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The Fourier series is instrumental in representing periodic functions, offering a powerful method to decompose such functions into a sum of sinusoids. This technique, however, necessitates modification when applied to nonperiodic functions. Consider a pulse-train waveform consisting of a series of rectangular pulses. When these pulses have a finite period, they can be accurately represented by a Fourier series. Yet, as the period approaches infinity, resulting in a single, isolated pulse, the discrete summation of the Fourier series transforms into a continuous integral known as the Fourier transform.

The transition from the Fourier series to the Fourier transform is pivotal for analyzing nonperiodic functions. The Fourier series decomposes a periodic function x(t) into a sum of sines and cosines, expressed as:

Equation1

Where xn are the Fourier coefficients and ω0​ is the fundamental angular frequency. As the period of the function extends to infinity, the fundamental frequency ω0 tends to zero, and the summation over discrete frequencies 0 evolves into an integral over a continuous frequency variable ω:

Equation2

This integral defines the Fourier transform X(ω), representing the original function x(t) in the frequency domain.

The initial skepticism about representing any periodic function with sinusoids led to the establishment of the Dirichlet conditions. These conditions provide criteria under which a periodic function can be expanded in terms of sinusoids. Specifically, a function x(t) can be represented by a Fourier series if the function has finite discontinuities, finite number of maxima and minima, and it is absolutely integrable over the period.

In practical applications, particularly in image processing, the Fourier transform plays a crucial role. It aids in enhancing images and filtering out noise, thereby making details more distinct and sharper. By transforming an image into the frequency domain, various filtering techniques can be applied to emphasize certain features or reduce noise, and then the inverse Fourier transform is used to convert the processed image back to the spatial domain. This approach is foundational in modern image analysis, enabling advanced techniques in medical imaging, remote sensing, and digital photography.

Tags
Fourier TransformFourier SeriesPeriodic FunctionsNonperiodic FunctionsPulse train WaveformFourier CoefficientsFundamental FrequencyDirichlet ConditionsImage ProcessingFrequency DomainNoise FilteringInverse Fourier TransformMedical Imaging

From Chapter 17:

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17.1 : Continuous -time Fourier Transform

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17.2 : Basic signals of Fourier Transform

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17.3 : Properties of Fourier Transform I

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17.4 : Properties of Fourier Transform II

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17.5 : Parseval's Theorem for Fourier transform

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17.6 : Discrete-time Fourier transform

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17.7 : Properties of DTFT I

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17.8 : Properties of DTFT II

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17.9 : Discrete Fourier Transform

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17.10 : Fast Fourier Transform

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