Fifty vertical electrical soundings were carried out in the Adamawa region of Cameroon. The interpretation was done using inverse slope method (ISM) and curve matching methods. The aim was to employ the applicability and suitability of the ISM in deciphering the vertical electrical sounding (VES) data for groundwater and hydrogeophysical purposes in the Pan-African aquifers. The ISM can be used to interpret VES data collected with any electrodes array. The results obtained by the ISM geo-electrical interpretation correlate/agree well with the available lithological logs used in constraining the interpretation. The resistivity values obtained through this method are in the range of 20–900 Ω m with a mean of 241 Ω m and a standard deviation of 228 Ω m. The aquifer thickness is in the range of 2–90 m, with an average of 33 m and a standard deviation of 21 m. Resistivity, thickness and depth of the Pan-African aquifer in the Adamawa region, Central Africa have been determined and characterized using both the ISM and an integrated protocol of interpolation technique. The ISM can therefore be recommended for the interpretation of VES measurements in the similar Pan-African context worldwide.

  • Electrical soundings were carried out in the study area.

  • The inverse slope method is simpler than the curve matching method.

  • Pan-African aquifer in the Adamawa region has been characterized.

  • The area has high and low resistivities.

  • The thickness and depth are in line with results obtained using other methods.

Direct current (DC) geo-electrical methods stand out in the domain of groundwater prospection due to their accuracy and high efficiency in comparison with traditional methods of pumping tests (George et al. 2014, Umo et al. 2022a, 2022b). Several quantitative software programs and inversion techniques have been proposed and discussed for interpreting DC earth-resistivity measurements. Ghosh (1971) determined inverse filter coefficients for the computation of apparent resistivity standard curves for a horizontally stratified earth. Zohdy (1975, 1985) modified Dar–Zarrouk functions for automatic interpretation of Schlumberger vertical electrical sounding (VES) curves, and later, improved this technique by adding Wenner sounding curves. Koefoed (1976) presented progressive developments in the direct interpretation of the resistivity sounding. Geo-electrical DC methods have been used to investigate groundwater in the Pan-African context of Central Africa region (Aretouyap et al. 2015a, 2015b). Recently, geo-electrical resistivity technology has been deployed through VES and electrical resistivity tomography (ERT) to study shallow/intermediate depths of investigation for reasons bordering on hydrogeology, environment, archeology, engineering, and mining surveys (Ngako & JegouzoNzenti 1991; Ibanga & George 2016; Obiora et al. 2016; Thomas et al. 2020; George et al. 2021; Mohammed et al. 2021; Ekanem et al. 2022; Ikpe et al. 2022). The results assisted in solving both environmental and ecological problems in their respective study areas. Uwa et al. (2019) studied the geohydrodynamics of a coastal environment using VES data. However, it is important to assess the limitations of each technique regarding its suitability and assets (accuracy) in relation to different subsurface conditions for, each one is based on a separate approach and methodology (Asfahani 2016). For example, when Aretouyap et al. (2019, 2021) used the conventional curve matching method (CMM) to derive the hydro-parameters of the Adamawa Plateau watershed, it was found that the resolution of this method is so poor, such as thin layers buried at important depth are simply indistinguishable on the logarithmic plot. These CMM limitations encouraged the use of an alternative approach, namely the inverse slope method (ISM) for the interpretation of VES data. ISM was previously developed by Sanker Narayan & Ramanujachary (1967) and recently applied by Mohamed et al. (2014). Asfahani (2016) successfully applied the ISM program in exploration geophysics to characterize phosphatic layers in Al-Sharquieh mine in Syria. Recently, George et al. (2022) used both the ISM and the computer-aided iterative least-square inversion technique to delineate hydrogeological units. The outcomes of the research gave well-resolved depths, and thicknesses, in which the ISM parameters were more consistent with geological units than the least-square inversion technique. The ISM technique is simpler than CMM and has numerous qualitative and quantitative advantages. It allows for a distinctively resolved delineation of geologic layers, no matter how thin the layer is and can be used to interpret VES data collected with any electrodes array (Mohamed et al. 2014; George et al. 2022). The ISM technique is used herein to reinterpret VES data already investigated by Aretouyap et al. (2015a, 2015b) for groundwater and hydrogeological related purposes. Interestingly, the main objective of the present paper is to employ the ISM programming technique in testing the suitability and the applicability of the ISM in the Pan-African context. The method is also applied to overcome major interpretation difficulties (e.g., the eclipse of thinner layers and the sensibility to electrodes array in VES data collection), associated with traditional CMM as well as comparing the results obtained from ISM, CMM and programming inversion methods. By applying the geo-electrical results of ISM for hydrogeophysical and aquifer characterization through the integral interpolation protocol technique in the Pan-African context of Central Africa, alternative and reliable results, which overcome the principles of suppression and equivalence, can be avoided, mostly when constrained with ground truth data. The data for this research were collected in 2015 with the field campaign in Cameroon, while data interpretation was done using ISM in 2022.

