer duration.
562
Acknowledgment
563
This research is fully supported by the Indian Institute of Technology Delhi, India. We would
564
like to thank Mr. Shushobhit Chaudhary from the Indian Institute of Technology Delhi for his
565
insight and expertise on the subject that greatly assisted this research work.
566
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24
Figure Captions Fig. 1 In-situ multi-PRB groundwater remediation system.
Fig. 2 Schematic representation of the hypothetical study area with (a) Plan view and (b) elevation view of 1st, 2nd and 3rd installed PRB. Fig. 3 Comprehensive methodology of the Permeable Reactive Barrier (PRB) modelling for groundwater contaminant(s) removal. Fig. 4 Variation of Chloride concentration with time in all observation wells for the cases of (a) no PRB installation, (b) 1st PRB installation, (c) 2nd PRB installation, (d) 3rd PRB installation, (e) (1st+2nd) PRB installation, and (f) (1st + 2nd + 3rd) PRB installation. Fig. 5 Maximum concentration of contaminants in all the monitoring wells in various cases of PRB installation.
Fig. 6 Concentration vs time graph for single PRB for six different cases of barrier thickness i.e. (a) 1 meter, (b) 2 meters, (c) 4 meters, (d) 6 meters, (e) 8 meters, and (f) 10 meters. Fig. 7 Concentration vs time graph for all the cases of PRB i.e. without PRB, 1st PRB, (1st+2nd) PRB and (1st+2nd+3rd) PRB for the variation in continuous pumping rate (a-d) Pumping rate = P; (e-h) Pumping rate = 5P; (i-l) Pumping rate = 10P respectively. Fig. 8. Concentration vs time graph of 1st PRB, (1st+2nd) PRB and (1st+2nd+3rd) PRB at a depth of (a-c) 5 meters, (d-f) 10 meters, (g-i) 20 meters and (j-l) 30 meters respectively.
Fig. 9 Spatial variation of contaminant plume (mg/L) in case of no PRB installation at time steps of (a) 90 days, (b) 450 days, (c) 900 days and (d) 1800 days.
31
Fig. 10 Spatial variation of a contaminant plume in case of 1st PRB installation at time steps of (a) 90 days, (b) 450 days, (c) 900 days and (d) 1800 days. Fig. 11 Spatial variation of a contaminant plume in case of (1st+2nd) PRB installation at time steps of (a) 90 days, (b) 450 days, (c) 900 days and (d) 1800 days. Fig. 12 Spatial variation of a contaminant plume in case of (1st+2nd+3rd) PRB installation at time steps of (a) 90 days, (b) 450 days, (c) 900 days and (d) 1800 days. Fig. 13 Percentage removal of Chloride (Cl-) in (a) Well 1, (b) Well 2, (c) Well 3, (d) Well 4, (e) Well 5, (f) Well 6, (g) Well 7, (h) Well 8, after installation of 1st PRB, 2nd PRB, 3rd PRB, (1st+2nd) PRB and (1st+2nd+3rd) PRB.
32
(b) 450 days
900
900
(a) 90 days
S2
C8
600
600
C8 C5
C6
C5 P
400
P
400
S2
C7
C3
C1 S1
C7
C4
200
200
C4
C6
C3
C1 S1
C2
-100
-100
C2
-100
0
300
600
900
1200
-100
1500
0
300
600
900
1200
1500
(d) 1800 days
900
900
(c) 900 days
600
S2
C8
C5
400
P
C6
S2
C5
C7
P
400
600
C8
C3
C1
C3
C1 S1
C2
C2
-100
-100
S1
C7
C4
200
200
C4
C6
-100
0
300
600
900
1200
1500
-100
0
300
600
900
1200
1500
(a) 90 days 900
900
(b) 450 days C8
S2
600
600
C8 C5
C6
C6
C7
400
C4
-100
0
200
C3
C1
300
600
900
1200
1500
-100
C3
C1
S1
C2
C2
-100
-100
200
C4 S1
C7
P
P
400
C5
S2
0
300
600
900
1200
1500
(d) 1800 days
900
900
(c) 900 days
C8
S2
600
600
C8 C5 C6
S2
C6
C7
C4
C1
200
200
C4 C3
C3
C1 S1
C2
C2
-100
-100
S1
C7
P
400
P
400
C5
-100
0
300
600
900
1200
1500
-100
0
300
600
900
1200
1500
(b) 450 days
900
900
(a) 90 days
C8
600
600
C8 S2
C5
C6
C5
C6
P
400
400
P
S2
C7
C4
200
200
C4 C3
C1 S1
C7
C3
C1 S1
C2
-100
-100
C2
-100
0
300
600
900
1200
1500
-100
0
300
600
900
1200
1500
(d) 1800 days
900
900
(c) 900 days
C8
600
600
C8 S2
C5
C6
S2
C7
C5
400
C6
P
400
P
C4 C3
C1 S1
200
200
C4
C7
C3
C1 S1
C2
-100
-100
C2
-100
0
