Lecture Objectives Learn about particle dynamics modeling

Slides:



Advertisements
Similar presentations
Transfer coefficient algorithm for small mass nodes in material point method Xia Ma, Balaji Jayaraman, Paul T. Giguere and Duan Z. Zhang CartaBlanca Team.
Advertisements

1 Application of for Predicting Indoor Airflow and Thermal Comfort.
Motion of particles trough fluids part 2
The Role of Controls for Indoor Air Quality Kent W. Peterson, PE, Fellow ASHRAE P2S Engineering, Inc. Mid Columbia ASHRAE Chapter.
Master’s Dissertation Defense Carlos M. Teixeira Supervisors: Prof. José Carlos Lopes Eng. Matthieu Rolland Direct Numerical Simulation of Fixed-Bed Reactors:
Dynamic model of a drop shot from an inkjet printer.
Lecture Objectives -Finish with modeling of PM -Discuss -Advance discretization -Specific class of problems -Discuss the CFD software.
Motion of particles trough fluids part 2
Fluid Kinematics Fluid Dynamics . Fluid Flow Concepts and Reynolds Transport Theorem ä Descriptions of: ä fluid motion ä fluid flows ä temporal and spatial.
CE 1501 CE 150 Fluid Mechanics G.A. Kallio Dept. of Mechanical Engineering, Mechatronic Engineering & Manufacturing Technology California State University,
Enclosure Fire Dynamics
Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Fluid Kinematics Fluid Mechanics July 14, 2015 
Fluid mechanics 3.1 – key points
Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Fluid Kinematics Fluid Mechanics July 15, 2015 Fluid Mechanics July 15, 2015 
Instructor: André Bakker
General Formulation - A Turbojet Engine
Lecture Objectives: Review discretization methods for advection diffusion equation Accuracy Numerical Stability Unsteady-state CFD Explicit vs. Implicit.
The University of Texas at Austin Spring 2013 CAEE Department Course: Modeling of Air and Pollutant Flows in Buildings Instructor: Dr. Atila Novoselac.
Two-fluid models for fluidized bed reactors: Latest trends and challenges Yassir Makkawi Chemical Engineering.
Address: Washington street 40 B-1050 Brussels Belgium Tel: Fax: rehva Federation of European.
1 CREL meeting 2004 CFD Simulation of Fisher-Tropsch Synthesis in Slurry Bubble Column By Andrey Troshko Prepared by Peter Spicka Fluent Inc. 10 Cavendish.
Lecture Objectives: -Define turbulence –Solve turbulent flow example –Define average and instantaneous velocities -Define Reynolds Averaged Navier Stokes.
Mechanistic Modeling and CFD Simulations of Oil-Water Dispersions in Separation Components Mechanistic Modeling and CFD Simulations of Oil-Water Dispersions.
Lecture Objectives Discuss specific class of problems
Next Class Final Project and Presentation – Prepare and me the ppt files 5-7 slides Introduce your problem (1-2 slides) – Problem – Why CFD? Methods.
A Hybrid Particle-Mesh Method for Viscous, Incompressible, Multiphase Flows Jie LIU, Seiichi KOSHIZUKA Yoshiaki OKA The University of Tokyo,
KINEMATICS Kinematics describes fluid flow without analyzing the forces responsibly for flow generation. Thereby it doesn’t matter what kind of liquid.
Mathematical Equations of CFD
Lecture Objectives: -Discuss the final project presentations -Energy simulation result evaluation -Review the course topics.
Sedimentation.
Lecture Objectives Unsteady State Simulation Example Modeling of PM.
