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<math>=c_1G(f) + c_2H(f)</math><br/> | <math>=c_1G(f) + c_2H(f)</math><br/> | ||
|- | |- | ||
+ | |||
+ | |Time Shifting | ||
+ | |<math>\mathfrak{F}(g(t - a)) = e^{-i2\pi fa}*G(f) </math> | ||
+ | |<math>\int_{-\infty}^\infty g(t-a)e^{-2\pi ft}dt </math><br/> | ||
+ | <math>\int_{-\infty}^\infty g(u)e^{-i2\pi f(u+a)} du </math><br/> | ||
+ | <math>e^{-i2\pi fa}\int_{-\infty}^|infty g(u)e^{-i2\pi fu} du <\math><br\> | ||
+ | <math>e^{-i2\pi fa}G(f)<\math><br/> | ||
|- | |- | ||
} | } |
Revision as of 20:31, 22 April 2018
Table of CT Fourier Series Coefficients and Properties
Fourier series Coefficients
Function | Fourier Series | Coefficients |
---|---|---|
Properties of CT Fourier systems
Property Name | Property | Proof |
---|---|---|
Linearity | $ \mathfrak{F}(c_1g(t) + c_2h(t) = c_1G(f) + c_2H(f) $ | $ \mathfrak{F}(c_1g(t) + c_2h(t) = \int_{-\infty}^\infty c_1g(t) dt + \int_{-\infty}^\infty c_2h(t) dt $ $ =c_1\int_{-\infty}^\infty g(t)e^{i2\pi ft} dt + c_2 \int_{-\infty}^\infty g(t)e^{i2\pi ft} dt $ |
Time Shifting | $ \mathfrak{F}(g(t - a)) = e^{-i2\pi fa}*G(f) $ | $ \int_{-\infty}^\infty g(t-a)e^{-2\pi ft}dt $ $ \int_{-\infty}^\infty g(u)e^{-i2\pi f(u+a)} du $ |