Wall film model - Introduction
|
|
- Rudolf Hutchinson
- 7 years ago
- Views:
Transcription
1 WALL FILM MODEL
2 Wall film model - Introduction To comply with the requirement of the industry a constant improvement of the accuracy of the physical model used in CFD is necessary. To predict the correct mixture formation and pollutant evolution a model for the wall film is required. The basic physics of the wall film formation and evolution is widely treated in literature. Our model is based on the one proposed by Foucart et al. (SAE Paper ) with the evaporation sub-model based on the work of O Rourke et al. (SAE Paper ) We have chosen to focus our work on the accuracy of the implementation of the model and on the resolution of the numerical issue that could arise.
3 WALL FILM THE PHYSICAL ISSUE WALL INTERACTION SPRAY GAS Two-dimensional flux over three-dimensional surfaces Impinging i i Spray Heat transfer with wall and gas Fuel evaporation Gravity and other body forces Shear forces at the interface with gas and wall
4 WALL FILM NUMERICAL MODEL HYPOTHESIS Boundary-layer approximation Laminar Flow Incompressible Flow Newtonian Fluid The equations of mass, momentum and energy are written and integrated q gy g following a finite volume approach. Because of the variation of mass inside a control volume these equations resemble a virtual compressibility.
5 INTEGRAL CONTINUITY EQUATION Nside Δ δ 1 ˆ S + ( V r ) d f n δili = Δt A i ρ A w i In order to underline the variable film height htused in the numerical solution, the equation is divided by ρa w The time derivative of film height in a control volume is related to the convective fluxes and to the interaction with gas and spray through the source terms S d w S d S s d S t d Spray-film interaction Film evaporation
6 SPRAY-WALL INTERACTION The impingement regime is a function of the Weber number (According to Stanton et. al SAE ) We = We 5 ρ du d σ 2 nd 5< We ρ < We 18.0 d d ν f σ ρ d d ν f < We σ The wall film model does not distinguish between different impact regimes. The droplets are supposed to adhere to the wall.
7 Δ ( δv f ) INTEGRAL MOMENTUM EQUATION r 1 Nside r r ˆ 1 Nside 1 1 Nedge r r r + Vf Vf n δil i = pn δil i+ δg + M tan + τia i t A i ρa ρa ρa ( ) ( ˆ ) ( ) Δ w i w i w w i z y Imposed the condition of film adhesion to the wall Different influences of the normal component of the impinging i i droplet velocity from the tangential ti one x A relative system of coordinates has been created
8 Δ r FILM PRESSURE DEFINITION ( δvδ V ) 1 Nside ( ) 1 Nside ( ) 1 1 Nedge f r r r r r + V ˆ ˆ f Vf n δili = pnδili+ δg+ Mtan + ( τiai) Δt A ρa ρa ρa i w i w i w w i p= p + p g d Pressure of the surrounding gas Dynamic pressure due the impinging droplets p d n = 4πρ A 1 ru ini t 3 i w i= Δ 1 The time-step used in calculations could be 3 longer or shorter than the duration of the droplet impingement. We choose to consider that the duration of the impact is equal to the computational timestep Δt
9 PRESSURE GRADIENT TERM ( δv Nside Nside Nedge f ) + 1 V ( ˆ) 1 ( ˆ) 1 1 f Vf n δili = pnδili+ δg r r + Mtan + ( τiai) Δ r r r r Δt A ρa ρa ρa i w i w i w w i p g p p The pressure gradient contribution to momentum of the j-th cell involves the valuation of pressure at the boundary faces. The different film heights between neighbour cells must be taken into account by appling the film pressure only over the common contact area, while the gas pressure is applied over the remaining boundary area
10 INTEGRAL ENERGY EQUATION ( ) Nside Δ δt 1 J i ˆ g Jw SH + T ( V r ) f n δi li = + Δt A ρca ρca ρca The film exchange: w i i p w p w p w Convective heat transfer with the gas (J g ) Conductive heat transfer with the wall (J w ) Energy with the spray (S h ) Fuel vaporization alters the structure of the turbulent boundary layer above the film because of the gas velocity normal to the wall induced by the vaporization. The wall film energy equation is integrated over the control volume with the hypothesis of parabolic temperature profile across the film height M difi d ll f ti i d t l l t th ll fil i ti t Modified wall functions are use in order to calculate the wall film vaporization rate (Stanton et al. SAE )
11 INTEGRATION METHOD - ALE The discretized equations are solved with an Arbitrary Lagrangian Eulerian (ALE) methodology with a fully explicit approach The diffusive terms in direction tangential to the wall are neglegible compared to convective terms. The high Peclet number justifies the use a first order upwind differencing scheme LAGRANGIAN PHASE δ φ = δ φ + S Δt L L n n L φ During the Lagrangian phase the computational cell moves with fluid and source terms are accounted for uur δ φ δ φ t φ V n δ l Nside n+ 1 n + 1 L L L L = +Δ ( ˆ f ) EULERIAN PHASE i= 1 i f i i i In the Eulerian phase the flow is frozen and remapped onto the computational In the Eulerian phase the flow is frozen and remapped onto the computational grid
12 FILM-GAS INTERFACE AT BOUNDARY EDGE The main limits of a continuous finite volume approach of the film models are at the boundary edges of the liquid phase: the approximation of constant film height over the control volume does not permit to reconstruct the characteristics of the interface. Real gas-film interface of boundary edge Computed gas-film interface of boundary edge This scattering of liquid film causes high numerical diffusion and an overextimation of evaporation, which is proportional to the area of contact with gas.
