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'Laplace transform'
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| Title of object: |
Laplace transform |
| Canonical Name: |
LaplaceTransform |
| Type: |
Definition |
| Created on: |
2003-06-11 18:29:49 |
| Modified on: |
2008-05-07 13:22:54 |
| Classification: |
msc:44A10 |
Revision comment (for changes between this and next version):
Preamble:
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Content:
Let $f(t)$ be a function defined on the interval $[0,\infty)$. The
\emph{Laplace transform} of $f(t)$ is the function $F(s)$ defined by
\[
F(s)\,=\,\int_{0}^{\infty}e^{-st} f(t)\,dt,
\]
provided that the integral converges. \footnote{Depending on the definition of
integral one is using, one may prefer to define the Laplace transform as
$\lim_{x \to 0+} \int_{x}^{\infty}e^{-st} f(t)\,dt$} It suffices that $f$ be defined when $t>0$ and $s$ can be complex. We will
usually denote the Laplace transform of $f$ by $\mathcal{L}\{f\}$. Some
of the most common Laplace transforms are:
\begin{enumerate}
\item $\mathcal{L}\{e^{at}\}\,=\,\frac{1}{s-a}\,,\,s>a$
\item $\mathcal{L}\{\cos(bt)\}\,=\,\frac{s}{s^{2}+b^{2}}\,,\,s>0$
\item $\mathcal{L}\{\sin(bt)\}\,=\,\frac{b}{s^{2}+b^{2}}\,,\,s>0$
\item $ \mathcal{L}\{t^{n}\}\,=\,\frac{\Gamma(n+1)}{s^{n+1}}\,,\,s>0, n>-1.$
\item $\mathcal{L}\{f'\} = s \mathcal{L}\{f\}-\lim_{x \to 0+}f(x)$
\end{enumerate}
Notice the Laplace transform is a linear transformation. It is worth noting that, if
$$\int_{0}^{\infty}e^{-st} |f(t)| \, dt < \infty$$
for some $s \in \mathbb{R}$, then $\mathcal{L}\{f\}$ is an analytic function in the complex half-plane $\{ z \mid \Re z > s \}$.
Much like the Fourier transform, the Laplace transform has a convolution. However, the form of the convolution used is different.
$$\mathcal{L}\{f*g\} = \mathcal{L}\{f\} \mathcal{L}\{g\}$$
where
$$(f*g) (t) = \int_0^t f(t-s) g(s) \, ds$$
and
$$\mathcal{L}\{fg\}(s) = \int_{c - i \infty}^{c + i \infty} \mathcal{L}\{f\}(z) \mathcal{L}\{g\}(s-z) \, dz$$
The most popular usage of the Laplace transform is to solve initial value problems by taking the Laplace transform of both sides of an ordinary differential equation. |
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