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GOVERNMENT OF THE PEOPLE’S REPUBLIC OF BANGLADESH<br />

MINISTRY OF POWER, ENERGY AND MINERAL RESOURCES<br />

ENERGY AND MINERAL RESOURCES DIVISION<br />

GEOLOGICAL SURVEY OF BANGLADESH<br />

153, Pioneer Road, Segunbagicha, Dhaka<br />

Geo-Hazard Risk Reduction in Bangladesh- On Site Training of<br />

Using <strong>GPR</strong> (Ground Penetrating Radar) <strong>for</strong> Turag River Dyke<br />

Monitoring in Bangladesh<br />

Prepared by<br />

Geological Survey of Bangladesh (<strong>GSB</strong>)<br />

&<br />

Norwegian Geotechnical Institute (NGI)<br />

ENVIRONMENTAL GEOLOGY AND NATURAL HAZARDS ASSESMENT BRANCH<br />

March, 2012


Contributors<br />

Contributors from Geological Survey of Bangladesh (<strong>GSB</strong>)<br />

Reshad Md. Ekram Ali, Director & Project Director.<br />

Salma Akter, Deputy Director.<br />

Md. Mahmood Hossain Khan, Assistant Director.<br />

Shahtaj Karim, Assistant Director.<br />

Mohammad Zohir Uddin, Assistant Director.<br />

Contributors from Norwegian Geotechnical Institute (NGI)<br />

Dr. Rajinder Kumar Bhasin<br />

Dr. Lloyd Tunbridge<br />

Dr. Fan-Nian Kong<br />

Mr. Pawel Jankowski


Summary<br />

The Norwegian Geotechnical Institute and the Geological Survey of Bangladesh have<br />

carried out a Ground Penetrating Radar (<strong>GPR</strong>) Survey along a River <strong>dyke</strong> in Dhaka<br />

Bangladesh. The purpose of this survey was to build-up capacity at <strong>GSB</strong> in using advanced<br />

technologies <strong>for</strong> sub-surface geotechnical investigations.<br />

Two different types of (<strong>GPR</strong>) antennas were used to demonstrate the capacity of detecting<br />

sub-surface materials. It was demonstrated that <strong>GPR</strong> can serve as a quick and non<br />

destructive method of testing that can be readily used in Bangladesh <strong>for</strong> detecting subsurface<br />

structures such as weak spots in <strong>dyke</strong>s or rebars in concrete.


Contents<br />

1 Introduction 5<br />

2 Principle of using <strong>GPR</strong> <strong>for</strong> <strong>river</strong> <strong>dyke</strong> monitoring 6<br />

3 NGI <strong>GPR</strong> system 6<br />

4 Test results 8<br />

4.1 Indoor test results 8<br />

4.2 <strong>GPR</strong> tests on <strong>dyke</strong><br />

4.3 <strong>GPR</strong> tests on road 9<br />

5 <strong>GPR</strong> theory revisited: Ground material property, wave speed and propagation<br />

attenuation 17<br />

6 Conclusions 18<br />

Appendices<br />

Appendix A: Wave propagation in ground medium<br />

Appendix B: Application on <strong>GPR</strong> <strong>for</strong> subsurface investigations<br />

Control and review page


1 Introduction<br />

The Geological Survey of Bangladesh (<strong>GSB</strong>) and the Norwegian Geotechnical (NGI)<br />

Institute are co-operating in an institutional co-operation project titled “Geodisaster Risk<br />

Reduction in Bangladesh”. In this project, one of the key Tasks is to build-up capacity at<br />

<strong>GSB</strong> in using advanced geophysical tools <strong>for</strong> investigation of <strong>river</strong> <strong>dyke</strong>s in Dhaka. The main<br />

goal of the project is to reduce the risks from natural hazards in Bangladesh by increasing<br />

the capacity of <strong>GSB</strong> through collaborative pilot project studies.<br />