13 FILM-GAS INTERFACE AT BOUNDARY EDGE In order to reproduce the effect of surface tension a fitting minimum threshold value is used to impose a minimum film height into a control volume Real interface Computed with threshold Yes No Min Height The convective fluxes are inhibited according to a double control on the minimum film height of two neighbour cells The area at the interface with gas is calculated by supposing that all the fluid inside the control volume has the minimum film height, avoiding the overextimation of wall film evaporation.
14 KIVA3 The wall film model has been implemented in our customized version of the KIVA3 code. The code has been updated regarding the combustion sub-models: Shell ignition model (Kong et al.) Characteristic-time combustion model (Abraham et al.), modified with the correction proposed by Bianchi et al. And the spray break-up and evaporation sub-models: Liquid jet and atomization model Hybrid model (Bianchi et al.) CLE coupling between gas and liquid phase (Beard et al.)
15 VALIDATION The wall film model has been tested against two cases that are representative of different wall film formation and dynamics : Diesel Engine (Single injection DI Engine) Pipe with pulsed injection (PFI-like condition) Both cases are choosen because the impact regime is prevalently sticky
16 VALIDATION DIESEL ENGINE SIMULATION Stanton et al. (SAE ) Two-Stroke DI Diesel Engine Simulation between IVC and EVO Injection and Combustion simulation Bore 150 mm Stroke 225 mm Number of cylinders 8 Engine speed 750 rpm Compression ratio 14 Fuel Diesel Wall temperature 673 K Inlet air pressure 2.94 bar Injected mass 12.3 mg/cycle Start of injection -19 ATDC Duration of injection 19 C.A. Injection pressure 174 bar Small angle between spray direction and bowl wall Prevalent impinging regime is Stick
17 VALIDATION DIESEL ENGINE SIMULATION Sensors position Sensor 1 Sensor 5 Sensor 3
18 VALIDATION PFI GASOLINE ENGINE Le Coz et al. (7th Int. Symp. on Application of Laser Techniques to Fluid Mechanics) Sauter Mean Diameter Droplet Velocity 90μm 16m/s Spray Cone Angle 30 Injection Duration 6.7ms Angle injector/tube 45 Injection frequency 40Hz Injected quantity per shot 21.5mm 3 Air flow rate 0.42m 3 /min Reproduces injection and liquid-film conditions similar to those occuring in PFI gasoline engines Pulsed injection with 8 injection events Characterized by low Weber number Prevalent impinging regime is Stick The experimental ldata has been compared with iththe result obtained dby Foucart et al. (SAE ) and by our model
19 VALIDATION PFI GASOLINE ENGINE Sensor 1 View Sensor 2
20 Wall film model comparison Evaluation of wall film models of other commercial CFD codes FLUENT v6.2 Lagrangian model with discrete particles transportation Model of interaction between particles and wall Equation of Mass, Momentum and Energy solved FIRE v8.4 Semi-implicit eulerian model Dynamic Mass and Energy equation Momentum equation with quasi stationary hupothesis
21 Comparision of wall film models of different commercial cfd code The wall film model in FLUENT intensifies the dynamic effect of spray impact on the momentum of wall film The evolution of the film far away from the impact zone is good The quasi stationary model of FIRE underextimate the dynamics of the film. The analysis of the equation of the model allows us identifying the cause in th elack of source terms of the momentum equation and to the quasi stationary HP of the velocity profiles imposed. The fully explicit model implemented in KIVA is y accurate in the prediction of film heigth and also well predicts the dynamics of the film
22 KIVA FIRE
23 Momentum equation in FIRE Quasi stationaty profiles Momentum equation
24 Wall Film - Conclusion A wall film model that also accounts for the spray-wall interaction has been implemented on our version of the KIVA3 code Particular attention has been given to the physics of the phenomenon and to the numerical and implementation issue that arise from its modelling The model resolves the film dynamic using an explicit integration method The model has been validated d against a PFI-like an Diesel engine case, giving good result both for the predicted film height and evaporation rate The model has been implemeted in FIRE (beta version)
25
RESEARCH PROJECTS. For more information about our research projects please contact us at: info@naisengineering.com
RESEARCH PROJECTS For more information about our research projects please contact us at: info@naisengineering.com Or visit our web site at: www.naisengineering.com 2 Setup of 1D Model for the Simulation
More informationCFD Simulation of HSDI Engine Combustion Using VECTIS
CFD Simulation of HSDI Engine Combustion Using VECTIS G. Li, S.M. Sapsford Ricardo Consulting Engineer s Ltd., Shoreham-by-Sea, UK ABSTRACT As part of the VECTIS code validation programme, CFD simulations
More informationME6130 An introduction to CFD 1-1
ME6130 An introduction to CFD 1-1 What is CFD? Computational fluid dynamics (CFD) is the science of predicting fluid flow, heat and mass transfer, chemical reactions, and related phenomena by solving numerically
More informationCONVERGE Features, Capabilities and Applications
CONVERGE Features, Capabilities and Applications CONVERGE CONVERGE The industry leading CFD code for complex geometries with moving boundaries. Start using CONVERGE and never make a CFD mesh again. CONVERGE
More informationLecture 16 - Free Surface Flows. Applied Computational Fluid Dynamics
Lecture 16 - Free Surface Flows Applied Computational Fluid Dynamics Instructor: André Bakker http://www.bakker.org André Bakker (2002-2006) Fluent Inc. (2002) 1 Example: spinning bowl Example: flow in
More informationExpress Introductory Training in ANSYS Fluent Lecture 1 Introduction to the CFD Methodology
Express Introductory Training in ANSYS Fluent Lecture 1 Introduction to the CFD Methodology Dimitrios Sofialidis Technical Manager, SimTec Ltd. Mechanical Engineer, PhD PRACE Autumn School 2013 - Industry
More informationComputational Fluid Dynamics (CFD) and Multiphase Flow Modelling. Associate Professor Britt M. Halvorsen (Dr. Ing) Amaranath S.
