Lagrangian Measurements of Two-Phase Pipe Flow Using Combined PIV/PTV

Measurements of two-phase particle suspension consisting of a liquid carrier phase and a solid particle phase are presented. Large diameter (d = [0.95−2.00] mm) and nearly neutral buoyant (ρp = 1050 kg m−3) particles are suspended in a turbulent fluid flow. The concentration of particles, φ ∼ 10−3, is slightly higher than previously reported in the literature. The carrier fluid is measured using particle image velocimetry (PIV), while the particle phase is measured with particle tracking velocimetry (PTV). There was found no evidence of turbulence modification within measurement accuracy, which is different form other studies using slightly heavier particles. Furthermore, challenges that arise with the use of combined PIV/PTV measurements at this flow regime and how these affects the measurements are discussed. GRAPHICAL ABSTRACT

[1]  C. J. Lawn,et al.  The determination of the rate of dissipation in turbulent pipe flow , 1971, Journal of Fluid Mechanics.

[2]  A. Cartellier,et al.  Acceleration statistics of inertial particles in turbulent flow , 2008 .

[3]  S. Drobniak,et al.  Coherent structures of free acoustically stimulated jet , 2002 .

[4]  Julio Soria,et al.  Stereoscopic PIV measurements of a turbulent boundary layer with a large spatial dynamic range , 2008 .

[5]  J. Westerweel Digital particle image velocimetry: theory and application , 1993 .

[6]  Harrison H. Zhou,et al.  The root–unroot algorithm for density estimation as implemented via wavelet block thresholding , 2010 .

[7]  R. Hout Time-resolved PIV measurements of the interaction of polystyrene beads with near-wall-coherent structures in a turbulent channel flow , 2011 .

[8]  E. Achenbach,et al.  Vortex shedding from spheres , 1974, Journal of Fluid Mechanics.

[9]  Markus Raffel,et al.  Particle Image Velocimetry: A Practical Guide , 2002 .

[10]  P. Moin,et al.  A direct numerical simulation study on the mean velocity characteristics in turbulent pipe flow , 2008, Journal of Fluid Mechanics.

[11]  C. Zheng,et al.  Experimental investigation on turbulence modification in a horizontal channel flow at relatively low mass loading , 2006 .

[12]  K. Christensen The influence of peak-locking errors on turbulence statistics computed from PIV ensembles , 2004 .

[13]  Z. C. Liu,et al.  Analysis and interpretation of instantaneous turbulent velocity fields , 2000 .

[14]  Jan Flusser,et al.  Image registration methods: a survey , 2003, Image Vis. Comput..

[15]  B. Efron Bootstrap Methods: Another Look at the Jackknife , 1979 .

[16]  J. Riley,et al.  Equation of motion for a small rigid sphere in a nonuniform flow , 1983 .

[17]  A. Jensen,et al.  Suspensions in turbulent liquid pipe flow: Kinetic modelling and added mass effects , 2009 .

[18]  Qian Liao,et al.  An efficient anti-aliasing spectral continuous window shifting technique for PIV , 2005 .

[19]  R. V. Hout,et al.  Measurement of polystyrene beads suspended in a turbulent square channel flow: Spatial distributions of velocity and number density , 2014 .

[20]  J. Westerweel,et al.  Universal outlier detection for PIV data , 2005 .

[21]  K. Kiger,et al.  PIV Technique for the Simultaneous Measurement of Dilute Two-Phase Flows , 2000 .

[22]  R. Mei,et al.  Velocity fidelity of flow tracer particles , 1996 .

[23]  Ian Eames,et al.  IUTAM Symposium on Computational Approaches to Multiphase Flow , Argonne, Illinois, USA , 2006 .

[24]  F. Toschi,et al.  Lagrangian Properties of Particles in Turbulence , 2009 .

[25]  Raf Theunissen,et al.  On improvement of PIV image interrogation near stationary interfaces , 2008 .

[26]  W. Merzkirch,et al.  A method of tracking ensembles of particle images , 1996 .

[27]  S. Balachandar,et al.  Turbulent Dispersed Multiphase Flow , 2010 .

[28]  M. Wand,et al.  Multivariate Locally Weighted Least Squares Regression , 1994 .