VI. Computational Fluid Dynamics 1. Examples of numerical simulation

Similar documents
Calculation of the Resistance of a Ship Mathematical Formulation. Calculation of the Resistance of a Ship Mathematical Formulation

SMS-618, Particle Dynamics, Fall 2003 (E. Boss, last updated: 10/8/2003) Conservation equations in fluids

Cartesian tensors. Order (rank) Scalar. Vector. 3x3 matrix

PECULIARITIES OF THE LIQUID CARGO DYNAMICS MODELING FOR THE CASE OF ROAD TANK TRANSIENT MOVEMENT MODES

Modelling of test case particle-laden jet with NEPTUNE_CFD

Outline. Review Solution Approaches. Review Basic Equations. Nature of Turbulence. Review Fluent Exercise. Turbulence Models

11/11/2017. Randal W. Samstag, MS, PE, BCEE Civil and Sanitary Engineer Bainbridge Island, WA US

Turbulence Modelling (CFD course)

Prediction of Wing Downwash Using CFD

CFD Analysis of Aerodynamic Drag Effects on Vacuum Tube Trains

CFD Modelling of Indoor Air Quality and Thermal Comfort

Numerical Simulation Of Three-dimension Unsteady Flow In The Compression Chambers Of A Scroll Compressor

Chapter 1 Introduction of boundary layer phenomena

Material Point Method Investigations of Trauma to Fluids and Elastic Solids Due to Finite Barriers

Numerical simulation of flow reattachment length in a stilling basin with a step-down floor

ME 321: FLUID MECHANICS-I

Separated Turbulent Flow Simulations Using a Reynolds Stress Model and Unstructured Meshes

Sound Transmission Throough Lined, Composite Panel Structures: Transversely Isotropic Poro- Elastic Model

OPTIMIZATION OF A NONCONVENTIONAL ENGINE EVAPORATOR

Improvement of Two-Equation Turbulence Model with Anisotropic Eddy-Viscosity for Hybrid Rocket Research

Vorticity equation 2. Why did Charney call it PV?

by Lauren DeDieu Advisor: George Chen

ME 425: Aerodynamics

Eulerian multiphase flow model

Module 6. Lecture 2: Navier-Stokes and Saint Venant equations

11/11/2017. Randal W. Samstag, MS, PE, BCEE Civil and Sanitary Engineer Bainbridge Island, WA US

Chapter 2. Review of Hydrodynamics and Vector Analysis

Fundamentals of Flame Stabilities. Fundamentals of Flame Stabilities Lecture Notes 3

International Journal of Engineering Trends and Technology (IJETT) Volume 42 Number-8 - December 2016

2.1 Constitutive Theory

Comparison between two solar tower receivers of different geometry

CFD MODELING FOR HELIUM RELEASES IN A PRIVATE GARAGE WITHOUT FORCED VENTILATION

PHYS 1443 Section 001 Lecture #4

Chapter 3: Vectors and Two-Dimensional Motion

The Euler-Lagrange Approach for Steady and Unsteady Flows. M. Sommerfeld. www-mvt.iw.uni-halle.de. Title. Zentrum für Ingenieurwissenschaften

The Elastic Wave Equation. The elastic wave equation

ME 425: Aerodynamics

CONSISTENT EARTHQUAKE ACCELERATION AND DISPLACEMENT RECORDS

Supporting Information for Self-Propelled Nanomotors Autonomously Seek and Repair Cracks

Numerical Simulation on Wind Flow over Step-shaped Cliff Topography with Rough Surface

Notes on the stability of dynamic systems and the use of Eigen Values.

8. TURBULENCE MODELLING IN CFD SPRING 2007

Free Convective Flow of a Visco-Elastic Fluid Bounded By an Oscillating Porous Flat Plate in Slip Flow Regime

Motion in Two Dimensions

Background and Motivation: Importance of Pressure Measurements

Turbulence Closure Schemes

Computational Fluid Dynamics. Computational Methods for Domains with Complex Boundaries

J i-1 i. J i i+1. Numerical integration of the diffusion equation (I) Finite difference method. Spatial Discretization. Internal nodes.

