How can duality be used to solve for the Fourier Transform of a constant?

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SUMMARY

The Fourier Transform of a constant function, specifically 1, is calculated as \(\mathscr{F}\{1\} = \sqrt{2\pi}\delta(\omega)\). This result is derived using the duality property of Fourier transforms, which states that the Fourier transform of a delta function results in a constant. The initial incorrect approach yielded an indeterminate form, highlighting the importance of applying the correct mathematical principles in Fourier analysis.

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dimension10
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How does one find the Fourier Transform of 1?

\mathscr{F}\{1\}=\mathcal{F}\{1\}=\int\limits_{-\infty}^{\infty}{e}^{-i \omega t} \mbox{d}t=?

I tried to solve it and came up with

\sqrt{\frac{2}{\pi}}\frac{1}{\omega}\lim_{t \rightarrow \infty}\sin\left(\omega t\right)

but that is indeterminate whereas actual answer is

\sqrt{2\pi}\delta\left(\omega\right)

So how does one actually solve this Fourier Transform.

Thanks in advance.
 
Last edited:
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Use duality. Compute the Fourier transform of the delta function and you get a constant, so the Fourier transform of a constant is a delta function. Just look up duality for Fourier transforms and you'll see what I mean.
 
homeomorphic said:
Use duality. Compute the Fourier transform of the delta function and you get a constant, so the Fourier transform of a constant is a delta function. Just look up duality for Fourier transforms and you'll see what I mean.

Thanks a lot!
 
Last edited:

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