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Journal of Environment and Earth Science
ISSN 2224-3216 (Paper) ISSN 2225-0948 (Online)
Vol. 3, No.10, 2013

www.iiste.org

Application of Vertical Electrical Sounding and Horizontal
Profiling Methods to Decipher the Existing Subsurface
Stratification in River Segen Dam Site, Tigray, Northern Ethiopia
Abraham Bairu*, Yirgale G/her, Gebrehiwot G/her
Tigray Water Resources Bureau, Mekelle, Tigray, Ethiopia
*E-mail: abrahambairu@ymail.com, AbrahamBairu@gmail.com.
Abstract
The study area Segen river dam site is situated in the southeastern zone of Tigray National Regional State in
between Hintalo Wajirat and Enderta weredas. It is geographically located at 37P between 541400 to 542600
UTME Latitude and 1481600 to 1482600 UTMN Longitude about 35 km southwestern part of Mekelle, the
capital of Tigray National Regional State. The study was conducted having an objective of the geophysical
assessment to provide important subsurface geophysical information useful in evaluating the subsurface
geological formations, geological structures, cavities and others for the dam site under investigation. Ten
Vertical Electical Sounding (VES) points along the two profile lines and a total of two Horizontal Profiling (EP)
with a Wenner electrode array were collected. VES datas were entered to the computer and curves were plotted
using IPI2win interpretation software. EP are entered into the computer and processed using Microsoft Office
Excel and Golden Software Surfer V. 8. The VES results have shown that weak zones at VES 2, VES 3 and VES
4 along profile 1 and at VES 2, VES 3 and VES 5 along profile 2 where the depth goes no more 20 m deep in
both profiles’ pseudo cross section except at VES 4 profile which extends up to 30 m deep. Similarly, the
electrical resistivity profiling results also have shown that the weak zones extend no more than 20 m of depth.
Hence, the result revealed that the investigation requires further core drilling investigations.
Key words: vertical electrical sounding, horizontal profiling, subsurface, goephysical, dam, Segen, Tigray,
Ethiopia
1. INTRODUCTION
The main economic means of Tigray region, located in the northern part of the country is rain fed agriculture.
The rainfall is erratic and unreliable. The topography of the area is undulating. Thus with the traditional
agricultural practices, natural resources are severely degraded due to human interference as well as natural
devastation; the land productivity is declining at alarming rate. As a result, because of moisture limitation and
the above reasons, the region is not in a position to cover the annual food requirement of the people.
To alleviate the challenges of food insecurity in the country, promotion of irrigated agriculture was given priority
in the strategy of the Nations (Mekuria, 2003). According to Abraham et. al. (2005) cited in Nata et. al. (2007),
irrigation is one of the methods used to increase food production in arid and semi-arid regions.
To avert the shortage of water and promote food security, the Ethiopian government has been involved in the
construction of different surface water harvesting structures such as micro-dams, river diversion weirs and ponds
in many parts of the country. In the Tigray National Regional State a number of micro-dams and several
diversion weirs have been built in the last decades. Preliminary studies (Woldearegay, 2001; Mintesinot et al.,
2004) indicate that the constructions of surface water harvesting schemes have economic, hydrological, and
environmental benefits.
Electrical methods namely resistivity were developed in early 1900’s but are more widely used since the 1970’s,
due primarily to the availability of computers to process and analyse the data. Electrical Resistivity techniques
are used extensively in the search for suitable groundwater sources, to monitor types of groundwater pollution, in
engineering surveys to locate sub-surface cavities, faults and fissures, permafrost, etc, in archaeology for
mapping out the area extent of remnants of buried formations of ancient buildings, amongst many other
applications. It is also used extensively in down whole logging (Reynolds, 2000). The electrical resistivity
technique of subsurface materials determines the composition of the overburden and depth to bedrock, and
thickness of sand, gravel or metal deposits or aquifers, detect fault zones, locate steeply dipping contacts
between different Earth materials.
The present study intends to determine the geoelectric parameters (layer resistivity, layer thickness, transverse
resistance and longitudinal conductance), delineate the weak zones, subsurface geological formations, geological
structures, cavities and others.

42
Journal of Environment and Earth Science
ISSN 2224-3216 (Paper) ISSN 2225-0948 (Online)
Vol. 3, No.10, 2013

2.

www.iiste.org

METHODOLOGY

2.1.Location
The Segen river dam site is located about 35Km southwestern part of Mekelle, the capital of Tigray National
Regional State. The dam site is situated between two Weredas of Southeastern Zone of Tigray: the Enderta
Wereda and Hintalo Wajirat. It is geographically located at 37P between 541400 to 542600 UTME Latitude and
1481600 to 1482600 UTMN Longitude. It is accessible through the Mekelle – Samre all seasons gravel pack
road and seasonal rural roads (Figure 1).

Figure 1. Location map of the Segen river dam site

2.2.Data collection and analysis
2.2.1.
Electrical methods
Both Vertical Electrical Sounding (VES) and Electrical Profiling (EP) were conducted following two profile
lines where one is on the proposed dam axis and the other is on the upper stream the dam axis. Profile lines are
aligned in the NE-SW direction.
Vertical electrical sounding (VES) with the commonly used Schlumberger configuration was used for the
purpose of determining the vertical variation of resistivity. The current and potential electrodes are maintained at
the same relative spacing and the whole spread is progressively expanded about a fixed central point (Philip and
Michael, 1984). Four electrodes are placed along a straight line on the Earth surface in the same order, A M N B,
as in the Wenner array but with AB ≥ 5 MN (Figure 2). For any linear symmetric array A M N B of electrodes,
the apparent resistivity (ρa) applying Schlumberger array where AM is the distance on the Earth surface between
the positive current electrode A and the potential electrode M. When two current electrodes A and B are used
and the potential difference (∆V) is measured between two measuring electrodes M and N, the apparent
resistivity can be written in the form:
ρa = π ∆V/I * [ ((AB/2)2 – (MN/2)2 ) / MN ] or ρa = π K ∆V/I…………………..(1)
The value of the apparent resistivity (ρ) depends on the geometry of the electrode array used, as defined by the
geometric factor (K) (Reynolds, 2000).

