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Turbulence characteristics in wall-wake flows downstream of wall-mounted and near-wall horizontal cylinders

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Abstract

Turbulent characteristics in wall-wake flows downstream of wall-mounted and near-wall cylinders are investigated. The distributions of the defect of streamwise velocity, Reynolds shear stress and turbulence intensities exhibit a certain degree of self-preserving characteristic when they are scaled by their respective peak defect values. For the velocity defect distributions, the vertical distances are scaled by the half-width of peak defect velocity. However, for the distributions of the defects of the Reynolds shear stress and the turbulence intensities, the vertical distances are scaled by the half-width of Reynolds shear stress defect. The peak defects of all the quantities reduce with longitudinal distance signifying the recovery of the upstream distributions of the individual quantities. The third-order correlations reveal that for the wall-mounted cylinder, a streamwise acceleration associated with a downward flux of streamwise Reynolds normal stress (SRNS) in the inner-layer of wall-wake composes sweeps and a streamwise deceleration associated with an upward flux of SRNS in the outer-layer forms ejections. On the other hand, for the near-wall cylinder, a streamwise deceleration associated with a downward flux of SRNS in the inner-layer of wall-wake flow and the gap flow produces the inward interaction events, while the outer-layer characteristic is similar to that of wall-mounted cylinder. The turbulent kinetic energy (TKE) budget in the wake flow demonstrates strong negative pressure energy diffusion in addition to a strong TKE dissipation and diffusion and that in the gap flow exhibits a minor positive peak of pressure energy diffusion and a minor negative peak of TKE diffusion.

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Abbreviations

D :

Cylinder diameter (L)

d 50 :

Median size of sand (L)

E D :

Nondimensional TKE dissipation rate (–)

\( \mathsf{F} \) :

Flow Froude number, \( \overline{U} \)/(gh)0.5 (–)

F ii :

Power spectral density function (L2T−1)

f :

Frequency (T−1)

f kw :

Vertical flux of TKE, \( \overline{{kw^{\prime}}} \) (L3T−3)

g :

Acceleration due to gravity (LT−2)

h :

Flow depth (L)

k :

TKE, 0.5(\( \overline{{u^{\prime}u^{\prime}}} \) + \( \overline{{v^{\prime}v^{\prime}}} \) + \( \overline{{w^{\prime}w^{\prime}}} \)) (L2T−2)

k s :

Roughness height (L)

k w :

Wave number (L−1)

M jk :

Third-order correlations (–)

P D :

Nondimensional pressure energy diffusion rate (–)

p′:

Fluctuations of hydrostatic pressure relative to mass density of fluid (L2T−2)

p D :

Pressure energy diffusion rate (L2T−3)

\( \mathsf{R} \) :

Reynolds number characterized by cylinder diameter, \( \overline{U} \) D/υ (–)

\( \mathsf{R}_{\text{*}} \) :

Shear-particle Reynolds number, u*ks/υ (–)

S uu :

Spectral density as a function of kw (L3T−2)

T D :

Nondimensional TKE diffusion rate (–)

T P :

Nondimensional TKE production rate (–)

t D :

TKE diffusion rate (L2T−3)

t P :

TKE production rate (L2T−3)

U :

Time-average approaching velocity at an elevation z (LT−1)

\( \overline{U} \) :

Depth-averaged approaching velocity (LT−1)

u :

Time-averaged streamwise velocity component (LT−1)

u′:

Fluctuations of streamwise velocity (LT−1)

u * :

Approaching shear velocity (LT−1)

v :

Time-averaged transverse velocity component (LT−1)

v′:

Fluctuations of spanwise velocity (LT−1)

v D :

Viscous diffusion rate (L2T−3)

w :

Time-averaged vertical velocity component (LT−1)

w′:

Fluctuations of vertical velocity (LT−1)

x :

Streamwise distance (L)

y :

Spanwise distance (L)

z :

Vertical distance (L)

z 1 :

Height of occurrence of half of maximum velocity defect (L)

z 2 :

Height of occurrence of half of peak RSS defect (L)

Δu :

Velocity defect, U(z) − u(z) (LT−1)

Δz :

Gap thickness (L)

Δτ :

RSS defect relative to mass density of fluid, τ(z)|upstream − τ(z)|downstream (L2T−2)

Δσ u :

Streamwise turbulence intensity defect, σu(z)|upstream − σu(z)|downstream (LT−1)

Δσ w :

Vertical turbulence intensity defect, σw(z)|upstream − σw(z)|downstream (LT−1)

ε :

TKE dissipation rate (L2T−3)

ρ :

Mass density of fluid (ML−3)

σ u :

Streamwise turbulence intensity (LT−1)

σ w :

Vertical turbulence intensity (LT−1)

τ :

RSS relative to mass density of fluid (L2T−2)

υ :

Kinematic viscosity of fluid (L2T−1)

m :

Peak value

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Dey, S., Lodh, R. & Sarkar, S. Turbulence characteristics in wall-wake flows downstream of wall-mounted and near-wall horizontal cylinders. Environ Fluid Mech 18, 891–921 (2018). https://doi.org/10.1007/s10652-018-9573-0

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