This paper applies spectral and cepstral decomposition techniques to a 2D channel sand model from the Niger Delta region. Specifically, it uses the Discrete Fourier Transform (DFT) and Complex Cepstral Transform (CCT) to analyze the model. The DFT represents the signal in the frequency domain, while the CCT represents it in the quefrency domain. The CCT helps to separate source and transmission path effects and recover sub-seismic geologic information. Results show that cepstral attributes reveal more detail than spectral attributes and can help enhance visualization of small-scale anomalies and estimate stratigraphic parameters. This has practical applications for clearer imaging and better interpretation of subtle discontinuities in the field.
Advances in Geological and Geotechnical Engineering Research Vol 5 No 3 July ...Bilingual Publishing Group
Contribution of GIS to Hydromorphometric Characterization of the Nkoup Watershed (Nun Plain-Cameroon)
On the Possible Cometary Nature of the Uchur Cosmic Body (Fall 3.08. 1993)
Investigation of Physicochemical Properties of Qalay Abdul Ali Soil, Kabul, Afghanistan
Some Results of Direct FR Technology Applied to Study Methane Seepage Areas in the Arctic Region
Weather Events Associated with Strong Earthquakes and Seismic Swarms in Italy
Multi-channel analysis of Surface Wave (MASW) profiling for delineation of su...IRJET Journal
This document summarizes a study that used Multi-channel Analysis of Surface Waves (MASW) profiling to delineate subsurface stratigraphy around the Kolkata High Court building in India. MASW data was collected along 6 profiles near the building to determine shear wave velocity with depth. The data showed that within 15 meters of the surface, shear wave velocities were low (<200 m/s), indicating soft soil that could cause settlement. Below 15 meters, velocities increased, indicating denser soil. This helps explain cracking observed in the heritage building, likely due to soft near-surface soil conditions. The study classified the near-surface soils as NEHRP Site Class F and deeper soils as Class E, providing information on
This document presents a novel preprocessing scheme to improve prediction of sand fraction from seismic attributes using neural networks. The scheme consists of three steps: 1) preprocessing the high-resolution well log sand fraction data using techniques like Fourier transform, wavelet decomposition, and empirical mode decomposition to better match the low-resolution seismic attributes, 2) training an artificial neural network on the preprocessed data, and 3) postprocessing the network predictions with 3D spatial filtering. The proposed preprocessing scheme is found to produce significantly better predictions of sand fraction compared to using the original well log data, helping with reservoir characterization from seismic data.
Geometric wavelet transform for optical flow estimation algorithmijcga
This paper described an algorithm for computing the optical flow (OF) vector of a moving objet in a video sequence based on geometric wavelet transform (GWT). This method tries to calculate the motion between two successive frames by using a GWT. It consists to project the OF vectors on a basis of geometric wavelet. Using GWT for OF estimation has been attracting much attention. This approach takes advantage of the geometric wavelet filter property and requires only two frames. This algorithm is fast and able to estimate the OF with a low-complexity. The technique is suitable for video compression, and can be used for stereo vision and image registration.
Mems based optical sensorMEMS BASED OPTICAL SENSOR FOR SALINITY MEASUREMENTprj_publication
In this paper, we purpose a two dimensional photonic crystal based optical sensor for
salinity measurement. The salinity percentage of is sea water changes as we go down the sea
water surface. This gives change to the index of refraction of the sea water at the different
levels. Thus the salinity percentage of sea water can be detected by measuring this change in the
effective refractive index of sea water. In this paper, the effective refractive index method has
been used for the detection of the salinity concentration from (0-40%). The slab waveguide is
designed and the effective refractive changed is captured. Even as the refractive index change
for the change in salinity of the sea water, is very small, the effective index change is visible,
making the sensor very sensitive.
Mems based optical sensor for salinity measurementprjpublications
1. The document describes a MEMS-based optical sensor using a two-dimensional photonic crystal slab waveguide for measuring salinity.
2. The sensor takes advantage of the fact that the refractive index of sea water changes with salinity concentration. It detects these small refractive index changes by measuring the resulting effective index change in the photonic crystal slab waveguide.
3. Simulation results show that even small refractive index changes due to salinity produce a more significant change in effective index, demonstrating the high sensitivity of the designed sensor. Effective index decreases exponentially with increasing salinity percentage measured.
Monitoring NDTI-River Temperature relationship along the river ganga in the s...IRJET Journal
This document presents a study that uses geospatial techniques to monitor the relationship between river temperature and turbidity, as indicated by Normalized Difference Turbidity Index (NDTI) values, along segments of the Ganges River near Ghazipur, Varanasi, and Mirzapur districts in India. Landsat 5 and 8 satellite imagery from 2010, 2015, 2019, and 2021 were analyzed to estimate river temperature and NDTI values for each stretch. Statistical analysis found high correlation between turbidity and temperature for the Varanasi stretch, followed by Mirzapur and Ghazipur. The Varanasi stretch had the highest recorded temperatures and turbidity levels, likely due to industrial and domestic waste flows. The study
Evaluation of the Back Propagation Neural Network for Gravity Mapping IRJET Journal
This document evaluates the ability of back propagation neural networks (BPN) to produce gravity maps. The study trained a BPN model with 646 patterns from a gravity map and satellite image of Khartoum City. The trained model was tested on the training patterns and 162 new patterns. The results showed that the BPN model was unable to produce an accurate gravity map. Therefore, the BPN architecture is not suitable for this application of artificial intelligence in gravity mapping.
Advances in Geological and Geotechnical Engineering Research Vol 5 No 3 July ...Bilingual Publishing Group
Contribution of GIS to Hydromorphometric Characterization of the Nkoup Watershed (Nun Plain-Cameroon)
On the Possible Cometary Nature of the Uchur Cosmic Body (Fall 3.08. 1993)
Investigation of Physicochemical Properties of Qalay Abdul Ali Soil, Kabul, Afghanistan
Some Results of Direct FR Technology Applied to Study Methane Seepage Areas in the Arctic Region
Weather Events Associated with Strong Earthquakes and Seismic Swarms in Italy
Multi-channel analysis of Surface Wave (MASW) profiling for delineation of su...IRJET Journal
This document summarizes a study that used Multi-channel Analysis of Surface Waves (MASW) profiling to delineate subsurface stratigraphy around the Kolkata High Court building in India. MASW data was collected along 6 profiles near the building to determine shear wave velocity with depth. The data showed that within 15 meters of the surface, shear wave velocities were low (<200 m/s), indicating soft soil that could cause settlement. Below 15 meters, velocities increased, indicating denser soil. This helps explain cracking observed in the heritage building, likely due to soft near-surface soil conditions. The study classified the near-surface soils as NEHRP Site Class F and deeper soils as Class E, providing information on
This document presents a novel preprocessing scheme to improve prediction of sand fraction from seismic attributes using neural networks. The scheme consists of three steps: 1) preprocessing the high-resolution well log sand fraction data using techniques like Fourier transform, wavelet decomposition, and empirical mode decomposition to better match the low-resolution seismic attributes, 2) training an artificial neural network on the preprocessed data, and 3) postprocessing the network predictions with 3D spatial filtering. The proposed preprocessing scheme is found to produce significantly better predictions of sand fraction compared to using the original well log data, helping with reservoir characterization from seismic data.
Geometric wavelet transform for optical flow estimation algorithmijcga
This paper described an algorithm for computing the optical flow (OF) vector of a moving objet in a video sequence based on geometric wavelet transform (GWT). This method tries to calculate the motion between two successive frames by using a GWT. It consists to project the OF vectors on a basis of geometric wavelet. Using GWT for OF estimation has been attracting much attention. This approach takes advantage of the geometric wavelet filter property and requires only two frames. This algorithm is fast and able to estimate the OF with a low-complexity. The technique is suitable for video compression, and can be used for stereo vision and image registration.
Mems based optical sensorMEMS BASED OPTICAL SENSOR FOR SALINITY MEASUREMENTprj_publication
In this paper, we purpose a two dimensional photonic crystal based optical sensor for
salinity measurement. The salinity percentage of is sea water changes as we go down the sea
water surface. This gives change to the index of refraction of the sea water at the different
levels. Thus the salinity percentage of sea water can be detected by measuring this change in the
effective refractive index of sea water. In this paper, the effective refractive index method has
been used for the detection of the salinity concentration from (0-40%). The slab waveguide is
designed and the effective refractive changed is captured. Even as the refractive index change
for the change in salinity of the sea water, is very small, the effective index change is visible,
making the sensor very sensitive.
Mems based optical sensor for salinity measurementprjpublications
1. The document describes a MEMS-based optical sensor using a two-dimensional photonic crystal slab waveguide for measuring salinity.
2. The sensor takes advantage of the fact that the refractive index of sea water changes with salinity concentration. It detects these small refractive index changes by measuring the resulting effective index change in the photonic crystal slab waveguide.
3. Simulation results show that even small refractive index changes due to salinity produce a more significant change in effective index, demonstrating the high sensitivity of the designed sensor. Effective index decreases exponentially with increasing salinity percentage measured.
Monitoring NDTI-River Temperature relationship along the river ganga in the s...IRJET Journal
This document presents a study that uses geospatial techniques to monitor the relationship between river temperature and turbidity, as indicated by Normalized Difference Turbidity Index (NDTI) values, along segments of the Ganges River near Ghazipur, Varanasi, and Mirzapur districts in India. Landsat 5 and 8 satellite imagery from 2010, 2015, 2019, and 2021 were analyzed to estimate river temperature and NDTI values for each stretch. Statistical analysis found high correlation between turbidity and temperature for the Varanasi stretch, followed by Mirzapur and Ghazipur. The Varanasi stretch had the highest recorded temperatures and turbidity levels, likely due to industrial and domestic waste flows. The study
Evaluation of the Back Propagation Neural Network for Gravity Mapping IRJET Journal
This document evaluates the ability of back propagation neural networks (BPN) to produce gravity maps. The study trained a BPN model with 646 patterns from a gravity map and satellite image of Khartoum City. The trained model was tested on the training patterns and 162 new patterns. The results showed that the BPN model was unable to produce an accurate gravity map. Therefore, the BPN architecture is not suitable for this application of artificial intelligence in gravity mapping.
IRJET-Evaluation of the Back Propagation Neural Network for Gravity Mapping IRJET Journal
This document evaluates the ability of back propagation neural networks (BPN) to produce gravity maps. The study trained a BPN model with 646 patterns from a gravity map and satellite image of Khartoum City. The trained model was tested on the training patterns and 162 new patterns. The results showed that the BPN model was unable to produce an accurate gravity map. Therefore, the BPN architecture is not suitable for this application of artificial intelligence in gravity mapping.
Time Domain Modelling of Optical Add-drop filter based on Microcavity Ring Re...iosrjce
IOSR Journal of Electronics and Communication Engineering(IOSR-JECE) is a double blind peer reviewed International Journal that provides rapid publication (within a month) of articles in all areas of electronics and communication engineering and its applications. The journal welcomes publications of high quality papers on theoretical developments and practical applications in electronics and communication engineering. Original research papers, state-of-the-art reviews, and high quality technical notes are invited for publications.
This document summarizes the time domain modeling of an optical add-drop filter based on microcavity ring resonators. It uses the Multiresolution Time Domain (MRTD) technique to analyze the transmission characteristics of single and double ring configurations. The MRTD method provides high numerical accuracy while reducing computational burden compared to FDTD. The analysis investigates parameters like gap size, distance between rings, and ring/waveguide width to understand their effects on transmitted power and quality factors. Studies of a 3.4 μm diameter ring show quality factors of several thousand and a free spectral range of 9 THz can be achieved in the 1.55 μm wavelength range.
This document describes research using an artificial neural network (ANN) model to predict the length of hydraulic jumps on rough beds. The ANN model takes the Froude number and relative roughness as inputs and predicts the non-dimensional jump length as the output. Experimental data from previous studies was used to train, validate and test the ANN model. The ANN model was found to predict jump length with higher accuracy than an existing empirical equation, with a coefficient of determination of 0.9596, mean absolute percentage error of 6.9231, and root mean square error of 3.2438. A sensitivity analysis showed that the Froude number has a greater influence on jump length prediction than relative roughness.
This document discusses using k-means clustering to detect minerals from remote sensing images. It begins with an abstract describing using k-means clustering on hyperspectral images to segment and extract features to detect minerals like giacomo. It then provides background on remote sensing, k-means clustering algorithms, and describes the giacomo mineral deposit in Peru that contains silicon dioxide and titanium dioxide. It concludes with discussing using sobel edge detection as part of the mineral detection process from remote sensing images.
Performance analysis of change detection techniques for land use land coverIJECEIAES
Remotely sensed satellite images have become essential to observe the spatial and temporal changes occurring due to either natural phenomenon or man-induced changes on the earth’s surface. Real time monitoring of this data provides useful information related to changes in extent of urbanization, environmental changes, water bodies, and forest. Through the use of remote sensing technology and geographic information system tools, it has become easier to monitor changes from past to present. In the present scenario, choosing a suitable change detection method plays a pivotal role in any remote sensing project. Previously, digital change detection was a tedious task. With the advent of machine learning techniques, it has become comparatively easier to detect changes in the digital images. The study gives a brief account of the main techniques of change detection related to land use land cover information. An effort is made to compare widely used change detection methods used to identify changes and discuss the need for development of enhanced change detection methods.
The document proposes a method to summarize remotely sensed data from over-the-horizon radar systems (OTHR-SW) using sea-land transitions. It involves correlating the received radar echo with a priori knowledge of coastline profiles to geo-reference the data in real-time. This allows the data to be assigned accurate coordinates without needing external data sources. The method is computationally inexpensive and could be used to continuously update an ionospheric model providing information about signal propagation through the ionosphere.
Mechanistic Investigation of FeO/MnO/ZnO Nanocomposites for UV Light Driven P...IRJET Journal
This document summarizes research on FeO/MnO/ZnO nanocomposites for photocatalytic performance under UV light. The nanocomposites (FMZ NCs) were prepared by ultrasonication assisted precipitation and analyzed using various characterization techniques. XRD analysis showed the FMZ NCs had a hexagonal wurtzite structure with an average crystalline size of 32 nm. SEM images revealed a spherical and flower-like morphology. UV-Vis spectroscopy showed the FMZ NCs had a decreased bandgap of 3.04 eV compared to undoped ZnO. Photoluminescence spectroscopy showed strong blue emission at 490 nm. Photocatalytic tests demonstrated the FMZ NCs achieved 91
Improved technique for radar absorbing coatings characterization with rectan...IJECEIAES
For materials characterization, several methods have been developed. Most of them need a sample to be machined prior to testing process. Hence, they are destructive and cannot be used for in-situ radar absorbing coatings testing. This requires employing a suitable measurement technique to extract their electromagnetic properties quickly and accurately. In this paper, the swept frequency of probe reflection technique is proposed for broadband nondestructive radar absorbing coatings characterization using finite flange open-ended rectangular waveguide. The technique is based on the fact that the frequency of measurement is an independent variable of probe’s reflection coefficient by which its data set of selected frequency points can be directly measured in one step by varying the frequency. Finite-difference time-domain (FDTD) method was adopted to calculate probe reflection coefficients at different test conditions. Simple interpolation approximation was employed since they are frequency dependent parameters. Error analysis was numerically performed to evaluate the influences of both flange size and coated material thickness on the accuracy of the measurements, which are carried out on several samples of radar absorbing coatings at X-band to verify the proposed technique. Comparing with the existing methods, the proposed technique simplifies and speeds up measurement process and improves its repeatability and accuracy.
Impact of detector thickness on imaging characteristics of the Siemens Biogra...Anax Fotopoulos
This document summarizes a Monte Carlo study using GATE simulation of a Siemens Biograph DUO PET/CT scanner. It investigates the impact of detector thickness on imaging characteristics by simulating the scanner with LSO detectors of 2cm and 3cm thickness. The results show that increasing thickness from 2cm to 3cm improves detection efficiency, resulting in a sharper energy peak at 511 keV, higher counts, and better energy resolution and signal-to-noise ratio. However, thicker detectors may also delay signal processing and increase device cost and complexity.
