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Interface Transmissivity of Multicomponent GCLs
Ahmed AbdelRazek1 and R. Kerry Rowe2
1 Ph.D. Candidate, GeoEngineering Centre at Queen’s-RMC, Queen’s University,
Ellis Hall, Kingston ON, Canada, K7L 3N6. Email: Ahmed.abdel.razek@ queensu.ca.
2 Professor, Canada Research Chair in Geotechnical and Geoenvironmental
Engineering, GeoEngineering Centre at Queen’s-RMC, Queen’s University, Ellis
Hall, Kingston ON, Canada K7L 3N6. E-mail: kerry.rowe@queensu.ca.
ABSTRACT:
Both a coated and laminated GCL from the same manufacturer are examined with
respect to the interface transmissivity between the geofilm and a smooth 2.0 mm HDPE
GMB. The laboratory apparatus and test methods are described. The results obtained
from the interface transmissivity tests conducted under vertical stress of 150 kPa and
hydraulic head of 1.2 m are reported. The preliminary results suggest similar low
interface transmissivities to water of 1.2x10-11 m2/s and 1.3x10-11 m2/s for the coated
and laminated GCLs.
INTRODUCTION
Composite barrier systems are comprised of a geomembrane (GMB) overlying either
a compacted clay liner (CCL) or geosynthetic clay liner (GCL) or both. The primary
objective of the geomembrane is to prevent advective contaminant migration and, for
some contaminants, to also effectively prevent diffusive migration where the GMB is
intact. GCLs are intended primarily to reduce the leakage through GMB holes due to
its low hydraulic conductivity but the leakage will also be greatly related to the lateral
flow of contaminant away from the hole at the interface between the GMB and GCL
and this will depend primarily on the interface transmissivity between the GMB and
GCL (Fukuoka 1986, Brown et al. 1988, Rowe 1998, Mendes et al. 2010, Rowe et al.
2013).
Recently, multicomponent GCLs (coated and laminated GCLs) have been developed.
A coated GCL has a molten polyolefin layer applied to the carrier geotextile and
allowed to solidify. A laminated GCL has a thin geofilm glued to one side of the GCL.
In terms of hydraulic conductivity, they lie between a GMB and a conventional GCL
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(Cleary and Lake 2011; von Maubeuge et al. 2011; Barral and Touze-Foltz 2012).
Barral and Touze-Foltz (2012) proposed an experimental device to quantify the flow
rate through undamaged multicomponent GCLs. Examining four multicomponent
GCLs, they concluded that, for a geofilm with a high mass per unit area, the flow rate
of multicomponent GCLs is significantly smaller than that of conventional GCLs and
one order of magnitude greater than a virgin geomembrane. Whereas in the case of low
mass per unit area of geofilm, the hydraulic performance was closer to that of a
conventional GCL rather than virgin geomembrane due to the discontinuities
(imperfections) in the geofilm component of the GCL.
Several researchers have investigated the water transmissivity of a GMB/GCL
interface under various configurations, stress level and hydraulic heads (Harpur et al
1993; Barroso et al 2006, 2008, 2010; Bannour et al. 2013; Mendes et al. 2010, Rowe
and Abdelatty 2013) as summarized by Rowe (2012). Published data also suggests that
the GMB texture and nature of the bentonite had minimal effect on the interface
transmissivity under steady state conditions for the cases examined at 50 kPa applied
normal stress (Barroso et al 2008; Mendes et al. 2010).
Bannour and Touze-Foltz (2013) investigated the transmissivity at the interface
between the coating/laminate and the bentonite component of the GCL for three
different multicomponent GCLs of diameter 0.2 m using a decimeter scale cell (Touze-
Foltz et al. 2006). These tests, conducted under normal stress of 50 kPa and a hydraulic
head of 0.3 m, examined one coated GCL (GCL-T1) with a geofilm mass per unit area
of 0.25 to 0.4 kg/m2. The other two GCLs (GCL-T2 and GCL-T3) were both laminated
with a geofilm of about 0.2 kg/m2. Flow was introduced through a 4 mm prescribed
hole in the GCL coating and flow between the coating and the upper bentonite was
monitored. Two cases were examined: (i) no GMB placed on top of the punctured
geofilm component of the GCL, and (ii) GMB with hole directly over the hole in the
geofilm component of the GCL, silicone grease was applied on the bottom surface of
GMB to ensure that flow can only occur through the coating/attached film hole then
through the interface layer between coating/ attached film and upper bentonite of the
GCL. For the case of no GMB, the interface transmissivity values ranged from 3.5x10-
11m2/s (coated GCL-T1) to 5.5x10-10 m2/s (laminated GCL-T3). The case with an
overlying GMB resulted in an interface transmissivity ranging from 2.6x10-11 m2/s
(coated GCL-T1) to 4.4x10-11 m2/s (laminated GCL-T2) which is lower than the case
of no GMB, suggesting that the coating/film rigidity may lead to decreased flow rate
and interface transmissivity between the coating and the rest of the GCL.
