Title: Experimental and numerical investigations of particle clustering in isotropic turbulence
1Experimental and numerical investigations of
particle clustering in isotropic turbulence
Workshop on Stirring and Mixing The Lagrangian
Approach Lorentz Center Leiden, The
Netherlands August 21-30, 2006
Cornell University SUNY Buffalo Max Planck Institute
Dr. Lance R. Collins Dr. Hui Meng Dr. Eberhard Bodenschatz
Juan Salazar Scott Woodward
Dr. Zellman Warhaft Lujie Cao
S. Ayyalasomayajula Jeremy de Jong
International Collaboration for Turbulence
Research (ICTR)
2Particle Clustering in Turbulence
Vortices
Strain Region
- Maxey (1987) Squires Eaton (1991) Wang
Maxey (1993) - Shaw, Reade, Verlinde Collins (1997)
- Falkovich, Fouxon Stepanov (2002) Zaichik
Alipchenkov (2003) Chun, Koch, Rani, Ahluwalia
Collins (2005)
3Turbulence in Clouds
Buoyancy
Cloud Condensation Nuclei (CCN)
4d2 Law
mass
energy
- Current microphysical models predict
- too slow condensational growth
- too narrow cloud droplet distributions
Shaw (2003)
5Beard Ochs (1993)
At this rate, we are quite a way off from
being able to predict, on firm micro-physical
grounds, whether it will rain.
0.1 mm
1 mm
10 mm
6Clouds in Climate Models
Visible Wavelengths
Infra Red
High, cold clouds
Low, warm clouds
Distribution of cloud cover profoundly influences
global energy balance
Raymond Shaw
7Collision Kernel
Particle clustering impacts the RDF
Sundaram Collins (1997) Wang, Wexler Zhou
(1998)
8Monodisperse clustering drift
Chun, Koch, Sarma, Ahluwalia Collins, JFM 2005
9Monodisperse clustering diffusion
Chun, Koch, Sarma, Ahluwalia Collins, JFM 2005
10Monodisperse clustering RDF
St 0.7
Chun, Koch, Sarma, Ahluwalia Collins, JFM 2005
11Bidisperse clustering
Chun, Koch, Sarma, Ahluwalia Collins, JFM 2005
12Bidisperse clustering
Chun, Koch, Sarma, Ahluwalia Collins, JFM 2005
13Bidisperse clustering stationary
Chun, Koch, Sarma, Ahluwalia Collins, JFM 2005
14Experiments and Simulations
RDF Measurements
Direct Numerical Simulations
15Turbulence Chamber
16Flow Characterization
Conditions at 6 Fan Speeds (MKS)
17Metal-Coated Hollow Glass Spheres
Mean 6 microns STD 3.8 microns 1-10
particles/cm3 FV 10-7
18Measurements of RDF
Wind Tunnel
Turbulence Box
Saw, Shaw, Ayyalasomayajula, Chuang Gylfason,
Warhaft (2006)
Wood, Hwang Eaton (2005)
19Why 3D?
2D Sampling
1D Sampling
Relations
Holtzer Collins (2002)
203D Particle Position Measurement Techniques
- Particle Tracking Velocimetry (PTV)
- Advantages Lagrangian particle information
- Disadvantages Limited particle number density.
- Holographic Particle Image Velocimetry (HPIV)
- Advantages Better particle number density than
PTV, larger 3D volume than Stereo PIV - Disadvantages Cannot resolve time evolution of
particles.
21Hybrid Digital HPIV
NdYag Laser 532 nm
Numerical Reconstruction Intensity-Based Particle
Extraction
Variable Beam Attenuator
Beam Expander
Reference Beam
40 cm
1k x 1k CCD
(4 cm)3 Volume
22Particle Concentration and Phase Averaging
23Size Distribution Evolution
24Time Dependence of RDF
25Direct Numerical Simulations
- 1283 Grid Points
- Rl 80
- 1.2 Million Particles (one way coupling)
- Experimental Particle Size Distribution
Keswani Collins (2004)
26Filtering by camera
Metal-coated hollow glass spheres
Mean 6 microns STD 3.8 microns
27Filtering by camera
Metal-coated hollow glass spheres
Mean 6 microns STD 3.8 microns
28Comparison at Rl 130
29Comparison at Rl 161
30Summary
- Clustering results from a competition between
inward drift and outward diffusion - Radial Distribution Function (RDF) is the measure
for collision kernel - Analysis of RDF involves Lagrangian statistics
along inertial particle trajectories - RDF mainly found in direct numerical simulation
- 3D measurements of RDF using holographic imaging
- Reasonable agreement between experiments and DNS
- Challenges for the measurement
- Characterizing flow (dissipation rate, e)
- Particle size distribution (will separate
particles) - Increasing resolution of experiment (smaller
separations)
International Collaboration for Turbulence
Research (ICTR)