ME 321: FLUID MECHANICS-I
|
|
- Miles Wilcox
- 5 years ago
- Views:
Transcription
1 8/7/18 ME 31: FLUID MECHANICS-I Dr. A.B.M. Toiqe Hasan Proessor Dearmen o Mechanical Engineering Bangladesh Uniersi o Engineering & Technolog BUET, Dhaka Lecre-13 8/7/18 Dierenial Analsis o Flid Moion eacher.be.ac.bd/oiqehasan/ oiqehasan@me.be.ac.bd Dr. A.B.M. Toiqe Hasan BUET L-3 T-1, De. o ME ME 31: Flid Mechanics-I Jan Dierenial Analsis The basic eqaions o lid dnamics in inegral orm or a inie conrol olme C are: 1 Conini eqaion: olme lo rae, Q A consan or incomressible lo mass lo rae, m A consan or an lo : comressible/incomressible Bernolli Eqaion: consan Bernolli consanor incomressible lo g These inegral eqaions are sel hen e are ineresed in gross behaior o a lo ield and is eec on arios lo ssems. Hoeer, he inegral aroach does no enable s o obain he deailed oin-b-oin knoledge o he lo ield. For eamle, he inegral aroach cold roide inormaion on he li generaed b a ing; i cold no be sed o deermine he ressre and shear sress disribions ha rodce he li on he ing. To see ha is haening in a lo in deail, i is reqired o se he dierenial eqaions o lid dnamics hich inoles an ininiesimal conrol olme, in conras o inie conrol olme. This aroach is knon as dierenial analsis. Dr. A.B.M. Toiqe Hasan BUET L-3 T-1, De. o ME ME 31: Flid Mechanics-I Jan. 18 1
2 8/7/18 Conseraion o Mass Mass can neiher be creaed nor desroed. Consider a er small olme o sace ininiesimal conrol olme hrogh hich a lid is loing. For simlici, a D lo is considered and he conrol olme is bonded b he sraces and as shon in igre. According o he la, he ne olo o mass hrogh he sraces srronding he olme ms be eqal o he decrease o mass ihin he olme. The mass lo rae is eqal o he rodc o densi, eloci comonen normal o srace and he area o ha srace. In ecor orm; s m nˆ da inlo e ρ, ρ olo +e olo +e inlo e Dr. A.B.M. Toiqe Hasan BUET L-3 T-1, De. o ME ME 31: Flid Mechanics-I Jan Conseraion o Mass A irs-order Talor series is sed o ealae he lo roeries a he aces o he elemen, since he roeries are a ncion o osiion coninm aroach Lecre-1. The ne olo o mass er ni o ime er ni deh is Talor series h h h ! olo +e area olo +e area inlo e inlo e inlo e ρ, ρ olo +e olo +e inlo e Dr. A.B.M. Toiqe Hasan BUET L-3 T-1, De. o ME ME 31: Flid Mechanics-I Jan. 18 4
3 8/7/18 3 Conseraion o Mass hich ms be eqal o he rae a hich he mass conained ihin he elemen decreases: mass in de o decrease e ; 1 mass= densi olme Eq aing he abo e o e ressions and di iding b Eqaing he aboe o eressions and diiding b - I -dimension is considered, he dierenial orm o he aboe eression comes as Dr. A.B.M. Toiqe Hasan BUET 5 L-3 T-1, De. o ME ME 31: Flid Mechanics-I Jan. 18 hich is knon as dierenial conini eqaion in ecor orm.,, oeraor, del and,, here ; Conseraion o Mass In case o sead los, Then he sead lo conini eqaion in dierenial orm becomes as- di di Then he sead lo conini eqaion in dierenial orm becomes as- Incomressible los ρ= consan Comressible los ρ consan Dr. A.B.M. Toiqe Hasan BUET 6 L-3 T-1, De. o ME ME 31: Flid Mechanics-I Jan. 18