Bannour and Touze-Foltz (2015) investigated the effect of scale on the flow rates of
multicomponent GCL. Tests were conducted using the same multicomponent GCLs
studied by Bannour and Touze-Foltz (2013) in a 1.0 meter diameter cell under same
test conditions (normal stress of 50 kPa and hydraulic head of 0.3 m). The only
difference was the use of protective geotextile of mass per unit area of 1.2 kg/m2 to
protect the coating from being punctured by a gravel layer placed over the geofilm
component of the GCL. One test was conducted for each of the three multicomponent
GCLs. An additional experiment was performed using GCL-T2 where the gravel was
placed, without a protective layer, directly on the coating to assess the effect of the
protective geotextile on the flow rate. It was reported that the protective geotextile had
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no effect on the transient and steady state flow rates. Interface transmissivity values of
2.0x10-11, 9.0x10-11, and 7.6 x10-11 m2/s were calculated for GCL-T1, GCL-T2 and
GCL-T3, respectively. The flow rates ranged from 4.6x10-12 to 3.0x10-11 m3/s for the
meter scale tests compared to flow rates of 1.5x10-11 to 2.8x10-10 m3/s for the decimeter
scale (other test condition being similar) at steady state. This suggests that the larger
meter scale tests reduced preferential paths related to irregularities in contact conditions
and also, possibly, the effect of the edges in decimeter scale tests and decreased the
deduced transmissivity somewhat compared to the smaller scale tests. The flow rates
at the interface between the geofilm and the rest of the GCL in the meter scale tests
(4.6x10-12 to 3.0x10-11 m3/s) were similar to a conventional GCL in contact with GMB
(4.x10-12 m3/s) and within the range for the GMB/GCL interfaces examined by Touze-
Foltz and Barroso (2006).
While the work cited above has examined the interface between the geofilm and the
bentonite component of the GCL, the transmissivity of an equally important interface
between the GMB and geofilm has not been examined. Thus, the objective of this paper
is to describe a different apparatus for measuring interface transmissivity of
multicomponent GCL in contact with HDPE GMB. Two tests are presented to examine
the interface transmissivity of a coated and laminated GCL in direct contact with a
smooth 2.0 mm thick HDPE GMB at a normal stress of 150 kPa to simulate the stress
under 10 to 15m of waste.
LABORATORY SET-UP
The laboratory set-up was designed to simulate a composite liner comprised of an
HDPE geomembrane (GMB) overlying a multicomponent geosynthetic clay liner
(GCL). The configuration was inverted compared to the typical field condition. The
test cell comprised a 0.2 m internal diameter, 15 mm wall thickness, and 0.11 m high
polyvinyl chloride (PVC) cylinder. The test set-up (Figure 1) involved (from bottom
up) a 2.0 mm HDPE GMB (MxC20) with a 10 mm hole in its center glued to the bottom
of the cell. The GCL was pre-hydrated with deionized water and cut to a diameter of
0.2 m. keeping the cover geotextile, a 25 mm ring of the carrier geotextile and bentonite
around the entire perimeter of the GCL was removed to create a space for the gravel
filter as shown in Figure 1. A geotextile strip having a thickness equal to the thickness
of bentonite and the carrier geotextile was placed around the bentonite. The GCL was
placed on the GMB with the laminated/coated carrier geotextile facing the GMB.
Fine gravel (4.75 mm < D < 5.6 mm) was placed around the GCL to transmit interface
flow to the effluent valve (Figure 1). A rubber bladder was placed on the top of GCL.
Bentonite paste was used to seal the edges of the bladder to the walls of the PVC cell.
Sand was used to fill the cell from the top of bladder to the top cap of the PVC cell.