Ground penetrating Radar is a useful tool <strong>for</strong> geophysical survey, which can be used to<br />

detect locations and extents of weak zone areas of a <strong>river</strong> <strong>dyke</strong>. Hence building up the<br />

ability <strong>for</strong> <strong>GSB</strong> personnel to use <strong>GPR</strong> <strong>for</strong> <strong>river</strong> <strong>dyke</strong> controlling becomes an important topic<br />

of this co-operation project. <strong>GSB</strong> personnel were trained at NGI in Norway July last year<br />

(2010) on how to use the NGI <strong>GPR</strong>. In March 2011 an on site training in Dhaka, Bangladesh<br />

took place.<br />

<strong>GSB</strong> personnel have the background of per<strong>for</strong>ming seismic survey. <strong>GPR</strong> has similar record<br />

as seismic survey. The main difference between <strong>GPR</strong> and seismic methods is that seismic<br />

reflection comes from a boundary where there is an acoustic impedance contrast and in the<br />

case of <strong>GPR</strong> the reflection comes from a boundary where there is a dielectric constant<br />

contrast. So the geoscientists of <strong>GSB</strong> are trying to extrapolate their knowledge from their<br />

training and seismic survey experience to <strong>GPR</strong> because in both cases the data (<strong>GPR</strong> &<br />

seismic) have similar 2D view. However, in seismic reflection method, the depth of<br />

penetration is very large so the geoscientists think about gross lithology but in case of <strong>GPR</strong><br />

they have to think very minutely about the lithology and other variation within a very shallow<br />

depth in the range of 10 m. For any geophysical methods, the detection resolution is a<br />

portion (<strong>for</strong> example, one tenth) of the test distance. There<strong>for</strong>e, <strong>GPR</strong> normally gives<br />

detection results with much higher resolution than the seismic method. The other<br />

advantages of using <strong>GPR</strong> are that <strong>for</strong> detection using electromagnetic wave, the sensors (or<br />

antennas) do not need to have good contact with the ground, which enables a fast survey<br />

speed, and that the <strong>GPR</strong> signal is generated by electronics, and is coherent and repetitive,<br />

which allows to use advanced signal and image processing methods.Figure 1 shows the<br />

<strong>GSB</strong> and NGI team at the office in Dhaka. In this Figure Professor Lars Ottemoller from the<br />

University of Bergen, second from right, is also present to plan the Task related to the<br />

seismic component of the project.<br />

Figure 1: <strong>GSB</strong> – NGI team at the <strong>GSB</strong> office in Dhaka


2 Principle of using <strong>GPR</strong> <strong>for</strong> <strong>river</strong> <strong>dyke</strong> monitoring<br />

The main purpose of on site training is to demonstrate the ability of using <strong>GPR</strong> to identify <strong>for</strong><br />

example, the disturbed and weak zones in the <strong>dyke</strong>, as well as re-bars in the concrete etc.<br />

The weak zones include loosely compacted layers, joints in different ground materials within<br />

the <strong>dyke</strong>s, presence of highly compressive layers, etc.<br />

<strong>GPR</strong> is a non-destructive method that can per<strong>for</strong>m quick surveys on top of a <strong>river</strong> <strong>dyke</strong>. The<br />

conventional <strong>GPR</strong> test mode uses the reflection wave, where two antennas with a fixed<br />

spacing are used, one <strong>for</strong> transmitting and the other <strong>for</strong> receiving signals. They are moved<br />

along the <strong>river</strong> <strong>dyke</strong>. Electromagnetic waves can be transmitted through the ground with the<br />

help of the transmitting antenna. The energy of the wave is reflected back towards the<br />

surface where the electric or magnetic properties change (due to the weak zones etc.) in the<br />

<strong>river</strong> <strong>dyke</strong>. A second antenna receives the reflected wave. The ground materials will<br />

attenuate the radar wave. The detection distance is there<strong>for</strong>e dependent on the types of <strong>river</strong><br />

