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Convergence proof

Consider an approximate description of the nonpenetration condition between the crack faces which can be obtained by putting c = 0 in (3.45). Similar to the case c > 0, we can analyse the equilibrium problem of the plates and prove the solution existence of the optimal control problem of the plates with the same cost functional. We aim at the convergence proof of solutions of the optimal control problem as —> 0. In this subsection we assume that T, is a segment of a straight line parallel to the axis x. [Pg.194]

Introduction. - Linear functionals and adjoint operators of different types are used as tools in many parts of modem physics [1]. They are given a strict and deep going treatment in a rich literature in mathematics [2], which unfortunately is usually not accessible to the physicists, and in addition the methods and terminology are unfamiliar to the latter. The purpose of this paper is to give a brief survey of this field which is intended for theoretical physicists and quantum chemists. The tools for the treatment of the linear algebra involved are based on the bold-face symbol technique, which turns out to be particularly simple and elegant for this purpose. The results are valid for finite linear spaces, but the convergence proofs needed for the extension to infinite spaces are usually fairly easily proven, but are outside the scope of the present paper. [Pg.372]

Convergence proofs are available under certain conditions (Finlayson, 1980), and once the iterate value gets close to the solution, the convergence is very rapid. This method is generally better than the successive substitution method, except for special cases, but sometimes a good initial guess is required. [Pg.308]

To complete the convergence proof for Verlet s method, we would still need to verify the second assumption. This requires the assumption that the force field F satisfy a Lipschitz condition ... [Pg.68]

Darcy was a civil engineer in the city of Dijon. In 1856 he published a book [4] in which he stated what later became known as Darcy law. His conclusions were made purely on the basis of practical experiments in the water supply system of his city. His law has survived ever since. Surprisingly, it was not before 1980 that a theoretical derivation of this law was given. In the papers Keller [10] the method of iwo-scale asymptotic expansions was used and in Tartar [13] a rigorous convergence proof was given. The basic assumptions of these derivations are that in the pore space of a porous medium laminar flow can be described by the standard Stokes equations... [Pg.86]

Two-scale convergence is a recently introduced notion that mimics what we just have described in the framework of functional analysis (see Allaire [1]). It is a unification of the concept of weak convergence and the idea of micro- and macro-variables. The attractive feature of the theory developed in this context is that it allows elegant and clearly structured convergence proofs. [Pg.88]

An explicit convergence proof for Sobolev norms can be found in [15). Let us fix the sampling nodes and increase the domain fi. What we observe is that, similar to the surface spline, the bicubic B-spline interpolant tends to a linear polynomial. [Pg.402]

Proof Let pm G be a minimizing sequence. It is bounded in and hence the convergence (2.135) can be assumed. For every m, the solution of the following variational inequality can be found ... [Pg.111]

Therefore, (2.270) leads to the second strong convergence shown in Theorem 2.29. The proof is complete. [Pg.163]

Proof. The condition ITi G means that there exists a sequence of smooth functions IT/ = strongly converging to ITi in... [Pg.254]

Although we have a proof that the major iteration always converges, the... [Pg.51]

Regarding accuracy, the finite difference approximations for the radial derivatives converge O(Ar ). The approximation for the axial derivative converges 0(Az), but the stability criterion forces Az to decrease at least as fast as Ar. Thus, the entire computation should converge O(Ar ). The proof of convergence requires that the computations be repeated for a series of successively smaller grid sizes. [Pg.277]

The proof of convergence of scheme (19) reduces to the estimation of a solution of problem (21) in terms of the approximation error. In the sequel we obtain such estimates using the maximum principle for domains of arbitrary shape and dimension. In an attempt to fill that gap, a non-equidistant grid... [Pg.247]

Alore a detailed proof of convergence of this scheme is concerned with the form (74) and a priori estimates obtained in Chapter 6, Section 2 and so it is omitted here. As a final result we deduce that scheme (70) converges uniformly with the rate 0(r -f lE). [Pg.486]

The proof of this formula is omitted here. It should be noted that from such reasoning it seems clear that due to the summarized approximation in the space Hg-i the convergence occurs in the space Hb- That is to say, the conditions... [Pg.621]

On the other hand, a direct observational proof in support of the AML scenario is not possible, since old stars in M 67 have by now converged to rather low rotational rates and we do not have information on the original rotational velocities. Nevertheless, support (or lack thereof) to the scenario of Li depletion due to AML can be found using at least two different empirical tests namely, i) additional observations of Li in large samples of old cluster stars ii) measurements of Be. [Pg.176]


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See also in sourсe #XX -- [ Pg.130 ]




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Proof of convergence

Proofing

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