Appendix A.

Slides:



Advertisements
Similar presentations
Heat Transfer to Solids in a Flowing Fluid
Advertisements

Chapter 2 Introduction to Heat Transfer
ES 202 Fluid and Thermal Systems Lecture 28: Drag Analysis on Flat Plates and Cross-Flow Cylinders (2/17/2003)
University of Western Ontario
Nozzle Study Yan Zhan, Foluso Ladeinde April, 2011.
Computer Aided Thermal Fluid Analysis Lecture 10
PETE 203 DRILLING ENGINEERING
II. Properties of Fluids. Contents 1. Definition of Fluids 2. Continuum Hypothesis 3. Density and Compressibility 4. Viscosity 5. Surface Tension 6. Vaporization.
Heat transfer to fluids without phase change
Experimental and Numerical Study of the Effect of Geometric Parameters on Liquid Single-Phase Pressure Drop in Micro- Scale Pin-Fin Arrays Valerie Pezzullo,
Internal Flow: Heat Transfer Correlations
Flow over an Obstruction MECH 523 Applied Computational Fluid Dynamics Presented by Srinivasan C Rasipuram.
First Wall Thermal Hydraulics Analysis El-Sayed Mogahed Fusion Technology Institute The University of Wisconsin With input from S. Malang, M. Sawan, I.
Fluid mechanics 3.1 – key points
Verification and Validation Diagram of a Control Rod Guide Tube on top of a hot box dome that has been gradually heating up. A hole was drilled here to.
Nelson Research, Inc – N. 88 th St. Seattle, WA USA aol.com Two Phase “Bubbly” Fluid Flow in a Vertical Chamber A.
Kern Method of SHELL-AND-TUBE HEAT EXCHANGER Analysis
Chapter 7 Sections 7.4 through 7.8
CHE/ME 109 Heat Transfer in Electronics LECTURE 19 – NATURAL CONVECTION FUNDAMENTALS.
Computational Modeling of Turbulent Asymmetric Jet Flows Prof. Ed Akin Mechanical Engineering and Materials Science Rice University Houston, Texas Jon.
Flow rate across a fluid element with top and bottom faces moving Fluid element h dx dy Consider the fluid element with dimensions dx, dy, and h (film.
Molecular Transport Equations. Outline 1.Molecular Transport Equations 2.Viscosity of Fluids 3.Fluid Flow.
高等輸送二 — 質傳 Lecture 8 Forced convection
Design Formulae for Mingled Shell-side stream P M V Subbarao Professor Mechanical Engineering Department I I T Delhi A Confluence Model for A Circuitous.
1 Numerical study of the thermal behavior of an Nb 3 Sn high field magnet in He II Slawomir PIETROWICZ, Bertrand BAUDOUY CEA Saclay Irfu, SACM Gif-sur-Yvette.
Optimization Of a Viscous Flow Between Parallel Plates Based On The Minimization Of Entropy Generation Presentation By Saeed Ghasemi.
Department Of Material Science And Engineering FINITE ELEMENT METHOD UNIVERSITY OF CHEMICAL TECHNOLOGY AND METALLURGY Sofia Nina Velikova, June 2010.
30 th June 20111Enrico Da Riva, V. Rao Parametric study using Empirical Results June 30 th 2011 Bdg 298 Enrico Da Riva,Vinod Singh Rao CFD GTK.
Convection: Internal Flow ( )
Convection in Flat Plate Boundary Layers P M V Subbarao Associate Professor Mechanical Engineering Department IIT Delhi A Universal Similarity Law ……
Modeling a Steam Generator (SG)
CFD Study of the Development of Vortices on a Ring Wing
INTRODUCTION TO CONVECTION
Stokes Solutions to Low Reynolds Number Flows
Distributed Resistances and Fan Models Chapter 4.
Internal Flow: Heat Transfer Correlations. Fully Developed Flow Laminar Flow in a Circular Tube: The local Nusselt number is a constant throughout the.

