SlideShare a Scribd company logo
1 of 8
Download to read offline
&EPA
United States
Environmental Protection
Hazardous wssre t:ngmeenno
Research Laboratory
Cincinnati OH 45268
Research and Development EPAI6001S2·88/035 Sept 1989
--------------~------------------
Project Summary
The Electrical Leak Location
Method for Geomembrane
Liners
Glenn T. Darilek and Jorge 0. Parra
An electrical method for locating
leaks in geomembrane liners was
developed and demonstrated lor a
wide variety of applications.
Geomembrane liners are sheets of
elastomerlc material used to prevent
the leakage of waste and to prevent
rainwater from Infiltrating solid waste
landfills and surface Impoundments.
When no leaks are present, a voltage
applied between the material in the
liner and the earth under the liner
produces a relatively uniform
electrical potential distribution in the
material In the liner. Leaks are
located by mapping the anomaly In
the potential distribution caused by
current flowing through a leak. A
computer simulation model of
layered earth sequences above and
below an insulating liner with a leak
was developed to efficiently predict
th~:~ effect of a wide range of
parameters on the leak signature.
Tests on a double·llned physical
model demonstrated the applicability
of the method for a variety of
drainage layers under various test
conditions such as leak size,
electrode depth, and presence of
protective cover soli. Leaks smaller
than 0.8 mm in the primary liner can
be reliably located to within 10 mm.
Lellllks In the bottom liner can be
detected, but not located. The
electrical leak location 111fltthod was
successful In finding a leak In a full·
1u::ale Impoundment that had been
fully tested using the vacuum box
method.
The method was adapted for
locating leaks In the geomembrane
liner of landfill cover systems. Scale
model tests demonstrated the
applicability of the method under a
wide range of cover soil thicknesses
and leak sizes. Special non-
polarizing electrodes were used to
locate leaks as small as 3 mm under
600 mm of cover soil.
This Project Summary was det~el·
oped by EPA's Hazardous Wattte
Engineering Research laboratory.
Cincinnati, OH, to announce key
findings of the research proJect that is
fully documented in a separate report
of the same title (see Project Report
ordering information at back}.
Introduction
The most common method of disposal
of solid and hazardous wastes is m
landfills and surface impoundments. To
prevent contamination. geomembrane
liner systems are often installed beneath
the landfill or impoundment to form an
essentially impermeable barrier that
prevents the migration of contammant
liqu1ds. Installation practices and
operational factors can result in leaks in
the form of punctures or separated
seams. An electncalleak locatton method
was developed to effectively locate ~s
in geomembrane liners to ensure that
liners have been installed ~nd seamed
properly and that no damage t1as oc·
currod
Technical Discussion
F1gure 1 shows the bas1c electncal
leak iocatton method for detectmg and
locat•ng leaks tn a geomembrane hner
The leak !ocai!On method makes use of
the h1gh electncal res1s!tvtty of the
geomemt'lrane l!ner matenal When no
leaks are present. a voltage tmpressed
across the liner produces a relatively
un,form voltage potential dtstnbut1on 111
the matenal above the lmer. If Ihe Imer IS
physically pl'nctured or separated.
conducttve fl•.,ld flows through the leak
establishino a conduct1ve path for current
flow. whtc~; produces an anomaly 1n the
measuzed potenllal 1n the v1C1111ty of the
leak. Therefore. leaks can be located by
measuring the potenllal d1 stn bulion
patterns in the matenal covermg the
liner The electncal leak locatiOn method
can be used in liqu1d Impoundments. as
a pre-service Inspection of sohd ....aste
landfills. and to locate leaks 1n the !mal
cover for landfills or tmpoundments. The
method will not damage the Imer.
Computer Simulation Model
Research Approach
A computer model was developed lo
tnvestigate the pt~rformance capabtlthel:i
of the electrical leak locat1on method.
The model can accommodate vanous
electflcal and dimensional parameters 1n
the three layers compnsmg the ltned
impoundment or landfill The electncal
anomaly of a c~rcular hole m a thm.
Cuffent
Flow lm~s
h•gh!y res•st1ve layer was used to model
the response of a geomembrane lined
Impoundment or la!ldflll contammg a
•iamaged geomembr.:ne liner. The .vaste
matenai, the liner. and the soli under the
liner are simulated by Infinite honzontal
layers. The secondary potential for a leak
10 a geomembrane hner IS in the form of
an mtegral equat.on. which encludes a
three·layer medium Green's funct1on.
Mull1ple c1rcular leaks m the th1n res1stive
liner can also be modeled
To venfy the validity of the modeling
technique. synthetic leak signatures were
computed and compared w1th field data
measured under the same conditions.
The excellent agreement between ex-
panmentat and synthetic model data
verified the accuracy of the general
solution for pred1cllng leak signatures.
Parametric Study
Model studies of the electrical leak
detection survey techmque were made to
charactenze the performance of the
method ' 1der vanous conditions of the
electnc"' elfameters of th'3 waste
matena~ ; ,: measurement electrode
array. 1 :ne .surement dipole depth and
prox1mn~ to the leak. the size and
number of leaks. and the 1mpoundment
depth. F•gure 2 shows a typical family of
leak anomaly responses illustratmg the
effects of vanous measurement depths
for a smgle leak located 1n a liqu1d waste
impoundment. A substantial •mprov9·
ment •n detection sens•tiVIIy is obtained
when the potential array IS closer to the
leak The peak·to·peak anomaly
amplitudes for d1fferent waste layer
2
~'I;
~
::.
~
'II
'5::.
~
~Q
resu>tiv1ty values ware calculated When a
constant current 1s mJected. the leak
detoctab1hty IS mcreasl)d linearly w1th the
reststMty ol the waste m,uenal
Fu~ure 3 shows the peak·!o-peak
anomaly responses ca:culatcd f,Jr vanous
dipole offset d•slances from the loak
center as a funct•on of the survey ht3•ght
above the hnor An Improvement 1n leak
deteclabihty IS observed for survey lmes
located w1thm a rad1us of 10 em from thz
leak Cfsnter when the depth of the c'3·
lector is 1ncroased.
Field data can be acqu•red tn
gaomembrane·liqu1d impoundm ~nts
using either horizontal or vertical d1pole
detectors Figure 4 shows that the
horizoY1tal dipole response is stronger
than the vert1cal dipole response beca1.1se
of the closer proximity of the two
ele':trodes to the plane of the liner.
However. it may be more practical to
make subsurface survey scans using a
vertical dipoie detector rather than a
horizontal d1pole detector With a vertical
dipole. the leak can be more easily and
accurately located because the leak is
located at the peak of the unipolar
response. The honzontal dipole detector
exhibits a bipolar anomaly in which the
Key.
s
h
Pw
Ps
=
=
=
electrode spacing
deptll of the water
res1st1v1ty of the liquid
res1shv1ty of the sorl under the
Imer
a = rad1us of the ieak
Zm = depth of electrodes
x = offset distance !rom the leak
20
.s 2m
16 h 1m Zn 09m
p* 15 O·m
10 p, 300·m
II 00004 m
5 lm- 05m
' .Oi

