DTFS

Creator
Creator
Seonglae Cho
Created
Created
2023 Sep 13 2:10
Editor
Edited
Edited
2023 Nov 22 3:2

Discrete Time Fourier series

  • x[n]=ejω0nx[n] = e^{j\omega_0n} is periodic only when ω0=2πmN\omega_0 = 2\pi\frac{m}{N}. The fundamental period is Ngcd(m,N)\frac{N}{gcd(m, N)}. ω0\omega_0 is the value of phase at n=1n=1
  • For x[n]=ej2πnNx[n] = e^{j2\pi\frac{n}{N}}, there are only NN distinct harmonics ϕk[n]=ej2πknN\phi_k[n] = e^{j2\pi\frac{kn}{N}}
k=<N>k=<N> indicates any period of duration NN and ω0=2πN\omega_0 = \frac{2\pi}{N}
Signal can be represented as orthogonal signal set {ϕk(t)=ejω0kt,k=<N>}\{\phi_k(t) = e^{j\omega_0kt}, k=<N>\}
x[n]=k=<N>akejkω0nak=1Nk=<N>x[n]ejkω0nx[n] = \sum_{k=<N>}a_ke^{jk\omega_0n} \newline a_k = \frac{1}{N} \sum_{k=<N>} x[n]e^{-jk\omega_0n}
There is no convergence issue since we are dealing with a finite number of harmonics.
  • kk is the variable for selecting a harmonic
  • nn is the variable for selecting the time instant
DTFS Notion
 
 
notion image
 
 
 

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