Trasformate di Laplace più significative
Indichiamo con $\lambda$ l'ascissa di convergenza. Inoltre definiamo

\begin{displaymath}\hbox{erf}\,(t)={\frac{2}{\sqrt\pi}}\int_0^te^{-x^2}\,dx,\qqu...
...ox{erfc}\,(t)={\frac{2}{\sqrt\pi}}\int_t^{+\infty}e^{-x^2}\,dx.\end{displaymath}


(1) \begin{displaymath}F(t),\qquad f(s)={\cal L}(F(t);s)=\int_0^{+\infty}\,e^{-st}f(t)\,dt
\end{displaymath}


(2) \begin{displaymath}G(t)=F(c\,t),\ c>0,\qquad g(s)={\frac{1}{c}}f({\frac{s}{c}}),\qquad\lambda_G=c\,\lambda_F
\end{displaymath}


(3) \begin{displaymath}G(t)=F(t-t_0),\ t_0>0,\qquad g(s)=e^{-t_0s}\,f(s),\qquad \lambda_G=\lambda_F
\end{displaymath}


(4) \begin{displaymath}G(t)=e^{at}F(t),\ a\in\,{\bf C},\qquad g(s)=f(s-a),\qquad \lambda_G=\lambda_F+\hbox{Re}\,a
\end{displaymath}


(5) \begin{displaymath}G(t)=-t\,F(t),\qquad g(s)={\frac{d}{ds}}f(s),\qquad \lambda_G=\lambda_F
\end{displaymath}


(6) \begin{displaymath}G(t)=F'(t),\qquad g(s)=sf(s)-F(0^+),\qquad\lambda_G=\max\{\lambda_F,\lambda_{F'}\}
\end{displaymath}


(7) \begin{displaymath}G(t)=\int_0^tF(\tau)\,d\tau,\qquad g(s)={\frac{f(s)}{s}},\qquad \lambda_G=\max\{0,\lambda_F\}
\end{displaymath}


(8) \begin{displaymath}G(t)={\frac{F(t)}{t}},\qquad g(s)=\int_s^\infty f(\tau)\,d\tau,\qquad \lambda_G=\lambda_F
\end{displaymath}


(9) \begin{displaymath}F(t)=H(t),\hfill\qquad f(s)={\frac{1}{s}},\qquad\lambda=0
\end{displaymath}


(10) \begin{displaymath}F(t)=H(t)e^{\alpha
t},\ \alpha\in\,{\bf
C},\hfill\qquad f(s)={\frac{1}{s-\alpha}},\qquad\lambda=\hbox{Re}\,\alpha
\end{displaymath}


(11) \begin{displaymath}F(t)=H(t)\sin\omega t,\ \omega\in\,{\bf
R},\hfill\qquad f(s)={\frac{\omega}{s^2+\omega^2}},\qquad\lambda=0
\end{displaymath}


(12) \begin{displaymath}F(t)=H(t)\cos\omega t,\ \omega\in\,{\bf
R},\hfill\qquad f(s)={\frac{s}{s^2+\omega^2}},\qquad\lambda=0
\end{displaymath}


(13) \begin{displaymath}F(t)=H(t)\sinh\omega t,\ \omega\in\,{\bf
R},\hfill\qquad f(s)={\frac{\omega}{s^2-\omega^2}},\qquad\lambda=\vert\omega\vert
\end{displaymath}


(14) \begin{displaymath}F(t)=H(t)\cosh\omega t,\ \omega\in\,{\bf
R},\hfill\qquad f(s)={\frac{s}{s^2-\omega^2}},\qquad\lambda=\vert\omega\vert
\end{displaymath}


(15) \begin{displaymath}F(t)=H(t)\,t^n,\ n\in\,{\bf N},\hfill\qquad f(s)={\frac{n!}{s^{n+1}}},\qquad\lambda=0
\end{displaymath}


(16) \begin{displaymath}F(t)=H(t)\,t^\alpha,\
\hbox{Re}\,\alpha>-1,\hfill\qquad f(s)={\frac{\Gamma(\alpha+1)}{s^{\alpha+1}}}
,\qquad\lambda=0
\end{displaymath}


(17) \begin{displaymath}F(t)=H(t)\,e^{-t^2},\hfill\qquad f(s)={\frac{\sqrt\pi}{2}}e^{s^2/4}\hbox{erfc}({\frac{s}{2}})
,\qquad\lambda=-\infty
\end{displaymath}


(18) \begin{displaymath}F(t)=H(t)\,\hbox{erf}(t),\hfill\qquad f(s)={\frac{1}{s}}e^{s^2/4}\hbox{erfc}({\frac{s}{2}}),\qquad\lambda=0
\end{displaymath}


(19) \begin{displaymath}F(t)=H(t)\,\hbox{erf}(\sqrt t),\hfill\qquad f(s)={\frac{1}{s\sqrt{s+1}}},\qquad\lambda=0
\end{displaymath}


(20) \begin{displaymath}F(t)=H(t)\ln t,\hfill\qquad f(s)={\frac{\Gamma'(1)-\log s}{s}},\qquad\lambda=0
\end{displaymath}


(21) \begin{displaymath}F(t)=H(t){\frac{1-e^{-t}}{t}},\hfill\qquad f(s)=\ln(1+{\frac{1}{s}}),\qquad\lambda=0
\end{displaymath}


(22) \begin{displaymath}F(t)=H(t)J_0(t),\hfill\qquad f(s)={\frac{1}{\sqrt{s^2+1}}},\qquad\lambda=0
\end{displaymath}


(23) \begin{displaymath}G(t)=(F_1*F_2)(t),\qquad g(s)=f_1(s)\cdot f_2(s),\qquad \lambda_G=\max\{\lambda_{F_1},\lambda_{F_2}\}
\end{displaymath}


(24) \begin{displaymath}G(t)=H(t)F(t):\ F(t+T)=F(t),\
T>0,\hfill\qquad g(s)={\frac{1}{1-e^{-sT}}}\int_0^Te^{-st}F(t)\,dt,\qquad\lambda=0
\end{displaymath}



 
Ugo Gianazza
2002-01-07