Unit Hydrograph (UH) is the most famous and generally utilized technique for analysing and deriving flood hydrograph resulting from a known storm in a basin area. For ungauged catchments, unit hydrograph are derived using either regional unit hydrograph approach. Central Water Commission (CWC) derived the regional unit hydrograph relationships for different sub-zones of India relating to the various unit hydrograph parameters with some prominent physiographic characteristics. The Study Area is located between Latitude 15º57′58′′ N to 16º11′25.6′′ N and 77º18′1′′ E to77º32′5.3′′ E Longitude and covers area of 360.97 km2, having maximum length of 26.17 km. The maximum and minimum elevation of the basin is 533 m and 323 m above MSL, respectively. The Peak discharge of unit hydrograph obtained is 311.469 m3/s. The final cumulative discharge is 1458.55 m3/s.
Dr. Mohan Babu Kuppam has received a PhD in physics from Grenoble University in France. He completed his PhD thesis on modeling ultrafast optoelectronic devices for RF signal processing and characterizing nanomaterials using optical and THz spectroscopy techniques. He has expertise in THz time-domain spectroscopy, optical pump-probe spectroscopy, and modeling electromagnetic devices. He has published several papers in these areas and presented his research at various conferences.
Morphometric Analysis and prioritization of watersheds of Mahanadi River Basi...RINKU MEENA
This document summarizes a student project analyzing watersheds in the Mahanadi River Basin in India using GIS. The objectives are to delineate watersheds and streams using DEM data in QGIS and calculate morphometric parameters to prioritize the watersheds. Methodology includes preprocessing DEM data in QGIS, extracting stream networks and channel networks, and delineating watersheds for five stations. Results show watershed delineation for specific stations. The conclusion discusses using QGIS tools for watershed delineation and how morphometric parameters can inform water and land use planning.
TOP CITED ARTICLE IN 2011 - INTERNATIONAL JOURNAL OF MOBILE NETWORK COMMUNICA...ijmnct
International Journal of Mobile Network Communications & Telematics (IJMNCT) is an open access peer-reviewed journal that addresses the impacts and challenges of mobile communications and telematics. The journal also aims to focus on various areas such as ecommerce, e-governance, Telematics, Telelearning nomadic computing, data management, related software and hardware technologies, and mobile user services. The journal documents practical and theoretical results which make a fundamental contribution for the development of mobile communication technologies
IRJET- Quantitative Morphometric Analysis of Panchganga Basin using GISIRJET Journal
This document presents a quantitative morphometric analysis of the Panchganga river basin in Maharashtra, India using GIS technology. Key findings include:
- The Panchganga basin has a dendritic drainage pattern and is elongated in shape. It has a total of 25043 streams of all orders and a stream length of 7201 km.
- The mean bifurcation ratio across all orders is 4.67. Relief-related parameters show the basin has a relief ratio of 3.78, absolute relief of 508 m, and channel gradient of 2.54%.
- Analysis of linear, areal and relief aspects revealed the basin has experienced significant erosion. There is an immediate need for development to conserve natural resources
Research on Precipitation Prediction Model Based on Extreme Learning Machine Ensemble
Outdoor Air Quality Monitoring with Enhanced Lifetime-enhancing Cooperative Data Gathering and Relaying Algorithm (E-LCDGRA) Based Sensor Network
Data Analytics of an Information System Based on a Markov Decision Process and a Partially Observable Markov Decision Process
On Software Application Database Constraint-driven Design and Development
ESTIMATION OF DEPTH OF RIVER BY BATHYMETRY OF SATELLITE IMAGESIRJET Journal
This document discusses using satellite imagery to estimate the depth of rivers. It outlines previous work using machine learning techniques like random forest and deep learning to process satellite images and generate bathymetry maps. The methodology section describes preprocessing steps like separating land and water pixels and correcting for light attenuation through the water column. It then explains Lyzenga's method for creating depth-invariant indices using ratios between spectral bands to estimate river depth without requiring water depth measurements. Results found combining high-resolution multispectral imagery with machine learning can generate accurate topographical maps for bathymetry. Future work involves applying these deep learning techniques to real satellite data and improving accuracy.
Spectral estimator effects on accuracy of speed-over-ground radarIJECEIAES
Spectral estimation is a critical signal processing step in speed-over-ground (SoG) radar. It is argued that, for accurate speed estimation, spectral estimation should use low bias and variance estimator. However, there is no evaluation on spectral estimation techniques in terms of estimating mean Doppler frequency to date. In this paper, we evaluate two common spectral estimation techniques, namely periodogram based on Fourier transformation and the autoregressive (AR) based on burg algorithm. These spectral estimators are evaluated in terms of their bias and variance in estimating a mean frequency. For this purpose, the spectral estimators are evaluated with different Doppler signals that varied in mean frequency and signal-to-noise ratio (SNR). Results in this study indicates that the periodogram method performs well in most of the tests while the AR method did not perform as well as these but offered a slight improvement over the periodogram in terms of variance.
1. The document describes the growth of (E)-2-nitro-3-phenylallyl hydrogen sulfate crystals using Baylis–Hillman derivatives.
2. The crystals were successfully grown using a low temperature solution growth method and characterized through techniques like X-ray diffraction, infrared spectroscopy, and powder X-ray diffraction.
3. These characterization techniques were used to analyze the crystal structure and confirm the identity and purity of the synthesized compound.
FRACTAL ANTENNA FOR AEROSPACE NAVIGATIONrupleenkaur23
This document is a dissertation submitted by Rupleen Kaur for the partial fulfillment of the requirements for the award of Master of Technology degree in Electronics and Communication Engineering from Guru Nanak Dev University. The dissertation is on the design of a fractal microstrip patch antenna for aerospace navigation. It discusses the design and simulation of different fractal microstrip patch antenna configurations using HFSS software to achieve multiband operation for aerospace navigation applications. The simulated results of return loss, radiation pattern, gain and VSWR of the different antenna designs are presented and validated.
Stressed Coral Reef Identification Using Deep Learning CNN Techniques
The Application of Information Systems to Improve Ambulance Response Times in the UK
Practical Considerations for Implementing Adaptive Acoustic Noise Cancellation in Commercial Earbuds
Development of Technology and Equipment for Non-destructive Testing of Defects in Sewing Mandrels of a Three-roll Screw Mill 30-80
Control and Treatment of Bone Cancer: A Novel Theoretical Study
Enhancing Semantic Segmentation through Reinforced Active Learning: Combating Dataset Imbalances and Bolstering Annotation Efficiency
Snowfall Shift and Precipitation Variability over Sikkim Himalaya Attributed to Elevation-Dependent Warming
Spatial and Temporal Variation of Particulate Matter (PM10 and PM2.5) and Its Health Effects during the Haze Event in Malaysia
Problems and opportunities for biometeorological assessment of conditions cold season
Case Study of Coastal Fog Events in Senegal Using LIDAR Ceilometer
Assessing the Impact of Gas Flaring and Carbon Dioxide Emissions on Precipitation Patterns in the Niger Delta Region of Nigeria Using Geospatial Analysis
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Performance analysis of change detection techniques for land use land coverIJECEIAES
Remotely sensed satellite images have become essential to observe the spatial and temporal changes occurring due to either natural phenomenon or man-induced changes on the earth’s surface. Real time monitoring of this data provides useful information related to changes in extent of urbanization, environmental changes, water bodies, and forest. Through the use of remote sensing technology and geographic information system tools, it has become easier to monitor changes from past to present. In the present scenario, choosing a suitable change detection method plays a pivotal role in any remote sensing project. Previously, digital change detection was a tedious task. With the advent of machine learning techniques, it has become comparatively easier to detect changes in the digital images. The study gives a brief account of the main techniques of change detection related to land use land cover information. An effort is made to compare widely used change detection methods used to identify changes and discuss the need for development of enhanced change detection methods.
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Improved technique for radar absorbing coatings characterization with rectan...IJECEIAES
For materials characterization, several methods have been developed. Most of them need a sample to be machined prior to testing process. Hence, they are destructive and cannot be used for in-situ radar absorbing coatings testing. This requires employing a suitable measurement technique to extract their electromagnetic properties quickly and accurately. In this paper, the swept frequency of probe reflection technique is proposed for broadband nondestructive radar absorbing coatings characterization using finite flange open-ended rectangular waveguide. The technique is based on the fact that the frequency of measurement is an independent variable of probe’s reflection coefficient by which its data set of selected frequency points can be directly measured in one step by varying the frequency. Finite-difference time-domain (FDTD) method was adopted to calculate probe reflection coefficients at different test conditions. Simple interpolation approximation was employed since they are frequency dependent parameters. Error analysis was numerically performed to evaluate the influences of both flange size and coated material thickness on the accuracy of the measurements, which are carried out on several samples of radar absorbing coatings at X-band to verify the proposed technique. Comparing with the existing methods, the proposed technique simplifies and speeds up measurement process and improves its repeatability and accuracy.
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This document summarizes a Monte Carlo study using GATE simulation of a Siemens Biograph DUO PET/CT scanner. It investigates the impact of detector thickness on imaging characteristics by simulating the scanner with LSO detectors of 2cm and 3cm thickness. The results show that increasing thickness from 2cm to 3cm improves detection efficiency, resulting in a sharper energy peak at 511 keV, higher counts, and better energy resolution and signal-to-noise ratio. However, thicker detectors may also delay signal processing and increase device cost and complexity.
Unit Hydrograph (UH) is the most famous and generally utilized technique for analysing and deriving flood hydrograph resulting from a known storm in a basin area. For ungauged catchments, unit hydrograph are derived using either regional unit hydrograph approach. Central Water Commission (CWC) derived the regional unit hydrograph relationships for different sub-zones of India relating to the various unit hydrograph parameters with some prominent physiographic characteristics. The Study Area is located between Latitude 15º57′58′′ N to 16º11′25.6′′ N and 77º18′1′′ E to77º32′5.3′′ E Longitude and covers area of 360.97 km2, having maximum length of 26.17 km. The maximum and minimum elevation of the basin is 533 m and 323 m above MSL, respectively. The Peak discharge of unit hydrograph obtained is 311.469 m3/s. The final cumulative discharge is 1458.55 m3/s.
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- The mean bifurcation ratio across all orders is 4.67. Relief-related parameters show the basin has a relief ratio of 3.78, absolute relief of 508 m, and channel gradient of 2.54%.
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On Software Application Database Constraint-driven Design and Development
ESTIMATION OF DEPTH OF RIVER BY BATHYMETRY OF SATELLITE IMAGESIRJET Journal
This document discusses using satellite imagery to estimate the depth of rivers. It outlines previous work using machine learning techniques like random forest and deep learning to process satellite images and generate bathymetry maps. The methodology section describes preprocessing steps like separating land and water pixels and correcting for light attenuation through the water column. It then explains Lyzenga's method for creating depth-invariant indices using ratios between spectral bands to estimate river depth without requiring water depth measurements. Results found combining high-resolution multispectral imagery with machine learning can generate accurate topographical maps for bathymetry. Future work involves applying these deep learning techniques to real satellite data and improving accuracy.
Spectral estimator effects on accuracy of speed-over-ground radarIJECEIAES
Spectral estimation is a critical signal processing step in speed-over-ground (SoG) radar. It is argued that, for accurate speed estimation, spectral estimation should use low bias and variance estimator. However, there is no evaluation on spectral estimation techniques in terms of estimating mean Doppler frequency to date. In this paper, we evaluate two common spectral estimation techniques, namely periodogram based on Fourier transformation and the autoregressive (AR) based on burg algorithm. These spectral estimators are evaluated in terms of their bias and variance in estimating a mean frequency. For this purpose, the spectral estimators are evaluated with different Doppler signals that varied in mean frequency and signal-to-noise ratio (SNR). Results in this study indicates that the periodogram method performs well in most of the tests while the AR method did not perform as well as these but offered a slight improvement over the periodogram in terms of variance.
1. The document describes the growth of (E)-2-nitro-3-phenylallyl hydrogen sulfate crystals using Baylis–Hillman derivatives.
2. The crystals were successfully grown using a low temperature solution growth method and characterized through techniques like X-ray diffraction, infrared spectroscopy, and powder X-ray diffraction.
3. These characterization techniques were used to analyze the crystal structure and confirm the identity and purity of the synthesized compound.
FRACTAL ANTENNA FOR AEROSPACE NAVIGATIONrupleenkaur23
This document is a dissertation submitted by Rupleen Kaur for the partial fulfillment of the requirements for the award of Master of Technology degree in Electronics and Communication Engineering from Guru Nanak Dev University. The dissertation is on the design of a fractal microstrip patch antenna for aerospace navigation. It discusses the design and simulation of different fractal microstrip patch antenna configurations using HFSS software to achieve multiband operation for aerospace navigation applications. The simulated results of return loss, radiation pattern, gain and VSWR of the different antenna designs are presented and validated.
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Evidence of Jet Activity from the Secondary Black Hole in the OJ 287 Binary S...Sérgio Sacani
Wereport the study of a huge optical intraday flare on 2021 November 12 at 2 a.m. UT in the blazar OJ287. In the binary black hole model, it is associated with an impact of the secondary black hole on the accretion disk of the primary. Our multifrequency observing campaign was set up to search for such a signature of the impact based on a prediction made 8 yr earlier. The first I-band results of the flare have already been reported by Kishore et al. (2024). Here we combine these data with our monitoring in the R-band. There is a big change in the R–I spectral index by 1.0 ±0.1 between the normal background and the flare, suggesting a new component of radiation. The polarization variation during the rise of the flare suggests the same. The limits on the source size place it most reasonably in the jet of the secondary BH. We then ask why we have not seen this phenomenon before. We show that OJ287 was never before observed with sufficient sensitivity on the night when the flare should have happened according to the binary model. We also study the probability that this flare is just an oversized example of intraday variability using the Krakow data set of intense monitoring between 2015 and 2023. We find that the occurrence of a flare of this size and rapidity is unlikely. In machine-readable Tables 1 and 2, we give the full orbit-linked historical light curve of OJ287 as well as the dense monitoring sample of Krakow.
SDSS1335+0728: The awakening of a ∼ 106M⊙ black hole⋆Sérgio Sacani
Context. The early-type galaxy SDSS J133519.91+072807.4 (hereafter SDSS1335+0728), which had exhibited no prior optical variations during the preceding two decades, began showing significant nuclear variability in the Zwicky Transient Facility (ZTF) alert stream from December 2019 (as ZTF19acnskyy). This variability behaviour, coupled with the host-galaxy properties, suggests that SDSS1335+0728 hosts a ∼ 106M⊙ black hole (BH) that is currently in the process of ‘turning on’. Aims. We present a multi-wavelength photometric analysis and spectroscopic follow-up performed with the aim of better understanding the origin of the nuclear variations detected in SDSS1335+0728. Methods. We used archival photometry (from WISE, 2MASS, SDSS, GALEX, eROSITA) and spectroscopic data (from SDSS and LAMOST) to study the state of SDSS1335+0728 prior to December 2019, and new observations from Swift, SOAR/Goodman, VLT/X-shooter, and Keck/LRIS taken after its turn-on to characterise its current state. We analysed the variability of SDSS1335+0728 in the X-ray/UV/optical/mid-infrared range, modelled its spectral energy distribution prior to and after December 2019, and studied the evolution of its UV/optical spectra. Results. From our multi-wavelength photometric analysis, we find that: (a) since 2021, the UV flux (from Swift/UVOT observations) is four times brighter than the flux reported by GALEX in 2004; (b) since June 2022, the mid-infrared flux has risen more than two times, and the W1−W2 WISE colour has become redder; and (c) since February 2024, the source has begun showing X-ray emission. From our spectroscopic follow-up, we see that (i) the narrow emission line ratios are now consistent with a more energetic ionising continuum; (ii) broad emission lines are not detected; and (iii) the [OIII] line increased its flux ∼ 3.6 years after the first ZTF alert, which implies a relatively compact narrow-line-emitting region. Conclusions. We conclude that the variations observed in SDSS1335+0728 could be either explained by a ∼ 106M⊙ AGN that is just turning on or by an exotic tidal disruption event (TDE). If the former is true, SDSS1335+0728 is one of the strongest cases of an AGNobserved in the process of activating. If the latter were found to be the case, it would correspond to the longest and faintest TDE ever observed (or another class of still unknown nuclear transient). Future observations of SDSS1335+0728 are crucial to further understand its behaviour. Key words. galaxies: active– accretion, accretion discs– galaxies: individual: SDSS J133519.91+072807.4
Anti-Universe And Emergent Gravity and the Dark UniverseSérgio Sacani
Recent theoretical progress indicates that spacetime and gravity emerge together from the entanglement structure of an underlying microscopic theory. These ideas are best understood in Anti-de Sitter space, where they rely on the area law for entanglement entropy. The extension to de Sitter space requires taking into account the entropy and temperature associated with the cosmological horizon. Using insights from string theory, black hole physics and quantum information theory we argue that the positive dark energy leads to a thermal volume law contribution to the entropy that overtakes the area law precisely at the cosmological horizon. Due to the competition between area and volume law entanglement the microscopic de Sitter states do not thermalise at sub-Hubble scales: they exhibit memory effects in the form of an entropy displacement caused by matter. The emergent laws of gravity contain an additional ‘dark’ gravitational force describing the ‘elastic’ response due to the entropy displacement. We derive an estimate of the strength of this extra force in terms of the baryonic mass, Newton’s constant and the Hubble acceleration scale a0 = cH0, and provide evidence for the fact that this additional ‘dark gravity force’ explains the observed phenomena in galaxies and clusters currently attributed to dark matter.
