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Unformatted text preview: Chapter 3 Vector integrals and integral theorems Syllabus covered: 1. Line, surface and volume integrals. 2. Vector and scalar forms of Divergence and Stokess theorems. Conservative fields: equivalence to curlfree and existence of scalar potential. Greens theorem in the plane. Calculus I and II covered integrals in one, two and three dimensional Euclidean (flat) space (i.e. R , R 2 and R 3 ). We are still working in R 3 so there is no generalization to be applied to volume or triple integrals, but one and two dimensional integration will be generalized from straight lines and planes to curves and surfaces. integraltext f ( x ) d x generalizes to integraltext C F . d r on a curve C , a line integral (section 3.1). integraltext integraltext f ( x , y ) d x d y generalizes to integraltext S F . d S over a surface S , a surface integral (section 3.2). We will then have to study the generalizations of integraldisplay b a d f d x dx = f ( b ) f ( a ) , (3.1) the fundamental theorem of calculus, which we use in the proofs. This theorem relates a onedimensional integral to a zerodimensional evaluation. The higher dimensional versions do the following. Stokess theorem 1 , relates the surface integral of a curl to a line integral (2 dimensions to 1): see section 3.5. The Divergence Theorem 2 relates the volume integral of a divergence to a surface integral (3 dimensions to 2): see section 3.3. There is also a special case of Stokess theorem where the surface is a plane: this is Greens theorem relating the integral of a curl to a line integral (2 dimensions to 1): see section 3.4. [Aside: All these are in fact special cases of the general Stokess theorem which relates an n 1 dimen sional integral of a field to the n dimensional integral of its derivative. Here the field is a generalization of a vector field called an ( n 1 )form field.] 1 A linguistic comment: For a name ending in s, it used to be customary to only add an apostrophe, e.g. Stokes. Modern use also adds an s e.g. Stokess. Books, and people, vary in which they prefer. 2 First discovered by Joseph Louis Lagrange in 1762, then independently rediscovered by Carl Friedrich Gauss in 1813, by George Green in 1825 and in 1831 by Mikhail Vasilievich Ostrogradsky, who also gave the first proof of the theorem. Thus the result may be called Gausss Theorem, Greens theorem, or Ostrogradskys theorem. 24 Finally we will discuss the application to potentials, and the proofs. Before all that, we consider the case where one wants to integrate a vector function F ( u ) of one variable, u , with respect to u . The integral can be calculated simply by integrating the components (in Cartesian coordinates) of F = ( f 1 , f 2 , f 3 ) : integraldisplay F d u = parenleftbigg integraldisplay f 1 d u , integraldisplay f 2 d u , integraldisplay f 3 d u parenrightbigg Integration of a vector in this case is just a set of three ordinary integrals. The restriction to Cartesian...
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This document was uploaded on 02/10/2010.
 Spring '09
 Magnetism

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