I am using the book Classical Dynamics of Particles and Systems by STEPHEN T. THORNTON, JERRY B. MARION, page: 67 and they use perturbation method to approximate: \begin{equation} T = \frac{kV + g}{gk}(1-e^{-kT}) \end{equation}
they first expand $-e^{-kT}$ to the third power for $k$, (hence $k^3$) thus we get: \begin{equation} T = \frac{kV + g}{gk}(kT-\frac{1}{2}k^2T^2 + \frac{1}{6}k^3T^3-\dots)\end{equation}
they let $k$ be small and thus from equation above makes sense because $k$ is small, larger the $n$ for $k^n$ the approximation becomes more an more accurate as $k^n \to 0$ Thus getting: \begin{equation} T = \frac{\frac{2V}{g}}{1+\frac{kV}{g}} +\frac{1}{3}kT^2 \end{equation} But then they go on to expand (below) to $k^2$ only \begin{equation} \frac{1}{1+\frac{kV}{g}}=1-(kV/g)+(kV/g)^2 -\dots\end{equation}
then they rearrange to get: \begin{equation}T = \frac{2V}{g}+(\frac{T^2}{3}-\frac{2V^2}{g^2})k+O(k^2) \end{equation}
then they discard $O(k^2)$
$\textbf{My Question:}$ I understand why they discarded $O(k^4)$ initially but then they seem to keep discarding and at different $O(k^n)$ as we move through the steps. I would like to know if there is some order to this discarding of terms. like why not do all at $O(k^4)$?