Localization and transformation of physically significant modes in relaxation of ensembles of spherical and cylindrical micelles

Standard

Localization and transformation of physically significant modes in relaxation of ensembles of spherical and cylindrical micelles. / Adzhemyan, Loran Ts.; Eroshkin, Yu A.; Shchekin, A. K.

In: Physica A: Statistical Mechanics and its Applications, Vol. 572, 125912, 01.06.2021.

Research output: Contribution to journal › Article › peer-review

BibTeX

@article{70e0c93498e7470a987143566f2ebfb5,

title = "Localization and transformation of physically significant modes in relaxation of ensembles of spherical and cylindrical micelles",

abstract = "A general picture of relaxation in micellar solution of nonionic one-component surfactant on the basis of numerical solution of linearized set of the Becker–D{\"o}ring equations for spherical and for cylindrical micelles has been analyzed in the form of a series in eigenvectors of the matrix of the kinetic coefficients. Two general characteristic cases have been considered as the initial conditions, the addition of monomers to the equilibrium system and the dilution of the equilibrium system. In both cases, the significant eigenvectors (relaxation modes) have been localized in the space of the aggregation numbers, that are responsible for the stages of ultrafast, fast, and slow relaxation, and corresponding eigenvalues (inverse relaxation times) have been selected from the huge number of all eigenvalues of the matrix of the kinetic coefficients. The analytical methods for finding the relaxation times of the ultrafast, fast and slow relaxation, recently developed and new ones proposed in this article, have been considered. The accuracy of the analytical calculations was controlled by comparison with much more resource-intensive computations using the matrix of the linearized equation. The analytical determination of the fast relaxation modes was based on the transition to the continual boundary-value problem with the potential for the distribution function of micelles over the aggregation numbers and using the perturbation theory. The spectrum was found numerically using the Runge–Kutta method. A new analytical solution for fast relaxation of the ensemble of cylindrical micelles with physically sound coefficients of monomer attachment to cylindrical micelles has been found with reducing the boundary value problem for the differential Becker–D{\"o}ring–Frenkel equation to the equation for the Airy function.",

keywords = "Micellization kinetics, Becker–D{\"o}ring equations, Relaxation modes and times, Micellization kinetics, Becker–D{\"o}ring equations, Relaxation modes and times, The Becker–D{\"o}ring equations",

author = "Adzhemyan, {Loran Ts.} and Eroshkin, {Yu A.} and Shchekin, {A. K.}",

note = "Publisher Copyright: {\textcopyright} 2021 Elsevier B.V.",

year = "2021",

month = jun,

day = "1",

doi = "10.1016/j.physa.2021.125912",

language = "English",

volume = "572",

journal = "Physica A: Statistical Mechanics and its Applications",

issn = "0378-4371",

publisher = "Elsevier",

}

RIS

TY - JOUR

T1 - Localization and transformation of physically significant modes in relaxation of ensembles of spherical and cylindrical micelles

AU - Adzhemyan, Loran Ts.

AU - Eroshkin, Yu A.

AU - Shchekin, A. K.

PY - 2021/6/1

Y1 - 2021/6/1

N2 - A general picture of relaxation in micellar solution of nonionic one-component surfactant on the basis of numerical solution of linearized set of the Becker–Döring equations for spherical and for cylindrical micelles has been analyzed in the form of a series in eigenvectors of the matrix of the kinetic coefficients. Two general characteristic cases have been considered as the initial conditions, the addition of monomers to the equilibrium system and the dilution of the equilibrium system. In both cases, the significant eigenvectors (relaxation modes) have been localized in the space of the aggregation numbers, that are responsible for the stages of ultrafast, fast, and slow relaxation, and corresponding eigenvalues (inverse relaxation times) have been selected from the huge number of all eigenvalues of the matrix of the kinetic coefficients. The analytical methods for finding the relaxation times of the ultrafast, fast and slow relaxation, recently developed and new ones proposed in this article, have been considered. The accuracy of the analytical calculations was controlled by comparison with much more resource-intensive computations using the matrix of the linearized equation. The analytical determination of the fast relaxation modes was based on the transition to the continual boundary-value problem with the potential for the distribution function of micelles over the aggregation numbers and using the perturbation theory. The spectrum was found numerically using the Runge–Kutta method. A new analytical solution for fast relaxation of the ensemble of cylindrical micelles with physically sound coefficients of monomer attachment to cylindrical micelles has been found with reducing the boundary value problem for the differential Becker–Döring–Frenkel equation to the equation for the Airy function.

AB - A general picture of relaxation in micellar solution of nonionic one-component surfactant on the basis of numerical solution of linearized set of the Becker–Döring equations for spherical and for cylindrical micelles has been analyzed in the form of a series in eigenvectors of the matrix of the kinetic coefficients. Two general characteristic cases have been considered as the initial conditions, the addition of monomers to the equilibrium system and the dilution of the equilibrium system. In both cases, the significant eigenvectors (relaxation modes) have been localized in the space of the aggregation numbers, that are responsible for the stages of ultrafast, fast, and slow relaxation, and corresponding eigenvalues (inverse relaxation times) have been selected from the huge number of all eigenvalues of the matrix of the kinetic coefficients. The analytical methods for finding the relaxation times of the ultrafast, fast and slow relaxation, recently developed and new ones proposed in this article, have been considered. The accuracy of the analytical calculations was controlled by comparison with much more resource-intensive computations using the matrix of the linearized equation. The analytical determination of the fast relaxation modes was based on the transition to the continual boundary-value problem with the potential for the distribution function of micelles over the aggregation numbers and using the perturbation theory. The spectrum was found numerically using the Runge–Kutta method. A new analytical solution for fast relaxation of the ensemble of cylindrical micelles with physically sound coefficients of monomer attachment to cylindrical micelles has been found with reducing the boundary value problem for the differential Becker–Döring–Frenkel equation to the equation for the Airy function.

KW - Micellization kinetics

KW - Becker–Döring equations

KW - Relaxation modes and times

KW - Micellization kinetics

KW - Becker–Döring equations

KW - Relaxation modes and times

KW - The Becker–Döring equations

UR - http://www.scopus.com/inward/record.url?scp=85102650387&partnerID=8YFLogxK

UR - https://www.mendeley.com/catalogue/bda0b680-5ecb-3578-a974-5a597be4cac7/

U2 - 10.1016/j.physa.2021.125912

DO - 10.1016/j.physa.2021.125912

M3 - Article

VL - 572

JO - Physica A: Statistical Mechanics and its Applications

JF - Physica A: Statistical Mechanics and its Applications

SN - 0378-4371

M1 - 125912

ER -

ID: 75066371