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The Wave Equations
HI PROPAGATION IN WAVEGUIDES
6 other sections not shown
bottom region boundary conditions branch cut due branch cut integral branch points contour cg cut becomes cylindrical waveguides denoted dielectric due to kx electric line source erfc(x evaluated field components following relation Fourier integral gamma function given in 102b half-space ikor ikor-i4 intercepted iokx Jm(kcr Kokx kyky leading term line source located Lorentz transformation Magnetic Line Source Maxwell's equations method of integration moving media Parallel to Y-Axis path of integration phase velocity point 9 pole potential functions Poynting vector radiated field rectangular waveguide residue of P(4 Riemann surface saddle point method satisfy semi-infinite shown in Fig side of point solution stationary medium steepest descent contour steepest descent path Taylor series TM modes transverse wave number vector potential wave equations wave impedance z-axis