scholarly journals Seismic modeling of two depositional systems

1994 ◽  
Vol 37 (5) ◽  
Author(s):  
G. Brancolini ◽  
G. Casula ◽  
C. De Cillia ◽  
A. Manzella ◽  
A. Polonia ◽  
...  

Two ideal lithologic sections representing a tidal bar system and a fluvial complex were drawn in order to run seismic modeling programs developed by OGS on behalf of the European Community. The simulations allowed an accurate analysis of the seismic expressions of the two sections. The tidal bar system is formed by a number of sandstone lenses interlayered with siltstone and mudstone deposits. These lenses meet together on an erosion surface, while they thin and vanish in the other direction. The fluvial complex is fonned by a limestone basement overlain by coarse alluvial plain sediments which in turn are transgressed by finer flood plain sediments, including sandstone lenses stacking towards the top in a meandering belt. These lithofacies associations represent potential multi-pool reservoirs in which the mudstone layers constitute the plugs. As a function of the granulometric and depositional features of each lithological unit, together with fluid content, wave velocities and densities were evaluated. A 2D modeling for elastic plane wave propagation in these hypothesized geologic sections was run on a Cray supercomputer. The numerical scheme is based on solving the full wave equation by pseudospectral methods.

2019 ◽  
Author(s):  
Christian Deplante ◽  
M. Costa ◽  
M. dos Santos ◽  
R. Dias ◽  
V. Mello ◽  
...  
Keyword(s):  

2014 ◽  
Vol 64 (3) ◽  
pp. 311-323 ◽  
Author(s):  
Ashu Khosla

Abstract A charophyte gyrogonite assemblage consisting of Platychara cf. sahnii, Nemegtichara grambastii and Microchara sp. is reported herein from two localities (Bara Simla Hill and Chui Hill sections) of the Lameta Formation at Jabalpur. he Lameta Formation locally underlying the Deccan traps has been shown to be pedogenically modified alluvial plain deposits containing one of the most extensive dinosaur nesting sites in the world. They are associated with dinosaur bones and freshwater ostracod assemblages that suggest a Late Cretaceous (Maastrichtian) age. This is the first detailed systematic account of charophyte gyrogonites from the Lameta Formation. This charophyte assemblage is compatible with the biostratigraphic attribution provided by the ostracods. From a biogeographic viewpoint, it exhibits considerable similarity to other infratrappean assemblages of the Nand, Dongargaon, and Dhamni-Pavna sections (Maharashtra), and some intertrappean assemblages of Kora in Gujarat, Rangapur in Andhra Pradesh and Gurmatkal in South India. Globally, the genus Microchara is well distributed throughout Eurasia, whereas the genus Platychara occurs richly in the Upper Cretaceous deposits of Europe, Asia, America and Africa. However, at the specific level, Platychara cf. sahnii shows close affinities with charophytes from the Maastrichtian of Iran whilst Nemegtichara grambastii shows distinct affinities with two species of Early Palaeogene deposits of China and Mongolia. The presence of charophyte gyrogonites in the Lameta sediments is attributed to local lacustrine and palustrine conditions within a flood plain environment.


Geophysics ◽  
2005 ◽  
Vol 70 (3) ◽  
pp. C17-C24 ◽  
Author(s):  
Hongliu Zeng ◽  
Milo M. Backus

We examine field seismic data to test the benefits of 90°-phase wavelets in thin-bed interpretation that are predicted by seismic modeling in part 1 of this paper. In an interbedded sandstone-shale Miocene succession in the Gulf of Mexico basin, a 90°-phase shift of nearly zero-phase seismic data significantly improves lithologic and stratigraphic interpretation. A match between seismic and acoustic impedance (AI) profiles results in a better tie between seismic amplitude traces and lithology-indicative logs. Better geometric imaging of AI units that does not use dual-polarity seismic events results in easier and more accurate reservoir delineation. Less amplitude distortion and the stratigraphy-independent nature of thin-bed interference significantly improves stratigraphic resolution and seismic stratigraphic profiling. For a Ricker-like wavelet having small side lobes, stratigraphic resolution of 90°-phase data is considerably higher than that of zero-phase data. In this specific case, stratigraphic resolution of 90°-phase data is λ/4 (λ = wavelength), compared with λ/2 for its zero-phase counterpart. Stratal slices made from 90°-phase data show geomorphologic patterns of depositional systems with less noise and fewer interference fingerprints. A Permian Basin field provides a real-world example of porous zones in thin, high-frequency carbonate sequences that are better visualized with 90°-phase seismic data than with zero-phase data.


