Modeling and analysis of ensemble average solvation energy and solute–solvent interfacial fluctuations

Variational implicit solvation models (VISMs) have gained extensive popularity in the molecular-level solvation analysis of biological systems due to their cost-effectiveness and satisfactory accuracy. Central in the construction of VISM is an interface separating the solute and the solvent. However...

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Main Authors: Shao Yuanzhen, Chen Zhan, Zhao Shan
Format: Article
Language:English
Published: De Gruyter 2024-12-01
Series:Computational and Mathematical Biophysics
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Online Access:https://doi.org/10.1515/cmb-2024-0017
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author Shao Yuanzhen
Chen Zhan
Zhao Shan
author_facet Shao Yuanzhen
Chen Zhan
Zhao Shan
author_sort Shao Yuanzhen
collection DOAJ
description Variational implicit solvation models (VISMs) have gained extensive popularity in the molecular-level solvation analysis of biological systems due to their cost-effectiveness and satisfactory accuracy. Central in the construction of VISM is an interface separating the solute and the solvent. However, traditional sharp-interface VISMs fall short in adequately representing the inherent randomness of the solute–solvent interface, a consequence of thermodynamic fluctuations within the solute–solvent system. Given that experimentally observable quantities are ensemble averaged, the computation of the ensemble average solvation energy (EASE)–the averaged solvation energy across all thermodynamic microscopic states–emerges as a key metric for reflecting thermodynamic fluctuations during solvation processes. This study introduces a novel approach to calculating the EASE. We devise two diffuse-interface VISMs: one within the classic Poisson–Boltzmann (PB) framework and another within the framework of size-modified PB theory, accounting for the finite-size effects. The construction of these models relies on a new diffuse interface definition u(x)u\left(x), which represents the probability of a point xx found in the solute phase among all microstates. Drawing upon principles of statistical mechanics and geometric measure theory, we rigorously demonstrate that the proposed models effectively capture EASE during the solvation process. Moreover, preliminary analyses indicate that the size-modified EASE functional surpasses its counterpart based on the classic PB theory across various analytic aspects. Our work is the first step toward calculating EASE through the utilization of diffuse-interface VISM.
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spelling doaj-art-21d8c32e7ea64026b3e16dcf55f9a1312025-01-20T11:08:25ZengDe GruyterComputational and Mathematical Biophysics2544-72972024-12-011211374310.1515/cmb-2024-0017Modeling and analysis of ensemble average solvation energy and solute–solvent interfacial fluctuationsShao Yuanzhen0Chen Zhan1Zhao Shan2Department of Mathematics, The University of Alabama, Tuscaloosa, AL, 35401, United States of AmericaDepartment of Mathematical Sciences, Georgia Southern University, GA, 30458, United States of AmericaDepartment of Mathematics, The University of Alabama, Tuscaloosa, AL, 35401, United States of AmericaVariational implicit solvation models (VISMs) have gained extensive popularity in the molecular-level solvation analysis of biological systems due to their cost-effectiveness and satisfactory accuracy. Central in the construction of VISM is an interface separating the solute and the solvent. However, traditional sharp-interface VISMs fall short in adequately representing the inherent randomness of the solute–solvent interface, a consequence of thermodynamic fluctuations within the solute–solvent system. Given that experimentally observable quantities are ensemble averaged, the computation of the ensemble average solvation energy (EASE)–the averaged solvation energy across all thermodynamic microscopic states–emerges as a key metric for reflecting thermodynamic fluctuations during solvation processes. This study introduces a novel approach to calculating the EASE. We devise two diffuse-interface VISMs: one within the classic Poisson–Boltzmann (PB) framework and another within the framework of size-modified PB theory, accounting for the finite-size effects. The construction of these models relies on a new diffuse interface definition u(x)u\left(x), which represents the probability of a point xx found in the solute phase among all microstates. Drawing upon principles of statistical mechanics and geometric measure theory, we rigorously demonstrate that the proposed models effectively capture EASE during the solvation process. Moreover, preliminary analyses indicate that the size-modified EASE functional surpasses its counterpart based on the classic PB theory across various analytic aspects. Our work is the first step toward calculating EASE through the utilization of diffuse-interface VISM.https://doi.org/10.1515/cmb-2024-0017biomolecule solvationpoisson–boltzmannvariational implicit solvation modelensemble average solvation energyfinite size effectprimary: 49q10secondary: 35j2092c40
spellingShingle Shao Yuanzhen
Chen Zhan
Zhao Shan
Modeling and analysis of ensemble average solvation energy and solute–solvent interfacial fluctuations
Computational and Mathematical Biophysics
biomolecule solvation
poisson–boltzmann
variational implicit solvation model
ensemble average solvation energy
finite size effect
primary: 49q10
secondary: 35j20
92c40
title Modeling and analysis of ensemble average solvation energy and solute–solvent interfacial fluctuations
title_full Modeling and analysis of ensemble average solvation energy and solute–solvent interfacial fluctuations
title_fullStr Modeling and analysis of ensemble average solvation energy and solute–solvent interfacial fluctuations
title_full_unstemmed Modeling and analysis of ensemble average solvation energy and solute–solvent interfacial fluctuations
title_short Modeling and analysis of ensemble average solvation energy and solute–solvent interfacial fluctuations
title_sort modeling and analysis of ensemble average solvation energy and solute solvent interfacial fluctuations
topic biomolecule solvation
poisson–boltzmann
variational implicit solvation model
ensemble average solvation energy
finite size effect
primary: 49q10
secondary: 35j20
92c40
url https://doi.org/10.1515/cmb-2024-0017
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AT chenzhan modelingandanalysisofensembleaveragesolvationenergyandsolutesolventinterfacialfluctuations
AT zhaoshan modelingandanalysisofensembleaveragesolvationenergyandsolutesolventinterfacialfluctuations