43
Journal of Environment and Earth Science
ISSN 2224-3216 (Paper) ISSN 2225-0948 (Online)
Vol. 3, No.10, 2013

www.iiste.org

Figure 2. Electrode configurations in Schlumberger array (Mines, 2003)
Electrical profiling (EP) method with Wenner array was used for determining the horizontal or lateral variation
of resistivity. In the Wenner array configuration the spacing between successive electrodes remains constant and
all electrodes are moved for each reading, this method can be more susceptible to near surface and lateral
variations in resistivity and it is sometimes called horizontal electrical profiling (HEP). The four electrodes are
collinear and the separations between adjacent electrodes are equal (a) with M,N in between A, B as shown in
Figure 3 (Parasnis, 1986). The choice of electrode spacing would primarily depend on the depth of the
anomalous resistivity feature (s) to be mapped (Sharma, 1986). The apparent resistivity applying Wenner array
cofiguration can be written in the form:
ρ = 2π a ∆V / I…………………………………………………(2)
Where: ρ is the apparent resistivity, 2πa is the geometric factor (K) and a is the electrode spacing, ∆V is the
potential difference and I is the electric current.

Figure 3. Electrode configurations in Wenner array (Mines, 2003)

44
Journal of Environment and Earth Science
ISSN 2224-3216 (Paper) ISSN 2225-0948 (Online)
Vol. 3, No.10, 2013

www.iiste.org

2.2.2. Data collection
The type of instrument used for the investigation was ABEM Terrameter SAS 4000/SAS 1000 with appropriate
electrodes, cables on reels, and other accessories.
Four electrode Schlumberger array was chosen in the vertical electrical sounding (VES) survey which could
provide better interpretation facility and relatively fast data acquisition mechanism. The vertical electrical
resistivity sounding was carried out on the profile lines which are on and on the upper stream of the dam axis
with the AB/2 and MN/2 spacing ranging from 1.5 – 220m and 0.5 – 45m respectively.Ten VES points were
collected along the two profile lines, five VES points each. The spacing between two successive VES points
VES 1, VES 2, VES 3, VES 4 and VES 5 in the profile 1 was in the order of 175m, 325m, 475m, 663m and
783m respectively from the 0 station at the Teklehaimanot church. While the spacing between two successive
VES points VES 1, VES 2, VES 3, VES 4 and VES 5 in the profile 2 was in the order of 175m, 325m, 475m,
650m and 800m respectively.
A total of two Electrical Profiling (EP) with a Wenner electrode array was conducted. It was done along the two
profile lines, profile 1 and profile 2 with profile length of 960m and 1025m respectively with a=5, 10, 20 and
30m along the proposed dam axis. The horizontal interval or spacing between the two profiles was
approximately 50m.
Table 1. GPS locations of VES points at both profiles
Designation
Along profile 1
Along profile 2
UTME
UTMN
Elevation
UTME
UTMN
Elevation
(m)
(m)
VES 1
542253
1482359
1852
542311
1482336
1852
VES 2
542152
1482252
1830
542215
1482238
1829
VES 3
542044
1482153
1832
542111
1482126
1829
VES 4
541900
1482038
1824
541997
1481998
1825
VES 5
541814
1481964
1839
541876
1481906
1849
Table 2. GPS location of the start and end coordinates of electrical profiling lines
GPS readings
Traverse Start
End
UTME UTMN
Elevation (m) UTME
UTMN
Elevation (m)
Profile 1 542344 1482485 1888
541657
1481829 1913
Profile 2 542402 1482475 1892
541720
1481780 1915

Remark
Each profile line is
approximately 50 m
away

2.3.Data processing
Based on the fundamental principles and methodologies of the geophysical survey, the collected data are
interpreted quantitatively in the case of VES and qualitatively in the case of EP to determine the thickness,
nature and lateral variations of the geological formations which are used to obtain a complete geological picture
of the area. VES data were entered to the computer and curves were plotted using IPI2win interpretation
software.The apparent resistivity and layer thicknesses were converted into useful geological meaning using
knowledge of the geological history and direct geological visual observations. EP survey data are entered into
the computer and processed using Microsoft Office Excel and Golden Software Surfer V. 8 to determine the
lateral variations of the geologic formations.
3.

RESULT AND DISCUSSION

3.1.Vertical electrical sounding (VES)
The VES survey data collected from different locations along the two profile lines are interpreted and presented
graphically with its possible geological meanings and the resistivity value, layer thickness and depth tabulated as
follows.
In terms of resistivity, Igneous rocks such as granite, diorite and gabbro have the highest resistivities while
Sedimentary rocks such as shale and sandstone have a lower resistivity compared to Igneous rocks; this is due to
the high fluid content in them. Metamorphic rocks on the other hand have intermediate but overlapping
resistivities (Felix, 2008)
The resistivity values of the 5 VES points along the profile 1 are stated in such a way that the resistivity values in
the first layer ranges from 12.94 to 106 Ohm-m and the depth ranging from 0.75 to 1.41m. This indicates that the
layer consists of clayey sand and shale formations. The second layer has an apparent resistivity values ranging
from 17.6 to 214 Ohm-m and a range of depth from 2.16 to 2.91m. This layer is weathered and fractured
limestone. The third layer has an apparent resistivity between 7.191 and 86.2 Ohm-m and the range of depth is

