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The Fourier Transform and its applications goals: present the Fourier ...

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F �s�=FT � f � x ��=CT �e �x �� – i ST �o �x ��<br />

i.e. <strong>Fourier</strong> <strong>Transform</strong> ⇔<br />

Cosine-<strong>Transform</strong> of <strong>the</strong> even <strong>and</strong> Sine-<strong>Transform</strong> of <strong>the</strong> odd part of f �x �<br />

Note: as e � x � <strong>and</strong> o � x� need to be defined only for x�0 , <strong>the</strong> continuation to x�0 being<br />

given by symmetry ( e �−x �=e � x � ; o �−x �=−o� x � ), <strong>the</strong> <strong>Fourier</strong> transform carries <strong>the</strong><br />

full information on f �x � , both for x�0 <strong>and</strong> x�0 , although <strong>the</strong> integration in <strong>the</strong> CT<br />

<strong>and</strong> ST only use e � x � <strong>and</strong> o � x� for x�0 .<br />

We can thus, like always, get f �x � back from F �s� through <strong>the</strong> "+i" transform, giving:<br />

f �x�=FT �i � F �s��=CT � E �s���i ST �O�s��<br />

i.e. <strong>Fourier</strong> Backtransform ⇔<br />

Cosine-<strong>Transform</strong> of <strong>the</strong> even <strong>and</strong> Sine-<strong>Transform</strong> of <strong>the</strong> odd part of F �s�<br />

Note: in <strong>the</strong> CT , ST -world (no FT known),<br />

given F �s� , calculate E �s� <strong>and</strong> O�s� , from this, throughCT resp. ST , calculate<br />

f �x �<br />

Symmetries of Cosine- <strong>and</strong> Sine-<strong>Transform</strong>: with F C �s�=CT � f �x �� , F S �s�=ST � f �x�� ,<br />

we have: F C �−s�=F C �s� Cosine-<strong>Transform</strong> is even in s,<br />

F S �−s�=−F S � s� Sine-<strong>Transform</strong> is odd in s<br />

<strong>The</strong> <strong>Fourier</strong> <strong>Transform</strong> <strong>and</strong> <strong>its</strong> Applications, Jürgen Stutzki, Sommersemester 2007<br />

math_ground_11.odt<br />

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