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Measuring segregation of inertial particles in turbulent flows by a Full Lagrangian approach. 4 th IMS Workshop on Clouds and Turbulence Institute for Mathematical Sciences Imperial College London 23-25 March 2009. E. Meneguz Ph.D. project: Rain in a box of turbulence
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Measuring segregation of inertial particles in turbulent flows by a Full Lagrangian approach 4th IMS Workshop on Clouds and Turbulence Institute for Mathematical Sciences Imperial College London 23-25 March 2009 E. Meneguz Ph.D. project: Rain in a box of turbulence Supervisor: M. W. Reeks PostDoc: R. H. A. IJzermans School of Mechanical and Systems Engineering UNIVERSITY OF NEWCASTLE
Outline Elena Meneguz ● 4th IMS Workshop on Clouds and Turbulence ● Imperial College London ● 24.03.09 slide 2 • Introduction; • Equations of motion of inertial particles and other equations; • Compressibility of the Particle Velocity Field: • - MEPVF (Eulerian) - FLA (Lagrangian) • Method • flow field description - numerical simulations • Results: • Compressibility of the particle vel. field in both approaches - preliminary results in DNS of HIT - moments of the particle number density (comparison with theor. predictions) • Conclusions and future developments
State of the art Elena Meneguz ● 4th IMS Workshop on Clouds and Turbulence ● Imperial College London ● 24.03.09 slide 3 • Importance of de-mixing of particles in turbulent flows: many environmental-industrial and statistical interest • Preferential concentration (Crowe et al, 1993 and Maxey (1987); Sundaram and Collins (1997) and Wang et al. (1998); • Recently studied from different viewpoints (Chen et al, 2006, Balkowsky et al, 2001, Sommerer & Ott (1993) and Wilkinson et al, 2005;2007) • Random Uncorrelated Motion - “sling effect” (Falkovich et al. 2002) or “crossing trajectories effect” (Wilkinson et al. 2005) • Fevrier et al. MEF as sum of two contributions: MEPVF and RUM; based on box-counting (EULERIAN); • Osiptsov’s method (Reeks 2004, Healy and Young 2005) LAGRANGIAN
Equations of motion (Lagrangian frame) Elena Meneguz ● 4th IMS Workshop on Clouds and Turbulence ● Imperial College London ● 24.03.09 slide 4 • Particles/droplets: spherical, rigid, identical and heavy • Dilute system • Effect of gravity and Brownian motion not included particle position particle velocity fluid velocity at the position of the particle normalized particle relaxation number
Compressibility of the PVF Elena Meneguz ● 4th IMS Workshop on Clouds and Turbulence ● Imperial College London ● 24.03.09 slide 5 • Flow field incompressible: • Preferential concentration: • PVF compressible • non-zero gradients in the particle number density • Continuity equation: • For sufficiently small Stokes number:
MEPVF and compressibility of PVF Elena Meneguz ● 4th IMS Workshop on Clouds and Turbulence ● Imperial College London ● 24.03.09 slide 6 i-th cell • According to Fevrier et al. 2005: MEPVF = PVF + RUM • PVF = To be obtained from finite differences
Lagrangian quantification of the compressibility Elena Meneguz ● 4th IMS Workshop on Clouds and Turbulence ● Imperial College London ● 24.03.09 slide 7 Evol. eqts. 2D EXAMPLE: Continuity equation and averaging over all particle trajectories:
Model of synthetic turbulent flow Elena Meneguz ● 4th IMS Workshop on Clouds and Turbulence ● Imperial College London ● 24.03.09 slide 8 To study effect of RUM: Threshold value: St=0.25 2D carrier flow field (Babiano et al. 2000):
Numerical methods (Lagrangian vs Eulerian) Elena Meneguz ● 4th IMS Workshop on Clouds and Turbulence ● Imperial College London ● 24.03.09 slide 9 • 10,000 inertial particles, uniformly distributed at t=0; • Periodic boundary conditions for particles; • Trajectories and equations for calculated by RK4 method; • Initial conditions: (Volume is initially a cube). • 1,000,000 inertial particles, uniformly distributed at t=0; • Trajectories calculated by RK4 method; • Periodic boundary conditions for particles; • Divergence of PVF calculated using 2nd order finite difference scheme; • Numerical resolution varied between 102 and 602 cells.
Compressibility in time Elena Meneguz ● 4th IMS Workshop on Clouds and Turbulence ● Imperial College London ● 24.03.09 slide 10 St=0.05 St=0.2 St=2 St=0.5
Influence of numerical resolution Elena Meneguz ● 4th IMS Workshop on Clouds and Turbulence ● Imperial College London ● 24.03.09 slide 11 Resolution:102 cells ---- 202 cells ---- 602 cells ---- d<ln|J|>/dt ---- St=0.2 Lagrangian method corresponds to limiting case for infinitely fine grid in Eulerian box-counting method
Compressibility in DNS of HIT Elena Meneguz ● 4th IMS Workshop on Clouds and Turbulence ● Imperial College London ● 24.03.09 slide 12 St=1 Picciotto et al. 2005 • Good agreement between Lagrangian and Eulerian method • Singularities seem to be detected better by Lagrangian method
Moments of particle number density Elena Meneguz ● 4th IMS Workshop on Clouds and Turbulence ● Imperial College London ● 24.03.09 slide 13 • Along particle trajectory: particle number density n related to J by: • Particle averaged value of is related to spatially averaged value: • Any space-averaged momentis readily determined, if J is known for all particles in the sub-domain (equivalent to counting particles) Trivial limits:
Elena Meneguz ● 4th IMS Workshop on Clouds and Turbulence ● Imperial College London ● 24.03.09 slide 14 Moments of particle number density St=0.2 St=0.5 • Particle number density is spatially strongly intermittent • Sudden peaks indicate singularities in particle velocity field
Comparison with analytical estimate Elena Meneguz ● 4th IMS Workshop on Clouds and Turbulence ● Imperial College London ● 24.03.09 slide 15 If St is sufficiently small: Trivial limits: In agreement with Balkovsky et al (2001, PRL)
Conclusions Elena Meneguz ● 4th IMS Workshop on Clouds and Turbulence ● Imperial College London ● 24.03.09 slide 16 • The Lagrangian and Eulerian method show good agreement in the compressibility of the PVF for a wide range of St; • Singularities in the PVF can be detected by Lagrangian method but not by Eulerian method, due to finite grid size in the latter; • Lagrangian method allows for determination of any space-averaged moment of the particle number density, in contrast with Eulerian which would have too limited spatial resolutions; • The determination of moments of the particle number density have shown very high spatial intermittency due to RUM. • For first time, numerical support for theory of • Balkovsky et al (2001, PRL): “is convex function of”.
Further developments Elena Meneguz ● 4th IMS Workshop on Clouds and Turbulence ● Imperial College London ● 24.03.09 slide 17 • Open question: high intermittency in particle number density in DNS? • 3D DNS of stationary HIT for different St numbers • pdf methods for two particle dispersion at higher Re numbers
Elena Meneguz ● 4th IMS Workshop on Clouds and Turbulence ● Imperial College London ● 24.03.09 slide 18 Thank you for your attention