Study area

This research is conducted in the Adamawa-Cameroon region, located in the heart of Central Africa between latitudes 6°–8° north and longitudes 11°–16° east (Figure 1). The study region extends over a length of about 410 km from west to east between the Federal Republic of Nigeria and the Central African Republic, with an area of 6,782 km2. The morphology of the region is made of volcanic highlands, resulting from tectonic uplift and subsidence accompanied by intense magmatic emissions (Vincent 1970; Tchameni et al. 2001). Although the average altitude is 1,100 m, this region of rugged terrain is limited to the north by a large cliff and an uneven escarpment of several hundred meters that dominates the area.
Figure 1

Geological map of the study area, with the locations of VES measurements (Maréchal 1976) as amended with map containing all major geological features that can influence the hydrogeological activities.

Figure 1

Geological map of the study area, with the locations of VES measurements (Maréchal 1976) as amended with map containing all major geological features that can influence the hydrogeological activities.

Close modal

The center of the plateau is marked by soft forms barely accented and swampy valleys, dotted with mountains or/and volcanic cones. At the east, there are massifs resulting from the former erosion and tectonic movements. In the west, the terrain is mountainous with hills. Volcanic inheritance covers the north, the east and the south parts of the area. One notes the presence of an assembly line which occupies an important part of the region, reaching altitudes of more than 2,240 m. There are also plains and basins (Toteu et al. 2000).

The geological history of the Adamawa-Cameroon region is marked by three major events (Toteu et al. 2000). These are (i) long period of continental erosion from Precambrian to Cretaceous, (ii) the onset of volcanism from Cretaceous to Quaternary and (iii) recurrent basement tectonics that explains the horst and graben structure of the Adamawa Plateau.

An investigation of superficial formations in the region has highlighted the Pan-African granite-gneiss bedrock, represented by Ordovician Granites, Gneisses and Pan-African Migmatites. The main geological formations encountered are basalts, trachytes and trachyphonolites based mostly on concordant calco-alkaline granites and discordant alkaline granites (Toteu et al. 2000).

Three main geological units are observed on the surface. Each type of those geological unit contains some VES locations. The largest formation, made up of granite contains the majority of VES points. Metamorphic Formations contain some pits such as P-11, P-34, P-36, etc. Pits P-28, P-29, etc. are located in volcano-sedimentary units.

In hydrological terms, 150–300 km wide, the Adamawa Plateau is called ‘the water tower of the region’ because it feeds three of the four major watersheds of the region, namely, the Lake Chad Basin, the Niger Basin in the North and the Sanaga Atlantic Basin in the south. Indeed, many rivers such as Mayo Deo, Mayo Banyo, Mbere, Vina (tributaries of the Logone), Mbam, Kim, Djerem and Lom (tributaries of the Sanaga) divert from this region. There are also many crater lakes including Tyson, Mbalang and Vina lakes resulting from a long volcanic history in the region (Nguetnkam et al. 2002). In addition to the existence of many lineaments in the region, this important hydrosphere may forecast the existence of aquifers located at interesting depths with significant thicknesses.

Geophysical survey reveals that the Pan-African belt was tectonically active, where many lineaments and faults occur (Cornacchia & Dars 1983; Dumont 1986; Robain et al. 1996; Toteu et al. 2004; Ngako et al. 2008; Njonfang et al. 2008). Those lineaments are supposed to constitute ‘highway’ for groundwater. Although groundwater productivity is directly linked to the bedrock alteration, there is no recent study aimed at locating and characterizing local aquifers. This situation justifies the interest of the present paper.

