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<record version="3" id="10918">
 <title>Laplace transform of $\frac{f(t)}{t}$</title>
 <name>LaplaceTransformOfFracftt</name>
 <created>2008-08-05 14:51:25</created>
 <modified>2008-08-05 17:20:27</modified>
 <type>Derivation</type>
<parent id="10637">Laplace transform of $t^nf(t)$</parent>
 <creator id="2872" name="pahio"/>
 <author id="2872" name="pahio"/>
 <classification>
	<category scheme="msc" code="44A10"/>
 </classification>
 <related>
	<object name="FundamentalTheoremOfCalculusClassicalVersion"/>
	<object name="SubstitutionNotation"/>
	<object name="CyclometricFunctions"/>
 </related>
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 <content>Suppose that the quotient
$$\frac{f(t)}{t} \,:=\; g(t)$$
is \PMlinkname{Laplace-transformable}{LaplaceTransform}.\, It follows easily that also $f(t)$ is such.\, According to the \PMlinkname{parent entry}{LaplaceTransformOfTnft}, we may write
$$\mathcal{L}^{-1}\left\{G'(s)\right\} \,=\, -t\,g(t) \,=\, -f(t) \,=\, \mathcal{L}^{-1}\left\{-F(s)\right\}.$$
Therefore
$$G'(s) \,=\, -F(s),$$
whence
\begin{align}
G(s) \,=\, -F^{(-1)}(s)+C
\end{align}
where $F^{(-1)}(s)$ means any antiderivative of $F(s)$.\, Since each Laplace transformed function vanishes in the infinity \,$s = \infty$\, and thus\, $G(\infty) = 0$,\, the equation (1) implies
$$C \,=\, F^{(-1)}(\infty)$$
and therefore
$$G(s) \,=\, F^{(-1)}(\infty)\!-\!F^{(-1)}(s) \,=\, \int_s^\infty F(u)\,du.$$
We have obtained the result
\begin{align}
\mathcal{L}\left\{\frac{f(t)}{t}\right\} \,=\, \int_s^\infty F(u)\,du.
\end{align}


\textbf{Application.}\, By the table of Laplace transforms,\, 
$\displaystyle\mathcal{L}\left\{\sin{t}\right\} = \frac{1}{s^2+1}.$\, Accordingly the formula (2) yields
$$\mathcal{L}\left\{\frac{\sin{t}}{t}\right\} = \int_s^{\,\infty}\!\frac{1}{u^2+1}\,du
= \sijoitus{s}{\quad\infty}\!\arctan{u} \,=\, \frac{\pi}{2}\!-\!\arctan{s} \,=\, \arccot{s}.$$
Thus we have
\begin{align}
\mathcal{L}\left\{\frac{\sin{t}}{t}\right\} \,=\, \arccot{s} \,=\, \arctan\frac{1}{s}.
\end{align}
This result is derived in the entry Laplace transform of sine integral in two other ways.



</content>
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