Fourier transform: Difference between revisions

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==Some Useful Fourier Transform Identities==
==Some Useful Fourier Transform Identities==
        {\hbox{\boldmath $\textstyle #1$}}
<math>
\mathcal{F}[\alpha(t)*\beta(t)]=\Alpha(f)\Beta(f)
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<br>
<math>
\mathcal{F}[\alpha(t)\beta(t)]=\Alpha(f)*\Beta(f)
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==A Second Approach to Fourier Transforms==
==A Second Approach to Fourier Transforms==

Revision as of 10:04, 10 December 2004

From the Fourier Transform to the Inverse Fourier Transform

An initially identity that is useful: X(f)=∫−∞∞x(t)e−j2πftdt

Suppose that we have some function, say β(t), that is nonperiodic and finite in duration.
This means that β(t)=0 for some Tα<|t|

Now let's make a periodic function γ(t) by repeating β(t) with a fundamental period Tζ. Note that limTζ→∞γ(t)=β(t)
The Fourier Series representation of γ(t) is
γ(t)=∑k=−∞∞αkej2πfkt where f=1Tζ
and αk=1Tζ∫−Tζ2Tζ2γ(t)e−j2πktdt
αk can now be rewritten as αk=1Tζ∫−∞∞β(t)e−j2πktdt
From our initial identity then, we can write αk as αk=1TζB(kf)
and γ(t) becomes γ(t)=∑k=−∞∞1TζB(kf)ej2πfkt
Now remember that β(t)=limTζ→∞γ(t) and 1Tζ=f.
Which means that β(t)=limf→0γ(t)=limf→0∑k=−∞∞fB(kf)ej2πfkt
Which is just to say that β(t)=∫−∞∞B(f)ej2πfktdf

So we have that ℱ[β(t)]=B(f)=∫−∞∞β(t)e−j2πftdt
Further ℱ−1[B(f)]=β(t)=∫−∞∞B(f)ej2πfktdf

Some Useful Fourier Transform Identities

ℱ[α(t)*β(t)]=A(f)B(f)
ℱ[α(t)β(t)]=A(f)*B(f)

A Second Approach to Fourier Transforms