Chapter 7 Natural convection systems. 7-1 Introduction  natural or free convection: the motion of the fluid due to density changes arising from heating.
Plots of Fluid Flow Data Profile plots- A profile plot indicates how the value of a scalar (or vector can be plotted but only the magnitude) property varies.
Pipe flow analysis.
COUPLED ANALYSES Chapter 7. Training Manual May 15, 2001 Inventory # Fluid-Structure Analysis “One Way” Analysis –Structural deformation effect.
Heat Transfer Su Yongkang School of Mechanical Engineering # 1 HEAT TRANSFER CHAPTER 8 Internal flow.
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.
Indian Institute of Space Science and Technology STUDY OF EFFECT OF GAS INJECTION OVER A TORPEDO ON FLOW-FIELD USING CFD.
Mixing Length of Hydrogen in an Air Intake Greg Lilik EGEE 520.
Momentum Equation and its Applications
Control Rod Nozzle Guide Tubes improved by 4 drilled holes. Model as two coaxial tubes of fluid connected by 4 holes. Two inlets at the bottom from the.
Fluid Mechanics, KU, 2011 Chap. 8: One-Dimensional Flows Incompressible Newtonian fluids considered here EOC + Navier-Stokes eq. (EOM with Newtonian CE)
Internal Flow: General Considerations. Entrance Conditions Must distinguish between entrance and fully developed regions. Hydrodynamic Effects: Assume.
Internal Flow: Heat Transfer Correlations Chapter 8 Sections 8.4 through 8.8.
Date of download: 9/26/2017 Copyright © ASME. All rights reserved.
Internal Flow: Heat Transfer Correlations
Chapter 8: Internal Flow
Internal Incompressible
Chapter 8 : Natural Convection
Date of download: 3/4/2018 Copyright © ASME. All rights reserved.
Slides for ME 115 Laboratory
Dimensional Analysis in Mass Transfer
Subject Name: FLUID MECHANICS
From: Modeling of Particle-Laden Cold Flow in a Cyclone Gasifier
Model Species Transport in a Static Mixer Reacting Flows – Homework 6
FLUID MECHANICS REVIEW
Heat Exchangers Heat Exchangers.
Lecture Objectives: Boundary Conditions Project 1 (software)
Internal Flow: General Considerations
Convective Heat Transfer
Subject Name: FLUID MECHANICS
Internal Flow: Heat Transfer Correlations Chapter 8 Sections 8.4 through 8.8.
Lecture 4 Dr. Dhafer A .Hamzah
Presentation transcript:

Appendix A

Exercise: Planar Couette Flow Description Wall-driven flow between infinite parallel plates, separated by a distance H. Upper horizontal wall moves at constant velocity, Vwall, while lower horizontal wall is fixed. Left and right vertical boundaries are periodic. May 15, 2001 Inventory #001477 Appendix A-2

Exercise (continued) : Planar Couette Flow Assumption Steady-state Incompressible VY = VZ = 0 VX = VX(Y) only Pressure field is constant No body forces Fluid properties are constant May 15, 2001 Inventory #001477 Appendix A-3

Exercise: Backward Facing Step May 15, 2001 Inventory #001477 Appendix A-4

Exercise (continued) : Backward Facing Step Input File: Step51 Data: Armaly, et. al., “Experimental and Theoretical Investigation of Backward Facing Step Flow", Journal of Fluid Mechanics (1983), vol. 127, pp. 473-496. Inlet length: 2.5 (can be varied by the user) Outlet length: 18 (can be varied by the user) Outlet Condition: P = 0 use density = 1.0 viscosity = .001 Hydraulic diameter Dh = 2(.52) = 1.04 Choose Reynolds Number between 200 and 1000: Watch for the length of the recirculation region and secondary recirculation regions. How much are results affected by the inlet velocity profile? How can the choice of the outlet condition be verified? May 15, 2001 Inventory #001477 Appendix A-5

Exercise: Tube Bundle Flow Description: Turbulent cross-flow over a bundle of circular tubes. Top and bottom horizontal boundaries are planes of symmetry Define all key points in terms of parameters: Create an ALL-QUAD mesh (requires concatenations just before meshing). Concentrate nodes towards tube walls: May 15, 2001 Inventory #001477 Appendix A-6

Exercise: Tube Bundle Flow Concatenated Line Assumptions Steady-state Incompressible Turbulent Fluid properties are constant May 15, 2001 Inventory #001477 Appendix A-7

Exercise: Jet Impingement Heat Exchanger Flow Description In this device, orifice plates are separated by spacer plates in a stack arrangement, with consecutive plates having an offset hole pattern. Multiple jets of coolant fluid impinge on conductive surfaces to maximize heat transfer. The plate stack is metalluragically bonded together to minimize conductive resistance. Flow is to be modeled in the quarter-symmetry section shown. May 15, 2001 Inventory #001477 Appendix A-8

Exercise: Jet Impingement Heat Exchanger Flow Symmetry Section Construct flowfield using top-down techniques. Generate the 12 map-meshable volumes shown below. (The file jetimp.inp can be used to create this geometry.) May 15, 2001 Inventory #001477 Appendix A-9

Map-Meshable Volumes Set ESIZE = 0.2 and map mesh with FLUID142 elements. The jet Reynolds number is 105. Assumptions Steady-state Incompressible Turbulent Fluid properties are constant May 15, 2001 Inventory #001477 Appendix A-10

Exercise: Fan Model Dimensions in inches — Fluid is air. Refer to Elements manual documentation to apply real constant data for fan. May 15, 2001 Inventory #001477 Appendix A-11

Exercise: Counter Current Heat Exchanger May 15, 2001 Inventory #001477 Appendix A-12