Computational Fluid Dynamics (CFD) and Multiphase Flow Modelling Associate Professor Britt M. Halvorsen (Dr. Ing) Amaranath S. Kumara (PhD Student), PO. Box 203, N-3901, N Porsgrunn, Norway What is CFD?
More informationIntroduction to CFD Analysis
Introduction to CFD Analysis 2-1 What is CFD? Computational Fluid Dynamics (CFD) is the science of predicting fluid flow, heat and mass transfer, chemical reactions, and related phenomena by solving numerically
More informationUse of OpenFoam in a CFD analysis of a finger type slug catcher. Dynaflow Conference 2011 January 13 2011, Rotterdam, the Netherlands
Use of OpenFoam in a CFD analysis of a finger type slug catcher Dynaflow Conference 2011 January 13 2011, Rotterdam, the Netherlands Agenda Project background Analytical analysis of two-phase flow regimes
More informationModeling of Diesel Fuel Spray Formation in OpenFOAM
Modeling of Diesel Fuel Spray Formation in OpenFOAM Anne Kösters (Chalmers Univ of Technology) Anders Karlsson (Volvo Technology Corporation) Motivation Sprays are involved in many applications (internal
More informationIntroduction to CFD Analysis
Introduction to CFD Analysis Introductory FLUENT Training 2006 ANSYS, Inc. All rights reserved. 2006 ANSYS, Inc. All rights reserved. 2-2 What is CFD? Computational fluid dynamics (CFD) is the science
More informationEXPERIMENTAL VALIDATION AND COMBUSTION CHAMBER GEOMETRY OPTIMIZATION OF DIESEL ENGINE BY USING DIESEL RK
INTERNATIONAL JOURNAL OF MECHANICAL ENGINEERING AND TECHNOLOGY (IJMET) International Journal of Mechanical Engineering and Technology (IJMET), ISSN 0976 6340(Print), ISSN 0976 6340 (Print) ISSN 0976 6359
More informationCustomer Training Material. Lecture 2. Introduction to. Methodology ANSYS FLUENT. ANSYS, Inc. Proprietary 2010 ANSYS, Inc. All rights reserved.
Lecture 2 Introduction to CFD Methodology Introduction to ANSYS FLUENT L2-1 What is CFD? Computational Fluid Dynamics (CFD) is the science of predicting fluid flow, heat and mass transfer, chemical reactions,
More informationDifferential Relations for Fluid Flow. Acceleration field of a fluid. The differential equation of mass conservation
Differential Relations for Fluid Flow In this approach, we apply our four basic conservation laws to an infinitesimally small control volume. The differential approach provides point by point details of
More informationNUMERICAL ANALYSIS OF THE EFFECTS OF WIND ON BUILDING STRUCTURES
Vol. XX 2012 No. 4 28 34 J. ŠIMIČEK O. HUBOVÁ NUMERICAL ANALYSIS OF THE EFFECTS OF WIND ON BUILDING STRUCTURES Jozef ŠIMIČEK email: jozef.simicek@stuba.sk Research field: Statics and Dynamics Fluids mechanics
More informationCFD SIMULATION OF SDHW STORAGE TANK WITH AND WITHOUT HEATER
International Journal of Advancements in Research & Technology, Volume 1, Issue2, July-2012 1 CFD SIMULATION OF SDHW STORAGE TANK WITH AND WITHOUT HEATER ABSTRACT (1) Mr. Mainak Bhaumik M.E. (Thermal Engg.)
More informationEngine Heat Transfer. Engine Heat Transfer
Engine Heat Transfer 1. Impact of heat transfer on engine operation 2. Heat transfer environment 3. Energy flow in an engine 4. Engine heat transfer Fundamentals Spark-ignition engine heat transfer Diesel
More informationTurbulence Modeling in CFD Simulation of Intake Manifold for a 4 Cylinder Engine
HEFAT2012 9 th International Conference on Heat Transfer, Fluid Mechanics and Thermodynamics 16 18 July 2012 Malta Turbulence Modeling in CFD Simulation of Intake Manifold for a 4 Cylinder Engine Dr MK
More informationFully Automatic In-cylinder Workflow Using HEEDS / es-ice / STAR-CD
Fully Automatic In-cylinder Workflow Using HEEDS / es-ice / STAR-CD Simon Fischer Senior ICE Application Support Engineer CD-adapco Nuremberg Office Gerald Schmidt Director/Powertrain - CD-adapco New York
More informationFlow distribution and turbulent heat transfer in a hexagonal rod bundle experiment
Flow distribution and turbulent heat transfer in a hexagonal rod bundle experiment K. Litfin, A. Batta, A. G. Class,T. Wetzel, R. Stieglitz Karlsruhe Institute of Technology Institute for Nuclear and Energy
More informationMultiphase Flow - Appendices
Discovery Laboratory Multiphase Flow - Appendices 1. Creating a Mesh 1.1. What is a geometry? The geometry used in a CFD simulation defines the problem domain and boundaries; it is the area (2D) or volume
More informationOptimization of Operating Parameters for a 2-stroke DI Engine with KIVA 3V and a Genetic Algorithm Search Technique
Optimization of Operating Parameters for a 2-stroke DI Engine with KIVA 3V and a Genetic Algorithm Search Technique Mark N. Subramaniam and Rolf D. Reitz Engine Research Center, University of Wisconsin-Madison
More informationDIESEL ENGINE IN-CYLINDER CALCULATIONS WITH OPENFOAM
DIESEL ENGINE IN-CYLINDER CALCULATIONS WITH OPENFOAM 1 Ervin Adorean *, 1 Gheorghe-Alexandru Radu 1 Transilvania University of Brasov, Romania KEYWORDS - diesel, engine, CFD, simulation, OpenFOAM ABSTRACT
More informationCFD MODELLING OF TOP SUBMERGED LANCE GAS INJECTION
CFD MODELLING OF TOP SUBMERGED LANCE GAS INJECTION Nazmul Huda PhD Student Faculty of Engineering and Industrial Science Swinburne University of Technology Melbourne, Australia Supervised by Dr. Jamal
More informationLecture 6 - Boundary Conditions. Applied Computational Fluid Dynamics
Lecture 6 - Boundary Conditions Applied Computational Fluid Dynamics Instructor: André Bakker http://www.bakker.org André Bakker (2002-2006) Fluent Inc. (2002) 1 Outline Overview. Inlet and outlet boundaries.
