International Journal of Geosciences
Vol.4 No.1(2013), Article ID:27027,8 pages DOI:10.4236/ijg.2013.41011

Preliminary Geophysical Investigation to Delineate the Groundwater Conductive Zones in the Coastal Region of Akwa Ibom State, Southern Nigeria, around the Gulf of Guinea

George N. Jimmy1*, Akpan A. Otu2, Umoh A. Asuquo3

1Department of Physics, Akwa Ibom State University, Akwa Ibom, Nigeria

2Department of Physics, University of Calaber, Calaber, Nigeria

3Department of Physics, University of Uyo, Uyo, Nigeria

Email: *nyaknojimmyg@yahoo.com

Received October 9, 2012; revised November 12, 2012; accepted December 13, 2012

Keywords: Freshwater; Saltwater; Ferruginized and Saline Sands; VES

ABSTRACT

This paper presents the first work of its kind within the confines of the study area. It unravels the distribution of the layers of conductive sand and their depths of interaction between freshwater from fresh sands and saltwater within the conductive layers in the coastal region of Akwa Ibom State (Nigeria) around the Gulf of Guinea. Vertical electrical sounding (VES) data whose fidelity was achieved by constraining the data by the available nearby logged borehole information during interpretation was the method applied. In the western region of the study area, the ferruginized and saline water layer is found within the depth range of 22 to 75 m deep. In the northern zone, conductive sandy layer is found within 50 to 210 m and in the eastern zone, the saline and ferruginized sandy layer is found within the depth of 88.5 m and above. Generally, the horizontal and vertical cross sections of the subsoil and the flow regime from water table depths have been delineated. With these information, water can be tapped in the area with caution and the flow direction determined can be used as input parameter in detailed contamination study.

1. Introduction

One of the major challenges faced by the communities within the coastal regions of any nation is the encroachment of seawater into the coastal aquifers due partly to excessive abstraction of groundwater in the coastal area. Salinity of water bearing units may also be due to infiltration of polluted water into the pervious and semi pervious geological formations that host the groundwater [1-4]. Groundwater sustains the flow of coastal streams and rivers and is a source of fresh water to coastal ponds, wetlands and other coastal ecosystem.

In the study area, when water is pumped in some boreholes, it is found to be hard, oily and rusty if allowed to stay in a container for sometimes. This observation provoked the decision to embark on this study to see the lithologic arrangements of water bearing formation and their depth of burial. The observation is viewed as a result of influx of conductive water from conductive sand into the borehole after some period of pumping or influx of ferruginized and saline water either from the river or permeable layer of paleowater aquifer into the over pumped borehole screen surrounding. This problem which is natural can be carefully mitigated by locating the screen in water bearing units away from the scientifically screened layer of conductive or ferruginized sandy layer. This layer can be identified through geophysical investigation applying electrical or electromagnetic method [5,6]. Generally, since conductive layers are interwoven with non conductive and pervious layers, it is believed that the recharge zones located at topographically high region can be one of the possible sources of the conductive water collected in impervious or semi-impervious layers within the subsurface. Hence, borehole screens stationed in the conductive aquifer will continue to yield water that is conductive.

2. Location and Geology

The study area cuts across Eastern Obolo, Onna, Eket and Ibeno Local Government Areas (Figure 1(a)) within the coastal region of Akwa Ibom State (Figure 1(b)).

The area falls within longitudes 7.301 to 8.201E and latitudes 4.301 to 5.301N in Nigeria (Figure 1(c)) around the Gulf of Guinea. The area has over 200 mm of rainfall per annum. Mean annual potential evaporation is about 4.6 mm/day and relative humidity is in the range of 60% to 90% [7]. The area is generally flat and lies within the beach dunes and large valleys. It is characterized by mangrove swamps, tidal creeks and brackish lagoons. The area is subjected to constant inundation by saline and brackish water. Geologically, the study area has major lithologic formations which include the Miocene Akata Formation (shales, intercalated sands and silstone), Miocene Pliocene Agbada Formation (sands and sandstones, intercalated with shales) and the Pliocene Benin Formation (coarse-grained, gravelly sands with minor intercalation of clays and shales). The middle and the upper sand units [7] of the Benin Formation form the major aquiferous units in the area. The part of the Tertiary Niger Delta in which the Study area falls is a large arcuate basin of wave-dominated type. It is characterized with little or no igneous intrusion and insignificant outward evidence of plate tectonics. The subsurface lithologic and geologic conditions are symptomatic of the marine depositional environments within the study area. This depositional pattern gives rise to the various rock units which are fresh at some depths and conductive at some other depths.