45
Journal of Environment and Earth Science
ISSN 2224-3216 (Paper) ISSN 2225-0948 (Online)
Vol. 3, No.10, 2013

www.iiste.org

from 6.237 to 9.18 m. This layer is interpreted as water-tighted weathered and fructured limestone. The fourth
layer has an apparent resistivity between 13 and 406.4Ohm-m and the range of depth is from 17.99 to 18m. This
layer represents fresh limestone (Loke, 1999; Keller and Frischknecht,1966) (Figures 4, 5, 6, 7 and 8).
Similarly, the resistivity values of the 5 VES points along the profile 2 have shown that the resistivity values in
the first layer ranges from 1.06 to 184 Ohm-m and the depth ranging from 0.75 to 2.884m. This indicates that the
layer consists of clay dominant sand associated with cobbles, pebbles and boulder formations. The second layer
has an apparent resistivity values ranging from 15.9 to 378 Ohm-m and a range of depth from 2.16 to 6.7m. This
layer is sand dominated clay associated with cobbles, pebbles and boulder formations. The third layer has an
apparent resistivity between 16.14 and 1434 Ohm-m and the range of depth is from 6.24 to 24.35 m. This layer is
interpreted as fractured limestone intercalated with shale. The fourth layer has an apparent resistivity between
11.7 and 3440 Ohm-m and the range of depth is from 18 to 94.43 m. This layer represents weathered dolerite
(Loke, 1999; Keller and Frischknecht,1966) (Figures 10, 11, 12, 13 and 14).
The pseudo cross section along the profile 1 shows that the weak zones mainly stretches from VES 2 to VES 4
from the surface level to about 5m deep at VES 2 to VES 3 and to about 100m deep at VES 3 to VES 4 (Figure
9). The pseudo cross section along the profile 2 has also shown that weak zones at VES 2 to VES 3 and VES 5.
Vertically under VES 3, there exists a hole-like weak zone which extends approximately from 20 to about 100m
below surface (Figure 15).

Figure 4. VES 1 on the profile 1(RMS = 2.29%)

Figure 5. VES 2 on the profile 1(RMS = 2.42%)

46
Journal of Environment and Earth Science
ISSN 2224-3216 (Paper) ISSN 2225-0948 (Online)
Vol. 3, No.10, 2013

www.iiste.org

Figure 6. VES 3 along the profile 1(RMS = 2.5%)

Figure 7. VES 4 along the profile 1(RMS = 1.85%)

Figure 8. VES 5 along the profile 1(RMS = 2.56%)

47
Journal of Environment and Earth Science
ISSN 2224-3216 (Paper) ISSN 2225-0948 (Online)
Vol. 3, No.10, 2013

www.iiste.org

Figure 9. Pseudo cross-section along the profile 1

Figure 10. VES 1 on profile 2(RMS = 2.27%)

Figure 11. VES 2 on profile 2(RMS = 1.58%)

48
Journal of Environment and Earth Science
ISSN 2224-3216 (Paper) ISSN 2225-0948 (Online)
Vol. 3, No.10, 2013

www.iiste.org

Figure 12. VES 3 on profile 2(RMS = 2.03%)

Figure 13. VES 4 on profile 2(RMS =2.3%)

Figure 14. VES 5 on profile 2(3.65%)

49
Journal of Environment and Earth Science
ISSN 2224-3216 (Paper) ISSN 2225-0948 (Online)
Vol. 3, No.10, 2013

www.iiste.org

Figure 15. Pseudo cross-section along the profile 2
3.2. Electrical profiling (EP)
Electrical profiling (EP) survey was conducted in the area across the Segen river with profile 1 on the proposed
dam axis with profile length of 960m and profile 2 on proposed upper stream of the dam aixs with profile length
of 1025m with sampling intervals of 5m, 10m, 20m and 30m along NE-SW direction The main target of the EP
survey is to identify the relative position and orientation of geological structures and lithologic contacts which
may have an importace for the dam construction.
Electrical profiling contour map plotted for profile 1 at 30m depth (AB/3 = 30m) is characterized by
heterogeneous resistivity. It shows high resistivities ranging from 35 – 120 Ohm-m at both corners of the profile
line. While the resistivity values at the middle of the profile declines from 35 – 10 Ohm-m with the exception of
the resisitivity of the profile line at 300 – 400m from the Teklehaimanot church shows a resistivity value of
greater than 35 Ohm-m. The contour map of the profile 1 shows a “graben-like” borundary between the NE –
SW direction (Figure 16).
The electrical profiling contour map plotted for profile 2 at 30m depth is also charaterized by heterogeneous
resistivity: highest resistivity values at the corners and smallest resistivity values at the middle of the profile line
(Figure 17).
The horizontal or surfacial contour maps plotted between the profile 1 and profile 2 at a = 5m, 10m, 20m and
30m also shows that smallest resistivity values at the middle while the highest values are obtained at the corners
of the profile lines with a “graben-like” structure at the center (Figures 18, 19, 20 and 21).

