ASN3 - Class Notes October 5: Difference between revisions

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<math> x(t)=  \int_{-\infty} ^ {\infty} x(t')[\int_{-\infty} ^ {\infty} e^{ j2 \pi f(t'-t)} df ]dt'  \!</math>
<math> x(t)=  \int_{-\infty} ^ {\infty} x(t')[\int_{-\infty} ^ {\infty} e^{ j2 \pi f(t'-t)} df ]dt'  \!</math>


note that the defination of the delta function is <math>\int_{-\infty} ^ {\infty} e^{ j2 \pi f(t'-t)} df \!</math>
note that the defination of the delta function is <math>\int_{-\infty} ^ {\infty} e^{ j2 \pi f(t'-t)} df \!</math>


<math> x(t)=  \int_{-\infty} ^ {\infty} x(t')\delta_(t'-t) dt'  \!</math>
<math> x(t)=  \int_{-\infty} ^ {\infty} x(t')\delta_(t'-t) dt'  \!</math>
THE GAME  
 
                THE GAME  


LTI (Linear Time Invariant System)
LTI (Linear Time Invariant System)
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Input    LTI                      Output        Reason
Input    LTI                      Output        Reason


 
<math> x(t)\longrightarrow  \int_{-\infty} ^ {\infty} x(t')\delta_(t'-t) dt'  \!</math>
 
<math> X(f)\longrightarrow  \int_{-\infty} ^ {\infty} X(f')\delta_(f'-f) df'  \!</math>
 
<math> x2(t) \!</math> '''.''' <math> e^{\frac{ -j2 \pi mt}{T}} = \int_{-\frac{T}{2}}^{\frac{T}{2}}\sum_{n=0}^\infty a_n e^{\frac{ j2 \pi nt}{T}}e^{\frac{ -j2 \pi mt}{T}} dt =\sum_{n=0}^\infty a_n \int_{-\frac{T}{2}}^{\frac{T}{2}} e^{\frac{ j2 \pi (n-m)t}{T}} dt =\sum_{n=0}^\infty a_n T \delta_{mn} \!</math>

Revision as of 13:55, 3 December 2009

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1/T⟶df

n/T⟶f

∑n=−∞∞1T⟶∫−∞∞()df


Can we make an unperiodic signal and make it periodic by taking the limit?

x(t)=limT→∞1T(∫−T2T2x(t′)e−j2πnt′Tdt′)ej2πntT

note that X(F)=ℱ[x(t)]∫−T2T2x(t′)e−j2πnt′Tdt′

becomes as the limit is taken n/t becomes f x(t)=∫−∞∞[∫−∞∞x(t′)e−j2πft′dt′]ej2πftdf

x(t)=∫−∞∞x(t′)[∫−∞∞ej2πf(t′−t)df]dt′

note that the defination of the delta function is ∫−∞∞ej2πf(t′−t)df

x(t)=∫−∞∞x(t′)δ(t′−t)dt′

               THE GAME 

LTI (Linear Time Invariant System)

Input LTI Output Reason

x(t)⟶∫−∞∞x(t′)δ(t′−t)dt′ X(f)⟶∫−∞∞X(f′)δ(f′−f)df′