'I• a
5
10'
.!U
r' 2 4 li S 1!• I? 14 •6 I B lO
H•>tti"''II!H Sran D•sr~;•u·f!! 1r tm•
200
~
160 • 002m
<:{
.:::: x- 0.05 m
c
~
"t; •- 008 m
., 120:::::
"""'
< 0 I m
-;;;
E
:?
~ 02m
<{
... 80
"'"'Cl.
;::
"""'.,Cl.
001 005
Figure 3_
leak loca!lon corresponds w1th the
crossover between tha bipolar leaks
Mu!t,ple leaks can be resoh,ed weth less
amc.qwty when a vert1cal d1pole 1S used
F11Jure 5 shows a typ1cal vert1cal dipole
anomaly response of a leak In !h1s case.
the leak IS d1rectly assocaated w1th the
max1mum anomaly response
The cletec!IOn capab1lltaes for multiple
leaks •n a ane-laned 1m·
poundmen! were analyzed by computmg
leak s1gnatures for two leaks Olienled
radially away !rom the curre11t source
6 shows honzortal d1pole teak
sognatures computed for two survey
Jepths when !he leaks are spaced two
•neter~ apart As expacteC:. when the
honzonlal separat10n between leaks
beo"Jmes less than th•3 honzonlal chrole
spacang. separate resolutaon oi lhe two
i&aks 1s lost When leaks cW'l 1ocatecl at
• 03m
0 I 015 02
H<>1gm Above Lmer h-Z·n (mJ
separat1ons approximating the horizontal
dipGie detector spacmg. the resolution IS
poor However. when measurements are
aCQUired usmg a small d1pole detector
spacmg. the resolution 1s rmproved.
Results of the Computf'r
Simulation Model Study
The denve(~ geomembrane leak
detect1on model 1S an important anl1
SH:Jmf~eant analys1s techmque for leak
locat1on and assessment of damaged
geomembrane lmers. Thts lechmque can
be Implemented as an a1cJ m planmng
surveys and processmg leak survey data
acqu;red 111 lmec1 Impoundments or
landfill!:. The computed leak responses
pomt out the pract1cal 1mportance of
performmg the survey measurements
near the bottom of the 1rr.poundment.
3
h
t Lmer
h 1m
s = 1m
p., 150·m
P• 300·m
a 0.0004 m
0.25 03
The results also mdicate that the
horizontal dipole detector spacmg must
be less than the leak separat1on or a
vert1cal dipole must be used to improve
leak resolution. The Injected current must
be increased to offset the effect of lower
measured leak anomaly attributed to
lower resistivity of the hquid_
Instrumentation for Scale Model
Tests and Full-Scale Field
Evaluations
Instrumentation was assembled to test
the electrical leak locat1on method on
outdoor phys1cal modeis and at full·
scale field 1nstallat1ons. A s1mphfied block
diagram of the electronic components is
shown 1n Figure 7 A transm1tter prov1des
the current needed to generate potentials
•n the impoundment. The rece•ver
200
15(;·
h Tm
p.. 15m
Po 30m
s s. 0.30m
a 0.0004m
h _s[L-~_J__
-~*--+r-- -----:,.----r- h-zm
Leak J I f
~
Liner
"(
'.::::
~
<:;
~
i4; Horizontal Dipole Response
~
Ill
§
1::
"(
...Ill
cf
~
..;.
Ill
cf
Vertical Dipole Response
0.01
Figun~ 4.
Oi.
1m
0.3m
150·m
300·m
0.0004m
0.05 0.1
-- Zm~0.95m
z,.,= 0.9 m
-2' --. ---~-- --·· •.
0 2 4 6 8 10 12 14 16 18 20
Hoflzontal Sctm Dtstance. y (m)
Figun~ 5.
0.15 0.2
Height Above Liner. h-Zm (m}
5r4'
""31~ t
~ 2~
' '~ Tt·
~ I
'k 01
>0 '
.:a _,i
:s f
~-2!
Q, '
rS-Ji
i
--4[
--5'
0
,~_,.-~.,...r-~-.,.---~--· .-.
 ~ •-"0.75m
s
h
)
1
__,  _1_ Zm 05 m
 1),
. l •-"0
2m j ',(1m f ·-1p... ~ 150·m li ·
Ps 300·m V /
00004m ''
v8
a ~
A
• l ' • • J ' • •
2 4 6 8 10 12 14 16 18 20
Horuontal Scan Dtstance. y (m)
Figur11 6.
4
025 03
Transmitter
l
HP Model62098
DC Power Supply
300V 0.1A
To Current
Return
Electrode
To Current
Source Electrode
in Water
Voltege
Sensing
Amplifier
Receiver
Recorded
Data to
Processing
Measurement
Electrodes
Figu,. 7.
Figur• B.
Ill
~
I'/-----~---- t
Current Electrode
measures the rE";>ultant potentials. wh1ch
are then logged by the computer. For
full-scale field surveys. a dual-drum
electric logging winch is equipped with
the logging cable and a nylon rope
drawn through a re!Tiote sheave. The
electrodes are suspended from two floats
to make potential gradient meas-
urements.
Double Liner Model Tests
Background
Double-kneel facilities are required to
meet EPA minimum technology stand-
ards for hazardous waste impoundments.
By placing the current return electrode in
electrical contact with the liquid·
saturated drainage layer located between
the two liners. the electrical leak location
method is applicable for detecting and
locating leaks in the upper liner. Simple
electrical continuity tests between the
drainage layer and the earth can also
determine the existence of a significant
leak in the bottom liner. but not the
location of that leak.
Research Approach
A scale model with dimensions of 3 m
x 3 m was used to test the electrical leak
location method for locating leaks with
various impoundment configurations.
mcluding different types of drainage
layers. various types of leaks, and a
protective soil cover over the primary
liner. An electrode support bar was used
to position the potential electrodes at a
cor-.stant depth as close as possible to
the. liner. Tests were conducted using
vanous electrode materials and geo-
metnes to determine the best and most
practical electrode configurations for
electrical leak location surveys in liquid·
filled impoundm'3nts.
5
Results of Double Uner
Model Tests
Figure 8 is a contour plot of the data
for a leak with a diameter of 5.1 mm with
a drainage layer consisting of a sandy
loam soil layer placed over the geotextile
mat. which is then placed over the
geonet material. The location of the leak
•s clearly indicated by the dipolar contour
pattern. The potential gradient pattern
caused by the current injection electrode
IS also evident in the data. OtMr tests
indicated that a leak with a diameter of 25
mm and a 15-cm slit leak produce
anomaly characteristics very similar to
the leak with a diameter of 5.1 mm.
However. the larger leaks required less
voltage to produce the same anomaly
amplitude.
The characteristic dipolar negative-
to-positive transition of the leak anomaly
was clearly indicated for a leak with a
diameter of 5.1 mm on tests conducted
with a protective soil cover with a
thickness of 15 em placed over the
geomembrane liner. The approximate
location of the leak can be determined
from the contour data. but the dipolar
pattern is weaker.
Figure 9 shows the relative leak
anomaly amplitudes for various elec-
trodes when the centerlines of the
electrodes were scanned directly over
the leak and 15 em offset from the leak.
The sensitivity of the stainless steel and
carbon electrodes was comparable.
When the electrodes were scanned
directly over the leak, the anomaly
amplitudes were inversely related to the
length of the electrodes. However, when
the electrodes were scanned along a line
15 em from the leak. the 30-cm line
electrode produced the largest anomaly.
Most importantly. the leak anomaly was
barely detected when the localized point
electrodes passed within 15 em of the
leak. where the longer electrodes
produced easily detectable anomalies.
Locating Leaks in Cover
Systems
Background
Geomembrane liner material is widely
~sed for landfill final cover systems. An
Impermeable cap is placed over the
hazardous waste to prevent rainwater
from percolating through the waste and
leaching chemicals that could migrate
into groundwater or surface water. The
100-~/~--~--~/~-,r-------------------------------~
Type of
Electrodlf
Figure 9.
-
90- >> :.;:-"' .· / "'
80- >· -·>.J ::_~~-
70- /
Stainless
Steel
Point
Carbon
Point
pH
Electrode
EZa Scan Over Lealc
electrical leak location method was
adapted to make surface soil potential
measurements to locate leaks in final
cover system geomembrane liners.
Polarization noise is caused by electro-
chemical reactions at the interface
between the soil and metal electrodes.
This noise can be reduced to a signif·
icant degree by using half·cell elec-
trodes. These electrodes typically
consist of a plastic tube with a porous
ceramic tip. Electrical contact is made
through a metal electrode in a saturated
salt solution in the half·cell.
Research Approach and Results
Experiments were conducted using a
physical model with dimensions of 5 m x
5 m. Figure 10 is a plot of the measured
leak anomaly for several soil cover
thicknesses. Although the peak-to-
peak amplitude of the anomaly
decreases rapidly with increasing soil
cover. the leak was easily detected for all
of the soil cover depths tested. Tests
were performed with 60 em of soil cover
to show that electrode contact noise is
reduced significantly when the
electrodes are inserted in the ground to a
depth of approximately 25 mm or when
the dry ground surface is scraped off
prior to the measurements.
15-cm 60-cm
Line Line
30-cm Protected
Line 25-cm
Line
IS:::I Scan Offsat t5 em
0
Lealc Dtameter = 3 mm
