Revision as of 17:34, 26 September 2008 by Apdelanc (Talk)

Defining an LTI System

For an input x(t), let the LTI system be defined as:

$ \ y(t)=0.5 x(t-5) u(t) $

Computing the Impulse Response and System Function

Inputting a delta into the system yields:

$ \ y(t)=h(t)=0.5 \delta(t-5) u(t) $

The System Function is defined by:

$ H(s)=\int_{-\infty}^{\infty} h(t)e^{-st}\,dt\, $

Now computing the actual response:

$ H(s)=\int_{-\infty}^{\infty} 0.5 \delta(t-5) u(t) e^{-st}\,dt\, $

which is turns into:


$ H(s)=\int_{0}^{\infty} 0.5 \delta(t-5) e^{-st}\,dt\, $

Now using the sifting property of the delta function we obtain:

$ \ H(s)= 0.5 e^{-5s} $

Remember$ \ s= jw $

Computing the Response of the Signal from Q1 using H(s)

When a periodic signal represented as a linear combination of complex exponential is inputted into a LTI system the output is

$ \ \Sigma a_{k} e^{jkwt} \longrightarrow sys \longrightarrow \Sigma H(jkw) a_{k} e^{jkwt} $

Therefore using this fact the system's output to the input of $ \ cos(2 \pi t/3) sin(2 \pi t/9) $ is

$ \ y(t)= $

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Abstract algebra continues the conceptual developments of linear algebra, on an even grander scale.

Dr. Paul Garrett