<strong>dyke</strong> materials. Generally speaking, materials such as concrete, sand, rock, gravel, sandy<br />

soil etc are good materials <strong>for</strong> radar wave to penetrate. However silty clay and wet clay etc<br />

are the difficult materials <strong>for</strong> radar wave to penetrate. For good materials the <strong>GPR</strong> detection<br />

distance can be longer than 10 m.<br />

Even though the detection distance is limited in clay material etc, the <strong>GPR</strong> reflection<br />

measurement on top of the <strong>river</strong> <strong>dyke</strong> is a commonly accepted method used <strong>for</strong> the <strong>dyke</strong><br />

monitoring. This is because <strong>river</strong> <strong>dyke</strong> material changes at shallow distances may imply that<br />

disturbances may take place in the internal part and thus de<strong>for</strong>m the shallow layered<br />

structure.<br />

As mentioned, the <strong>GPR</strong> survey is non-destructive investigation method, as well as being<br />

quick. Survey speed can be as fast as 2-3 km/hour. For an experienced operator, the<br />

interpretation of the survey results can be made on site without further data processing<br />

(inversion etc.). Hence, the <strong>GPR</strong> survey is low cost geotechnical investigation method.<br />

3 NGI <strong>GPR</strong> system<br />

At NGI there has been a continuous activity in developing and testing radars <strong>for</strong> different<br />

subsurface mapping tasks since 1989. The work has included development of hardware and<br />

software <strong>for</strong> data acquisition and algorithms <strong>for</strong> data processing and interpretation. In parallel<br />

with the development work, NGI has carried out more than hundred service jobs, gaining a<br />

lot of practical experience. The NGI Ground Penetrating Radar (<strong>GPR</strong>) employs an Agilent<br />

E5062 network analyser as the transmitter and receiver. It uses step frequency radar<br />

signals instead of the impulse signals that most of the commercial <strong>GPR</strong> use. NGI <strong>GPR</strong> has<br />

been successfully used <strong>for</strong> over 100 field tests in around 20 countries since 1989. The NGI<br />

radar systems have been exported to USA, South Korea, France, Taiwan, Malaysia, India,<br />

Denmark and Bhutan.


Figure 2: <strong>GSB</strong> personnel operating the NGI radar system<br />

The advantages of using a network analyser based <strong>GPR</strong> system are:<br />

The NGI system can work within the frequency band 0.3 MHz to 3000 MHz, which has a<br />

wider bandwidth coverage than most of the commercial <strong>GPR</strong> systems.<br />

The radar signal bandwidth can be adjusted by software at the test site in order to best<br />

match the ground conditions to the antenna resonance frequency. Conventional <strong>GPR</strong><br />

systems, which use impulse signals, need to change hardware to modify radar signals.<br />

The frequency step number can be adjusted by software to make the best use of signal<br />

power <strong>for</strong> target detection under different ground conditions.<br />

The receiver of the NGI system has a higher processing dynamic range than<br />

conventional <strong>GPR</strong> systems.<br />

The NGI system has a perfect frequency response, flat and no-dispersion within the<br />

assigned bandwidth. It is in itself a good tool <strong>for</strong> measuring ground material parameters<br />

and antenna response.<br />

The NGI system makes it simpler to employ frequency-domain signal processing method<br />

such as filtering, deconvolution, Hilbert trans<strong>for</strong>m, etc.<br />

Figure 3: Layout of measuring floor at <strong>GSB</strong> office building where horn antennas of length 10<br />

cm are used


Figure 4: Layout of measuring on Prottasha bridge where a pair of 1.2 m antennas are used<br />

4 Test results<br />

NGI has designed two types of tests <strong>for</strong> this on site training of <strong>GSB</strong> personnel. One is the<br />

indoor test to detect re-bars in the concrete and brick wall etc. The other is the outdoor test<br />

on a <strong>river</strong> <strong>dyke</strong>. In the indoor test, horn (Transmitting & Receiving) antennas of length 10 cm<br />

have been used (see Figure 3). The outdoor tests use two antennas of length 1.2 m: one <strong>for</strong><br />

transmitting the signal and the other <strong>for</strong> receiving the signal. Both antennas are tied with a<br />

rope with 1 m separation between them (see Figure 4).<br />

4.1 Indoor test results<br />

Figure 5 shows the test result obtained while the radar antennas moved on a concrete floor<br />