ZONE 37P
UTME 541657
UTMN 1481829

Depth (in meter) x10

ZONE 37P
UTME 542344
UTMN 1482485
-100

-200

-300
100

200

300

400

500

600

700

800

900

Profile length (in meter)
0

200

400

600

800

Figure 16. Apparent resistivity contour map of EP profile 1 showing the lateral variation

50

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90
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70
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60
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50
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Journal of Environment and Earth Science
ISSN 2224-3216 (Paper) ISSN 2225-0948 (Online)
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ZONE 37P
UTME 541720
UTMN 1481780

Depth (in meter) x10

ZONE 37P
UTME 542402
UTMN 1482475
-100

-200

-300
100

200

300

400

500

600

700

800

900

1000

Profile length ( in meter)
0

200

400

600

800

250
240
230
220
210
200
190
180
170
160
150
140
130
120
110
100
90
80
70
60
50
40
30
20
10
0

Figure 17. Apparent resistivity contour map of EP profile 2 showing the lateral variation

Profile interval (in meter) x10

Profile 1

Profile 2

0

-100

-200

-300

-400

-500
100

200

300

400

500

600

700

800

900

1000

Profile length (in meter)
0
200
400
600
800
Figure 18. Apparent resistivity contour map between EP profile 1 and 2 at 5m depth

51

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240
230
220
210
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10
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Journal of Environment and Earth Science
ISSN 2224-3216 (Paper) ISSN 2225-0948 (Online)
Vol. 3, No.10, 2013

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290

Profile 1

270
0

Profile interval (in meter) x10

250

Profile 2

230
-100
210
190
-200

170
150

-300

130
110

-400

90
70
50

-500
100

200

300

400

500

600

700

800

900

1000

Profile length (in meter)

30
10

0
200
400
600
800
Figure 19. Apparent resistivity contour map between EP profile 1 and 2 at 10m depth

Profile interval (in meter) x10

Profile 1

Profile 2

0

-100

-200

-300

-400

-500
100

200

300

400

500

600

700

800

900

1000

Profile length (in meter)
0
200
400
600
800
Figure 20. Apparent resistivity contour map between EP profile 1 and 2 at 20m depth

52

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260
250
240
230
220
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Journal of Environment and Earth Science
ISSN 2224-3216 (Paper) ISSN 2225-0948 (Online)
Vol. 3, No.10, 2013

Profile interval (in meter) x10

Profile 1

Profile 2

www.iiste.org

0

-100

-200

-300

-400

-500
100

200

300

400

500

600

700

800

900

1000

Profile length (in meter)
0
200
400
600
800
Figure 21. Apparent resistivity contour map between EP profile 1 and 2 at 30m depth

4.

CONCLUSION AND RECOMMENDATIONS
4.1. Conclusion
The vertical electrical resistivity sounding and the electrical resistivity profiling data collected and interpreted
above have shown similar trends which is the resistivity values goes inclining from center of the river bed
towards both abutments/flanks. The VES results have shown that weak zones at VES 2, VES 3 and VES 4 along
profile 1 and at VES 2, VES 3 and VES 5 along profile 2 where the depth goes no more 20 m deep in both
profiles’ pseudo cross section except at VES 4 profile which extends up to 30 m deep. Similarly, the electrical
resistivity profiling results also have shown that the weak zones extend no more than 20 m of depth. This
requires further core drilling investigation before construction is commenced.
4.2. Recommendations
Core drilling should be conducted in the proposed dam axis and upper stream of the dam axis where the VES
and electrical resistivity profiling were conducted. Specifically, through profile 1 at VES 2, VES 3 and VES 4
which are located at 325, 475 and 663 m and through VES 2, VES 3 and VES 5 which are also located at a
distance of 325, 475 and 800 m from the starting point at the Teklehaimanot church.
ACKNOWLEDGEMENTS
We, the authors of this work, would like to express our most grateful and thankful gratitude to Mr. Abdulwhab
Mohammedjemal for his invaluable prompt training in collecting electrical resistivity profiling data using
Wenner array and the highlight on Surfer software and the Tigray Regional National Water Resources
Development field drivers who have always driven us to the field works.
REFERENCES
Felix Onovughe Oghenekohwo (2008). A Comparison of Resistivity and Electromagnetics as Geophysical
Techniques. African Institute for Mathematical Sciences, University of Cape Town, South Africa.
Keller, G.V. and Frischknecht, F.C. (1966). Electrical Methods in Geophysical Prospecting. Pergamon Press,
Oxford, 519 pp.
Loke, M.H. (1999). Electrical imaging surveys for environmental and engineering studies. A practical guide to
2-D and 3-D surveys, Penang, Malaysia, 57 pp.
Mekuria, T. (2003). Small Scale Irrigation for Food Security in Sub – Saharan Africa, Report and
Recommendation of CTA Studies Used, Jan 20 – 29, Ethiopia, www.cta.int/pubs/wd8031.pdf. Accessed
11/09/2008.
Mines. (2003). Colorado School of Mines,(http://www.mines.edu).
Mintesinot B., Kifle W., Lulseged T. (2004). Fighting famine and poverty through water harvesting in northern
Ethiopia. Comprehensive Assessment Bright Spot Final Report. Pp. 63-72.

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ISSN 2224-3216 (Paper) ISSN 2225-0948 (Online)
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Nata, Tadesse and Asmelash, Berhane (2007). Recharging Practices for the enhancement of hand dug wells
discharge in Debre Kidane watershed, North Ethiopia. 4th International Work Shop on Water Management and
Irrigation: Focus on groundwater. Mekelle University, Mekelle, Ethiopia.
Parasnis, D. S. (1986). Principles of Applied Geophysics. Fourth Edition, Chapman and Hall, London.
Philip Kearey and Michael Brooks (1984). An Introduction to Geophysical Exploration. Blackwell, London.
Reynolds, J. M. (2000). An Introduction to Applied and Environmental Geophysics. John Wiley and Sons, Inc.,
New York, USA.
Sharma, P. V. (1986). Geophysical Methods in Geology, Second Edition, Elsevier Science Publishing Co., Inc.,
New York ,USA.
Woldearegay K. (2001). Surface water harvesting and groundwater recharge with implications to conjunctive
water management in arid to semi-arid environments (with the model of the Mekelle area, northern Ethiopia).
Proceedings of the International Conference on Public Management, Policy and Development, June 3-6, 2001,
Addis Ababa.

