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Let f be a piecewise smooth function defined for t between 0 and infinity and let s be positive. Then the Laplace transform F of f is defined by
The Laplace transform is a close relative of the Fourier transform. However, the fact that the Laplace transform is defined on the semi-infinite interval from 0 to infinity rather than on the whole real line, makes it somewhat more useful for dealing with initial value problems for ordinary differential equations. In addition, the Laplace transform is useful in determining solutions of partial differential equations -- particularly where the time or spatial domains are semi-infinite, e.g., heat flow in an infinite rod where the temperature at one end is known.
Just as with the Fourier transform, the convolution of functions plays an important role in calculating Laplace transforms and inverse Laplace transforms. For the Laplace transform, the appropriate convolution f * g is given by
With this definition of convolution, if F is the Laplace transform of f and G is the Laplace transform of g, the Laplace transform of f * g is just the product of F and G.
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