In
mathematics and in particular,
functional analysis, the
Laplace transform of a
function <math>f(t)</math> defined for all
real numbers t ≥ 0 is the function <math>F(s)</math>, defined by:
- <math>F(s)
= \left\{\mathcal{L} f\right\}(s)
=\int_0^\infty e^{-st} f(t)\,dt.</math>
A sometimes convenient abuse of notation, prevailing especially among engineers and physicists, writes this in the following form:
- <math>F(s)
= \mathcal{L} \left\{f(t)\right\}
=\int_0^\infty e^{-st} f(t)\,dt.</math>
The Laplace transform <math>F(s)</math> typically exists for all real numbers <math>s > a</math>, where <math>a</math> is a constant which depends on the growth behavior of <math>f(t)</math>.
The Laplace transform is named after its discoverer Pierre-Simon Laplace.
The transform has a number of properties that make it useful for analysing linear dynamic system.
Properties
- <math>\mathcal{L}\left\{a f(t) + b g(t) \right\}
= a \mathcal{L}\left\{ f(t) \right\} +
b \mathcal{L}\left\{ g(t) \right\}</math>
- <math>\mathcal{L}\{f'\}
= s \mathcal{L}(f) - f(0)</math>
- <math>\mathcal{L}\{f\}
= s^2 \mathcal{L}(f) - s f(0) - f'(0)</math>
- <math>\mathcal{L}\left\{ f^{(n)} \right\}
= s^n \mathcal{L}\{f\} - s^{n - 1} f(0) - \cdots - f^{(n - 1)}(0)</math>
- <math>\mathcal{L}\{ t f(t)\}
= -F'(s)</math>
- <math>\mathcal{L}\left\{ \frac{f(t)}{t} \right\} = \int_s^\infty F(\sigma) d\sigma</math>
- <math>\mathcal{L}\left\{ \int_0^t f(\tau) d\tau \right\}
= {1 \over s} \mathcal{L}\{f\}</math>
- <math>\mathcal{L}\left\{ e^{at} f(t) \right\}
= F(s - a)</math>
- <math>\mathcal{L}^{-1} \left\{ F(s - a) \right\}
= e^{at} f(t)</math>
- <math>\mathcal{L}\left\{ f(t - a) u(t - a) \right\}
= e^{-as} F(s)</math>
- <math>\mathcal{L}^{-1} \left\{ e^{-as} F(s) \right\}
= f(t - a) u(t - a)</math>
Note: <math>u(t)</math> is the
step function.
- <math>\mathcal{L}\{f * g\}
= \mathcal{L}\{ f \} \mathcal{L}\{ g \}</math>
- <math>\mathcal{L}\{ f \}
= {1 \over 1 - e^{-ps}} \int_0^p e^{-st} f(t) dt</math>
See also
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