More informationMEL 807 Computational Heat Transfer (2-0-4) Dr. Prabal Talukdar Assistant Professor Department of Mechanical Engineering IIT Delhi
MEL 807 Computational Heat Transfer (2-0-4) Dr. Prabal Talukdar Assistant Professor Department of Mechanical Engineering IIT Delhi Time and Venue Course Coordinator: Dr. Prabal Talukdar Room No: III, 357
More informationA Common Engine Platform for Engine LES Development and Validation
A Common Engine Platform for Engine LES Development and Validation Volker Sick, D. Reuss, P. Abraham, A. Alharbi, O. Almagri, & H. Chen University of Michigan, Ann Arbor, MI, USA Chris Rutland & Y. Zhang,
More informationDimensional analysis is a method for reducing the number and complexity of experimental variables that affect a given physical phenomena.
Dimensional Analysis and Similarity Dimensional analysis is very useful for planning, presentation, and interpretation of experimental data. As discussed previously, most practical fluid mechanics problems
More informationContents. Microfluidics - Jens Ducrée Physics: Navier-Stokes Equation 1
Contents 1. Introduction 2. Fluids 3. Physics of Microfluidic Systems 4. Microfabrication Technologies 5. Flow Control 6. Micropumps 7. Sensors 8. Ink-Jet Technology 9. Liquid Handling 10.Microarrays 11.Microreactors
More informationAdaptation of General Purpose CFD Code for Fusion MHD Applications*
Adaptation of General Purpose CFD Code for Fusion MHD Applications* Andrei Khodak Princeton Plasma Physics Laboratory P.O. Box 451 Princeton, NJ, 08540 USA akhodak@pppl.gov Abstract Analysis of many fusion
More informationBasic Equations, Boundary Conditions and Dimensionless Parameters
Chapter 2 Basic Equations, Boundary Conditions and Dimensionless Parameters In the foregoing chapter, many basic concepts related to the present investigation and the associated literature survey were
More informationTWO-DIMENSIONAL FINITE ELEMENT ANALYSIS OF FORCED CONVECTION FLOW AND HEAT TRANSFER IN A LAMINAR CHANNEL FLOW
TWO-DIMENSIONAL FINITE ELEMENT ANALYSIS OF FORCED CONVECTION FLOW AND HEAT TRANSFER IN A LAMINAR CHANNEL FLOW Rajesh Khatri 1, 1 M.Tech Scholar, Department of Mechanical Engineering, S.A.T.I., vidisha
More informationCFD Based Air Flow and Contamination Modeling of Subway Stations
CFD Based Air Flow and Contamination Modeling of Subway Stations Greg Byrne Center for Nonlinear Science, Georgia Institute of Technology Fernando Camelli Center for Computational Fluid Dynamics, George
More informationDesign and Analysis of Engine Cooling Fan
International Journal of Current Engineering and Technology ISSN 2277-4106 2014 INPRESSCO. All Rights Reserved. Available at http://inpressco.com/category/ijcet Research Article Design and Analysis of
More informationPart IV. Conclusions
Part IV Conclusions 189 Chapter 9 Conclusions and Future Work CFD studies of premixed laminar and turbulent combustion dynamics have been conducted. These studies were aimed at explaining physical phenomena
More informationHEAT TRANSFER ANALYSIS IN A 3D SQUARE CHANNEL LAMINAR FLOW WITH USING BAFFLES 1 Vikram Bishnoi
HEAT TRANSFER ANALYSIS IN A 3D SQUARE CHANNEL LAMINAR FLOW WITH USING BAFFLES 1 Vikram Bishnoi 2 Rajesh Dudi 1 Scholar and 2 Assistant Professor,Department of Mechanical Engineering, OITM, Hisar (Haryana)
More informationDiesel injection, ignition, and fuel air mixing
Diesel injection, ignition, and fuel air mixing 1. Fuel spray phenomena. Spontaneous ignition 3. Effects of fuel jet and charge motion on mixingcontrolled combustion 4. Fuel injection hardware 5. Challenges
More informationGraduate Certificate Program in Energy Conversion & Transport Offered by the Department of Mechanical and Aerospace Engineering
Graduate Certificate Program in Energy Conversion & Transport Offered by the Department of Mechanical and Aerospace Engineering Intended Audience: Main Campus Students Distance (online students) Both Purpose:
More informationLecturer, Department of Engineering, ar45@le.ac.uk, Lecturer, Department of Mathematics, sjg50@le.ac.uk
