Abstract:The bifurcation function for an elliptic boundary value problem is a vector field B(ω) on R d whose zeros are in a one-to-one correspondence with the solutions of the boundary value problem. Finite element approximations of the boundary value problem are shown to give rise to an approximate bifurcation function B h (ω), which is also a vector field on R d . Estimates of the difference B(ω) − B h (ω) are derived, and methods for computing B h (ω) are discussed.
“…Since E h (λ) → E(λ) as h → 0, it follows that we also have E h (λ) → E(λ) as h → 0. The next result, proven in [19], gives an estimate of the difference between the computable quantities σ h (ω, λ), z h (ω, λ), B h (ω, λ) and the theoretical quantities σ(ω, λ)z(ω, λ), B(ω, λ).…”
Section: Finite Element Approximations Of B and E(λ)mentioning
confidence: 85%
“…This article follows and extends the methods and results of our previous article [19], which discusses the basic process of reduction to a bifurcation function B(ω, λ) and the use of finite elements to obtain an approximating bifurcation function B h (ω, λ). The main results of [19] are error estimates on the approximations B h ≈ B and z h ≈ z, where z and z h are potentially (see Section II) a solution and its approximation. A key ingredient in these estimates is an error estimate for a solution v = σ(ω, λ) of an auxiliary boundary value problem.…”
Section: Introductionmentioning
confidence: 92%
“…Its solution requires the use of projections and a pseudo-inverse. Implementation and algorithmic issues are discussed in [19].…”
Section: Examplesmentioning
confidence: 99%
“…These estimates, which show the Morse indices and energy levels can be accurately computed, are presented in Section IV. The article concludes with several examples in Section V. Remarks on implementation and examples discussing convergence can be found in [19].…”
A numerical method for computing all solutions of an elliptic boundary value problem Au + g [u, λ] = 0 and their Morse indices as steady-states of the parabolic problem ut + Au + g [u, λ] = 0, is presented. Morse decompositions are also determined. The method uses a finite element approach that is based on the method of alternative problems. Error estimates for the finite element approximations are verified and examples are given.
“…Since E h (λ) → E(λ) as h → 0, it follows that we also have E h (λ) → E(λ) as h → 0. The next result, proven in [19], gives an estimate of the difference between the computable quantities σ h (ω, λ), z h (ω, λ), B h (ω, λ) and the theoretical quantities σ(ω, λ)z(ω, λ), B(ω, λ).…”
Section: Finite Element Approximations Of B and E(λ)mentioning
confidence: 85%
“…This article follows and extends the methods and results of our previous article [19], which discusses the basic process of reduction to a bifurcation function B(ω, λ) and the use of finite elements to obtain an approximating bifurcation function B h (ω, λ). The main results of [19] are error estimates on the approximations B h ≈ B and z h ≈ z, where z and z h are potentially (see Section II) a solution and its approximation. A key ingredient in these estimates is an error estimate for a solution v = σ(ω, λ) of an auxiliary boundary value problem.…”
Section: Introductionmentioning
confidence: 92%
“…Its solution requires the use of projections and a pseudo-inverse. Implementation and algorithmic issues are discussed in [19].…”
Section: Examplesmentioning
confidence: 99%
“…These estimates, which show the Morse indices and energy levels can be accurately computed, are presented in Section IV. The article concludes with several examples in Section V. Remarks on implementation and examples discussing convergence can be found in [19].…”
A numerical method for computing all solutions of an elliptic boundary value problem Au + g [u, λ] = 0 and their Morse indices as steady-states of the parabolic problem ut + Au + g [u, λ] = 0, is presented. Morse decompositions are also determined. The method uses a finite element approach that is based on the method of alternative problems. Error estimates for the finite element approximations are verified and examples are given.
“…In particular, one may search for folds in nonlinear maps defined on functions with unbounded domains, which are natural in physical situations. Fibers also provide the conceptual starting point for algorithms that solve a class of partial differential equations, an idea originally suggested by Smiley ([31], [32]) and later implemented for finite spectral interaction of the Dirichlet Laplacian on rectangles in [8].…”
Since the seminal work of Ambrosetti and Prodi, the study of global folds was enriched by geometric concepts and extensions accomodating new examples. We present the advantages of considering fibers, a construction dating to Berger and Podolak's view of the original theorem. A description of folds in terms of properties of fibers gives new perspective to the usual hypotheses in the subject. The text is intended as a guide, outlining arguments and stating results which will be detailed elsewhere.
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