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Application of vertical electrical sounding and horizontal profiling methods to decipher the existing subsurface stratification

  • 1. Journal of Environment and Earth Science ISSN 2224-3216 (Paper) ISSN 2225-0948 (Online) Vol. 3, No.10, 2013 www.iiste.org Application of Vertical Electrical Sounding and Horizontal Profiling Methods to Decipher the Existing Subsurface Stratification in River Segen Dam Site, Tigray, Northern Ethiopia Abraham Bairu*, Yirgale G/her, Gebrehiwot G/her Tigray Water Resources Bureau, Mekelle, Tigray, Ethiopia *E-mail: abrahambairu@ymail.com, AbrahamBairu@gmail.com. Abstract The study area Segen river dam site is situated in the southeastern zone of Tigray National Regional State in between Hintalo Wajirat and Enderta weredas. It is geographically located at 37P between 541400 to 542600 UTME Latitude and 1481600 to 1482600 UTMN Longitude about 35 km southwestern part of Mekelle, the capital of Tigray National Regional State. The study was conducted having an objective of the geophysical assessment to provide important subsurface geophysical information useful in evaluating the subsurface geological formations, geological structures, cavities and others for the dam site under investigation. Ten Vertical Electical Sounding (VES) points along the two profile lines and a total of two Horizontal Profiling (EP) with a Wenner electrode array were collected. VES datas were entered to the computer and curves were plotted using IPI2win interpretation software. EP are entered into the computer and processed using Microsoft Office Excel and Golden Software Surfer V. 8. The VES results have shown that weak zones at VES 2, VES 3 and VES 4 along profile 1 and at VES 2, VES 3 and VES 5 along profile 2 where the depth goes no more 20 m deep in both profiles’ pseudo cross section except at VES 4 profile which extends up to 30 m deep. Similarly, the electrical resistivity profiling results also have shown that the weak zones extend no more than 20 m of depth. Hence, the result revealed that the investigation requires further core drilling investigations. Key words: vertical electrical sounding, horizontal profiling, subsurface, goephysical, dam, Segen, Tigray, Ethiopia 1. INTRODUCTION The main economic means of Tigray region, located in the northern part of the country is rain fed agriculture. The rainfall is erratic and unreliable. The topography of the area is undulating. Thus with the traditional agricultural practices, natural resources are severely degraded due to human interference as well as natural devastation; the land productivity is declining at alarming rate. As a result, because of moisture limitation and the above reasons, the region is not in a position to cover the annual food requirement of the people. To alleviate the challenges of food insecurity in the country, promotion of irrigated agriculture was given priority in the strategy of the Nations (Mekuria, 2003). According to Abraham et. al. (2005) cited in Nata et. al. (2007), irrigation is one of the methods used to increase food production in arid and semi-arid regions. To avert the shortage of water and promote food security, the Ethiopian government has been involved in the construction of different surface water harvesting structures such as micro-dams, river diversion weirs and ponds in many parts of the country. In the Tigray National Regional State a number of micro-dams and several diversion weirs have been built in the last decades. Preliminary studies (Woldearegay, 2001; Mintesinot et al., 2004) indicate that the constructions of surface water harvesting schemes have economic, hydrological, and environmental benefits. Electrical methods namely resistivity were developed in early 1900’s but are more widely used since the 1970’s, due primarily to the availability of computers to process and analyse the data. Electrical Resistivity techniques are used extensively in the search for suitable groundwater sources, to monitor types of groundwater pollution, in engineering surveys to locate sub-surface cavities, faults and fissures, permafrost, etc, in archaeology for mapping out the area extent of remnants of buried formations of ancient buildings, amongst many other applications. It is also used extensively in down whole logging (Reynolds, 2000). The electrical resistivity technique of subsurface materials determines the composition of the overburden and depth to bedrock, and thickness of sand, gravel or metal deposits or aquifers, detect fault zones, locate steeply dipping contacts between different Earth materials. The present study intends to determine the geoelectric parameters (layer resistivity, layer thickness, transverse resistance and longitudinal conductance), delineate the weak zones, subsurface geological formations, geological structures, cavities and others. 42
  • 2. Journal of Environment and Earth Science ISSN 2224-3216 (Paper) ISSN 2225-0948 (Online) Vol. 3, No.10, 2013 2. www.iiste.org METHODOLOGY 2.1.Location The Segen river dam site is located about 35Km southwestern part of Mekelle, the capital of Tigray National Regional State. The dam site is situated between two Weredas of Southeastern Zone of Tigray: the Enderta Wereda and Hintalo Wajirat. It is geographically located at 37P between 541400 to 542600 UTME Latitude and 1481600 to 1482600 UTMN Longitude. It is accessible through the Mekelle – Samre all seasons gravel pack road and seasonal rural roads (Figure 1). Figure 1. Location map of the Segen river dam site 2.2.Data collection and analysis 2.2.1. Electrical methods Both Vertical Electrical Sounding (VES) and Electrical Profiling (EP) were conducted following two profile lines where one is on the proposed dam axis and the other is on the upper stream the dam axis. Profile lines are aligned