Solution of a diffusion problem in a non-homogeneous flow and diffusion field by the integral representation method (IRM)

OUTLINE FOR Chapter 2-2. Basic Laws

A comparison of Lagrangian dispersion models coupled to a meteorological model for high stack air pollution forecast

Method of Moment Area Equations

Chiral Dynamics and Peripheral Transverse Densities

WALAILAK JOURNAL OF SCIENCE AND TECHNOLOGY

Normal Random Variable and its discriminant functions

Motion analysis and joint angle measurement of skier gliding on the actual snow field using inertial sensors

Observer Design for Nonlinear Systems using Linear Approximations

Wall treatment in Large Eddy Simulation

Available online at ScienceDirect. Procedia Engineering 90 (2014 )

Large-Eddy Simulation of a Circular Cylinder on Unstructured Grids

II The Z Transform. Topics to be covered. 1. Introduction. 2. The Z transform. 3. Z transforms of elementary functions

Electromagnetic energy, momentum and forces in a dielectric medium with losses

Comprehensive Integrated Simulation and Optimization of LPP for EUV Lithography Devices

NATURAL CONVECTION No mechanical force to push the fluid pump, fan etc. No predefined fluid flowrate and velocity can t prescribe Reynolds

Advanced time-series analysis (University of Lund, Economic History Department)

( ) G. Narsimlu Department of Mathematics, Chaitanya Bharathi Institute of Technology, Gandipet, Hyderabad, India

Derivation of the basic equations of fluid flows. No. Conservation of mass of a solute (applies to non-sinking particles at low concentration).

Unsteady MHD Free Convective Flow Through Porous Media Past on Moving Vertical Plate with Variable Temperature and Viscous Dissipation

Block 5 Transport of solutes in rivers

Displacement, Velocity, and Acceleration. (WHERE and WHEN?)

The Development of a Three-Dimensional Material Point Method Computer Simulation Algorithm for Bullet Impact Studies

Methods of Improving Constitutive Equations

Chapters 2 Kinematics. Position, Distance, Displacement

Computation of Flow, Turbulence and Bed Evolution with Sand Waves

HEAT CONDUCTION PROBLEM IN A TWO-LAYERED HOLLOW CYLINDER BY USING THE GREEN S FUNCTION METHOD

Navier-Stokes Eqns. υ ρ. Conservative form momentum eqn; x-component only. u x. u y. p z. u x. uv y

A MODEL ORDER AND TIME-DELAY SELECTION METHOD FOR MIMO NON-LINEAR SYSTEMS AND IT S APPLICATION TO NEURAL MODELLING. D. W. Yu, J. B. GOMM AND D. L.

DEPTH-AVERAGED SHALLOW WATER EQUATIONS

Atmospheric Dynamics 11:670:324. Class Time: Tuesdays and Fridays 9:15-10:35

International Journal of Pure and Applied Sciences and Technology

THERMODYNAMICS 1. The First Law and Other Basic Concepts (part 2)

Unsteady laminar flow of visco-elastic fluid of second order type between two parallel plates

Stochastic Programming handling CVAR in objective and constraint

Dynamic Model of the Axially Moving Viscoelastic Belt System with Tensioner Pulley Yanqi Liu1, a, Hongyu Wang2, b, Dongxing Cao3, c, Xiaoling Gai1, d

An investigation of MHD Flows of Nanofluid over. an oscillating surface with Joule Heating

Heat and Mass Transfer on the Unsteady MHD Flow of Chemically Reacting Micropolar Fluid with Radiation and Joule Heating

Let s treat the problem of the response of a system to an applied external force. Again,

Comparative Study of Netonian Sinusoidal Blood Flow through Normal and Stenosed Carotid Artery

Dispersive Systems. 1) Schrödinger equation 2) Cubic Schrödinger 3) KdV 4) Discreterised hyperbolic equation 5) Discrete systems.

Bianchi Type II Stiff Fluid Tilted Cosmological Model in General Relativity

Simulation of Wind driven currents for continental shelf of Golestan Province (Iran)

Chapter Lagrangian Interpolation

Including the ordinary differential of distance with time as velocity makes a system of ordinary differential equations.

