Signals and systems/GF Fourier: Difference between revisions

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==Changing Basis Functions==
==Changing Basis Functions==


==Notes==
==Identities==
<math>e^{j \theta} = \cos \theta + j \sin  \theta \, </math>
<math>e^{j \theta} = \cos \theta + j \sin  \theta \, </math>
<math>\sin x = \frac{e^{jx}-e^{-jx}}{2j} \,</math>
<math>\cos x = \frac{e^{jx}+e^{-jx}}{2} \,</math>


<math> \left \langle n \mid m \right \rangle = T \delta_{n,m} \,</math>
<math> \left \langle n \mid m \right \rangle = T \delta_{n,m} \,</math>

Revision as of 12:07, 29 October 2006

Fourier series

The Fourier series is used to analyze arbitrary periodic functions by showing them as a composite of sines and cosines.

A function is considered periodic if x(t)=x(t+T) for T≠0.

The exponential form of the Fourier series is defined as x(t)=∑n=−∞∞αnej2πnt/T

Determining the coefficient αn

⟨Bra∣Ket⟩ Notation

Linear Time Invariant Systems

Changing Basis Functions

Identities

ejθ=cos⁡θ+jsin⁡θ

sin⁡x=ejx−e−jx2j

cos⁡x=ejx+e−jx2

⟨n∣m⟩=Tδn,m