in the NE-SW direction. Vertical electrical sounding (VES) with the commonly used Schlumberger configuration was used for the purpose of determining the vertical variation of resistivity. The current and potential electrodes are maintained at the same relative spacing and the whole spread is progressively expanded about a fixed central point (Philip and Michael, 1984). Four electrodes are placed along a straight line on the Earth surface in the same order, A M N B, as in the Wenner array but with AB ≥ 5 MN (Figure 2). For any linear symmetric array A M N B of electrodes, the apparent resistivity (ρa) applying Schlumberger array where AM is the distance on the Earth surface between the positive current electrode A and the potential electrode M. When two current electrodes A and B are used and the potential difference (∆V) is measured between two measuring electrodes M and N, the apparent resistivity can be written in the form: ρa = π ∆V/I * [ ((AB/2)2 – (MN/2)2 ) / MN ] or ρa = π K ∆V/I…………………..(1) The value of the apparent resistivity (ρ) depends on the geometry of the electrode array used, as defined by the geometric factor (K) (Reynolds, 2000). 43
  • 3. Journal of Environment and Earth Science ISSN 2224-3216 (Paper) ISSN 2225-0948 (Online) Vol. 3, No.10, 2013 www.iiste.org Figure 2. Electrode configurations in Schlumberger array (Mines, 2003) Electrical profiling (EP) method with Wenner array was used for determining the horizontal or lateral variation of resistivity. In the Wenner array configuration the spacing between successive electrodes remains constant and all electrodes are moved for each reading, this method can be more susceptible to near surface and lateral variations in resistivity and it is sometimes called horizontal electrical profiling (HEP). The four electrodes are collinear and the separations between adjacent electrodes are equal (a) with M,N in between A, B as shown in Figure 3 (Parasnis, 1986). The choice of electrode spacing would primarily depend on the depth of the anomalous resistivity feature (s) to be mapped (Sharma, 1986). The apparent resistivity applying Wenner array cofiguration can be written in the form: ρ = 2π a ∆V / I…………………………………………………(2) Where: ρ is the apparent resistivity, 2πa is the geometric factor (K) and a is the electrode spacing, ∆V is the potential difference and I is the electric current. Figure 3. Electrode configurations in Wenner array (Mines, 2003) 44
  • 4. Journal of Environment and Earth Science ISSN 2224-3216 (Paper) ISSN 2225-0948 (Online) Vol. 3, No.10, 2013 www.iiste.org 2.2.2. Data collection The type of instrument used for the investigation was ABEM Terrameter SAS 4000/SAS 1000 with appropriate electrodes, cables on reels, and other accessories. Four electrode Schlumberger array was chosen in the vertical electrical sounding (VES) survey which could provide better interpretation facility and relatively fast data acquisition mechanism. The vertical electrical resistivity sounding was carried out on the profile lines which are on and on the upper stream of the dam axis with the AB/2 and MN/2 spacing ranging from 1.5 – 220m and 0.5 – 45m respectively.Ten VES points were collected along the two profile lines, five VES points each. The spacing between two successive VES points VES 1, VES 2, VES 3, VES 4 and VES 5 in the profile 1 was in the order of 175m, 325m, 475m, 663m and 783m respectively from the 0 station at the Teklehaimanot church. While the spacing between two successive VES points VES 1, VES 2, VES 3, VES 4 and VES 5 in the profile 2 was in the order of 175m, 325m, 475m, 650m and 800m respectively. A total of two Electrical Profiling (EP) with a Wenner electrode array was conducted. It was done along the two profile lines, profile 1 and profile 2 with profile length of 960m and 1025m respectively with a=5, 10, 20 and 30m along the proposed dam axis. The horizontal interval or spacing between the two profiles was approximately 50m. Table 1. GPS locations of VES points at both profiles Designation Along profile 1 Along profile 2 UTME UTMN Elevation UTME UTMN Elevation (m) (m) VES 1 542253 1482359 1852 542311 1482336 1852 VES 2 542152 1482252 1830 542215 1482238 1829 VES 3 542044 1482153 1832 542111 1482126 1829 VES 4 541900 1482038 1824 541997 1481998 1825 VES 5 541814 1481964 1839 541876 1481906 1849 Table 2. GPS location of the start and end coordinates of electrical profiling lines GPS readings Traverse Start End UTME UTMN Elevation (m) UTME UTMN Elevation (m) Profile 1 542344 1482485 1888 541657 1481829 1913 Profile 2 542402 1482475 1892 541720 1481780 1915 Remark Each profile line is approximately 50 m away 2.3.Data processing Based on the fundamental principles and methodologies of the geophysical survey, the collected data are interpreted quantitatively in the case of VES and qualitatively in the case of EP to determine the thickness, nature and lateral variations of the geological formations which are used to obtain a complete geological picture of the area. VES data were entered to the computer and curves were plotted using IPI2win interpretation software.The apparent resistivity and layer thicknesses were converted into useful geological meaning using knowledge of the geological history and direct geological visual observations. EP survey data are entered into the computer and processed using Microsoft Office Excel and Golden Software Surfer V. 8 to determine the lateral variations of the geologic formations. 3. RESULT AND DISCUSSION 3.1.Vertical electrical sounding (VES) The VES survey data collected from different locations along the two profile lines are interpreted and presented graphically with its possible geological meanings and the resistivity value, layer thickness and depth tabulated as follows. In terms of resistivity, Igneous rocks such as granite, diorite and gabbro have the highest resistivities while Sedimentary rocks such as shale and sandstone have a lower resistivity compared to Igneous rocks; this is due to the high fluid content in them. Metamorphic rocks on the other hand have intermediate but overlapping resistivities (Felix, 2008) The resistivity values of the 5 VES points along the profile 1 are stated in such a way that the resistivity values in the first layer ranges from 12.94 to 106 Ohm-m and the depth ranging from 0.75 to 1.41m. This indicates that the layer consists of clayey sand and shale formations. The second layer has an apparent resistivity values ranging from 17.6 to 214 Ohm-m and a range of depth from 2.16 to 2.91m. This layer is weathered and fractured limestone. The third layer has an apparent resistivity between 7.191 and 86.2 Ohm-m and the range of depth is 45