Embracing Deep Variability For Reproducibility and Replicability
Abstract: Reproducibility (aka determinism in some cases) constitutes a fundamental aspect in various fields of computer science, such as floating-point computations in numerical analysis and simulation, concurrency models in parallelism, reproducible builds for third parties integration and packaging, and containerization for execution environments. These concepts, while pervasive across diverse concerns, often exhibit intricate inter-dependencies, making it challenging to achieve a comprehensive understanding. In this short and vision paper we delve into the application of software engineering techniques, specifically variability management, to systematically identify and explicit points of variability that may give rise to reproducibility issues (eg language, libraries, compiler, virtual machine, OS, environment variables, etc). The primary objectives are: i) gaining insights into the variability layers and their possible interactions, ii) capturing and documenting configurations for the sake of reproducibility, and iii) exploring diverse configurations to replicate, and hence validate and ensure the robustness of results. By adopting these methodologies, we aim to address the complexities associated with reproducibility and replicability in modern software systems and environments, facilitating a more comprehensive and nuanced perspective on these critical aspects.
https://hal.science/hal-04582287
Mending Clothing to Support Sustainable Fashion_CIMaR 2024.pdfSelcen Ozturkcan
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PPT on Alternate Wetting and Drying presented at the three-day 'Training and Validation Workshop on Modules of Climate Smart Agriculture (CSA) Technologies in South Asia' workshop on April 22, 2024.
The cost of acquiring information by natural selectionCarl Bergstrom
This is a short talk that I gave at the Banff International Research Station workshop on Modeling and Theory in Population Biology. The idea is to try to understand how the burden of natural selection relates to the amount of information that selection puts into the genome.
It's based on the first part of this research paper:
The cost of information acquisition by natural selection
Ryan Seamus McGee, Olivia Kosterlitz, Artem Kaznatcheev, Benjamin Kerr, Carl T. Bergstrom
bioRxiv 2022.07.02.498577; doi: https://doi.org/10.1101/2022.07.02.498577
BIRDS DIVERSITY OF SOOTEA BISWANATH ASSAM.ppt.pptxgoluk9330
Ahota Beel, nestled in Sootea Biswanath Assam , is celebrated for its extraordinary diversity of bird species. This wetland sanctuary supports a myriad of avian residents and migrants alike. Visitors can admire the elegant flights of migratory species such as the Northern Pintail and Eurasian Wigeon, alongside resident birds including the Asian Openbill and Pheasant-tailed Jacana. With its tranquil scenery and varied habitats, Ahota Beel offers a perfect haven for birdwatchers to appreciate and study the vibrant birdlife that thrives in this natural refuge.
Compositions of iron-meteorite parent bodies constrainthe structure of the pr...Sérgio Sacani
Magmatic iron-meteorite parent bodies are the earliest planetesimals in the Solar System,and they preserve information about conditions and planet-forming processes in thesolar nebula. In this study, we include comprehensive elemental compositions andfractional-crystallization modeling for iron meteorites from the cores of five differenti-ated asteroids from the inner Solar System. Together with previous results of metalliccores from the outer Solar System, we conclude that asteroidal cores from the outerSolar System have smaller sizes, elevated siderophile-element abundances, and simplercrystallization processes than those from the inner Solar System. These differences arerelated to the formation locations of the parent asteroids because the solar protoplane-tary disk varied in redox conditions, elemental distributions, and dynamics at differentheliocentric distances. Using highly siderophile-element data from iron meteorites, wereconstruct the distribution of calcium-aluminum-rich inclusions (CAIs) across theprotoplanetary disk within the first million years of Solar-System history. CAIs, the firstsolids to condense in the Solar System, formed close to the Sun. They were, however,concentrated within the outer disk and depleted within the inner disk. Future modelsof the structure and evolution of the protoplanetary disk should account for this dis-tribution pattern of CAIs.
JAMES WEBB STUDY THE MASSIVE BLACK HOLE SEEDSSérgio Sacani
The pathway(s) to seeding the massive black holes (MBHs) that exist at the heart of galaxies in the present and distant Universe remains an unsolved problem. Here we categorise, describe and quantitatively discuss the formation pathways of both light and heavy seeds. We emphasise that the most recent computational models suggest that rather than a bimodal-like mass spectrum between light and heavy seeds with light at one end and heavy at the other that instead a continuum exists. Light seeds being more ubiquitous and the heavier seeds becoming less and less abundant due the rarer environmental conditions required for their formation. We therefore examine the different mechanisms that give rise to different seed mass spectrums. We show how and why the mechanisms that produce the heaviest seeds are also among the rarest events in the Universe and are hence extremely unlikely to be the seeds for the vast majority of the MBH population. We quantify, within the limits of the current large uncertainties in the seeding processes, the expected number densities of the seed mass spectrum. We argue that light seeds must be at least 103 to 105 times more numerous than heavy seeds to explain the MBH population as a whole. Based on our current understanding of the seed population this makes heavy seeds (Mseed > 103 M⊙) a significantly more likely pathway given that heavy seeds have an abundance pattern than is close to and likely in excess of 10−4 compared to light seeds. Finally, we examine the current state-of-the-art in numerical calculations and recent observations and plot a path forward for near-future advances in both domains.
Advances in Geological and Geotechnical Engineering Research | Vol.2, Iss.2 April 2020
1.
2. Ph.D in Civil Engineering, Aristotle University of Thessaloniki, Greece. Pro-
fessor of Geotechnical Engineering and Architectural Preservation of historic buildings, Conservation Department, faculty of
archaeology, Cairo university., Egypt
Editor-in-Chief
Professor. Dr. Sayed Hemeda
Editorial Board Members
Reza Jahanshahi, Iran
Salvatore Grasso, Italy
Fangming Zeng, China
Shenghua Cui, China
Golnaz Jozanikohan, Iran
Mehmet Irfan Yesilnacar, Turkey
Ziliang Liu, China
Abrar Niaz, Pakistan
Sunday Ojochogwu Idakwo, Nigeria
Angelo Doglioni, Italy
Jianwen Pan, China
Changjiang Liu, China
Wen-Chieh Cheng, China
Wei Duan, China
Jule Xiao, China
Intissar Farid, Tunisia
Jalal Amini, Iran
Jun Xiao, China
Jin Gao, China
Chong Peng, China
Bingqi Zhu, China
Zheng Han,China
Vladimir Aleksandrovich Naumov, Russian Federation
Dongdong Wang, China
Jian-Hong Wu, Taiwan
Abdessamad Didi, Morocco
Abdel Majid Messadi, Tunisia
Himadri Bhusan Sahoo, India
Ashraf M.T. Elewa, Egypt
Jiang-Feng Liu, China
Vasiliy Anatol’evich Mironov, Russian Federation
Maysam Abedi, Iran
Anderson José Maraschin, Brazil
Alcides Nobrega Sial, Brazil
Renmao Yuan, China
Ezzedine Saïdi, Tunisia
Xiaoxu Jia, China
Mokhles Kamal Azer, Egypt
Ntieche Benjamin, Cameroon
Sandeep Kumar Soni, Ethiopia
Jinliang Zhang, China
Keliu Wu, China
Kamel Bechir Maalaoui, Tunisia
Fernando Carlos Lopes,Portugal
Shimba Daniel Kwelwa,Tanzania
Jian Wang, China
Antonio Zanutta, Italy
Xiaochen Wei, China
Nabil H. Swedan, United States
Mirmahdi Seyedrahimi-Niaraq, Iran
Bo Li, China
Irfan Baig, Norway
Shaoshuai Shi, China
Sumit Kumar Ghosh, India
Bojan Matoš, Croatia
Roberto Wagner Lourenço, Brazil
Massimo Ranaldi, Italy
Zaman Malekzade, Iran
Xiaohan Yang, Australia
Gehan Mohammed, Egypt
Márton Veress, Hungary
Vincenzo Amato, Italy
Fangqiang Wei, China
Sirwan Hama Ahmed, Iraq
Siva Prasad BNV, India
Ahm Radwan, Egypt
Yasir Bashir, Malaysia
Nadeem Ahmad Bhat, India
Boonnarong Arsairai, Thailand
Neil Edwin Matthew Dickson, Norfolk Island
Mojtaba Rahimi, Iran
Mohamad Syazwan Mohd Sanusi, Malaysia
Sohrab Mirassi, Iran
Gökhan Büyükkahraman, Turkey
Kirubakaran Muniraj, India
Nazife Erarslan, Turkey
Prasanna Lakshitha Dharmapriyar, Sri Lanka
Harinandan Kumar, India
Amr Abdelnasser Khalil, Egypt
Zhouhua Wang, China
Frederico Scarelli, Brazil
Bahman Soleimani,Iran
Luqman Kolawole Abidoye,Nigeria
Tongjun Chen,China
Vinod Kumar Gupta,France
Waleed Sulaiman Shingaly,Iraq
Saeideh Samani,Iran
Khalid Elyas Mohamed E.A.,Saudi Arabia
Xinjie Liu,China
Mualla Cengiz,Turkey
Hamdalla Abdel-Gawad Wanas,Saudi Arabia
Peace Nwaerema,Nigeria
Gang Li,China
Nchofua Festus Biosengazeh,Cameroon
Williams Nirorowan Ofuyah,Nigeria
Ashok Sigdel,Nepal
Richmond Uwanemesor Ideozu,Nigeria
Ramesh Man Tuladhar,Nepal
Swostik Kumar Adhikari,Nepal
3. Professor. Dr. Sayed Hemeda
Journal of
Geological Research
Editor-in-Chief
Volume 2 Issue 2 · April 2020· ISSN 2630-4961 (Online)
5. 1
Journal of Geological Research | Volume 02 | Issue 02 | April 2020
Distributed under creative commons license 4.0 DOI: https://doi.org/10.30564/jgr.v2i2.2046
Journal of Geological Research
https://ojs.bilpublishing.com/index.php/jgr-a
ARTICLE
Seismic Edge Detection by Application of Cepstral Decomposition to
Data Driven Modeled Geologic Channel Feature in Niger Delta
Orji, O.M.1*
Ugwu, S.A.2
Ofuyah, W.N.3
1. Department of Petroleum Engineering and Geoscience, Petroleum Training Institute, Effurun, Nigeria
2. Department of Geology, University of Port Harcourt, Nigeria
3. Department of Earth Sciences, Federal University of Petroleum Resources, Effurun, Nigeria
ARTICLE INFO ABSTRACT
Article history
Received: 23 June 2020
Accepted: 8 July 2020
Published Online: 30 July 2020
Seismic edge detection algorithm unmasks blurred discontinuity in an
image and its efficiency is dependent on the precession of the processing
scheme adopted. Data-driven modeling is a fast machine learning scheme
and a formal automatic version of the empirical approach in existence for
a long time and which can be used in many different contexts. Here, a de-
sired algorithm that can identify masked connection and correlation from
a set of observations is built and used. Geologic models of hydrocarbon
reservoirs facilitate enhanced visualization, volumetric calculation, well
planning and prediction of migration path for fluid. In order to obtain new
insights and test the mappability of a geologic feature, spectral decompo-
sition techniques i.e. Discrete Fourier Transform (DFT), etc and Cepstral
decomposition techniques, i.e Complex Cepstral Transform (CCT), etc can
be employed. Cepstral decomposition is a new approach that extends the
widely used process of spectral decomposition which is rigorous when an-
alyzing very subtle stratigraphic plays and fractured reservoirs. This paper
presents the results of the application of DFT and CCT to a two dimension-
al, 50Hz low impedance Channel sand model, representing typical geologic
environment around a prospective hydrocarbon zone largely trapped in
various types of channel structures. While the DFT represents the frequen-
cy and phase spectra of a signal, assumes stationarity and highlights the
average properties of its dominant portion, assuming analytical, the CCT
represents the quefrency and saphe cepstra of a signal in quefrency domain.
The transform filters the field data recorded in time domain, and recovers
lost sub-seismic geologic information in quefrency domain by separating
source and transmission path effects. Our algorithm is based on fast Fou-
rier transform (FFT) techniques and the programming code was written
within Matlab software. It was developed from first principles and outside
oil industry’s interpretational platform using standard processing routines.
The results of the algorithm, when implemented on both commercial and
general platforms, were comparable. The cepstral properties of the channel
model indicate that cepstral attributes can be utilized as powerful tool in
exploration problems to enhance visualization of small scale anomalies
and obtain reliable estimates of wavelet and stratigraphic parameters. The
practical relevance of this investigation is illustrated by means of sample
results of spectral and cepstral attribute plots and pseudo-sections of phase
and saphe constructed from the model data. The cepstral attributes reveal
more details in terms of quefrency required for clearer imaging and better
interpretation of subtle edges/discontinuities, sand-shale interbedding, dif-
ferences in lithology. These positively impact on production as they serve
as basis for the interpretation of similar geologic situations in field data.
Keywords:
Complex Cepstral Transform
Fourier transform
Gamnitude
Quefrency
Saphe
*Corresponding Author:
Orji, O.M.,
Department of Petroleum Engineering and Geoscience, Petroleum Training Institute, Effurun, Nigeria;
Email: orji_om@pti.edu.ng
6. 2
Journal of Geological Research | Volume 02 | Issue 02 | April 2020
Distributed under creative commons license 4.0
1. Introduction
S
eismic edge detection algorithm unambiguously
unmasks blurred discontinuity in an image and its
efficiency is dependent on the precession of the
processing scheme adopted. Data-driven modeling is a
fast developing machine learning scheme and a formal
usually automatic version of the empirical approach in
existence for long time and which can be used in many
different contexts, i.e. when manual processing and infor-
mal observations are used. Here, a desired algorithm that
can identify masked connection and correlation from a set
of observations or data is built and used.
Geologic models of hydrocarbon reservoirs facilitate
enhanced visualization, volumetric calculation, well plan-
ning and prediction of migration path for fluid. In order to
obtain new insights and test the mappability of a geologic
feature, spectral decomposition techniques i.e. Discrete
Fourier Transform (DFT), Short-Time Fourier Transform
(STFT), etc and Cepstral decomposition techniques,
i.e. Real Cepstral Transform (RCT), Complex Cepstral
Transform (CCT), etc. can be employed. Cepstral decom-
position is a new approach that extends the widely used
process of spectral decomposition which is rigorous when
analyzing very subtle stratigraphic plays and fractured
reservoirs.
This paper presents the results of the application of
DFT and CCT to a two dimensional, 50Hz low impedance
Channel sand model, representing typical geologic envi-
ronment around a prospective hydrocarbon zone. A large
number of oil and gas fields have been found to be trapped
in various types of channel structures. While the DFT
represents the frequency and phase spectra of a signal in
frequency domain, assumes stationarity and highlights
the average properties of its dominant portion, assuming
analytical, the CCT represents the quefrency and saphe
cepstra of a signal in quefrency domain. The transform
filters the field data recorded in time domain, and recovers
lost sub-seismic geologic information in quefrency do-
main by separating source and transmission path effects.
Our algorithm is based on fast Fourier transform (FFT)
techniques and the programming code was written within
Matlab software. It was developed from first principles
and outside oil industry’s interpretational platform using
standard processing routines. The results of the algorithm,
when implemented on both oil industry (e.g. Kingdom
Suite, Petrel) and general platforms, were comparable.
