Particle Resuspension Model for Indoor Air Quality Applications.

Slides:



Advertisements
Similar presentations
NATO ASI Conference, Kyiv Pollutant Dispersion Investigation of buoyancy effects on distribution of mean concentration field in the turbulent circulation.
Advertisements

Using DEM-CFD method to model colloids aggregation and deposition
Chapter 22--Examples.
Granular Jets Alexander BarnaveliGeorgia If a steel ball is dropped onto a bed of dry sand, a "splash" will be observed that may be followed by the ejection.
Thermal Contact Conductance of Metal/Polymer Joints J.J. Fuller Mechanical Engineering Department Clemson University Clemson, SC and E.E. Marotta.
An Experimental Study and Fatigue Damage Model for Fretting Fatigue
Heat Exchanger Fouling and Cleaning – 2011 June , 2011 Influence of soluble polysaccharides on the adherence of particulate soils Y. Touré, P.G.
Gaseous And Particulate Dispersion In Street Canyons
Lecture Objectives -Finish with modeling of PM -Discuss -Advance discretization -Specific class of problems -Discuss the CFD software.
Interactive System for Pulverized Coal Combustion Visualization with Fluid Simulator Marek Gayer, Pavel Slavík and František Hrdlička Department of Computer.
Computational Fluid Dynamics (CFD) Study on the Influence of Airflow Patterns on Carbon Dioxide Distribution and Emission Rate in a Scaled Livestock Building.
1 Copyright © 2011, Elsevier Inc. All rights Reserved. Computational Fluid Dynamics of Particle Transport and Deposition Chapter 2 Goodarz Ahmadi.
Short Version : 22. Electric Potential Electric Potential Difference Conservative force: Electric potential difference  electric potential energy.
Conductors in Electrostatic Equilibrium. Electrostatic Equilibrium No net flow of electric charge No current.
ES 246 Project: Effective Properties of Planar Composites under Plastic Deformation.
Estimation of Engine Frictional Power P M V Subbarao Professor Mechanical Engineering Department Understand and Analyze All means of Power Draining…
Two-Phase Heat Transfer Laboratory Texas A&M University Experimental Study of Condensation on Micro Grooved Plates R. Barron-jimenez, H. Y. Hu, G. P. Peterson.
Task 2.B Resuspension of Dust Particles Due to Walking.
Single and multi-phase flows through rock fractures occur in various situations, such as transport of dissolved contaminants through geological strata,
Increasing atmospheric concentrations of greenhouse gases are known to be causing a gradual warming of the Earth's surface and potentially disastrous changes.
© The Lubrizol Corporation 2014, all rights reserved Formulating High Performance Coatings with Novel Adhesion Test Methods Dr. Yutao Yang NW Coatings.
November 14, 2013 Mechanical Engineering Tribology Laboratory (METL) Sina Mobasher Moghaddam Ph.D. Research Assistant Effect of Mean Stress on Rolling.
Jayadeep U.B. PhD (MED) IISc
UNLOCKING OPTIMAL FLOTATION: is the AIR RECOVERY the key? Jan Cilliers Royal School of Mines Imperial College London.
CAPTURING PHYSICAL PHENOMENA IN PARTICLE DYNAMICS SIMULATIONS OF GRANULAR GOUGE Effects of Contact Laws, Particle Size Distribution, and the 3 rd Dimension.
Weiyi Wang (Michelle) Research Assistant
Lead Technology Task 6.2 Materials for mechanical pump for HLM reactors M. Tarantino – ENEA Work Package Meeting – ENEA Bologna, November 17th, 2010.
Evaluating Scour Potential in Stormwater Catchbasin Sumps Using a Full-Scale Physical Model and CFD Modeling Humberto Avila Universidad del Norte, Department.
Carlos Gomes – Bin Hu – James Freihaut Slide 1 MindBend 2005 Resuspension of allergen-containing particles under mechanical and aerodynamic forces from.