VES data recording and interpretation

Schlumberger configuration is used to locate and characterize the aquifers in the study region. Electrical resistivity variations are expressed in this array as a function of depth (Ekanem et al. 2020). Fifty VES have been carried out in the study area, using the Terrameter ABEM SAS-1000 with a spacing of current electrodes varying from 1 to 600 m. This device directly measured the resistance, which enabled to calculate the apparent resistivity of the rock using the Ohm's law expressed by Equation (1), and taking into account the geometrical factor k of the used array expressed in Equation (2):
(1)
(2)

I is the intensity of the electrical current injected in the ground by electrodes A and B, and UMN is the voltage potential between electrodes M and N.

The resistivity meter with the electrodes cables and other accessories is the main measuring equipment. The CMM is generally used to interpret the smoothened field curve to generate initial layer resistivities and thicknesses of the layers (Zohdy et al. 1974; George 2020). The initial layer indices are thereafter used as inputs in the computer-aided quantitative interpretation software program, which in this research is done by the use of a one-dimensional (1D) least-square forward modeling software program called WINRESIST (Vander Velpen & Sporry 1993; Udosen & George 2018). The program software made use of the input data to generate a theoretical model and then establishes a fit between the model and the measured field data to give the final 1D resistivity model curves. The goodness of fit is expressed in terms of the root-mean square error (RMSE) (Bandani 2011). The values of the measured apparent resistivity ρa depend on several factors such as true layers resistivities and thicknesses, and the electrode's location. The accuracy of their determination depends on the homogeneity of the substratum. For a heterogeneous medium, CMM interpretation does not provide enough accurate results.

However, some ambiguity problems can arise during the interpretation. A sample interpretation exercise must be carried out before each project in order to solve such encountered problems. If those ambiguity problems are too complex, further methods such as seismic and test wells are required (Asfahani 2007). Sometimes, the use of an alternative independent method is indispensable (Asfahani 2013).

The results of the CMM (Orellana & Mooney 1966) are used in the present paper for comparison with those obtained by ISM. For the CMM technique, an inverse technique programme fits thereafter both theoretical and field curves for each experimental VES (Zohdy 1985; Zohdy & Bisdorf 1989). This operation requires the double condition of accuracy in calculations and reasonable geological modeling. Furthermore, the medium is known as a one-dimensional model 1D (Dey & Morrison 1979). The 1D quantitative interpretation of the 50 VES by using both the CMM and the inversion software program of WinResist enabled the identification of hydrogeoelectrical characteristics of the Pan-African deposits (Aretouyap et al. 2015a, 2015b).

Inverse slope method

ISM can be used to obtain directly the resistivities and the thicknesses of subsurface layers from field data (Sanker Narayan & Ramanujachary 1967). Asfahani (2016) in an attempt to explore for sulfate minerals explained all the steps methodically used in ISM approach. The inverse resistivities for (AB/2)/ρa were plotted against the electrode separation (AB/2). The apparent resistivity of each can be obtained using the slope (mi) in each segment using expression . Each line segment resulting from this graph represents a layer; and the intersection of the line segments, multiplied by a factor of 2/3, and corresponds to the depth of a particular layer. Concretely, let t1tn be intersection points, then 2/3 ×ti is equal to the depth of the ith interface. Similarly, when (AB/2)/ρa is plotted versus AB/2, the slope gives the resistivity of the ith layer except when the segment representing the high-resistivity layer shows a negative slope. In this case, the resistivity of the layer is taken as infinity (Asfahani 2016). The thickness of each layer is defined by the difference between the depths of two consecutive strata and at the point of intersection (George et al. 2022). The application of ISM is that it is possible to decipher thin layers even if they are buried at great depths. The work of Asfahani (2016) has been confirmed by George et al. (2022) and the result shows that ISM is more sensitive to CMM based on the closeness of results from ISM to ground truths. Based on the above analyses with ISM and CMM methods, the primary geo-electric indices (layer resistivity, layer thickness and depth) were determined as presented in Table 1. These parameters are used in characterizing the Pan- African aquifer systems. The layer resistivities realized showed high and low values, indicating the variations in the geological materials within the subsurface (Akpan et al. 2013; George et al. 2017; Ibuot et al. 2017).