  • 5. Journal of Environment and Earth Science ISSN 2224-3216 (Paper) ISSN 2225-0948 (Online) Vol. 3, No.10, 2013 www.iiste.org from 6.237 to 9.18 m. This layer is interpreted as water-tighted weathered and fructured limestone. The fourth layer has an apparent resistivity between 13 and 406.4Ohm-m and the range of depth is from 17.99 to 18m. This layer represents fresh limestone (Loke, 1999; Keller and Frischknecht,1966) (Figures 4, 5, 6, 7 and 8). Similarly, the resistivity values of the 5 VES points along the profile 2 have shown that the resistivity values in the first layer ranges from 1.06 to 184 Ohm-m and the depth ranging from 0.75 to 2.884m. This indicates that the layer consists of clay dominant sand associated with cobbles, pebbles and boulder formations. The second layer has an apparent resistivity values ranging from 15.9 to 378 Ohm-m and a range of depth from 2.16 to 6.7m. This layer is sand dominated clay associated with cobbles, pebbles and boulder formations. The third layer has an apparent resistivity between 16.14 and 1434 Ohm-m and the range of depth is from 6.24 to 24.35 m. This layer is interpreted as fractured limestone intercalated with shale. The fourth layer has an apparent resistivity between 11.7 and 3440 Ohm-m and the range of depth is from 18 to 94.43 m. This layer represents weathered dolerite (Loke, 1999; Keller and Frischknecht,1966) (Figures 10, 11, 12, 13 and 14). The pseudo cross section along the profile 1 shows that the weak zones mainly stretches from VES 2 to VES 4 from the surface level to about 5m deep at VES 2 to VES 3 and to about 100m deep at VES 3 to VES 4 (Figure 9). The pseudo cross section along the profile 2 has also shown that weak zones at VES 2 to VES 3 and VES 5. Vertically under VES 3, there exists a hole-like weak zone which extends approximately from 20 to about 100m below surface (Figure 15). Figure 4. VES 1 on the profile 1(RMS = 2.29%) Figure 5. VES 2 on the profile 1(RMS = 2.42%) 46
  • 6. Journal of Environment and Earth Science ISSN 2224-3216 (Paper) ISSN 2225-0948 (Online) Vol. 3, No.10, 2013 www.iiste.org Figure 6. VES 3 along the profile 1(RMS = 2.5%) Figure 7. VES 4 along the profile 1(RMS = 1.85%) Figure 8. VES 5 along the profile 1(RMS = 2.56%) 47
  • 7. Journal of Environment and Earth Science ISSN 2224-3216 (Paper) ISSN 2225-0948 (Online) Vol. 3, No.10, 2013 www.iiste.org Figure 9. Pseudo cross-section along the profile 1 Figure 10. VES 1 on profile 2(RMS = 2.27%) Figure 11. VES 2 on profile 2(RMS = 1.58%) 48
  • 8. Journal of Environment and Earth Science ISSN 2224-3216 (Paper) ISSN 2225-0948 (Online) Vol. 3, No.10, 2013 www.iiste.org Figure 12. VES 3 on profile 2(RMS = 2.03%) Figure 13. VES 4 on profile 2(RMS =2.3%) Figure 14. VES 5 on profile 2(3.65%) 49
  • 9. Journal of Environment and Earth Science ISSN 2224-3216 (Paper) ISSN 2225-0948 (Online) Vol. 3, No.10, 2013 www.iiste.org Figure 15. Pseudo cross-section along the profile 2 3.2. Electrical profiling (EP) Electrical profiling (EP) survey was conducted in the area across the Segen river with profile 1 on the proposed dam axis with profile length of 960m and profile 2 on proposed upper stream of the dam aixs with profile length of 1025m with sampling intervals of 5m, 10m, 20m and 30m along NE-SW direction The main target of the EP survey is to identify the relative position and orientation of geological structures and lithologic contacts which may have an importace for the dam construction. Electrical profiling contour map plotted for profile 1 at 30m depth (AB/3 = 30m) is characterized by heterogeneous resistivity. It shows high resistivities ranging from 35 – 120 Ohm-m at both corners of the profile line. While the resistivity values at the middle of the profile declines from 35 – 10 Ohm-m with the exception of the resisitivity of the profile line at 300 – 400m from the Teklehaimanot church shows a resistivity value of greater than 35 Ohm-m. The contour map of the profile 1 shows a “graben-like” borundary between the NE – SW direction (Figure 16). The electrical profiling contour map plotted for profile 2 at 30m depth is also charaterized by heterogeneous resistivity: highest resistivity values at the corners and smallest resistivity values at the middle of the profile line (Figure 17). The horizontal or surfacial contour maps plotted between the profile 1 and profile 2 at a = 5m, 10m, 20m and 30m also shows that smallest resistivity values at the middle while the highest values are obtained at the corners of the profile lines with a “graben-like” structure at the center (Figures 18, 19, 20 and 21). ZONE 37P UTME 541657 UTMN 1481829 Depth (in meter) x10 ZONE 37P UTME 542344 UTMN 1482485 -100 -200 -300 100 200 300 400 500 600 700 800 900 Profile length (in meter) 0 200 400 600 800 Figure 16. Apparent resistivity contour map of EP profile 1 showing the lateral variation 50 120 115 110 105 100 95 90 85 80 75 70 65 60 55 50 45 40 35 30 25 20 15 10
