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Wake development in staggered short cylinder arrays within a channel

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Abstract

Staggered arrays of short cylinders, known as pin–fins, are commonly used as a heat exchange method in many applications such as cooling electronic equipment and cooling the trailing edge of gas turbine airfoils. This study investigates the near wake flow as it develops through arrays of staggered pin fins. The height-to-diameter ratio was unity while the transverse spacing was kept constant at two cylinder diameters. The streamwise spacing was varied between 3.46 and 1.73 cylinder diameters. For each geometric arrangement, experiments were conducted at Reynolds numbers of 3.0e3 and 2.0e4 based on cylinder diameter and velocity through the minimum flow area of the array. Time-resolved flowfield measurements provided insight into the dependence of row position, Reynolds number, and streamwise spacing. Decreasing streamwise spacing resulted in increased Strouhal number as the near wake length scales were confined. In the first row of the bundle, low Reynolds number flows were mainly shear-layer-driven while high Reynolds number flows were dominated by periodic vortex shedding. The level of velocity fluctuations increased for cases having stronger vortex shedding. The effect of streamwise spacing was most apparent in the reduction of velocity fluctuations in the wake when the spacing between rows was reduced from 2.60 diameters to 2.16 diameters.

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Abbreviations

d P :

Tracer particle diameter

D :

Pin–fin diameter

D h :

Duct hydraulic diameter

E uu :

One-dimensional energy spectrum of streamwise velocity

f :

Frequency

H :

Channel height, pin–fin height

k :

Turbulent kinetic energy

L r :

Wake closure position

Re D :

Reynolds number, \( Re_{\text{D}} = U_{\max } D\nu^{ - 1} \)

S L :

Longitudinal/streamwise pin–fin spacing (X-direction)

S T :

Transverse pin–fin spacing (Y-direction)

St:

Strouhal number, \( {\text{St}} = {fDU}_{\max }^{ - 1} \)

Stk:

Stokes number, \( {\text{Stk}} = \left( {{{d_{\text{P}} \rho_{\text{P}} } \mathord{\left/ {\vphantom {{d_{\text{P}} \rho_{\text{P}} } {18\mu }}} \right. \kern-\nulldelimiterspace} {18\mu }}} \right)\left( {{{U_{\max } } \mathord{\left/ {\vphantom {{U_{\max } } D}} \right. \kern-\nulldelimiterspace} D}} \right) \)

U m :

Time-mean bulk channel velocity

U max :

Time-mean velocity through minimum array flow area

\( \overline{U} \) :

Local time-averaged streamwise velocity

u′:

Local fluctuating streamwise velocity, or RMS velocity

\( \overline{V} \) :

Local time-averaged transverse velocity

v′:

Local fluctuating transverse velocity, or RMS velocity

X :

Longitudinal/streamwise direction

Y :

Transverse direction

Z :

Wall-normal direction

ρP :

Tracer particle density

ν:

Air kinematic viscosity

μ:

Air dynamic viscosity

\( \tilde{\omega }_{Z} \) :

Instantaneous Z-vorticity

ϕ:

Phase angle

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Acknowledgments

The authors would like to acknowledge the Department of Defense and the SMART fellowship program for providing funding for this work.

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Correspondence to Jason K. Ostanek.

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Ostanek, J.K., Thole, K.A. Wake development in staggered short cylinder arrays within a channel. Exp Fluids 53, 673–697 (2012). https://doi.org/10.1007/s00348-012-1313-5

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