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6.38. A coaxial line of inner and outer radii a and b, respectively, is mounted on an infinite conducting ground plane. Assuming that the electric field over the aperture of the coax is Ea = -ấp a

6.38. A coaxial line of inner and outer radii a and b, respectively, is mounted on an infinite conducting ground plane. Assuming that the electric field over the aperture of the coax is Ea = -ấp a

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6.38. A coaxial line of inner and outer radii a and b, respectively, is mounted on an infinite conducting ground plane. Assuming that the electric field over the aperture of the coax is Ea = -ấp a <p' sb e In(b/a) p where V is the applied voltage and & is the permittivity of medium in the coax, find the far-zone spherical electric and magnetic field components radiated by the aperture. Use equivalent currents M, and J, such that ZA -2n x Ea, a < p' <b M, = elsewhere b. J, = 0 everywhere y х
Transcribed Image Text:6.38. A coaxial line of inner and outer radii a and b, respectively, is mounted on an infinite conducting ground plane. Assuming that the electric field over the aperture of the coax is Ea = -ấp a <p' sb e In(b/a) p where V is the applied voltage and & is the permittivity of medium in the coax, find the far-zone spherical electric and magnetic field components radiated by the aperture. Use equivalent currents M, and J, such that ZA -2n x Ea, a < p' <b M, = elsewhere b. J, = 0 everywhere y х
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