4 8/7/18 Conseraion o Momenm Linear Momenm Eqaion: The ne orce acing on a lid aricle is eqal o he ime rae o change o he linear momenm o he lid aricle. As lid elemen moes in sace, is eloci, densi, shae and olme ma change, b is mass is consered. Conseraion o momenm can be rien as- F m D D D direcion : F m D D direcion : F m D D direcion : F m D ;,, and F F, F, F 1 The eloci o a lid aricle is, in general, an elici ncion o ime as ell as o is osiion,,. Frhermore, he osiion coordinaes,, o he lid aricle are hemseles a ncion o ime. The deriaie in he aboe eression is reqenl ermed as aricle, oal or sbsanial deriaie D/D o eloci Lecre-: aricle acceleraion. Dr. A.B.M. Toiqe Hasan BUET L-3 T-1, De. o ME ME 31: Flid Mechanics-I Jan Conseraion o Momenm Since,,,,,,,,, D D D D oal local ; conecie,, Similarl D D D D A > A Area=A 1 A < A 3 1 Sead lo eloci increases 1 o eloci decreases o 3 a Conecie acceleraion Dr. A.B.M. Toiqe Hasan BUET L-3 T-1, De. o ME ME 31: Flid Mechanics-I Jan
5 8/7/18 Conseraion o Momenm The rincial orces ih hich e are concerned are hose hich ac direcl on he mass o he lid elemen, he bod orce, and hose hich ac on is srace, he ressre orces and shear orces. The sress ssem acing on an elemen o he srace is shon in igre: There is a oal o 6 shear sresses and 3 normal sresses acing on a lid elemen. The roeries o mos lids hae no reerred direcion in sace; ha is, lids are isoroic. Asa resl- ace shear shear ace ace normal Dr. A.B.M. Toiqe Hasan BUET L-3 T-1, De. o ME ME 31: Flid Mechanics-I Jan Conseraion o Momenm In general, he arios sresses change rom oin o oin coninm aroach. Ths, he rodce ne orces on he lid aricle, hich case i o accelerae. To simli he illsraion o he orce balance on he lid aricle, consider a D lo, as indicaed in igre. The reslan orce in -direcion or a ni deh in he -direcion is here is he bod orce er ni mass in -direcion. Inclding lo in he -direcion, he reslan orce in he -direcion- F Dr. A.B.M. Toiqe Hasan BUET L-3 T-1, De. o ME ME 31: Flid Mechanics-I Jan
6 8/7/18 6 Conseraion o Momenm Use his eression in eqn. 1 or -direcion: D D D F Similarl, or - and -direcions D Dr. A.B.M. Toiqe Hasan BUET 11 L-3 T-1, De. o ME ME 31: Flid Mechanics-I Jan. 18 These are he basic orms o Naier-Sokes eqaions NS eqaions. Oher lid mechanical relaions are obios o sole sch eqaions. NS eqaions are he mos amos eqaions or adanced analsis in lid dnamics. Sress-deormaion relaion: For incomressible Neonian lids i is knon ha he sresses are linearl relaed o he raes o deormaion and can be eressed in Caresian coordinaes,, as: Naier Sokes Eqaions sresses : normal For here μ is he moleclar iscosi o lid Dr. A.B.M. Toiqe Hasan BUET 1 L-3 T-1, De. o ME ME 31: Flid Mechanics-I Jan. 18 here μ is he moleclar iscosi o lid. Pa.s 1 1. Pa.s aer air
7 8/7/18 7 Naier Sokes Eqaions sresses : shear For No, se hese sress-deormaion relaions in NS eqaion in -direcion: Dr. A.B.M. Toiqe Hasan BUET 13 L-3 T-1, De. o ME ME 31: Flid Mechanics-I Jan. 18 Naier Sokes Eqaions conini eqaion ; = Dr. A.B.M. Toiqe Hasan BUET 14 L-3 T-1, De. o ME ME 31: Flid Mechanics-I Jan. 18
8 8/7/18 8 Naier Sokes Eqaions : Finall, he comlee se o Naier-Sokes eqaions in Caresian Coordinaes,, are: : : nd order arial dierenial eqaions Non-linear arial dierenial eqaions Dr. A.B.M. Toiqe Hasan BUET 15 L-3 T-1, De. o ME ME 31: Flid Mechanics-I Jan. 18 q q Since he Naier-Sokes eqaions are nonlinear, second-order arial dierenial eqaions, hese are no manageable or eac mahemaical solions ece in a e simliied lid lo cases. Nmerical solion is a ms o sole mch comlicaed arial dierenial eqaions NS eqaions. This oens a broad horion o mechanical engineering.
