laplace transformation
\[Y(t)= \frac{ e^{-\pi s} }{ (s+1)^2+1 }\]
Take the inverse
First, the left side should be Y(s).
So, this is a form of \[L \left\{ f(t) \right\} = e^{-as}F(s)\] Which would mean your f(t) has the form \[U(t-a)f(t-a)\] In this case, "a" is just pi. As for your F(s) portion, it comes from an f(t) of the form\[e^{at}\sin(kt)\] So looking at the F(s) portion\[\frac{ 1 }{ (s+1)^{2} + 1 }\] we see a is -1 and k is 1, meaning F(s) is\[e^{-t}sin(t)\]Therefore our inverse transform gives us \[Y(t) =U(t-\pi )[e^{-(t- \pi )}\sin(t-\pi )]\]
I got it, but I though the answer is \[e^{-t} \sin(t) [u(t-\pi)]\]
how did you get e^-(t-pi) sin(t-pi)
It's just the form of that kind of inverse transform. I didn't really get it from anywhere other than saying that since our laplace transform is \[e^{-as}F(s)\] where F(s) is the transform of \[f(t) = e^{at}\sin(kt)\]Taking the inverse transform of \[e^{-as}F(s) \] gives \[U(t-a)f(t-a)\] So that required be to do the t-pi substitution into \[f(t) = e^{at}\sin(kt)\] also, not just the U part.
My only question is how you got U(t-a) f(t-a)
is it because it is transformed?
Right. If I were to separate original functions f(t) and their transforms L{f(t)}, for this problem we have our f(t)'s equal to: \[U(t-a)f(t-a)\] \[e^{at}\sin(kt)\] These are functions prior to taking their laplace transform. Our function was a laplace transform of these. \[f(t) = U(t-a)f(t-a)\] \[L \left\{ f(t) \right\} = L[U(t-a)f(t-a)] = e^{-as}F(s)\] F(s) was the laplace transform of \[f(t) = e^{at}\sin(kt)\]So that gave us: \[L \left\{ f(t) \right\}= L[e^{at}\sin(kt)] = \frac{ k }{ (s-a)^{2}+k^{2} }\] So everything I have labeled as f(t) is the result after taking the inverse transform (or before taking the laplace transform if you prefer)
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