Matthias Albert Augustin's A Method of Fundamental Solutions in Poroelasticity to Model PDF

By Matthias Albert Augustin

ISBN-10: 3319170783

ISBN-13: 9783319170787

ISBN-10: 3319170791

ISBN-13: 9783319170794

This monograph makes a speciality of the numerical tools wanted within the context of constructing a competent simulation software to advertise using renewable strength. One very promising resource of strength is the warmth kept within the Earth’s crust, that's harnessed by way of so-called geothermal amenities. Scientists from fields like geology, geo-engineering, geophysics and particularly geomathematics are referred to as upon to aid make geothermics a competent and secure power creation procedure. one of many demanding situations they face contains modeling the mechanical stresses at paintings in a reservoir.
The target of this thesis is to enhance a numerical answer scheme via which the fluid strain and rock stresses in a geothermal reservoir should be made up our minds ahead of good drilling and through construction. For this function, the strategy may still (i) comprise poroelastic results, (ii) supply a method of together with thermoelastic results, (iii) be low-cost by way of reminiscence and computational energy, and (iv) be versatile with reference to the destinations of knowledge points.
After introducing the elemental equations and their family members to extra conventional ones (the warmth equation, Stokes equations, Cauchy-Navier equation), the “method of basic ideas” and its power worth referring to our activity are mentioned. in keeping with the houses of the basic suggestions, theoretical effects are tested and numerical examples of tension box simulations are provided to evaluate the method’s functionality. The first-ever 3D pictures calculated for those subject matters, which neither requiring meshing of the area nor concerning a time-stepping scheme, make this a pioneering volume.

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J;1 ; : : : ; j;n 1 /. 0/ W yn > 0g, (d) If . j;1 ; : : : ; j;n / and . 0/. m 1 For the different kinds of regularity, we have (v) H) (iv) H) (iii) H) (i). These regularity properties require ˝ to lie on only one side of its boundary, whereas the cone property does not impose this condition. 15 (i) If ˝ is bounded, the requirements for ˝ being strong local Lipschitz reduce to the condition that for each point x 2 @˝, there exists a neighborhood U of x such that U \ @˝ is the graph of a Lipschitz-continuous function.

And the functions 1; : : : ; n belong to The following summary of regularity conditions is taken from the book by Adams [3, pp. 66f] and is just slightly adapted. z/ and an open cover fUj g of a set ˝ is said to be locally finite if any compact set in Rn can intersect at most finitely many elements of fUj g[3, p. 65ff]. 14 (Regularity of Domains) Let ˝ has Rn , n 2 N, be a domain. 3 Function Spaces 19 (ii) The cone property if there exists a finite cone C such that each point x 2 ˝ is the vertex of a finite cone Cx contained in ˝ and congruent to C .

The integral on the left-hand side is well known from the theory of linear elasticity. It defines a symmetric bilinear form e. ˝/ . Continuity results from the Cauchy-Schwarz inequality. 56) ˝ for isotropic materials with > 0, > 0. To show that e. 5 (Korn’s Inequality) Let ˝ be a domain in R3 . 57) and, thus, the mapping v 7! ˝/ . , [102]. From Korn’s inequality, the coercivity of e. 6 Let ˝ be a domain in R3 , let d be a measurable subset of @˝. ˝/. If meas. , on the space V, the semi-norm v 7!

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A Method of Fundamental Solutions in Poroelasticity to Model the Stress Field in Geothermal Reservoirs by Matthias Albert Augustin


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