MHB Alexander's question via email about Laplace Transforms

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The evaluation of the Laplace Transform involves the Heaviside function, indicating a shift in the function. By substituting \( u = t - 4 \), the expression simplifies to \( e^{20} e^{5(t - 4)} \). Applying the second shift theorem leads to \( e^{20 - 4s} \) multiplied by the Laplace Transform of \( \sin(6t) e^{5t} \). The final result incorporates the first shift theorem, yielding \( e^{20 - 4s} \left[ \frac{6}{(s - 5)^2 + 36} \right] \). The calculations confirm the correctness of the evaluation.
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Evaluate $\displaystyle \mathcal{L}\left\{ H\left( t - 4 \right) \sin{ \left[ 6 \left( t - 4 \right) \right] } \,\mathrm{e}^{5\,t} \right\} $

The Heaviside function suggests a second shift, but to do that, the entire function needs to be a function of $\displaystyle t - 4$.

Let $\displaystyle u = t - 4 \implies t = u + 4$, then

$\displaystyle \begin{align*} \mathrm{e}^{5\,t} &= \mathrm{e}^{5\left( u + 4 \right) } \\ &= \mathrm{e}^{5\,u + 20} \\
&= \mathrm{e}^{5\left( t - 4 \right) + 20} \\ &= \mathrm{e}^{20}\,\mathrm{e}^{5\left( t - 4 \right) } \end{align*}$

So

$\displaystyle \begin{align*} \mathcal{L}\left\{ H \left( t - 4 \right) \sin{\left[ 6\left( t - 4 \right) \right] } \,\mathrm{e}^{5\,t} \right\} &= \mathrm{e}^{20}\,\mathcal{L}\left\{ H\left( t - 4 \right) \sin{ \left[ 6\left( t - 4 \right) \right] }\, \mathrm{e}^{5\left( t - 4 \right) } \right\} \\ &= \mathrm{e}^{20}\,\mathrm{e}^{-4\,s} \,\mathcal{L} \left\{ \sin{ \left( 6\,t \right) }\, \mathrm{e}^{5\,t} \right\} \textrm{ by the second shift theorem} \\ &= \mathrm{e}^{20 - 4\,s } \left[ \frac{6}{s^2 + 6^2} \right] _{s \to s - 5} \textrm{ by the first shift theorem} \\ &= \mathrm{e}^{20 - 4\,s} \left[ \frac{6}{\left( s - 5 \right) ^2 + 36} \right] \end{align*}$
 
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