Page 571 - Engineering Electromagnetics, 8th Edition
P. 571

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                                                          APPENDIX










                     Vector Analysis





                     A.1 GENERAL CURVILINEAR COORDINATES

                     Let us consider a general orthogonal coordinate system in which a point is located
                     by the intersection of three mutually perpendicular surfaces (of unspecified form or
                     shape),
                                                 u = constant
                                                  ν = constant
                                                 w = constant
                     where u, ν, and w are the variables of the coordinate system. If each variable is
                     increased by a differential amount and three more mutually perpendicular surfaces
                     are drawn corresponding to these new values, a differential volume is formed which
                     approximates a rectangular parallelepiped. Because u, ν, and w need not be measures
                     of length, such as, the angle variables of the cylindrical and spherical coordinate
                     systems, each must be multiplied by a general function of u, ν, and w in order to
                     obtain the differential sides of the parallelepiped. Thus we define the scale factors h 1 ,
                     h 2 , and h 3 each as a function of the three variables u, ν, and w and write the lengths
                     of the sides of the differential volume as
                                                 dL 1 = h 1 du
                                                 dL 2 = h 2 dν
                                                 dL 3 = h 3 dw
                         In the three coordinate systems discussed in Chapter 1, it is apparent that the
                     variables and scale factors are
                                Rectangular:   u = x    ν = y     w = z
                                               h 1 = 1  h 2 = 1   h 3 = 1
                                Cylindrical:   u = ρ    ν = φ     w = z
                                               h 1 = 1  h 2 = ρ   h 3 = 1           (A.1)
                                Spherical:     u = r    ν = θ     w = φ
                                               h 1 = 1  h 2 = r   h 3 = r sin θ

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