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宽带讯号传输系统的模型可以归结为如下形式:讯号源经由内阻R
0
通过介入电路驱动电容(惯性量)C
0
。电压增益函数记为F
12
。应用能量守恒律
并引用对偶互易定理及Parseval定理
作者得到功率增益的频率域积分(定理): integral from -∞ to ∞ (|F
12
(jω)|
2
dω/2π)=1/R
0
[1/2C
0
-W(∞)-sum from i (R
i
) integral from 0 to ∞ (i
i
2
(t)dt)]其中W(∞)为这一系统在C
0
二端受单元脉冲电流冲击后在t=∞时的贮能
R
i
为介入电路中第i个电阻阻值(其中流动的单元脉冲响应电流为i
i
(t)))。文章指出integral from -∞ to ∞ (|F
2
(jω)|
2
dω/2π代表着系统的频域和时域传输品质。 如果介入电路为抗性电路
且满足一定条件使W(∞)得为0
则积分取极大值1/2C
0
R
0
。由此可见在一定条件下系统的传输品质是守恒的
它不随介入电路的结构形式(在前述条件下)及元件参量而改变。因而
如果使F
12
的通带集中在一定窄的区域
可以取得无源增益。 由于沿袭有线通讯系统的习惯
往往讯号传输系统被终端于一定电阻。根据所得的定理
对于宽带系统
应该使终端免于阻性负载
才能使品质最良好。
Let a sluggish load of capacity Co be driven by a source of internal resistance Ro via an intermediate two-terminal pair. And let F12 denote the voltoge transmission fun-ction. The integral is indicated to have an interpretation as anindex of grade of performance of the transmission system matter not in frequency domain or in time domain senses. The author obtained through time domain artifice the power gain integral theorem formulated thus:Where W(∞) stands for the total stored energy in the complete system at t=∞ after being kicked across Co by a unit impulse current introduced at t = 0
and Ri for the ith resistance in the inserted network with impulse response current ii (t) flowing in it.The integral will assume its maximum value when the intermediate network is all reactive and satisfying certain guite weak limitations such that W(∞) = 0. Hence it is concluded that transmission models under said limitations will behave with performance of transmission invariant of circuit structure and parameters of the intermediate network. It is also concluded that confining the pass band of F12 in narrow interval may result in greater than unity gain with the system being inert.The paper also points out that the usual desposition of loading transmission circuit in resistive termination for"matching" considerations should receive a con when the circuit is to work for wide band purposes; for example
delay lines never should be loaded with resistance(as the situation may tolerate) aside from unavoidable stray capacitance.
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