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The Planck–Benzinger thermal work function in the condensation of water vapor

Authors

  • Paul W. Chun

    Corresponding author
    1. Department of Biochemistry and Molecular Biology, University of Florida College of Medicine, Gainesville, Florida 32610-0245
    • Department of Biochemistry and Molecular Biology, University of Florida College of Medicine, Gainesville, Florida 32610-0245
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Abstract

Based on the Planck–Benzinger thermal work function using Chun's method, the innate temperature-invariant enthalpy at 0 K, ΔH0(T0), for the condensation of water vapor as well as the dimer, trimer, tetramer, and pentamer form in the vapor phase, was determined to be 0.447 kcal mol−1 for vapor, 1.127 for the dimer, 0.555 for the trimer, 0.236 for the tetramer, and 0.079 kcal mol−1 for the pentamer using ΔG(T) data reported by Kell et al. in 1968 and Kell and McLaurin in 1969. These results suggest that the predominant dimeric form is the most stable of these n-mers. Using Nemethy and Scheraga's 1962 data for the Helmholtz free energy of liquid water, the value of ΔH0(T0) was determined to be 1.21 kcal mol−1. This is very close to the value for the energy of the hydrogen bond EH of 1.32 kcal mol−1 reported by Nemethy and Scheraga, using statistical thermodynamics. It seems clear that very little energy is required for interconversion between the hypothetical supercooled water vapor and glassy water at 0 K. A hypothetical supercooled water vapor at 0 K is apparently almost as highly associated as glassy water at that temperature, suggesting a dynamic equilibrium between vapor and liquid. This water vapor condensation is highly similar in its thermodynamic behavior to that of sequence-specific pairwise (dipeptide) hydrophobic interaction, except that the negative Gibbs free energy change minimum at 〈Ts〉, the thermal setpoint for vapor condensation, where TΔS = 0, occurs at a considerably lower temperature, 270 K (below 0°C) compared with ∼350 K. The temperature of condensation 〈Tcond〉 at which ΔG(T) = 0, where water vapor begins to condense, was found to be 383 K. In the case of a sequence-specific pairwise hydrophobic interaction, the melting temperature, 〈Tm〉, where ΔG(Tm) = 0 was found to be 460 K. Only between two temperature limits, 〈Th〉 = 99 K and 〈Tcond〉 = 383 K, where ΔG(Tcond) = 0, is the net chemical driving force favorable for polymorphism of glassy water and hypothetical supercooled water vapor. Analysis of the water vapor condensation process based on the Planck–Benzinger thermal work function confirms that a thermodynamic molecular switch occurs at 10 K, wherein a change of sign in [ΔCp(T)]cond leads to a true negative minimum in the Gibbs free energy of vapor condensation, and hence a maximum in the related equilibrium constant, Kcond. © 2006 Wiley Periodicals, Inc. Int J Quantum Chem, 2006

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