Abstract
Based on an analogy between polymer translocation across a free energy barrier associated with polymer worming through a hole and classical nucleation and growth process, the escape time τ is predicted asymptotically to be N(N/ρ)1/3ν. N is the polymer length, ρ is the monomer density prior to escape, and ν is the radius of gyration exponent. Monte Carlo simulation data collected in the high salt limit ( ν3/5) are in agreement with the asymptotic law and provide vivid details of the escape.