Source: A. Mason-Jones, PhD thesis Cardiff University (2010) Moving Mesh ApproachTime-averaged Approach.

Slides:



Advertisements
Similar presentations
Boundary layer with pressure gradient in flow direction.
Advertisements

Introduction Irina Surface layer and surface fluxes Anton
Introduction to Computational Fluid Dynamics
School of Mechanical, Aerospace & Civil Engineering Postgraduate Research Conference, PGR-MACE10 Performance of two k T -k L -ω models in a separation-induced.
Instructor: André Bakker
TURBULENCE MODELING A Discussion on Different Techniques used in Turbulence Modeling -Reni Raju.
Section 2: The Planetary Boundary Layer
Turbulent Models.  DNS – Direct Numerical Simulation ◦ Solve the equations exactly ◦ Possible with today’s supercomputers ◦ Upside – very accurate if.
Separation in B.L.T. context
MODELLING OF CAVITATION FLOW IN A DIESEL INJECTION NOZZLE S. Martynov 1, D. Mason 2, M. Heikal 2 1 Department of Mechanical Engineering, University College.
External Convection: Laminar Flat Plate
Boundary Layer Flow Describes the transport phenomena near the surface for the case of fluid flowing past a solid object.
..perhaps the hardest place to use Bernoulli’s equation (so don’t)
Advanced CFD Analysis of Aerodynamics Using CFX
Generalities Separated Flows Wakes and Cavities. 1.1 What is separation ? A streamline leaves the body and turns into the interior of the fluid 2D separation.
Anisotropic Pressure and Acceleration Spectra in Shear Flow Yoshiyuki Tsuji Nagoya University Japan Acknowledgement : Useful discussions and advices were.
0.1m 10 m 1 km Roughness Layer Surface Layer Planetary Boundary Layer Troposphere Stratosphere height The Atmospheric (or Planetary) Boundary Layer is.
Eddy Viscosity Model Jordanian-German Winter Academy February 5 th -11 th 2006 Participant Name : Eng. Tareq Salameh Mechanical Engineering Department.
1 B. Frohnapfel, Jordanian German Winter Academy 2006 Turbulence modeling II: Anisotropy Considerations Bettina Frohnapfel LSTM - Chair of Fluid Dynamics.
Boundary Layer Meteorology Lecture 4 Turbulent Fluxes Energy Cascades Turbulence closures TKE Budgets.
CHE/ME 109 Heat Transfer in Electronics
DETAILED TURBULENCE CALCULATIONS FOR OPEN CHANNEL FLOW
Flow past bluff-bodies
Estimation of Prandtls Mixing Length
Chapter 15: Human Movement in a Fluid Medium
Suspended Load Above certain critical shear stress conditions, sediment particles are maintained in suspension by the exchange of momentum from the fluid.
Fluid Dynamics: Boundary Layers
FUNDAMENTAL EQUATIONS, CONCEPTS AND IMPLEMENTATION
CFD Modeling of Turbulent Flows
The Effect of Plugging Tubes on the Gas Mixing in AGR Boilers Alastair West 1 st Year EngD student.
Modeling Turbulent Flows
Boundary Layer Laminar Flow Re ‹ 2000 Turbulent Flow Re › 4000.
Chapter 9 Turbulence Introduction to CFX.
CFD Pre-Lab 2 Simulation of Turbulent Flow around an Airfoil Seong Mo Yeon, and Timur Dogan 11/12/2013.
Governing equations: Navier-Stokes equations, Two-dimensional shallow-water equations, Saint-Venant equations, compressible water hammer flow equations.
Basic Fluid Dynamics.
Momentum Equations in a Fluid (PD) Pressure difference (Co) Coriolis Force (Fr) Friction Total Force acting on a body = mass times its acceleration (W)
Turbulent properties: - vary chaotically in time around a mean value - exhibit a wide, continuous range of scale variations - cascade energy from large.
Mass Transfer Coefficient
Fluid Flow in Rivers Outline 1.Flow uniformity and steadiness 2.Newtonian fluids 3.Laminar and turbulent flow 4.Mixing-length concept 5.Turbulent boundary.
A canopy model of mean winds through urban areas O. COCEAL and S. E. BELCHER University of Reading, UK.
© Fluent Inc. 12/18/2015 D1 Fluent Software Training TRN Modeling Turbulent Flows.
Quantification of the Infection & its Effect on Mean Fow.... P M V Subbarao Professor Mechanical Engineering Department I I T Delhi Modeling of Turbulent.
Reynolds Analogy It can be shown that, under specific conditions (no external pressure gradient and Prandtle number equals to one), the momentum and heat.
CE 1501 Flow Over Immersed Bodies Reading: Munson, et al., Chapter 9.
MECH 221 FLUID MECHANICS (Fall 06/07) Chapter 8: BOUNDARY LAYER FLOWS
INTRODUCTION TO CONVECTION
Conference on PDE Methods in Applied Mathematics and Image Processing, Sunny Beach, Bulgaria, 2004 NUMERICAL APPROACH IN SOLVING THE PDE FOR PARTICULAR.
Scales of Motion, Reynolds averaging September 22.
BOUNDARY LAYERS Zone of flow immediately in vicinity of boundary Motion of fluid is retarded by frictional resistance Boundary layer extends away from.
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.
CONVECTION : An Activity at Solid Boundary P M V Subbarao Associate Professor Mechanical Engineering Department IIT Delhi Identify and Compute Gradients.
05:53 Fluid Mechanics Basic Concepts.
Turbulent Fluid Flow daVinci [1510].
External flow: drag and Lift
The Standard, RNG, and Realizable k- Models. The major differences in the models are as follows: the method of calculating turbulent viscosity the turbulent.
Introduction to the Turbulence Models
Ship Hydrodynamics - Resistance
K-ε model, ASM model.
Introduction to Symmetry Analysis
The k-ε model The k-ε model focuses on the mechanisms that affect the turbulent kinetic energy (per unit mass) k. The instantaneous kinetic energy k(t)
Flow Through a Pipe Elbow (Comsol)
Lecture Objectives Learn about Implementation of Boundary Conditions
Characteristics of Turbulence:
Fluid properties 1.
Lecture Objectives: Boundary Conditions Project 1 (software)
Lecture Objectives: Start using CFD Software Class project 1
Chapter 2 Navier-Stokes Modeling for HAWT by CFX 5.7
Turbulence 1: Turbulent Boundary layer
Presentation transcript:

Source: A. Mason-Jones, PhD thesis Cardiff University (2010) Moving Mesh ApproachTime-averaged Approach

0.5m 0.25m 1.4m 0.5m 1.54m 0.84m 0.17m 0.84m 0.17m

P∞P∞ P WAKE P 95% P∞P∞

k-epsilon Eddy viscosity from single length scale Turbulent diffusion occurs only at specified scale RNG k-epsilon Account for different scales of motion k-omega Viscous sub-layer flows Adverse pressure gradients and separating flows

Shear Stress Transport (SST) k-ω near boundary k-ε in free-stream Adverse pressure gradients & separating flows Reynolds Stress Model (RSM) Reynolds Stresses directly computed Directional effects of Reynolds stress fields More suitable for anisotropic turbulence

Turbulence Models affect Hydrodynamics Lack of Measured Data for Validation Possibly better represent turbulence