Laplace Transform of t by Sine a t
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Theorem
Let $\sin$ denote the real sine function.
Let $\laptrans f$ denote the Laplace transform of a real function $f$.
Then:
- $\laptrans {t \sin a t} = \dfrac {2 a s} {\paren {s^2 + a^2}^2}$
Proof 1
\(\ds \laptrans {t \sin a t}\) | \(=\) | \(\ds -\map {\dfrac \d {\d s} } {\laptrans {\sin a t} }\) | Derivative of Laplace Transform | |||||||||||
\(\ds \) | \(=\) | \(\ds -\map {\dfrac \d {\d s} } {\dfrac a {s^2 + a^2} }\) | Laplace Transform of Sine | |||||||||||
\(\ds \) | \(=\) | \(\ds \dfrac {2 a s} {\paren {s^2 + a^2}^2}\) | Quotient Rule for Derivatives |
$\blacksquare$
Proof 2
We have:
\(\ds \laptrans {\cos a t}\) | \(=\) | \(\ds \int_0^\infty e^{-s t} \cos a t \rd t\) | Definition of Laplace Transform | |||||||||||
\(\text {(1)}: \quad\) | \(\ds \) | \(=\) | \(\ds \dfrac s {s^2 + a^2}\) | Laplace Transform of Cosine |
Hence:
\(\ds \dfrac \d {\d a} \int_0^\infty e^{-s t} \cos a t \rd t\) | \(=\) | \(\ds \int_0^\infty e^{-s t} \paren {\map {\dfrac \partial {\partial a} } {\cos a t} } \rd t\) | Derivative of Integral | |||||||||||
\(\ds \) | \(=\) | \(\ds \int_0^\infty e^{-s t} \paren {-t \sin a t} \rd t\) | Derivative of Cosine Function | |||||||||||
\(\ds \) | \(=\) | \(\ds -\laptrans {t \sin a t}\) | Definition of Laplace Transform | |||||||||||
\(\ds \) | \(=\) | \(\ds \map {\dfrac \d {\d a} } {\dfrac s {s^2 + a^2} }\) | from $(1)$ | |||||||||||
\(\ds \) | \(=\) | \(\ds -\dfrac {2 a s} {\paren {s^2 + a^2}^2}\) | Quotient Rule for Derivatives |
and the result follows.
$\blacksquare$
Sources
- 1968: Murray R. Spiegel: Mathematical Handbook of Formulas and Tables ... (previous) ... (next): $\S 32$: Table of Special Laplace Transforms: $32.43$