2 3 4
Distance (Meters}
· 15.2 em Soil 25.4 em Sod
.• 30.5 em Soil - 61 em Sod
Figure 10.
Other Leak Location
Methods for Cover Systems
5
The infrared imaging techmque was
evaluated for detecting subtle
6
temperature differences in the soil cover
related to localized areas of low thermal
conductivity caused by the drainage of
soil moisture through a leak in the
underlying geomembrane. The hypo-
thesis was that during early morning or
1mmediately after sunset. when solar
heating was Introduced or removed, heat
would not be conducted as well in the
slightly drier soil above a large leak in the
geomembrane. which would result in a
detectable temperature difference
associated with the leak. The tests
mdicated that the infrared imaging
technique was not applicable because no
temperature anomalies were detected,
even with only 67 mm of soil cover.
Other methods for detecting leaks in
the geomembrane liner of cover systems.
tncludmg ground-penetrating radar.
tracer gas. the electromagnetic induction
method. encapsulated chem-icals, and
electronic transponders. were analyzed.
Ground-penetrating radar was judged to
offer the highest likelihood of success.
Under suitable conditions, the method
can detect areas of concentrated
mo1sture beneath the geomembrane liner
caused by leaks m the liner. However,
the success of the method depends upon
the soil having only moderate
conductivity and. hence, reasonably low
dissipation of electro-magnetic energy.
Ground-penetrating radar may offer the
additional capability of mapping the
depth of the soil cover and the lateral
extent of the seepage through a leak.
Uner Resistivity Tests
Research Approach
Tests were conducted to measure
electrical resistance changes in liners
over a period of time to determine
whether the electrical resistance of the
liner materials changes after exposure to
waste liquids. thereby reducing the
usefulness of the survey technique. The
tests were performed in triplicate usmg
five different types of liner matenal
exposed to four different liqu1ds. The
liner materials tested included polyv1nyl
chloride. high·density polyethylene. two
thicknesses of chlorosulfonated poly-
ethylene. and chlorinated polyethylene.
The liquids used in the tests included
sodium hydroxide solution, pH of 10;
sulfunc acid solution. pH of 1; sodium
chloride solution, 10 percent by weight;
and deionized water.
Results of Uner Resistivity Tests
The test results indicated that the
measured resistance values were at least
two orders of magnitude higher than tho
resistance needed to allow the practical
application of the electrical leak location
method. The electrical leak detection
technique will not be affected for liner
systems constructed from the materials
tested under exposure to these liquids
Field Demonstration Surveys
Full-scale surveys at the Southwest
Research Institute test 1mpoundment
were performed to detect and locate four
small circular leaks. each 0.79 mm m
diameter. Tho impoundment was filled
with water to a depth of approximately 46
em. The contour plot of the data shown
in Figure 11 graphically indicates the
locations of the four leaks. The contour
plot, together with the potential plots for
each survey line. prov1de a
straightforward means to analyze and
1nterpret the data for leak detect1on and
location purposes.
The electrical leak location method
was demonstrated at another full-scale
Impoundment in the San Anton10. Texas
area. Although the complete liner had
been tested previously using the vacuum
box method, a 2.0-cm long leak was
found. The characteristic leak anomaly
was clearly ev1dent on scan lines as far
away from the leak as 1 5 m. and no
false Indications were obtained
Conclusions and
Recommendations
An electrical method for detecting and
locating leaks in geomembrane liners for
hazardous waste impoundments and
landfills has been developed and
demonstrated successfully in a w1de
variety of applications The protect
demonstrates the validity and usefulness
of the electrical leak location method for
testing the integrity of the geomembrane
for single and double liners and finai
cover systems. The technique is cost
effective for construction quality
assurance and .n-service performance
rnonitoring.
The computer simulation mode! effi-
ciently and accurately predicts the effect
of a w•de range of mea5urement
parameters on the leak s1gnature. The
computer s1mulation model indicates that
leak location sens•tiv;ty IS increased very
sigmficantty when the electrodes are
scanned as close to the liner as posssble.
For a g1ven level of injected current. leak
0 5 10 15
Figure 11.
location sens1tiv1ty .ncreases propor-
tionally w1th the res1sbvrty of the material
on the liner.
Tests on a double-lined model
demonstrated that the method can be
applied to a wide vanety of double liner
conf•gurations of drainage layers with
vanous test parameters such as leak
size, electrode depth. and protectiVe soil
cover. leaks smaller than 0.8 mm in
diameter can be reliably located. leaks
can be detected from distances greater
than 1.5 m from the leak. Linear
electrodes oriented perpendicular to the
scan direction. with scans offset by ap-
proxtmately the length of the electrodes.
produce the highest likelihood of
detecting all leaks compared with
surveys us1ng localized electrodes. The
electncal leak location method is less
senstttve for locatmg leaks in
geomembrane liners with liquid and
protective soil cover over the liner. The
shape and size of the leak have littie
effect upon the shape of thE leak
stgnature However. the leak size affects
the leak current. thereby increas.ng the
amplitude of the leak Stgnature. A simple
conttnwty test can indicatd the presence.
but not locat1on. of leaks '" the bottom
liner.
The electncal leak location method is
also an effective meihod for locatmg
leaks in geomembrane lmers .1f waste
7
20 25 30 35
Meters
impoundment or landfill final cover
systems Non-polarizing half-cell
electrodes were used to greatly reduce
the polarization voltage noise. The
method was very successful in locating
leaks as small as 3 mm under 60 em of
soil cover.
The most promising method studied
for locating leaks in final cover systems,
other than the electrical leak location
method. ss ground-penetrating radar.
limited testing using infrared imaging
was unsuccessful in detecting localized
areas of low thermal conductivity caused
by drainage of soil moisture through a
leak.
laboratory tests indicated that there
was no significant decrease in the
resistivity of typical liner materials during
a 13-week exposure to water. salt water.
ac1d1c solution. and basic solution.
Exposure of these typical liner materials
to these chemicals had no effect on the
applicability of the electrical leak location
method.
The equipment and procedures for
conducting full-scale leak location
surve~ s also can detect leaks with a
dtameter of 0.8 mm up to 1.5 m away
from the leak. A leak was found in an
Impoundment t:1at had been fully tested
ustng the vacuum box method.
The electrical leak location method has
been developed to the stage of industry
use for nonhazardous applications,
including pre-service leak location
surveys for impoundments and landfills
and surveys of nonhazardous in-service
impoundments. Additional development
will bring the method into application for
hazardous material impoundments and
for final cover systems. The electrical
leak location method should be
demonstrated at one or more field
installations for final cover systems and
for a liner with a protective soil cover 10
place. The ground-penetrating radar
technique should be evaluated for
detecting leaks in final cover systems.
Methods should be developed to repair
in-service geomembranes.
Glenn T. Darilel< and Jorge 0. Parra are with the Southwest Research Institute.
San Antonio. TX 78284.
Charles J. Moench, Jr., is the EPA Project Officer (see below).
The complete report. entitled "The Electrical Leak Location Method for Geo-
membrane Liners." (Order No. PB 88-220 496tAS: Cost: S 79.95. subject to
change) will be available only from:
National Technicallnformat1on Service
5285 Port Royal Road
Springfield. VA 22161
Telephone: 703-487-4650
The EPA Project Officer can be contacted at:
Hazardous Waste Engineering Research Laboratory
U.S. Environmental Protection Agency
Cincinnati. OH 45268
United States
Environmental Protection
Agency
Center for Environmental Research
Information
BULK RATE
POSTAGE & FEES PAID
EPACincinnati OH 45268
PERMIT No. G-3:i
Official Business
Penalty for Private Use $300
EPA/600/52-88/035

