Undergrad Proving Fourier Method: Decompose Wave Forms with Sines & Cosines

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SUMMARY

The discussion confirms that every wave form can be decomposed into a sum of sines and cosines under specific conditions, particularly when considering "almost everywhere" convergence and functions in L1 space. It highlights that the Fourier series of a continuous 2π-periodic function does not converge pointwise at every point, as stated in section 6 of the referenced paper. The concept of "almost everywhere" convergence and the properties of L1 functions are crucial for understanding this decomposition.

PREREQUISITES
  • Understanding of Fourier series and their convergence properties
  • Knowledge of Real Analysis, specifically Lebesgue measure and integration
  • Familiarity with continuous 2π-periodic functions
  • Basic concepts of L1 space in functional analysis
NEXT STEPS
  • Study the properties of Fourier series and their convergence types
  • Explore Lebesgue measure and integration techniques
  • Investigate the concept of L1 space and its applications in analysis
  • Review the implications of "almost everywhere" convergence in functional analysis
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Mathematicians, students of Real Analysis, and anyone interested in the theoretical foundations of Fourier analysis and wave form decomposition.

davidge
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Is it possible to show that every kind of possible wave form can be decomposed into a sum of sines and cosines? If so, how is it done?
 
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You are asking to prove that every possible wave form can be represented as the limit of it's Fourier series. First you have to specify what type of limit convergence and what type of wave form you are talking about. The statement is not true for pointwise convergence and all continuous, periodic functions.

From section 6 of https://mat.iitm.ac.in/home/mtnair/public_html/FS-kesavan.pdf, we have
"A basic question that can be asked is the following: does the Fourier series of a continuous 2π-periodic function, f, converge to f(t) at every point t ∈ [−π, π]? Unfortunately, the answer is ‘No!’".

The statement is true if we specify "almost everywhere" and functions in L1. See the section "Absolutely Convergent Fourier Series" in https://sites.math.washington.edu/~burke/crs/555/555_notes/fourier.pdf.
The definition of "almost everywhere" and L1 are subjects in Real Analysis related to Lebesgue measure, and Lebesgue integration.
 
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