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UCLA - PHILOS - 22
1Philosophy 22 - Kant Handout (1)The problem: how to account for the unconditional nature of moral obligation: that morality authoritativelydirects action without regard to natural feelings and motives, and we are able to act as it commands. (Acommand
UCLA - PHILOS - 22
Philosophy 22 - Kant Notes (2)More on the Formula of Universal Law test (CI procedure):When you bring a maxim of action to the CI procedure, what do you find out? If the maxim fails, it is notpermissible to act on that maxim. If the failing maxim is a
UCLA - PHILOS - 22
More Hume notes.Natural and Artificial Virtues a PuzzleVirtuous actions derive their merit from virtuous motives. (203)An action is just a set of events. Our moral approval of it is directed at its cause, the agents motive or reasonsfor acting. The ac
UCLA - HIST - 21
Lectures Week 2, January 11-15, 20111. Arabia before Muhammada. a desert surrounded by fertile landb. Tribal pastoral nomads, surrounded to the North and East by the greatMediterranean civilizationsc. Those bands always a nuisance to settled lands, n
UCLA - KOREA - 154
Click to edit Master subtitle style9/18/11K1545/17/11Today:1.Introduction to Film2.Film: Im a Cyborg, but Thats OK- dir. Pak Chanuk, 2006* Due Friday: final paper topic/research question(print)9/18/119/18/11Picture 29/18/11Director: Pak Ch
UC Davis - MUS - 106
Music106InfoMusic106InfoRobSabinorlsabino@ucdavis.edu5308487148OfficehoursbyappointmentDavidVerbucdverbuc@ucdavis.eduListeningSitehttp:/listening.ucdavis.eduGoalsofmusic106Goalsofmusic106develop your earsdemystify musical abilityhear great musi
UC Davis - MUS - 106
ApointfordiscussionApointfordiscussionBonoPopmusicoftentellsyoueverythingisok,whilerockmusictellsyouthatitsnotok,butyoucanchangeitPostWWIIEnglandPostWWIIEnglandTheMods(modernists)lowerclassyetverytrendy,nicesuits,shorthair,scooters:PeteTownshend(T
UC Davis - MUS - 106
WhentheMusicsOverIhearaverygentlesoundVerynearyetveryfarVerysoft,yeah,veryclearCometoday,cometodayWhathavetheydonetotheearth?Whathavetheydonetoourfairsister?RavagedandplunderedandrippedherandbitherStuckherwithknivesinthesideofthedawnAndtiedherwit
UC Davis - MUS - 106
Violenceinthe60sViolenceinthe60sMay62RaceriotinBirmingham,AL 62USmilitarycouncilestablishedinVietnam 62Cubanmissilecrisis Fall623000soldiersquellriotswhenJamesMeredithentersOleMiss 63violentcivilrightsdemonstrations,Birmingham,AL 22Nov.63JFKassassi
UC Davis - MUS - 106
Mainstream70sRockMainstream70sRockRodStewartb.1945MaggieMayForeigner76presentFeelsLiketheFirstTimeAC/DC73presentBackInBlackBoston76presentMoreThanaFeelingRush68presentTomSawyerAerosmith70presentWalkThisWayBachmanTurnerOverdrive7304TakinCareOfBusin
UC Davis - MUS - 106
MTVMTVLaunchedAugust1,1981inNewYorkCityThefirstvideowasVideoKilledtheRadioStarbyTheBugglesMichaelJacksonwasitsbiggeststarinthe80sThriller14minuteslongandplayedtwiceanhourMadonnarosetofameduetoMTVandTheMTVawardsshowItnowcarriesyouthcultureoriented
UC Davis - PHE - 44
Sandra SamarronTop 9 Must Eat Foods Lecture OutlineLife Has Physical Demands-Think of Yourself as an AthleteHow Did You Start Your Day?Top Must Eat Foods1. Bagelsa. Fiber, Fiber, Fiber!b. Water Insoluble Fiberc. Carbohydrates provide the largest p
UC Davis - PHE - 44
PhysicalHealthTalkCoachlou71211ExerciseandDiseasePrevention1. ReducedriskofHeartDiseasestrongerheartandmoreefficientcardiorespiratorysystem2. PreventionofHighBloodPressurerelatedissuesduetolowerbloodpressure3. ReducedArterialDiseaseduetolowerchole
UC Davis - PHE - 44
What is your STRESS?1. What was the stressor?The midterm / assignmentorprocrastinationyour guilt, frustration,It is our job, why we are hereOrganize!The Game, what we doPrioritizeThe Way we get where we want to goPlay on-CompeteIf the Cause of
Auburn - ME - 563
Introduction to TurbulencebyHkan GustavssonDivision of Fluid MechanicsLule University of TechnologyForewordThe intention with these pages is to present the student with the basic theoretical concepts ofturbulence and derive exact relations from the
Auburn - ME - 563
1Turbulence & mixingTurbulence & mixing4th lectureFACE 8 2007Turbulence & mixing2 Program08:15-08:4508:45-09:0009:00-09:1509:15-10:0010:00-12:00Lecture: Derivation of RANSExercise: Questions about turbulenceBreakLecture: Turbulence models
