Book Review: Solution of continuous nonlinear PDEs through order completion

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Arbitrary Continuous Nonlinear PDEs through the Order Completion Method

In 1994 we showed that very large classes of systems of nonlinear PDEs have solutions which can be assimilated with usual measurable functions on the Euclidean domains of definition of the respective equations. Recently, the regularity of such solutions has significantly been improved by showing that they can in fact be assimilated with Hausdorff continuous functions. The method of solution of ...

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Hausdorff Continuous Solutions of Nonlinear PDEs through the Order Completion Method

It was shown in [13] that very large classes of nonlinear PDEs have solutions which can be assimilated with usual measurable functions on the Euclidean domains of definition of the respective equations. In this paper the regularity of these solutions has significantly been improved by showing that they can in fact be assimilated with Hausdorff continuous functions. The method of solution of PDE...

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The Order Completion Method for Systems of Nonlinear PDEs Revisited

In this paper we presents further developments regarding the enrichment of the basic Theory of Order Completion as presented in (Oberguggenberger and Rosinger, 1994). In particular, spaces of generalized functions are constructed that contain generalized solutions to a large class of systems of continuous, nonlinear PDEs. In terms of the existence and uniqueness results previously obtained for ...

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existence and approximate $l^{p}$ and continuous solution of nonlinear integral equations of the hammerstein and volterra types

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The Order Completion Method for Systems of Nonlinear PDEs: Solutions of Initial Value Problems

and Applied Analysis 3 With respect to the pointwise order u ≤ v ⇐⇒ ( ∀x ∈ Ω : u (x) ≤ v (x) ) (11) the setNL(Ω) is a Dedekind complete lattice. In particular, the supremum and infimum of a setA ⊂ NL(Ω) is given by inf A = (I ∘ S) (φ) , (12) supA = (I ∘ S) (ψ) , (13) respectively, where φ : Ω ∋ x 󳨃→ inf{u(x) : u ∈ A} and ψ : Ω ∋ x 󳨃→ sup{u(x) : u ∈ A}. Furthermore, the lattice NL(Ω) is fully di...

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ژورنال

عنوان ژورنال: Bulletin of the American Mathematical Society

سال: 1996

ISSN: 0273-0979

DOI: 10.1090/s0273-0979-96-00620-9