More Related Content

Similar to Geoelectrica epa

Similar to Geoelectrica epa (20)

Integrated geophysical methods for groundwater exploration in a k
Integrated geophysical methods for groundwater exploration in a kIntegrated geophysical methods for groundwater exploration in a k
Integrated geophysical methods for groundwater exploration in a k
 
Crosshole Seismic Reflection: Coal Mine Fields
Crosshole Seismic Reflection: Coal Mine FieldsCrosshole Seismic Reflection: Coal Mine Fields
Crosshole Seismic Reflection: Coal Mine Fields
 
Lls
Lls Lls
Lls
 
Stm
StmStm
Stm
 
PIPELINE PLANNING WITH AIRBORNE ELECTROMAGNETICS
PIPELINE PLANNING WITH AIRBORNE ELECTROMAGNETICSPIPELINE PLANNING WITH AIRBORNE ELECTROMAGNETICS
PIPELINE PLANNING WITH AIRBORNE ELECTROMAGNETICS
 
Moisture content investigation in the soil samples using microwave dielectric...
Moisture content investigation in the soil samples using microwave dielectric...Moisture content investigation in the soil samples using microwave dielectric...
Moisture content investigation in the soil samples using microwave dielectric...
 
ztautau
ztautauztautau
ztautau
 
Bioinstrumentation research
Bioinstrumentation researchBioinstrumentation research
Bioinstrumentation research
 
PRB_wellock_1999
PRB_wellock_1999PRB_wellock_1999
PRB_wellock_1999
 
Patch clamp recording
Patch clamp recordingPatch clamp recording
Patch clamp recording
 
H021201058064
H021201058064H021201058064
H021201058064
 
The Control on Pollution
The Control on PollutionThe Control on Pollution
The Control on Pollution
 
Stm 07.08.13
Stm 07.08.13Stm 07.08.13
Stm 07.08.13
 
Technical Engineering Memorandum_2015
Technical Engineering Memorandum_2015Technical Engineering Memorandum_2015
Technical Engineering Memorandum_2015
 
Geophysical well logging
Geophysical well loggingGeophysical well logging
Geophysical well logging
 
Publication 2 (2014)
Publication 2 (2014)Publication 2 (2014)
Publication 2 (2014)
 
emitechtalk.pptx
emitechtalk.pptxemitechtalk.pptx
emitechtalk.pptx
 
Final-Thesis-present.pptx
Final-Thesis-present.pptxFinal-Thesis-present.pptx
Final-Thesis-present.pptx
 
KIChE RED Poster 20151021
KIChE RED Poster 20151021KIChE RED Poster 20151021
KIChE RED Poster 20151021
 
OSU_labfinal
OSU_labfinalOSU_labfinal
OSU_labfinal
 

Recently uploaded

Interfacing Analog to Digital Data Converters ee3404.pdf
Interfacing Analog to Digital Data Converters ee3404.pdfInterfacing Analog to Digital Data Converters ee3404.pdf
Interfacing Analog to Digital Data Converters ee3404.pdfragupathi90
 
Maher Othman Interior Design Portfolio..
Maher Othman Interior Design Portfolio..Maher Othman Interior Design Portfolio..
Maher Othman Interior Design Portfolio..MaherOthman7
 
electrical installation and maintenance.
electrical installation and maintenance.electrical installation and maintenance.
electrical installation and maintenance.benjamincojr
 
Artificial intelligence presentation2-171219131633.pdf
Artificial intelligence presentation2-171219131633.pdfArtificial intelligence presentation2-171219131633.pdf
Artificial intelligence presentation2-171219131633.pdfKira Dess
 
Augmented Reality (AR) with Augin Software.pptx
Augmented Reality (AR) with Augin Software.pptxAugmented Reality (AR) with Augin Software.pptx
Augmented Reality (AR) with Augin Software.pptxMustafa Ahmed
 
Fuzzy logic method-based stress detector with blood pressure and body tempera...
Fuzzy logic method-based stress detector with blood pressure and body tempera...Fuzzy logic method-based stress detector with blood pressure and body tempera...
Fuzzy logic method-based stress detector with blood pressure and body tempera...IJECEIAES
 
UNIT 4 PTRP final Convergence in probability.pptx
UNIT 4 PTRP final Convergence in probability.pptxUNIT 4 PTRP final Convergence in probability.pptx
UNIT 4 PTRP final Convergence in probability.pptxkalpana413121
 
litvinenko_Henry_Intrusion_Hong-Kong_2024.pdf
litvinenko_Henry_Intrusion_Hong-Kong_2024.pdflitvinenko_Henry_Intrusion_Hong-Kong_2024.pdf
litvinenko_Henry_Intrusion_Hong-Kong_2024.pdfAlexander Litvinenko
 
Circuit Breakers for Engineering Students
Circuit Breakers for Engineering StudentsCircuit Breakers for Engineering Students
Circuit Breakers for Engineering Studentskannan348865
 
NEWLETTER FRANCE HELICES/ SDS SURFACE DRIVES - MAY 2024
NEWLETTER FRANCE HELICES/ SDS SURFACE DRIVES - MAY 2024NEWLETTER FRANCE HELICES/ SDS SURFACE DRIVES - MAY 2024
NEWLETTER FRANCE HELICES/ SDS SURFACE DRIVES - MAY 2024EMMANUELLEFRANCEHELI
 
SLIDESHARE PPT-DECISION MAKING METHODS.pptx
SLIDESHARE PPT-DECISION MAKING METHODS.pptxSLIDESHARE PPT-DECISION MAKING METHODS.pptx
SLIDESHARE PPT-DECISION MAKING METHODS.pptxCHAIRMAN M
 
handbook on reinforce concrete and detailing
handbook on reinforce concrete and detailinghandbook on reinforce concrete and detailing
handbook on reinforce concrete and detailingAshishSingh1301
 
