These are also called transmission parameters. Here, voltage and current and of input part are expressed in term of output part. Here,
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Thus, the cause and effect relationship between the output and input is related to each other through a transfer function. In a Laplace Transform, if the input is represented by R(s) and the output is represented by C(s), then the transfer function will be:
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Now we apply the sifting property of the impulse. Since the impulse is 0 everywhere but t=0, we can change the upper limit of the integral to 0+. Since e-st is continuous at t=0, that is the same as saying it is constant from t=0- to t=0+. So, we can replace e-st by its value evaluated at t=0.
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Integration by parts is useful at this point |
A typical example of an infinite duration signal is: A finite duration counterpart of the above signal could be The value of a finite (or infinite) duration signal may or may not be finite. For example |
The convolution theorem for Laplace transform states that
The standard proof uses Fubini-like argument of switching the order of integration The convolution theorem can be used to solve integral and integral–differential equations. Let us assume the mathematical model of a system consists of the following integral equation where the functions f and u are known time-dependent functions and y(t) is the unknown function. Application of the Laplace transform which is The inverse Laplace transform of Y(s) is
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Now with the help of the above general network function, we can describe the necessary conditions for the stability of all the network functions. There are three mains necessary conditions for the stability of these network functions, and they are written below:
Where, Q(s) is a Hurwitz polynomial.There are five important properties of Hurwitz polynomials and they are written below: