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| URL | https://lpsa.swarthmore.edu/LaplaceXform/FwdLaplace/LaplaceXform.html |
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| Meta Title | The Laplace Transform |
| Meta Description | Linear Physical Systems Analysis, Laplace Transforms |
| Meta Canonical | null |
| Boilerpipe Text | The definition of the Laplace Transform that we will use is called a
"one-sided" (or unilateral) Laplace Transform and is given by: The Laplace Transform seems, at first, to be a fairly abstract and esoteric
concept. In practice, it allows one to (more) easily solve a huge variety
of problems that involve linear systems, particularly differential equations. It allows for compact
representation of systems (via the "Transfer Function"), it simplifies
evaluation of the convolution integral, and it turns problems involving
differential equations into algebraic problems. As indicated by the quotes
in the animation above (from some students at Swarthmore College), it almost magically simplifies problems that otherwise
are very difficult to solve. There are a few things to note about the Laplace Transform. Before we show how the Laplace Transform is useful, we need to lay some
groundwork. We start by finding the Laplace Transform of some functions
and from there move on to finding properties of the Laplace Transform. With tables of the Laplace Transform of
Functions and Properties
of the Laplace Transform it becomes possible to find the Laplace Transform
of almost any function of interest without resorting to the integral shown above. Applications of the Laplace Transform
are discussed next - mostly the use of the Laplace Transform to solve
differential equations. Finally, the inverse Laplace Transform is covered
(though this is a large enough topic that it has its
own page
elsewhere ). References |
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| Shard | 45 (laksa) |
| Root Hash | 9311362577169933845 |
| Unparsed URL | edu,swarthmore!lpsa,/LaplaceXform/FwdLaplace/LaplaceXform.html s443 |