ME 425: Aerodynamics
3/4/18 ME 45: Aerodnamics Dr. A.B.M. Toiqe Hasan Proessor Deparmen o Mechanical Engineering Bangladesh Uniersi o Engineering & Technolog BUET Dhaka Lecre-6 3/4/18 Fndamenals so Aerodnamics eacher.be.ac.bd/oiqehasan/
More informationME 425: Aerodynamics
ME 45: Aerodnamics Dr. A.B.M. Toiqe Hasan Proessor Deparmen o Mechanical Engineering Bangladesh Uniersi o Engineering & Technolog BUET, Dhaka Lecre-7 Fndamenals so Aerodnamics oiqehasan.be.ac.bd oiqehasan@me.be.ac.bd
More informationAtmospheric Dynamics 11:670:324. Class Time: Tuesdays and Fridays 9:15-10:35
Amospheric Dnamics 11:67:324 Class ime: esdas and Fridas 9:15-1:35 Insrcors: Dr. Anhon J. Broccoli (ENR 229 broccoli@ensci.rgers.ed 848-932-5749 Dr. Benjamin Linner (ENR 25 linner@ensci.rgers.ed 848-932-5731
More informationATMS 310 The Vorticity Equation. The Vorticity Equation describes the factors that can alter the magnitude of the absolute vorticity with time.
ATMS 30 The Vorici Eqaion The Vorici Eqaion describes he acors ha can aler he magnide o he absole orici ih ime. Vorici Eqaion in Caresian Coordinaes The (,,,) orm is deried rom he rimiie horional eqaions
More informationVorticity equation 2. Why did Charney call it PV?
Vorici eqaion Wh i Charne call i PV? The Vorici Eqaion Wan o nersan he rocesses ha roce changes in orici. So erie an eression ha incles he ime eriaie o orici: Sm o orces in irecion Recall ha he momenm
More informationCFD Modelling of Indoor Air Quality and Thermal Comfort
Proceedings of he nd IASME / WSEAS Inernaional Conference on Coninm Mechanics (CM'07), Pororo, Sloenia, Ma 5-7, 007 CFD Modelling of Indoor Air Qali and Thermal Comfor LÁSZLÓ KAJTÁR ANITA LEITNER Dearmen
More informationINTERMEDIATE FLUID MECHANICS
INTERMEDIATE FLID MECHANICS Lecre 1: Inrodcion Benoi Cshman-Roisin Thaer School of Engineering Darmoh College Definiion of a Flid As opposed o a solid a flid is a sbsance ha canno resis a shear force iho
More informationRTT relates between the system approach with finite control volume approach for a system property:
8//8 ME 3: FLUI MECHANI-I r. A.B.M. Tofiqe Hasan Professor eparmen of Mecanical Enineerin Banlades Universiy of Enineerin & Tecnoloy (BUET, aka Lecre- 8//8 Flid ynamics eacer.be.ac.bd/ofiqeasan/ bd/ofiqeasan/
More informationME 3560 Fluid Mechanics
ME3560 Flid Mechanics Fall 08 ME 3560 Flid Mechanics Analsis of Flid Flo Analsis of Flid Flo ME3560 Flid Mechanics Fall 08 6. Flid Elemen Kinemaics In geneal a flid paicle can ndego anslaion, linea defomaion
More informationMesoscale Meteorology: Supercell Dynamics 25, 27 April 2017 Overview Supercell thunderstorms are long-lived single-cell thunderstorms, with
Mesoscale Meeorolog: Sercell Dnamics 5, 7 Aril 7 Oerie Sercell hndersorms are long-lied single-cell hndersorms, ih longeiies ranging rom o oer 6 h. In conras o single-cell hndersorms, hich hae no areciable
More informationIntegration of the equation of motion with respect to time rather than displacement leads to the equations of impulse and momentum.