Lecture Objectives -Finish with age of air modeling -Introduce particle dynamics modeling -Analyze some examples related to natural ventilation.
FLOW THROUGH GRANULAR BEDS AND PACKED COLUMN
Lecture Objectives -Finish Particle dynamics modeling -See some examples of particle tracking -Eulerian Modeling -Define deposition velocity -Fluid Dynamics.
Lecture Objectives Meshing Unsteady State CFD.
Turbulence Models Validation in a Ventilated Room by a Wall Jet Guangyu Cao Laboratory of Heating, Ventilating and Air-Conditioning,
Lecture Objectives: Review discretization methods for advection diffusion equation –Accuracy –Numerical Stability Unsteady-state CFD –Explicit vs. Implicit.
Lecture Objectives: Define 1) Reynolds stresses and
1. Integral vs Differential Approach
Lecture Objectives -Analyze some examples related to natural ventilation.
Lecture Objectives: - Numerics. Finite Volume Method - Conservation of  for the finite volume w e w e l h n s P E W xx xx xx - Finite volume.
Lecture Objectives Review wall functions Discuss: Project 1, HW2, and HW3 Project topics.
Convection Heat Transfer in Manufacturing Processes P M V Subbarao Professor Mechanical Engineering Department I I T Delhi Mode of Heat Transfer due to.
Heat Transfer Su Yongkang School of Mechanical Engineering # 1 HEAT TRANSFER CHAPTER 6 Introduction to convection.
Heat Transfer Su Yongkang School of Mechanical Engineering # 1 HEAT TRANSFER CHAPTER 7 External flow.
Course : Civil Engineering Division : C (3 rd Semester). Subject : Fluid Mechanics Subject Code : Guided By :HIREN JARIWALA(H.O.D) :DIXIT CHAUHAN(ASSI.PROF.)
Lecture Objectives: Accuracy of the Modeling Software.
CFD ANALYSIS OF MULTIPHASE TRANSIENT FLOW IN A CFB RISER
Objective Introduce Reynolds Navier Stokes Equations (RANS)
Design of Port Injection Systems for SI Engines
Chapter 4 Fluid Mechanics Frank White
Buildings Course: Modeling of Air and Pollutant Flows in
Lecture Objectives Unsteady State Ventilation Modeling of PM.
MULTIPHASE FLOW More complicated than single phase flow. Flow pattern is not simply laminar or turbulent. Types of multiphase flow: Solid-fluid flows (e.g.
Thermal analysis Friction brakes are required to transform large amounts of kinetic energy into heat over very short time periods and in the process they.
Lecture Objectives Discuss HW4 Multizone modeling
Lecture Objectives Learn about Implementation of Boundary Conditions
Lecture Objectives Finish with boundary conditions Unsteady State Flow.
Particle (s) motion.
Space Distribution of Spray Injected Fluid
Lecture Objectives LES Multizone modeling.
Lecture Objectives Discuss HW4
Fluid Kinematics Fluid Dynamics.
Lecture Objectives Review for exam Discuss midterm project
Lecture Objectives Ventilation Effectiveness, Thermal Comfort, and other CFD results representation Surface Radiation Models Particle modeling.
MAE 3241: AERODYNAMICS AND FLIGHT MECHANICS
Lecture Objectives: Boundary Conditions Project 1 (software)
II. Theory for numerical analysis of multi-phase flow (Practice)
Lecture 16 Multiphase flows Part 1.
Study of forward and inverse airflow models for use in systematic design of indoor air sensor systems Y. Lisa Chen1,2 and Dr. Jin Wen2 1Koerner Family.
Presentation transcript:

Lecture Objectives Learn about particle dynamics modeling Discuss project and result accuracy evaluation

Particulate matters (PM) Properties Size, density, liquid, solid, combination, … Sources Airborne, infiltration, resuspension, ventilation,… Sinks Deposition, filtration, ventilation (dilution),… Distribution - Uniform and nonuniform Human exposure

Properties ASHRAE Transaction 2004

Particle size distribution ASHRAE Transaction 2004 Ventilation system affect the PM concentration in indoor environment !

Human exposure ASHRAE Transaction 2004

Two basic approaches for modeling of particle dynamics Lagrangian Model particle tracking For each particle ma=SF Eulerian Model Multiphase flow (fluid and particles) Set of two systems of equations

Lagrangian Model particle tracking A trajectory of the particle in the vicinity of the spherical collector is governed by the Newton’s equation m∙a=SF Forces that affect the particle (rVvolume) particle ∙dvx/dt=SFx (rVvolume) particle ∙dvy/dt=SFy (rVvolume) particle ∙dvz/dt=SFz System of equation for each particle Solution is velocity and direction of each particle

Lagrangian Model particle tracking Basic equations - momentum equation based on Newton's second law Drag force due to the friction between particle and air - dp is the particle's diameter, - p is the particle density, - up and u are the particle and fluid instantaneous velocities in the i direction, - Fe represents the external forces (for example gravity force). This equation is solved at each time step for every particle. The particle position xi of each particle are obtained using the following equation: For finite time step

Algorithm for CFD and particle tracking Steady state airflow Unsteady state airflow Airflow (u,v,w) Airflow (u,v,w) for time step  Steady state Injection of particles Injection of particles Particle distribution for time step  Particle distribution for time step  Particle distribution for time step + Airflow (u,v,w) for time step + Particle distribution for time step +2 Particle distribution for time step + ….. ….. Case 1 when airflow is not affected by particle flow Case 2 particle dynamics affects the airflow One way coupling Two way coupling

Eulerian Model Solve several sets of NS equations Define the boundary conditions in-between phases Multiphase/Mixture Model Mixture model Secondary phase can be granular Applicable for solid-fluid simulations Granular physics Solve total granular pressure to momentum equation Use Solids viscosity for dispersed solid phase Density difference should be small. Useful mainly for liquid-solids multiphase systems There are models applicable for particles in the air

Multiphase flow Multiphase flow can be classified in the following regimes: gas-liquid or liquid-liquid flows gas-solid flows particle-laden flow: discrete solid particles in a continuous gas pneumatic transport: flow pattern depends on factors such as solid loading, Reynolds numbers, and particle properties. Typical patterns are dune flow, slug flow, packed beds, and homogeneous flow. fluidized beds: consist of a vertical cylinder containing particles where gas is introduced through a distributor. liquid-solid flows three-phase flows

Multiphase Flow Regimes Fluent user manual 2006

Challenging Problem: Application of CFD in a large space EXAMPLE: Five-Story Parking Garage Ventilation Multi-space building Course grid model properties www.airpak.fluent.com - The geometry should present correct geometry around large openings - The ratio between the total flow area and the floor area should be the same as in full scale - Air supply and return openings should be defined in a coarse grid sufficient for momentum and energy flow predictions The result will define global air and energy flow between zones but accuracy is insufficient for an analysis of the detail air velocity distribution in the zones.

Detail air velocity distribution in room Detail description of geometry Simple Description of Interior Furnishings can be described as A volume with additional pres- sure drop in the momentum Equations:

Engineering Application Unlimited number of problems! For example: http://www.ansys.com/products/airpak/solutions.asp?name=p1 http://www.cd-adapco.com/applications/building.html

Human Exposure Airflow in the room vs. Airflow in vicinity of occupant CO2 distribution - Course mesh - Simple geometry CO2 sources Occupied zone

Simulation of an occupant Detailed geometry: Good for local convection coefficient calculation at the skin Effect of breathing an movement decrease accuracy

Different level of geometry details Avaraged geometry can be used for global effects Simple geometry can be used for semi-global effects Detailed geometry should be used for local effects Conclusions from geometry analysis (Peter Nielsen) Semi-global effect Differences in geometry have a small influence on velocity, temperature distribution, contaminant distribution far from the manikin Local effect Differences in geometry have an effect on velocity and concentration distribution close to a person and exposure of a person

We Often Need Experimental Validation Room with nonuniform temporal and spatial distribution of particles (for example smoke) Validation results for 0.74 m S1 CFD model Monitoring Position S1 Monitoring Position S2 S2 Pollution Source active 2 minutes Experiment

Examples of CFD application in Indoor environment research Some hot topics Particle Transport in a boundary layer Surface Chemistry Air and particle flow in lung Various analyses of fluid flow in building components and HVAC systems