Chris' Page for HW 4 (Fourier Transforms): Difference between revisions
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== Mathematical Description == |
== Mathematical Description == |
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The Fourier Transform is detonated by; |
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The Inverse Fourier Transform is; |
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:<math>x(t) = \frac{1}{2\pi} \int_{-\infty}^{\infty} X(\omega)\ e^{ j\omega t}\,d\omega, </math> |
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== Relation to Laplace Transform == |
== Relation to Laplace Transform == |
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Unless otherwise noted, a Laplace Transform is defined by the unilateral or one-sided integral |
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:<math>\mathcal{L} \left\{f(t)\right\}=\int_{0^-}^\infty e^{-st} f(t) \,dt. </math> |
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The Laplace Transform can be applied from <math>-\infty</math> to <math>\infty</math>, this is known as the Bilateral Laplace Transform and is denoted by |
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: <math>\mathcal{L}\left\{f(t)\right\} =\int_{-\infty}^{\infty} e^{-st} f(t)\,dt.</math> |
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== Examples == |
== Examples == |
Revision as of 00:03, 3 November 2007
The Fourier Transform is a process or formula that converts a signal from one domain to another. Often it is used to go between the time domain and the frequency domain.
Developed by Frenchman, Jean Baptiste Joseph Fourier (1768 - 1830), the Fourier Transform stems from the more general Fourier Analysis, which is the representation of a function with sine and cosine terms. Unlike the Fourier Series the Fourier Transform is capable of representing aperiodic signals.
Mathematical Description
The Fourier Transform is detonated by;
The Inverse Fourier Transform is;
Relation to Laplace Transform
Unless otherwise noted, a Laplace Transform is defined by the unilateral or one-sided integral
The Laplace Transform can be applied from to , this is known as the Bilateral Laplace Transform and is denoted by