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Frequency Response

Let a network be described by a transfer function H(s). Let us denote the input signal as r(t) and the output signal as y(t). I am interested in finding the output y(t) when the input is a sinusoidal function, i.e., tex2html_wrap_inline234.

The Laplace transform of the input is:
displaymath210
and hence the output can be written as:
displaymath211
Let
 equation23

 equation36

Let
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This implies:
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Then:
eqnarray55
Noting that
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we can write:
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In the above we haven't paid any attention to the third part of the expression on the left hand side of the equation (1). Let us look at that expression now.
displaymath208
Note that both tex2html_wrap_inline346 and tex2html_wrap_inline348 can be either real or complex. When tex2html_wrap_inline348 is real then tex2html_wrap_inline346 is also real. For complex tex2html_wrap_inline348 there will be another tex2html_wrap_inline356 and in general we can write:
displaymath209
It is easy to see that when (Real part of tex2html_wrap_inline352) tex2html_wrap_inline360 then tex2html_wrap_inline362.

For all passive RLC networks tex2html_wrap_inline364 is always less than 0. The condition tex2html_wrap_inline360 also means that all the roots of the denominator of the transfer function H(s) are in the left half of the complex plane. Roots of the denominator of the transfer function are also known as the system poles; zeros are the roots of the transfer function numerator.

In other words for any system with the poles in the left half complex plane the steady-state response to a sinusoid of frequency tex2html_wrap_inline370\ can be worked out by evaluating the magnitude and the phase of the complex number tex2html_wrap_inline372 and then noting that the magnitude of the output is given by the magnitude of the input sinusoid times the magnitude of tex2html_wrap_inline372 and the phase shift between the input sinusoid and the output is given by the phase of tex2html_wrap_inline372.




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Himanshu Pota
Thu Aug 27 11:17:58 EST 1998