The cepstral properties of the channel model indicate
that cepstral attributes can be utilized as powerful tool in
exploration problems to enhance visualization of small
scale anomalies and obtain reliable estimates of wavelet
and stratigraphic parameters. The practical relevance of
this investigation is illustrated by means of sample results
of spectral and cepstral attribute plots and pseudo-sections
of phase and saphe constructed from the model data. The
cepstral attributes reveal more details in terms of quefren-
cy required for clearer imaging and better interpretation
of subtle edges/discontinuities, sand-shale interbedding,
differences in lithology and generally better delineation
and delimitation of stratigraphic features than the spectral
attributes.
Seismic visibility is enhanced through the change of
the seismic data outlook from the standard amplitude mea-
surement to a new domain in order separate fact from arti-
fact in seismic processing and interpretation. Seismic data
are usually contaminated by noise, even when the data has
been migrated reasonably well and are multiple-free [1]
. In
frequency and quefrency domains, the technique separates
fact from artifact and better geologic picture emerges.
This is necessary in hydrocarbon reservoir characteriza-
tion since a clear knowledge of a reservoir facilitates en-
hanced recovery [2]
. The Cepstrum is the Fourier transform
of the log of the spectrum of the data [3]
.
This paper is an attempt to describe aspect of innova-
tive and unconventional methods and new technology
developed for application in areas of uncertain data or
complex geology such as in deep waters, marginal fields,
fractured zones, etc. for the purpose of their development.
The presentation outline is as follows: Section one, this
section, introduces the concept of edge detection, model
types, and interpretation in more resolving domains rather
than in time, (natural data acquisition domain), and ge-
ology of the study area. In section two, the concepts of
Spectral and Cepstral decompositions are addressed, while
in section three, the methodology adopted is presented.
Section four contains the results and analysis and finally,
in section 5, the conclusions of this study are highlighted.
Geologic Background
The source of our data is the ‘Tomboy’ Basin in Niger
delta region (Figure 1). The region is a prolific hydro-
carbon province formed during three depositional cycles
from middle cretaceous to recent in Nigeria. It is located
in Nigeria between latitudes 30
N and 60
N and longitudes
40
301
E and 90
E and bounded in the west by the Benin
flank, in the east by the Calabar flank and in the north by
the older tectonic elements e.g. Anambra basin, Abakaliki
uplift and the Afikpo syncline. The Niger delta basin is
one of the largest subaerial basins in Africa. It has a sub-
aerial area of about 75,000 km2
, a total area of 300,000
km2
, and a sediment fill of 500,000 km3 [4]
. The region is
a large arcuate delta of the destructive wave dominated
DOI: https://doi.org/10.30564/jgr.v2i2.2046
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Journal of Geological Research | Volume 02 | Issue 02 | April 2020
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type and is divided into the continental, transitional and
marine environments. In order of deposition, a sequence
of under compacted marine shale (Akata formation, depth
from about 11121 ft, and main source rock of the Niger
delta), is overlain by paralic or sand/shale deposits (Agba-
da formation, depth from about 7180-11121ft, are present
throughout. This is the major oil and natural gas bearing
facies in the basin. The paralic interval is overlain by a
varying thickness of continental sands (Benin formation,
depth from 0-about 6000ft, contains no commercial hy-
drocarbons, although several minor oil and gas stringers
are present) [5,6]
. Growth faults strongly influenced the
sedimentation pattern and thickness distribution of sands
and shales. Oil and gas are trapped by roll-over anticlines
and growth faults [7]
. The ages of the formations become
progressively younger in a down-dip direction and range
from Paleocene to Recent [8]
). Hydrocarbon is trapped in
many different trap configurations. The implication of this
is that geological and geophysical analyses must be so-
phisticated, a departure from the conventional, in order to
unmask hidden/by-passed reserves, usually stratigraphic
and laden with huge hydrocarbon accumulation.
N
(a) Tomboy Field, Niger Delta, cited in[9]
(b) Tomboy Field, Niger Delta: Base map of survey area showing the
arbitrary line (in Red) in the field
Figure 1. Tomboy Field, Niger Delta: (a) Bathymetric
Sea‐floor image of the Niger Delta obtained from a
dense grid of two-dimensional seismic reflection profiles
and the global bathymetric database showing the location
of the Study Area (b) Base map of survey area showing
the Arbitrary line(in Red). The Arbitrary line connects the
entire six wells (black dots). The well under consideration
is TMB 06 is deviated and located at coordinates inline
6009 and crossline 1565, right of the vertical line
2. Theory
2.1 Fourier Transform
Fourier analysis decomposes a signal into its sinusoidal
components based on the assumption that the frequency
is not changing with time (stationary). Fourier transform
allows insights of average properties of a reasonably large
portion of trace but it does not ordinarily permit exam-
ination of local variations) [10]
. This is because the convo-
lution of a source wavelet with a random geologic series
of wide window produces an amplitude spectrum that re-
sembles the wavelet. To obtain a wavelet overprint which
reflects the local acoustic properties and thickness of the
subsurface layers, a narrow window as in STFT can be
adopted. In practice, the standard algorithm used in digital
computers for the computation of Fourier transform is the
Fast Fourier Transform (FFT/DFT).
2.2 Discrete Fourier Transform (DFT)
The Discrete Fourier Transform (DFT) is the digital
equivalent of the continuous Fourier transform and is ex-
pressed as
f w f t iwt
exp
( )
= −
t
w
∑
= −∞
−∞
( ) ( )(1)
While the inverse discrete Fourier transform is
f t f w iwt
exp
( )
t
w
∑
= −∞
−∞
= ( ) ( ) (2)
where, w is the Fourier dual of the variable “t”. If ‘t’
signifies time, then ‘w’ is the
angular frequency which is related to the linear (tempo-
ral frequency) ‘f’. Also, F(w)
comprises both real (Fr(w) and imaginary Fi(w) compo-
nents. Hence
F w Fr w iFi w
( ) ( ) ( )
= + (3)
A w F w F w
[ ]
( )
= +
r i
2 2 1/2
( ) ( ) (4)
ϕ( ) tan
w = −1
F w
F w
r
i ( )
( )
(5)
Where A(w) ard φ (w) are the amplitude and phase
spectra respectively [11]
2.3 Cepstral Transform (CT)
Cepstral decomposition is a new approach that extends
DOI: https://doi.org/10.30564/jgr.v2i2.2046
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Journal of Geological Research | Volume 02 | Issue 02 | April 2020
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the widely used process of spectral decomposition. This
measures bed thickness even when the bed itself cannot
be interpreted [12]
. While spectral decomposition maps are
typically interpreted qualitatively using geomorphologic
pattern recognition or semi quantitatively, to infer relative
thickness variability Spectral decomposition is rigorous
when analyzing subtle stratigraphic plays and fractured
reservoirs. The Cepstrum processing technique gives a
solution of other signals which have been convolved or
multiplied in time domain because the operation of the
nonlinear mapping can be processed by the generalized
linear system (Homomorphic system) [13.
Cepstral analysis
is a special case of Homomorphic filtering. Homomor-
phic filtering is a generalized technique involving (a) a
nonlinear mapping to a different domain where (b) linear
filters are applied, followed by (c) mapping back to the
original domain. The independent variable of the Ceps-
trum is nominally time though not in the sense of a signal
in the time domain, and of a Cepstral graph is called the
Quefrency but it is interpreted as a frequency since we
are treating the log spectrum as a waveform. To empha-
size this interchanging of domains, [14]
coined the term
Cepstrum by swapping the order of the letters in the word
Spectrum. The name of the independent variable of the
Cepstrum is known as a Quefrency, and the linear filtering
operation is known as Liftering. The Cepstrum is useful
because it separates source and filter and can be applied to
detect local periodicity. There is a complex cepstrum [15]
and a real Cepstrum. In the “real Cepstrum”, as opposed
to the complex Cepstrum used here, only the log ampli-
tude of a spectrum is used [16].
Complex Cepstrum uses
the information of both the magnitude and phase spectra
from the observed signal. The complex Cepstrum method
is used to recover signals generated by a convolution pro-
cess and has been called Homomorphic deconvolution [17]
.
The applications can be found from seismic signal, speech
and imaging processing. Kepstrum was named by [18]
and
used for seismic signal analysis, although the literature
on its application is limited. The Kepstrum and complex
Cepstrum give almost same results for most purpose.
The Cepstrum can be defined as the Fourier transform
of the log of the spectrum. Given a noise free trace in time
(t) domain as x (t) obtained by convolution of a wavelet
w(t) and reflectivity series r(t) and assuming X (f), W (f)
and R (f) are their frequency domain equivalents, then,
Since the Fourier transform is a linear operation, the Cep-
strum is
F X F W F R
[ln (mod )] [ln(mod ) [ln (mod )]
= + (6)
To distinguish this new domain from time, to which
it is dimensionally equivalent, several new terms were
coined. For instance, frequency is transformed to Quefren-
cy, Magnitude to Gamnitude, Phase to Saphe, Filtering to
Liftering, even Analysis to Alanysis. Only Cepstrum and
Quefrency are in widespread today, though liftering is
popular in some fields [19]
.
3. Methodology
3.1 Field Data Analysis
The 3D seismic and well data used in this study were
obtained over ‘Tomboy’ field by Chevron Corporation Ni-
geria. The field data comprises a base map, a suite of logs
from six (6) wells, and four hundred (400) seismic Inlines
and 220 Crosslines. Some of the log types provided are
Gamma-Ray (GR), Self-Potential (SP), Resistivity, Den-
sity, Sonic, etc. Lithologic logs of Gamma-Ray and Self
Potential were first plotted to identify the sand (hydrocar-
bon) unit of interest and then correlated with Resistivity
logs. This Interval corresponds to 2648-2672 milliseconds
using time-depth conversion. It is important to state that
rather than use measured seismic line near the well (TMB
06) under examination for seismic-to-well tie, as is tradi-
tionally done, a line (arbitrary) connecting the entire wells
was constructed to enhance the seismic data quality for
the tie since it integrates the general geologic information
in the survey.
3.2 Computation and Decomposition of Channel
Model
We computed the frequency attributes of a Channel sand
model of low impedance.. The Channel represents spatial
variation of the distribution of sediments and rocks in
the subsurface and can exist anywhere from river basins
to deep-sea environments. Several of the world’s oil and
gas fields are developed from channel environments. It
was examined with a zero phase Ricker wavelet of 50Hz
center frequency using the fast Fourier transform (FFT)
convolution technique. The Ricker wavelet was convolved
with a four-layer reflectivity series, where the third layer
is the channel feature. The computed model is presented
as Figure 8. The acoustic velocity values used are 7926.83
ft/s inside the channel and 9031.45 ft/s outside the chan-
nel showing that channel bed, about 35.4 ms thick, is a
low impedance layer (Tables 1.0 and 1.1). The computed
model is inherently noisy since well data was involved in
its computation. Recall that Seismic data are usually con-
taminated by noise, even when the data has been migrated
reasonably well and are multiple-free [20]
.
The effective offset in Figure 8 is 0 to 2T, where T rep-
resents period. The Thickness of the channel is denoted in
DOI: https://doi.org/10.30564/jgr.v2i2.2046
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Journal of Geological Research | Volume 02 | Issue 02 | April 2020
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units of the dominant (center) period corresponding to the
dominant frequency of the Ricker wavelet (zero-phase)
used in modeling. The center frequency used for simulation
is 50Hz implying a period of 20 milliseconds. The spectral
and cepstral properties of the model such as amplitude and
phase spectra as well as and gamnitude and saphe cepstra
highlighting tuning effects are displayed as Figure 9.
The model was data- driven and developed to test the
resolution capability of the transforms algorithms and
to calibrate the model. The transforms employed are the
Discrete Fourier Transform (DFT) and the Complex Cep-
stral Transform (CCT). The SEG Y data was loaded into
Petrel software and a reconnaissance was performed on
the seismic sections of the field. A channel feature was
identified between inlines 5880 and 6190 and crossline
1565. Well 06 penetrated the structure around inline 6009.
From the log data of Well 06, some model parameters
were extracted and then used to compute new parameters
necessary for model computation. The Shale reference
point was set at 60 American Petroleum Institute (API)
units for GR log. Therefore, Formations with less than ()
60API units were read as Sands, while those greater than
() 60 API units were read as Shale. Representative model
parameters were extracted from Well 06 log data at appro-
priate depths. The data consist of the GR, RHOB and ITT
readings. The logs were correlated with Self Potential (SP)
and Resistivity logs. This was followed by the computa-
tion of parameters like velocity, acoustic impedance and
reflection coefficient used for the modeling of the channel
sand structure. The convolution equation used is given by
S t W t R t
( ) ( ) * ( )
= (7)
Where S (t) = Synthetic Seismogram; W (t) = Ricker
Wavelet and R (t) = Reflection Coefficient.
The maximum useful frequency or centre frequency
was set at 50Hz. This frequency was selected on the basis
of apriori information of the general seismic bandwidth
of 5-65Hz and the need to capture some structural events.
Majority of the stratigraphic traps have structural elements
and in some cases the distinction is difficult [21]
. Several
center frequencies were explored (Figure 6). The channel
seismogram consists of 50 seismic traces presented in the
wiggle format.
4. Results and Interpretation
In seismic attribute analysis, amplitude or magnitude, or
envelope indicates local concentration of energy, bright
spots, gas accumulation, sequence boundaries, unconfor-
mities, major changes in lithology, thin bed tuning effects,
etc; phase measures lateral continuity/discontinuity/edge)
or faulting, shows detailed visualization of bedding con-
figuration and has no amplitude information. In the case of
the phase attribute, there is a flip owing to sign reversal [22]
.
The frequency attribute reflects attenuation spots, indicates
hydrocarbon presence by its low frequency anomaly, shows
edges of low impedance thin beds, fracture zone indica-
tion-appears as low frequency zones, and also indicates
bed thickness. Higher frequencies indicate sharp interfaces
or thin shale bedding, lower frequencies indicate sand rich
bedding, sand/shale ratio indicator [23]
. In Cepstral domain,
the Gamnitude, Saphe and Quefrency are interpreted in a
similar manner to Magnitude, Phase and Frequency in the
Spectral domain. Saphe highlights discontinuity/edge and
lithologic changes, while Quefrency indicates fracture zone,
hydrocarbon presence by its low values.
Figure 2. Tomboy Field, Niger Delta: Seismic Section
showing Channel feature. (Petrel Platform)
Figure 3. Well log analysis: Gamma Ray Log of Well
06 showing picked horizons for model computation.
