Free_shear_flows(1)

Course: ME 563, Spring 2011
School: Auburn
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Flow Turbulent and Transport 4 4.1 4.2 Free Shear Flows I: Jets, Wakes, etc.Solutions Based on Simple MeanFlow Closure Schemes Meanflow closure schemes for free shear flows. Spreading of a velocity discontinuity with downstream distance in steady flow. The nature of the laminar flow solution and its stability. Similarity solution for turbulent flow, based on Prandtls second closure hypothesis. Comparison with...

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Flow Turbulent and Transport 4 4.1 4.2 Free Shear Flows I: Jets, Wakes, etc.Solutions Based on Simple MeanFlow Closure Schemes Meanflow closure schemes for free shear flows. Spreading of a velocity discontinuity with downstream distance in steady flow. The nature of the laminar flow solution and its stability. Similarity solution for turbulent flow, based on Prandtls second closure hypothesis. Comparison with experiment. Plane and axisymmetric jets. The momentum flow constraint. Comments on laminar jets and their stability. Scaling laws for jet width (radius) and maximum velocity in turbulent jets. Similarity solution for the far region based on Prandtls second closure hypothesis. Comparison with experiment. Entrainment in jets and secondary flows induced by jets. Simple integral methods for jets based on an entrainment hypothesis. Plane and axisymmetric wakes. The momentum defect constraint. Scaling laws width velocity and defect in turbulent wakes. Similarity and integral solutions for far wake region.Comparison with experiment. Distribution of passive scalars (concentration or temperature) in the far region of jets and wakes, neglecting buoyancy effects. 4.3 4.4 for 4.5 Readings: White. 2nd ed. 470481 (see also pp. 253260, 301304 for laminar flow). Pope. Chap. 4 & 5 Schlichting. 7th ed. Chap. 24 (see also pp. 183185 for laminar flow). For turbulent shear layer: Champagne, Pao, & Wygnaski, J. Fluid Mech ., 74 (1976): 209250. Hinze. Chapter 6. Abramovich. The Theory of Turbulent Jets: 103113, 120125. Rajaratnam. "Turbulent Jets." Elsevier, 1976. Rodi. I n "Studies in Convection" B. E. Launder. ed. Academic Press, 1975: 79 ff. Townsend. Chap.6 in The Structure of Turbulent Shear Flow. 2nd ed. Cambridge, 1976. Further reading: Handouts: Selected experimental data & summaries.
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Auburn - ME - 563
Turbulent Flow and Transport1Review of Fundamental Laws and ConstitutiveEquations1.1Fundamental laws governing continuum flow, expressed in terms of (i) materialvolumes (closed systems) and (ii) control volumes.1.2Mass conservation equation; integ
Auburn - ME - 563
Generalized Harmonic Analysis Generalized Harmonic Analysis (see Davenport and Root, Introduction to the Theory of Random Signals and Noise) Parseval's Theorem: 1 2-f (t ) 2 dt =- F ( )2d(1)For random variable f(t), consider a modification to Pars
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Transition to Turbulent Flow in AerodynamicsRobert I. BowlesPhilosophical Transactions: Mathematical, Physical and Engineering Sciences, Vol. 358, No.1765, Science into the Next Millenium: Young Scientists Give Their Visions of the Future: II.Mathemat
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Ph 136a5 February 2003CHAPTER 14: TURBULENCEReading:Chapter 14 of Blandford and Thorne.ProblemsA. Do:1. Exercise 14.1 part (ii): Spreading of a Laminar Wake Behind a Sphere, ANDExercise 14.4 part (ii): Turbulent Wake Behind a Sphere [Note: Kip wil
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Lectures in Turbulence for the 21st CenturyWilliam K. George Professor of Turbulence Chalmers University of Technology Gothenburg, Sweden2Contents1 The 1.1 1.2 1.3 1.4 1.5 1.6 1.7 Nature of Turbulence The turbulent world around us . What is turbulence
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The First Few Lectures in a First Course on TurbulenceTony Burden's Lecture Notes, Spring 2007These lecture notes are intended to make life easier for the lecturer and the students by reducing the amount of text that is first written on the blackboard a
Auburn - ME - 563
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Tony Burdens Lecture Notes on Turbulence, Spring 20073c Plane jetCompared to the general analysis of a thin shear layer, the freestream velocity U = 0, and the freestream pressure is constant, so, U0 U and dP = 0. dxConstant momentum ux Within the free
Auburn - ME - 563
Tony Burdens Lecture Notes on Turbulence, Spring 2007Chapter 5. Mean Kinetic EnergyThis chapter is based on the Navier-Stokes equation in the form, where, sij = 1 ui uj + 2 xj xi , ui ui p 2sil , + ul = + t xl xi xlis the rate-of-strain tensor. The cor
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INTRODUCTORYLECTURES on TURBULENCEPhysics, Mathematics and ModelingJ. M. McDonoughDepartments of Mechanical Engineering and MathematicsUniversity of Kentuckyc 2004Contents1 Fundamental Considerations1.1 Why Study Turbulence? . . . . . . . . . . .
