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Boundary layer of elastic turbulence. / Belan, S.; Chernykh, A.; Lebedev, V.

In: Journal of Fluid Mechanics, Vol. 855, 25.11.2018, p. 910-921.

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Harvard

Belan, S, Chernykh, A & Lebedev, V 2018, 'Boundary layer of elastic turbulence', Journal of Fluid Mechanics, vol. 855, pp. 910-921. https://doi.org/10.1017/jfm.2018.662

APA

Belan, S., Chernykh, A., & Lebedev, V. (2018). Boundary layer of elastic turbulence. Journal of Fluid Mechanics, 855, 910-921. https://doi.org/10.1017/jfm.2018.662

Vancouver

Belan S, Chernykh A, Lebedev V. Boundary layer of elastic turbulence. Journal of Fluid Mechanics. 2018 Nov 25;855:910-921. doi: 10.1017/jfm.2018.662

Author

Belan, S. ; Chernykh, A. ; Lebedev, V. / Boundary layer of elastic turbulence. In: Journal of Fluid Mechanics. 2018 ; Vol. 855. pp. 910-921.

BibTeX

@article{47b30134fdbd4397b6d0e6688c105969,
title = "Boundary layer of elastic turbulence",
abstract = "We investigate theoretically the near-wall region in elastic turbulence of a dilute polymer solution in the limit of large Weissenberg number. As has been established experimentally, elastic turbulence possesses a boundary layer where the fluid velocity field can be approximated by a steady shear flow with relatively small fluctuations on the top of it. Assuming that at the bottom of the boundary layer the dissolved polymers can be considered as passive objects, we examine analytically and numerically the statistics of the polymer conformation, which is highly non-uniform in the wall-normal direction. Next, imposing the condition that the passive regime terminates at the border of the boundary layer, we obtain an estimate for the ratio of the mean flow to the magnitude of the flow fluctuations. This ratio is determined by the polymer concentration, the radius of gyration of polymers and their length in the fully extended state. The results of our asymptotic analysis reproduce the qualitative features of elastic turbulence at finite Weissenberg numbers.",
keywords = "complex fluids, low-Reynolds-number flows, polymers, SHEAR, DYNAMICS, POLYMER-SOLUTIONS, RANDOM FLOW",
author = "S. Belan and A. Chernykh and V. Lebedev",
year = "2018",
month = nov,
day = "25",
doi = "10.1017/jfm.2018.662",
language = "English",
volume = "855",
pages = "910--921",
journal = "Journal of Fluid Mechanics",
issn = "0022-1120",
publisher = "Cambridge University Press",

}

RIS

TY - JOUR

T1 - Boundary layer of elastic turbulence

AU - Belan, S.

AU - Chernykh, A.

AU - Lebedev, V.

PY - 2018/11/25

Y1 - 2018/11/25

N2 - We investigate theoretically the near-wall region in elastic turbulence of a dilute polymer solution in the limit of large Weissenberg number. As has been established experimentally, elastic turbulence possesses a boundary layer where the fluid velocity field can be approximated by a steady shear flow with relatively small fluctuations on the top of it. Assuming that at the bottom of the boundary layer the dissolved polymers can be considered as passive objects, we examine analytically and numerically the statistics of the polymer conformation, which is highly non-uniform in the wall-normal direction. Next, imposing the condition that the passive regime terminates at the border of the boundary layer, we obtain an estimate for the ratio of the mean flow to the magnitude of the flow fluctuations. This ratio is determined by the polymer concentration, the radius of gyration of polymers and their length in the fully extended state. The results of our asymptotic analysis reproduce the qualitative features of elastic turbulence at finite Weissenberg numbers.

AB - We investigate theoretically the near-wall region in elastic turbulence of a dilute polymer solution in the limit of large Weissenberg number. As has been established experimentally, elastic turbulence possesses a boundary layer where the fluid velocity field can be approximated by a steady shear flow with relatively small fluctuations on the top of it. Assuming that at the bottom of the boundary layer the dissolved polymers can be considered as passive objects, we examine analytically and numerically the statistics of the polymer conformation, which is highly non-uniform in the wall-normal direction. Next, imposing the condition that the passive regime terminates at the border of the boundary layer, we obtain an estimate for the ratio of the mean flow to the magnitude of the flow fluctuations. This ratio is determined by the polymer concentration, the radius of gyration of polymers and their length in the fully extended state. The results of our asymptotic analysis reproduce the qualitative features of elastic turbulence at finite Weissenberg numbers.

KW - complex fluids

KW - low-Reynolds-number flows

KW - polymers

KW - SHEAR

KW - DYNAMICS

KW - POLYMER-SOLUTIONS

KW - RANDOM FLOW

UR - http://www.scopus.com/inward/record.url?scp=85054758700&partnerID=8YFLogxK

U2 - 10.1017/jfm.2018.662

DO - 10.1017/jfm.2018.662

M3 - Article

AN - SCOPUS:85054758700

VL - 855

SP - 910

EP - 921

JO - Journal of Fluid Mechanics

JF - Journal of Fluid Mechanics

SN - 0022-1120

ER -

ID: 17116618