39 th AIAA Fluid Dynamics Conference, San Antonio, Texas. A selective review of CFD transition models D. Di Pasquale, A. Rona *, S. J. Garrett Marie Curie EST Fellow, Engineering, ddp2@le.ac.uk * Lecturer,
More informationTurbulence, Heat and Mass Transfer (THMT 09) Poiseuille flow of liquid methane in nanoscopic graphite channels by molecular dynamics simulation
Turbulence, Heat and Mass Transfer (THMT 09) Poiseuille flow of liquid methane in nanoscopic graphite channels by molecular dynamics simulation Sapienza Università di Roma, September 14, 2009 M. T. HORSCH,
More informationRadial-axial Radial mixing is based on the premise that the fluids to be mixed enter the mixer in the correct proportions simultaneously
Brochure E-0501 1 Introduction. Static mixers are used for a wide range of applications including mixing, heat exchange and dispersion, due to numerous unique innovations our products are especially suitable
More informationCBE 6333, R. Levicky 1 Review of Fluid Mechanics Terminology
CBE 6333, R. Levicky 1 Review of Fluid Mechanics Terminology The Continuum Hypothesis: We will regard macroscopic behavior of fluids as if the fluids are perfectly continuous in structure. In reality,
More informationProblem Statement In order to satisfy production and storage requirements, small and medium-scale industrial
Problem Statement In order to satisfy production and storage requirements, small and medium-scale industrial facilities commonly occupy spaces with ceilings ranging between twenty and thirty feet in height.
More informationLES SIMULATION OF A DEVOLATILIZATION EXPERIMENT ON THE IPFR FACILITY
LES SIMULATION OF A DEVOLATILIZATION EXPERIMENT ON THE IPFR FACILITY F. Donato*, G. Rossi**, B. Favini**, E. Giacomazzi*, D. Cecere* F.R. Picchia*, N.M.S. Arcidiacono filippo.donato@enea.it * ENEA-UTTEI/COMSO
More informationBasic Principles in Microfluidics
Basic Principles in Microfluidics 1 Newton s Second Law for Fluidics Newton s 2 nd Law (F= ma) : Time rate of change of momentum of a system equal to net force acting on system!f = dp dt Sum of forces
More informationFluids and Solids: Fundamentals
Fluids and Solids: Fundamentals We normally recognize three states of matter: solid; liquid and gas. However, liquid and gas are both fluids: in contrast to solids they lack the ability to resist deformation.
More informationSet up and solve a transient problem using the pressure-based solver and VOF model.
Tutorial 18. Using the VOF Model This tutorial was run using ANSYS FLUENT 12.1. The results have been updated to reflect the change in the default setting of node-based smoothing for the surface tension
More informationEffect of Aspect Ratio on Laminar Natural Convection in Partially Heated Enclosure
Universal Journal of Mechanical Engineering (1): 8-33, 014 DOI: 10.13189/ujme.014.00104 http://www.hrpub.org Effect of Aspect Ratio on Laminar Natural Convection in Partially Heated Enclosure Alireza Falahat
More information1. Fluids Mechanics and Fluid Properties. 1.1 Objectives of this section. 1.2 Fluids
1. Fluids Mechanics and Fluid Properties What is fluid mechanics? As its name suggests it is the branch of applied mechanics concerned with the statics and dynamics of fluids - both liquids and gases.
More informationNUMERICAL INVESTIGATION OF HEAT AND MASS TRANSFER IN A REFRIGERATED TRUCK COMPARTMENT
NUMERICAL INVESTIGATION OF HEAT AND MASS TRANSFER IN A REFRIGERATED TRUCK COMPARTMENT T. LAFAYE DE MICHEAUX (a), V. SARTRE (a)*, A. STUMPF (b), J. BONJOUR (a) (a) Université de Lyon, CNRS INSA-Lyon, CETHIL,
More informationModeling and Simulation of Complex Multiphase Flows in the Pharmaceutical Industry
SIMNET Days 2010 Februar 10, 2010 Modeling and Simulation of Complex Multiphase Flows in the Pharmaceutical Industry D. Suzzi a, G. Toschkoff a, S. Radl a,b, Th. Hörmann a, M. Schaffer a, D. Machold a,
More informationRavi Kumar Singh*, K. B. Sahu**, Thakur Debasis Mishra***
Ravi Kumar Singh, K. B. Sahu, Thakur Debasis Mishra / International Journal of Engineering Research and Applications (IJERA) ISSN: 48-96 www.ijera.com Vol. 3, Issue 3, May-Jun 3, pp.766-77 Analysis of
More informationFUNDAMENTALS OF ENGINEERING THERMODYNAMICS
