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    • 5. 发明授权
    • Broadband ferrite transformer-fed whip antenna
    • 宽带铁氧体变压器鞭状天线
    • US4028704A
    • 1977-06-07
    • US605338
    • 1975-08-18
    • Judd Blass
    • Judd Blass
    • H01Q9/16H01Q9/30H01Q1/32
    • H01Q9/30H01Q9/16
    • The feed point of a whip antenna having a length less than one quarter-wavelength at the lowest frequency of operation is raised above a counterpoise ground plane by a short base sleeve. Gain over a 2.5:1 bandwidth of radio frequencies closely approaches the gain of a standard quarter-wavelength antenna without requiring use of power-dissipating resistance loading. A ferrite transformer at the whip antenna feedpoint is utilized to reduce the high anti-resonance impedance of the broadband whip antenna to the characteristic impedance of a coaxial cable transmission system and to minimize the VSWR thereof. The base sleeve raises the antenna resistance at the resonant frequency near the lower end of the bandwidth to make the transformer effective as an impedance matching element over the entire radio frequency band.A pair of the whip antennas are axially aligned and electrically coupled in series to realize a broadband dipole having increased gain. A pair of dipoles are energized in phased relationship to realize even higher gain and directivity.
    • 在最低工作频率下具有小于四分之一波长的长度的鞭状天线的馈电点通过短的基座套筒升高到平衡地平面之上。 无线电频率2.5:1带宽的增益接近标准四分之一波长天线的增益,而不需要使用功率耗散电阻负载。 利用鞭状天线馈电点处的铁氧体变压器将宽带鞭状天线的高抗共振阻抗降低到同轴电缆传输系统的特性阻抗,并使其VSWR最小化。 基座套管以接近带宽下端的共振频率提高天线电阻,使变压器在整个无线电频段成为阻抗匹配元件。
    • 6. 发明授权
    • Broadband whip antennas
    • 宽带天线
    • US3950757A
    • 1976-04-13
    • US557836
    • 1975-03-12
    • Judd Blass
    • Judd Blass
    • H01Q1/32H01Q9/30
    • H01Q9/30H01Q1/32
    • A whip antenna with a substantially constant impedance over a broad band of radio frequencies includes a mounting section, a high-power-dissipation low-resistance assembly, a first whip section, a second whip section, and a high-impedance quarter-wavelength transformer section concentrically formed around the first whip section and extending from the resistance assembly to the junction of the first and second whip sections. The low-resistance termination is attached close to the base of the antenna and is transformed to a high resistance at the junction of the first and second whip sections at the frequency where the matching section length equals one quarter-wavelength. The resistive power loss only occurs over a limited band centered at the design frequency of the matching section. Instability caused by emplacement of a high-mass resistive termination towards the top of the complete antenna is thus avoided.