2003
DOI: 10.1021/jp0302111
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Birefringence, Deformation, and Scattering of Wormlike Macromolecules under an External Agent. Steady-State Properties in an Electric Field

Abstract: In this paper, we study the steady-state birefringence, deformation, and scattering of wormlike macromolecules under the influence of an electric field. We use a model of N + 1 pointlike elements whose connectors define N axially symmetric subunits. The model is able to describe some properties of segmentally flexible and wormlike macromolecules depending on the choice of N. We use the Monte Carlo computer simulation technique to characterize the effect of the electric field on the orientation and deformation … Show more

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Cited by 4 publications
(7 citation statements)
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References 36 publications
(61 reference statements)
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“…For flexible models made up of beads connected by virtual bonds, the usual ap-proximation is to assume that associated with each virtual bond is an electric polarizability tensor, which is axially symmetric about the bond vector. [20][21][22][23] As a summary, the orientation mechanism of flexible macroions is complex and the pairwise additive models may be as good as we can do at the present time. This model of orienting mechanism has been named sometimes as "pairwise additive."…”
Section: B Orienting Mechanismsmentioning
confidence: 78%
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“…For flexible models made up of beads connected by virtual bonds, the usual ap-proximation is to assume that associated with each virtual bond is an electric polarizability tensor, which is axially symmetric about the bond vector. [20][21][22][23] As a summary, the orientation mechanism of flexible macroions is complex and the pairwise additive models may be as good as we can do at the present time. This model of orienting mechanism has been named sometimes as "pairwise additive."…”
Section: B Orienting Mechanismsmentioning
confidence: 78%
“…As argued in a previous work, 23 there are different ways of defining the flexibility of a wormlike molecule. ͑2͒, P is the persistence length and L is the contour length.…”
Section: ͑2͒mentioning
confidence: 93%
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“…These theories made some simplifying assumptions about hydrodynamic interactions, but it seems that a set of characteristic relaxation times really exists for every flexible molecule; indeed, it has been shown that τ 1 is the same regardless of the property or technique used in its measurement. 10,11 All these considerations illustrate the complexity of describing the full dynamics (simultaneously translational, internal, etc.) of flexible macromolecules.…”
Section: Types Of Macromolecular Flexibilitymentioning
confidence: 99%