Line 73: Line 73:
 
| <math> \int_{0}^{t}F(u)G(t-u)du </math>
 
| <math> \int_{0}^{t}F(u)G(t-u)du </math>
 
|-
 
|-
| align="right" style="padding-right: 1em;" | please continue
+
| align="right" style="padding-right: 1em;" |  
| place formula here
+
| <math> \int_{s}^{\infty}f(u)du </math>
|-<math> af_1(s)+bf_2(s)</math>
+
| <math> \frac{F(t)}t</math>
 
|-
 
|-
 
| align="right" style="padding-right: 1em;" | please continue
 
| align="right" style="padding-right: 1em;" | please continue

Revision as of 15:29, 5 November 2010

Laplace Transform Pairs and Properties
Definition
Laplace Transform $ X(s)=\int_{-\infty}^\infty x(t) e^{-st}dt, \ s\in {\mathbb C} \ $
Inverse Laplace Transform add formula here
Properties of the Laplace Transform
f(s) F(t)
$ af_1(s)+bf_2(s) $ $ aF_1(t)+bF_2(t) $
$ f(s/a) $ $ aF(at) $
$ f(s-a) $ $ e^{at}F(t) $
$ e^{-as}f(s) $ $ u(t-a) = \begin{cases} F(t-a) & t>a \\ 0 & t<a \end{cases} $
$ sf(s)-F(0) $ $ F'(t) $
$ s^2f(s)-sF(0)-F'(0) $ $ F''(t) $
$ s^{n}f(s)-s^{n-1}F(0)-s^{n-2}F'(0)-...-F^{n-1}(0) $ $ F^{(n)}(t) $
$ f'(s) $ $ -tF(t) $
$ f''(s) $ $ t^2F(t) $
$ f^{(n)}(s) $ $ (-1)^{(ntn)}F(t) $
$ \frac{f(s)}s $ $ \int_{0}^{t} F(u) du $
$ \frac{f(s)}{s^n} $ $ \int_{0}^{t}...\int_{0}^{t}F(u)du^n = \int_{0}^{t}\frac{{(t-u)}^{n-1}}{(n-1)!} F(u)du $
$ f(s)g(s) $ $ \int_{0}^{t}F(u)G(t-u)du $
$ \int_{s}^{\infty}f(u)du $ $ \frac{F(t)}t $
please continue place formula here
please continue place formula here
please continue place formula here
please continue place formula here
please continue place formula here
Laplace Transform Pairs
notes Signal Laplace Transform ROC
unit impulse/Dirac delta $ \,\!\delta(t) $ 1 $ \text{All}\, s \in {\mathbb C} $
unit step function $ \,\! u(t) $ $ \frac{1}{s} $ $ \mathcal{R} \mathfrak{e} \lbrace s \rbrace > 0 $
$ \,\! -u(-t) $ $ \frac{1}{s} $ $ \mathcal{R} \mathfrak{e} \lbrace s \rbrace < 0 $
$ \frac{t^{n-1}}{(n-1)!}u(t) $ $ \frac{1}{s^{n}} $ $ \mathcal{R} \mathfrak{e} \lbrace s \rbrace > 0 $
$ -\frac{t^{n-1}}{(n-1)!}u(-t) $ $ \frac{1}{s^{n}} $ $ \mathcal{R} \mathfrak{e} \lbrace s \rbrace < 0 $
$ \,\!e^{-\alpha t}u(t) $ $ \frac{1}{s+\alpha} $ $ \mathcal{R} \mathfrak{e} \lbrace s \rbrace > -\alpha $
$ \,\! -e^{-\alpha t}u(-t) $ $ \frac{1}{s+\alpha} $ $ \mathcal{R} \mathfrak{e} \lbrace s \rbrace < -\alpha $
$ \frac{t^{n-1}}{(n-1)!}e^{-\alpha t}u(t) $ $ \frac{1}{(s+\alpha )^{n}} $ $ \mathcal{R} \mathfrak{e} \lbrace s \rbrace > -\alpha $
$ -\frac{t^{n-1}}{(n-1)!}e^{-\alpha t}u(-t) $ $ \frac{1}{(s+\alpha )^{n}} $ $ \mathcal{R} \mathfrak{e} \lbrace s \rbrace < -\alpha $
$ \,\!\delta (t - T) $ $ \,\! e^{-sT} $ $ \text{All}\,\, s\in {\mathbb C} $
$ \,\cos( \omega_0 t)u(t) $ $ \frac{s}{s^2+\omega_0^{2}} $ $ \mathcal{R} \mathfrak{e} \lbrace s \rbrace > 0 $
$ \, \sin( \omega_0 t)u(t) $ $ \frac{\omega_0}{s^2+\omega_0^{2}} $ $ \mathcal{R} \mathfrak{e} \lbrace s \rbrace > 0 $
$ \,e^{-\alpha t}\cos( \omega_0 t) u(t) $ $ \frac{s+\alpha}{(s+\alpha)^{2}+\omega_0^{2}} $ $ \mathcal{R} \mathfrak{e} \lbrace s \rbrace > -\alpha $
$ \, e^{-\alpha t}\sin( \omega_0 t)u(t) $ $ \frac{\omega_0}{(s+\alpha)^{2}+\omega_0^{2}} $ $ \mathcal{R} \mathfrak{e} \lbrace s \rbrace > -\alpha $
$ u_n(t) = \frac{d^{n}\delta (t)}{dt^{n}} $ $ \,\!s^{n} $ $ All\,\, s $
$ u_{-n}(t) = \underbrace{u(t) *\dots * u(t)}_{n\,\,times} $ $ \frac{1}{s^{n}} $ $ \mathcal{R} \mathfrak{e} \lbrace s \rbrace > 0 $

Back to Collective Table

Alumni Liaison

Abstract algebra continues the conceptual developments of linear algebra, on an even grander scale.

Dr. Paul Garrett