(Gnuplot-General platform)
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Journal of Geological Research | Volume 02 | Issue 02 | April 2020
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TABLES OF MODEL PARAMETERS
Table 1.0: Extracted Values of Some Well Parameters of Well 06
s/n Depth
(ft)
Layer H
(ft)
TWT
(ms)
TWT (AVE)
(ms)
GR
(API units)
SP
( mV)
RHOB
‘δ’
(g/cm3
)
TT
(µsec/ft)
ɸ
(%)
Vsh
1 5738.0 A Top 37.5 2217.92 2225.16 70.30 346.42 2.17 115.56 35.93 0.3036
5775.5 Base 2232.41 63.75 325.56 2.25 123.86
2 7368.5 B Top 56.5 2855.23 2866.25 59.92 299.66 2.23 110.41 33.41 0.2746
7424.0 Base 2877.28 67.99 283.10 2.32 111.04
3 7435.0 C Top 90.5 2881.39 2899.09 14.11 306.86 2.18 129.64 37.54 0.0364
7525.5 Base 2916.80 29.85 289.31 2.08 122.85
4 9105.0 Top 187.5 3534.57 3571.13 96.25 -49.12 2.40 110.85 32.30 0.6324
9292.5 D Base 3607.70 76.38 -32.58 2.21 103.50
5 9675.0 Top 3757.14 94.68 -20.81 2.26 102.84
Table 1.1: Computed Values of Some Well Parameters of Well 06
s/n Depth (ft) Layer H (ft) TWT
(AVE)
RHOB ‘δ’
(g/cm3
)
Velocity
‘V’
(ft/s)
AV E
‘δ’
AV E
‘V’
Z = δV Zb-Za Zb+Za RC==
𝑍𝑍2−𝑍𝑍1
𝑍𝑍2+𝑍𝑍1
1 5738.0 A 37.5 2225.16 2.17 8653.51 2.21 8363.57 18483.48 Z1 Z2-Z1 Z2 +Z1 0.0517 R1
5775.5 2.25 8073.63 2017.91 38984.87
2 7368.5 B 56.5 2866.25 2.23 9057.15 2.27 9031.45 20501.39 Z2 Z3 –Z2 Z3+Z2 -0.0967 R2
7424.0 2.32 9005.76 -3617.25 37385.53
3 7435.0 C 90.5 2899.09 2.18 7713.66 2.13 7926.83 16884.14 Z3 Z4-Z3 Z4 +Z3 0.1199 R3
7525.5 2.08 8140.00 4601.33 38369.61
4 9105.0 D 187.5 3571.04 2.40 9021.19 2.30 9341.51 21485.47 Z4 Z5-Z4 Z5+Z4 0.0114 R4
9292.5 2.21 9661.83 497.18 43468.12
5 9675.0 2.26 9726.84 2.26 9726.84 21982.65 Z5
Where h = Interval Thickness; Z =Acoustic Impedance; RC= Reflection Coefficient; AVE = Average Values; TWT = Two Way Travel Time; TT =
Transit Time; ɸ = Porosity; Vsh = Volume of Shale; Velocity ‘V’ =
106
𝑡𝑡
where t = Sonic Transit time or Wave Slowness (µsec/ft), RC =
𝑍𝑍2−𝑍𝑍1
𝑍𝑍2+𝑍𝑍1
A schematic diagram incorporating all model parame-
ters of the channel is shown in Figure 4.
Figure 4. A Schematic diagram of the Channel Feature
(Shown in Red)
-80 -60 -40 -20 0 20 40 60 80
-0.5
0
0.5
1
ZERO PHASE RICKER WAVELET,CENTER FREQUENCY:50.0HZ
WAVE
AMPLITUDE
WAVELET TIME INTERVAL,K[MS]:(SAMPLING TIME UNIT)
Figure 5. Zero Phase Ricker Wavelet for Channel Sand
Model with Centre Frequency of 50Hz
-80 -60 -40 -20 0 20 40 60 80
-0.5
0
0.5
1
ZERO PHASE RICKER WAVELET,CENTER FREQUENCY:5.0HZ
WAVE
AMPLITUDE
WAVELET TIME INTERVAL,K[MS]:(SAMPLING TIME UNIT)
(a) Zero Phase Ricker Wavelet for Channel Sand Model at Centre
Frequency of 5Hz
-80 -60 -40 -20 0 20 40 60 80
-0.5
0
0.5
1
ZERO PHASE RICKER WAVELET,CENTER FREQUENCY:10.0HZ
WAVE
AMPLITUDE
WAVELET TIME INTERVAL,K[MS]:(SAMPLING TIME UNIT)
(b) Zero Phase Ricker Wavelet for Channel Sand Model at Centre
Frequency of 10Hz
-80 -60 -40 -20 0 20 40 60 80
-0.5
0
0.5
1
ZERO PHASE RICKER WAVELET,CENTER FREQUENCY:20.0HZ
WAVE
AMPLITUDE
WAVELET TIME INTERVAL,K[MS]:(SAMPLING TIME UNIT)
(c) Zero Phase Ricker Wavelet for Channel Sand Model at Centre
Frequency of 20Hz
-80 -60 -40 -20 0 20 40 60 80
-0.5
0
0.5
1
ZERO PHASE RICKER WAVELET,CENTER FREQUENCY:25.0HZ
WAVE
AMPLITUDE
WAVELET TIME INTERVAL,K[MS]:(SAMPLING TIME UNIT)
(d) Zero Phase Ricker Wavelet for Channel Sand Model at Centre
Frequency of 25Hz
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-80 -60 -40 -20 0 20 40 60 80
-0.5
0
0.5
1
ZERO PHASE RICKER WAVELET,CENTER FREQUENCY:30.0HZ
WAVE
AMPLITUDE
WAVELET TIME INTERVAL,K[MS]:(SAMPLING TIME UNIT)
(e) Zero Phase Ricker Wavelet for Channel Sand Model at Centre
Frequency of 30Hz
-80 -60 -40 -20 0 20 40 60 80
-0.5
0
0.5
1
ZERO PHASE RICKER WAVELET,CENTER FREQUENCY:40.0HZ
WAVE
AMPLITUDE
WAVELET TIME INTERVAL,K[MS]:(SAMPLING TIME UNIT)
(f) Zero Phase Ricker Wavelet for Channel Sand Sand Model at
Centre Frequency of 40Hz
-80 -60 -40 -20 0 20 40 60 80
-0.5
0
0.5
1
ZERO PHASE RICKER WAVELET,CENTER FREQUENCY:50.0HZ
WAVE
AMPLITUDE
WAVELET TIME INTERVAL,K[MS]:(SAMPLING TIME UNIT)
(g) Zero Phase Ricker Wavelet for Channel Sand Model at Centre
Frequency of 50Hz
-80 -60 -40 -20 0 20 40 60 80
-0.5
0
0.5
1
ZERO PHASE RICKER WAVELET,CENTER FREQUENCY:60.0HZ
WAVE
AMPLITUDE
WAVELET TIME INTERVAL,K[MS]:(SAMPLING TIME UNIT)
(i) Zero Phase Ricker Wavelet for Channel Sand Model at Centre
Frequency of 60Hz
Figure 6. Zero Phase Ricker Wavelet Analysis at Various
Center Frequencies and Time Breadths
0 10 20 30 40 50 60 70 80 90 100
0
2
4
6
8
AMPLITUDE AND PHASE SPECTRA(50HZ RICKER WAVELET)
ABS.
MAGNITUDE
0 10 20 30 40 50 60 70 80 90 100
-0.2
-0.15
-0.1
-0.05
0
PHASE
[DEGREES]
FREQUENCY [HERTZ]
(a): Amplitude and Phase Spectra (50Hz Ricker Wavelet)
0 10 20 30 40 50 60 70 80 90 100
0
0.5
1
1.5
2
AMPLITUDE AND PHASE SPECTRA(SAND-REFLECTIVITY)
ABS.
MAGNITUDE
0 10 20 30 40 50 60 70 80 90 100
0
0.02
0.04
0.06
0.08
PHASE
[DEGREES]
FREQUENCY [HERTZ]
(b) Amplitude and Phase Spectra (Sand-Reflectivity)
0 10 20 30 40 50 60 70 80 90 100
0
0.5
1
1.5
AMPLITUDE AND PHASE SPECTRA(SHALE-REFLECTIVITY)
ABS.
MAGNITUDE
0 10 20 30 40 50 60 70 80 90 100
0
0.05
0.1
0.15
0.2
0.25
PHASE
[DEGREES]
FREQUENCY [HERTZ]
(c) Amplitude and Phase Spectra (Shale-Reflectivity)
Figure 7. Amplitude and Phase Spectra (Sand and Shale
Reflectivities)
0 0.02 0.04 0.06 0.08 0.1 0.12 0.14
-4500
-4000
-3500
-3000
-2500
-2000
CHANNEL SAND MODEL SIMULATED WITH 5OHz RICKER WAVELET
TRACE(TWT)(mSECONDS)
LINE(PERIOD,T(SECONDS))
Figure 8. 50-Trace, 50Hz Field Data-Derived Channel
Model: Original amplitude
DOI: https://doi.org/10.30564/jgr.v2i2.2046
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Journal of Geological Research | Volume 02 | Issue 02 | April 2020
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0 10 20 30 40 50 60 70 80 90 100
0
2
4
6
8
MAGNITUDE AND PHASE SPECTRA OF CHANNEL MODEL
ABS.
MAGNITUDE
0 10 20 30 40 50 60 70 80 90 100
0
2000
4000
6000
8000
10000
12000
PHASE
[DEGREES]
FREQUENCY [HERTZ]
(a) Magnitude and Phase Spectra of Channel Model
0 10 20 30 40 50 60 70 80 90 100
0
100
200
300
400
GAMNITUDE AND SAPHE CEPSTRA OF CHANNEL MODEL
ABS.
GAMNITUDE
0 10 20 30 40 50 60 70 80 90 100
0
0.5
1
1.5
2
x 10
4
SAPHE
[DEGREES]
QUEFRENCY [HERTZ]
(b) Gamnitude and Saphe Cepstra of Channel Model
Figure 9. Spectra and Cepstra of 50Hz Field Data-De-
rived Channel Model. There is more information recovery
in the Cepstra plot as reflected in the attributes shown
0 10 20 30 40 50 60 70 80 90 100
0
5
GAMNITUDE AND SAPHE CEPSTRA OF CHANNEL MODEL
ABS.GAM.
QUEF[Hz]
0 10 20 30 40 50 60 70 80 90 100
0
1
2
x 10
5
SAPHE[DEG.]
QUEF.[Hz]
0 10 20 30 40 50 60 70 80 90 100
0
5
MAGNITUDE AND PHASE SPECTRA OF CHANNEL MODEL
ABS.MAG
FREQ[Hz]
0 10 20 30 40 50 60 70 80 90 100
0
5000
10000
PHASE[DEG]
FREQ[Hz]
Figure 10. 50 Hz Field Data-Derived Channel Model: An
integrated display of Spectral and Cepstral attributes plots
to illustrate their resolving capabilities
Figure 11. Seismic Section Showing Channel Feature.
(Petrel Platform)
0 0.02 0.04 0.06 0.08 0.1 0.12 0.14
-4500
-4000
-3500
-3000
-2500
-2000
CHANNEL SAND MODEL SIMULATED WITH 5OHz RICKER WAVELET
TRACE(TWT)(mSECONDS)
LINE(PERIOD,T(SECONDS))
Figure 12. 50-Trace, 50 Hz Field Data-Derived Channel
Model: Original Model Data
(a) Field Seismic Section showing channel feature. (Petrel Platform)
0 0.02 0.04 0.06 0.08 0.1 0.12 0.14
-4500
-4000
-3500
-3000
-2500
-2000
CHANNEL SAND MODEL SIMULATED WITH 5OHz RICKER WAVELET
TRACE(TWT)(mSECONDS)
LINE(PERIOD,T(SECONDS))
(b) 50-Trace, 50 Hz Field Data-Derived Channel Model: Original
Model Data
0 0.02 0.04 0.06 0.08 0.1 0.12 0.14
-4500
-4000
-3500
-3000
-2500
-2000
CHANNEL SAND MODEL SIMULATED WITH 5OHz RICKER WAVELET
TRACE(TWT)(mSECONDS)
PHASE(PERIOD,T(SECONDS))
data1
data2
data3
data4
(c) An abridged four (4)-trace Phase Attribute Section by Discrete
Fourier Transform to indicate improved lithologic change/segmen-
tation. Data1: Shale, data2: Sand, data3: Sand, data4: Shale.
DOI: https://doi.org/10.30564/jgr.v2i2.2046
13. 9
Journal of Geological Research | Volume 02 | Issue 02 | April 2020
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0 0.02 0.04 0.06 0.08 0.1 0.12 0.14
-4500
-4000
-3500
-3000
-2500
-2000
CHANNEL SAND MODEL SIMULATED WITH 5OHz RICKER WAVELET
TRACE(TWT)(mSECONDS)
SAPHE(PERIOD,T(SECONDS))
data1
data2
data3
data4
(d) An abridged four (4)-trace Saphe Attribute Section by Cepstral
Transform to indicate enhanced Lithologic change/segmentation.
Data1: Shale, data2: Sand, data3: Sand, data4: Shale,
Figure 13. 50 Hz: Comparative display of Field Seismic
Section, Data-Derived Channel Model, and an abridged
Phase and Saphe Attribute Sections
. 0 0.02 0.04 0.06 0.08 0.1 0.12 0.14
-4500
-4000
-3500
-3000
-2500
-2000
CHANNEL SAND MODEL SIMULATED WITH 5OHz RICKER WAVELET
TRACE(TWT)(mSECONDS)
LINE(PERIOD,T(SECONDS))
(a) 50 Hz Field Data-Derived Channel Model: Original Model Data
0 0.02 0.04 0.06 0.08 0.1 0.12 0.14
-4500
-4000
-3500
-3000
-2500
-2000
CHANNEL SAND MODEL SIMULATED WITH 5OHz RICKER WAVELET
TRACE(TWT)(mSECONDS)
PHASE(PERIOD,T(SECONDS))
(b) 50 Hz Field Data-Derived Channel Model: DFT Phase Section
0 0.02 0.04 0.06 0.08 0.1 0.12 0.14
-4500
-4000
-3500
-3000
-2500
-2000
CHANNEL SAND MODEL SIMULATED WITH 5OHz RICKER WAVELET
TRACE(TWT)(mSECONDS)
SAPHE(PERIOD,T(SECONDS))
(c) 50 Hz Field Data-Derived Channel Model: CCT Saphe Section
Figure 14. Comparative Display of Field Data-Derived
50Hz Channel Model, DFT Phase and CCT Saphe attri-
butes
5. Conclusions
We have investigated spectral and cepstral decomposition
of data driven geologic channel sand, about 35ms thick
obtained by convolution of a 50 Hz zero phase Ricker
wavelet with a four-layer reflectivity series, where the
third layer is the channel bed. The Discrete Fourier and
Complex Cepstral transforms were used to highlight the
channel’s average/response and precise attributes. Our
aim was to develop a practical method for processing and
mapping of stratigraphy which is usually masked after
normal data interpretation. The DFT and CCT were used
to calibrate and analyze a computed channel model with
respect to subtle signal variation as obtained in field strati-
graphic works.
The results obtained(from the samples presented) show
the resolution capability of the Complex Cepstrum in
separating source and filter and the detection of local peri-
odicity which are critical geological parameters in under-
standing stratigraphic details and hydrocarbon fairways
which impact on enhanced recovery. We implemented
it on both standard and general platforms and found the
match, on comparison to be convincing. This technology
has application in the delimitation, delineation and char-
acterization of subtle geologic targets such as thin-bed
reservoir, areas of uncertainty in data and time such as in
complex geologic environments as in deep waters, mar-
ginal fields, etc and and similar geologic situations.
Acknowledgments
The authors wish to thank Chevron Corporation, Nigeria
for making the Seismic and well data available for use.
Thanks are also due to the Authorities of University of
Port Harcourt, Nigeria, Federal University of Petroleum
Resources, Effurun, Nigeria and the Petroleum Training
Institute, Effurun, Nigeria for the use of their computing
facilities.
References
[1] Satinder, C., Marfurt, K. J., Misra, S. Seismic Attri-
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[3] Hall, M. Predicting Stratigraphy with Cepstral de-
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leum Geologists, Tulsa, Oklahoma, 1978: 96-200.