Auburn - ME - 563
1Turbulence & mixingTurbulence & mixing4th lectureFACE 8 2007Turbulence & mixing2 Program08:15-08:4508:45-09:0009:00-09:1509:15-10:0010:00-11:3011:20-12:00Lecture: The LES approachExercise: RANS+ QuestionsBreakLecture: Smagorinsky SGS mod
Auburn - ME - 563
Turbulent Flow and Transport77.1 7.2 7.3 S.Buoyant Plumes, Thermals, etc.Jets, plumes, forced plumes, thermals, etc. Stable and unstable atmospheres. The Boussinesq approximation and the conditions for its applicability. Integral equations for a stea
Auburn - ME - 563
Turbulent Flow and Transport8Introduction to Turbulence Models8.1Approaches to closure. Eddy diffusivity defined in terms of local turbulencelength scale.8.2Equations for (i) the kinetic energy of the mean motion and for (ii) the mean kinetic ene
Auburn - ME - 563
Turbulent Flow and Transport9Dispersion in Pipe and Channel flow9.1Dispersion in laminar pipe flow. Purely diffusive dispersion, purelyconvective dispersion, and Taylor (or TaylorAris) dispersion. Scaling laws that definethe conditions under which t
Auburn - ME - 563
Chapter 12Foundations of Fluid DynamicsVersion 0212.2 28 Jan 03Please send comments, suggestions, and errata via email to kip@tapir.caltech.edu and rdb@caltech.edu,or on paper to Kip Thorne, 130-33 Caltech, Pasadena CA 9112512.1OverviewHaving studi
Auburn - ME - 563
Chapter 14TurbulenceVersion 0214.2, 5 February 2003Please send comments, suggestions, and errata via email to kip@tapir.caltech.edu and alsoto rdb@caltech.edu, or on paper to Kip Thorne, 130-33 Caltech, Pasadena CA 9112514.1OverviewIn Chap. 12, we
Auburn - ME - 563
42CHAPTER 2. FUNDAMENTAL LAWSwhere is the density of the uid and vn is the face-normal velocity across the face of area A of a control volume (see Problem 2.7.7).2.6 The Law of SimilarityThe law of similarity [7, 8] enables in some situations to use a
Auburn - ME - 563
Chapter 3 Laminar ows3.1 AssumptionsFlow equations discussed in Chapter 2 provide analytical solutions only in some special cases. In this chapter we shall consider the equations for incompressible ow: (2.4), (2.22) and (2.74), assuming that all the coe
Auburn - ME - 563
Chapter 4 Turbulent ows4.1 Transition to turbulenceIn the case of free ows transition to turbulence occurs much earlier than in conned ows. In terms of Reynolds number, it is a matter of several hundred for the unbounded ows around objects, and a matter
Auburn - ME - 563
FUNDAMENTAL AND CONCEPTUAL ASPECTS OF TURBULENT FLOWSProfessor and Marie Curie Chair in Fundamental and Conceptual Aspects of Turbulent Flows Institute for Mathematical Sciences and Department of Aeronautics, Imperial College LondonLectures series as a
Auburn - ME - 563
FUNDAMENTAL AND CONCEPTUAL ASPECTS OF TURBULENT FLOWSProfessor and Marie Curie Chair in Fundamental and Conceptual Aspects of Turbulent Flows Institute for Mathematical Sciences and Department of Aeronautics, Imperial College LondonLectures series as a
Auburn - ME - 563
FUNDAMENTAL AND CONCEPTUALASPECTS OF TURBULENT FLOWSArkady TsinoberProfessor and Marie Curie Chair in Fundamental and Conceptual Aspects of Turbulent FlowsInstitute for Mathematical Sciences and Department of Aeronautics, Imperial College LondonLectu
Auburn - ME - 563
FUNDAMENTAL AND CONCEPTUALASPECTS OF TURBULENT FLOWSArkady TsinoberProfessor and Marie Curie Chair in Fundamental and Conceptual Aspects of Turbulent FlowsInstitute for Mathematical Sciences and Department of Aeronautics, Imperial College LondonLectu
Auburn - ME - 563
FUNDAMENTAL AND CONCEPTUALASPECTS OF TURBULENT FLOWSArkady TsinoberProfessor and Marie Curie Chair in Fundamental and Conceptual Aspects of Turbulent FlowsInstitute for Mathematical Sciences and Department of Aeronautics, Imperial College LondonLectu
Auburn - ME - 563
FUNDAMENTAL AND CONCEPTUALASPECTS OF TURBULENT FLOWSArkady TsinoberProfessor and Marie Curie Chair in Fundamental and Conceptual Aspects of Turbulent FlowsInstitute for Mathematical Sciences and Department of Aeronautics, Imperial College LondonLectu
Auburn - ME - 563
FUNDAMENTAL AND CONCEPTUAL ASPECTS OF TURBULENT FLOWSProfessor and Marie Curie Chair in Fundamental and Conceptual Aspects of Turbulent Flows Institute for Mathematical Sciences and Department of Aeronautics, Imperial College LondonLectures series as a