2014 ◽  
Vol 32 (3) ◽  
pp. 497
Author(s):  
Gary Corey Aldunate ◽  
Reynam C. Pestana

ABSTRACT. The 3-D acoustic wave equation is generally solved using finite difference schemes on the mesh which defines the velocity model. However, whennumerical solution of the wave equation is done by finite difference schemes, attention should be taken with respect to dispersion and numerical stability. To overcomethese problems, one alternative is to solve the wave equation in the Fourier domain. This approach is stabler and makes possible to separate the full wave equation inits unidirectional equations. Thus, the full wave equation is decoupled in two first order differential equations, namely two equations related to the vertical component:upgoing (-Z) and downgoing (+Z) unidirectional equations. Among the solution methods, we can highlight the Split-Step-Plus-Interpolation (SS-PSPI). This methodhas been proven to be quite adequate for migration problems in 3-D media, providing satisfactory results at low computational cost. In this work, 3-D seismic modelingis implemented using Huygens’ principle and an equivalent simulation of the full wave equation solution is obtained by properly applying the solutions of the twouncoupled equations. In this procedure, a point source wavefield located at the surface is extrapolated downward recursively until the last depth level in the velocityfield is reached. A second extrapolation is done in order to extrapolate the wavefield upwards, from the last depth level to the surface level, and at each depth level thepreviously stored wavefield (saved during the downgoing step) is convolved with a reflectivity model in order to simulate secondary sources. To perform depth pre-stackmigration of 3-D datasets, the decoupled wave equations were used and the same process described for seismic modeling is applied for the propagation of sources andreceivers wavefields. Thus, depth migrated images are obtained using appropriate image conditions: the upgoing and downgoing wavefields of sources and receiversare correlated and the migrated images are formed. The seismic modeling and migration methods using upgoing and downgoing wavefields were tested on simple 3-Dmodels. Tests showed that the addition of upgoing wavefield in seismic migration, provide better result and highlight steep deep reflectors which do not appear in theresults using only downgoing wavefields.Keywords: 3-D seismic modeling and migration, Upoing and downgoing wavefields, Split-Step Phase Shift Plus Interpolation method, Decoupled wave equations,One-Way equations.RESUMO. A equação da onda acústica tridimensional é normalmente resolvida usando-se esquemas de diferenças finitas sobre a malha que define o modelo develocidade. Entretanto, deve-se ter cuidado com a dispersão e a estabilidade numérica durante o processo de propagação da onda na malha. Uma outra alternativa, bastante eficiente de se resolver a equação completa da onda, é desacoplando-a em duas equações de onda unidirecionais no domínio transformado de Fourier (solução pseudo-espectral). Assim, a equação completa da onda é separada em duas equações diferenciais de primeira ordem relativa á componente vertical: equação da ondaascendente (-Z) e da onda descendente (+Z). Normalmente, a equação unidirecional é resolvida com diferentes ordens de aproximação. Entre esses métodos, podemos destacar o método “Split-Step-Plus-Interpolation” (SS-PSPI), que tem sido bastante adequado para problemas de migração em meios 3-D, fornecendo resultados aum baixo custo computacional. Neste trabalho, o modelamento sísmico 3-D foi implementado usando-se o princípio de Huygens com as duas equações de onda unidirecionais desacopladas. Com o objetivo de simular uma solução equivalente à solução da equação completa, uma fonte pontual localizada na superfície é extrapoladaem profundidade, de forma recursiva, até atingir o último nível de profundidade na malha do modelo de velocidades. Uma segunda extrapolação é realizada para extrapolar para cima o campo de onda, desde o último nível em profundidade até à superfície do modelo. Assim, os receptores localizados na superfície registram ocampo de onda ascendente, que trazem informações dos refletores em subsuperfície na forma de reflexões e difrações. Para realizar a migração pré-empilhamento em profundidade de dados 3-D, usando-se as equações de onda desacopladas, o mesmo procedimento descrito para o modelamento sísmico é utilizado para a propagação dos campos de onda de fontes e receptores. Imagens migradas são obtidas usando-se condições de imagem apropriadas, onde os campos de onda da fonte e dos receptores, descendente e ascendente, são correlacionados. Sobre modelos 3-D simples foram testados os métodos de modelamento e migração, levando em conta oscampos de onda ascendente e descendente. Ficando, assim, evidenciado que no método de migração sísmica, proposto aqui, a adição do campo de onda ascendente fornece um melhor resultado, ressaltando os refletores íngremes que não aparecem nos resultados utilizando-se apenas a extrapolação do campo de onda descendente.Palavras-chave: Migração e modelagem sísmica 3-D, Migração em duas etapas mais interpolação, equações de ondas unidirecionais.


