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Experimental investigation of mixing and axial dispersion in Taylor–Couette flow patterns

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Abstract

The flow and mixing in a Taylor–Couette device have been characterized by means of simultaneous particle image velocimetry and planar laser-induced fluorescence (PLIF) measurements. Concentration of a passive tracer measurements was used to investigate mixing efficiency for different flow patterns (from steady Taylor vortex flow to modulated wavy vortex flow, MWVF). Taylor–Couette flow is known to evolve toward turbulence through a sequence of flow instabilities. Macroscopic quantities, such as axial dispersion and mixing index, are extremely sensitive to internal flow structures. PLIF measurements show clear evidences of different transport mechanisms including intravortex mixing and tracer fluxes through neighboring vortices. Under WVF and MWVF regimes, intravortex mixing is controlled by chaotic advection, due to the 3D nature of the flow, while intervortex transport occurs due to the presence of waves between neighboring vortices. The combination of these two mechanisms results in enhanced axial dispersion. We show that hysteresis may occur between consecutive regimes depending on flow history, and this may have a significant effect on mixing for a given Reynolds number.

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Abbreviations

c :

Critical

i :

Inner cylinder

e :

Outer cylinder

r :

Radial direction

θ :

Azimuthal direction

x :

Axial direction

\(r-x\) :

Meridional plane

0:

Initial condition

A :

Area of pixels with value 1 (−)

C :

Concentration (−)

\(\overline{C}\) :

Mean concentration (−)

\(C_{0}\) :

Injection concentration (g L−1)

\(C_{f}\) :

Final concentration (−)

\(D_{x}\) :

Dispersion coefficient (m2 s−1)

da :

Instantaneous area (m2)

dA :

Reference area (m2)

e :

Annular gap width (m)

f :

Frequency (s−1)

\(f_{\rm WVF}\) :

Traveling wave frequency (s−1)

F :

Spectral density of the gray level (−)

I :

Intensity of segregation (−)

\(I_{rx}\) :

Intensity of segregation in (−) the meridional plane (\(r-x\))

\(I_{\theta }\) :

Intensity of segregation in (−) the azimuthal direction (θ)

\(I_{v}\) :

Intensity of segregation (−) between adjacent vortices

L :

Column height (m)

m :

Azimuthal wave number (−)

\(m_{\rm inflow}\) :

Azimuthal wave number in inflow zone (−)

\(m_{\rm outflow}\) :

Azimuthal wave number in outflow zone

\(n_D\) :

Refraction index (−)

R :

Radius (m)

Re :

Reynolds number (−)

s :

Area stretch (−)

\(S_{a}\) :

Rate of stretching (s−1)

\(s_{i}\) :

Vortex size (m2)

S :

Taylor-cell size (m2)

t :

Time (s)

\(t_{\rm acc}\) :

Acceleration time (s)

\(T_{c}\) :

Inner cylinder rotational period (s)

\(T_{d}\) :

Vortex center rotational period (s)

U :

Velocity (m s−1)

\(V_{\phi }\) :

Phase velocity (rad s−1)

λ :

Wavelength (m)

\(\lambda _{x}\) :

Axial wavelength (m)

\(\sigma _{c}\) :

Standard deviation of concentration (−)

\(\sigma _{0}\) :

Mean max deviation (−)

η :

Radius ratio (−)

μ :

Dynamic viscosity (Pa s)

\(\nu\) :

Kinematic viscosity (m2 s−1)

ρ :

Density (kg m−3)

\(\varGamma\) :

Column aspect ratio (−)

\(\varOmega\) :

Inner cylinder rotational speed (s−1)

\(\varPhi\) :

Phase shift (−)

RTD:

Residence time distribution

PIV:

Particle image velocimetry

PLIF:

Planar laser-induced fluorescence

TVF:

Taylor vortex flow

WVF:

Wavy vortex flow

MWVF:

Modulated wavy vortex flow

TTVF:

Turbulent Taylor vortex flow

WIB:

Wavy inflow boundary

WOB:

Wavy outflow boundary

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Acknowledgments

The authors would like to thank M. Marchal, from IMFT, and F. Lamadie, from CEA Marcoule, for experimental support and fruitful discussions.

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Correspondence to Eric Climent.

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Nemri, M., Cazin, S., Charton, S. et al. Experimental investigation of mixing and axial dispersion in Taylor–Couette flow patterns. Exp Fluids 55, 1769 (2014). https://doi.org/10.1007/s00348-014-1769-6

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