(Figure 3). A figure like Figure 5 is called as a radargram. The horizontal axis of the figure is<br />

the trace number or the measurement number. In this test we move 2 cm to per<strong>for</strong>m one<br />

measurement. There<strong>for</strong>e in the figure, each horizontal unit is 2 cm. The vertical axis is the<br />

travelling time. In the figure the red arrow points to the time reference corresponding to the<br />

ground surface. The blue arrow points to the time when the reflection from the bottom of the<br />

floor concrete block arrives. The travelling time difference between the reflections from the<br />

ground surface and the bottom of the concrete plate is about t = 2.5 ns. If we assume the<br />

wave speed in the concrete is v =14 cm/ns. The thickness of the concrete block is s = v t/2<br />

= 17.5 cm. According to theory, the reflection from a point target appears as a hyperbolic<br />

curve in a radargram. In the radargram, we find many hyperbolas (yellow arrows in the<br />

figure), which are the reflections from the re-bars inside the concrete floor.


Figure 5: Radargram <strong>for</strong> the test on 6 th floor ground<br />

Figure 6: Radargram <strong>for</strong> the test along a verticalwWall of Reshad’s room.<br />

This radargram in Figure 6 has also been collected by 10cm length antenna. Again we use<br />

the red arrow to represent the time reference corresponding to the ground (wall) surface and<br />

the blue arrow to point the time of the reflection from the other side of the wall. The travelling<br />

time between those two reflections is about 3 ns. Assuming the wave speed 12 cm/ns and<br />

using s = v t/2 , we obtain the wall thickness of 18 cm. Here we have used the typical value<br />

of the wave speed in brick material. The actual wave speed can be obtained by a calibration<br />

test on a known thickness material layer. In Figure 6, we have clearly seen the interface<br />

between two layers of bricks (brown arrow).<br />

4.2 <strong>GPR</strong> tests on <strong>dyke</strong><br />

The project area is located in the North and north-western part of the Dhaka city on Turag<br />

<strong>dyke</strong>.This <strong>dyke</strong> is approximately 30 kilometres of earthen embankment along Tongi khal,


Turag River, and Buriganga River. A total of 11 regulators at the outfall of khals to the<br />

surrounding <strong>river</strong>s along the embankment. One pumping station at the outfall of Kallyanpur<br />

khal to the Turag River, and another one at the outfall of Dholai khal to the Buriganga River.<br />

These pump stations are <strong>for</strong> draining rainwater from parts of Dhaka West. The main goal of<br />

the test project is to detect risk and flood hazards by details <strong>GPR</strong> (Ground Penetration<br />

Radar) survey on Turag-Buriganga <strong>dyke</strong> detecting weak zones due to fracture/cracks,<br />

organic material, and void space etc. in <strong>dyke</strong>. Locations of test survey areas are shown in<br />

figure 7<br />

4.2.1 <strong>GPR</strong> survey on Tongi Dyke<br />

The geoscientists of <strong>GSB</strong> have carried out a <strong>GPR</strong> survey on Tongi Dyke. They have<br />

selected the sluice gate area <strong>for</strong> their survey location. The starting and ending positions of<br />

data acquisition are 23º49′48″N, 90º49′44″E to 23º49′44″N, 90º20′39″E. The main purpose<br />

of this survey is to locate the sluice gate zone with <strong>GPR</strong>. Figure 8 shows a radargram across<br />

the measurement line.<br />

For collecting a radargram in the sluice gate area a pair of 1.2 m length antennas such as<br />

shown in Figure 4 have been used with 1m spacing between receiving and transmitting<br />

antennas.<br />

Figure 7: Location map of 3 test study areas (Sluice Gate, Rostampur and Prottasha Bridge<br />

areas) on the Turag <strong>dyke</strong>s in Dhaka.<br />

In Figure 8 there are four distinct reflections observed in the radargram: the 1 st is the<br />

reflection at the interface between air and layer 1, the 2 nd reflection is at the interface<br />

between layer 1 and layer 2, the third reflection is at the interface between layer 2 and layer<br />

3 and the fourth reflection is at the interface between layer 3 and layer 4.<br />

It is certain from our survey that the uppermost layer (layer 1) represents combine pitch (tar),<br />

brick, brick chips with sand. The layer 2 may represent the pre-existing footpath over which


new pitch road has been made. The third layer may represent compacted soil below the preexisting<br />

footpath. Below the third layer earth fill that is the layer 4 <strong>for</strong>med by silty clay to clay<br />

materials found with slight variation of materials, compactness and wetness.<br />