[6] Merki, P. J. Structural Geology of the Cenozoic Ni-
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[7] Weber, K. J. Hydrocarbon Distribution patterns in
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[11] Yilmaz, O. Seismic data processing, Oklahoma. Soci-
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[13] Jeong, J. Kepstrum Analysis and Real-Time Appli-
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[14] Bogert,B.P. Healy, M. J. R., Tukey,: J. W. The Que-
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[20] Satinder, C., Marfurt, K. J., Misra, S. Seismic Attri-
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[21] Reza Mohebian, Mohammad Ali Riahi, Omid
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Distributed under creative commons license 4.0 DOI: https://doi.org/10.30564/jgr.v2i2.2066
Journal of Geological Research
https://ojs.bilpublishing.com/index.php/jgr-a
ARTICLE
Analysis of Heavy Metals Contamination and Quality Parameters of
Groundwater in Ihetutu, Ishiagu
A. G. Benibo*
R. Sha’Ato R. A. Wuana A. U. Itodo
Department of Chemistry and Centre for Agrochemical Technology Environmental Research (CATER), Federal Uni-
versity of Agriculture, Makurdi, Nigeria
ARTICLE INFO ABSTRACT
Article history
Received: 28 June 2020
Accepted: 14 July 2020
Published Online: 30 July 2020
The levels of some quality parameters and heavy metals in groundwater in
Ihetutu minefield of Ishiagu were analyzed in four seasons (rainy, late rainy,
dry, and late dry), in order to evaluate the deterioration of the groundwater
qualities in the area. Pb-Zn mining and several other related activities have
been going on for several decades in Ihetutu, and thus render the groundwa-
ter resources in the area less available for consumption, through toxic chem-
ical substances expected to be constantly discharged to the groundwater
bodies from the mines and other domestic wastes. The aim of this study was
thus to determine the levels of heavy metals and other physico-chemical
properties in the groundwater, to assess its suitability for drinking and other
domestic purposes in Ihetutu. Samples were collected from dug-wells and
underground water platforms, and analyzed using standard procedures, for
their physico-chemical properties and heavy metals levels. Results obtained
for the various seasons ranged as pH = 6.80-8.72, EC = 190.00-1120.00 µS/
cm, alkalinity = 4.20-30.60 mg/L, TDS = 105.00-567.00 mg/L, TH = 8.00-
44.00 mg/L, Cl- = 26.00-126.00 mg/L, Cu = 0.00-0.30 mg/L, Zn = 0.00-
0.42 mg/L, Fe = 0.00-3.93 mg/L, Mn = 0.00-0.59 mg/L, and Pb = 0.00-0.43
mg/L. Average levels of analyzed parameters in study area were: pH = 7.56,
EC = 424.06 µS/cm, alkalinity = 17.88 mg/L, TDS = 218.69 mg/L, TH =
21.88 mg/L, Cl- = 54.31 mg/L, Cu = 0.20 mg/L, Zn = 0.51 mg/L, Fe = 2.55
mg/L, Mn = 0.32 mg/L, Pb = 0.38 mg/L. Mean levels of most parameters
were found to be within standard guidelines/limits but were above control
levels, giving an indication of deterioration of the groundwater qualities in
the area. Also, seasonal concentrations of most parameters, including the
heavy metals were in the order of LDSDRSLRSRNS. Heavy metals
mean concentrations also trended in the order of FeZnPbMnCu. Cor-
relations among heavy metals were all positive, with the strongest between
Cu and Pb (r = 0.921) while the least was between Cu and Mn (r = 0.176).
ANOVA showed no statistically significant differences among sampling
stations in study area, as p-values (0.757) was higher than the significance
level (α=0.05). Comparison of the results with control values, indicated
cases of deterioration of the groundwater quality in the study area. This
confirmed that the groundwater resources in the area were adversely affect-
ed by wastes and discharges from the mining activities and several other
sources including domestic wastes.
Keywords:
Contamination
Pollution
Environment
Mining
Groundwater
*Corresponding Author:
A. G. Benibo,
Department of Chemistry and Centre for Agrochemical Technology Environmental Research (CATER), Federal University of
Agriculture, Makurdi, Nigeria;
Email: ao_benibo@yahoo.com
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Journal of Geological Research | Volume 02 | Issue 02 | April 2020
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1. Introduction
M
ining has become an indispensable component
of economic resource at Ihietutu, Ishiagu, in
Ivo River Local Government Area of Ebonyi
State of Nigeria. Ihetutu mine in Ishiagu is the oldest
mine in his study on lead (Pb) mining carried out at four
mining sites in Ebonyi State [1]
. It is thus expected that
various toxic chemical substances including heavy metals,
etc must have accumulated to very high levels in the area,
considering the very long time of existence and operation
of the mines.
Mining operations constitute the most important sourc-
es of pollutants such as heavy metals and many other tox-
ic chemical substances in the environment. It is a business
that seriously damages the environment [2]
. Its operations
and associated industries generate large volumes of waste-
water, drainage wastes and tailings, which plunders the
landscape and contaminate the surrounding environment
with inorganic pollutants, particularly heavy metals. Most
mining operations have serious adverse effect on air, wa-
ter, soil and vegetation [3]
. On a global scale, it was esti-
mated that about 3000 billion tons of mine overburden is
dumped annually, and that about 386,000 hectares of land
is disturbed by mining activities [4]
.
Activities of mining are well known for their danger-
ous impact on the environment due to deposition of large
volume of waste on the soil and water. Adverse environ-
mental consequences of open pit mining include sediment
and water qualities degradation due to destruction of veg-
etation, exposure of the soil to surface run-offs, as well as
dumps that have been confirmed to accommodate harmful
minerals and chemicals that contaminate the soil, plant,
water and air quality [5]
.
Various chemicals used during ore processing cause
high degree of pollution of groundwater bodies. Through
wrong application, faulty disposal system, poor storage
system and several other conditions prevalent at the time
of operations, these chemicals used at mine sites could
also cause intense pollution of the environment [6]
. Water
pollution increases due to human population, industrial-
ization, the use of fertilizers in agriculture and man-made
activity[7]
, which include mining operations, artisan activi-
ties; and natural sources such as weathering of rocks.
The objective of this research was to evaluate the qual-
ity of groundwater available for drinking and other do-
mestic purposes in Ihetutu where several mining activities
have been ongoing for several decades now. Groundwater
resources were only some few kilometers away from the
numerous Pb-Zn mining sites, and were thus expected to
be seriously polluted by wastes leachates and discharges
from the mines and its wastes dumps and tailings; and
other point and non-point sources including domestic
wastes and run-offs from farms. This suspicion made it
imperative to carry out this study. Huge amount of toxic
chemical substances constantly discharged into ground-
water bodies have become sources of contamination and
threat to human health, thus making assessment of their
levels and impacts a necessary one.
2. Materials and Methods
2.1 The Study Area
The Ihetutu Hill is located in Ishiagu, Ebonyi State of
Nigeria, and is within the Lower Benue trough. Lead-zinc
and hard rock (aggregate) mining has been ongoing in the
area since the 1950s. The Ishiagu area covers an expanse
of about 450 km2
and supports an estimated population
of over two hundred and fifty thousand persons [8,9]
. The
study area falls within latitudes 5o
51/
N and 5o
59/
N and
longitudes 7o
24/
E and 7o
40/
E covering an area of over
450 km2
. The area is accessible through the Enugu - Port
Harcourt Railway line, the Enugu-Port Harcourt oil pipe-
line, the Enugu - Port Harcourt Express Road, the Lekwe-
si-Obiagu Road which, and the Okigwe - Afikpo Road [10]
(Figures 1).
Figure 1. Map showing sampling stations in study and
control areas
2.2 Sample Collection and Analysis
Samples were collected in four seasons including rainy
season (May), late rainy season (September), dry season
(December), and late dry season (April) from both study
and control areas (which is about 12 km away from the
study area). Four groundwater samples were collected from
the study area, each season, directly from dug-wells and
underground spring water platforms and labeled as SGW9,
DOI: https://doi.org/10.30564/jgr.v2i2.2066
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SGW10, SGW11, SGW12, while one sample was collected
from the control area and labeled as CGW2 each season also.
Collected samples were digested and analyzed to determine
the physico-chemical parameters and heavy metal concen-
trations, using standard methods and procedures[11]
. pH and
Electrical Conductivity were determined in-situ (on site).
Table 1. Sampling Field Data Summary
Sampling
Stations
Sampling Dates
Sampling
Seasons
Station
Locations
Latitude Longitude
CGW2
(Control)
13/05/2018;
29/09/2018;
29/11/2018;
12/04/2019
RNS;
LRS;
DRS;
LDS
Ukwu
Okwe
Well, Utu-
ru.
N 5o
50'54 E 7o
29'32
SGW9
13/05/2018;
01/10/2018;
01/12/2018;
14/04/2019
RNS;
LRS;
DRS;
LDS
Ogwu
spring
well, Ihetu-
tu.
N 5o
57'3 E 7o
33'4
SGW10
13/05/2018;
01/10/2018;
01/12/2018;
14/04/2019
RNS;
LRS;
DRS;
LDS
Idu Com-
pound
Well, Ihet-
utu.
N 5o
57'7 E 7o
33'6
SGW11
13/05/2018;
01/10/2018;
01/12/2018;
14/04/2019
RNS;
LRS;
DRS;
LDS
Amaog-
wute
Well, Ihet-
utu.
N 5o
57'11 E 7o
33'8
SGW12
13/05/2018;
01/10/2018;
01/12/2018;
14/04/2019
RNS;
LRS;
DRS;
LDS
Amaukwa
Well,
Ihetutu.
N 5o
57'12 E 7o
33'15
Note: RNS = Rainy Season, LRS = Late Rainy Season, DRS = Dry Sea-
son, LDS = Late Dry Season
3. Results and Discussion
3.1 Physico-chemical Properties of Groundwater
in Ihetutu
3.1.1 pH
pH peaked during the dry season (DRS) at CGW10,
CGW11, CGW12 but during the late dry season (LDS) at
CGW9 and the control station (CGW2); while the lowest
values at all sampling stations were recorded during the
rainy season (RNS) (Figure 2). Mean pH values range was
7.46-7.67, with SGW10 having the highest and SGW12
the lowest. However, the control groundwater (CGW2)
with a mean value of 7.32 is lower than the mean pH
values of all the samples from the study area (Table 2).
Average pH value in study area was 7.56 (Table 3). This
value was within the standard guidelines of USEPA,
SON, NESREA and WHO (Table 4). The increased pH
values in the groundwater samples could be due to the in-
creasing buffering capacity of alkaline minerals leaching
from surrounding underground and surface rocks/soil, to
the groundwater. The increase in pH could also be due
to the reduction in the rate of photosynthetic activities in
the well, and absorption of carbon dioxide and bicarbon-
ates[12]
. Discharge of domestic waste and other organic
pollutants into the water bodies that run through the farms
and located along the paths of the villagers could also be
responsible for the increase in pH[13]
.
Table 2. Mean values of physico-chemical parameters and
Heavy Metals in groundwater
Parameter (CGW2) SGW9 SGW10 SGW11 SGW12
pH 7.32 7.53 7.67 7.58 7.46
EC (µS/cm) 184.75 251.25 475.50 662.00 307.50
TDS (mg/L) 128.50 136.50 245.00 333.50 159.75
TH (mg/L) 22.00 13.90 25.15 23.53 24.95
Alkalinity (mg/L) 19.03 11.88 26.28 19.95 13.40
Cl-
(mg/L) 70.75 42.25 56.25 79.00 39.75
Cu (mg/L) 0.25 0.14 0.27 0.18 0.27
Fe (mg/L) 3.39 1.86 3.52 3.47 2.23
Zn (mg/L) 2.40 000 0.41 0.38 0.74
Mn (mg/L) 0.07 0.10 0.37 0.54 0.22
Pb (mg/L) 0.33 0.00 0.42 0.30 0.41
3.1.2 Electrical Conductivity
Mean EC ranged from 251.25 to 662.00 µS/cm with
SGW11 having the highest value while SGW9 had the
lowest. All study area values were higher than that of con-
trol (CGW2) (Table 2). Seasonal conductivity values for
groundwater samples from the study area also increased in
the order of RNSLRSDRSLDS (Figure 3), exception
of SGW12 which peaked during the dry season (DRS).
Average conductivity value in study area was 424.06 µS/
cm (Table 3). This was above EU standard value of 250
µS/cm but below SON standard value of 1000 µS/cm (Ta-
ble 4). High concentration of dissolved salts due to poor
irrigation management, minerals from rain water runoffs,
or discharges (leachates) from mines could lead to in-
crease in conductivity[14]
.
3.1.3 Total Dissolved Solids (TDS)
Mean TDS values ranged from 136.50 to 333.50 mg/L,
and were all higher than the mean value of the control sam-
ple (CGW2) which was 128.50 mg/L (Table 2). Seasonal
TDS values for the samples also increased in the order of
RNSLRSDRSLDS, exception of SGW12 which rather
peaked during the dry season (DRS) (Figure 4). Average
TDS value in study area was 218.69 mg/L (Table 3), and
was below USEPA, SON and NESREA guidelines (Table
4). The groundwater samples mean values were all below
standard reference values indicating a rating of no overall
pollution. Decrease in mean TDS concentration in ground-
DOI: https://doi.org/10.30564/jgr.v2i2.2066
18. 14
Journal of Geological Research | Volume 02 | Issue 02 | April 2020
Distributed under creative commons license 4.0
water samples could also result from high dilution effect
from the rain water during the rainy seasons. The low con-
centration of TDS especially in the groundwater, and some
surface water samples could also be due to the presence of
granitic materials which resists dissolution in that area[15]
.
3.1.4 Alkalinity
Alkalinity increased from rainy to dry season in the sam-
ples, though there was a decrease in the late dry season
(LDS) at SGW10, SGW11 and SGW12 (Figure 5). Mean
values also ranged from 11.88 to 26.28 mg/L, with SGW9
having the lowest value and SGW10 the highest. Com-
pared with control (CGW2) value of 19.03 mg/L, SGW9
and SGW12 values were lower while those of SGW10
and SGW11 were higher (Table 2). Increase in alkalinity
could be due to the discharge of carbonate and bicarbon-
ate salts from surrounding rocks/soils to the water bodies.
Average alkalinity value in study area was 17.88 mg/L
(Table 3). It has been reported that, in the Ishiagu mining
area, there is significant volume of mine waste and large
scale presence of carbonate minerals, especially dolomite
and siderite, which makes the acid mine drain (AMD) in
the area to tend towards a neutral or alkaline state [16]
.
-
2.00
4.00
6.00
8.00
10.00
S
G
W
9
S
G
W
1
0
S
G
W
1
1
S
G
W
1
2
C
G
W
2
pH
Value
Sampling Stations
pH
RNS
LRS
DRS
LDS
Figure 2. Seasonal levels of pH
-
200.00
400.00
600.00
800.00
1,000.00
1,200.00
S
G
W
9
S
G
W
1
0
S
G
W
1
1
S
G
W
1
2
C
G
W
2
Conductivity
(µS/cm
)
Sampling Stations
EC
RNS
LRS
DRS
LDS
Figure 3. Seasonal concentrations of EC
-
100.00
200.00
300.00
400.00
500.00
600.00
S
G
W
9
S
G
W
1
0
S
G
W
1
1
S
G
W
1
2
C
G
W
2
Concentration
(mg/L)
Sampling Stations
TDS
RNS
LRS
DRS
LDS
Figure 4. Seasonal concentrations of TDS
-
5.00
10.00
15.00
20.00
25.00
30.00
35.00
S
G
W
9
S
G
W
1
0
S
G
W
1
1
S
G
W
1
2
C
G
W
2
Concentration
(mg/L)
Sampling Stations
Alkalinity
RNS
LRS
DRS
LDS
Figure 5. Seasonal concentrations of alkalinity
-
10.00
20.00
30.00
40.00
50.00
S
G
W
9
S
G
W
1
0
S
G
W
1
1
S
G
W
1
2
C
G
W
2
Concentration
(mg/L
Sampling Stations
Total Hardness
RNS
LRS
DRS
LDS
Figure 6. Seasonal concentrations of Total Hardness
DOI: https://doi.org/10.30564/jgr.v2i2.2066
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-
20.00
40.00
60.00
80.00
100.00
120.00
140.00
S
G
W
9
S
G
W
1
0
S
G
W
1
1
S
G
W
1
2
C
G
W
2
Concentration
(mg/L)
Sampling Stations
Chloride
RNS
LRS
DRS
LDS
Figure 7. Seasonal concentrations of Chloride
-
0.50
1.00
1.50
2.00
2.50
SGW9
SGW10
SGW11
SGW12
CGW2
WHO
USEPA
EU
SON
NESREA
Concentration
(mg/L)
[Cu]
Figure 8. Mean Conc. of Cu in Groundwater, with Con-
trol and Standard guidelines
-
1.00
2.00
3.00
4.00
5.00
6.00
SGW9
SGW10
SGW11
SGW12
CGW2
WHO
USEPA
EU
SON
NESREA
Concentration
(mg/L)
[Zn]
Figure 9. Mean Conc. of Zn in Groundwater, with Con-
trol and Standard guidelines
-
0.50
1.00
1.50
2.00
2.50
3.00
3.50
4.00
SGW9
SGW10
SGW11
SGW12
CGW2
WHO
USEPA
EU
SON
NESREA
Concentration
(mg/L)
[Fe]
Figure 10. Mean Conc. of Fe in Groundwater, with Con-
trol and Standard guidelines
-
0.10
0.20
0.30
0.40
0.50
0.60
SGW9
SGW10
SGW11
SGW12
CGW2
WHO
USEPA
EU
SON
NESREA
Concentration
(mg/L)
[Mn]
Figure 11. Mean Conc. of Mn in Groundwater, with Con-
trol and Standard guidelines
0.00
0.10
0.20
0.30
0.40
0.50
SGW9
SGW10
SGW11
SGW12
CGW2
WHO
USEPA
EU
SON
NESREA
Concentration
(mg/L)
[Pb]
Figure 12. Mean Conc. of Pb in Groundwater, with Con-
trol and Standard guidelines
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3.1.5 Total Hardness
Hardness is a measure of the capacity of water to form
precipitates or foam with soap and scales with certain
ions present in the water[17]
. It is defined as the sum of
the concentrations of calcium (Ca2+
) and magnesium
(Mg2+
) ions expressed as mg/L of CaCO3, since soap
is precipitated mostly by these ions[18]
. Mean levels in
groundwater ranged from 13.90 mg/L at SGW9 to 25.15
mg/L at SGW10 (Table 1). Seasonal concentrations were
highest during late dry seasons (LDS) at SGW9, SGW10,
SGW11 and SGW2 (control station) but during dry sea-
son (DRS) at SGW12 (Figure 6). Average total hardness
value in study area was 21.88 mg/L (Table 3), and was
below SON, NESREA and WHO guidelines (Table 4).
