Find the Laplace transform of the following function. f (t) = t^3 H( t − 2) + e^4t H (t − 3)
\[f (t) = t^3 H( t − 2) + e^{4t} H (t − 3)\]\[\mathcal L \{f(t)\}=\]
\[\Large L(f(t-\alpha).H(t-\alpha)) = \int_{0}^{\infty}e^{-st}.f(t-\alpha).H(t-\alpha)dt\]\[\Large = \int_{\alpha}^{\infty}e^{-st}f(t-\alpha)dt\] Taking \(z = t-\alpha \) \[\Large = \int_{0}^{\infty}e^{-s(z+\alpha)}f(z)dz = e^{-s\alpha}\int_{0}^{\infty}e^{-sz}f(z)dz \]\[\Large =e^{-s\alpha}L(f(t)) \]So, what you want to do is to express the given function as a sum of f(t-a).H(t-a) and then apply this relation
H is the heavyside function I take it?
i think so
\[\mathcal L\{u_c(t)g(t)\}=e^{-cs}\mathcal L\{g(t+c)\}\]may work
\(u_c\) is how I write the heaviside function
my book uses \[h(t − a) \]
oh for the heaviside, nvmd
same thing\[h(t-a)=h_a(t)\]
yerh for the unit heavyside step function
these set of lectures (specially the second one might help you with this problem) http://home.iitk.ac.in/~sghorai/TEACHING/MTH203/ode17.pdf http://home.iitk.ac.in/~sghorai/TEACHING/MTH203/ode18.pdf http://home.iitk.ac.in/~sghorai/TEACHING/MTH203/ode19.pdf
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