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phasenstarre waveguide oscillators

机译:相星光波导振荡器

摘要

1,242,228. Oscillators. WESTERN ELECTRIC CO. Inc. 26 July, 1968 [27 July, 1967], No. 35713/68. Heading H3T. An oscillator has a negative resistance active element (a tunnel diode 11) disposed in energy transferring relationship to a waveguide 10, a shunt inductive element 12 being arranged close to the diode 11 to suppress oscillations below the cut-off frequency of the wavepath, thereby ensuring that oscillation at a frequency not less than the cut-off frequency is produced at the output. The spacing 11-12 is preferably a quarter of a wavelength and transverse to the direction of propagation. The waveguide 10 is tapered to match its impedance to that of the diode, to which a phase-locking input is connected by an isolator 15. The inductive element 12 is adjustable in position by a portion 13 thereof which extends through a slit 14 in the wall of the waveguide. In a second embodiment (Fig. 3, not shown) the tunnel diode (31) is arranged in an inductive iris formed by two elements (32), the frequency being adjusted by a piston (37). The microwave power is supplied by way of a circulator (38). The tunnel diode in both embodiments could be replaced by a Gunn effect or L.S.A. device. The effect of the inductive element 12(32) is explained in terms of the frequency dependent capacitive impedance curve of the diode (1, Fig. 2A, not shown) which is crossed, in the absence of the element 12, by the circuit inductive impedance curves at two points (A,B) respectively above and blow the cut-off frequency, oscillation tending to occur at the lower frequency (A). In the presence of the inductive element 12 the circuit inductive impedance curves are modified (Fig. 2B, not shown) so that a cross-over occurs only at a frequency above the cut-off frequency; and oscillation therefore occurs at this frequency (C).
机译:1,242,228。振荡器。 WESTERN ELECTRIC CO。Inc.,1968年7月26日[1967年7月27日],编号35713/68。标题H3T。振荡器具有与波导10能量传递关系地设置的负电阻有源元件(隧道二极管11),分流电感元件12被布置为靠近二极管11以抑制在波路径的截止频率以下的振荡,从而确保在输出端产生不小于截止频率的振荡。间隔11-12优选地是波长的四分之一并且垂直于传播方向。波导10是锥形的,以使其阻抗与二极管的阻抗相匹配,通过隔离器15将锁相输入连接到该二极管。电感元件12的一部分可以通过其位置13进行调整,该部分13延伸穿过波导10中的狭缝14。波导壁。在第二实施例中(图3,未示出),隧道二极管(31)布置在由两个元件(32)形成的感应虹膜中,该频率由活塞(37)调节。微波功率通过循环器(38)供应。在两个实施例中的隧道二极管都可以用耿氏效应或L.S.A代替。设备。电感元件12(32)的作用是根据二极管(1,图2A,未示出)的频率相关的电容性阻抗曲线来解释的,该二极管在没有元件12的情况下与电路电感相交。阻抗曲线分别出现在截止频率以上的两个点(A,B)并吹响截止频率,在较低的频率(A)上容易发生振荡。在存在电感元件12的情况下,电路的电感阻抗曲线被修改(图2B,未示出),使得仅在高于截止频率的频率处发生交越;因此,仅在截止频率以上才发生交越。因此在该频率(C)发生振荡。

著录项

  • 公开/公告号DE000001766811A

    专利类型

  • 公开/公告日1972-03-30

    原文格式PDF

  • 申请/专利权人 WESTERN ELECTRIC CO;

    申请/专利号DE1766811A

  • 发明设计人 EMANUEL GOELL JAMES;LEE CLOUSER PAUL;

    申请日1968-07-23

  • 分类号H03B7/14;

  • 国家 DE

  • 入库时间 2022-08-23 08:31:36

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