Auburn - ME - 563
ME 563 - Intermediate Fluid Dynamics - SuLecture 31 - Instability: more on Kelvin-Helmholtz, and thermal convectionReading: Acheson, 9.2-9.3. To recap what we did with Kelvin-Helmholtz instability in the last lecture We dened our undisturbed, two-dimens
Auburn - ME - 563
ME 563 - Intermediate Fluid Dynamics - SuLecture 36 - Turbulence: more on scaling, and the Reynolds stressIn the last class we looked at the Kolmogorov similarity hypotheses, which expressed the idea that the smaller scales of turbulence approach a univ
Auburn - ME - 563
Introduction to Large Eddy Simulation of Turbulent Flows 1J. Frohlich, W. Rodi Institute for Hydromechanics, University of Karlsruhe, Kaiserstra e 12, D-76128 Karlsruhe, GermanyContents1 Introduction1.1 Resolution requirements of DNS . . . . . . . . .
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On the nature of turbulenceA. S. MoninInstitute of Oceanology, USSR Academy of Sciences Usp. Fiz. Nauk 125, 97-122 (May 1978) The definition of turbulence and the differences between turbulence and random wave motions of liquids or gases are discussed.
Auburn - ME - 563
NASA/CR-1998-206909ICASE Report No. 98-5A Kinematically Consistent Two-Point CorrelationFunctionJ. R. RistorcelliICASEInstitute for Computer Applications in Science and EngineeringNASA Langley Research CenterHampton, VAOperated by Universities Sp
Auburn - ME - 563
J. Fluid Mech. (1998), vol. 377, pp. 6597.c 1998 Cambridge University PressPrinted in the United Kingdom65The structure and dynamics of vorticity and rateof strain in incompressible homogeneousturbulenceBy K E I K O K. N O M U R AANDG A R Y K. P
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T URBULENCE AND S IGNAL A NALYSISPierre Borgnat (email Pierre.Borgnat@ens-lyon.fr)Laboratoire de Physique (UMR-CNRS 5672) ENS Lyon 46 all e dItalie 69364 Lyon Cedex 07eAbstractTurbulence deals with the complex motions in uid at high velocity and/or i
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Turbulent Flow & Transport Problem 3.1: Scales of turbulent motion. An ordinary hand-held electric kitchen mixer is to be used for mixing 1.5 liters of liquid. The mixer has counter-rotating strirrers with blades formed from 6 mm wide metal strips (lo
Auburn - ME - 563
Turbulent Flow and TransportProblem 5.1: The Kolmogorov microscale, the viscous sublayer, and the inertialsublayerConsider a fully developed, turbulent flow in a smooth-walled, circular pipe of radius a.(a) Suppose we define a nominal thickness v of t
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Turbulent Flow and TransportProblem: Friction in Turbulent Hydrodynamic BearingsReferences:(1) Shinkle, J. N. and K. G. Hornung, Frictional characteristics of a liquid journalbearing. Trans. ASME J. Basic Engineering. (1965): 163-169.(2) Wasson, K. L
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Mixing driven by Rayleigh-Taylor Instability in the MesoscaleModelled with Dissipative Particle DynamicsWitold DzwinelAGH Institute of Computer Science, al. Mickiewicza 30, 30-059, Krakw, PolandDavid A.Yuen1Minnesota Supercomputer Institute, Universi
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Tony Burdens Lecture Notes on Turbulence, Spring 2007Chapter 2. Reynolds Equation and the Reynolds StressIn this chapter the basic equations of uid mechanics are subjected to averaging andin particular Reynolds equation for the mean velocity is derived
Auburn - ME - 563
The Length, Time and Velocity Scales of TurbulenceTony Burdens Lecture Notes, Spring 2006These lecture notes are intended to make life easier for the lecturer and the students by reducing the amount of text that is rst written on the blackboard and then
Auburn - ME - 563
Turbulent Flow and Transport5Bounded Flows I: General NearWall Scaling Laws;Flows in Pipes, Channels, etc.5.1Division of a wallbounded turbulent shear flow into an inner (or constantshear) layer near the wall, and an "outer layer." Prandtls "unive
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Chapter 7Solutions2.1 Using the denitions for Ret and Re , the relation between and ( = 15 u2 /2 ), andthe estimate = u3 /Lturb , we obtain:Re =uu2 215u4 Lturb15 u21/2= 15Ret Re = 15Ret Re2 = 2 = u2 2 = u32.2 Using u = 10 m/s and u/u = 0.1, w
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Stability and Transition to TurbulenceLinear estimates for neutral stability To estimate conditions under which parallel flows begin to be unstable, look at conditions under which an initially infinitesimal disturbance will grow exponentially. Begin with
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A.3. CURVILINEAR COORDINATES75A.3.1 Tensor invarianceLets presume that xi is the old Cartesian coordinate system, and x j represents the new curvilinear coordinate system. Both systems are related by transformation rules (A.4) and (A.10). The distance
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Prof. Dr. May-Britt KallenrodeFachbereich PhysikModeling TransportOsnabrck, 13th November 2006 uContents1 What is Transport? 1.1 What is transport? A Guided Tour . . . . . . . . . . . . . . . . . . 1.2 Help, I still cant dene Transport . . . . . . .