Each division of the vertical axis is 20 ns representing a depth of 1m with the assumption of<br />

the wave speed 10 cm/ns. So the approximate depth of layers 1, 2 and 3 are about 0.5 m<br />

each. Due to their thinness, it is very hard to differentiate among pitch, brick and brick chips<br />

zone within the uppermost layer (layer 1). Horn antenna or 60cm length antenna may give<br />

good result <strong>for</strong> identification of pitch layer in the uppermost layer.<br />

Figure 8: Radargram Over Mirpur Sluice Gate.<br />

Figure 9: The Sluice gate zone in between yellow mark (Red Circle).


In the radargram shown in Figure 9, two sets of anomaly are found. One is between the<br />

trace number 355 to 380 and the other is in between 320 to 340. The anomaly in the red<br />

circle represents the sluice gate. The lines representing the reflections from the ground<br />

layers suddenly end from both side of red circle indicating the existence of the sluice gate.<br />

The anomaly in between traces 320 to 350 shows a different reflection pattern from the other<br />

one. This discontinuity of signal may be due to the beginning part of the sluice gate<br />

structure.<br />

4.2.2 <strong>GPR</strong> survey on Rostampur area<br />

Figure 10: <strong>GPR</strong> test layout at Rostampur area<br />

A <strong>GPR</strong> Survey was per<strong>for</strong>med in Rostampur Cross <strong>dyke</strong> (23º52′32″ N, 90º21′01″ E) to<br />

identify subsurface lithology (Fig 11) and the test result is shown in Figure 10. In this survey<br />

the 1.2m antenna has been used. Between the traces #1 and #110, three lithological layers<br />

can easily be identified from the radargram. The uppermost unit is mainly composed of brick<br />

chips and silty clay materials with a thickness 0.5m. Below the top layer there is another<br />

layer of thickness 0.5m. The lithology of this layer has not been identified. Below the second<br />

layer the main dam materials silty clay to clay are found. From trace #111 to the end of the<br />

radargram, we can only see two layers.<br />

Figure 11: Test result in Rostampur area.


4.2.3 <strong>GPR</strong> survey on Prottasha bridge and on highway nearby<br />

Figure 12 shows the <strong>GPR</strong> survey at Prottasha Bridge (23º54′21″ N, 90º22′35″ E) using the<br />

1.2 m antenna used in all of the outdoor tests.<br />

Figure 12: <strong>GPR</strong> team in action (test on Prottasha Bridge)<br />

Figure 13: Radargram along connecting road of Prottasha bridge.


Figure 14: Side view of Prottasha bridge and the connecting road<br />

In Figure 13 the uppermost red line represents the response from base of pitch and stone<br />

chips. The 2 nd red line marks the response from base of brick and below this the whole<br />

material might be silty clay.<br />

The area within trace nos. 10-25 marked by the red circle may indicate the junction between<br />

the highway and the bridge connecting road which can be identified by the criss-crossed<br />

nature of the signal. Here, on the sloping side of the highway, new materials have been<br />

dumped <strong>for</strong> the bridge connecting road construction. From trace no. 133-173 the signal<br />

shows a concave nature. The area within this section might be more compacted compared<br />

to its adjacent sides.<br />

Figure 14 shows the side view of the bridge and the connecting road. The measurement is<br />

taken from the right hand side to the left hand side.<br />

Figure 15: Results of <strong>GPR</strong> measurement on the highway beside Prottasha bridge


Figure 15 shows the radargram <strong>for</strong> <strong>GPR</strong> measurement on the highway beside Prottasha<br />

bridge. From this figure one can clearly see that the ground structure of the section between<br />

two yellow lines (trace number 125 to 265) is different to the adjacent sections at both sides.<br />

This is the section when the <strong>GPR</strong> moves close to the bridge connecting road. The red lines<br />

show the reflections from a shallow layer (brick to sand interface?). At trace numbers 30, 85,<br />

