Line 21: | Line 21: | ||
| <math>\sum^{\infty}_{k=-\infty} a_{k}e^{ikw_{0}t}</math> | | <math>\sum^{\infty}_{k=-\infty} a_{k}e^{ikw_{0}t}</math> | ||
| <math>2\pi\sum^{\infty}_{k=-\infty}a_{k}\delta(w-kw_{0}) \ </math> | | <math>2\pi\sum^{\infty}_{k=-\infty}a_{k}\delta(w-kw_{0}) \ </math> | ||
+ | |- | ||
| <math>\sum^{\infty}_{n=-\infty} \delta(t-nT) \ </math> | | <math>\sum^{\infty}_{n=-\infty} \delta(t-nT) \ </math> |
Revision as of 16:35, 14 November 2018
CTFT of periodic signals and some properties with proofs
Function | CTFT | |
---|---|---|
$ sin(\omega_0t) $ | $ \frac{\pi}{j}(\delta(\omega - \omega_0) - \delta(\omega+\omega_0)) $ | |
$ cos(\omega_0t) $ | $ \pi(\delta(\omega - \omega_0) + \delta(\omega+\omega_0)) $ | |
$ e^{j\omega_0t} $ | $ 2\pi\delta(\omega - \omega_0) $ | |
$ \sum^{\infty}_{k=-\infty} a_{k}e^{ikw_{0}t} $ | $ 2\pi\sum^{\infty}_{k=-\infty}a_{k}\delta(w-kw_{0}) \ $ | |
$ \sum^{\infty}_{n=-\infty} \delta(t-nT) \ $ | $ \frac{2\pi}{T}\sum^{\infty}_{k=-\infty}\delta(w-\frac{2\pi k}{T}) $ |
Name | $ x(t) \longrightarrow \ $ | $ \mathcal{X}(\omega) $ |
---|---|---|
Linearity | $ ax(t) + by(t) \ $ | $ a \mathcal{X}(\omega) + b \mathcal{Y} (\omega) $ |
Time Shifting | $ x(t-t_0) \ $ | $ e^{-j\omega t_0}X(\omega) $ |
Frequency Shifting | $ e^{j\omega_0 t}x(t) $ | $ \mathcal{X} (\omega - \omega_0) $ |
Conjugation | $ x^{*}(t) \ $ | $ \mathcal{X}^{*} (-\omega) $ |
Scaling | $ x(at) \ $ | $ \frac{1}{|a|} \mathcal{X} (\frac{\omega}{a}) $ |
Multiplication | $ x(t)y(t) \ $ | $ \frac{1}{2\pi} \mathcal{X}(\omega)*\mathcal{Y}(\omega) $ |
Convolution | $ x(t)*y(t) \ $ | $ \mathcal{X}(\omega)\mathcal{Y}(\omega) \! $ |
Differentiation | $ tx(t) \ $ | $ j\frac{d}{d\omega} \mathcal{X} (\omega) $ |
Parseval's Relation | $ \int_{-\infty}^{\infty} |x(t)|^2 dt = $ | $ \frac{1}{2\pi} \int_{-\infty}^{\infty} |\mathcal{X}(w)|^2 dw $ |