FUNDAMENTALS OF ENGINEERING THERMODYNAMICS System: Quantity of matter (constant mass) or region in space (constant volume) chosen for study. Closed system: Can exchange energy but not mass; mass is constant
More informationNumerical Investigation of Heat Transfer Characteristics in A Square Duct with Internal RIBS
merical Investigation of Heat Transfer Characteristics in A Square Duct with Internal RIBS Abhilash Kumar 1, R. SaravanaSathiyaPrabhahar 2 Mepco Schlenk Engineering College, Sivakasi, Tamilnadu India 1,
More informationAeroacoustic Analogy for the Computation of Aeroacoustic Fields in Partially Closed Domains
INSTITUT FÜR MECHANIK UND MECHATRONIK Messtechnik und Aktorik Aeroacoustic Analogy for the Computation of Aeroacoustic Fields in Partially Closed Domains A. Hüppe 1, M. Kaltenbacher 1, A. Reppenhagen 2,
More informationCE 204 FLUID MECHANICS
CE 204 FLUID MECHANICS Onur AKAY Assistant Professor Okan University Department of Civil Engineering Akfırat Campus 34959 Tuzla-Istanbul/TURKEY Phone: +90-216-677-1630 ext.1974 Fax: +90-216-677-1486 E-mail:
More informationINTRODUCTION SOME USES OF SPRAY NOZZLES INTRODUCTION TYPES OF SPRAY NOZZLES
SOME USES OF SPRAY NOZZLES It is important that the nozzle you select is appropriate for your particular application Liquid sprays are used in a seemingly endless variety of applications Some of the more
More informationGCMs with Implicit and Explicit cloudrain processes for simulation of extreme precipitation frequency
GCMs with Implicit and Explicit cloudrain processes for simulation of extreme precipitation frequency In Sik Kang Seoul National University Young Min Yang (UH) and Wei Kuo Tao (GSFC) Content 1. Conventional
More informationCh 2 Properties of Fluids - II. Ideal Fluids. Real Fluids. Viscosity (1) Viscosity (3) Viscosity (2)
Ch 2 Properties of Fluids - II Ideal Fluids 1 Prepared for CEE 3500 CEE Fluid Mechanics by Gilberto E. Urroz, August 2005 2 Ideal fluid: a fluid with no friction Also referred to as an inviscid (zero viscosity)
More informationEffect of Pressure Ratio on Film Cooling of Turbine Aerofoil Using CFD
Universal Journal of Mechanical Engineering 1(4): 122-127, 2013 DOI: 10.13189/ujme.2013.010403 http://www.hrpub.org Effect of Pressure Ratio on Film Cooling of Turbine Aerofoil Using CFD Vibhor Baghel
More informationOverset Grids Technology in STAR-CCM+: Methodology and Applications
Overset Grids Technology in STAR-CCM+: Methodology and Applications Eberhard Schreck, Milovan Perić and Deryl Snyder eberhard.schreck@cd-adapco.com milovan.peric@cd-adapco.com deryl.snyder@cd-adapco.com
More informationdu u U 0 U dy y b 0 b
BASIC CONCEPTS/DEFINITIONS OF FLUID MECHANICS (by Marios M. Fyrillas) 1. Density (πυκνότητα) Symbol: 3 Units of measure: kg / m Equation: m ( m mass, V volume) V. Pressure (πίεση) Alternative definition:
More informationTHERMAL STRATIFICATION IN A HOT WATER TANK ESTABLISHED BY HEAT LOSS FROM THE TANK
THERMAL STRATIFICATION IN A HOT WATER TANK ESTABLISHED BY HEAT LOSS FROM THE TANK J. Fan and S. Furbo Abstract Department of Civil Engineering, Technical University of Denmark, Brovej, Building 118, DK-28
More informationHeat Transfer Prof. Dr. Ale Kumar Ghosal Department of Chemical Engineering Indian Institute of Technology, Guwahati
Heat Transfer Prof. Dr. Ale Kumar Ghosal Department of Chemical Engineering Indian Institute of Technology, Guwahati Module No. # 04 Convective Heat Transfer Lecture No. # 03 Heat Transfer Correlation
More informationCOMPUTATIONAL FLOW MODEL OF WESTFALL'S 4000 OPEN CHANNEL MIXER 411527-1R1. By Kimbal A. Hall, PE. Submitted to: WESTFALL MANUFACTURING COMPANY
COMPUTATIONAL FLOW MODEL OF WESTFALL'S 4000 OPEN CHANNEL MIXER 411527-1R1 By Kimbal A. Hall, PE Submitted to: WESTFALL MANUFACTURING COMPANY FEBRUARY 2012 ALDEN RESEARCH LABORATORY, INC. 30 Shrewsbury
More informationCoupling Forced Convection in Air Gaps with Heat and Moisture Transfer inside Constructions
Coupling Forced Convection in Air Gaps with Heat and Moisture Transfer inside Constructions M. Bianchi Janetti 1, F. Ochs 1 and R. Pfluger 1 1 University of Innsbruck, Unit for Energy Efficient Buildings,
More informationFluid Mechanics: Static s Kinematics Dynamics Fluid