Table 1

The Pan-African aquifer resistivity, thickness and depth

Stn. N°CMM results
ISM results
Resistivity (Ω m)Thickness (m)Depth (m)Resistivity (Ω m)Thickness (m)Depth (m)
P-1 565 40 18.4 320 42.1 21 
P-2 200 38 23 190 35 22 
P-3 157 10.7 210 8.4 14.5 
P-4 410 40 40.2 350 37 43 
P-5 640 30 44 751 39.5 37.4 
P-6 100 22 41.2 197 15 36 
P-7 114.1 19 36.5 137 58 14 
P-8 53 62 22.1 47 47.2 26 
P-9 341 23 22 289 31.6 21.8 
P-10 408 31 31 420 42 20 
P-11 446 43 17.4 387 30 20 
P-12 110.8 38 18.1 122 35.4 22 
P-13 472 16.0 382 4.2 16.6 
P-14 362.1 47 24.8 263 31.7 29 
P-15 61 93 29 11 15 
P-16 392.6 70 19.1 408 86 18 
P-17 387 14 22 524 19.8 24.5 
P-18 137 43.7 241 40 
P-19 13 39.4 25 11.2 40 
P-20 112.9 17 22 203 12.8 26 
P-21 21 69 11 32.1 79 
P-22 134 43 50.2 98 51.4 39.7 
P-23 207 19 24.1 196 33 30 
P-24 20 11 22 12 10 
P-25 10.8 16 13.5 
P-26 212 52 20 259 50 22 
P-27 422 28 9.8 602 19.2 14 
P-28 25 33 20.1 38 25 23 
P-29 47 85 14.7 69 77 17 
P-30 811 25 42 726 31 39 
P-31 502 39 717 10 41 
P-32 221.5 19 25.7 150 12 27 
P-33 270.4 32 32.8 302 37 37.45 
P-34 825 38 51.1 900 32 48 
P-35 10 11 41 14 17 43.45 
P-36 479 42 24 611 34 29.75 
P-37 29.4 20 12 24 
P-38 216.1 15 29.4 198 21 32 
P-39 40 60 33 69 58 38 
P-40 28 27 30 56 24 22.9 
P-41 26 34 31 31 32 28.25 
P-42 46 46 35.8 30 17 16 
P-43 177 48 30.4 168 29 28 
P-44 22 37 33 41 25 30 
P-45 188 61 21 200 51 25 
P-46 608 20 35 618 26 37 
P-47 48 59 50.1 50 61 42.9 
P-48 175.7 48 27.9 187 50 32.5 
P-49 62 101 18.5 100 90 21.45 
P-50 104 33 5.1 47 85 17 
Stn. N°CMM results
ISM results
Resistivity (Ω m)Thickness (m)Depth (m)Resistivity (Ω m)Thickness (m)Depth (m)
P-1 565 40 18.4 320 42.1 21 
P-2 200 38 23 190 35 22 
P-3 157 10.7 210 8.4 14.5 
P-4 410 40 40.2 350 37 43 
P-5 640 30 44 751 39.5 37.4 
P-6 100 22 41.2 197 15 36 
P-7 114.1 19 36.5 137 58 14 
P-8 53 62 22.1 47 47.2 26 
P-9 341 23 22 289 31.6 21.8 
P-10 408 31 31 420 42 20 
P-11 446 43 17.4 387 30 20 
P-12 110.8 38 18.1 122 35.4 22 
P-13 472 16.0 382 4.2 16.6 
P-14 362.1 47 24.8 263 31.7 29 
P-15 61 93 29 11 15 
P-16 392.6 70 19.1 408 86 18 
P-17 387 14 22 524 19.8 24.5 
P-18 137 43.7 241 40 
P-19 13 39.4 25 11.2 40 
P-20 112.9 17 22 203 12.8 26 
P-21 21 69 11 32.1 79 
P-22 134 43 50.2 98 51.4 39.7 
P-23 207 19 24.1 196 33 30 
P-24 20 11 22 12 10 
P-25 10.8 16 13.5 
P-26 212 52 20 259 50 22 
P-27 422 28 9.8 602 19.2 14 
P-28 25 33 20.1 38 25 23 
P-29 47 85 14.7 69 77 17 
P-30 811 25 42 726 31 39 
P-31 502 39 717 10 41 
P-32 221.5 19 25.7 150 12 27 
P-33 270.4 32 32.8 302 37 37.45 
P-34 825 38 51.1 900 32 48 
P-35 10 11 41 14 17 43.45 
P-36 479 42 24 611 34 29.75 
P-37 29.4 20 12 24 
P-38 216.1 15 29.4 198 21 32 
P-39 40 60 33 69 58 38 
P-40 28 27 30 56 24 22.9 
P-41 26 34 31 31 32 28.25 
P-42 46 46 35.8 30 17 16 
P-43 177 48 30.4 168 29 28 
P-44 22 37 33 41 25 30 
P-45 188 61 21 200 51 25 
P-46 608 20 35 618 26 37 
P-47 48 59 50.1 50 61 42.9 
P-48 175.7 48 27.9 187 50 32.5 
P-49 62 101 18.5 100 90 21.45 
P-50 104 33 5.1 47 85 17 

Results obtained, respectively, using CMM and ISM are displayed in the same table for comparison. Some values are similar while there is a clear difference between other ones.