Total hardness values of all samples were within standard
limits/guidelines and thus satisfactory. Also according to
some standard classifications[]19]
, the water samples were
classified to be soft, as their concentrations were all within
the range of 0 - 60 mg/L.
3.1.6 Chloride
Mean concentration ranged from 39.75-79.00 mg/L. Ex-
ception of SGW11, all study area samples had concentra-
tions lower than control (CSW2) value (Table 2). Chloride
levels in samples also increased from rainy to dry season,
exception of SGW10 and SGW12 whose concentrations,
Table 3. Seasonal levels of physico-chemical parameters and Heavy Metals in groundwater
Sample
Station
Sample
Season
pH EC (µS/cm)
TDS (mg/
L)
TH (mg/L) Alk (mg/L)
Cl-
(mg/L)
Cu
(mg/L)
Fe (mg/L) Zn (mg/L)
Mn (mg/
L)
Pb (mg/L)
RNS 6.80 190.00 105.00 10.00 10.60 26.00 0.08 0.44 0.001 0.09 0.001
SGW9 LRS 7.00 232.00 109.00 8.00 11.00 30.00 0.09 0.45 0.001 0.10 0.001
DRS 8.15 285.00 143.00 18.70 12.00 55.00 0.18 3.11 0.001 0.10 0.001
LDS 8.17 298.00 189.00 18.90 13.92 58.00 0.20 3.43 0.001 0.11 0.001
RNS 7.00 360.00 198.00 14.00 26.00 52.00 0.001 0.001 0.001 0.17 0.001
SGW10 LRS 7.80 382.00 201.00 15.00 26.40 56.00 0.001 0.001 0.001 0.21 0.001
DRS 8.72 578.00 289.00 31.90 30.60 58.60 0.30 3.11 0.41 0.59 0.42
LDS 7.16 582.00 292.00 39.70 22.10 58.40 0.24 3.92 0.41 0.51 0.43
RNS 6.90 220.00 121.00 12.00 19.00 38.00 0.06 0.001 0.001 0.49 0.001
SGW11 LRS 7.60 258.00 121.00 13.00 20.00 42.00 0.11 0.001 0.001 0.53 0.001
DRS 8.60 1 050.00 525.00 30.80 22.40 110.00 0.24 3.01 0.34 0.59 0.29
LDS 7.20 1 120.00 567.00 38.30 18.40 126.00 0.30 3.93 0.42 0.54 0.30
RNS 6.80 210.00 116.00 12.00 4.20 32.00 0.001 0.29 0.001 0.001 0.001
SGW12 LRS 7.50 225.00 110.00 18.00 4.40 33.00 0.001 0.001 0.001 0.001 0.001
DRS 8.43 483.00 241.00 44.00 27.00 55.00 0.27 2.75 0.42 0.23 0.42
LDS 7.09 312.00 172.00 25.80 18.00 39.00 0.27 3.66 1.06 0.21 0.41
AVER-
AGE
7.56 424.06 218.69 21.88 17.88 54.31 0.20 2.55 0.51 0.32 0.38
RNS 5.80 13.00 72.00 10.00 11.60 44.00 0.001 3.60 0.001 0.07 0.001
CGW2 LRS 6.10 15.00 75.00 16.00 12.50 45.00 0.001 3.96 0.001 0.06 0.001
(control) DRS 8.67 352.00 176.00 31.00 25.00 98.00 0.25 2.87 0.40 0.06 0.32
LDS 8.70 359.00 191.00 31.00 27.00 96.00 0.24 3.12 4.40 0.08 0.33
Note: RNS = Rainy Season; LRS = Late Rainy Season; DRS = Dry Season; LDS = Late Dry Season.
Table 4. Standard Guidelines for Drinking Water
Parameter USEPA[20]
SON[21]
NESREA[22]
WHO[23]
EU[24]
pH 6.5 - 9.5 6.5 - 8.5 6.5 - 9.2 6.5 - 9.5 NM
EC (µS/cm) NM 1,000.00 NG NG 250.00
TDS (mg/L) 500.00 500.00 1,500.00 NG NM
Chloride (mg/L) 250.00 250.00 600.00 250.00 250.00
TH (mg/L) NM 150.00 500.00 200 NM
Alkalinity (mg/L) NG NG NG NG NG
Cu (mg/L) 1.30 1.00 0.075 2.00 2.00
Zn (mg/L) 5.00 3.00 0.80 NG NM
Fe (mg/L) 0.30 0.30 1.00 NG 0.20
Mn (mg/L) 0.05 0.20 0.50 NG 0.05
Pb (mg/L) 0.015 0.01 0.075 0.01 0.010
Note: NG = No guidelines; NM = Not mentioned
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like that of the control sample (CGW2), decreased during
the late dry season (LDS) (Figure 7). Average chloride
level of 54.31 mg/L obtained in the study area (Table 3)
was below referenced standard guidelines (Table 4). High
presence of chloride in water could be due to pesticides
from farms, continuous discharge of mine wastes, and ef-
fluents containing chloride salts from chloride rich rocks
in the area. However, the lower chloride concentrations
observed during the rainy reason could be due to dilution
of the water by rain water[7]
. High chloride content in
water causes eye and nose irritation, stomach discomfort,
increase in corrosive character of the water[12]
.
3.2 Heavy Metals in Groundwater
3.2.1 Copper
Mean copper concentrations in groundwater ranged from
0.14 mg/L at SGW9 (Ogwu spring well) to 0.27 mg/L at
both SGW10 and SGW12 (Table 2). SGW9 and SGW11
were lower in mean concentrations than that of control
(CGW2). Average level of Cu in study area was 0.20 mg/
L while seasonal concentrations were also higher in the
dry seasons than in the rainy seasons, and in the order of
RNSLRSDRSLDS (Table 3). All samples were with-
in the standard guidelines of USEPA, SON, WHO, and
EU[20][21][23][24]
but higher than that of NESREA[22]
(Figure
8).
3.2.2 Zinc
Mean concentrations of Zn ranged from 0.00 mg/L at
SGW9 (seasonal concentrations 0.001 mg/L) to 0.74
mg/L at SGW12 (Table 2). All stations had lower mean
concentrations than the control groundwater (CGW2) in
Uturu. Average Zn concentration in study area was 0.51
mg/L, and seasonal concentrations were higher in the dry
seasons than in the rainy seasons (Table 3). Zn concen-
trations were below USEPA, SON, and NESREA lim-
its[20][21][22]
(Figure 9). The percentage of zinc in the earth
crust is approximately 0.05 g/kg, and its major common
mineral is sphalerite (ZnS), which usually unites with
other sulfides[19]
, and could infiltrate underground water
resources.
3.2.3 Iron
Mean Fe concentration ranged from 1.86 mg/L at SGW9
to 3.52 mg/L at SGW10. SGW9 and SGW12 had lower
mean concentrations than the control sample (CGW2) at
Uturu (Table 2). Groundwater samples in the study area
were observed to be polluted with iron, as they all had
mean concentrations well above USEPA, SON, and NES-
REA limits[20][21][22]
(Figure 10). Average Fe concentration
in study area was 2.55 mg/L, while seasonal levels were
also higher in the dry seasons than in the rainy seasons,
in the order of RNSLRSDRSLDS (Table 3). Iron in
groundwater could result from natural sources such as
minerals from sediments and rocks; or from mining, in-
dustrial wastes, and corroding metals in the surrounding
soil[25]
3.2.4 Manganese
Groundwater samples in the study area had mean man-
ganese concentrations ranged of 0.10 mg/L at SGW9 to
0.54 mg/L at SGW11. All samples from the study area had
higher mean manganese concentrations than the control
(CGW2) sample (Table 2). Only SGW11 has higher Mn
concentration than NESREA recommended value of 0.50
mg/L (Figure 11). Average level of Mn in the study area
was 0.32 mg/L, while seasonal concentrations were also
higher in the dry seasons than in the rainy seasons (Table
3).
3.2.5 Lead
Lead mean concentrations ranged from 0.00 mg/L at
SGW11 (0.001 mg/L seasonal concentrations) to 0.42
mg/L at SGW10. However, control (CGW2) value
was higher than that of SGW9 and SGW11 (Table 2).
Average Pb concentration in study area was 0.38 mg/
L and seasonal levels higher in the dry seasons than in
the rainy seasons (Table 3). All samples also had higher
mean values than referenced standard limits of USEPA,
SON, NESREA, WHO, and EU[20][21][22][23][24]
(Figure 12),
exception of SGW9 (Ogwu Spring well). This indicated
a situation of lead pollution of the underground water
bodies at the affected stations in the study area, which
could be due to high concentrations of lead ore deposits
in the area[26]
. Water-soluble zinc in soils can contami-
nate groundwater[27]
through leaching from the soil to the
water body.
3.3 Correlations of Heavy Metals in Groundwater
There were positive correlations among the heavy metals.
However, strongest positive correlation was between Cu
and Pb (r = 0.921) while the least was between Cu and
Mn (r = 0.176) (Table 5). The positive correlations could
be an indication of the same source of heavy metals pollu-
tion [28]
, which could be natural sources including weath-
ering of rocks, the Pb-Zn mining activities in several parts
of the Ihetutu area, and other sundry point and non-point
sources such as leachates from domestic wastes dumps.
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Table 5. Correlation of heavy metals in groundwater sam-
ples from Ihetutu hills
Cu Zn Fe Mn Pb
Cu 1
Zn 0.829069551 1
Fe 0.347291232 0.223578813 1
Mn 0.175777928 0.287296924 0.917268323 1
Pb 0.921198549 0.883311653 0.597831537 0.525299475 1
3.4 Analysis of Variance (ANOVA)
ANOVA was carried out on the means of the different
stations, using Microsoft Office Excel (2007), at a signif-
icance level, α = 0.05. The results showed no statistically
significant differences in means of the parameters among
sampling stations in study area, as p-values was higher
than the significance level (p = 0.757).
4. Conclusion
This research was undertaken to analyze heavy metals
contamination and quality of groundwater within Ihetutu
mining areas in Ishiagu. The study has revealed that the
quality of groundwater available in the area was poor,
though most of the results obtained were within standard
guidelines/limits of USEPA, SON, NESREA, WHO, and
the EU. Also, exception of SGW9 (Ogwu spring well),
mean levels of Pb, Cu, Fe, Zn and Mn in the study area
were higher than the control (pre-mining/background)
level; and were in the order of FeZnPbMnCu. This
indicated a case of quality deterioration of the groundwa-
ter available at these stations/locations when compared
to the control values obtained; and also confirmed that
groundwater resources in the study area have been ad-
versely impacted upon by leachates/discharges from the
mine wastes, tailings, surrounding rocks, and several oth-
er point and non-point anthropogenic sources including
domestic wastes and run-offs from farms. Seasonal levels
of most of the parameters analyzed including TDS, EC,
pH, total hardness, chloride, and the heavy metals were
also higher in the dry seasons than in the rainy seasons,
and in the order of RNSLRSDRSLDS. However, it is
recommended that adequate measures must be urgently
taken by the mining companies operating in the area to
ensure that wastes and other toxic substances generated
from their operations are not discharged into the ground-
water bodies which serve as the main sources of drinking
water to the people. The government must through its
regulatory agencies including NESREA urgently ensure
proper monitoring of the activities of mining companies
and other waste disposal processes in the area; and also
enforce compliance with laid down standards/regulations.
This will safeguard the groundwater resources in the area,
and consequently human lives that depend on it.
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Distributed under creative commons license 4.0 DOI: https://doi.org/10.30564/jgr.v2i2.2140
Journal of Geological Research
https://ojs.bilpublishing.com/index.php/jgr-a
REVIEW
Review of Groundwater Potentials and Groundwater Hydrochemistry
of Semi-arid Hadejia-Yobe Basin, North-eastern Nigeria
Saadu Umar Wali1*
Ibrahim Mustapha Dankani2
Sheikh Danjuma Abubakar2
Murtala
Abubakar Gada2
Abdulqadir Abubakar Usman1
Ibrahim Mohammad Shera1
Kabiru
Jega Umar3
1. Department of Geography, Federal University Birnin kebbi, P.M.B 1157. Kebbi State, Nigeria
2. Department of Geography, Usmanu Danfodiyo University Sokoto, P.M.B. 2346. Sokoto State, Nigeria
3. Department of Pure and Industrial Chemistry, Federal University Birnin kebbi, P.M.B 1157. Kebbi State, Nigeria
ARTICLE INFO ABSTRACT
Article history
Received: 13 July 2020
Accepted: 24 July 2020
Published Online: 30 July 2020
Understanding the hydrochemical and hydrogeological physiognomies of
subsurface water in a semi-arid region is important for the effective man-
agement of water resources. This paper presents a thorough review of the
hydrogeology and hydrochemistry of the Hadejia-Yobe basin. The hydro-
chemical and hydrogeological configurations as reviewed indicated that the
Chad Formation is the prolific aquifer in the basin. Boreholes piercing the
Gundumi formation have a depth ranging from 20-85 meters. The hydro-
chemical composition of groundwater revealed water of excellent quality,
as all the studied parameters were found to have concentrations within
WHO and Nigeria’s standard for drinking water quality. However, further
studies are required for further evaluation of water quality index, heavy
metal pollution index, and irrigation water quality. Also, geochemical, and
stable isotope analysis is required for understanding the provenance of sa-
linity and hydrogeochemical controls on groundwater in the basin.
Keywords:
Hydrogeology
Sedimentary aquifers
Basement complex terrain
Physical parameters
Chemical parameters
*Corresponding Author:
Saadu Umar Wali,
Department of Geography, Federal University Birnin kebbi, P.M.B 1157. Kebbi State, Nigeria;
Email: saadu.umar@fubk.edu.ng
1. Introduction
The hydrochemical assessment of subsurface for local,
industrial, and agricultural uses required a valuation of the
hydrochemical and hydrogeologic configurations of the
subsurface aquifers [1]
. In a typical semi-arid region like
north-eastern Nigeria, groundwater is the most important
source of water supply for households, irrigation agricul-
ture, and industrial demands [2]
. The quality and availability
of subsurface water have been impacted by increased an-
thropological activities associated with urbanization, indus-
trialization, increased irrigated agriculture, and population
growth [3-6]
. Groundwater protection and conservation pro-
cedures have been largely ignored in mainstream practices
[2]
. Agriculture is the primary and major source of subsur-
face water pollution in arid and semi-arid areas [7,8]
. Results
indicated that pesticides, irrigation water quality, and nitro-
gen fertilizers as major sources of pollutants in aquifers [9]
.
In arid and semi-arid regions like the Hadejia-Yobe ba-
sin, salinization of groundwater is the major cause of the
decline of water quality impacting the sustainable use of
water resources. It limits the use of water for industrial,
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domestic, and agricultural uses [10]
. The problem intensifies
in arid regions where the anthropological activities accel-
erate the deterioration of groundwater quality by a range of
issues which include: (a) subsurface movement of effluents
from irrigation fields; (b) upward flow of groundwater that
has infiltrated the aquifer during irrigation; (c) seepage of
highly effluent-rich surface flows concentrated in urban
and/or municipal effluents during inundation event(s); (d)
overexploitation of aquifer or recycling of wastewater; and
irrigation return flows from irrigated fields [10]
.