3. Material and Method

The geophysical screening of the subsurface that led to the discrimination of the lithologic units was performed using the Vertical electrical sounding (VES) method employing the Schlumberger electrode configuration (Figure 2) in three profiles (Figure 1(a)) with average distance of 100 m between VES points [8-12]. The minimum and maximum potential and current electrode separations were 0.5, 50 m (i.e. 0.25 - 25.00 m of half of MN) and 2.00 m, 1000 m (i.e. 1.00 - 500 m of half of

Figure 1. Location maps showing (a) Study area and VES transects; (b) Study area in Akwa Ibom State and (c) Location of Akwa Ibom State in Nigeria.

Figure 2. The Schlumberger electrode configuration used in the study area.

AB) respectively. With the aid of ABEM Terrameter SAS 4000 and its accessories, the apparent resistivity (ρa) was measured in twelve locations using Equation (1)

(1)

The equation is simplified as in Equation (2)

(2)

where the geometric factor

;

AB and MN are the current and potential electrode separations respectively and R is the measured resistance. This was done by measuring the earth’s resistance through the effect of injected current sent into the ground. The measured R was multiplied by the geometric factor k, determined by the electrode configuration. The coordinates of the locations were taken using the Global Positioning System (GPS). The processing of apparent resistivity values was done using Resist Software. The software employs the principle of inversion with the help of a well-known Resistivity Transform. The backward different formula was used for the analysis. This led to the determination of the model representative curves in Figures 3(a)-(e). The represented curves shown in the figures were chosen on the basis proximity to borehole locations. From the curves, the water table (saturated top layer), depth, thickness and resistivity were determined [13,14-16].The depth, thickness and resistivity values of each layer were predetermined by the software.

(a)(b)(c)(d)(e)

Figure 3. (a) VES curve at VES1; (b) VES curve at VES3; (c) VES curve at VES5; (d) VES curve at VES7; (e) VES curve at VES12.

4. Results and Discussion

The determined water tables from VES interpretation were used to predict the direction of flow shown in Figure 4. This shows on the average that the northern zone is topographically high while the southern region is topographically low [8]. The establishment of the inequality in the water table suggests that groundwater flows from the north (high hydraulic head) to the south (low hydraulic level). This implies that the northern zone is the recharge zone while the southern region is the sink. With this infiltration by hydraulic connection, the source and sink of pollutants has elevated the concentration of fluid conductivity in the impervious and semi-impervious aquifers around the Gulf of Guinea [17,18].

Figures 5(a)-(c) show the geological provinces of the three transects with four VES points in each. The geosections show the different lithologic units from top to bottom in each of the profiles. Although the determined units which were constrained by logged borehole are somewhat similar, the depths of burial and the thicknesses of distribution in the subsurface differ from one transect to another.

Figure 5(b) represents the geosection drawn along the profile of VES1 Iko Town to VES4 (Onna) at the western part of the study area. The gosection of Figure 5(a) shows from top to bottom lateritic top soil with average thickness and depth of 19.5 m; conductive sandy layer with average depth and thickness of 70.4 m and 51.3 m respectively. Fine sand has average depth and thickness of 115.1 m and 44.2 m respectively. The fine sand is underlain with coarse sand which shows infinite depth within the maximum current electrode separations. The description of these lithologic units was aided by the borehole near VES2.

