Fourier Series coefficients, orthogonal?

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SUMMARY

The discussion focuses on the orthogonality of Fourier series coefficients using complex exponentials. The key equation discussed is the proof of the integral relationship \(\frac{1}{T}\int^T_0 e^{inw_0t}e^{-imw_0t} dt = \delta_{m}{n}\), where \(m\) and \(n\) are integers. The user initially struggles with the proof but receives guidance to approach it by considering cases where \(m = n\) and \(m \neq n\). This method simplifies the integration process and leads to a clearer understanding of the orthogonality concept.

PREREQUISITES
  • Understanding of Fourier series and their coefficients
  • Familiarity with complex exponentials and integration
  • Knowledge of Dirac delta function and Kronecker delta function
  • Basic calculus skills for performing integrals
NEXT STEPS
  • Study the derivation of Fourier series using complex exponentials
  • Learn about the properties of the Dirac delta function in signal processing
  • Explore the application of orthogonality in Fourier analysis
  • Practice integration techniques involving complex functions
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Students and educators in mathematics or engineering, particularly those studying signal processing, Fourier analysis, or complex analysis.

Dollydaggerxo
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Homework Statement



Hello. I need help with orthogonality of the Fourier series coefficients. I know you can use the dirac delta function, (or the kronecker function) in the orthogonality relationship. I want to try and see the derivation using complex form rather than sines and cosines.

Homework Equations



proof of
\frac{1}{T}\int^T_0 e^{inw_0t}e^{-imw_0t} dt = \delta_{m}{n}

The Attempt at a Solution



Basically I haven't got very far, do not know where to start in this proof. any help would be appreciated?

thanks
 
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Obviously, m and n must be integers, which makes things really easy. Just assume m=n, do the integration and write down what you get. Then assume m \neq n, do the integration and write down what you get.
 
Okay I have got it. Thanks!
 
Last edited:

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