Numerical modelling of scour around complex 3D structures Greg Melling 1, Justin Dix 1, Stephen Turnock 2 and Richard Whitehouse 3 1 Ocean and Earth Science,
Academic Background: Ph.D. Student in Water Resources Engineering at the University of Alabama. Currently working on Computational Fluid Dynamics and Physical.
Lecture Objectives Discuss specific class of problems
November 14, 2013 Mechanical Engineering Tribology Laboratory (METL) Arnab Ghosh Ph.D. Research Assistant Analytical Modeling of Surface and Subsurface.
Introduction to Tribology Surakshith. P Rane (28) Rajath. B Das (07) Venu. M (37) Shivanand. P (18)
ES 240 Project: Finite Element Modeling of Nano- Indentation of Thin Film Materials.
A dynamic analysis on the contaminant particles’ removal mechanism in cryogenic carbon dioxide (CO 2 ) cleaning process Dept. of Mechanical Engineering.
A Unified Lagrangian Approach to Solid-Fluid Animation Richard Keiser, Bart Adams, Dominique Gasser, Paolo Bazzi, Philip Dutré, Markus Gross.
Example: Radially Polarized Tube. Introduction This is a 2D static axisymmetric piezoelectric benchmark problem A radially polarized piezoelectric tube.
Comparison of strength behavior of unidirectional HMC and HSC composite subjected to biaxial loading J. Krystek, R. Kottner, L. Bek 19 th Conference on.
ELECTRICITY PHY1013S GAUSS’S LAW Gregor Leigh
M. Omang, S. Børve, and J. Trulsen
EPSRC Portfolio Partnership in Complex Fluids and Complex Flows Use Of Protein Structure Data For The Prediction Of Ultrafiltration Separation Processes.
ERMSAR 2012, Cologne, Germany, March 21 – 23, 2012 Aerosol Retention in Containment Leak Paths: Indications for a Code Model in the Light of COLIMA Experimental.
Turbulence Models Validation in a Ventilated Room by a Wall Jet Guangyu Cao Laboratory of Heating, Ventilating and Air-Conditioning,
Direct Numercal Simulation of two-phase turbulent boundary layer over waved water surface O. A. Druzhinin, Yu.I. Тroitskaya Institute of Applied Physics.
Numerical calculation of dielectrophoretic forces acting on micro-scale particles Dr Matt Praeger, Z Li, J M Smallwood and P L Lewin 15 th April 2015.
MULTI-COMPONENT FUEL VAPORIZATION IN A SIMULATED AIRCRAFT FUEL TANK C. E. Polymeropoulos Department of Mechanical and Aerospace Engineering, Rutgers University.
Charging by Friction pp Learning Goals Be able to use the electrostatic series to predict the charges of objects rubbed together Be able to.
Friction.
Example 3.5: Slowing the fall
Measurement of Transport in the PME EPA03 Task 2.B
Predicting NMR Response in Micro-CT images and Networks
Lecture Objectives Learn about particle dynamics modeling
Particle Transport, Deposition and Resuspension
Clarkson UNIVERSITY defy convention
Atomistic materials simulations at The DoE NNSA/PSAAP PRISM Center
Multiparticle Adhesive Dynamics
The State Diagram for Cell Adhesion Mediated by Two Receptors
Deposition and Removal
Current Model Model is 2D. FIDAP equates force and moment on the wafer surface and rotates the wafer into equilibrium.
COMPUTATIONAL MODELING OF PARTICLE TRANSPORT IN TURBULENT AIRFLOW
MODULE II: SIMULATIONS
E. Papanikolaou, D. Baraldi
Lecture Objectives Ventilation Effectiveness, Thermal Comfort, and other CFD results representation Surface Radiation Models Particle modeling.
Jianfeng Luo and David A. Dornfeld
Particle Resuspension Model for Indoor Air Quality Applications
ELECTRO-HYDRODYNAMICS ANALYSIS OF COROTRONS
Thrust 2. 0: Effect of Human Activity on Exposure PM Pollutants T2
Sample Applications of Fluent to Multiphase Flows
Potters field air quality
Presentation transcript:

Particle Resuspension Model for Indoor Air Quality Applications Goodarz Ahmadi Clarkson University Potsdam, NY

SAC Review 07/26-27/ Outline o Motivation and Objectives o Adhesion & Detachment of Particles with elastic & Plastic deformation o Particle Adhesion & Detachment with Capillary & Electrostatic Forces o Particle Removal from Rough Surfaces: u Small Roughness u Bumpy Particles u Highly Rough Surfaces o Particle Removal due to Human Walking u Model Description u Sample Results o Conclusions and Future work

SAC Review 07/26-27/ Motivation and general Objectives o Concentrations of particle pollutants in the indoor environment are often higher than outdoor. Particle resuspension due to human activity is expected to be one cause for the increase in PM. o Primary goal of this thrust is to provide quantitative understanding of the contribution of particle resuspension to PM concentration in the indoor environment

SAC Review 07/26-27/ Specific Objectives o Develop a particle detachment/re-suspension model for spherical and non-spherical particles from surfaces in the presence of capillary and electrostatic forces for indoor air quality applications. o To validate the detachment/re-suspension model. o To Develop a user defines subroutine for implementation of the model in the CFD codes. o To asses the contribution of the resuspension to the increase in indoor PM concentration due to human activities.

SAC Review 07/26-27/ Particle Resuspension from Smooth Surfaces Forces Acting on a Particle  Rolling Detachment  Elastic and Plastic Deformations

SAC Review 07/26-27/ Maximum Resistance to Rolling JKR Adhesion Model Thermodynamic Work of Adhesion Composite Young Modulus

SAC Review 07/26-27/ Maximum Resistance to Rolling (DMT) DMT and Maugis-Pollock Adhesion Model Maximum Resistance to Rolling (MP)

SAC Review 07/26-27/ Particle Resuspension Critical shear velocities for particle resuspension as predicted by different adhesion models. Model Predictions Results Polystyrene- Polystyrene Burst, Rolling JKR DMT Maugis-Pollock d (μm)

SAC Review 07/26-27/ Particle Resuspension Model Predictions Results d (μm) Calcium Carbonate- Calcium Carbonate Burst, Rolling With Capillary JKR DMT Maugis-Pollock Critical shear velocities for particle resuspension as predicted by different adhesion models.

SAC Review 07/26-27/ Particle Resuspension Model Predictions Results Comparison of the model predcition with the experimental data of Taheri and Bragg [39] (□) and Ibrahim et al. [40] (○). d (μm) Glass-Glass Burst, Rolling JKR DMT Maugis-Pollock With Capillary Without Capillary □ Taheri and Bragg [39] ○ Ibrahim et al. [40]

SAC Review 07/26-27/ Particle Resuspension Model Predictions Results Comparison of the model predictions with the experimental data of Zimon [38] (□), Ibrahim et al. [40] (○) and Ibrahim et al. [41] (◊). d (μm) Glass-Steel Burst, Rolling JKR DMT Maugis-Pollock With Capillary Without Capillary □ Zimon [38] ○ Ibrahim et al. [40] ◊ Ibrahim et al. [41]

SAC Review 07/26-27/ mg Resuspension of Rough Particles mg

SAC Review 07/26-27/ Comparison of the critical shear velocities as predicted by the burst model with the experimental data of Zimon [38] Resuspension of Rough Particles

SAC Review 07/26-27/ Bumpy Particles Bumpy particle model of compact irregular particles

SAC Review 07/26-27/ Charge Hays Electrostatic Forces for Bumpy Particles

SAC Review 07/26-27/ Bumpy Particles Critical shear velocities for bumpy particle resuspension in the presence of capillary and electrostatic forces.

SAC Review 07/26-27/ Bumpy Particles Critical shear velocities for bumpy particle resuspension in the presence of capillary and electrostatic forces.

SAC Review 07/26-27/ Bumpy Particles Critical shear velocities for bumpy particle resuspension in the presence of capillary and electrostatic forces.

SAC Review 07/26-27/ Bumpy Particles Critical shear velocities for bumpy particle resuspension in the presence of capillary and electrostatic forces.

SAC Review 07/26-27/ Bumpy Particles Comparison of the critical electric field with the experimental data of Hays (1978)

SAC Review 07/26-27/ Resuspension form Highly Rough Surfaces Adhesion Force Hydrodynamic Forces

SAC Review 07/26-27/ Sample Surface and Airflow Velocity (m/s) Contours over a Randomly generated surface with a roughness value of 5 micron.

SAC Review 07/26-27/ Sample Particle Removal

SAC Review 07/26-27/ Removal Areas for 2.5 µm Particles V = 5 m/s

SAC Review 07/26-27/ Particles Pairs Removal

SAC Review 07/26-27/ A Model for Particle Resuspension by Walking Assumptions o Shoe floor contact is modeled as two circular disks. o Squeezed film and wall jet models are used for the air low velocity. o Step down and up in the gait cycle are treated. o Particle re-deposition is accounted for.

SAC Review 07/26-27/ Evaluation of Squeezing Velocity Inside Foot Area (r < R) Outside Foot Area (r > R)

SAC Review 07/26-27/ A Model for Particle Resuspension by Walking Squeezed Film Wall Jet Critical radius for particle detachment for rolling detachment mechanisms at stepping down process.

SAC Review 07/26-27/ Particle Resuspension __ Simulation d=3~4μm x--- Experiment d=3~4μm __ Simulation d=5~7.5μm *--- Experiment d=5~7.5μm h=2.3 Comparison of the predicted particle concentration with the experimental data of Ferro and Qian (2006) for hard floor. t (min)

SAC Review 07/26-27/ Conclusions o A particle resuspension model from smooth and rough surfaces in presence of capillary force and electrostatic forces was developed. o The model was applied to particle resuspension in indoor environment due to human activities. o Preliniary comparisons with experimental data was performed.

SAC Review 07/26-27/ Future Work o Validate the model against additional data. o Perform detailed analysis of particle resuspenion in indoor environment due to human activities. o Develop detailed effect of large surface roughness on particle resuspension. o Develop a user defines subroutine for implementation of the model in the CFD codes. o Develop a model for resuspension form carpeted surfaces.