I'm trying to solve this Laplace problem from Laplace Transform by Schaum's Outline, chapter 1, math 167(a). But no matter what approach I follow, I end up with this line:
$L(\frac{1-\cos t}{t^2}) = \frac{\pi}{2} + \frac{1}{2}s\ln(\frac{s^2}{s^2+1}) - \tan^{-1}(s)$
And by definition, $L(\frac{1-\cos t}{t^2}) = \int_0^{\infty} e^{-st} (\frac{1-\cos t}{t^2})dt$
So I've no idea why and how the problem expects me to end up from $\frac{\pi}{2} + \frac{1}{2}s\ln(\frac{s^2}{s^2+1}) - \tan^{-1}(s)$ to $\frac{\pi}{2} - s\ln(\frac{s^2}{s^2+1}) + 2\tan^{-1}(s)$
Looking for your kind help.
You have to use $$ L\bigg\{\frac{f(t)}{t}\bigg\}=\int_s^\infty F(\tau)d\tau $$ twice, where $F(s)=L\{f(t)\}$. Let $f(t)=\frac{1-\cos t}{t}$ and then \begin{eqnarray} F(s)=L\{f(t)\}&=&\int_s^\infty L\{1-\cos t\}(\tau)d\tau=\int_s^\infty\bigg(\frac1\tau-\frac{\tau}{\tau^2+1}\bigg)d\tau\\ &=&\frac12\ln\bigg(\frac{\tau^2}{\tau^2+1}\bigg)\bigg|_s^\infty=-\frac12\ln\bigg(\frac{s^2}{s^2+1}\bigg). \end{eqnarray} So \begin{eqnarray} L\bigg\{\frac{1-\cos t}{t^2}\bigg\}&=&L\bigg\{\frac{f(t)}{t}\bigg\}=\int_s^\infty F(\tau)d\tau\\ &=&-\frac12\int_s^\infty \ln\bigg(\frac{\tau^2}{\tau^2+1}\bigg)d\tau\\ &=&\cdots \end{eqnarray} You finish the rest.