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Thickness of the elastic sublayer in the velocity field of diluted polymeric solutions

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Abstract

Results from a series of Theological and pipe flow experiments using watersoluble hydroxyethylcellulose and polyethyleneoxide are presented. Phenomena of drag reduction were investigated for values of concentration (in weight) of polymers in water ranging x = 10-4 to x = 5 · 10-3. Velocity measurements by using a laser-Doppler anemometer to type DISA-Mark II served for determining the variation in thickness of the elastic sublayer in the turbulent flow exhibiting drag reduction.

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Abbreviations

A :

coefficient in Eq. (1)

B :

coefficient in Eq. (1)

D :

pipe diameter

D:

shear velocity

K :

consistency parameter in Eq. (5)

n :

flow index of non-newtonian fluids

r :

radial distance from the pipe center

Re :

Reynolds number

R :

pipe radius

y :

distance from the pipe wall

y + :

dimensionless distance from the pipe wall, (R-r)u * ϱ/μ

y e + :

experimental value of the dimensionless thickness of the viscous and elastic sublayer

y s + :

dimensionless thickness of the viscous and the elastic sublayer

u + :

dimensionless local velocity, ΰ/*

u * :

dynamic friction velocity, w(λ/8) o.5

ΰ :

time-averaged local instantaneous velocity of flow

w :

average velocity over the cross-section of the pipe

X :

weight fraction of polymer in water solution

μ :

viscosity

λ :

fraction factor

ϱ :

density

v :

kinematic viscosity

τ :

shear stress

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Lodesová, D., Lodes, A. Thickness of the elastic sublayer in the velocity field of diluted polymeric solutions. Experiments in Fluids 7, 379–382 (1989). https://doi.org/10.1007/BF00193418

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