The sand had a maximum dry density of 1.7 Mg/m3 at a moisture content of 12%. The
permeant was introduced to the cell through an influent valve at the bottom of the cell.
Whereas the effluent was collected in 250 mL HDPE capped bottle (with a thin air
pressure equilibration tube) through a lateral valve at the level of interface between the
GCL and GMB. A control collection bottle showed negligible evaporation of effluent
at room temperature in the laboratory.
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An upper gravel layer (Figure 1) was used as a detection layer to indicate if there was
any leakage between the bladder and the cell walls. A port was located at the mid height
of the gravel layer to monitor any such leakage (none was detected).
Air pressure was applied through the main pressure line with a regulator to control
the pressure to the desired value. The hydraulic head causing interface flow was applied
through 1000 ml graduated cylinder connected to the cell through a flexible tube with
water stopper placed on top of the cylinder to control the influent evaporation (but with
a thin pressure equilibration tube). For the tests reported herein, a hydraulic head of
1.2 m and a vertical stress of 150 kPa were applied to simulate a landfill that contains
waste of an average height 10 to 15 m (depending on waste density).
FIG. 1. Laboratory set-up for measuring interface transmissivity between a
GMB and GCL.
GCL
Two GCLs were examined. GCL-A (Bentofix CNSL) was a coated needle-punched
GCL comprised of 3.77 kg/m2 fine granular natural sodium bentonite between a staple
fiber needle-punched nonwoven cover geotextile (280 g/m2) and a woven carrier
geotextile with a polypropylene coating (combined mass per unit area of 350 g/m2; the
coating was so well bonded to the geotextile it was not possible to separate and
independently assess the mass of the two components). GCL-B (Bentofix LNSL) was
a laminated GCL comprised of 3.89 kg/m2 fine granular natural sodium bentonite
between a staple fiber nonwoven cover geotextile (288 g/m2) and a woven carrier
geotextile (145 g/m2) with an about 0.2 mm thick (170 g/m2) polyethylene film glued
to the woven geotextile (Table 1). Figure 2a and 2b show the top view and cross section
Leak
Detection
Valve
Effluent
Valve
GMB
Influent Valve
GCL with coating/laminate in
contact with GMB
Gravel
Compacted Sand
Gravel
Compacted Sand
Pneumatic Pressure
Fixed
Head
Tank
H (m)
Bladder
Bentonite
Paste
GTX
strip
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(with bentonite shaken out) view of GCL-A and GCL-B respectively.
Both GCLs were pre-hydrated prior to placement in the cell with deionized water for
two days (100% gravimetric water content) to provide initial GCL hydration that might
simulate a relative high degree of hydration from the subsoil in the field before
permeating fluid reached the hole in the geomembrane.
Table 1. GCL Properties (all masses are dry mass)
Generic
identifier
Average dry
mass of
GCL1
(g/m2)
Average
dry mass
of carrier
geotextile1
(g/m2)
Average
dry mass
of cover
geotextile1
(g/m2)
Average
dry mass
of
bentonite1
(g/m2)
Geofilm
thickness
(mm)
Average
dry
mass of
geofilm
(g/m2)
GCL-A
4410 ± 143
350a
280c
3770
- a
- a
GCL-B
4520 ± 545
145b
288c
3890
0.2
170
ASTM
D5993
D5261
D5261
D5993
D5199
D5261
1Average of five virgin GCL samples each 100 x 100 mm, taken from the same area
on the GCL roll.
a Woven geotextile with geofilm coating that could not be separated for independent
measurement
b Woven GTX to which laminate had been attached was easily separated allowing
measurement of both independently.
c Needle-punched nonwoven geotextile
(a) (b)
FIG. 2. Photographs of multicomponent GCLs (a) GCL-A (b) GCL-B.
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RESULTS AND DISCUSSION
Inflow rates were measured by monitoring the volume change of water in the burette
used to monitor inflow over prescribed time intervals (as in falling head test). Eq. 1 was
used for calculate the interface transmissivity (Harpur et al. 1993).
