Solvent Structure, Dynamics, and Ion Mobility in Aqueous Solutions at 25 °C
Abstract
We calculate the mobilities u i of the metal cations Li +, Na +, K +, Rb +, Cs +, and Ca 2+ and the halides F -, Cl -, Br -, and I - at infinite dilution by molecular dynamics simulation using the SPC/E model for water at 25 °C and a reaction field for the long-range interactions. The ion mobilities show the same trends as the experimental results with distinct maxima for cations and anions. The mobilities (defined by u i = D i / kT ) of the corresponding uncharged species are also determined by simulation and are in qualitative agreement with Stokes' law. The mobilities of Li +, Na +, K +, Rb + and F - increase on discharge, whereas Cl, Br, and I have smaller mobilities than the corresponding anions. The mobility of the fictitious I + ion, which differs from I - only in its charge, lies between that of I - and I in the order u I < u I + < u I − . The residence time of water in the first solvation shell of small cations (Li + and Na + ) and Ca 2+ decreases when the ions are discharged, while the opposite is observed on neutralizing I -, suggesting the formation of a solvent cage around the large uncharged I which partially breaks up on charging, increasing the mobility of the corresponding ion. The cage breakup is greater for I - than for I + which correlates with the asymmetry in the entropies of solvation of I - and I +, in SPC/E water on charge reversal, providing an explanation for the trends in the mobilities of I, I -, and I + . The residence times of water in the primary hydration shell around cations pass through a minimum as a function of size that correlates with the maximum in the corresponding solvation entropy, suggesting different types of hydration, i.e., electrostatic ion solvation (hydrophilic) and cage formation (hydrophobic) respectively for small and large cations. The results are in accord with recent calculations of the solvation entropy and free energy as continuous functions of the charge and size (Lynden-Bell, R. M.; Rasaiah, J. C. J. Chem. Phys. 1997, 107, 1981). Hydrophilic and hydrophobic solvation are reflected in the exchange dynamics of the water in the hydration shells around charged and uncharged solutes. The solvation dynamics of individual cations and anions are distinct at short times but characterized by the solvent at long times. Solvent dynamics, structure, and caging modulated by the charge and size of the ions are strongly implicated in determining their mobilities.
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By replacing the electrolyte solution with an intrinsic semiconductor, the electrostatic solution of the electrolyte region can be calculated by solving the semiconductor equations within that region.
“By replacing the electrolyte solution with an intrinsic semiconductor, the electrostatic solution of the electrolyte region can therefore be calculated by solving the semiconductor equations within this region.”
From Numerical simulation of ISFET structures for biosensing devices with TCAD tools (2015) · cites this paper as [8]
The Poisson-Boltzmann equation describing charge distribution in the electric double layer can be viewed as the semiconductor equation applied to an intrinsic material.
“With this approximation the Poisson-Boltzmann (PB) equation, describing the charge distribution in the electric double layer, can be viewed as the semiconductor equation applied to an intrinsic material [8].”
From Numerical simulation of ISFET structures for biosensing devices with TCAD tools (2015) · cites this paper as [8]
The adopted simulation scheme has been used for the analysis of conventional biosensors such as Silicon NanoWires (SiNW) on a larger scale.
“We adopted a simulation scheme which has been used for the analysis of”
From Numerical simulation of ISFET structures for biosensing devices with TCAD tools (2015) · cites this paper as [8]
The sensitivity of the segmented ISFET is in agreement with simulation findings obtained in [8], even for small localized charges at bigger distance from the conductive channel.
“Actually, its sensitivity is in agreement with simulation findings obtained in [8], even for small localized charges at bigger distance from the conductive channel.”
From Numerical simulation of ISFET structures for biosensing devices with TCAD tools (2015) · cites this paper as [8]
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- Authors
- Koneshan, S., Rasaiah, J. C., Lynden-Bell, R. M., & Lee, S. H.
- Affiliations
- Kyungsung University (KR)
- Venue
- The Journal of Physical Chemistry B
- Publisher
- American Chemical Society (ACS)
- Published
- 1998-05-01
- Volume
- 102
- Issue
- 21
- Pages
- 4193-4204
- ISSN
- 1520-5207 (ISSN-L)
- 1520-6106
- OpenAlex
- W2052737939
- Cited by
- 965
- References
- 0
- Citations by year
- 2026: 24 · 2025: 36 · 2024: 29 · 2023: 33 · 2022: 38 · 2021: 35 · 2020: 37 · 2019: 53 · 2018: 33 · 2017: 31 · 2016: 34 · 2015: 36 · 2014: 54 · 2013: 45 · 2012: 56
- FWCI
- 11.26
- Type
- journal article
- Language
- en
- Open access
- closed
- Locations
- The Journal of Physical Chemistry B (publishedVersion)
- Topics
- Physical Sciences › Physics and Astronomy › Atomic and Molecular Physics, and Optics › Spectroscopy and Quantum Chemical Studies
- Physical Sciences › Chemistry › Physical and Theoretical Chemistry › Advanced Physical and Chemical Molecular Interactions
- Physical Sciences › Physics and Astronomy › Atomic and Molecular Physics, and Optics › Advanced Chemical Physics Studies
- Keywords
- ion mobility, aqueous solutions, SPC/E water model, solvation entropy, ion solvation, hydrophobic solvation, halide ions, alkali metal cations, calcium cations, iodide, charge reversal, Stokes' law, water exchange dynamics, reaction field
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