2012 ◽  
Vol 4 (3) ◽  
pp. 365-372 ◽  
Author(s):  
Guido Valerio ◽  
Alessandro Galli ◽  
Donald R. Wilton ◽  
David R. Jackson

In this work, a very efficient mixed-potential integral-equation formulation is implemented for the rigorous analysis of multilayered structures with arbitrarily shaped two-dimensional periodic metallic and/or dielectric inclusions. Original acceleration techniques have been developed for the computation of the components of the scalar and dyadic Green's functions, based on different types of asymptotic extractions according to the potential considered. The theoretical approach and its computational convenience have been validated through different full-wave analyses concerning both scattering problems and complex-mode dispersive behaviors in various frequency-selective structures for microwave applications.


Author(s):  
Pedro Walfir Martins Souza Filho ◽  
Maâmar El-Robrini

The Bragança Coastal Plain is located in the Northeastern of Pará, in the Bragança-Viseu CoaxialBasin (Cretaceous), with an approximate surface area of 1,570 Km2. The geometry of the basin and itspaleotopography, associated with recent tectonic movements have controlled the distribution and thethickness of the tertiary and quaternary deposits. This coastal plain constitutes a macrotidal (6 m) depositionalsystem, developed in a hot and humid equatorial climate, with a dry and wet well defined seasons and anannual precipitation averaging 3,000 mm.The geomorphology of the area is subdivided into three main morphologic realms: (1) alluvial plain,with fluvial channel, levees and flood plain; (2) estuarine plain, with an estuarine channel subdivided intoestuarine funnel segment, straight segment, meandering segment and upstream channel, tidal creek and,floodplain and; (3) coastal plain, with salt marsh (inner and outer), tidal plain (supratidal mangroves,intertidal mangroves and sand flats with tidal shoals), chenier, coastal dunes and beach environments.The recent morpho-sedimentary units are separated from highland by a line of inactive cliffs that issituated 25 km from the coastline. This cliffs mark the higher Holocene sea level, very well knowed inbrazilian east coast as Holocenic Transgression (5,100 years B.P.). During this event was deposited a basaltransgressive sequence (S1), constituted by estuarine sand and mud and marine sand. Afterwards, underregressive or stillstand sea level the mangrove deposits prograde over the transgressive sand sheet buildinga prograding sequence (S2). Nowadays, this sequence are being overlain by a recent transgressive sequence(S3).The sedimentary model, based on lithostratigraphy and sedimentary processes, proposed to BragançaCoastal Plain show a complex coastal depositional system, constituted by different sedimentaryenvironments with singular sedimentary, stratigraphic and morphologic characteristics in relation to itsgeometry and spacial distribution of the environments.The morpho-sedimentary unit show that the environments studied from the alluvial plain to coastalplain represent a dynamic area dominated by macrotides and influenced by waves along the shoreline.Therefore, the depositional model proposed is composed by a coastal plain depositional system withfluvial-estuarine-tidal flat environments with dune-beach ridge associated.


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