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Tony Burdens Lecture Notes on Turbulence, Spring 2007Chapter 3. Thin Shear Layers and Free Shear Flows 3a Thin-shear-layer Equationsexamples free shear ows, such as jets, wakes and mixing layers, and wallbounded ows, such as boundary layers and wall jet
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FACE8 Turbulence and MxingTurbulence and mixingFACE8 20071Course outlineLARFACE8 Turbulence and Mxing1 MMIntroduction to turbulenceBasic concepts of turbulent flowTurbulent flow structuresEnergy cascadeTurbulent energy spectrum2 MM Introduct
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FACE8 Turbulence and MixingTurbulence and MixingFACE8 20061Recommended readingFACE8 Turbulence and MixingFrank M. White (1991): Viscous fluid flow, McGrawHill International Editions, Mechanical EngineeringSeries. ISBN0-07-100995-7H. Schlichting an
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FACE8 Turbulence and MixingTurbulence and Mixing3rd lectureBoundary layers revisittedFree shear flowsFACE8 20071Buffer layerHigh dissipation2Laminar/viscous sublayerTurbulence freeFACE8 Turbulence and MixingTurbulent boundary layersFACE8 Tur
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FACE8TurbulenceTurbulenceLectures3&4Modelling1Courseoutline2MM3MM4MM21MMFACE8Turbulence5MM Introductiontoturbulence Basicconceptsofturbulentflow Turbulentflowstructures Energycascade Turbulentenergyspectrum Turbulentlengthandtimescales
Auburn - ME - 563
Lessons from Hydrodynamic TurbulenceTurbulent flows, with their irregular behavior, confound any simple attempts to understand them. But physicists have succeeded in identifying some universal properties of turbulence and relating them to broken symmetri
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3D TURBULENCE13D TURBULENCEW. D. Smyth and J. N. Moum, College of Oceanic & Atmospheric Sciences, Oregon State University, Corvallis, OR 97330, USACopyright^2001 Academic Pressdoi:10.1006/rwos.2001.0134Introduction0001000200030004This article
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Lecture Notes in TurbulenceSteve Berg2nd June 2004Contents1 Conservation Equations21.1Conservation of Mass . . . . . . . . . . . . . . . . . . . . . . . .21.2Conservation of Moment . . . . . . . . . . . . . . . . . . . . . .42 Turbulent Theory
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Turbulent Mixing in the MicroscaleW.Dzwinel1, W.Alda1, M.Pogoda1 and D.A.Yuen21University of Mining and Metallurgy, Institute of Computer Science, 30-059 Krakw, Poland2Minnesota Supercomputer Institute, University of Minnesota, Minneapolis, USAAbstr
Auburn - ELEC - 7250
LOGIC SIMULATION AND FAULTDIAGNOSISBY JINS DAVIS ALEXANDERELEC 7250 PRESENTATION14/20/2006ELEC7250: AlexanderPROBLEM STATEMENT2To write a logic simulator to verify combinationalcircuits given a set of input vectors and the expectedoutput respon
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A Robust Logic Simulator UsingRobustDynamic LevelizationDynamicKasi L. K. AnbumonyDept. of Electrical EngineeringAuburn University, AL 36849 USA20 April 2006VLSI Testing-Final Project Presentation1Motivation for This Work Logic simulator to ver
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Brad HillELEC 7250Logic Simulator4/25/20064/25/2006ELEC7250: Hill1Simulation Table Table createdTableGate NameFan-in and Fan-out Input and Output Array Signal Array Holds Signal Value during simulation Set to 0 before each vector is applied
Auburn - ELEC - 7250
ELEC 7250 VLSI Testing (Spring 2006)Place and Time: Broun 235, Tuesday/Thursday, 11:00AM-12:15PM Course Website: http:/www.eng.auburn.edu/~vagrawal/COURSE/E7250_06/course.html Catalog data: ELEC 7250. VLSI Testing (3) Lec. 3. Pr., ELEC 6770. Introduction
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