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  • 1
    Monograph available for loan
    Monograph available for loan
    Cambridge [u.a.] : Cambridge Univ. Press
    Call number: 9/M 11.0074
    Description / Table of Contents: Presenting a rigorous treatment of the physical and mechanical basis for the modelling of sedimentary basins, this book supplies geoscientists with practical tools for creating their own models. It begins with a thorough grounding in properties of porous media, linear elasticity, continuum mechanics and rock compressibility. Chapters on heat flow, subsidence, rheology, flexure and gravity consider sedimentary basins in the context of the Earth's lithosphere, and the book concludes with coverage of pore space cementation, compaction and fluid flow. The volume introduces basic, state-of-the-art models and demonstrates how to reproduce results using tools like MATLAB and Octave. Main equations are derived from first principles, and their basic solutions obtained and then applied.
    Type of Medium: Monograph available for loan
    Pages: XV, 527 S. , Ill., graph. Darst.
    ISBN: 0521761255 , 978-0-521-76125-3
    Classification:
    Sedimentology
    Location: Reading room
    Branch Library: GFZ Library
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  • 2
    Electronic Resource
    Electronic Resource
    Oxford, UK : Blackwell Publishing Ltd
    Geophysical journal international 119 (1994), S. 0 
    ISSN: 1365-246X
    Source: Blackwell Publishing Journal Backfiles 1879-2005
    Topics: Geosciences
    Notes: A numerical model of combined fluid flow and heat flow is used to study convection in sedimentary basins during compaction. the main issue of the paper is the interaction of non-Rayleigh convection flow with compaction flow and/or meteoric flow. It is shown that under reasonable assumptions, the flow inside a permeable layer is the superposition of the compaction flow through the layer and the thermal convection flow in the layer. These assumptions are expressed in terms of the time constants involved. Non-Rayleigh convection roll(s) will therefore appear if the compaction flow (or the meteoric flow) is less than the thermally induced flow. This condition can be stated by a simple expression involving the Rayleigh number for the layer and the absolute value of the flow velocity through the layer. Two case studies are presented, which show non-Rayleigh convection in compacting basins. A numerical example of Rayleigh convection is also presented, which demonstrates that Rayleigh convection, under realistic conditions such as compressible rock and non-perfect thermal conducting top and bottom boundaries, is a complex process. This case study shows that even a ‘small’ amount of vertical excess pressure gradient is enough to stabilize the fluid inside a layer.sedimentary basinsthermal convection
    Type of Medium: Electronic Resource
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  • 3
    Electronic Resource
    Electronic Resource
    Oxford, UK : Blackwell Publishing Ltd
    Geophysical journal international 121 (1995), S. 0 
    ISSN: 1365-246X
    Source: Blackwell Publishing Journal Backfiles 1879-2005
    Topics: Geosciences
    Notes: The 1-D models of segregated two-phase flow in reservoir engineering are utilized to model lateral secondary migration of hydrocarbons in slightly inclined and permeable layers. It is assumed that the layers are sealed below and above by low-permeability strata. The flow is then characterized by a gravity number and a mobility ratio when capillary forces are neglected. For buoyancy-driven migration, gravity numbers (much) larger than 1, these models imply that the Darcy velocity of the flow is only given by the buoyancy force due to the density difference between water and oil. For gravity numbers larger than 1, the thickness of the hydrocarbon zone below the sealing top is proportional to the inverse gravity number. Furthermore, if the oil flow in the layer is only a small fraction of the total flow, the height of the hydrocarbon zone is also proportional to this fraction. It is therefore concluded that in buoyancy-driven migration with large gravity numbers, where the hydrocarbon part of the total flow is small, only a small fraction of the upper part of the layer is saturated with oil. Therefore, only a little oil may be lost due to irreducible saturation, and long-range migration is possible.