=a.ln(R2
R1)ln(h2
h1)
2t (1)
where:
= interface transmissivity (m2/s)
h = difference between head at hole and head at specimen boundary (m)
R2 = outer radius of specimen (m)
R1 = hole radius (m)
a = cross sectional area of falling head burette (m2)
h2 = head at the end of monitoring interval (m)
h1 = head at start of monitoring interval (m)
t = monitoring time interval (s)
Figure 3 shows the interface transmissivity values versus time for GCL-A (coated
GCL) as calculated using Eq. 1. The transmissivity dropped over time from 7x10-11
m2/s after 5 hours to 5.9x10-12 m2/s after 22 days and increased to 1.2x10-11 m2/s at 43
days after test initiation. The test is still in progress.
FIG. 3. Interface transmissivity versus time for coated GCL-A
GCL A
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For the laminated GCL-B, the interface transmissivity values decreased from
7.7x10-11 m2/s after 11 hours of test initiation to 1.3x10-11 m2/s after 43 days (Figure 4).
FIG. 4. Interface Transmissivity versus time for laminated GCL-B
AbdelRazek et al. (2016) reported that after 300 days of testing, the interface
transmissivity of a smooth 1.5 mm-thick HDPE geomembrane (MxC15) with a GCL
having powdered sodium bentonite was 9 x 10-13 m2/s and that with a GCL having a
granular sodium bentonite was 5 x 10-13 m2/s at 150 kPa. These values are lower than
the interface transmissivity of the GMB with the coated (1.2x10-11 m2/s; Figure 3) and
laminated (1.3x10-11 m2/s; Figure 4) GCLs. There are some factors thought to be
affecting the interface transmissivity values obtained for the granular and powdered
sodium bentonite at 150 kPa including the time dependent uptake of moisture and
intrusion of bentonite into the cover geotextile over the 300 days these test were
conducted which serve to reduce the interface transmissivity with time (AbdelRazek et
al. 2016). In contrast, the interface transmissivity values for the coated (1.2x10-11 m2/s)
and laminated (1.3x10-11 m2/s) GCLs reported above were similar to but slightly lower
than the values reported by Bannour and Touze Foltz (2013) where the interface
transmissivity values between coating/ attached film and upper part of bentonite for the
case of GMB were 2.6x10-11 m2/s and 4.4x10-11 m2/s respectively under 50 kPa and
hydraulic head of 0.3m. The difference in transmissivity values reported herein and the
study conducted by Bannour and Touze Foltz (2013) can be attributed to the difference
between transmissivity of GMB and the coating/ attached film to transmissivity
between coating/attached film and upper part of bentonite. When dealing with
transmissivity of multicomponent GCLs, two interface layers should be considered;
first, the interface between the coating and GMB, second, the interface between the
coating and bentonite component of the GCL (Rowe 2016). It is hypothesized that, for
the aligned holes of GMB and geofilm, the transmissivity between the coating and
GCL B
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bentonite component would govern the leakage estimation. Further research is currently
carried out to examine the performance of multicomponent GCLs with
damaged/undamaged geofilm in contact with GMB to assess the interface
transmissivity for geofilm/bentonite and GMB/geofilm. Also the test result reported in
this paper for the coated and laminated GCL in contact with a GMB were slightly lower
but similar to the interface transmissivity for conventional GCLs in contact with GMB
which is usually in range of 2-4x10-11 m2/s. The much lower values reported
AbdelRazek et al. (2016) may be due to the greater bentonite movement that could
occur in those tests with time over the 300 days of those tests.
CONCLUSIONS
The procedure developed for measuring interface transmissivity has performed well
for multicomponent GCLs with an undamaged geofilm placed in contact with HDPE
GMB.
The preliminary interface transmissivity values to water obtained for the coated and
laminated GCLs were both low at 1.2x10-11 m2/s and 1.3x10-11 m2/s, respectively after
43 days of testing at 150 kPa. These values are broadly in line with, or lower than, the
interface transmissivity values of GMB with conventional GCLs. This finding is
subject to further confirmation as the tests continue over longer period of time.
Other factors not considered here that may also potentially affect the interface
transmissivity include the presence of imperfections in the coating, alignment of the
GMB puncture with a coating imperfection, geomembrane roughness, and performance
at low stress levels. More work is needed to fully understand the interactions occurring
at the GMB/GCL interface with time.
ACKNOWLEDGMENTS
The research reported in this paper was supported by a Natural Sciences and
Engineering Research Council of Canada (NSERC) grant (A1007) to Dr. R.K. Rowe.
The equipment used was funded by Canada Foundation for Innovation (CFI) and the
Government of Ontario Ministry of research and Innovation.
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