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Tunnel diode oscillator with series RLC

时间:04-06 整理:3721RD 点击:
It is said that negative resistance devices must use a series LC oscillator while a negative conductance device, e.g. a tunnel diode, must use a parallel LC oscillator. However, focusing on negative conductance device, the conductance vs voltage (across the tunnel diode) may be modeled as a (U) parabola as shown below. The minimum is the negative conductance of the device (at optimally biased). With a parallel LC oscillator (and the tunnel diode optimally biased), the oscillation amplitude will increase until the negative conductance decreases (i.e. more positive) and balanced by the positive conductance in the (lossy) oscillator.

闂傚倸鍊搁崐椋庣矆娓氣偓楠炲鍨鹃幇浣圭稁缂傚倷鐒﹁摫闁告瑥绻橀弻鐔碱敍閿濆洣姹楅悷婊呭鐢帡鎮欐繝鍥ㄧ厪濠电倯鈧崑鎾绘煛鐎n偆澧垫慨濠呮閹瑰嫰濡搁妷锔惧綒闂備胶鎳撻崵鏍箯閿燂拷...



Inverting the conductance gives the resistivity and is shown below.

闂傚倸鍊搁崐椋庣矆娓氣偓楠炲鍨鹃幇浣圭稁缂傚倷鐒﹁摫闁告瑥绻橀弻鐔碱敍閿濆洣姹楅悷婊呭鐢帡鎮欐繝鍥ㄧ厪濠电倯鈧崑鎾绘煛鐎n偆澧垫慨濠呮閹瑰嫰濡搁妷锔惧綒闂備胶鎳撻崵鏍箯閿燂拷...



Now, with a series RLC oscillator, where R is smaller than the magnitude of the negative resistance (so oscillation should be able to start) and the tunnel diode is assumed biased (as in the parallel case above), will there be any oscillation with such a series RLC? If there is any response to the RLC at all, what will be observed? (The negative resistance will increase with amplitude if oscillation is possible and the amplitude would diverge.)

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