    Type of Medium: Electronic Resource
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  • 4
    Electronic Resource
    Electronic Resource
    Oxford, UK : Blackwell Publishing Ltd
    Geophysical journal international 110 (1992), S. 0 
    ISSN: 1365-246X
    Source: Blackwell Publishing Journal Backfiles 1879-2005
    Topics: Geosciences
    Notes: This article is about what influence continuous sedimentation has on the excess pressure, compaction and temperature in a sedimentary basin. We give an answer in terms of two dimensionless numbers Λ0 and Λ0, which characterize the pressure and the temperature solution respectively. Λ0= 1 is shown to define a transitional zone between excess pressured basins (with low compaction) and hydrostatic basins (with high compaction). The Λ0 parameter generalizes earlier results of Gibson. The most important physical parameter in Λ0 is the ratio between the permeability and the sedimentation rate. By means of Λ0 we can quantify when ‘high’ sedimentation rates and ‘low’ permeability yield high excess pressures.This analysis is based on the porosity given by formulae of the form φ=φ(αps), where ps is the effective stress, and α is some scaling factor.In an analogous manner, Λ1= 1 defines a transitional zone when moving boundary effects become marked on the temperature. The most important parameter in Λ1 is the ratio between α and the sedimentation rate.Simulation results are obtained by solving dimensionless pressure and temperature equations. The numerical pressure solution is compared with the exact solution given by Gibson, and is shown to be in excellent accordance.
    Type of Medium: Electronic Resource
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  • 5
    Electronic Resource
    Electronic Resource
    Oxford, UK : Blackwell Publishing Ltd
    Geophysical journal international 115 (1993), S. 0 
    ISSN: 1365-246X
    Source: Blackwell Publishing Journal Backfiles 1879-2005
    Topics: Geosciences
    Notes: We present a simple 1-D and one-lithology model of integrated hydrocarbon generation and vertical migration. Although the model is very simple, it captures some of the most basic features of the vertical migration process, like expulsion from source rocks, and vertical migration in carrier beds above and below the source rock. The dynamics in the model are caused by sedimentation, which is done at a constant rate. Owing to sedimentation, the source rock is brought down to the depths where kerogen breakdown starts. This two-phase model is based on fractional flow theory, which makes it possible to avoid a pressure equation. The solution of the saturation equation is characterized by a dimensionless number, the gravity number, and the ‘size’ of the capillary forces. When the gravity number is less than 1, buoyancy is less important, while for gravity numbers greater than 1, buoyancy is dominating. We discuss capillary effects, and estimate a Peclet number for the migration process, which shows that capillary forces are less important in this one-lithology model. In the special case of no compaction, negligible capillarity and no generation of pore space due to the kerogen breakdown, we can approximate a solution to the saturation equation by considering Riemann problems. We find that above the source region, we get at least a shock and possibly a rarefaction, too. Below the source region, we have at least a rarefaction wave, and possibly a shock. We present explicit expressions for the shock position, and the characteristics propagating saturations. These solutions enable us to decide if, and when, the shock will reach the top of the basin. If we know the total oil production, we can read off from the flux function curve an approximation of the saturation propagated upwards. Although these solutions apply to the case of no compaction, negligible capillarity and no generation of pore space, they are useful approximations if any of these restrictions is only ‘weakly violated.
    Type of Medium: Electronic Resource
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  • 6
    Electronic Resource
    Electronic Resource
    Springer
    Transport in porous media 26 (1997), S. 299-318 
    ISSN: 1573-1634
    Keywords: non-Rayleigh convection ; aquifer flow.
    Source: Springer Online Journal Archives 1860-2000
    Topics: Geosciences , Technology
    Notes: Abstract Non-Rayleigh convection is studied in aquifers, where the lateral variations of the temperature field are caused by the ground surface. Analytical solutions for the stream function, the Darcy velocities and the excess water pressure are found for a confined, rectangular and homogeneous aquifer situated at a given depth. The Darcy velocity field and the excess pressure are also found for an unconfined aquifer with a prescribed fluid potential at the top surface of the aquifer. Approximate solutions for excess pressure and Darcy velocities are found for the unconfined aquifer with a free surface. General estimates for the convective Darcy velocities are derived from these solutions. It is also shown that non-Rayleigh flow is unlikely in an unconfined aquifer.
