Monte Carlo simulation strategies for computing the wetting properties of fluids at geometrically rough surfaces J. Chem. Phys. 135, 184702 (2011) Semi-bottom-up coarse graining of water based on microscopic simulations J. Chem. Phys. 135, 184101 (2011) Hydrophobic interactions in presence of osmolytes urea and trimethylamine-N-oxide J. Chem. Phys. 135, 174501 (2011) Potential of mean force between identical charged nanoparticles immersed in a size-asymmetric monovalent electrolyte J. Chem. Phys. 135, 164705 (2011) Additional information on J. Chem. Phys. Thermodynamics, equilibrium structure, and dynamics of glass-forming liquids Ca͑NO 3 ͒ 2 · nH 2 O, n = 4, 6, and 8, have been investigated by molecular dynamics ͑MD͒ simulations. A polarizable model was considered for H 2 O and NO 3 − on the basis of previous fluctuating charge models for pure water and the molten salt 2Ca͑NO 3 ͒ 2 · 3KNO 3 . Similar thermodynamic properties have been obtained with nonpolarizable and polarizable models. The glass transition temperature, T g , estimated from MD simulations was dependent on polarization, in particular the dependence of T g with electrolyte concentration. Significant polarization effects on equilibrium structure were observed in cation-cation, cation-anion, and water-water structures. Polarization increases the diffusion coefficient of H 2 O, but does not change significantly the diffusion coefficients of ions. Viscosity decreases upon inclusion of polarization, but the conductivity calculated with the polarizable model is smaller than the nonpolarizable model because polarization enhances anion-cation interactions.