Interpolation technique

Aquifer's parameters investigated in this paper have been measured or computed punctually (especially on VES sites). Yet, an efficient and sustainable management of groundwater resources requires an accurate and continuous determination of hydrodynamic parameters. As opined by Varol et al. (2021), geostatistics is often useful in predicting, assessing and interpolating the distinct components of a system such as an aquifer system comprising resistivity, depth and thickness.

The technique applied herein is essentially based on the notions of semivariogram and Kriging according to Aretouyap et al. (2016).

Semiariogram

Caridad & Jury (2013) designated the variogram as a geostatistical tool used to describe the spatial continuity of a phenomenon (Carvalho et al. 2013). Its theoretical formulation is given in the following equation:
(3)

In this equation, Var is the variance applied to the difference between two observations h(x) and h(x+r) separated by a distance r.

Kriging

Kriging is known for its ability to interpolate and predict spatial data considered as a set of some observable variables. Those observations may be spatially correlated. If applied adequately, Kriging provides the expected value and variance for every point within a region. Hence, this approach can be used to estimate the unknown value h* (Equation (4)) of a variable at a point from the surrounding known values hi, with a unique solution:
(4)

In this relation, represent the Kriging weights.

Equation (5) expresses the minimum estimation variance of the system (kriging variance):
(5)

Determination of Kriging weights, which are needed to estimate a point defined by the linear estimator is explained in Aretouyap et al. (2014).

This approach is very important in the context of developing countries where data collected are generally sparse and irregular. One observes the following three steps, which aid efficiently in investigating the parameters such as exploratory data analysis, structural data analysis and prediction (interpolation).

Exploratory data analysis

Data consistency has been checked, outliers (strange values which are very high or very low compared to the dataset) removed and statistical distribution identified. Indeed, an optimal application of Kriging techniques requires normal data distribution. For this, the mean and the median values of the parameters to be estimated should be very similar.

Structural data analysis

Kriging uses a scattered set of points with z-values to generate an estimated surface. The regionalized variable is the main theory used by this technique. The theory assumes a well statistical homogeneity throughout the surface of the spatial variation in the phenomenon represented by the z-values (Chilès & Delfiner 1999). The spatial variation is quantified by the semivariogram. The sample semivariogram is calculated from the sample data (Equation (6)):
(6)
For discrete variables, this function can be written as shown in the following equation:
(7)
where z(xi) is the value of the variable Z at location xi, h the lag, and N(h) the number of pairs of VES points, separated by h.

Prediction

The best semivariogram model (on the basis of cross validation) is selected to interpolate each parameter. Hence, various types of errors were computed and compared. Those are mean error (ME), mean square error (MSE), RMSE, average standard error (ASE) and root-mean square standardized error (RMSSE). ME 0 when predictions are unbiased. Unfortunately, this ME is strongly dependent upon the scale of the data, and usually is indifferent to the wrongness of semivariogram. Because of these weaknesses, ME is generally standardized by the MSE, being ideally equal to zero.

Yet, a strong similarity between the MSE and the ASE (RMSE ∼ ASE) indicates a good assessment of prediction. However, when RMSE < ASE (or RMSSE < 1), the variability of predictions is overestimated; and if the RMSE > ASE (or RMSSE > 1), the variability of predictions is underestimated. The thematic map of each parameter to be estimated has been drawn using the best semivariogram model. Those errors are expressed in Equations (8)–(12) according to Goovaerts (1997) and Gorai & Kumar (2013):
(8)
(9)
(10)
(11)
(12)
where σ2(xi) is the Kriging variance, Z*(xi) and Z(xi) are the estimated and the measured values of the geophysical parameter at the location xi, respectively.

