How Fourier Expansion indicates the Amplitude w.r.t a certain frequency?

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SUMMARY

The discussion focuses on extracting the amplitude of a sinusoidal component from a continuous wave using Fourier Expansion. The key formula used is F(ω) = ∫ f(t) e^{-j ω t} dt, where the user attempts to find the amplitude at a specific frequency ω_0. The user initially misinterprets the result as Re{F(ω)} = A * (sin(ω_0 - ω) / (ω_0 - ω)), but later realizes that the correct amplitude is given by |F(ω)|, complicating the calculation further. This highlights the importance of understanding the distinction between real parts and magnitudes in Fourier analysis.

PREREQUISITES
  • Understanding of Fourier Transform and its applications
  • Familiarity with complex numbers and exponential functions
  • Knowledge of integrals and limits in calculus
  • Basic concepts of sinusoidal functions and their properties
NEXT STEPS
  • Study the properties of the Fourier Transform, focusing on amplitude extraction
  • Learn about the relationship between the Fourier Transform and frequency response
  • Explore the concept of the magnitude of complex functions in signal processing
  • Practice solving problems involving Fourier Expansion with various waveforms
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Students in electrical engineering, signal processing enthusiasts, and anyone studying Fourier analysis who seeks to deepen their understanding of amplitude extraction from continuous waves.

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Homework Statement



I want to know how could I extract the amplitude(of the sinusoid component) of a random continuous wave w.r.t a certain frequency response? The teacher said the Fourier Expansion can do that but I'm really confused by the limits and integrals.


Homework Equations



F(\omega)=\int f(t) e^{-j \omega t} dt

The Attempt at a Solution



I tried the very easy example and want to extract the amplitude where the frequency matches(say \omega = \omega_0). f(t)=A \cdot cos\omega_0t,\hat{f}(t)=A \cdot e^{j \omega_0 t},\hat{F}(\omega)=\int \hat{f}(t) \cdot e^{-j \omega t} dt, range (-\infty ,\infty), but it turned out to be Re\{ \hat{F}( \omega ) \}=A \cdot \frac{sin(\omega_0 - \omega ) (t_2-t_1)}{\omega_0 - \omega}, where t_2=\infty,t_1=-\infty , it's weird if I follow the basic operation of sin function, I got Re\{ \hat{F}( \omega ) \}=2 \cdot A \cdot \frac{sin(\omega_0 - \omega ) \infty}{\omega_0 - \omega}, and then although applying that lim \frac{sinx}{x} -> 1 while x->0, it's 2A, besides I don't even know if this's right.

I have no idea what happened...

Any help will be appreciated !
 
Last edited:
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Terribly sorry that my teacher has corrected my mistakes, the Amplitude should be |F(\omega)| instead of Re \{ \hat{F}(\omega) \},but the calculation becomes even harder, I'm still trying on this question.
 

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