Laplace Transform of Sine Integral Function/Proof 4
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Theorem
- $\laptrans {\map \Si t} = \dfrac 1 s \arctan \dfrac 1 s$
where:
- $\laptrans f$ denotes the Laplace transform of the function $f$
- $\Si$ denotes the sine integral function
Proof
Let $\map f t := \map \Si t = \ds \int_0^t \dfrac {\sin u} u \rd u$.
Then:
- $\map f 0 = 0$
and:
\(\ds \map \Si t\) | \(=\) | \(\ds \int_0^t \dfrac {\sin u} u \rd u\) | Definition of Sine Integral Function | |||||||||||
\(\ds \) | \(=\) | \(\ds \int_0^1 \dfrac {\sin t v} v \rd v\) | Integration by Substitution $u = t v$ | |||||||||||
\(\ds \leadsto \ \ \) | \(\ds \laptrans {\map \Si t}\) | \(=\) | \(\ds \laptrans {\int_0^1 \dfrac {\sin t v} v \rd v}\) | |||||||||||
\(\ds \) | \(=\) | \(\ds \int_0^\infty e^{-s t} \paren {\int_0^1 \dfrac {\sin t v} v \rd v} \rd t\) | Definition of Laplace Transform | |||||||||||
\(\ds \) | \(=\) | \(\ds \int_0^1 \dfrac 1 v \paren {\int_0^\infty e^{-s t} \sin t v \rd t} \rd v\) | exchanging order of integration | |||||||||||
\(\ds \) | \(=\) | \(\ds \int_0^1 \dfrac {\laptrans {\sin t v} } v \rd v\) | Definition of Laplace Transform | |||||||||||
\(\ds \) | \(=\) | \(\ds \int_0^1 \dfrac {\d v} {s^2 + v^2}\) | Laplace Transform of Sine | |||||||||||
\(\ds \) | \(=\) | \(\ds \intlimits {\dfrac 1 s \arctan \dfrac v s} 0 1\) | Primitive of $\dfrac 1 {x^2 + a^2}$ | |||||||||||
\(\ds \) | \(=\) | \(\ds \dfrac 1 s \arctan \dfrac 1 s\) |
$\blacksquare$
Sources
- 1965: Murray R. Spiegel: Theory and Problems of Laplace Transforms ... (previous) ... (next): Chapter $1$: The Laplace Transform: Solved Problems: The Sine, Cosine and Exponential Integrals: $36$: Method $4$