Adsorption (mass transfer operations 2) ppt
Adsorption (mass transfer operations 2) pptAdsorption (mass transfer operations 2) ppt
Adsorption (mass transfer operations 2) pptjigup7320
 
Tembisa Central Terminating Pills +27838792658 PHOMOLONG Top Abortion Pills F...
Tembisa Central Terminating Pills +27838792658 PHOMOLONG Top Abortion Pills F...Tembisa Central Terminating Pills +27838792658 PHOMOLONG Top Abortion Pills F...
Tembisa Central Terminating Pills +27838792658 PHOMOLONG Top Abortion Pills F...drjose256
 
5G and 6G refer to generations of mobile network technology, each representin...
5G and 6G refer to generations of mobile network technology, each representin...5G and 6G refer to generations of mobile network technology, each representin...
5G and 6G refer to generations of mobile network technology, each representin...archanaece3
 
Seizure stage detection of epileptic seizure using convolutional neural networks
Seizure stage detection of epileptic seizure using convolutional neural networksSeizure stage detection of epileptic seizure using convolutional neural networks
Seizure stage detection of epileptic seizure using convolutional neural networksIJECEIAES
 
Final DBMS Manual (2).pdf final lab manual
Final DBMS Manual (2).pdf final lab manualFinal DBMS Manual (2).pdf final lab manual
Final DBMS Manual (2).pdf final lab manualBalamuruganV28
 
Research Methodolgy & Intellectual Property Rights Series 1
Research Methodolgy & Intellectual Property Rights Series 1Research Methodolgy & Intellectual Property Rights Series 1
Research Methodolgy & Intellectual Property Rights Series 1T.D. Shashikala
 
Diploma Engineering Drawing Qp-2024 Ece .pdf
Diploma Engineering Drawing Qp-2024 Ece .pdfDiploma Engineering Drawing Qp-2024 Ece .pdf
Diploma Engineering Drawing Qp-2024 Ece .pdfJNTUA
 
Artificial Intelligence in due diligence
Artificial Intelligence in due diligenceArtificial Intelligence in due diligence
Artificial Intelligence in due diligencemahaffeycheryld
 

Recently uploaded (20)

Interfacing Analog to Digital Data Converters ee3404.pdf
Interfacing Analog to Digital Data Converters ee3404.pdfInterfacing Analog to Digital Data Converters ee3404.pdf
Interfacing Analog to Digital Data Converters ee3404.pdf
 
Maher Othman Interior Design Portfolio..
Maher Othman Interior Design Portfolio..Maher Othman Interior Design Portfolio..
Maher Othman Interior Design Portfolio..
 
electrical installation and maintenance.
electrical installation and maintenance.electrical installation and maintenance.
electrical installation and maintenance.
 
Artificial intelligence presentation2-171219131633.pdf
Artificial intelligence presentation2-171219131633.pdfArtificial intelligence presentation2-171219131633.pdf
Artificial intelligence presentation2-171219131633.pdf
 
Augmented Reality (AR) with Augin Software.pptx
Augmented Reality (AR) with Augin Software.pptxAugmented Reality (AR) with Augin Software.pptx
Augmented Reality (AR) with Augin Software.pptx
 
Fuzzy logic method-based stress detector with blood pressure and body tempera...
Fuzzy logic method-based stress detector with blood pressure and body tempera...Fuzzy logic method-based stress detector with blood pressure and body tempera...
Fuzzy logic method-based stress detector with blood pressure and body tempera...
 
UNIT 4 PTRP final Convergence in probability.pptx
UNIT 4 PTRP final Convergence in probability.pptxUNIT 4 PTRP final Convergence in probability.pptx
UNIT 4 PTRP final Convergence in probability.pptx
 
litvinenko_Henry_Intrusion_Hong-Kong_2024.pdf
litvinenko_Henry_Intrusion_Hong-Kong_2024.pdflitvinenko_Henry_Intrusion_Hong-Kong_2024.pdf
litvinenko_Henry_Intrusion_Hong-Kong_2024.pdf
 
Circuit Breakers for Engineering Students
Circuit Breakers for Engineering StudentsCircuit Breakers for Engineering Students
Circuit Breakers for Engineering Students
 
NEWLETTER FRANCE HELICES/ SDS SURFACE DRIVES - MAY 2024
NEWLETTER FRANCE HELICES/ SDS SURFACE DRIVES - MAY 2024NEWLETTER FRANCE HELICES/ SDS SURFACE DRIVES - MAY 2024
NEWLETTER FRANCE HELICES/ SDS SURFACE DRIVES - MAY 2024
 
SLIDESHARE PPT-DECISION MAKING METHODS.pptx
SLIDESHARE PPT-DECISION MAKING METHODS.pptxSLIDESHARE PPT-DECISION MAKING METHODS.pptx
SLIDESHARE PPT-DECISION MAKING METHODS.pptx
 
handbook on reinforce concrete and detailing
handbook on reinforce concrete and detailinghandbook on reinforce concrete and detailing
handbook on reinforce concrete and detailing
 
Adsorption (mass transfer operations 2) ppt
Adsorption (mass transfer operations 2) pptAdsorption (mass transfer operations 2) ppt
Adsorption (mass transfer operations 2) ppt
 
Tembisa Central Terminating Pills +27838792658 PHOMOLONG Top Abortion Pills F...
Tembisa Central Terminating Pills +27838792658 PHOMOLONG Top Abortion Pills F...Tembisa Central Terminating Pills +27838792658 PHOMOLONG Top Abortion Pills F...
Tembisa Central Terminating Pills +27838792658 PHOMOLONG Top Abortion Pills F...
 
5G and 6G refer to generations of mobile network technology, each representin...
5G and 6G refer to generations of mobile network technology, each representin...5G and 6G refer to generations of mobile network technology, each representin...
5G and 6G refer to generations of mobile network technology, each representin...
 
Seizure stage detection of epileptic seizure using convolutional neural networks
Seizure stage detection of epileptic seizure using convolutional neural networksSeizure stage detection of epileptic seizure using convolutional neural networks
Seizure stage detection of epileptic seizure using convolutional neural networks
 
Final DBMS Manual (2).pdf final lab manual
Final DBMS Manual (2).pdf final lab manualFinal DBMS Manual (2).pdf final lab manual
Final DBMS Manual (2).pdf final lab manual
 
Research Methodolgy & Intellectual Property Rights Series 1
Research Methodolgy & Intellectual Property Rights Series 1Research Methodolgy & Intellectual Property Rights Series 1
Research Methodolgy & Intellectual Property Rights Series 1
 
Diploma Engineering Drawing Qp-2024 Ece .pdf
Diploma Engineering Drawing Qp-2024 Ece .pdfDiploma Engineering Drawing Qp-2024 Ece .pdf
Diploma Engineering Drawing Qp-2024 Ece .pdf
 
Artificial Intelligence in due diligence
Artificial Intelligence in due diligenceArtificial Intelligence in due diligence
Artificial Intelligence in due diligence
 

