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Hydrodynamic and Nonhydrodynamic Contributions to the Bimolecular Collision Rates of Solute Molecules in Supercooled Bulk Water
[Image: see text] Bimolecular collision rate constants of a model solute are measured in water at T = 259–303 K, a range encompassing both normal and supercooled water. A stable, spherical nitroxide spin probe, perdeuterated 2,2,6,6-tetramethyl-4-oxopiperidine-1-oxyl, is studied using electron param...
Autores principales: | , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
American Chemical
Society
2014
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Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4076007/ https://www.ncbi.nlm.nih.gov/pubmed/24874024 http://dx.doi.org/10.1021/jp501330x |
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author | Peric, Ida Merunka, Dalibor Bales, Barney L. Peric, Miroslav |
author_facet | Peric, Ida Merunka, Dalibor Bales, Barney L. Peric, Miroslav |
author_sort | Peric, Ida |
collection | PubMed |
description | [Image: see text] Bimolecular collision rate constants of a model solute are measured in water at T = 259–303 K, a range encompassing both normal and supercooled water. A stable, spherical nitroxide spin probe, perdeuterated 2,2,6,6-tetramethyl-4-oxopiperidine-1-oxyl, is studied using electron paramagnetic resonance spectroscopy (EPR), taking advantage of the fact that the rotational correlation time, τ(R), the mean time between successive spin exchanges within a cage, τ(RE), and the long-time-averaged spin exchange rate constants, K(ex), of the same solute molecule may be measured independently. Thus, long- and short-time translational diffusion behavior may be inferred from K(ex) and τ(RE), respectively. In order to measure K(ex), the effects of dipole–dipole interactions (DD) on the EPR spectra must be separated, yielding as a bonus the DD broadening rate constants that are related to the dephasing rate constant due to DD, W(dd). We find that both K(ex) and W(dd) behave hydrodynamically; that is to say they vary monotonically with T/η or η/T, respectively, where η is the shear viscosity, as predicted by the Stokes–Einstein equation. The same is true of the self-diffusion of water. In contrast, τ(RE) does not follow hydrodynamic behavior, varying rather as a linear function of the density reaching a maximum at 276 ± 2 K near where water displays a maximum density. |
format | Online Article Text |
id | pubmed-4076007 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2014 |
publisher | American Chemical
Society |
record_format | MEDLINE/PubMed |
spelling | pubmed-40760072015-05-29 Hydrodynamic and Nonhydrodynamic Contributions to the Bimolecular Collision Rates of Solute Molecules in Supercooled Bulk Water Peric, Ida Merunka, Dalibor Bales, Barney L. Peric, Miroslav J Phys Chem B [Image: see text] Bimolecular collision rate constants of a model solute are measured in water at T = 259–303 K, a range encompassing both normal and supercooled water. A stable, spherical nitroxide spin probe, perdeuterated 2,2,6,6-tetramethyl-4-oxopiperidine-1-oxyl, is studied using electron paramagnetic resonance spectroscopy (EPR), taking advantage of the fact that the rotational correlation time, τ(R), the mean time between successive spin exchanges within a cage, τ(RE), and the long-time-averaged spin exchange rate constants, K(ex), of the same solute molecule may be measured independently. Thus, long- and short-time translational diffusion behavior may be inferred from K(ex) and τ(RE), respectively. In order to measure K(ex), the effects of dipole–dipole interactions (DD) on the EPR spectra must be separated, yielding as a bonus the DD broadening rate constants that are related to the dephasing rate constant due to DD, W(dd). We find that both K(ex) and W(dd) behave hydrodynamically; that is to say they vary monotonically with T/η or η/T, respectively, where η is the shear viscosity, as predicted by the Stokes–Einstein equation. The same is true of the self-diffusion of water. In contrast, τ(RE) does not follow hydrodynamic behavior, varying rather as a linear function of the density reaching a maximum at 276 ± 2 K near where water displays a maximum density. American Chemical Society 2014-05-29 2014-06-26 /pmc/articles/PMC4076007/ /pubmed/24874024 http://dx.doi.org/10.1021/jp501330x Text en Copyright © 2014 American Chemical Society Terms of Use (http://pubs.acs.org/page/policy/authorchoice_termsofuse.html) |
spellingShingle | Peric, Ida Merunka, Dalibor Bales, Barney L. Peric, Miroslav Hydrodynamic and Nonhydrodynamic Contributions to the Bimolecular Collision Rates of Solute Molecules in Supercooled Bulk Water |
title | Hydrodynamic
and Nonhydrodynamic Contributions to
the Bimolecular Collision Rates of Solute Molecules in Supercooled
Bulk Water |
title_full | Hydrodynamic
and Nonhydrodynamic Contributions to
the Bimolecular Collision Rates of Solute Molecules in Supercooled
Bulk Water |
title_fullStr | Hydrodynamic
and Nonhydrodynamic Contributions to
the Bimolecular Collision Rates of Solute Molecules in Supercooled
Bulk Water |
title_full_unstemmed | Hydrodynamic
and Nonhydrodynamic Contributions to
the Bimolecular Collision Rates of Solute Molecules in Supercooled
Bulk Water |
title_short | Hydrodynamic
and Nonhydrodynamic Contributions to
the Bimolecular Collision Rates of Solute Molecules in Supercooled
Bulk Water |
title_sort | hydrodynamic
and nonhydrodynamic contributions to
the bimolecular collision rates of solute molecules in supercooled
bulk water |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4076007/ https://www.ncbi.nlm.nih.gov/pubmed/24874024 http://dx.doi.org/10.1021/jp501330x |
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