330, there may be reflections from pipes or cables under the highway.<br />

Figure 16 shows the working environment when testing on the main dike which is a highway.<br />

Figure 16: <strong>GPR</strong> test on a heavy traffic road connected to Prottasha bridge<br />

4.3 <strong>GPR</strong> tests on road<br />

<strong>GPR</strong> Survey was per<strong>for</strong>med at two places on Tongi-Pubail highway. The first survey was<br />

carried out road on Madhupur clay deposits which fall within 23º56′07″ N to 23º56′06″N<br />

Latitude and 90º28′19″ E to 90º28′19″ E Longitude (Figure 17). The second survey was road<br />

on depression deposit in between 23º54′54″ N to 23º54′51″N Latitude and 90º25′28″ E to<br />

90º25′23″ E Longitude (Figure 19). In this survey, 1.2m antenna has been used. The total<br />

length of survey area was about 203m and 133m respectively.<br />

Figure 17: <strong>GPR</strong> survey, road on Madhupur Clay deposit


Figure 18: Results of <strong>GPR</strong> measurement road on Madhupur Clay deposit<br />

In Figure 18, there are some layerings at the upper part. These layering are due to the<br />

minute variation of Madhupur Clay. There is a channel fill like deposit in between 75 and 45<br />

trace. The depth of the filling materials is about 12feet. The channel is filled by sandy<br />

material which is confirmed by the depth penetration of the radar. There is also a warping<br />

near to the No 10 trace. It seems that the left side of warping push upward compared to the<br />

right side. The left site of the warping is more sandy than the right side. Presence of warping<br />

in the radar gram indicates that the site has effected by neo-tectonic activity.<br />

Figure 19: <strong>GPR</strong> survey, road on depression deposits<br />

Figure 20: Results of <strong>GPR</strong> measurement road on depression deposit


In Figure 20, there is no continuous layering of either sediment or road materials. This may<br />

be due to plastic nature of the underlying sediment. When heavy traffic moves over the road<br />

it initiates a vibration of the underlying materials. Due to its plastic nature (Density lower than<br />

the overlying sediment), it try to move upward (indicated by red arrow) and destroy the<br />

continuous layering of the sediment as well as road materials.<br />

5 <strong>GPR</strong> theory revisited: Ground material property, wave speed and propagation<br />

attenuation<br />

There are two types of the material properties, which have effects on the electromagnetic<br />

wave propagating inside the material. One is the relative dielectric constant ε r, and the other<br />

is the resistivity. Tables 1 and 2 show respectively the dielectric constants εr and the<br />

resistivities R <strong>for</strong> common ground materials.<br />

Table 1: Material dielectric constants<br />

Material Dielectric<br />

Constant εr<br />

Air 1 0.3<br />

Sand 4 0.15<br />

Granite 5 0.13<br />

Sandy soil 6 0.12<br />

Wet clay soil 12 0.09<br />

Fresh water 80 0.03<br />

Table 2: Material resistivities<br />

Wave speed<br />

m/ns<br />

At 100 MHz


In Appendix A, we have derived how the wave speed and propagation attenuation are<br />

related to the ground material properties. According to equation A4 in Apendix A, the wave<br />

velocity can be written<br />

v<br />

2 f<br />

k<br />

real<br />

1<br />

0<br />

r<br />

c<br />

r<br />

where c is the speed of light in air and c = 0.3 m/ns. The list of wave speeds in ground<br />

materials shown in Table 1 is calculated by using the above equation.<br />

A general rule is that <strong>for</strong> detecting deep targets one uses low frequency and long antennas.<br />

Assuming the detection distance is 5 wavelengths and knowing the antenna length is half<br />

wavelength, we obtain that the detection distance is 10 times of the antenna length. The<br />

above empirical relationship can help to choose antenna lengths according to the detection<br />

depth. The resolution is also related to the wavelength used. Here we adapt the criterion that<br />

the detection resolution is ¼ wavelength, i.e., half of the antenna length. Hence our 10 cm<br />

antenna is best suited <strong>for</strong> detection distance 1 m with a resolution 5 cm, while our 1.2 m<br />

antenna is best suited <strong>for</strong> detection distance 12 m with a resolution 60 cm.<br />

