MHB Having trouble with the Laplace Transform

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The discussion revolves around solving the differential equation using Laplace transforms, specifically $y'' + 4y' + 4y = e^t$ with initial conditions $y(0) = 1$ and $y'(0) = 0$. The user successfully derived the expression for $Y$ but encountered difficulties with partial fraction decomposition. They initially found $A = 1$ but were unsure about determining $B$, later opting for polynomial long division to simplify the problem. The final solution yielded $1 - 2e^{-2t} + 2te^{-2t}$, leading to a question about why Wolfram Alpha represents the constant term as a delta function. The explanation provided clarifies that the Laplace transform of the delta function equals 1, linking it back to the original equation.
shamieh
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Solve by Laplace Transforms.

$y'' + 4y' + 4y = e^t$ $y(0) = 1$, $y'(0) = 0$So I've got

$s^2Y - s + 4sY - 1 + 4Y = \frac{1}{s+1}$

then I got:
$ Y = \frac{s^2+2s+2}{(s+2)(s+2)}$

Now here is where I am getting lost on the partial fraction decomposition..

I've got $s^2+2s+2 = A(s+2) + B$ I got $A =1$ but can't remember what to do to get $B$ .. is $B=0$?
 
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Nevermind, I solved it using polynomial long division which really sucked.

But I ended up with $1 - 2e^{-2t} + 2te^{-2t}$ but why does wolphram alpha replace the 1 with a $\delta$?
 
shamieh said:
Nevermind, I solved it using polynomial long division which really sucked.

But I ended up with $1 - 2e^{-2t} + 2te^{-2t}$ but why does wolphram alpha replace the 1 with a $\delta$?

... because is ...

$\displaystyle \mathcal {L} \{ \delta (t) \} = \int_{0}^{\infty} \delta (t)\ e^{- s\ t}\ d t = e^{0} = 1 \implies \mathcal{L}^{-1} \{ 1\} = \delta(t)\ (1)$

Kind regards

$\chi$ $\sigma$
 

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