RF/Microwave Engineering and Applications in Energy Systems. Abdullah Eroglu

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      1.2.5 Surface Integral

      (1.46)integral Underscript upper S Endscripts ModifyingAbove upper F With right-arrow dot ModifyingAbove a With ampersand c period circ semicolon Subscript n Baseline italic d s equals integral StartAbsoluteValue ModifyingAbove upper F With right-arrow EndAbsoluteValue cosine left-parenthesis theta right-parenthesis italic d s

      The normal vector ModifyingAbove a With ampersand c period circ semicolon Subscript n is normal on S at any point. The outward flux of the vector ModifyingAbove upper F With right-arrow shown for a closed surface is then defined by

      (1.47)psi equals contour-integral Underscript upper S Endscripts ModifyingAbove upper F With right-arrow dot d ModifyingAbove s With right-arrow

      1.2.6 Volume Integral

      The volume integral for scalar quantities such as charge densities over the given volume is defined as

      In this section, vector differential operators del, gradient, and curl are discussed. In addition, divergence and Stokes' theorem are presented.

      1.3.1 Del Operator

      The del operator, ∇, is used as a differential operator and can be used to find the gradient of a scalar, divergence of a vector, curl of a vector, or Laplacian of a scalar in electromagnetics. These operations can be expressed as

       ∇F for finding the gradient of a scalar

        for finding the divergence of a vector

        for finding the curl of a vector

       ∇2F for finding the Laplacian of a scalar

      The del operator, in three different coordinate systems, can be written in the following forms

      (1.49)Cartesian coordinate right-arrow nabla equals StartFraction partial-differential Over partial-differential x EndFraction ModifyingAbove x With ampersand c period circ semicolon plus StartFraction partial-differential Over partial-differential y EndFraction ModifyingAbove y With ampersand c period circ semicolon plus StartFraction partial-differential Over partial-differential z EndFraction ModifyingAbove z With ampersand c period circ semicolon

      (1.50)Cylindrical coordinate right-arrow nabla equals StartFraction partial-differential Over partial-differential r EndFraction ModifyingAbove r With ampersand c period circ semicolon plus StartFraction 1 Over r EndFraction StartFraction partial-differential Over partial-differential phi EndFraction ModifyingAbove phi With ampersand c period circ semicolon plus StartFraction partial-differential Over partial-differential z EndFraction ModifyingAbove z With ampersand c period circ semicolon

      (1.51)Spherical coordinate right-arrow nabla equals StartFraction partial-differential Over partial-differential upper R EndFraction ModifyingAbove upper R With ampersand c period circ semicolon plus StartFraction 1 Over upper R EndFraction StartFraction partial-differential Over partial-differential theta EndFraction ModifyingAbove theta With ampersand c period circ semicolon plus StartFraction 1 Over upper R sine theta EndFraction StartFraction partial-differential Over partial-differential phi EndFraction ModifyingAbove phi With ampersand c period circ semicolon

      1.3.2 Gradient

      The gradient is used to identify the maximum change in direction and magnitude for a scalar field. Consider a scalar field ϕ(x, y, z). The gradient of ϕ(x, y, z) is defined as

      (1.52)grad phi equals ModifyingAbove nabla With bar phi equals ModifyingAbove x With ampersand c period circ semicolon StartFraction partial-differential phi Over partial-differential x EndFraction plus ModifyingAbove y With ampersand c period circ semicolon StartFraction partial-differential phi Over partial-differential y EndFraction plus ModifyingAbove z With ampersand c period circ semicolon StartFraction partial-differential phi Over partial-differential z EndFraction

      The change in ϕ from ModifyingAbove r With right harpoon with barb up to ModifyingAbove r With right harpoon with barb up plus d ModifyingAbove r With right harpoon with barb up can be found from

      (1.53)ModifyingAbove nabla With bar phi dot d r overbar equals left-parenthesis ModifyingAbove x With ampersand c period circ semicolon StartFraction partial-differential phi Over partial-differential x EndFraction plus ModifyingAbove y With ampersand c period circ semicolon StartFraction partial-differential phi Over partial-differential y EndFraction plus ModifyingAbove z With ampersand c period circ semicolon StartFraction partial-differential phi Over partial-differential z EndFraction right-parenthesis dot left-parenthesis ModifyingAbove x With ampersand c period circ semicolon italic d x plus ModifyingAbove y With ampersand c period circ semicolon italic d y plus ModifyingAbove z With ampersand c period circ semicolon italic d z right-parenthesis

      (1.54)equals StartFraction partial-differential phi Over partial-differential x EndFraction italic d x plus StartFraction partial-differential phi Over partial-differential y EndFraction italic d y plus StartFraction partial-differential phi Over partial-differential z EndFraction italic d z equals italic d phi

      If we assume r overbar equals ModifyingAbove r With bar left-parenthesis s right-parenthesis and s is the arc along a curve, then

      (1.55)

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