Inegraion of he equaion of moion wih respec o ime raher han displacemen leads o he equaions of impulse and momenum. These equaions greal faciliae he soluion of man problems in which he applied forces ac
More informationDepartment of Chemical Engineering University of Tennessee Prof. David Keffer. Course Lecture Notes SIXTEEN
D. Keffe - ChE 40: Hea Tansfe and Fluid Flow Deamen of Chemical Enee Uniesi of Tennessee Pof. Daid Keffe Couse Lecue Noes SIXTEEN SECTION.6 DIFFERENTIL EQUTIONS OF CONTINUITY SECTION.7 DIFFERENTIL EQUTIONS
More informationLecture 5. Differential Analysis of Fluid Flow Navier-Stockes equation
Lectre 5 Differential Analsis of Flid Flo Naier-Stockes eqation Differential analsis of Flid Flo The aim: to rodce differential eqation describing the motion of flid in detail Flid Element Kinematics An
More information3D Coordinate Systems. 3D Geometric Transformation Chapt. 5 in FVD, Chapt. 11 in Hearn & Baker. Right-handed coordinate system:
3D Geomeric ransformaion Chap. 5 in FVD, Chap. in Hearn & Baker 3D Coordinae Ssems Righ-handed coordinae ssem: Lef-handed coordinae ssem: 2 Reminder: Vecor rodc U V UV VU sin ˆ V nu V U V U ˆ ˆ ˆ 3D oin
More informationM E FLUID MECHANICS II
Name: Sden No.: M E 335.3 FLUID MECHANICS II Depamen o Mechanical Enineein Uniesi o Saskachean Final Eam Monda, Apil, 003, 9:00 a.m. :00 p.m. Insco: oesso Daid Smne LEASE READ CAREFULLY: This eam has 7
More informationConcept of Stress at a Point
Washkeic College of Engineering Section : STRONG FORMULATION Concept of Stress at a Point Consider a point ithin an arbitraril loaded deformable bod Define Normal Stress Shear Stress lim A Fn A lim A FS
More informationChapter 12: Velocity, acceleration, and forces
To Feel a Force Chaper Spring, Chaper : A. Saes of moion For moion on or near he surface of he earh, i is naural o measure moion wih respec o objecs fixed o he earh. The 4 hr. roaion of he earh has a measurable
More informationCheck in: 1 If m = 2(x + 1) and n = find y when. b y = 2m n 2
7 Parameric equaions This chaer will show ou how o skech curves using heir arameric equaions conver arameric equaions o Caresian equaions find oins of inersecion of curves and lines using arameric equaions
More informationMethod of Moment Area Equations
Noe proided b JRR Page-1 Noe proided b JRR Page- Inrodcion ehod of omen rea qaions Perform deformaion analsis of flere-dominaed srcres eams Frames asic ssmpions (on.) No aial deformaion (aiall rigid members)
More informationAdvanced Control Systems Problem Sheet for Part B: Multivariable Systems
436-45 Advanced Conrol Ssems Problem Shee for Par B: Mlivariable Ssems Qesion B 998 Given a lan o be conrolled, which is described b a sae-sace model A B C Oline he rocess b which o wold design a discree
More informationSynoptic Meteorology II: The Q-Vector Form of the Omega Equation. 3-5 March 2015
Snoic Meeorolo II: he Q-Vecor Form o he Omea Eqaion 3-5 March 15 eadins: Secion.3 o Midlaide Snoic Meeorolo. Moiaion: Wh Do We Need Anoher Omea Eqaion? he qasi-eosrohic omea eqaion is an ecellen dianosic
More informationCSE-4303/CSE-5365 Computer Graphics Fall 1996 Take home Test
Comper Graphics roblem #1) A bi-cbic parameric srface is defined by Hermie geomery in he direcion of parameer. In he direcion, he geomery ecor is defined by a poin @0, a poin @0.5, a angen ecor @1 and
More informationPhysics Notes - Ch. 2 Motion in One Dimension
Physics Noes - Ch. Moion in One Dimension I. The naure o physical quaniies: scalars and ecors A. Scalar quaniy ha describes only magniude (how much), NOT including direcion; e. mass, emperaure, ime, olume,
More informationThe Euler-Lagrange Approach for Steady and Unsteady Flows. M. Sommerfeld. www-mvt.iw.uni-halle.de. Title. Zentrum für Ingenieurwissenschaften
Tile The Eler-Lagrange Aroach for Seady and Unseady Flows Joseh-Lois Lagrange (736 83) M. Sommerfeld Leonard Eler (707 783) Zenrm für Ingenierwissenschafen D-06099 Halle (Saale), Germany www-mv.iw.ni-halle.de
More informationKinematics in two Dimensions
Lecure 5 Chaper 4 Phsics I Kinemaics in wo Dimensions Course websie: hp://facul.uml.edu/andri_danlo/teachin/phsicsi PHYS.141 Lecure 5 Danlo Deparmen of Phsics and Applied Phsics Toda we are oin o discuss:
More informationHeat and Mass Transfer on the Unsteady MHD Flow of Chemically Reacting Micropolar Fluid with Radiation and Joule Heating
Inernaional Jornal of heoreical and Alied Mahemaics 7; (): - h://.scienceblishinggro.com//iam doi:.68/.iam.7. Hea and Mass ransfer on he nsead MHD Flo of hemicall Reacing Microolar Flid ih Radiaion and
More informationCSE 5365 Computer Graphics. Take Home Test #1
CSE 5365 Comper Graphics Take Home Tes #1 Fall/1996 Tae-Hoon Kim roblem #1) A bi-cbic parameric srface is defined by Hermie geomery in he direcion of parameer. In he direcion, he geomery ecor is defined
More informationLecture 2: Telegrapher Equations For Transmission Lines. Power Flow.
