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parametric schaltungsanordnung with feldeffekt transistor

机译:带场效应晶体管的参量电路装置

摘要

1,043,900. Field effect transistor circuits; frequency modulation. RADIO CORPORATION OF AMERICA. Nov. 20, 1963 [Dec. 3, 1962], No. 45855/63. Headings H3R and H3T. An insulated - gate fieldeffect transistor comprises a biased gate electrode 61, Fig. 3, separated by a highresistance silicon dioxide layer from a lightly doped P- type silicon substrate 64 having source and drain electrodes 62, 63 forming with the substrate reversed biased rectifying junctions 72, 71 which act as variable capacitors when a variable control voltage across terminals 73, 74 is applied to the substrate electrode 64. With the stray capacitances between gate electrode 61 and source 62, and between source 62 and earth (67 being an R.F. choke), the transistor circuit forms a Colpitts oscillator with the frequency determined by inductor 69 and the capacitances. The oscillator may be frequency controlled by an A.F.C. voltage or frequency modulated by a signal voltage applied at 73, 74 over choke 75 to the capacitors 71, 72. When the signal voltage becomes positive, rectifier junction 72 forms a resistor, the net effect decreasing the oscillator frequency. Alternatively, a switching voltage forwardly biasing both rectifier junctions 71, 72 may key the oscillator on and off. Capacitor 76 which is optional also influences the circuit frequency characteristics, and an additional capacitor between the gate and source electrodes 61, 62 may be provided to reduce the increase in oscillation amplitude arising with positively increasing substrate voltage. In a modification, Fig. 6 (not shown), the source electrode 62 is positively biased by a resistor in series with the choke 67. Also a variable resistor or a signal source is connected between the positively biased drain and the substrate electrode 64 so that diode 72 is always forwardly biased and varies the effective value of capacitor 71. In Fig. 7 the transistor circuit is an R.F. or I.F. tuned amplifier with input applied over capacitor 92 and A.G.C. also applied to the gate electrode 91 to vary the current and therefore the voltage across a tapped resistor 100 in series with a tuned output circuit 99. The D.C. voltage at the resistor tapping 102 is applied to the substrate electrode to vary the transistor capacitance shunting the tuned circuit and lower its frequency response with increased A.G.C. voltage. This variation of the frequency response of circuit 99 with the A.G.C. voltage results in an essentially flat frequency response characteristic over a predetermined signal pass-band. This arrangement may be used as a television receiver inter-carrier I.F. amplifier to provide enhanced response to the video carrier when the carrier signal level is weak.
机译:1,043,900。场效应晶体管电路;调频。美国无线电公司。 1963年11月20日[十二月[1962年3月],第45855/63号。标题H3R和H3T。绝缘栅场效应晶体管包括图3的偏置栅电极61,该栅栅电极由高电阻二氧化硅层与轻掺杂的P型硅衬底64隔开,该P型硅衬底64的源极和漏极62、63形成有衬底反向偏置的整流结当在端子73、74之间的可变控制电压施加到衬底电极64上时,其用作可变电容器的72、71。栅极61和源极62之间以及源极62和地之间(67是RF扼流圈)之间的杂散电容),晶体管电路形成一个由电感器69和电容确定的频率的Colpitts振荡器。振荡器可以由A.F.C.通过在扼流圈75上施加到电容器71、72的73、74处的信号电压调制的电压或频率。当信号电压变为正时,整流器结72形成电阻器,净效应降低了振荡器频率。备选地,向前偏置两个整流器结71、72的开关电压可以使振荡器接通和断开。可选的电容器76也影响电路频率特性,并且可以在栅电极61和源电极62之间设置附加电容器以减小由正向增加的基板电压引起的振荡幅度的增加。在图6的变型中(未示出),源电极62由与扼流圈67串联的电阻器正偏置。可变电阻器或信号源也连接在正偏置的漏极和衬底电极64之间,从而二极管72总是正向偏置并改变电容器71的有效值。在图7中,晶体管电路为RF或者如果。输入端经过电容器92和A.G.C.也将其施加到栅电极91以改变电流,并因此改变与调谐输出电路99串联的抽头电阻器100两端的电压。电阻器抽头102处的DC电压被施加到衬底电极以改变晶体管的电容分流。通过增加AGC调整电路并降低其频率响应电压。电路99的频率响应随A.G.C变化。电压导致在预定信号通带上的频率响应特性基本平坦。该布置可用作电视接收机载波间IF。当载波信号电平较弱时,放大器可增强对视频载波的响应。

著录项

  • 公开/公告号DE000001441834A

    专利类型

  • 公开/公告日1969-05-22

    原文格式PDF

  • 申请/专利权人 RCA CORP;

    申请/专利号DE1441834A

  • 发明设计人 JOHN CARLSON DAVID;

    申请日1963-12-03

  • 分类号H03C3/16;

  • 国家 DE

  • 入库时间 2022-08-23 12:21:22

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