In the present study, an unstructured grid-based mesh is made by discretizing the subsurface using Delaunay triangulations. Given N (< = 3) non-linear and noncyclic discrete points in a plane, Delaunay triangles are drawn such that no point in set N is inside the circumcircle of any Delaunay triangle. This property ensures that Delaunay triangulation maximizes every triangle’s minimum angle among all conceivable triangulation of the given point set. This characteristic will avoid the generation of silver triangles. For a given set of points in a plane, there is a unique associated Delaunay-triangulation. This property provides a unique subsurface discretization for multiple code runs, making our forward and inverse modelling results reproducible. Voronoi diagrams are the dual graph of Delaunay triangles. We can draw a Voronoi diagram by connecting the circumcenter of Delaunay triangles. The Voronoi diagram’s vertices are circumcenters of Delaunay triangles, and the edges of the Voronoi diagram are along the perpendicular bisector of sides of Delaunay triangles. Modelling the subsurface by regular gridding is widespread for the forward and inverse problems. In turn, Unstructured grid-based modelling provides the following benefits:
We have designed the framework of forward modelling for Gravity, Magnetic, DC resistivity and IP Methods in such a way that it can support the resulted anomaly due to a three-sided polygon which in our case is a Delaunay triangular cell. Since, Gravity, Magnetic, DC resistivity and IP Methods are potential field based methods, hence they follow the principle of superposition and allows us to calculate the net response of the anomalous subsurface structure by summing the effect due to all individual triangular cells. For inversion, we have used the optimization scheme of the Conjugate Gradient method (CGM) and Gauss-Newton algorithm. CGM guarantees the convergence within n-steps for n-dimensional model space. We have provided preconditioning to our CGM to improve the kernel matrix's condition number and to achieve a faster convergence to the solution. Preconditioning is also compensating for depth decay of potential field anomalies. Non linear inversion equation of DC resisitivity and IP methods is handled by employing Gauss-Newton algorithm.
By making a relationship between two different set of geophysical model parameters, individual inversion results can be improved to provide trustworthy subsurface structures. We have implemented a cooperative style of inversion methodology. Same subsurafce discretization is applied for the forward modeling of different geophysical methods. First, we have tried to invert in one model domain (say density), and then use this inverted density model inside our resistivity inversion algorithm as an additional set of model parameters and invert this density-resistivity combined model parameters simultaneously, constrained by introducing Fuzzy C-Means clustering (FCM) algorithm. For application of FCM, we are required to provide number of geological unit as apriori information, this information can be collected from the geological field scenarios under consideration.
The developed approach is tested on a real field data set for large scale Gravity-ERT profile of Cheb basin (Nickschick et. al., 2019). This data when incorporated in individual inversion is producing the different subsurface structures. There is lack of structural similarity between subsurface models produced by individual density and resistivity inversion. The power of Joint inversion is discernible in these results, It is capable of producing the similar gravity-resistivity subsurface structures. This research is also ready with the joint inversion framework of Gravity and Magnetic, and this framework is successful in recovering the inverted model of a synthetic cuboid shape body buried in subsurface, We look forward to apply it on a real field data set. A further intention of this research is to employ different methodology for joining the different geophysical methods in the joint inversion framework, Design methodology to couple different geophysical model parameters and test the designed algorithm on more field data sets.
Examination | University | Institute | Year |
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PhD (Course Work) | IIT Bombay | IIT Bombay | Ongoing (CPI 9.82) |
Post Graduation | IIT Bombay | IIT Bombay | 2019 |
Graduation | University of Delhi | Rajdhani College | 2017 |
Intermediate/+2 | CBSE | Kendriya Vidyalaya Dhanpuri | 2013 |
Matriculation | CBSE | Kendriya Vidyalaya Dhanpuri | 2011 |
Course Code | Course Name | Credits | Grade |
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GP 525 | Computational Geophysics | 6.0 | AA |
GS 543 | Computer Programming for Geosciences | 6.0 | AA |
GS 649 | Tectonics and Mechanism of Mobile Belts | 6.0 | AB |
GS 663 | Exploration Geophysics | 6.0 | AA |
GS 809 | Computational Methods in Exploration Seismology | 6.0 | AA |
GSS801 | Seminar | 4.0 | AA |
HS 791 | Communication Skills -I | 2.0 | PP |
GS 792 | Communication Skills -II | 4.0 | PP |
March, 2020 | ● Secured AIR 05 in GATE 2020, Geology and Geophysics |
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March, 2019 | ● Secured 92.21 Percentile in GATE 2019, Geology and Geophysics |
March, 2017 | ● Secured 97.63 percentile score in Joint Admission Test for M.Sc. (IIT JAM) Physics |
June, 2017 | ● Secured AIR 10 in Banaras Hindu University (BHU), PG Entrance Test |
Teaching Assistantship IIT Bombay | GS 543 Computer Programing for Geosciences |
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Teaching Assistantship IIT Bombay | GP 414 Electrical Methods |
Teaching Assistantship IIT Bombay | GP 521 Electromagnetic Lab |
Teaching Assistantship IIT Bombay | GP 503 Geophysical Signal Processing |
Teaching Assistantship IIT Bombay | GP 505 Electromagnetic Methods |
PMRF Teaching Deliverables | Numerical problems in Applied Geophysics (At the Department of Geophysics, Andhra University) |
E-mail:
vishnu.kant.verma1@gmail.com,
194060004@iitb.ac.in
Address:
AS Sir Lab, Department of Earth Sciences, Indian Institute of Technology, Bombay, Mumbai, India - 400076