Fluid Mechanics: Fluid mechanics may be defined as that branch of engineering science that deals with the behavior of fluid under the condition of rest and motion Fluid mechanics may be divided into three
More informationDr Jagannath K Professor, Dept of Mechanical and Mfg Engg, MIT Manipal, Manipal University, India
Dr Jagannath K Professor, Dept of Mechanical and Mfg Engg, MIT Manipal, Manipal University, India 1 Nucleate Boiling Nucleate Boiling is an efficient mode of heat transfer. It has useful application in
More informationCOMPUTATIONAL FLUID DYNAMICS (CFD) ANALYSIS OF INTERMEDIATE PRESSURE STEAM TURBINE
Research Paper ISSN 2278 0149 www.ijmerr.com Vol. 3, No. 4, October, 2014 2014 IJMERR. All Rights Reserved COMPUTATIONAL FLUID DYNAMICS (CFD) ANALYSIS OF INTERMEDIATE PRESSURE STEAM TURBINE Shivakumar
More informationFLUID DYNAMICS. Intrinsic properties of fluids. Fluids behavior under various conditions
FLUID DYNAMICS Intrinsic properties of fluids Fluids behavior under various conditions Methods by which we can manipulate and utilize the fluids to produce desired results TYPES OF FLUID FLOW Laminar or
More informationAN EFFECT OF GRID QUALITY ON THE RESULTS OF NUMERICAL SIMULATIONS OF THE FLUID FLOW FIELD IN AN AGITATED VESSEL
14 th European Conference on Mixing Warszawa, 10-13 September 2012 AN EFFECT OF GRID QUALITY ON THE RESULTS OF NUMERICAL SIMULATIONS OF THE FLUID FLOW FIELD IN AN AGITATED VESSEL Joanna Karcz, Lukasz Kacperski
More informationA. Hyll and V. Horák * Department of Mechanical Engineering, Faculty of Military Technology, University of Defence, Brno, Czech Republic
AiMT Advances in Military Technology Vol. 8, No. 1, June 2013 Aerodynamic Characteristics of Multi-Element Iced Airfoil CFD Simulation A. Hyll and V. Horák * Department of Mechanical Engineering, Faculty
More informationHYBRID ROCKET TECHNOLOGY IN THE FRAME OF THE ITALIAN HYPROB PROGRAM
8 th European Symposium on Aerothermodynamics for space vehicles HYBRID ROCKET TECHNOLOGY IN THE FRAME OF THE ITALIAN HYPROB PROGRAM M. Di Clemente, R. Votta, G. Ranuzzi, F. Ferrigno March 4, 2015 Outline
More informationNUMERICAL SIMULATION OF FLOW FIELDS IN CASE OF FIRE AND FORCED VENTILATION IN A CLOSED CAR PARK
FACULTY OF ENGINEERING NUMERICAL SIMULATION OF FLOW FIELDS IN CASE OF FIRE AND FORCED VENTILATION IN A CLOSED CAR PARK Xavier Deckers, Mehdi Jangi, Siri Haga and Bart Merci Department of Flow, Heat and
More informationTHE USE OF AIR ATOMIZING NOZZLES TO PRODUCE SPRAYS WITH FINE DROPLETS
14th International Water Mist Conference THE USE OF AIR ATOMIZING NOZZLES TO PRODUCE SPRAYS WITH FINE DROPLETS Dr.Gökhan BALIK Etik Muhendislik Danismanlik Tasarim ve Egitim Hizmetleri Ltd.Şti. Istanbul
More informationComputational Fluid Dynamics (CFD) Markus Peer Rumpfkeil
Computational Fluid Dynamics (CFD) Markus Peer Rumpfkeil January 13, 2014 1 Let's start with the FD (Fluid Dynamics) Fluid dynamics is the science of fluid motion. Fluid flow is commonly studied in one
More informationIntroduction to Computational Fluid Dynamics (CFD) for Combustion. www.reaction-eng.com (801) 364-6925
Introduction to Computational Fluid Dynamics (CFD) for Combustion www.reaction-eng.com (801) 364-6925 What is CFD? CFD stands for Computational Fluid Dynamics CFD uses computers to represent (or model)
More informationA NODAL MODEL FOR DISPLACEMENT VENTILATION AND CHILLED CEILING SYSTEMS IN OFFICE SPACES
A NODAL MODEL FOR DISPLACEMENT VENTILATION AND CHILLED CEILING SYSTEMS IN OFFICE SPACES Simon J. Rees and Philip Haves School of Mechanical & Aerospace Engineering, Oklahoma State University, Stillwater,
More informationA COMPUTATIONAL FLUID DYNAMICS STUDY ON THE ACCURACY OF HEAT TRANSFER FROM A HORIZONTAL CYLINDER INTO QUIESCENT WATER
A COMPUTATIONAL FLUID DYNAMICS STUDY ON THE ACCURACY OF HEAT TRANSFER FROM A HORIZONTAL CYLINDER INTO QUIESCENT WATER William Logie and Elimar Frank Institut für Solartechnik SPF, 8640 Rapperswil (Switzerland)
More informationCFD Grows Up! Martin W. Liddament Ventilation, Energy and Environmental Technology (VEETECH Ltd) What is Computational Fluid Dynamics?
