Solution 1
(a) Let the signal at the bottom node of the block
diagram be denoted by e ( t ). Then we
have the following relations
![](Solution_Template1_files/Solution_Template_clip_image002.gif)
![](Solution_Template1_files/Solution_Template_clip_image004.gif)
Writing the above equations in Laplace domain, we
have
![](Solution_Template1_files/Solution_Template_clip_image006.gif)
![](Solution_Template1_files/Solution_Template_clip_image008.gif)
Eliminating the auxiliary signal e ( t
), we get
![](Solution_Template1_files/Solution_Template_clip_image010.gif)
![](Solution_Template1_files/Solution_Template_clip_image012.gif)
Hence we get the following differential equation,
![](Solution_Template1_files/Solution_Template_clip_image014.gif) ![](Solution_Template1_files/Top.gif)
(b) From the system function H ( s
) found in the previous part we see that the poles
of the system are at s = -1. Since the system
is given to be causal, and the right most pole of the
system is left of the imaginary axis, the system is
stable. ![](Solution_Template1_files/Top.gif)
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