Abstract. We propose a new weighted weak formulation for the Fokker-Planck equation of the finitely extensible nonlinear elastic dumbbell model and prove its well-posedness in weighted Sobolev spaces. We also propose simple and efficient semi-implicit time-discretization schemes which are unconditionally stable, i.e., the step size of time marching does not depend on the number of the bases used in configurational space. We then restrict ourselves to the two-dimensional case and construct two Fourier-Jacobi spectral-Galerkin algorithms which enjoy the following properties: (i) they are unconditionally stable, spectrally accurate, and of optimal computational complexity; (ii) they conserve the volume and provide accurate approximation to higher-order moments of the distribution function; and (iii) they can be easily extended to coupled nonhomogeneous systems. Numerical results are presented to show how to choose a proper weight to get the best numerical results of the distribution function and the polymer stress. 1. Introduction. The finitely extensible nonlinear elastic (FENE) dumbbell model (cf., for instance, [30,11,29] and the references therein) is a well-known coarsegrained model for dilute polymer solutions in which every polymer molecule is modeled by a dumbbell.Let r 1 and r 2 be the position of the two beads of a dumbbell; then the center of the molecule is x = (r 1 +r 2 )/2, and the direction vector of the molecule is q = r 2 −r 1 . In kinetic theory, a configurational distribution function (CDF) f (t, x, q) is used to describe the probability density of finding a molecule at position x and at time t with orientational director q. Then, the whole polymer solutions in the background of macroscopic flow field can be described by a macroscopic-mesoscopic coupled system which consists of the Navier-Stokes equations