10/3,6 - The Game: Difference between revisions

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|<math>=H(\omega_n)\,\!</math>
|<math>=\left \langle h \mid e^{j2\pi \omega_n u} \right \rangle e^{j2\pi \omega_n t}</math>
|Different notation
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|<math>=H(\omega_n)e^{j2\pi \omega_n t}</math>
|Different notation
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*Note that <math>\int_{-\infty}^{\infty} e^{-j2\pi \omega_nu} h(n)\, du</math> can be written as <math>\left \langle h \mid e^{j2\pi \omega_n u} \right \rangle</math> or <math>H(\omega_u)\,\!</math>
*Explain the rest of the page

Revision as of 17:36, 12 November 2008

The Game

The idea behind the game is to use linearity (superposition and proportionality) and time invariance to find an output for a given input. An initial input and output are given.

Input LTI System Output Reason
δ(t) ⟹ h(t) Given
δ(t−λ) ⟹ h(t−λ) Time Invarience
x(λ)δ(t−λ) ⟹ x(λ)h(t−λ) Proportionality
x(t)=∫−∞∞x(λ)δ(t−λ)dx ⟹ ∫−∞∞x(λ)h(t−λ)dx⏟ConvolutionIntegral Superposition

With the derived equation, note that you can put in any x(t) to find the given output. Just change your t for a lambda and plug n chug.

Example

Let x(t)=ej2πnt/T=ej2πωnt

ej2πωnt =∫−∞∞ej2πωnλh(t−λ)dλ Let t−λ=u thus du=−dλ
=−∫∞−∞ej2πωn(t−u)h(u)du The order of integration switched due to changing from −λ=u
=(∫−∞∞e−j2πωnuh(u)du)⏟eigenvalueej2πωnt⏟eigenfunction
=⟨h∣ej2πωnu⟩ej2πωnt Different notation
=H(ωn)ej2πωnt Different notation