    Type of Medium: Electronic Resource
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  • 7
    Electronic Resource
    Electronic Resource
    New York, NY [u.a.] : Wiley-Blackwell
    International Journal for Numerical and Analytical Methods in Geomechanics 17 (1993), S. 401-432 
    ISSN: 0363-9061
    Keywords: Engineering ; Engineering General
    Source: Wiley InterScience Backfile Collection 1832-2000
    Topics: Architecture, Civil Engineering, Surveying , Geosciences
    Notes: This article presents a numerical model of heat and fluid flow in compacting sedimentary basins formulated in Lagrangian co-ordinates. The Lagrangian co-ordinates are the sediment particle positions of the completely compacted basin. A finite element formulation of excess water pressure and temperature in these Lagrangian co-ordinates is presented, in addition to an equivalent formulation in the real co-ordinates. The later formulation is also Lagrangian of nature, since the elements of the grid in the real co-ordinates always frame the same sediment particles. In other words, it is the Lagrangian grid mapped to the real space. This is done in an iterative loop which solves for excess water pressure, and then updates the real co-ordinates of the sediment particles. By comparing the two finite element formulations it is concluded that the one in real space is the simplest, most efficient and most precise.The model is validated by comparison with two dimensionless one-dimensional solutions, one analytical for the linear case, and one numerical for the non-linear case. Both these one-dimensional solutions are obtained on the unit interval, where the moving top boundary caused by continuous sedimentation is incorporated.
    Additional Material: 17 Ill.
    Type of Medium: Electronic Resource
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  • 8
    Electronic Resource
    Electronic Resource
    New York, NY [u.a.] : Wiley-Blackwell
    International Journal for Numerical and Analytical Methods in Geomechanics 21 (1997), S. 91-120 
    ISSN: 0363-9061
    Keywords: finite elements ; oil migration ; immiscible two-phase flow ; compaction ; Engineering ; Civil and Mechanical Engineering
    Source: Wiley InterScience Backfile Collection 1832-2000
    Topics: Architecture, Civil Engineering, Surveying , Geosciences
    Notes: The upstream-weighted finite element method with lumped mass matrix is applied to the modelling of oil migration in compacting sedimentary basins. An implicit formulation is made in Lagrangian co-ordinates of a pressure, saturation and a temperature equation, which is based on immiscible two-phase flow of oil and water. The formulation accounts for the compaction of the sediments, the generation of oil from solid organic material (kerogen), the eventual pore space generated by kerogen breakdown, and the density variations of the fluids which may set up thermal convection. The model is validated by comparison with results from a one-dimensional (1D) fractional flow-based migration model. A 2D case example showing oil expulsion from source rocks, and the filling of a trap is presented. The mass balance of the model is easily checked because all oil in the basin originates from breakdown of kerogen. Compared with other alternatives, the simple upstream-weighted finite element method is suggested as a possible first choice for a numerical method for the modelling of oil migration in compacting sedimentary basins. It easily deals with the complex geometry of a basin, it yields reasonably good results, is simple to implement, and the same implementation applies to all spatial dimensions. © 1997 by John Wiley & Sons, Ltd.
    Additional Material: 10 Ill.
    Type of Medium: Electronic Resource
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  • 9
    Electronic Resource
    Electronic Resource
    New York, NY [u.a.] : Wiley-Blackwell
    International Journal for Numerical and Analytical Methods in Geomechanics 15 (1991), S. 705-733 
    ISSN: 0363-9061
    Keywords: Engineering ; Engineering General
    Source: Wiley InterScience Backfile Collection 1832-2000
    Topics: Architecture, Civil Engineering, Surveying , Geosciences
    Notes: In this article we solve the equations for a 2D model of compaction of sedimentary basins saturated with water by the finite-element method. This compaction model considers the rock described by the porosity as a function of effective stress, and both the anisotropic permeability and the anisotropic heat conductivity as functions of porosity. The water density is approximated linearly in the water pressure and temperature, and the water viscosity is a function of temperature. The main variables in the model are the water excess pressure and the temperature, and we account for an implicit solution scheme where we solve for both main variables simultaneously. The non-linearities in the model are either dealt with by the Newton method or by fixed-point iterations. We compare the coupled solution of temperature and pressure with the same decoupled equations. Then we study the contribution to the temperature by convection, the effect of the non-constant water density, and some anisotropic case examples.
    Additional Material: 19 Ill.
    Type of Medium: Electronic Resource
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  • 10
    Publication Date: 2011-06-01
    Print ISSN: 0920-4105
    Electronic ISSN: 1873-4715
    Topics: Chemistry and Pharmacology , Geosciences , Process Engineering, Biotechnology, Nutrition Technology
    Published by Elsevier
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