Effect of a Vector Wall on the Thermal Field in a SRU Thermal Reactor

DESIGN OF TENSION MEMBERS

CFD modeling of precipitation of nanoparticles in Confined Impinging Jet Reactors

ON THE ACCURACY OF NUMERICAL PREDICTION IN TRANSONIC-SUPERSONIC FLOW ARROUND MISSILES

Journal of Engineering Science and Technology Review 9 (4) (2016) Research Article

ESTIMATION OF DYNAMIC LINEAR MODELS IN SHORT PANELS WITH ORDINAL OBSERVATION

THE EFFECTS OF RADIATION ON UNSTEADY MHD CONVECTIVE HEAT TRANSFER PAST A SEMI-INFINITE VERTICAL POROUS MOVING SURFACE WITH VARIABLE SUCTION

Transcription:

VI. Comaonal Fld Dnamcs 1. Eamles of nmercal smlaon Eermenal Fas Breeder Reacor, JOYO, wh rmar of coolan sodm. Uer nner srcre Uer lenm Flow aern and emerare feld n reacor essel n flow coas down Core Hh ressre lenm Lower lenm Veloc ecors emerare conors

Vore Horse-shoe ore Londnal ore Flow Vorc n bondar laer on a fla lae Horse-shoe ore Flow Vore lnes and edd-scos conors

. Conseraon eqaons of mass, momenm, and ener.1 Eqaon of conn rae of ncrease of mass rae of mass n rae of mass o [ ] [ ]

or ne rae of mass addon er n olme b conecon rae of ncrease of mass er n olme D Larane derae or D D D D Larane derae Incomressble fld consan dens Sff: reea

. Eqaon of moon rae of ncrease of momenm rae of momenm n rae of momenm o eernal force on he fld rae of momenm n - rae of momenm o

eernal force on he fld h shear sress ressre and bod force rae of ncrease of momenm

hree dmensonal

Vecor eresson rae of ncrease of momenm er n olme ne rae of momenm addon er n olme b conecon ne rae of momenm addon er n olme b moleclar ransor eernal force on he fld er n olme D D or D D [ ]

3 Sress ensor 3 3

D D 3 D 3 D D D 3 D D 3

Naer-Soes eqaon D D Eler eqaon when D D

D D β β β Dmensonless arables,,,, 1 l l Non-dmensonal eresson 3 1 / / / 1 l l l D D β Re Gr Re 1 D D scos force nera force / / Re l l l V Renolds nmber 3 1 Gr β L Grashof nmber nera force force boanc / Re Gr 1 1 β β l

.3 Eqaon of ener f b eernal wor done on ssem rae of h b moleclar wor done on ssem rae of b moleclar hea addon ne rae of ener addon nernal nec and ne rae of l and nec of ncrease rae of ra b forces b sresses mechansms condcon ransor ransor b conece ener addon ener nernal U 1 [ ] [ ] [ ] e e e e e e e e e e e e

e e 1 e e U 1 1 U U q [ ] [ ] rae of ncrease of ener er n olme U rae of ncrease of nernal ener er n olme rae of ener addon er n olme b conecon rae of ener addon er n olme b hea condcon rae of wor done on fld er n olme b ressre force [ U] q : ne rae of nernal ener addon er n olme b conecon rae of reersble nernal rae of ener nernal addon ener er n ncrease er olme b n olme hea b condcon comresson rae of wor done on fld er n olme b scos force rreersble rae of nernal ener ncrease er n olme b scos dssaon rae of wor done on fld er n olme b eernal force

D c λ λ D D D D c λ D Fld wh consan dens D D c λ c λ Q

.4 Dmensonless ros

Phscal nerreaon of dmensonless ros

3. Calclaon of rblen flow Wae of crclar clnder n waer flow Moon s sreled wh almnm owder.. Cebec, A. M. O. Smh, "Analss of rblen Bondar Laers," Aled Mahemacs and Mechancs 15, Academc Press 1974. F. 1.7 Insananeos eloc rofles n a rblen bondar laer on a fla lae Re1 5 5f from leadn ede, Measremen wh hdroen bbble mehod.. Cebec, A. M. O. Smh, "Analss of rblen Bondar Laers," Aled Mahemacs and Mechancs 15, Academc Press 1974. F. 1.3

