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Fast Fourier Transforms on Motorola's Digital Signal Processors

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“. . . a digital<br />

signal<br />

processor can<br />

efficiently<br />

compute the<br />

<str<strong>on</strong>g>Fourier</str<strong>on</strong>g><br />

transform and<br />

perform specific<br />

frequencydomain<br />

tasks. . .”<br />

SECTION 1<br />

Introducti<strong>on</strong> to the<br />

<str<strong>on</strong>g>Fourier</str<strong>on</strong>g> Integral<br />

1.1 Definiti<strong>on</strong> and History<br />

The scientific and engineering communities have attempted<br />

to represent changing signals in two<br />

fundamental domains: time and frequency. Temporal<br />

changes are easily shown <strong>on</strong> oscilloscopes, for instance,<br />

where change in time is directly proporti<strong>on</strong>al<br />

to distance across a screen. Representati<strong>on</strong> of signals<br />

in terms of frequencies falls under the general<br />

category of “spectrum analysis”, and has generated a<br />

lot of attenti<strong>on</strong> recently, due to the increased availability<br />

of hardware which makes such representati<strong>on</strong>s<br />

possible. The first formal approach to spectrum analysis<br />

probably dates back to the work of <str<strong>on</strong>g>Fourier</str<strong>on</strong>g>, who<br />

showed how to mathematically represent a general<br />

class of time-varying phenomena in terms of sine and<br />

cosine functi<strong>on</strong>s of particular frequencies. His work is<br />

best known as the <str<strong>on</strong>g>Fourier</str<strong>on</strong>g> Integral (inverse <str<strong>on</strong>g>Fourier</str<strong>on</strong>g><br />

transform) (see Reference 1):<br />

+∞<br />

∫<br />

χ() t Xf ()ej2πft =<br />

dt<br />

+∞<br />

Eqn. 1-1<br />

where: j = – 1 and ej2πft = cos( 2πft)<br />

+ jsin( 2πft)<br />

MOTOROLA 1-1

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