Find $$\sum_{n=1}^\infty \tan^{-1} \left(\frac{3}{n^2 + n - 1}\right)$$
I know this can be simplified to a telescoping series of the form
$$\sum_{n=1}^\infty\tan^{-1}(n+2) - \tan^{-1}(n-1)$$
The correct answer, on evaluating the limit for this would be,
$\tan^{-1} (n+2) + \tan^{-1} (n+1) +\tan^{-1} (n)- \tan^{-1} 0 - \tan^{-1} (1) - \tan^{-1} (2) =\frac{ 3\pi}4 - \cot^{-1} 2$
But when summing to infinity why do we have remanent $\tan^{-1} (n+2) + \tan^{-1} (n+1) +\tan^{-1} (n)$ since for every $ \tan^{-1} n$ we would have a $-\tan^{-1} n$. Something similar to the argument how set of natural numbers and integers is equal $(n(N) = n(I))$.
In problems I've done before the telescoping sum usually tends to 0 so I might be thinking of it in the wrong way.
What you did is the partial sum
$$\begin{align}S_n&=\sum_{k=1}^n \tan^{-1} \left(\frac{3}{k^2 + k - 1} \right)\\ \\ S_n&=\tan^{-1} (n+2) + \tan^{-1} (n+1) +\tan^{-1} (n)- \tan^{-1} 0 - \tan^{-1} (1) - \tan^{-1} (2)\end{align}$$
the series equals the limit of the partial sum, namely
$$\sum_{k=1}^\infty \tan^{-1} \left(\frac{3}{k^2 + k - 1} \right)=\lim_{n\to\infty}S_n=\frac{5\pi}4 - \tan^{-1} (2)$$