In drylands, the salinization, and anthropological activ-
ities are often followed by some natural processes such as
the dissolution of soluble salts and rock-water interactions
in the unsaturated zone which gradually salinizes ground-
water. All these aforementioned factors necessitate con-
tinued analysis and monitoring of groundwater resources
in arid environments for improved water resources man-
agement [10]
. Consequently, several studies were conduct-
ed to evaluate the physical and chemical composition of
groundwater in different parts of the world [9,11-23]
, results
indicated that groundwater is influenced by both anthro-
pological and lithological factors.
Groundwater analysis in some parts of the Hadejia-Yobe
basin showed major variations are correlated to natural and
anthropogenic processes [24]
. Evaluation of groundwater
chemistry using multivariate statistics by Garba, Ekanem
[25]
, inferred that the status of water quality in Hadejia is fit
for human consumption. Similarly, analysis of groundwa-
ter chemistry, dynamics, and storage in parts of Jigawa by
Hamidu, Falalu [26]
revealed water of low hardness and dis-
solved salts that are within the WHO and Nigerian standard
for drinking water quality. Evaluation of fluoride distribu-
tion, geogenic origin, and concentration in groundwater
in some parts of Yobe showed that the area had fluoride
concentrations slightly above WHO reference guidelines
[27]
. Appraisal of toxicity and trace elements concentrations
in Yobe revealed anthropological inputs [28]
. While there is
a significant reporting on the hydrochemistry of aquifers in
the Hadejia-Yobe basin, there is a need for reviewing the
extent of hydrogeological and hydrochemical analysis in
the basin. This is attempted in this study.
2. The Hadejia-Yobe Basin
2.1 Location and Climate
The Hadejia Yobe Basin (also known as Yobe-Jamaare
floodplain), is a trilateral basin, with its summit in
north-eastern Nigeria as depicted by Figure 1 [29-33]
. The
basin coincides roughly with the western Chad basin (un-
confined aquifer) groundwater area. It is underlain by both
the sedimentary formation and basement complex rocks.
The basin is drained in the southwest and northeast by
the tributaries of the River Komadugu Yobe, comprising
mainly Rivers Kano, Gaya, Hadejia, Katagum, Jamaare,
and Gama. These rivers link up at a different point to
form the drainage system of the Komadugu Yobe, flowing
towards the north-eastern summit of the triangular basin
[29-34]
. Together with the eastern Chad basin of Nigeria, it
covers the southwestern part of the Lake Chad.
The major town in the basin includes Kano, Hadejia,
Azare, Potiskum, and Katsina while Bauchi is just outside
the southern boundary. It is bounded to the north by the
Niger Republic. It is situated along with the latitude 10o
N
and has a very hot and dry climate (Figure 1). The annual
rainfall is comparatively low, and annual evaporation is
also very high, reaching up to 1500mm. The scenery is
wide-ranging, extending from the rocky hills and insel-
bergs of the basement complex rocks of the southwest, to
less protuberant, low lying dull rolling dunes of sedimen-
tary formations to the northeast, along Azare, Geidam,
and Gumel. A line of massive granitic mountains, which
perhaps indicate the contact between the two formations
marks the basement-sedimentary frontier.
Figure 1. Hadejia-Jamaare Floodplain [33]
2.2 Relief and Drainage
In terms of drainage, the Hadejia-Yobe-River System con-
trols the entire basin. The tributaries of this river system
rise from near western parts of the North-Central Plateau
(Kano, Katsina, and Jos plateau), with comparatively
higher precipitation than the rest of the province. The De-
limi River, with its headwaters on the Jos Plateau and the
River lgi flowing from the Mingi Hills, the River Kano
from Liruwe Hills, and the Hadejia River from western
Kano, all donates to Hadejia-Yobe-River System [31,33,34]
.
The Hadejia-Yobe or Komadugu-Yobe, as it is sometimes
described, collects water from entire tributaries before
flowing to the Lake Chad. Most of the tributaries of the
Haqdejia-Yobe River System are mechanically measured.
The river flow from the area of high precipitation in the
southwestern axis to lesser precipitation in the direction of
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the lake chad. The intensity of rainfall displays a progres-
sive fall from the southwest to the northeast. The average
annual estimate of rainy days varies from around eighty
days in the southwest to less than the forty days near Lake
Chad. The temperatures are generally high and vary from
20o
C to 28o
C from southwest to northeast. The river Hade-
jia-Yobe is one of the most exploited and monitored river
system in Nigeria [30-32,35,36]
.
Many gauging stations are set along its sequence, from
its source area, in the southwest, to Gashua, near Lake
Chad, where the river empties its headwaters. The river
system is affluent, in the upland basement complex ar-
eas. The river also influent in the Lower Hadejia-Gashua
sedimentary dispersal or wetland area, where the river
valley is exposed to seasonal run-offs and flooding. Con-
sequently, losing a substantial volume of its flow to the
riparian alluvial groundwater aquifers. Owing to the high
evaporation rates exceeding 90%, only about 10% or less
of this flow is accessible by the river as it squalls through
its course of the lake. This flow is induced to recharge into
the underlying aquifers of this part of the Chad basin [37-
40]
. Later, with the increase in evapotranspiration, down-
stream, and the losses into the underlying groundwater
aquifers, as the river feasts out and winds its sequence
towards the Lake Chad, the flow drops considerably.
The river flow, between 1964 to 1965, along the Ha-
dejia - Yobe dropped from 5.6x10m in the upland area, to
0.63x10m in Yau, after flowing through the wetland areas,
51.5 km to the lake. The situation is believed to have wors-
ened. There is also a rise in the groundwater input to the
river flow downstream, 35% at Challawa, and over 50%
towards Wudil. Generally, the river system contributes very
little to the water of the current Lake Chad, which added to
the drying of the lake. Most of its water is lost, seemingly in
the wetland swamps and pools between Hadejia and Geid-
am. The Hadejia-Yobe River System with its large alluvial
expanses is seasonal and only starts flowing around June to
July, after the onset of the rainy season.
2.3 Geological setting
The geology of the Yobe-Hadejia basin is comprised of
the basement complex and sedimentary formations [38,41,42]
.
The Chad Formation is the newest in the Hadejia-Yobe
Basin. A detailed stratigraphical description of the Chad
Formation is not common literature compared to the other
older formations in the basin. The sedimentology of the
formation, which segregates the deposits into three mem-
bers based on color and claystone/sandstone sections were
described in detail by [43]
. The sedimentation of the Chad
Formation has been an incessant process that began in the
Late Miocene to the present, whereby river and aeolian
sand and clay elements are still being added.
Some of the detailed stratigraphies of the Chad Forma-
tion indicated that the lithostratigraphy of Chad Formation
encountered in Korowanga borehole, Dogara borehole
and outcrop section at Abakire, represent numerous het-
erolithic sandstone and claystone in varying proportions.
These sands range from silty, medium, and coarse-grained
in size. In the Tuma well, for instance, the Chad Forma-
tion is characterized by light grey colossal claystone, mi-
nor sand particles, and some occasional pebbly horizons,
and indicating some ferruginization in the deposits [43]
.
Eight lithofacies components were defined based on their
physiognomies such as structure, facies type, grain size,
boniness, sorting, color, and compaction [43]
. The account
of the faces components (summarized in three parts) is
shown in Figure 2.
2.3.1 The Lithofacies Part 1-3
Part 1 comprises greyish sandy claystone. These facies
component range from 50 to 70 meters and also is en-
countered between 305 m and 345 meters below the sur-
face. It is highly rich in organic matter with insignificant
sand particles ranging between silt and minor pebbles.
The lithofacies is also accompanied by lignite. The lower
interlude has filthy claystone displaying roughening-up-
ward sequences and sorting from clayey granite through
to sandy claystone, and weakly-sorted sandstone at the
uppermost [43]
. Part 2 is comprised of micaceous claystone
which occurred only in the interval of 70-90 meters. The
carbonaceous clay is mainly related to mica flecks partic-
ularly muscovite with negligible silt particles. The exis-
tence of muscovite proposes a felsic parent rock source
and lengthy-distance transference. Its high content in or-
ganic matter signposts a lacustrine depositional scenery[43]
.
Part 3 is comprising mainly of lithified claystone. The
lithofacies occurred at the interval of 90 to 195 meters, also
exist as reedy-bedded interpolated deposits at the interme-
diate interlude of the entire unit. The claystone is sturdily
lithified and marginally ferruginized. It is comprised of
slight mica flecks with no sign of biological opulence. Near
the lower part of this interlude, the claystone contrasts from
bright to murky grey, signifying cumulative organic abun-
dance and accumulation in a reducing condition [43]
.
2.3.2 The Kerrikerri Formation
This geologic formation is characterized by horizon-
tal-laying to moderately plummeting basal conglomerate,
grit, sandstone, siltstone, and clay which unconformably
rests above the Maastrichtian Fika Shale and Gombe
Sandstone [44,45]
. Five stratigraphic units (including the
type section at Kadi) and lithology were reviewed. The
DOI: https://doi.org/10.30564/jgr.v2i2.2140
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formation attained a depth of about 200 meters at Duku
[44,45]
. The substantial mineral suite is comprised of rutile,
zircon, kyanite, staurolite, limonite, tremolite, sillimanite,
pyroxene, hornblende, and tourmaline, which are sugges-
tive of origin from the adjoining basement complex and
previous alluvial rocks [44,45]
.
Figure 2. Lithofacies type and depositional/precipitated
palaeoenvironment of the Chad Formation [43]
The occasional basal deposits, well-sedimented silt-
stones and the occurrence of contraction fissures, clay-rein-
forced pebbles, local channel sandstones, and tinny vistas
of coal and carbonaceous clay propose a distinctive deltaic,
peripheral and deltaic lacustrine depositional environment.
The occurrence of the pollens Monocolpites marginatus
and Spinizonocolpites baculatus confirmed a Paleocene age
for the formation. The explanation of the superficial and
subsurface information is constant with an irregular graben
edifice of the Kerrikerri basin. The western boundary of the
basin was fault-controlled and active during the deposition
of sediments through the Early Tertiary [44]
. Borehole data
showed that the intermittent nature of the Paleocene age
Kerri-Kerri Formation as an aquifer in Darazo [45]
.
The series, parasequences, and their borders are be-
lieved to have been formed in reaction to cycles of vir-
tual fall and increase of sea level. Within strings, several
systems bands can be notable and developed all through
an explicit component of a full cycle of virtual sea-level
transformation [46]
. The source of this layered congrega-
tions was the consequence of the interface between the
ratios of variation of basin settling, residue contribution,
and eustasy[46]
. The stratigraphic sequences recognized are
truncated stand system bands, transgressive system bands,
high stand systems bands, and a sequence boundary. The
base of the Gombe Sandstone was not encountered in the
Fika area perhaps owing to lack of outcrops. The uncon-
formity between these two formations (Gombe Sandstone
and Kerri-Kerri Formation), shows a most important top-
most series edge [46]
.
Based on previous investigations, the Gombe Formation
was dated as Late Maastrichtian in age, whereas the Ker-
ri-Kerri Formation age data is not available, nonetheless,
Palaeocene pollens were traced [46]
. The formation of pro-
gression frontiers can be credited to tectonics. However,
there is some indication for Santonian-Campanian folding
simultaneously with the existence of a sharp unconformity
[46]
. The major stratigraphic sequence of the Kerrikerri For-
mation is presented in Figure 3. It is dominated by thick
limestone and sandstone which are Palaeocene in age. The
stratigraphic sequence occurred under erratic conditions
with each sediment correspond to one full cycle of trans-
gression and regression [47]
. The Kerri-Kerri Formation
superimposed a slight area in the southeast, toward Azare.
The formation, containing a succession of grits sandstones
and clays, lies against the crystalline rock in this area. It
is usually not easy to differentiate the formation from the
younger superimposing Chad Formation, as both seem to
be in contact and present the same lithological physiogno-
mies. The formation is up to 200 meters thick in its core
area of existence in the upper Benue and thins out to the
northwest near Azare in the Hadejia-Yobe basin.
0
5
10
15
20
25
30
35
40
45
50
60
70
80
90
Meters Lithology
Paleocene
Continental
Age
Depositional
Environment
Explanation
Sandstone
Limestone
Figure 3. Stratigraphic section of Kerrikerri Formation [47]
2.3.3 The Gundumi Formation
The Gundumi Formation is characterized by the river and
lacustrine deposits, which include moderately grainier
materials (Figure 4). The formation is also characterized
by intermittent lenses of quartz and feldspar pebble grav-
DOI: https://doi.org/10.30564/jgr.v2i2.2140
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el, which are interbedded with the richer clay and clayey
sand [48]
. However, the formation contained a great deal
of melded clay. The sandy beds decline, and clay beds
upsurge with depth down to the contact with the pre-Cre-
taceous basement rocks. Near the base of the Gundumi
Formation, a conglomerate of smoothed quartz stones up
0.0381 meters in diameter occurred in an outlier [48]
. The
sand and gravel beds are comprised of sharp to sub-an-
gular quartz particles, but several beds are abundant in
feldspathic and micaceous substance and rock fragments.
Colors in the Gundumi varied widely. Brown, red, pink,
yellow, white, and even purple are regular, and in some
clay layers, some of these colors may exist in spotted
forms. The sedimentary formations lie above the Precam-
brian basement complex formation. The formation ranged
in age from Palaeozoic to Quaternary. It is assumed to be
a tectonic cross point between the northeast and southwest
trending the “Tibesti-Cameroun Trough” and a north-
west-trending Aïr-Chad Trough”. It has been estimated
that over 3600 m sediments have been deposited[49]
.
Figure 4. Stratigraphic section of Gundumi Formation
The outcrops of the basement complex formation in the
east, southeast, southwest, and the north of the basin are
noticeable. The configuration below the sediments across
the lake was similar to the graben and horst zone [49]
. The
hydrogeology and hydrochemistry of the basement com-
plex section of Chad formation are characteristic of Nige-
ria’s basement complex terrain. There are some published
data on Nigeria’s basement complex [50-60]
. Results indicat-
ed that the groundwater evolution hangs on reactivity and
pH. The hydrochemistry of aquifers is a direct signal of
the catchment geology [58]
.
3. The Sedimentary Aquifers
Hydrogeologically, the Chad Formation is a profound
aquifer in the Hadejia-Yobe basin [26,61,62]
. The aquifer
comprises of a series of clays, sandy clays, and silt, in
which bands and lenses of silt and grit appear at several
spots. The coarse sand and gravel are well developed. In
this area, the Chad Formation superimposes the Kerrikerri
Formation which lies on a more stable basement rock [37]
.
The Chad Formation does not exceed 165 meters in thick-
ness and thins out erratically, nonetheless gently towards
the southern and western borders where it seems to over-
step the basement complex terrain [37,63]
. At Gumel (Jigawa
State), the sediment is reported to attain a thickness of
132 meters, 115 meters at Nguru (Yobe State), 132 meters
at Marguba, and 76 meters at Kunshe. In this province,
groundwater is found an underwater table or sub artesian
conditions depending on the existing hydrogeological
condition (Figure 5).
Figure 5. Lithologic section of boreholes penetrating
Chad Formation.
Borehole yields ranged from 3.3 to 5 lits/sec on aver-
age. However, transmissivity ranged from 6.87m2
/day and
429.4m2
/day, with a mean value of 65.7m2
/day [37]
. The
parting of the Chad Formation into the Upper, Middle,
and Lower aquifers cannot be defined in this part of the
basin. Alternatively, it shows recurrences of clays, sand,
and silts, the sandy layers intersecting the aquiferous
layers. The upper 20-30 meters of the grainy sands of the
Hadejia-Yobe basin, store a lot of water as bank storage,
directly recharged from the river flows [37]
. A lithological
unit along the river outline, based on available borehole
records, displays a top 0-10 meters silty fine-grained
sands, underlain by a thick sequence of coarse sand and
gravel, with two main interbedded clay/shale deposits.
Some of the borehole drilled in this area gave the follow-
ing lithological sections and output [37,64]
.
DOI: https://doi.org/10.30564/jgr.v2i2.2140