Book contents
- Frontmatter
- Contents
- Editor's Statement
- Foreword by Felix E. Browder
- Preface
- Chapter 0 Preliminaries
- Chapter 1 Introduction
- Chapter 2 The Cauchy Problem
- Chapter 3 The Initial-Value Problem
- Chapter 4 The Initial-Boundary-Value Problem for the Quarter Plane with Temperature-Boundary Specification
- Chapter 5 The Initial-Boundary-Value Problem for the Quarter Plane with Heat-Flux-Boundary Specification
- Chapter 6 The Initial-Boundary-Value Problem for the Semi-Infinite Strip with Temperature-Boundary Specification and Heat-Flux-Boundary Specification
- Chapter 7 The Reduction of Some Initial-Boundary-Value Problems for the Semi-Infinite Strip, to Integral Equations: Some Exercises
- Chapter 8 Integral Equations
- Chapter 9 Solutions of Boundary-Value Problems for All Times and Periodic Solutions
- Chapter 10 Analyticity of Solutions
- Chapter 11 Continuous Dependence upon the Data for Some State-Estimation Problems
- Chapter 12 Some Numerical Methods for Some State-Estimation Problems
- Chapter 13 Determination of an Unknown Time-Dependent Diffusivity a(t) from Overspecified Data
- Chapter 14 Initial- and/or Boundary-Value Problems for General Regions with Hölder Continuous Boundaries
- Chapter 15 Some Properties of Solutions in General Domains
- Chapter 16 The Solution in a General Region with Temperature-Boundary Specification: The Method of Perron-Poincaré
- Chapter 17 The One-Phase Stefan Problem with Temperature-Boundary Specification
- Chapter 18 The One-Phase Stefan Problem with Flux-Boundary Specification: Some Exercises
- Chapter 19 The Inhomogeneous Heat Equation ut = uxx + f(x, t)
- Chapter 20 An Application of the Inhomogeneous Heat Equation: The Equation ut = uxx + F(x,t,u,ux)
- Some References to the Literature on ℒ(u) ≡ uxx – ut
- Symbol Index
- Subject Index
Chapter 16 - The Solution in a General Region with Temperature-Boundary Specification: The Method of Perron-Poincaré
Published online by Cambridge University Press: 05 February 2012
- Frontmatter
- Contents
- Editor's Statement
- Foreword by Felix E. Browder
- Preface
- Chapter 0 Preliminaries
- Chapter 1 Introduction
- Chapter 2 The Cauchy Problem
- Chapter 3 The Initial-Value Problem
- Chapter 4 The Initial-Boundary-Value Problem for the Quarter Plane with Temperature-Boundary Specification
- Chapter 5 The Initial-Boundary-Value Problem for the Quarter Plane with Heat-Flux-Boundary Specification
- Chapter 6 The Initial-Boundary-Value Problem for the Semi-Infinite Strip with Temperature-Boundary Specification and Heat-Flux-Boundary Specification
- Chapter 7 The Reduction of Some Initial-Boundary-Value Problems for the Semi-Infinite Strip, to Integral Equations: Some Exercises
- Chapter 8 Integral Equations
- Chapter 9 Solutions of Boundary-Value Problems for All Times and Periodic Solutions
- Chapter 10 Analyticity of Solutions
- Chapter 11 Continuous Dependence upon the Data for Some State-Estimation Problems
- Chapter 12 Some Numerical Methods for Some State-Estimation Problems
- Chapter 13 Determination of an Unknown Time-Dependent Diffusivity a(t) from Overspecified Data
- Chapter 14 Initial- and/or Boundary-Value Problems for General Regions with Hölder Continuous Boundaries
- Chapter 15 Some Properties of Solutions in General Domains
- Chapter 16 The Solution in a General Region with Temperature-Boundary Specification: The Method of Perron-Poincaré
- Chapter 17 The One-Phase Stefan Problem with Temperature-Boundary Specification
- Chapter 18 The One-Phase Stefan Problem with Flux-Boundary Specification: Some Exercises
- Chapter 19 The Inhomogeneous Heat Equation ut = uxx + f(x, t)
- Chapter 20 An Application of the Inhomogeneous Heat Equation: The Equation ut = uxx + F(x,t,u,ux)
- Some References to the Literature on ℒ(u) ≡ uxx – ut
- Symbol Index
- Subject Index
Summary
INTRODUCTION
We consider the problem
where f, g, h, s1, and s2 are continuous functions of their respective arguments, f(a) = g(0), and f(b) = h(0). (See Fig. 16.1.1.) Let
and let BT denote its boundary. For what follows it is convenient to define
Denoting by F the triple (g, f, h) on BT, Problem (16.1.1) condenses to the Statement
From the definition of DT, we see that for, any point (x, t) ∈ DT, there exists a closed polygonal region P with one side a line segment contained in {T} ∩ DT, another a line segment contained in {τ} ∩ DT, 0 < τ < t, and the remaining boundary of P consisting of two nonintersecting polygonal curves whose line segments are not characteristics and which connect, respectively, the left endpoint of the line segment on t = τ to the left endpoint of the line segment on t = T and the right endpoint to the right endpoint, such that (x, t) ∈ P°, the interior of P.
Remark. We shall call all such polygonal regions P admissible. Moreover, we shall utilize only admissible P in the discussion below.
For all such admissible P, we define the following operator MP on continuous functions in DT ∪ BT.
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- The One-Dimensional Heat Equation , pp. 265 - 280Publisher: Cambridge University PressPrint publication year: 1984