At the transect covering VES5 (Ikot Akpatek) to VES 8 (Effoi) at the northern part of the study area, the geosection in Figure 5(b) was drawn. The geosection shows four different lithologic units from top to bottom. The top soil is lateritic sand with average depth and thickness of 14.1 m. Underlying this layer is the gravelly sand of average depth and thickness of 60.3 m and 46.2 m respectively. Below the gravelly sand is a thick layer of conductive sand whose average depth and thickness are 167.6 m and 107.2 m respectively. At VES5, this layer is more developed up to a depth of 210 m. However, at VES6, the conductive layer is less than 150 m deep. Along the transect, the layer deepens gradually again up to 175 m at VES8. The infinitely thick layer of coarse sand whose thickness and depth could not be determined within the maximum current electrode separation lies below the conductive layer. The transect at the eastern part covers VES9 (Abat) to VES12 (QIC School, Ibeno). The topmost layer is lateritic soil with an average depth and thickness of 17.2 m. This layer is immediately underlain with gravelly sand of average depth and thickness of 42.2 m and 25.2 m respectively. Just below this layer lies a thick layer of coarse sand with average depth and thickness of 102.2 m and 59.6 m respectively. This layer deepens most at VES10 and VES11 and seems to thin out at VES12 and is underlain by an infinite layer of conductive sand whose depth and thickness could not be determined within the maximum current electrode separation used in this work. In brief, the ranges of resistivities of layers for the different transects can be obtained from Table 1. These ranges are significant in determining whether a layer is conductive (saline) or not.

Figure 4. Grid vector map showing groundwater flow in the study area.

(a)(b)(c)

Figure 5. (a) Western geosection along VES1-4 and the logged borehole near VES2; (b) Northern geosection along VES5-8 and the logged borehole near VES6; (c) Eastern geosection along VES9-12 and the logged borehole near VE10.

Table 1. Summary of location and geoelectric parameters for the three transects.

5. Conclusions

In summary, the establishment of the flow direction can be used in contamination study. For the transect at the western part, saline and ferruginized water can be avoided by locating the screen of a borehole in the fine sand layer (75 m depth on the average) or in the coarse sand (above 100 m deep). In transect at the northern part, the saline water layer is well mapped out. The decision to avoid this layer is predicated on the location. On the average, borehole depth should be located from 220 m deep in order to get water that is devoid of contamination of this layer. Again on transect at the eastern part, the saline and ferruginized layer is deeply seated and good quality water can be obtained from 40 - 75 m deep. However, over pumping can cause intrusion of conductive water from the depth range of 88.5 m (VES12) to 116.2 m (VES11) into the borehole located in the coarse sand.

With this geophysical method, saline and ferruginized layers are clearly spelt out for water resources to be assessed with caution. The method is thus benign, noninvasive and friendly to the environment [19,20] and so it is recommended that wildcat drilling should be discouraged in order to avoid locating borehole depth at the conductive layers.

