“…Also, the pressure of the polymer phase, P 0 , corresponding to the temperature and the equilibrium density of water, is known from the results of such a simulation. The chemical potential of water in polymer phase is then calculated from the target excess chemical potential, m ex w,p (T, P 0 ), via eqn (3) and expanded in terms of pressure [33][34][35]37 as a first-order Taylor series, i.e., where V w,p is the partial molar volume of water in polymer phase, P is the equilibrium pressure (unknown), and P 0 is the pressure obtained from in the grand canonical ensemble simulation of the polymer phase. Following the procedure outlined in our previous publication, 35 another simulation, in the grand canonical ensemble, for water in the gas phase is done.…”