$\mathscr{L}\{\delta'(t-1)\}=F(s) $
Im having a hard time thinking this.
My first thought was doing $F(s) =e^{-s} s$
But when i do the inverse laplace transform of this i get
$f(t)= \delta'(t-1) Heaviside(t-1)$
$\mathscr{L}\{\delta'(t-1)\}=F(s) $
Im having a hard time thinking this.
My first thought was doing $F(s) =e^{-s} s$
But when i do the inverse laplace transform of this i get
$f(t)= \delta'(t-1) Heaviside(t-1)$
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I also think that the Laplace transform of $\delta'(t-1)$ is $s e^{-s}.$ Formally we have: $$ \mathscr{L}\{\delta'(t-1)\} = \int_0^\infty \delta'(t-1) \, e^{-st} \, dt \\ = \underbrace{\left[ \delta(t-1) \, e^{-st} \right]_0^\infty}_{=0} - \int_0^\infty \delta(t-1) \, (-s) e^{-st} \, dt \\ = s \int_0^\infty \delta(t-1) \, e^{-st} \, dt = s e^{-s\cdot 1} = s e^{-s} $$