  • 10. Journal of Environment and Earth Science ISSN 2224-3216 (Paper) ISSN 2225-0948 (Online) Vol. 3, No.10, 2013 www.iiste.org ZONE 37P UTME 541720 UTMN 1481780 Depth (in meter) x10 ZONE 37P UTME 542402 UTMN 1482475 -100 -200 -300 100 200 300 400 500 600 700 800 900 1000 Profile length ( in meter) 0 200 400 600 800 250 240 230 220 210 200 190 180 170 160 150 140 130 120 110 100 90 80 70 60 50 40 30 20 10 0 Figure 17. Apparent resistivity contour map of EP profile 2 showing the lateral variation Profile interval (in meter) x10 Profile 1 Profile 2 0 -100 -200 -300 -400 -500 100 200 300 400 500 600 700 800 900 1000 Profile length (in meter) 0 200 400 600 800 Figure 18. Apparent resistivity contour map between EP profile 1 and 2 at 5m depth 51 250 240 230 220 210 200 190 180 170 160 150 140 130 120 110 100 90 80 70 60 50 40 30 20 10 0
  • 11. Journal of Environment and Earth Science ISSN 2224-3216 (Paper) ISSN 2225-0948 (Online) Vol. 3, No.10, 2013 www.iiste.org 290 Profile 1 270 0 Profile interval (in meter) x10 250 Profile 2 230 -100 210 190 -200 170 150 -300 130 110 -400 90 70 50 -500 100 200 300 400 500 600 700 800 900 1000 Profile length (in meter) 30 10 0 200 400 600 800 Figure 19. Apparent resistivity contour map between EP profile 1 and 2 at 10m depth Profile interval (in meter) x10 Profile 1 Profile 2 0 -100 -200 -300 -400 -500 100 200 300 400 500 600 700 800 900 1000 Profile length (in meter) 0 200 400 600 800 Figure 20. Apparent resistivity contour map between EP profile 1 and 2 at 20m depth 52 270 260 250 240 230 220 210 200 190 180 170 160 150 140 130 120 110 100 90 80 70 60 50 40 30 20 10
  • 12. Journal of Environment and Earth Science ISSN 2224-3216 (Paper) ISSN 2225-0948 (Online) Vol. 3, No.10, 2013 Profile interval (in meter) x10 Profile 1 Profile 2 www.iiste.org 0 -100 -200 -300 -400 -500 100 200 300 400 500 600 700 800 900 1000 Profile length (in meter) 0 200 400 600 800 Figure 21. Apparent resistivity contour map between EP profile 1 and 2 at 30m depth 4. CONCLUSION AND RECOMMENDATIONS 4.1. Conclusion The vertical electrical resistivity sounding and the electrical resistivity profiling data collected and interpreted above have shown similar trends which is the resistivity values goes inclining from center of the river bed towards both abutments/flanks. The VES results have shown that weak zones at VES 2, VES 3 and VES 4 along profile 1 and at VES 2, VES 3 and VES 5 along profile 2 where the depth goes no more 20 m deep in both profiles’ pseudo cross section except at VES 4 profile which extends up to 30 m deep. Similarly, the electrical resistivity profiling results also have shown that the weak zones extend no more than 20 m of depth. This requires further core drilling investigation before construction is commenced. 4.2. Recommendations Core drilling should be conducted in the proposed dam axis and upper stream of the dam axis where the VES and electrical resistivity profiling were conducted. Specifically, through profile 1 at VES 2, VES 3 and VES 4 which are located at 325, 475 and 663 m and through VES 2, VES 3 and VES 5 which are also located at a distance of 325, 475 and 800 m from the starting point at the Teklehaimanot church. ACKNOWLEDGEMENTS We, the authors of this work, would like to express our most grateful and thankful gratitude to Mr. Abdulwhab Mohammedjemal for his invaluable prompt training in collecting electrical resistivity profiling data using Wenner array and the highlight on Surfer software and the Tigray Regional National Water Resources Development field drivers who have always driven us to the field works. REFERENCES Felix Onovughe Oghenekohwo (2008). A Comparison of Resistivity and Electromagnetics as Geophysical Techniques. African Institute for Mathematical Sciences, University of Cape Town, South Africa. Keller, G.V. and Frischknecht, F.C. (1966). Electrical Methods in Geophysical Prospecting. Pergamon Press, Oxford, 519 pp. Loke, M.H. (1999). Electrical imaging surveys for environmental and engineering studies. A practical guide to 2-D and 3-D surveys, Penang, Malaysia, 57 pp. Mekuria, T. (2003). Small Scale Irrigation for Food Security in Sub – Saharan Africa, Report and Recommendation of CTA Studies Used, Jan 20 – 29, Ethiopia, www.cta.int/pubs/wd8031.pdf. Accessed 11/09/2008. Mines. (2003). Colorado School of Mines,(http://www.mines.edu). Mintesinot B., Kifle W., Lulseged T. (2004). Fighting famine and poverty through water harvesting in northern Ethiopia. Comprehensive Assessment Bright Spot Final Report. Pp. 63-72. 53 140 135 130 125 120 115 110 105 100 95 90 85 80 75 70 65 60 55 50 45 40 35 30 25 20 15
  • 13. Journal of Environment and Earth Science ISSN 2224-3216 (Paper) ISSN 2225-0948 (Online) Vol. 3, No.10, 2013 www.iiste.org Nata, Tadesse and Asmelash, Berhane (2007). Recharging Practices for the enhancement of hand dug wells discharge in Debre Kidane watershed, North Ethiopia. 4th International Work Shop on Water Management and Irrigation: Focus on groundwater. Mekelle University, Mekelle, Ethiopia. Parasnis, D. S. (1986). Principles of Applied Geophysics. Fourth Edition, Chapman and Hall, London. Philip Kearey and Michael Brooks (1984). An Introduction to Geophysical Exploration. Blackwell, London. Reynolds, J. M. (2000). An Introduction to Applied and Environmental Geophysics. John Wiley and Sons, Inc., New York, USA. Sharma, P. V. (1986). Geophysical Methods in Geology, Second Edition, Elsevier Science Publishing Co., Inc., New York ,USA. Woldearegay K. (2001). Surface water harvesting and groundwater recharge with implications to conjunctive water management in arid to semi-arid environments (with the model of the Mekelle area, northern Ethiopia). Proceedings of the International Conference on Public Management, Policy and Development, June 3-6, 2001, Addis Ababa. 54
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