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Helms - Potential Theory

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Helms Potential Theory
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    Potential Theory
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Potential Theory presents a clear path from calculus to classical potential theory and beyond, with the aim of moving the reader into the area of mathematical research as quickly as possible. The subject matter is developed from first principles using only calculus. Commencing with the inverse square law for gravitational and electromagnetic forces and the divergence theorem, the author develops methods for constructing solutions of Laplaces equation on a region with prescribed values on the boundary of the region. The latter half of the book addresses more advanced material aimed at those with the background of a senior undergraduate or beginning graduate course in real analysis. Starting with solutions of the Dirichlet problem subject to mixed boundary conditions on the simplest of regions, methods of morphing such solutions onto solutions of Poissons equation on more general regions are developed using diffeomorphisms and the Perron-Wiener-Brelot method, culminating in application to Brownian motion. In this new edition, many exercises have been added to reconnect the subject matter to the physical sciences. This book will undoubtedly be useful to graduate students and researchers in mathematics, physics, and engineering.;Preliminaries -- Laplaces Equation -- The Dirichlet Problem -- Green Functions -- Negligible Sets -- Dirichlet Problem for Unbounded Regions -- Energy -- Interpolation and Monotonicity -- Newtonian Potential -- Elliptic Operators -- Apriori Bounds -- Oblique Derivative Problem -- Application to Diffusion Processes

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Lester L. Helms Universitext Potential Theory 2nd ed. 2014 10.1007/978-1-4471-6422-7_1
Springer-Verlag London 2014
1. Preliminaries
Lester L. Helms 1
(1)
University of Illinois, Urbana, IL, USA
Lester L. Helms
Email:
Abstract
The first chapter establishes the notation to be used throughout the book, reviews the Arcola-Ascoli theorems that are indispensable for selecting subsequences of sequences of functions or their derivatives and convergence of sequences of measures. In preparation for exercises throughout the book, conservative vector fields and their associated potential functions are reviewed. The chapter concludes with exercises that the typical reader will recall from undergraduate physics.
1.1 Notation
An element of the Potential Theory - image 1 -dimensional Euclidean space Potential Theory - image 2 , will be denoted by Potential Theory - image 3 and its length Potential Theory - image 4 is defined by Potential Theory - image 5 . If Potential Theory - image 6 and Potential Theory - image 7 , the inner product Potential Theory - image 8 is defined by Potential Theory - image 9 , and the distance between Picture 10 and Picture 11 is defined to be Picture 12 . The angle between two nonzero vectors Picture 13 and Potential Theory - image 14 is defined to be the angle Potential Theory - image 15 such that Potential Theory - image 16 and
Potential Theory - image 17
The zero vector of Potential Theory - image 18 is denoted by Potential Theory - image 19 . The ball with center and radius is defined by the sph - photo 20 with center and radius is defined by the sphere with center - photo 21 and radius is defined by the sphere with center and radius - photo 22 is defined by the sphere with center and radius is defined by - photo 23 ; the sphere with center and radius is defined by The closure of a set - photo 24 and radius is defined by The closure of a set is denoted by - photo 25 is defined by The closure of a set is denoted by or by it - photo 26 . The closure of a set Picture 27 is denoted by Picture 28 or by Picture 29 , its interior by Picture 30 , and its complement by Potential Theory - image 31 . The standard basis for Potential Theory - image 32 will be denoted by Potential Theory - image 33 where Picture 34 has a Picture 35 in the Potential Theory - image 36 th position and Potential Theory - image 37 in all other positions.
The spherical coordinates of a point Potential Theory - image 38 in Potential Theory - image 39 are defined as follows: if Potential Theory - image 40 , then
Potential Theory - image 41
is a point of Potential Theory - image 42 , the unit sphere with center at Picture 43 . The Picture 44 and Picture 45 of the ordered pair Picture 46 are called the spherical coordinates of the point This transformation from rectangular coordinates to spherical coordinates is - photo 47 . This transformation from rectangular coordinates to spherical coordinates is essentially the mapping where Letting is the cosine of the - photo 48 where
Letting is the cosine of the angle between - photo 49
Letting Potential Theory - image 50 , Potential Theory - image 51
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