CIBSE/ASHRAE Meeting CFD Grows Up! Martin W. Liddament Ventilation, Energy and Environmental Technology (VEETECH Ltd) 10 th December 2003 What is Computational Fluid Dynamics? CFD is a numerical means
More informationThe ADREA-HF CFD code An overview
The ADREA-HF CFD code An overview Dr. A.G. Venetsanos Environmental Research Laboratory (EREL) National Centre for Scientific Research Demokritos, Greece venets@ipta.demokritos.gr Slide 2 Computational
More informationOpenFOAM Opensource and CFD
OpenFOAM Opensource and CFD Andrew King Department of Mechanical Engineering Curtin University Outline What is Opensource Software OpenFOAM Overview Utilities, Libraries and Solvers Data Formats The CFD
More informationEco Pelmet Modelling and Assessment. CFD Based Study. Report Number 610.14351-R1D1. 13 January 2015
EcoPelmet Pty Ltd c/- Geoff Hesford Engineering 45 Market Street FREMANTLE WA 6160 Version: Page 2 PREPARED BY: ABN 29 001 584 612 2 Lincoln Street Lane Cove NSW 2066 Australia (PO Box 176 Lane Cove NSW
More informationGEOMETRIC, THERMODYNAMIC AND CFD ANALYSES OF A REAL SCROLL EXPANDER FOR MICRO ORC APPLICATIONS
2 nd International Seminar on ORC Power Systems October 7 th & 8 th, 213 De Doelen, Rotterdam, NL GEOMETRIC, THERMODYNAMIC AND CFD ANALYSES OF A REAL SCROLL EXPANDER FOR MICRO ORC APPLICATIONS M. Morini,
More informationLecture 3 Fluid Dynamics and Balance Equa6ons for Reac6ng Flows
Lecture 3 Fluid Dynamics and Balance Equa6ons for Reac6ng Flows 3.- 1 Basics: equations of continuum mechanics - balance equations for mass and momentum - balance equations for the energy and the chemical
More informationNUMERICAL INVESTIGATIONS ON HEAT TRANSFER IN FALLING FILMS AROUND TURBULENCE WIRES
NUMERICAL INVESTIGATIONS ON HEAT TRANSFER IN FALLING FILMS AROUND TURBULENCE WIRES Abstract H. Raach and S. Somasundaram Thermal Process Engineering, University of Paderborn, Paderborn, Germany Turbulence
More informationInnovation with CFD. Solutions and Equipment
Innovation with CFD Solutions and Equipment 2 Innovation with CFD Why our customers choose us According to our customers, we: Possess exceptional experience in our chosen technologies Possess unique abilities
More informationChapter 10. Flow Rate. Flow Rate. Flow Measurements. The velocity of the flow is described at any
Chapter 10 Flow Measurements Material from Theory and Design for Mechanical Measurements; Figliola, Third Edition Flow Rate Flow rate can be expressed in terms of volume flow rate (volume/time) or mass
More informationVISUAL PHYSICS School of Physics University of Sydney Australia. Why do cars need different oils in hot and cold countries?
VISUAL PHYSICS School of Physics University of Sydney Australia FLUID FLOW VISCOSITY POISEUILLE'S LAW? Why do cars need different oils in hot and cold countries? Why does the engine runs more freely as
More informationTHE CFD SIMULATION OF THE FLOW AROUND THE AIRCRAFT USING OPENFOAM AND ANSA
THE CFD SIMULATION OF THE FLOW AROUND THE AIRCRAFT USING OPENFOAM AND ANSA Adam Kosík Evektor s.r.o., Czech Republic KEYWORDS CFD simulation, mesh generation, OpenFOAM, ANSA ABSTRACT In this paper we describe
More information4.What is the appropriate dimensionless parameter to use in comparing flow types? YOUR ANSWER: The Reynolds Number, Re.
CHAPTER 08 1. What is most likely to be the main driving force in pipe flow? A. Gravity B. A pressure gradient C. Vacuum 2.What is a general description of the flow rate in laminar flow? A. Small B. Large
More informationCFD Simulation of Subcooled Flow Boiling using OpenFOAM
Research Article International Journal of Current Engineering and Technology E-ISSN 2277 4106, P-ISSN 2347-5161 2014 INPRESSCO, All Rights Reserved Available at http://inpressco.com/category/ijcet CFD
More informationINTERNATIONAL JOURNAL OF MECHANICAL ENGINEERING AND TECHNOLOGY (IJMET)
INTERNATIONAL JOURNAL OF MECHANICAL ENGINEERING AND TECHNOLOGY (IJMET) Proceedings of the 2 nd International Conference on Current Trends in Engineering and Management ICCTEM -2014 ISSN 0976 6340 (Print)
More informationAbaqus/CFD Sample Problems. Abaqus 6.10
Abaqus/CFD Sample Problems Abaqus 6.10 Contents 1. Oscillatory Laminar Plane Poiseuille Flow 2. Flow in Shear Driven Cavities 3. Buoyancy Driven Flow in Cavities 4. Turbulent Flow in a Rectangular Channel
More information13th Multiphase Flow Conference and Short Course: Simulation, Experiment and Application Dresden, 24-26 November 2015
Tuesday, 24 November 2015 Short Course on Multiphase Flows 08:30 09:15 Registration 09:15 09:25 D. Lucas Rossendorf Welcome 09:25 10:20 G. Scheuerer ANSYS Germany, Otterfing Mathematical Models for Multiphase
More informationEngine Efficiency and Power Density: Distinguishing Limits from Limitations
Engine Efficiency and Power Density: Distinguishing Limits from Limitations Chris F. Edwards Advanced Energy Systems Laboratory Department of Mechanical Engineering Stanford University Exergy to Engines
More informationDevelopment of Ventilation Strategy in Diesel Engine Power Plant by Using CFD Modelling
Development of Ventilation Strategy in Diesel Engine Power Plant by Using CFD Modelling Panu Mustakallio and Risto Kosonen Halton Oy, Haltonintie 1-3, 47400 Kausala, Finland E-mail: panu.mustakallio@halton.com
More informationCFD: What is it good for?
CFD: What is it good for? Tom O Mahoney TNO Fluid Dynamics Introduction to CFD CFD - Computational Fluid Dynamics Computational the using of computers to simulate the physics of fluids Fluid Either gas
More informationEngineering, Bharathiyar College of Engineering and Technology, Karaikal, Pondicherry 609 609, India
74 The Open Fuels & Energy Science Journal, 2008, 1, 74-78 Open Access Some Comparative Performance and Emission Studies on DI Diesel Engine Fumigated with Methanol and Methyl Ethyl Ketone Using Microprocessor
More information