Whies, EE 481/581 Lecure 2 Page 1 of 13 Lecure 2: Telegraher Equaions For Transmission Lines. Power Flow. Microsri is one mehod for making elecrical connecions in a microwae circui. I is consruced wih
More informationKinematics in two dimensions
Lecure 5 Phsics I 9.18.13 Kinemaics in wo dimensions Course websie: hp://facul.uml.edu/andri_danlo/teaching/phsicsi Lecure Capure: hp://echo36.uml.edu/danlo13/phsics1fall.hml 95.141, Fall 13, Lecure 5
More informationComputing with diode model
ECE 570 Session 5 C 752E Comuer Aided Engineering for negraed Circuis Comuing wih diode model Objecie: nroduce conces in numerical circui analsis Ouline: 1. Model of an examle circui wih a diode 2. Ouline
More informationSurfaces in the space E
3 Srfaces in he sace E Le ecor fncion in wo ariables be efine on region R = x y y whose scalar coorinae fncions x y y are a leas once iffereniable on region. Hoograh of ecor fncion is a iece-wise smooh
More informationSMS-618, Particle Dynamics, Fall 2003 (E. Boss, last updated: 10/8/2003) Conservation equations in fluids
SMS-68 Parcle Dnamcs Fall 3 (E. Boss las daed: /8/3) onseraon eqaons n flds onces e need: ensor (Sress) ecors (e.g. oson eloc) and scalars (e.g. S O). Prode means o descrbe conseraon las h comac noaon
More informationDerivation of the basic equations of fluid flows. No. Conservation of mass of a solute (applies to non-sinking particles at low concentration).
Deriation of the basic eqations of flid flos. No article in the flid at this stage (net eek). Conseration of mass of the flid. Conseration of mass of a solte (alies to non-sinking articles at lo concentration).
More informationVelocity is a relative quantity
Veloci is a relaie quani Disenangling Coordinaes PHY2053, Fall 2013, Lecure 6 Newon s Laws 2 PHY2053, Fall 2013, Lecure 6 Newon s Laws 3 R. Field 9/6/2012 Uniersi of Florida PHY 2053 Page 8 Reference Frames
More informationDESIGN OF TENSION MEMBERS
CHAPTER Srcral Seel Design LRFD Mehod DESIGN OF TENSION MEMBERS Third Ediion A. J. Clark School of Engineering Deparmen of Civil and Environmenal Engineering Par II Srcral Seel Design and Analysis 4 FALL
More informationScalar Conservation Laws
MATH-459 Nmerical Mehods for Conservaion Laws by Prof. Jan S. Heshaven Solion se : Scalar Conservaion Laws Eercise. The inegral form of he scalar conservaion law + f ) = is given in Eq. below. ˆ 2, 2 )
More informationTheory of! Partial Differential Equations!
hp://www.nd.edu/~gryggva/cfd-course/! Ouline! Theory o! Parial Dierenial Equaions! Gréar Tryggvason! Spring 011! Basic Properies o PDE!! Quasi-linear Firs Order Equaions! - Characerisics! - Linear and
More informationEquations of motion for constant acceleration
Lecure 3 Chaper 2 Physics I 01.29.2014 Equaions of moion for consan acceleraion Course websie: hp://faculy.uml.edu/andriy_danylo/teaching/physicsi Lecure Capure: hp://echo360.uml.edu/danylo2013/physics1spring.hml
More informationand v y . The changes occur, respectively, because of the acceleration components a x and a y
Week 3 Reciaion: Chaper3 : Problems: 1, 16, 9, 37, 41, 71. 1. A spacecraf is raveling wih a veloci of v0 = 5480 m/s along he + direcion. Two engines are urned on for a ime of 84 s. One engine gives he
More informationTheory of! Partial Differential Equations-I!
