In the Lagrangian formalism with a dissipative frictional force $F$, we can write
$$\frac{d}{dt}\frac{\partial\mathcal{L}}{\partial\dot{q}_{k}}-\frac{\partial\mathcal{L}}{\partial q_{k}}=Q^{(nc)}_{k}$$
where I have indicated the generalised force
$$Q^{(nc)}_{k}(\mathbf{q} )=\frac{\partial r_{j}(\mathbf{q})}{\partial q_{k}}\ F_j(\mathbf{\dot{r}})$$
and '$nc$' stands for non-conservative.
Let us assume that the system is driven by some conservative forces $\bf Q^{(c)}$ such that $$Q_k^{(c)}=-\frac{\partial U}{\partial q_k}$$ where $U$ is the internal energy.
In the paper below, the system has no inertial forces ($Re=0$) and once they have determined $\bf q$, $\partial r_{j}/\partial q_j(\mathbf{q})$ and $F_j(\mathbf{r})$ they go straight onto solving the following force balance $$Q_k^{(c)}=Q_k^{(nc)}.$$ Why?
Reference
Polotzek, Katja, and Benjamin M Friedrich. “A Three-Sphere Swimmer for Flagellar Synchronization.” New Journal of Physics 15, no. 4 (April 10, 2013): 045005. https://doi.org/10.1088/1367-2630/15/4/045005.
Fragment of interest