If someone could help me solve for $$\mathcal{L}\left\{\frac{\cos(at)}{t}\right\}$$ it would be great.
Step-by-step I have so far:
$$\begin{align}\int_0^\infty \frac{\cos(at)\space e^{-st}}{t}\space\text{d}s &= \int_s^\infty \frac{s}{s^2+a^2}\space\text{d}s \\ &= \frac{1}{2} \int_s^\infty \frac{2s}{s^2+a^2}\space\text{d}s \\ \end{align}$$ Help me after this step please
Maybe I am misunderstanding something, but the integral should be in $t$, right? Ordinarily, if we have a function $f(t)$, the Laplace transform is $$(\mathcal Lf)(s) = \int^\infty_0 f(t) e^{-st} dt.$$ Here, because of the behavior near $t =0$, we see that the integral $$\int_0^\infty \frac{\cos(at)}{t} e^{-st} dt$$ doesn't converge. Indeed, for small $\varepsilon > 0$, we see by Taylor expansion that $$\int^\varepsilon_0 \frac{\cos(at)}{t} e^{-st} dt \approx \int^\varepsilon_0 \frac 1 t dt$$ which diverges.