6 Conclusions<br />

The tests during this on-site training period show that <strong>GPR</strong> can make quick and continuous<br />

measurements on <strong>river</strong> <strong>dyke</strong> etc. <strong>GPR</strong> can provide high-resolution image of the ground<br />

layering in<strong>for</strong>mation.<br />

Two types of antennas are used <strong>for</strong> measurements, one is 10 cm antenna, and the other is<br />

1.2 m length antenna. It is known that on top of the <strong>dyke</strong> there is 6 cm thick asphalt<br />

carpeting with stone chips. Below the asphalt layer there is 13 cm thick compacted layer of<br />

brick chips mixed with sand (Locals in<strong>for</strong>m maximum thickness of the brick chips layer is<br />

about 40 cm). Below brick chips there is sand. There is no brick soling below the brick chips<br />

layer. <strong>GPR</strong> test using 1.2 m antenna cannot resolve the layers with thickness 6cm and<br />

13cm. However, Figures 3 and 5 show that using 10 cm antennas can detect those layers.<br />

<strong>GPR</strong> can be used to detect the material discontinuities along the measurement direction<br />

(e.g., see Figure 13 and 15). Those discontinuity locations may suggest that the ground is<br />

built by different materials or the ground is de<strong>for</strong>med, and may indicate weak locations of a<br />

<strong>dyke</strong>.


Kontroll- og referanseside/<br />

Review and reference page<br />

Dokumentin<strong>for</strong>masjon/Document in<strong>for</strong>mation<br />

Dokumenttittel/Document title<br />

On site training of using <strong>GPR</strong> (ground penetrating radar) <strong>for</strong> <strong>river</strong><br />

<strong>dyke</strong> monitoring in Bangladesh<br />

Dokumenttype/Type of<br />

document<br />

Rapport/Report<br />

Teknisk notat/Technical<br />

Note Oppdragsgiver/Client<br />

Geological Survey of Bangladesh<br />

Distribusjon/Distribution<br />

Fri/Unlimited<br />

Begrenset/Limited<br />

Ingen/None<br />

Emneord/Keywords<br />

Geophysics, Ground Penetrating Radar, <strong>river</strong> <strong>dyke</strong>s<br />

Stedfesting/Geographical in<strong>for</strong>mation<br />

Land, fylke/Country, County<br />

Bangladesh<br />

Kommune/Municipality<br />

Dhaka<br />

Sted/Location<br />

Dhaka<br />

Kartblad/Map<br />

UTM-koordinater/UTM-coordinates<br />

Dokument nr/Document<br />

No.<br />

20092021-00-6-R<br />

Dato/Date<br />

22 Nov. 2011<br />

Rev.nr./Rev.No.<br />

0<br />

Havområde/Offshore<br />

area<br />

Feltnavn/Field name<br />

Sted/Location<br />

Felt, blokknr./Field,<br />

Block No.<br />

Dokumentkontroll/Document control<br />

Kvalitetssikring i henhold til/Quality assurance according to NS-EN ISO9001<br />

Rev.<br />

/<br />

Rev.<br />

Revisjonsgrunnlag/Reason <strong>for</strong> revision<br />

Egenkontroll<br />

/ Self<br />

review<br />

av/by:<br />

Sideman<br />

ns-<br />

kontroll/<br />

Colleagu<br />

e review<br />

av/by:<br />

0 Original document FK RKB LT<br />

Uavheng<br />

ig<br />

kontroll/<br />

Independ<br />

ent<br />

review<br />

av/by:<br />

Tverrfag<br />

lig<br />

kontroll/<br />

Interdisciplin<br />

ary<br />

review<br />

av/by:<br />

Skj.nr. 043


Kontroll- og referanseside/<br />

Review and reference page<br />

Dokument godkjent <strong>for</strong><br />

utsendelse/<br />

Document approved <strong>for</strong><br />

release<br />

Dato/Date<br />

22/11/2011<br />

Sign. Prosjektleder/Project Manager<br />

Rajinder Bhasin<br />

Skj.nr. 043


Kontroll- og referanseside/<br />

Review and reference page<br />

Skj.nr. 043

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