In this paper, we study the isotropic-nematic phase transition for the nematic liquid crystal based on the Landau-de Gennes-tensor theory. We justify the limit from the Landau-de Gennes flow to a sharp interface model: in the isotropic region, ≡ 0 ; in the nematic region, the-tensor is constrained on the manifolds = {s + (⊗ − 1 3), ∈ 2 } with s + a positive constant, and the evolution of alignment vector field obeys the harmonic map heat flow, while the interface separating the isotropic and nematic regions evolves by the mean curvature flow. This problem can be viewed as a concrete but representative case of the Rubinstein-Sternberg-Keller problem introduced in Rubinstein et al.