MHB Problem of the Week #64 - June 17th, 2013

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The discussion centers around Problem of the Week #64, which involves finding the Taylor series for the function f(t) defined piecewise and verifying its Laplace transform. Participants were encouraged to solve the problem, with Sudharaka providing the correct answer. The problem emphasizes the importance of understanding series expansions and Laplace transforms in mathematical analysis. The thread highlights the collaborative nature of problem-solving within the community.
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Thanks again to those who participated in last week's POTW! Here's this week's problem!

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Problem: Let
\[f(t)=\begin{cases}\dfrac{\sin t}{t}, & t\neq 0\\ 1, & t=0.\end{cases}\]

(a) Find the Taylor series for $f$ about $0$.
(b) Assuming that the Laplace transform can be computed term by term, verify that $\mathcal{L}\{f(t)\}=\arctan(1/s)$ for $s>1$.

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This week's question was correctly answered by Sudharaka. You can find his solution below.

(a)

\begin{eqnarray}

f(t)&=&\begin{cases}\frac{\sin t}{t}, & t\neq 0\\ 1, & t=0\end{cases}\\

&=&\begin{cases}\frac{1}{t}\sum_{n=0}^{\infty} \frac{(-1)^n t^{2n+1}}{(2n+1)!}, & t\neq 0\\ 1, & t=0\end{cases}\\

&=&\begin{cases}\sum_{n=0}^{\infty} \frac{(-1)^n t^{2n}}{(2n+1)!}, & t\neq 0\\ 1, & t=0\end{cases}\\

\therefore f(t) &=&\sum_{n=0}^{\infty} \frac{(-1)^n t^{2n}}{(2n+1)!}

\end{eqnarray}

(b)

\begin{eqnarray}

\mathcal{L}\{ f(t) \}&=&\sum_{n=0}^{\infty} \frac{(-1)^n \mathcal{L}\{t^{2n}\}}{(2n+1)!}\\

&=&\sum_{n=0}^{\infty} \frac{(-1)^n}{(2n+1)!}\left(\frac{(2n)!}{s^{2n+1}}\right) \mbox{ where }s>0\\

&=&\sum_{n=0}^{\infty} \frac{(-1)^n}{2n+1}\left(\frac{1}{s}\right)^{2n+1} \mbox{ where }s>0\\

\therefore \mathcal{L}\{ f(t) \}&=& \arctan\left(\frac{1}{s}\right) \mbox{ where }\frac{1}{s}\leq 1

\end{eqnarray}

That is,

\[\mathcal{L}\{ f(t) \}= \arctan\left(\frac{1}{s}\right) \mbox{ where }s\geq 1\]

Note: Here we have assumed \(s\) to be a real number. Although the Laplace transform is defined for complex \(s\) as well.
 

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