300
600
900
1200
1500
-100
0
300
600
900
1200
1500
Percentage Removal
1st PRB
Percentage Removal
(1st+2nd) PRB
(1st+2nd+3rd) PRB
(b)
100
Well 1
80
Well 2
80
60
60
40
40
20
20
0
0 450
900
1350
1800
(c)
100
0
450
900
60
40
40
20
20
0
1800
Well 4
80
60
1350
(d)
100
Well 3
80
0 0
Percentage Removal
3rd PRB
(a)
100
0
450
900
1350
1800
(e)
100
0
450
900
60
40
40
20
20
0
1800
Well 6
80
60
1350
(f)
100
Well 5
80
0 0
Percentage Removal
2nd PRB
450
900
1350
1800
(g)
100
450
900
60
40
40
20
20
0
1800
Well 8
80
60
1350
(h)
100
Well 7
80
0
0 0
450
900
Time (days)
1350
1800
0
450
900
Time (days)
1350
1800
(a) 99.58 m
87.72 m
No Flow Boundary
C8
S2
C5
C6
C7
P
C4
C8
S1
C2
100.00 m
C1
88.00 m
No Flow Boundary
(b) 0m P C5
C6
C7
30 m
1st PRB
2nd PRB
3rd PRB
Constant Head Boundary
S-Contaminant Source
C-Concentration Well
P-Pumping Well
C8
C7
C6
C5
C4
C3
Concentration (mg/L)
(a) 3000
3000
Without PRB
2000
2000
1000
1000
1st PRB
0 0
450
900
1350
1800
0
450
(c)
Concentration (mg/L)
C1
(b)
0
3000
900
1350
1800
(d) 3000
2nd PRB
2000
2000
1000
1000
0
3rd PRB
0 0
450
900
1350
1800
0
450
(e)
Concentration (mg/L)
C2
3000
900
1350
1800
(f) 3000
(1st+2nd)PRB
2000
2000
1000
1000
0
(1st+2nd+3rd)PRB
0 0
450
900
Time (days)
1350
1800
0
450
900
Time (days)
1350
1800
3500 C1
C2
C3
C4
C5
C6
C7
C8
3000
Concentration(mg/L)
2500
2000
1500
1000
500
0 Without PRB
1st PRB
2nd PRB
3rd PRB
Without PRB Concentration (mg/L)
C8 Pumping Rate = P (a)
C7
C6
C5 C4 Pumping Rate = 5P (e)
3000
3000
2000
2000
2000
1000
1000
1000
0
0 450
900
1350 1800
0 0
450
1st PRB Concentration (mg/L)
(b)
900
1350
1800
0
3000
2000
2000
2000
1000
1000
1000
0
0 900
1350 1800
450
900
1350
1800
0
3000
2000
2000
2000
1000
1000
1000
0 900
1350 1800
1800
1350
1800
450
900
1350
1800
0
(h) 3000
3000
2000
2000
2000
1000
1000
1000
0 450 900 1350 1800 Time (days)
450 900 1350 Time (days)
1800
450
900 (l)
3000
0
900
0 0
(d)
0
1350
450
(k)
3000
450
1800
(g)
3000
0
1350
0 0
(c)
0
900 (j)
3000
450
450
(f)
3000
0
(1st+2nd) PRB Concentration (mg/L)
C2 C1 Pumping Rate = 10P (i)
3000
0
(1st+2nd+3rd) PRB Concentration (mg/L)
C3
0 0
450 900 1350 Time (days)
1800
0
C8
C7
C6
C5
5 Meter Depth Concentration (mg/L)
1st PRB (a)
10 Meter Depth Concentration (mg/L)
C2
3000
2000
2000
2000
1000
1000
1000
0
0 450
900
1350 1800
0 0
450
900
1350 1800
0
3000
3000
2000
2000
2000
1000
1000
1000
0 450
900
1350 1800
450
900
1350 1800
0
3000
2000
2000
2000
1000
1000
1000
0 900
1350 1800
450
900
1350 1800
0
(k) 3000
3000
2000
2000
2000
1000
1000
1000
0 450 900 1350 1800 Time (days)
450
900
1350 1800
(l)
3000
0
1350 1800
0 0
(j)
0
900 (i)
3000
450
450
(h)
3000
0
1350 1800
0 0
(g)
0
900 (f)
3000
0
450
(e)
0
C1
(1st+2nd+3rd) PRB (c)
3000
(d)
20 Meter Depth Concentration (mg/L)
C3
3000
0
30 Meter Depth Concentration (mg/L)
C4
(1st+2nd) PRB (b)
0 0
450 900 1350 1800 Time (days)
0
450 900 1350 1800 Time (days)
(a) 90 days 900
900
(b) 450 days C8
S2
600
600
C8 C5
C6
C5
C6
C4
200
200
C4 C3
C1 S1
C3
C1 S1
C2
C2
-100
-100
-100
0
300
600
900
1200
1500
-100
0
300
600
(c) 900 days
900
1200
1500
900
900
(d) 1800 days
S2
C8
600
600
C8 C5
C6
C5
C6
C4
200
200
C3
C1 C2
C3
C1
S1
C2
-100
-100
S1
C7
P
400
P
400
S2
C7
C4
-100
C7
P
400
P
400
S2
C7
0
300
600
900
1200
1500
-100
0
300
600
900
1200
1500
Highlights
Multi-Reactive
Barriers
provide
highly
efficient
groundwater
remediation
performance.
Location, orientation, and depth of installed barriers are important to determine PRB performance.
Barriers placed nearby to contaminant sources are more likely to remediate the aquifer.
Removal of the contaminant sequentially increased with the installation of multibarriers.
Continuous pumping increases the remediation rate of the barrier system in the vicinity.