Suppose I have a system of differential equations for the unknowns $(x_1,v_1,\ldots,x_N,v_N)$ (interpreted as the positions & velocities of $N$ labeled particles), $$\begin{cases}\dot{x}_{i,\epsilon} = v_{i,\epsilon} \\ \dot{v}_{i,\epsilon} = \displaystyle-\frac{1}{\epsilon}\sum_{1\leq j\leq N} \nabla W(x_{i,\epsilon}-x_{j,\epsilon}) \\ (x_{i,\epsilon},v_{i,\epsilon})\vert_{t=0} = (x_i^0,v_i^0), \end{cases} \qquad 1\leq i\leq N. \tag{1}$$ Above, $\epsilon>0$ is small parameter, and for simplicity, let's assume that the positions $x_{i,\epsilon}\in \mathbb{T}^d$ ($[-\frac12,\frac12]^d$ with periodic boundary conditions) and $v_{i,\epsilon}\in\mathbb{R}^d$. $W$ is some function, the exact form is not so important for formulating the question.
Multiplying both sides of the second equation by $\epsilon$ and sending $\epsilon\rightarrow 0$, I would formally expect that $(x_{i,\epsilon},v_{i,\epsilon})_{i=1}^N$ to converge to a solution $(x_i,v_i)_{i=1}^N$ of the system. $$\begin{cases}\dot{x}_i = v_i \\ \displaystyle0 = -\sum_{1\leq j\leq N}\nabla W(x_i-x_j) \\ (x_i,v_i)\vert_{t=0} = (x_i^0,v_i^0), \end{cases} \qquad 1\leq i\leq N.\tag{2}$$ Introducing the potential energy $$P = \frac12\sum_{1\leq i,j\leq N} W(x_i-x_j),$$ the second equation of (2) says that $(x_i)_{i=1}^N$ is a critical point of $P$ for all time. So the $N$ particles are just translated in space through the set of critical points of the potential energy.
I'm interested in references that have studied these singular limit problems and, in particular, the assumptions on $W$ needed to show convergence.