The original paper is in English. Non-English content has been machine-translated and may contain typographical errors or mistranslations. ex. Some numerals are expressed as "XNUMX".
Copyrights notice
The original paper is in English. Non-English content has been machine-translated and may contain typographical errors or mistranslations. Copyrights notice
리액턴스 부하 빔 틸팅 다이폴 안테나의 적용은 많은 연구자들에 의해 보고되었습니다. 현재까지 보고된 애플리케이션에 탑재된 리액턴스 요소는 빔 틸팅 목적으로만 사용되었습니다. 본 논문에서는 급전점에서의 임피던스 정합을 위해 하나의 리액턴스 소자를 사용하는 빔 틸팅 다이폴 안테나 소자의 기본 특성을 제시한다. 적절하게 결정된 구동점 위치에 따라 방사 패턴이 기울어지며, 로딩 리액턴스를 사용하여 기울임 각도의 큰 변화 없이 강제 공진을 얻습니다. 수치 결과는 빔 경사각의 변화가 거의 없이 안테나의 강제 공진을 얻기 위해서는 구동점이 위치한 영역에 리액턴스 요소를 탑재해야 함을 보여줍니다. 제안된 0.8λ 길이의 강제 공진 빔 틸팅 안테나를 중심으로부터 0.2λ에서 구동할 경우, 메인 빔 틸트 각도는 57.7도, 가장 높은 전력 이득은 8.6dB, VSWR=2.2를 얻는다.
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부
Ki-Chai KIM, Ick Seung KWON, "Beam Tilting Dipole Antenna Elements with Forced Resonance by Reactance Loading" in IEICE TRANSACTIONS on Communications,
vol. E83-B, no. 1, pp. 77-83, January 2000, doi: .
Abstract: The applications of reactance-loaded beam tilting dipole antennas have been reported by many researchers. The reactance elements loaded on the applications reported up to date have been used only for the purpose of beam tilting. This paper presents the basic characteristics of the beam tilting dipole antenna element in which one reactance element is used for the impedance matching at the feed point. The radiation pattern is tilted by the properly determined driving point position, and the loading reactance is used to obtain forced resonance without great changes in tilt angle. The numerical results demonstrate that the reactance element should be loaded in the region where the driving point is placed to obtain forced resonance of the antenna with little changes in beam tilt angle. In case the proposed forced resonant beam tilting antenna with 0.8λ length is driven at 0.2λ from the center, the main beam tilt angle of 57.7 degrees, the highest power gain of 8.6 dB, and VSWR=2.2 are obtained.
URL: https://global.ieice.org/en_transactions/communications/10.1587/e83-b_1_77/_p
부
@ARTICLE{e83-b_1_77,
author={Ki-Chai KIM, Ick Seung KWON, },
journal={IEICE TRANSACTIONS on Communications},
title={Beam Tilting Dipole Antenna Elements with Forced Resonance by Reactance Loading},
year={2000},
volume={E83-B},
number={1},
pages={77-83},
abstract={The applications of reactance-loaded beam tilting dipole antennas have been reported by many researchers. The reactance elements loaded on the applications reported up to date have been used only for the purpose of beam tilting. This paper presents the basic characteristics of the beam tilting dipole antenna element in which one reactance element is used for the impedance matching at the feed point. The radiation pattern is tilted by the properly determined driving point position, and the loading reactance is used to obtain forced resonance without great changes in tilt angle. The numerical results demonstrate that the reactance element should be loaded in the region where the driving point is placed to obtain forced resonance of the antenna with little changes in beam tilt angle. In case the proposed forced resonant beam tilting antenna with 0.8λ length is driven at 0.2λ from the center, the main beam tilt angle of 57.7 degrees, the highest power gain of 8.6 dB, and VSWR=2.2 are obtained.},
keywords={},
doi={},
ISSN={},
month={January},}
부
TY - JOUR
TI - Beam Tilting Dipole Antenna Elements with Forced Resonance by Reactance Loading
T2 - IEICE TRANSACTIONS on Communications
SP - 77
EP - 83
AU - Ki-Chai KIM
AU - Ick Seung KWON
PY - 2000
DO -
JO - IEICE TRANSACTIONS on Communications
SN -
VL - E83-B
IS - 1
JA - IEICE TRANSACTIONS on Communications
Y1 - January 2000
AB - The applications of reactance-loaded beam tilting dipole antennas have been reported by many researchers. The reactance elements loaded on the applications reported up to date have been used only for the purpose of beam tilting. This paper presents the basic characteristics of the beam tilting dipole antenna element in which one reactance element is used for the impedance matching at the feed point. The radiation pattern is tilted by the properly determined driving point position, and the loading reactance is used to obtain forced resonance without great changes in tilt angle. The numerical results demonstrate that the reactance element should be loaded in the region where the driving point is placed to obtain forced resonance of the antenna with little changes in beam tilt angle. In case the proposed forced resonant beam tilting antenna with 0.8λ length is driven at 0.2λ from the center, the main beam tilt angle of 57.7 degrees, the highest power gain of 8.6 dB, and VSWR=2.2 are obtained.
ER -