Geoelectrica epa

  • 1. &EPA United States Environmental Protection Hazardous wssre t:ngmeenno Research Laboratory Cincinnati OH 45268 Research and Development EPAI6001S2·88/035 Sept 1989 --------------~------------------ Project Summary The Electrical Leak Location Method for Geomembrane Liners Glenn T. Darilek and Jorge 0. Parra An electrical method for locating leaks in geomembrane liners was developed and demonstrated lor a wide variety of applications. Geomembrane liners are sheets of elastomerlc material used to prevent the leakage of waste and to prevent rainwater from Infiltrating solid waste landfills and surface Impoundments. When no leaks are present, a voltage applied between the material in the liner and the earth under the liner produces a relatively uniform electrical potential distribution in the material In the liner. Leaks are located by mapping the anomaly In the potential distribution caused by current flowing through a leak. A computer simulation model of layered earth sequences above and below an insulating liner with a leak was developed to efficiently predict th~:~ effect of a wide range of parameters on the leak signature. Tests on a double·llned physical model demonstrated the applicability of the method for a variety of drainage layers under various test conditions such as leak size, electrode depth, and presence of protective cover soli. Leaks smaller than 0.8 mm in the primary liner can be reliably located to within 10 mm. Lellllks In the bottom liner can be detected, but not located. The electrical leak location 111fltthod was successful In finding a leak In a full· 1u::ale Impoundment that had been fully tested using the vacuum box method. The method was adapted for locating leaks In the geomembrane liner of landfill cover systems. Scale model tests demonstrated the applicability of the method under a wide range of cover soil thicknesses and leak sizes. Special non- polarizing electrodes were used to locate leaks as small as 3 mm under 600 mm of cover soil. This Project Summary was det~el· oped by EPA's Hazardous Wattte Engineering Research laboratory. Cincinnati, OH, to announce key findings of the research proJect that is fully documented in a separate report of the same title (see Project Report ordering information at back}. Introduction The most common method of disposal of solid and hazardous wastes is m landfills and surface impoundments. To prevent contamination. geomembrane liner systems are often installed beneath the landfill or impoundment to form an essentially impermeable barrier that prevents the migration of contammant liqu1ds. Installation practices and operational factors can result in leaks in the form of punctures or separated seams. An electncalleak locatton method was developed to effectively locate ~s in geomembrane liners to ensure that liners have been installed ~nd seamed
  • 2. properly and that no damage t1as oc· currod Technical Discussion F1gure 1 shows the bas1c electncal leak iocatton method for detectmg and locat•ng leaks tn a geomembrane hner The leak !ocai!On method makes use of the h1gh electncal res1s!tvtty of the geomemt'lrane l!ner matenal When no leaks are present. a voltage tmpressed across the liner produces a relatively un,form voltage potential dtstnbut1on 111 the matenal above the lmer. If Ihe Imer IS physically pl'nctured or separated. conducttve fl•.,ld flows through the leak establishino a conduct1ve path for current flow. whtc~; produces an anomaly 1n the measuzed potenllal 1n the v1C1111ty of the leak. Therefore. leaks can be located by measuring the potenllal d1 stn bulion patterns in the matenal covermg the liner The electncal leak locatiOn method can be used in liqu1d Impoundments. as a pre-service Inspection of sohd ....aste landfills. and to locate leaks 1n the !mal cover for landfills or tmpoundments. The method will not damage the Imer. Computer Simulation Model Research Approach A computer model was developed lo tnvestigate the pt~rformance capabtlthel:i of the electrical leak locat1on method. The model can accommodate vanous electflcal and dimensional parameters 1n the three layers compnsmg the ltned impoundment or landfill The electncal anomaly of a c~rcular hole m a thm. Cuffent Flow lm~s h•gh!y res•st1ve layer was used to model the response of a geomembrane lined Impoundment or la!ldflll contammg a •iamaged geomembr.:ne liner. The .vaste matenai, the liner. and the soli under the liner are simulated by Infinite honzontal layers. The secondary potential for a leak 10 a geomembrane hner IS in the form of an mtegral equat.on. which encludes a three·layer medium Green's funct1on. Mull1ple c1rcular leaks m the th1n res1stive liner can also be modeled To venfy the validity of the modeling technique. synthetic leak signatures were computed and compared w1th field data measured under the same conditions. The excellent agreement between ex- panmentat and synthetic model data verified the accuracy of the general solution for pred1cllng leak signatures. Parametric Study Model studies of the electrical leak detection survey techmque were made to charactenze the performance of the method ' 1der vanous conditions of the electnc"' elfameters of th'3 waste matena~ ; ,: measurement electrode array. 1 :ne .surement dipole depth and prox1mn~ to the leak. the size and number of leaks. and the 1mpoundment depth. F•gure 2 shows a typical family of leak anomaly responses illustratmg the effects of vanous measurement depths for a smgle leak located 1n a liqu1d waste impoundment. A substantial •mprov9· ment •n detection sens•tiVIIy is obtained when the potential array IS closer to the leak The peak·to·peak anomaly amplitudes for d1fferent waste layer 2 ~'I; ~ ::. ~ 'II '5::. ~ ~Q resu>tiv1ty values ware calculated When a constant current 1s mJected. the leak detoctab1hty IS mcreasl)d linearly w1th the reststMty ol the waste m,uenal Fu~ure 3 shows the peak·!o-peak anomaly responses ca:culatcd f,Jr vanous dipole offset d•slances from the loak center as a funct•on of the survey ht3•ght above the hnor An Improvement 1n leak deteclabihty IS observed for survey lmes located w1thm a rad1us of 10 em from thz leak Cfsnter when the depth of the c'3· lector is 1ncroased. Field data can be acqu•red tn gaomembrane·liqu1d impoundm ~nts using either horizontal or vertical d1pole detectors Figure 4 shows that the horizoY1tal dipole response is stronger than the vert1cal dipole response beca1.1se of the closer proximity of the two ele':trodes to the plane of the liner. However. it may be more practical to make subsurface survey scans using a vertical dipoie detector rather than a horizontal d1pole detector With a vertical dipole. the leak can be more easily and accurately located because the leak is located at the peak of the unipolar response. The honzontal dipole detector exhibits a bipolar anomaly in which the Key. s h Pw Ps = = = electrode spacing deptll of the water res1st1v1ty of the liquid res1shv1ty of the sorl under the Imer a = rad1us of the ieak Zm = depth of electrodes x = offset distance !rom the leak 20 .s 2m 16 h 1m Zn 09m p* 15 O·m 10 p, 300·m II 00004 m 5 lm- 05m ' .Oi 'I• a 5 10' .!U r' 2 4 li S 1!• I? 14 •6 I B lO H•>tti"''II!H Sran D•sr~;•u·f!! 1r tm•
