Laplace Transform of Dirac Delta Function/Proof 1
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Theorem
Let $\map \delta t$ denote the Dirac delta function.
The Laplace transform of $\map \delta t$ is given by:
- $\laptrans {\map \delta t} = 1$
Proof
\(\ds \laptrans {\map \delta t}\) | \(=\) | \(\ds \int_0^{\to +\infty} e^{-s t} \map \delta t \rd t\) | Definition of Laplace Transform | |||||||||||
\(\ds \) | \(=\) | \(\ds e^{-s \times 0}\) | Integral to Infinity of Dirac Delta Function by Continuous Function | |||||||||||
\(\ds \) | \(=\) | \(\ds e^0\) | ||||||||||||
\(\ds \) | \(=\) | \(\ds 1\) |
$\blacksquare$