On the rheology of linear wormlike micellar solutions

The shear rheology of linear wormlike micellar solutions (WMSs) is described by both Poisson renewal (PRM) and shuffling (SFM) models with different values of the model parameters. For low shear strains and rates of strains, the micellar solutions behave as a Maxwellian body with constant elasticity and viscosity. The excellent description of experimental data in the literature using PRM or SFM suggests that both models predict identical dependencies of the dynamic storage and loss moduli on the frequency of oscillations. It is shown in the literature, that the PRM becomes equivalent to the SFM, when the breaking time is constant, τ br , and the characteristic reptation time, τ rep , is equal to π 2 τ d0 , where τ d0 is the reptation time evaluated with respect to the average length of the chain. Three independent rheological tests (apparent viscosity vs shear rate, stress vs strain at constant shear rates, strain oscillations at low amplitudes and different frequencies) are applied to low, medium, and high zero-shear viscosity WMSs to obtain the PRM and SFM model parameters (elasticity, viscosity, relaxation, breaking, and reptation times). The known closed-form analytical expression for the Laplace image of the stress relaxation function and the respective infinite series for the complex modulus give possibility for the reported here precise systematic calculations of the storage and elastic moduli, the crossover frequency, and the elasticity for all values of ζ br = τ br / τ rep ≤ 100. The predictions of the PRM length-dependent breaking-time versions are indistinguishable from those of the SFM for the obtained universal dependencies of the characteristic time, τ B0 , on ζ br . The applicability of the Vasquez–Cook–McKinley and the single-mode Oldroyd 8-constant models to describe the rheological behavior of WMSs is tested. The theoretical findings and conclusions are confirmed experimentally and illustrate the self-consistency of the used rheological regimes.

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Publication Details

Journal
JCIS Open
Published
2025-11-12
DOI
https://doi.org/10.1016/j.jciso.2025.100160
Citations
1
Primary Topic
Rheology and Fluid Dynamics Studies
Type
article
Field-Weighted Citation Impact
0.72
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article

On the rheology of linear wormlike micellar solutions

Gergana M. Radulova, Yee Wei Ung, Jordan T. Petkov, Krassimir D. Danov
1 citations
JCIS Open
Rheology and Fluid Dynamics Studies
0.72
article

On the rheology of linear wormlike micellar solutions

Gergana M. Radulova, Yee Wei Ung, Jordan T. Petkov, Krassimir D. Danov
article en
1 citations

Abstract

The shear rheology of linear wormlike micellar solutions (WMSs) is described by both Poisson renewal (PRM) and shuffling (SFM) models with different values of the model parameters. For low shear strains and rates of strains, the micellar solutions behave as a Maxwellian body with constant elasticity and viscosity. The excellent description of experimental data in the literature using PRM or SFM suggests that both models predict identical dependencies of the dynamic storage and loss moduli on the frequency of oscillations. It is shown in the literature, that the PRM becomes equivalent to the SFM, when the breaking time is constant, τ br , and the characteristic reptation time, τ rep , is equal to π 2 τ d0 , where τ d0 is the reptation time evaluated with respect to the average length of the chain. Three independent rheological tests (apparent viscosity vs shear rate, stress vs strain at constant shear rates, strain oscillations at low amplitudes and different frequencies) are applied to low, medium, and high zero-shear viscosity WMSs to obtain the PRM and SFM model parameters (elasticity, viscosity, relaxation, breaking, and reptation times). The known closed-form analytical expression for the Laplace image of the stress relaxation function and the respective infinite series for the complex modulus give possibility for the reported here precise systematic calculations of the storage and elastic moduli, the crossover frequency, and the elasticity for all values of ζ br = τ br / τ rep ≤ 100. The predictions of the PRM length-dependent breaking-time versions are indistinguishable from those of the SFM for the obtained universal dependencies of the characteristic time, τ B0 , on ζ br . The applicability of the Vasquez–Cook–McKinley and the single-mode Oldroyd 8-constant models to describe the rheological behavior of WMSs is tested. The theoretical findings and conclusions are confirmed experimentally and illustrate the self-consistency of the used rheological regimes.

JCIS OpenVol. 20
University of Manchester (GB), CE Technologies (United Kingdom) (GB), Sofia University "St. Kliment Ohridski" (BG)
Openalex Percentile: Top 26%
Rheology and Fluid Dynamics Studies
0.72
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