Data validation by Nash–Sutcliffe optimization criterion

Data validation is a key factor in measurement. The Nash–Sutcliffe optimization criterion (NSOC) optimization criterion was adopted in order to estimate the data consistency between CMM and ISM. This was performed according to the proposition of Yao et al. (2007) in the following equation:
(13)
where is the observed aquifer resistivity in Ohm-m obtained from CMM, is the estimated/calculated aquifer resistivity from ISM and is the mean value of the observed aquifer resistivity for the ith resistivity values considered to constitute the aquifer units in the different locations surveyed. As opined by Yao et al. (2007), the percentage ranges of values given below are advanced for adjudging model efficacy:
  • NSOC ≥ 90%: the model is excellent;

  • 80% < NSOC < 90%: the model is very satisfactory;

  • 60% < NSOC < 80%: the model is satisfactory;

  • NSOC < 60%: the model is bad.

The above percentage ranges of parameters (aquifer resistivities) of model validation indicate that for NSOC between what is observed and what is alternatively calculated to be efficient, the calculated/modeled resistivity values should be close to the observed aquifer resistivities.

The 50 VES measurements have been interpreted by using ISM to firstly identify qualitatively different geo-electrical layers, and to secondly obtain quantitatively resistivities and thicknesses of those respective layers. Figure 4 compares the results obtained by both ISM and CMM with the available field lithological descriptions for the VES (P-8, P-9, P-14, P-17, P-22, P-23, P-26, P-31, P-13, P-39, P-40). CMM and ISM provide, for example, for VES (P-17) the same results in terms of quantity (number of layers and their respective thicknesses), which are well fitted with the lithological field description. However, some significant differences are noticed between ISM and CMM results for VES (P-9, P-13 and P-14), for which one can, for example, observe that CMM interpretation does not display the clay layer (Figure 2).
Figure 2

Comparative results obtained, respectively, from CMM and ISM alongside with the lithological description of some available boreholes. The CMM interpretation in the left, the ISM interpretation in the middle and the lithological pattern in the right.

Figure 2

Comparative results obtained, respectively, from CMM and ISM alongside with the lithological description of some available boreholes. The CMM interpretation in the left, the ISM interpretation in the middle and the lithological pattern in the right.

Close modal
CMM interpretation gives on the other side the same results as the available field drilling descriptions for the VES (P-23, P-39 and P-40). Overall, ISM results are the ones which produce the results that are closest to geological reality as it is shown in Figure 3. The geo-electrical ISM results are in good agreement with the available lithological descriptions for the studied VES in the region.
Figure 3

An example of the interpretation results of VES data using ISM. The VES data are processed and the output is directly compared with the real lithology obtained from drilling.

Figure 3

An example of the interpretation results of VES data using ISM. The VES data are processed and the output is directly compared with the real lithology obtained from drilling.

Close modal

Figure 3 is extracted from Figure 2 to illustrate clearly the pits’ interpretation using ISM. The interpretation of VESs P-9, P-13, P-14 and P-23 with ISM shows a good agreement with the available lithological description of those points. These ISM results are compared with the true lithological description. One can observe that both the ISM results and lithological logs have exactly the same number of layers with respective thicknesses slightly different. It is observed for all the interpreted pits that the last segment is characterized by a very low slope, equivalent to a very high resistivity (>2,500 Ω m). This high-resistive layer corresponds to the bedrock, made of granite. It also observed some differences in terms of layer numbers and resistivities, thicknesses and depths between the ISM results and those obtained using CMM (Aretouyap et al. 2015a, 2015b). Table 1 compares the Pan-African aquifer characteristics obtained from both CMM and ISM methods.

The qualitative interpretation of P-15 reveals three main layers: clay, cracking granite and granite arranged downward. The quantitative interpretation allowed for the respective delineation of resistivities as 502, 11 and 2,531 Ω m, and their respective thicknesses as 6 m, 15 m and infinite.

The clay resistivity for this pit VES P-15 is very high, and may be higher for the following pits. These high values are due to the nonpure character of the clay. In fact, this is a mixture of clay and laterite (Koita et al. 2013). The VES P-42 exhibits four layers with the clay (748 Ω m, 16 m) at the top and the granitic bedrock (5,217 Ω m) at the bottom. Intermediary layers are basalt (104 Ω m, 33 m) and ferruginous clay (3 Ω m, 17 m).

All of the 50 pits have been interpreted similarly by using ISM, where the local Pan-African aquifer made up of the upper weathering portion of the granitic basement has been characterized as shown in Table 2.

