1977
DOI: 10.1109/tap.1977.1141698
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Coupled Yagi arrays

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Cited by 3 publications
(2 citation statements)
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“…Suppose the antenna will be designed on dielectric substrate with relative permittivity of ε r = 2.65 at the center frequency of 2.4 GHz. The radius and flared angle of the principal sectorial dipole can be calculated by (2) [40], where ε e is relative dielectric constant that can be estimated by empirical expressions indicated in [41], ν is the circumferential eigen-number determined by the flared angle α, and χ ν1 is the first root of the first-order derivative of the ν-order Bessel function of the first kind, respectively [39,40]. When the flared angle is set as β = 270° [39], the radius can be initially calculated as R 0 = 26.5 mm [42].…”
Section: A Equivalent Six-source Modelmentioning
confidence: 99%
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“…Suppose the antenna will be designed on dielectric substrate with relative permittivity of ε r = 2.65 at the center frequency of 2.4 GHz. The radius and flared angle of the principal sectorial dipole can be calculated by (2) [40], where ε e is relative dielectric constant that can be estimated by empirical expressions indicated in [41], ν is the circumferential eigen-number determined by the flared angle α, and χ ν1 is the first root of the first-order derivative of the ν-order Bessel function of the first kind, respectively [39,40]. When the flared angle is set as β = 270° [39], the radius can be initially calculated as R 0 = 26.5 mm [42].…”
Section: A Equivalent Six-source Modelmentioning
confidence: 99%
“…Yagi-Uda antennas enjoy many advantages over conventional elementary antennas, such as high gain/directivity, easy to set up, and low cost. Since invented in 1926 [1], variants of Yagi-Uda antennas have been extensively developed and presented [2][3][4]. Up to now, Yagi-Uda antennas can be basically classified into four distinctive types.…”
Section: Introductionmentioning
confidence: 99%