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Variable permittivity dielectric material loaded stepped-horn antenna

Variable permittivity dielectric material loaded stepped-horn antenna

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CHAPTER 4NUMERICAL RESULTSIn Chapter 2, the hybrid numerical technique is presented to analyze <strong>stepped</strong>-<strong>horn</strong> <strong>antenna</strong><strong>loaded</strong> with variable <strong>permittivity</strong> <strong>dielectric</strong> <strong>material</strong>. In this model, mode matching techniqueis used in step approximated tapered section of the <strong>horn</strong> modeled with NI uniform rectangularwaveguide sections. Hence, it is very important to choose the size of each waveguidesection, A/ = L/NI properly so that the pyramidal tapered section is accurately modeled.Choice of 30 steps per wavelength has been found to work well in numerical evaluations.As a first example, empty pyramidal <strong>horn</strong> <strong>antenna</strong> with input waveguide section sizeal = 0.675A, b1 = 0.3A and aperture size aA = 1.25A, bA = 0.5A, length of the taperedsection, L = 2.5A is considered. It is assumed that TE10 mode in an incident wave at theinput of the feed waveguide has a power density of 1 Watt/m² . Table 4.1 shows amplitudeand phase of reflection and transmission coefficient of TE10 mode and the total powerPtot, Ptot = Prad Pref where Pradand Pre f are radiated and reflected power densities,respectively. Total number of modes used in this example were 3. As it seen from Table4.1, A/30 waveguide section size is enough for convergence to until fifth significant digit.Notice that power conservation check is also satisfied for every waveguide section size.Same study is repeated for <strong>dielectric</strong> <strong>loaded</strong> <strong>horn</strong> <strong>antenna</strong> and the similiar results wereobtained as seen in Table 4.2. Notice that the wavelength, A inside the <strong>dielectric</strong> mediumis smaller than the wavelength of the empty <strong>horn</strong>, the number of waveguide section, NIshould be bigger compared to the empty one. As it was expected, power conservation is alsosatisfied for <strong>dielectric</strong> <strong>loaded</strong> <strong>horn</strong> <strong>antenna</strong>. However, there is a small difference comparedto the the empty <strong>horn</strong> <strong>antenna</strong>, decrease in the wavelengths necessitated to include higherorder modes which were excited at the aperture. Hence, the chosen total mode number41

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