Auburn - ME - 563
FUNDAMENTAL AND CONCEPTUALASPECTS OF TURBULENT FLOWSArkady TsinoberProfessor and Marie Curie Chair in Fundamental and Conceptual Aspects of Turbulent FlowsInstitute for Mathematical Sciences and Department of Aeronautics, Imperial College LondonLectu
Auburn - ME - 563
FUNDAMENTAL AND CONCEPTUALASPECTS OF TURBULENT FLOWSArkady TsinoberProfessor and Marie Curie Chair in Fundamental and Conceptual Aspects of Turbulent FlowsInstitute for Mathematical Sciences and Department of Aeronautics, Imperial College LondonLectu
Auburn - ME - 563
Lecture Notes. Waves in Random MediaGuillaume Bal1January 9, 20061Department of Applied Physics and Applied Mathematics, Columbia University, New York NY,10027; gb2030@columbia.eduContents1 Wave equations and First-order hyperbolic systems1.1 Int
Auburn - ME - 563
Tony Burdens Lecture Notes on Turbulence, Spring 2006Wall-bounded shear owsversion 1: channel owFully developed channel owSee the example in the section of the lecture notes which present Reynolds equationand the Reynolds stress.For fully developed,
Auburn - ME - 563
Turbulent Flow and Transport6Introduction to Turbulent Boundary Layers6.1The nature of flow in turbulent boundary layers. Inner and outer regions, eddydiffusivity distributions, intermittency, etc.6.2Integral form of the mean flow boundary layer e
Auburn - ME - 563
Cambridge University Engineering Department4A12: TurbulenceLecture NotesDr. E. MastorakosHopkinson LabE-mail: em257@eng.cam.ac.ukhttp:/www.eng.cam.ac.uk/ em2571Chapter 1Introduction1.1AimsThe main aims of this course are:1. To introduce some
Auburn - ME - 563
Chapter 3Governing equations3.1Instantaneous equations (incompressible uid)Conservation of massNavier-Stokesui=0xi(3.1)1 p1 ikui (uk ui )=+ gi ++txk xi xk(3.2)with the shear stress given by:ij = 2sij = ui uj+xjxi(3.3)with sij
Auburn - ME - 563
Chapter 5Free thin shear owsIn this Chapter, we will discuss a large class of ows called thin shear ows. We will focuson ows far from a solid surface (the wall boundary layer is discussed in Chapter 6) andwe will aim to understand the structure of jet
Auburn - ME - 563
Approach to Chaos 0. Introduction There are two major reasons for studying non-linear systems. The first and most basic is that the equations of motion of almost all real systems are non-linear. The second reason is that even a relatively simple system wh
Auburn - ME - 563
4A8: Environmental Fluid MechanicsMixing and Reactions in Turbulent Flows3. Statistical description of turbulent mixingIn this Chapter, we will derive the governing equation for a reacting scalar in a turbulentflow and we will demonstrate why the turb
Auburn - ME - 563
Turbulent Flow and Transport3Concepts in Turbulence3.1Comments on laminar flow, its stability, and the transition to turbulent flow.3.2Features of turbulent flows (high Reynolds number, "randomness", threedimensionality of fluctuations, intermitte
Auburn - ME - 563
Cambridge University Engineering Department4A12: TurbulenceData CardAssume incompressible uid with constant properties.Continuity: ui=0xiMean momentum: ui uj ui ui1 p+ uj=+ 2 ui /x2 + gijtxj xixjMean scalar: 2 ui + ui=D 2 txixi
Auburn - ME - 563
Publication 97/2An Introduction to TurbulenceModelsLars Davidson, http:/www.tfd.chalmers.se/ladaDepartment of Thermo and Fluid DynamicsC HALMERS U NIVERSITY OF T ECHNOLOGYG teborg, Sweden, November 2003o ! Nomenclature31Turbulence1.1 Intro
Auburn - ME - 563
yrCkD DwR1 ww VDDuq j qwk yuuDya ywk uwVDC w DDwa quw xyuwT yD y W 1$ w3 yD1 q k q r DCky DDyV wu wj T uuyaC yDV hD" Dr$qw y V yx Dw1 Cu w VDDuCrqydyxTy1Twcfw_rDqxww)uDyauwRDwwC1DDwa
Auburn - ME - 563
Turbulent Flow and Transport44.1 4.2Free Shear Flows I: Jets, Wakes, etc.Solutions Based on Simple MeanFlow Closure SchemesMeanflow closure schemes for free shear flows. Spreading of a velocity discontinuity with downstream distance in steady flow.
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
Auburn - ME - 563
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
Auburn - ME - 563
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
Auburn - ME - 563
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
Auburn - ME - 563
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
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