Table 2

Summary of the Pan-African aquifer characteristics derived from ISM in Adamawa, Central Africa

MinMaxMeanStandard deviation
Resistivity (Ω m) 20 900 241 228 
Thickness (m) 90 33 21 
Depth (m) 79 37 16 
MinMaxMeanStandard deviation
Resistivity (Ω m) 20 900 241 228 
Thickness (m) 90 33 21 
Depth (m) 79 37 16 

For some pits, the number of layers obtained from both interpretations (CMM and ISM) are different. CMM does not split some thinner layers, where those thin layers are detected by ISM. Furthermore, significant differences are observed in layers thicknesses and resistivities for the aquifer. For P-1 for example, CMM interpretation provides 565 Ω m resistivity, 40 m thickness and 18.4 depths while ISM interpretation provides, respectively, 320 Ω m, 42.1 m and 21 m for the same parameters as shown and compared in Table 1. Such differences are observed for almost all other VES points. Given the importance of aquifer resistivity and thickness in groundwater productivity and management (Asfahani 2007; Aretouyap et al. 2015a, 2015b), these dissimilarities observed from different techniques demonstrate the necessity of using and comparing both methods in the context of accurate interpretation and efficient water resources management. The high standard deviation noticed in the table is due to the heterogeneous nature of the geologic units serving as aquifers. This hinges on the fact that aquifer systems in the Pan-African region are made of suites of intercalations of geologic units, which give a dynamic range of the primary geo-electric indices. However, the efficacy of the model is validated by the use of NSOC, which checks for the consistency between the universal model (CMM) and the alternative model (ISM). The NSOC gave 87.93% as the correlative optimization between the CMM and ISM using Equation (13). The value of NSOC according to Yao et al. (2007), suggests that the model is satisfactory.

Some aquifers at times are characterized by probably a lower-resistive layer stuck between two higher-resistive layers (Akpan et al. 2018). The local Pan-African aquifer is predominantly made of the upper weathered part of the granitic bedrock, whose prolificacy depends on the fractures embedded in the granite. The spatial distribution of the main aquifer parameters (resistivity, thickness and depth) obtained from ISM interpretations were contoured using their coordinates in the surfer software programme and their results are represented in Figures 46.
Figure 4

Iso-resistivity map of the Pan-African aquifer in the Adamawa region. Resistivity values obtained from VES points using ISM are interpolated continuously throughout the whole study area.

Figure 4

Iso-resistivity map of the Pan-African aquifer in the Adamawa region. Resistivity values obtained from VES points using ISM are interpolated continuously throughout the whole study area.

Close modal
Figure 5

Isothickness map of the Pan-African aquifer in the Adamawa region. Thickness values obtained from VES points using ISM are interpolated continuously throughout the whole study area.

Figure 5

Isothickness map of the Pan-African aquifer in the Adamawa region. Thickness values obtained from VES points using ISM are interpolated continuously throughout the whole study area.

Close modal
Figure 6

Isopach map of the Pan-African aquifer in the Adamawa region. Depth values obtained from VES points using ISM are interpolated continuously throughout the whole study area.

Figure 6

Isopach map of the Pan-African aquifer in the Adamawa region. Depth values obtained from VES points using ISM are interpolated continuously throughout the whole study area.

Close modal

Figure 6 shows the distribution of the Pan-African aquifer resistivity deduced from the ISM interpretation of the 50 pits. Minimum values are observed in the northeast part of the region above VES location P-4 and maximum values are observed in the southwest part where is located P-20. Given that the local Pan-African aquifer is almost made up of a weathered portion of the granitic bedrock, minimum values of the aquifer resistivity correspond to a more cracked basement while maximum resistivity values correspond to a less fractured basement portion. One can also observe that the northeast part of the region is covered with volcano-sedimentary formations (see Figure 1). Other geological and geothermal factors as age and temperature can explain these maximum and minimum values. The resistivity map divides the area into two zones: a high-resistive zone in the southwest and a low-resistive zone in the northeast. Groundwater therefore may flow from the northeast (where is concentrated the recharge area) to the southwest.

Figure 6 shows the distribution of the saturated Pan-African aquifer thickness h deduced from the use of the 50 VES points interpreted by ISM. The minimum thickness is observed northward above VES P-4 point and the maximum eastward at VES P-6. The aquifer formations correspond with the low-resistivity layers. Higher aquifer thickness is observed in the eastern part of the study area.