REFERENCES

  1. M. P. Anderson and C. A Berkebile, “Evidence of Salt Water Intrusion in Southeastern Long Island,” Groundwater, Vol. 14, No. 5, 1976, pp. 315-319. doi:10.1111/j.1745-6584.1976.tb03121.x
  2. A. Vengosh and A. Ben-Zvi. “Formation of a Saltplume in the Coastal Plain Aquifer of Israel: The Beer Toviyya Region,” Journal of Hydrology, Vol. 160, No. 1-4, 1994, pp. 2l-52. doi:10.1016/0022-1694(94)90032-9
  3. A. Vengosh and E. Rosenthal, “Saline Groundwater in Israel: Its Bearing on the Water Crisis in the Country,” Journal of Hydrology, Vol. 156, No. 1-4, 1994, pp. 389- 430. doi:10.1016/0022-1694(94)90087-6
  4. C. Petalas and N. Lambakis “Simulation of Intense Salinization Phenomena of Coastal Aquifer of Thrace,” Journal of Hydrology, Vol. 324, No. 1-4, 2006, pp. 51-64. doi:10.1016/j.jhydrol.2005.09.031
  5. R. Guerin, Y. Mehheni, G. R. Iondrasoa and Tabbagh, “Interpretation of Slingraam Conductivity Mapping in NearSurface Geophysics: Using a Single Parameter Fitting with 1D Model,” Geophysical Prospecting, Vol. 44, No. 2, 1996, pp. 233-249.
  6. R. D. Barker, T. V. Rao and M. Thangarajan, “Dealineation of Contaminant Zone through Electrical Imaging Technique” Research Communications, Current Science, Vol. 81, No. 3, 2001, pp. 101-107.
  7. O. E. Esu and C. S. Okereke, “Delineation of Shallow Groundwater Aquifers in the Coastal Plain Sands of Calabar Area (Southern Nigeria) Using Surface Resistivity and Hydrological Data,” Journal of African Earth Science, Vol. 35, No. 3, 2002, pp. 433-443. doi:10.1016/S0899-5362(02)00148-3
  8. J. D. Mc-Nell, “Electrical Conductivity of Soil and Rocks,” Hydrological Processes, Vol. 17, 2003, pp. 1197-1211.
  9. V. I. Obianwu, N. J. George and A. A. Okiwelu, “Preliminary Geophysical Deduction of Lithological and Hydrological Conditions of the North-Eastern Sector of Akwa Ibom State, Southern Nigeria,” Research Journal of Applied Sciences, Engineering and Technology, Vol. 3, No. 8, 2011, pp. 806-811.
  10. N. George, V. Obianwu and K. Udofia, “Estimation of Aquifer Hydraulic Parameters via Coplementing Surficial Geophysical Measurements on the Aquifer Core Samples,” International Review of Physics, Vol. 5, No. 2, 2011, pp. 88-97.
  11. N. J. George, A. E. Akpan, I. B. Obot and N. J. Akpanetuk, “Geoelectical, Investigation Flooding Using the Lithologic Compositions of Erosion and Flood-Stricken Road in Ukanafun Local Government Area, Akwa Ibom State, Southern Nigeria,” Journal of Disaster Advances, Vol. 1, No. 4, 2008, pp. 46-52.
  12. F. S. Akpan, O. N. Etim and A. E. Akpan, “Geoelectrical Investigation of Groundwater Potential in Parts of Etim Ekpo Local Government Area, Akwa Ibom State,” Nigerian Journal of Physics, Vol. 18, 2006, pp. 39-44.
  13. A. E. Edet, “Groundwater Quality Assessment in Parts of Eastern Niger Delta,” Environmental Geology, Vol. 22, No. 1, 1993, pp. 41-46. doi:10.1007/BF00775283
  14. P. K. Tsagarakis and A. N. Angelakis, “Water Resource Management in Crete (Greece) Including Water Recycing and Rescue and Proposed Quality Criteria,” Agricultural Water Management, Vol. 66, No. 1, 2004, pp. 35-47. doi:10.1016/j.agwat.2003.09.004
  15. R. J. Kalinski, W. E. Kelly, Bogardi and G. Pesti, “Combined Use of Geoelectric Sounding and Profiling to Quantify Aquifer protection Properties,” Journal of Applied Geophysics, Vol. 16, No. 3, 1993, pp. 323-329.
  16. M. K. Hubbert, “The Theory of Groundwater Motion,” Journal of Geology, Vol. 48, No. 8, 1940, pp. 785-944. doi:10.1086/624930
  17. F. D. Borner and J. H. Schon, “A Relationship between Quadrature Component of Electrical Conductivity and the Specific Surface Area of Sedimentary Rocks,” Log Analyst, Vol. 32, 1991, pp. 612-613.
  18. A. C. Ekwe, N. N. Onu and K. M. Onuoha, “Estimation of Aquifer Hydraulic Characteristics from Electrical sounding Data: The Case of Middle Imo River Basin Aquifers, Southern Nigeria,” Journal of Spatial Hydrology, Vol. 6, No. 2, 2006, pp. 121-132.
  19. D. D. C. Mbonu, J. O. Ebeniro, C. O. Ofoegbu and A. S. Ekine, “Geoelectrical Sounding for Determination of Aquifer Characteristics in Parts of Umuahia Area of Nigeria,” Geophysics, Vol. 56, No. 5, 1991, pp. 284-291.
  20. S. K. Sandberg, L. D. Slater and R. Versteeg, “An Integrated Geophysical Investigation of Hydrology of an Anisotropic Unconfined Aquifer,” Journal of Hydrology, Vol. 267, No. 3-4, 2002, pp. 227-243. doi:10.1016/S0022-1694(02)00153-1

NOTES

*Corresponding author.