Aal eloc flcaons measred wh a ho-wre Locaon: 56 n. from leadn ede,. n. off srface. Cebec, A. M. O. Smh, "Analss of rblen Bondar Laers," Aled Mahemacs and Mechancs 15, Academc Press 1974. F. 1.3 Insananeos eloc s searaed o meaerae one and flcaon comonen,, me

Relae rblence nenses alon a fla lae. Cebec, A. M. O. Smh, "Analss of rblen Bondar Laers," Aled Mahemacs and Mechancs 15, Academc Press 1974. F. 1.1

Eqaons of conn momenm and ener are me aeraed Eqaons of conn, momenm and ener are me-aeraed Sbsn In case of ncomressble fld Conn Renolds eqaon me-aeraed momenm eqaons D D 1 Renolds sress addonal erms

3.1 Prandl mn lenh model Edd dffs of momenm M M lenh eloc l M l m l Mn lenh κ l m on Karman s consan κ.41

on Karman Karmans consan κ.41 an Dress hohess near a wall 1/ 1/ 1 e w lm κ, A A 6. B.E. Lander, D. B. Saldn, Lecres n Maehemacal Models of rblence, Academc Press, 197. Nladses formla for e flow l m.14.81 R R 4.6 1, R Nladse. Cebec, A. M. O. Smh, "Analss of rblen Bondar Laers," Aled Mahemacs and Mechancs 15, Academc Press 1974. F. 4.15 3

. Cebec, A. M. O. Smh, "Analss of rblen Bondar Laers," Aled Mahemacs and Mechancs 15, Academc Press 1974. F. 4.16 Edd dffs M n e flow Problems of Prandl s mn lenh model - I s dffcl o redc recrclan flow wh ero eloc raden where sress and eloc raden are comlcaed. - I aes no accon of rocesses of conecon or dffson of rblence 4

. Renolds aerae rblence model.1 One eqaon model of rblence Renolds sresses R rblence ener 1/ 1 Momenm eqaons for,, are meaeraed and smmed. l R D D

D D

/ Aromaon l C σ 1/ Local soro, 3/ l C D C D 3/ l C D D σ

. wo-eqaon model of rblence rblence ener rblence model low Renolds nmber model Jones-Lander s model 197 rblence ener 1/ M M M σ Dssaon rae 1 1. f C f C M M M σ Edd dffs f M C Hh Renolds nmber model: las erms nder bar are omed.

f 1 1. f f 1..3e e R [.5 1 R 5 ] Renolds nmber of rblence R C C1 C σ Jones-Lander 9.9 155 1.55. 1 1. 13 1.3 Bondar condons rblence model low Renolds nmber model σ on sold wall rblence model hh Renolds nmber model 3 1 C 1 C on sold wall C κ Veloc rofle near sold wall: Lo law

rblence model rblence ener rblence model be cee e M D D Dssaon rae σ D σ f C C D D 1 Renolds sress σ D Edd dffs δ 3 f M C

Naano-aawa model where Abe e al. model where f 1 e 6 1 4.1 3 / 4 1 e f Renolds nmber of rblence R f 6 e 14 R, R 1.3e 6.5 Frcon eloc 5 R 1 e, 3 / 4 R 1 R f 1 e 1.3e 3.1 1/ 4 w 6.5 R

Model consans C 1 σ σ C C Naano-aawa.9 1.45 1.9 1.4 1.3 Abe e al..9 1.5 1.9 1.4 1.4

Problem 5 Dere ma r 1 R 1/ 7 sn he follown eqaons: w.3955 3 5, for 3 1 < Re < 1 1/ 4 Re d where Re n,,, w

Problem 6 Dere.5ln C sn he follown eqaons: l m l m κκ κ. 4,, w