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[...]... the coordinate axes) to yield Ax = A cos α, etc., as in Eq (1.4) We may choose to refer to the vector as a single quantity A or to its components (Ax , Ay , Az ) Note that the subscript x in Ax denotes the x component and not a dependence on the variable x The choice between using A or its components (Ax , Ay , Az ) is essentially a choice between a geometric and an algebraic representation Use either... equivalent Then the physical system being analyzed or the physical law being enunciated cannot and must not depend on our choice or orientation of the coordinate axes Specifically, if a quantity S does not depend on the orientation of the coordinate axes, it is called a scalar 3 This section is optional here It will be essential for Chapter 2 8 Chapter 1 Vector Analysis FIGURE 1.6 Rotation of Cartesian coordinate... xk as coordinate lines (j = k) are assumed to be perpendicular (two or three dimensions) or orthogonal (for any number of dimensions) Equivalently, we may assume that xj and xk (j = k) are totally independent variables If j = k, the partial derivative is clearly equal to 1 In redefining a vector in terms of how its components transform under a rotation of the coordinate system, we should emphasize two... any point in our Cartesian reference frame; we choose the origin for simplicity This freedom of shifting the origin of the coordinate system without affecting the geometry is called translation invariance 4 Chapter 1 Vector Analysis FIGURE 1.5 Cartesian components and direction cosines of A (x, y, z), is denoted by the special symbol r We then have a choice of referring to the displacement as either... of physics and related fields This approach incorporates theorems that are usually not cited under the most general assumptions, but are tailored to the more restricted applications required by physics For example, Stokes’ theorem is usually applied by a physicist to a surface with the tacit understanding that it be simply connected Such assumptions have been made more explicit PROBLEM-SOLVING SKILLS... linear combination of x, y, and z Since x, y, and z are linearly independent (no one is a linear combination of the other two), they form a basis for the real three-dimensional Euclidean space Finally, by the Pythagorean theorem, the magnitude of vector A is |A| = A2 + A2 + A2 x y z 1/2 (1.6) Note that the coordinate unit vectors are not the only complete set, or basis This resolution of a vector into... (relative to the water) on a steady compass heading of 40◦ east of north The sailboat is simultaneously carried along by a current At the end of the hour the boat is 6.12 km from its starting point The line from its starting point to its location lies 60◦ east of north Find the x (easterly) and y (northerly) components of the water’s velocity ANS veast = 2.73 km/hr, vnorth ≈ 0 km/hr 1.1.6 A vector equation... with us at the origin Show that this recession of the galaxies from us does not imply that we are at the center of the universe Specifically, take the galaxy at r1 as a new origin and show that Hubble’s law is still obeyed 1.1.12 1.2 Find the diagonal vectors of a unit cube with one corner at the origin and its three sides lying along Cartesian coordinates axes Show that there are four diagonals with length... AXES3 In the preceding section vectors were defined or represented in two equivalent ways: (1) geometrically by specifying magnitude and direction, as with an arrow, and (2) algebraically by specifying the components relative to Cartesian coordinate axes The second definition is adequate for the vector analysis of this chapter In this section two more refined, sophisticated, and powerful definitions are presented... and special functions (Chapters 11–13) more extensively, and add Fourier series (Chapter 14), integral transforms (Chapter 15), integral equations (Chapter 16), and the calculus of variations (Chapter 17) CHANGES TO THE SIXTH EDITION Improvements to the Sixth Edition have been made in nearly all chapters adding examples and problems and more derivations of results Numerous left-over typos caused by . Edition. CHAPTER 1 VECTOR ANALYSIS 1.1 DEFINITIONS,ELEMENTARY APPROACH In science and engineering we frequently encounter quantities that have magnitude and magnitude only: mass, time, and temperature the x component and not a dependence on the variable x. The choice between using A or its components (A x ,A y ,A z ) is essentially a choice between a geometric and an algebraic representation Transform of Derivatives 946 15.5 Convolution Theorem 951 15.6 Momentum Representation 955 15.7 Transfer Functions 961 15.8 Laplace Transforms 965 Contents ix 15.9 Laplace Transform of Derivatives 971 15.10

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