Attentive analysis of Figures 5 and 6 insinuates that aquifer depth and resistivity vary inversely. Indeed, the highest depth values are observed south-eastward while the highest resistivity values are observed north-westward. This situation has an advantage and inconvenience. Having in mind that more productive aquifers in terms of flow or recharge are less resistive, citizens can drill productive hand-made wells in the region. However, because of the shallow location of these wells, they are very vulnerable to pollution, quality alteration and climate variability. ISM allows for precise determination of the hydraulic parameters such as resistivity, thickness and depth of the aquifer. These parameters are very useful in the integrated and sustainable management of groundwater resources. Their importance is also due to the potential environmental impacts they can generate in case of poor control. Such impacts can be wetland desiccation and especially structural damage as in London and Birmingham (Biwas 1992).

In fact, Biwas (1992) stated that any groundwater project needs a good environmental impact assessment. In particular, developing countries such as Cameroon are very concerned. Based on the primary geo-electric indices in Table 1, correlations have been determined between the ISM and CMM through the cross-plot in Figures 7 and 8. The cross-plot between ISM resistivity and CMM resistivity of the aquifer system and that of the ISM depth and CMM depth of the aquifer system in the study area show the coefficient of determination as 0.89 (89%) and 0.70 (70%), respectively. This shows that the trends in the primary geo-electric indices are consistent. The equations realized in Figures 7 and 8 indicate a strong relation between ISM and CMM results as reflected in their respective coefficient of determination.
Figure 7

A cross-plot between the ISM resistivity and CMM resistivity. According to this plot, resistivity values obtained from ISM are somewhat compliant with the ones obtained from CMM.

Figure 7

A cross-plot between the ISM resistivity and CMM resistivity. According to this plot, resistivity values obtained from ISM are somewhat compliant with the ones obtained from CMM.

Close modal
Figure 8

A cross-plot between the ISM depth and CMM depth. Depth values obtained from ISM are moderately correlated to the values obtained from CMM.

Figure 8

A cross-plot between the ISM depth and CMM depth. Depth values obtained from ISM are moderately correlated to the values obtained from CMM.

Close modal

Comparatively, the reliability of the method can be seen in the coefficients of determination and correlation coefficients (R) for the aquifer resistivity and depth in Figures 7 and 8. The CMM-ISM plot for aquifer resistivity gave while the CMM-ISM plot for depth gave . The correlations indicate strong relation in resistivity and depth between CMM and ISM, which implies the uniqueness of the method.

The application of the ISM in the present paper for interpreting VES data demonstrated the suitability of this method in the Pan-African context of groundwater purpose. Based on the goodness of fit, the method, which can avoid the principle of suppression and equivalence, has the capacity to overcome to quantitatively interpret geo-electrical units better than the CMM. ISM is simpler than CMM and has numerous qualitative and quantitative advantages. It allowed for the unique determination of all geologic layers. Even thinner layers can be determined with ease using ISM methods. ISM can be used to interpret VES data collected with any electrodes array (Asfahani 2013; Aretouyap et al. 2022; George et al. 2022). Its application has allowed for the characterization and derivation of the hydrogeophysical parameters of the Pan-African aquifer in the Adamawa region through the integrated protocol of interpolation technique, which can be useful for further groundwater modeling and assessment. The PAA resistivity values obtained by applying this ISM are in the range of 20–900 Ω m with a mean of 241 Ω m and a standard deviation of 228 Ω m. The aquifer thickness ranged from 2 to 90 m, with an average of 33 m and a standard deviation of 21 m. The high standard deviation is symptomatic of the high variability in the primary geo-electric indices, caused by variation in sand grains and depth of burial of aquifer systems. This economically exploitable aquifer is globally located at 37 m. The NSOC proposed by Yao et al. (2007) indicates that the model percentage is 87.93% reflecting that the chosen model is satisfactory. The correlation of CMM with the new technique (ISM) from the graphical analysis showed correlation coefficient is greater than 80% in resistivity and depth determination of the economic aquifers. These results enhance the understanding of the uneven Pan-African terrain and may be taken into account when planning groundwater management in the context of sustainable development. It is envisaged to identify the VES database in the region for future hydrogeophysical investigations.

The authors are very thankful to the anonymous reviewers who helped them to improve this article. They are also very thankful to the managing editor, Maryam Shabani, who handled the manuscript.

All relevant data are available on request.

The authors declare there is no conflict.

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