  • 3. 200 ~ 160 • 002m <:{ .:::: x- 0.05 m c ~ "t; •- 008 m ., 120::::: """' < 0 I m -;;; E :? ~ 02m <{ ... 80 "'"'Cl. ;:: """'.,Cl. 001 005 Figure 3_ leak loca!lon corresponds w1th the crossover between tha bipolar leaks Mu!t,ple leaks can be resoh,ed weth less amc.qwty when a vert1cal d1pole 1S used F11Jure 5 shows a typ1cal vert1cal dipole anomaly response of a leak In !h1s case. the leak IS d1rectly assocaated w1th the max1mum anomaly response The cletec!IOn capab1lltaes for multiple leaks •n a ane-laned 1m· poundmen! were analyzed by computmg leak s1gnatures for two leaks Olienled radially away !rom the curre11t source 6 shows honzortal d1pole teak sognatures computed for two survey Jepths when !he leaks are spaced two •neter~ apart As expacteC:. when the honzonlal separat10n between leaks beo"Jmes less than th•3 honzonlal chrole spacang. separate resolutaon oi lhe two i&aks 1s lost When leaks cW'l 1ocatecl at • 03m 0 I 015 02 H<>1gm Above Lmer h-Z·n (mJ separat1ons approximating the horizontal dipGie detector spacmg. the resolution IS poor However. when measurements are aCQUired usmg a small d1pole detector spacmg. the resolution 1s rmproved. Results of the Computf'r Simulation Model Study The denve(~ geomembrane leak detect1on model 1S an important anl1 SH:Jmf~eant analys1s techmque for leak locat1on and assessment of damaged geomembrane lmers. Thts lechmque can be Implemented as an a1cJ m planmng surveys and processmg leak survey data acqu;red 111 lmec1 Impoundments or landfill!:. The computed leak responses pomt out the pract1cal 1mportance of performmg the survey measurements near the bottom of the 1rr.poundment. 3 h t Lmer h 1m s = 1m p., 150·m P• 300·m a 0.0004 m 0.25 03 The results also mdicate that the horizontal dipole detector spacmg must be less than the leak separat1on or a vert1cal dipole must be used to improve leak resolution. The Injected current must be increased to offset the effect of lower measured leak anomaly attributed to lower resistivity of the hquid_ Instrumentation for Scale Model Tests and Full-Scale Field Evaluations Instrumentation was assembled to test the electrical leak locat1on method on outdoor phys1cal modeis and at full· scale field 1nstallat1ons. A s1mphfied block diagram of the electronic components is shown 1n Figure 7 A transm1tter prov1des the current needed to generate potentials •n the impoundment. The rece•ver
  • 4. 200 15(;· h Tm p.. 15m Po 30m s s. 0.30m a 0.0004m h _s[L-~_J__ -~*--+r-- -----:,.----r- h-zm Leak J I f ~ Liner "( '.:::: ~ <:; ~ i4; Horizontal Dipole Response ~ Ill § 1:: "( ...Ill cf ~ ..;. Ill cf Vertical Dipole Response 0.01 Figun~ 4. Oi. 1m 0.3m 150·m 300·m 0.0004m 0.05 0.1 -- Zm~0.95m z,.,= 0.9 m -2' --. ---~-- --·· •. 0 2 4 6 8 10 12 14 16 18 20 Hoflzontal Sctm Dtstance. y (m) Figun~ 5. 0.15 0.2 Height Above Liner. h-Zm (m} 5r4' ""31~ t ~ 2~ ' '~ Tt· ~ I 'k 01 >0 ' .:a _,i :s f ~-2! Q, ' rS-Ji i --4[ --5' 0 ,~_,.-~.,...r-~-.,.---~--· .-. ~ •-"0.75m s h ) 1 __, _1_ Zm 05 m 1), . l •-"0 2m j ',(1m f ·-1p... ~ 150·m li · Ps 300·m V / 00004m '' v8 a ~ A • l ' • • J ' • • 2 4 6 8 10 12 14 16 18 20 Horuontal Scan Dtstance. y (m) Figur11 6. 4 025 03
  • 5. Transmitter l HP Model62098 DC Power Supply 300V 0.1A To Current Return Electrode To Current Source Electrode in Water Voltege Sensing Amplifier Receiver Recorded Data to Processing Measurement Electrodes Figu,. 7. Figur• B. Ill ~ I'/-----~---- t Current Electrode measures the rE";>ultant potentials. wh1ch are then logged by the computer. For full-scale field surveys. a dual-drum electric logging winch is equipped with the logging cable and a nylon rope drawn through a re!Tiote sheave. The electrodes are suspended from two floats to make potential gradient meas- urements. Double Liner Model Tests Background Double-kneel facilities are required to meet EPA minimum technology stand- ards for hazardous waste impoundments. By placing the current return electrode in electrical contact with the liquid· saturated drainage layer located between the two liners. the electrical leak location method is applicable for detecting and locating leaks in the upper liner. Simple electrical continuity tests between the drainage layer and the earth can also determine the existence of a significant leak in the bottom liner. but not the location of that leak. Research Approach A scale model with dimensions of 3 m x 3 m was used to test the electrical leak location method for locating leaks with various impoundment configurations. mcluding different types of drainage layers. various types of leaks, and a protective soil cover over the primary liner. An electrode support bar was used to position the potential electrodes at a cor-.stant depth as close as possible to the. liner. Tests were conducted using vanous electrode materials and geo- metnes to determine the best and most practical electrode configurations for electrical leak location surveys in liquid· filled impoundm'3nts. 5 Results of Double Uner Model Tests Figure 8 is a contour plot of the data for a leak with a diameter of 5.1 mm with a drainage layer consisting of a sandy loam soil layer placed over the geotextile mat. which is then placed over the geonet material. The location of the leak •s clearly indicated by the dipolar contour pattern. The potential gradient pattern caused by the current injection electrode IS also evident in the data. OtMr tests indicated that a leak with a diameter of 25 mm and a 15-cm slit leak produce anomaly characteristics very similar to the leak with a diameter of 5.1 mm. However. the larger leaks required less voltage to produce the same anomaly amplitude. The characteristic dipolar negative- to-positive transition of the leak anomaly was clearly indicated for a leak with a diameter of 5.1 mm on tests conducted with a protective soil cover with a thickness of 15 em placed over the geomembrane liner. The approximate location of the leak can be determined from the contour data. but the dipolar pattern is weaker. Figure 9 shows the relative leak anomaly amplitudes for various elec- trodes when the centerlines of the electrodes were scanned directly over the leak and 15 em offset from the leak. The sensitivity of the stainless steel and carbon electrodes was comparable. When the electrodes were scanned directly over the leak, the anomaly amplitudes were inversely related to the length of the electrodes. However, when the electrodes were scanned along a line 15 em from the leak. the 30-cm line electrode produced the largest anomaly. Most importantly. the leak anomaly was barely detected when the localized point electrodes passed within 15 em of the leak. where the longer electrodes produced easily detectable anomalies. Locating Leaks in Cover Systems Background Geomembrane liner material is widely ~sed for landfill final cover systems. An Impermeable cap is placed over the hazardous waste to prevent rainwater from percolating through the waste and leaching chemicals that could migrate into groundwater or surface water. The
  • 6. 100-~/~--~--~/~-,r-------------------------------~ Type of Electrodlf Figure 9. - 90- >> :.;:-"' .· / "' 80- >· -·>.J ::_~~- 70- / Stainless Steel Point Carbon Point pH Electrode EZa Scan Over Lealc electrical leak location method was adapted to make surface soil potential measurements to locate leaks in final cover system geomembrane liners. Polarization noise is caused by electro- chemical reactions at the interface between the soil and metal electrodes. This noise can be reduced to a signif· icant degree by using half·cell elec- trodes. These electrodes typically consist of a plastic tube with a porous ceramic tip. Electrical contact is made through a metal electrode in a saturated salt solution in the half·cell. Research Approach and Results Experiments were conducted using a physical model with dimensions of 5 m x 5 m. Figure 10 is a plot of the measured leak anomaly for several soil cover thicknesses. Although the peak-to- peak amplitude of the anomaly decreases rapidly with increasing soil cover. the leak was easily detected for all of the soil cover depths tested. Tests were performed with 60 em of soil cover to show that electrode contact noise is reduced significantly when the electrodes are inserted in the ground to a depth of approximately 25 mm or when the dry ground surface is scraped off prior to the measurements. 15-cm 60-cm Line Line 30-cm Protected Line 25-cm Line IS:::I Scan Offsat t5 em 0 Lealc Dtameter = 3 mm 2 3 4 Distance (Meters} · 15.2 em Soil 25.4 em Sod .