In this article, we mainly study the critical points of solutions to the Laplace equation with Dirichlet boundary conditions in an exterior domain in ℝ2. Based on the fine analysis about the structures of connected components of the super-level sets {x ∈ ℝ2 Ω: u(x) > t} and sub-level sets {x ∈ ℝ2 Ω: u(x) < t} for some t, we get the geometric distributions of interior critical point sets of solutions. Exactly, when Ω is a smooth bounded simply connected domain, \(u{|_{\partial \Omega }} = \psi (x),\,\,{\lim _{|x| \to \infty }}u(x) = - \infty \) and ψ(x) has K local maximal points on ∂Ω, we deduce that \(\sum\nolimits_{i = 1}^l {{m_i} \le K} \) , where m1, …, ml; are the multiplicities of interior critical points x1, …, xl; of solution u respectively. In addition, when ψ(x) has only K global maximal points and K equal local minima relative to ℝ2 Ω on ∂Ω, we have that \(\sum\nolimits_{i = 1}^l {{m_i} = K} \) . Moreover, when Ω is a domain consisting of l disjoint smooth bounded simply connected domains, we deduce that \(\sum\nolimits_{{x_i} \in \Omega } {{m_i} + {1 \over 2}} \sum\nolimits_{{x_j} \in \partial \Omega } {{m_j} = l - 1} \) , and the critical points are contained in the convex hull of the l simply connected domains.