• 30.5 em Soil - 61 em Sod Figure 10. Other Leak Location Methods for Cover Systems 5 The infrared imaging techmque was evaluated for detecting subtle 6 temperature differences in the soil cover related to localized areas of low thermal conductivity caused by the drainage of soil moisture through a leak in the underlying geomembrane. The hypo- thesis was that during early morning or 1mmediately after sunset. when solar heating was Introduced or removed, heat would not be conducted as well in the slightly drier soil above a large leak in the geomembrane. which would result in a detectable temperature difference associated with the leak. The tests mdicated that the infrared imaging technique was not applicable because no temperature anomalies were detected, even with only 67 mm of soil cover. Other methods for detecting leaks in the geomembrane liner of cover systems. tncludmg ground-penetrating radar. tracer gas. the electromagnetic induction method. encapsulated chem-icals, and electronic transponders. were analyzed. Ground-penetrating radar was judged to offer the highest likelihood of success. Under suitable conditions, the method can detect areas of concentrated mo1sture beneath the geomembrane liner caused by leaks m the liner. However, the success of the method depends upon the soil having only moderate conductivity and. hence, reasonably low dissipation of electro-magnetic energy. Ground-penetrating radar may offer the additional capability of mapping the depth of the soil cover and the lateral extent of the seepage through a leak. Uner Resistivity Tests Research Approach Tests were conducted to measure electrical resistance changes in liners over a period of time to determine whether the electrical resistance of the liner materials changes after exposure to waste liquids. thereby reducing the usefulness of the survey technique. The tests were performed in triplicate usmg five different types of liner matenal exposed to four different liqu1ds. The liner materials tested included polyv1nyl chloride. high·density polyethylene. two thicknesses of chlorosulfonated poly- ethylene. and chlorinated polyethylene. The liquids used in the tests included sodium hydroxide solution, pH of 10; sulfunc acid solution. pH of 1; sodium chloride solution, 10 percent by weight; and deionized water.
  • 7. Results of Uner Resistivity Tests The test results indicated that the measured resistance values were at least two orders of magnitude higher than tho resistance needed to allow the practical application of the electrical leak location method. The electrical leak detection technique will not be affected for liner systems constructed from the materials tested under exposure to these liquids Field Demonstration Surveys Full-scale surveys at the Southwest Research Institute test 1mpoundment were performed to detect and locate four small circular leaks. each 0.79 mm m diameter. Tho impoundment was filled with water to a depth of approximately 46 em. The contour plot of the data shown in Figure 11 graphically indicates the locations of the four leaks. The contour plot, together with the potential plots for each survey line. prov1de a straightforward means to analyze and 1nterpret the data for leak detect1on and location purposes. The electrical leak location method was demonstrated at another full-scale Impoundment in the San Anton10. Texas area. Although the complete liner had been tested previously using the vacuum box method, a 2.0-cm long leak was found. The characteristic leak anomaly was clearly ev1dent on scan lines as far away from the leak as 1 5 m. and no false Indications were obtained Conclusions and Recommendations An electrical method for detecting and locating leaks in geomembrane liners for hazardous waste impoundments and landfills has been developed and demonstrated successfully in a w1de variety of applications The protect demonstrates the validity and usefulness of the electrical leak location method for testing the integrity of the geomembrane for single and double liners and finai cover systems. The technique is cost effective for construction quality assurance and .n-service performance rnonitoring. The computer simulation mode! effi- ciently and accurately predicts the effect of a w•de range of mea5urement parameters on the leak s1gnature. The computer s1mulation model indicates that leak location sens•tiv;ty IS increased very sigmficantty when the electrodes are scanned as close to the liner as posssble. For a g1ven level of injected current. leak 0 5 10 15 Figure 11. location sens1tiv1ty .ncreases propor- tionally w1th the res1sbvrty of the material on the liner. Tests on a double-lined model demonstrated that the method can be applied to a wide vanety of double liner conf•gurations of drainage layers with vanous test parameters such as leak size, electrode depth. and protectiVe soil cover. leaks smaller than 0.8 mm in diameter can be reliably located. leaks can be detected from distances greater than 1.5 m from the leak. Linear electrodes oriented perpendicular to the scan direction. with scans offset by ap- proxtmately the length of the electrodes. produce the highest likelihood of detecting all leaks compared with surveys us1ng localized electrodes. The electncal leak location method is less senstttve for locatmg leaks in geomembrane liners with liquid and protective soil cover over the liner. The shape and size of the leak have littie effect upon the shape of thE leak stgnature However. the leak size affects the leak current. thereby increas.ng the amplitude of the leak Stgnature. A simple conttnwty test can indicatd the presence. but not locat1on. of leaks '" the bottom liner. The electncal leak location method is also an effective meihod for locatmg leaks in geomembrane lmers .1f waste 7 20 25 30 35 Meters impoundment or landfill final cover systems Non-polarizing half-cell electrodes were used to greatly reduce the polarization voltage noise. The method was very successful in locating leaks as small as 3 mm under 60 em of soil cover. The most promising method studied for locating leaks in final cover systems, other than the electrical leak location method. ss ground-penetrating radar. limited testing using infrared imaging was unsuccessful in detecting localized areas of low thermal conductivity caused by drainage of soil moisture through a leak. laboratory tests indicated that there was no significant decrease in the resistivity of typical liner materials during a 13-week exposure to water. salt water. ac1d1c solution. and basic solution. Exposure of these typical liner materials to these chemicals had no effect on the applicability of the electrical leak location method. The equipment and procedures for conducting full-scale leak location surve~ s also can detect leaks with a dtameter of 0.8 mm up to 1.5 m away from the leak. A leak was found in an Impoundment t:1at had been fully tested ustng the vacuum box method. The electrical leak location method has been developed to the stage of industry
  • 8. use for nonhazardous applications, including pre-service leak location surveys for impoundments and landfills and surveys of nonhazardous in-service impoundments. Additional development will bring the method into application for hazardous material impoundments and for final cover systems. The electrical leak location method should be demonstrated at one or more field installations for final cover systems and for a liner with a protective soil cover 10 place. The ground-penetrating radar technique should be evaluated for detecting leaks in final cover systems. Methods should be developed to repair in-service geomembranes. Glenn T. Darilel< and Jorge 0. Parra are with the Southwest Research Institute. San Antonio. TX 78284. Charles J. Moench, Jr., is the EPA Project Officer (see below). The complete report. entitled "The Electrical Leak Location Method for Geo- membrane Liners." (Order No. PB 88-220 496tAS: Cost: S 79.95. subject to change) will be available only from: National Technicallnformat1on Service 5285 Port Royal Road Springfield. VA 22161 Telephone: 703-487-4650 The EPA Project Officer can be contacted at: Hazardous Waste Engineering Research Laboratory U.S. Environmental Protection Agency Cincinnati. OH 45268 United States Environmental Protection Agency Center for Environmental Research Information BULK RATE POSTAGE & FEES PAID EPACincinnati OH 45268 PERMIT No. G-3:i Official Business Penalty for Private Use $300 EPA/600/52-88/035