hp://users.wpi.edu/~grear/me61.hml! Ouline! Theory o! Parial Dierenial Equaions-I! Gréar Tryggvason! Spring 010! Basic Properies o PDE!! Quasi-linear Firs Order Equaions! - Characerisics! - Linear and
More informationPH2130 Mathematical Methods Lab 3. z x
PH130 Mahemaical Mehods Lab 3 This scrip shold keep yo bsy for he ne wo weeks. Yo shold aim o creae a idy and well-srcred Mahemaica Noebook. Do inclde plenifl annoaions o show ha yo know wha yo are doing,
More informationInternational Journal of Pure and Applied Sciences and Technology
In. J. Pre Appl. Sci. echnol. () (4) pp. -8 Inernaional Jornal of Pre and Applied Sciences and echnolog ISSN 9-67 Aailable online a.ijopaasa.in Research Paper Effec of Variable Viscosi on hird Grade Flid
More informationNumerical Modeling of the Effect of Fine Water Mist on the Small Scale Flame Spreading Over Solid Combustibles
Nmerical Modeling of he Effec of Fine Waer Mis on he Small Scale Flame Spreading Oer Solid Combsibles A.I. KARPOV 1, V. NOVOZHILOV, V.K. BULGAKOV 3, and A.A. GALAT 1 1 eparmen of Comper Science Komsomolsk-on-Amr
More informationExperimental Study and Three-Dimensional Numerical Flow Simulation in a Centrifugal Pump when Handling Viscous Fluids
IUST Inernaional Jornal o Engineering Science, Vol. 17, No.3-, 6, Page 53-6 Experimenal Sdy and Three-Dimensional Nmerical Flo Simlaion in a Cenrigal Pmp hen andling Viscos Flids Donloaded rom ijiepr.is.ac.ir
More informationThe Pressure Perturbation Equation: Exposed!
Pressre Perrbain Eqain Page f 6 The Pressre Perrbain Eqain: Esed! The rainal dnamics f sercell srms hae a l d ih he ressre errbains creaed b he air fl. I is his effec ha makes sercells secial. Phase :
More informationINSTANTANEOUS VELOCITY
INSTANTANEOUS VELOCITY I claim ha ha if acceleraion is consan, hen he elociy is a linear funcion of ime and he posiion a quadraic funcion of ime. We wan o inesigae hose claims, and a he same ime, work
More informationNEWTON S SECOND LAW OF MOTION
Course and Secion Dae Names NEWTON S SECOND LAW OF MOTION The acceleraion of an objec is defined as he rae of change of elociy. If he elociy changes by an amoun in a ime, hen he aerage acceleraion during
More informationWe may write the basic equation of motion for the particle, as
We ma wrie he basic equaion of moion for he paricle, as or F m dg F F linear impulse G dg G G G G change in linear F momenum dg The produc of force and ime is defined as he linear impulse of he force,
More informationMath 2214 Solution Test 1 B Spring 2016
Mah 14 Soluion Te 1 B Spring 016 Problem 1: Ue eparaion of ariable o ole he Iniial alue DE Soluion (14p) e =, (0) = 0 d = e e d e d = o = ln e d uing u-du b leing u = e 1 e = + where C = for he iniial
More informationLecture 16 (Momentum and Impulse, Collisions and Conservation of Momentum) Physics Spring 2017 Douglas Fields
Lecure 16 (Momenum and Impulse, Collisions and Conservaion o Momenum) Physics 160-02 Spring 2017 Douglas Fields Newon s Laws & Energy The work-energy heorem is relaed o Newon s 2 nd Law W KE 1 2 1 2 F
More informationOne-Dimensional Kinematics
One-Dimensional Kinemaics One dimensional kinemaics refers o moion along a sraigh line. Een hough we lie in a 3-dimension world, moion can ofen be absraced o a single dimension. We can also describe moion
More informationThe Vorticity Equation
The Vorticit Eqation Potential orticit Circlation theorem is reall good Circlation theorem imlies a consered qantit dp dt 0 P g 2 PV or barotroic lid General orm o Ertel s otential orticit: P g const Consider
More informationTwo Dimensional Dynamics
Physics 11: Lecure 6 Two Dimensional Dynamics Today s lecure will coer Chaper 4 Exam I Physics 11: Lecure 6, Pg 1 Brie Reiew Thus Far Newon s Laws o moion: SF=ma Kinemaics: x = x + + ½ a Dynamics Today
More informationModelisation and Simulation of Heat and Mass Transfers during Solar Drying of Sewage Sludge with Introduction of Real Climatic Conditions
Jornal o Alied Flid Mechanics, Vol., No.,. 65-659, 7. Aailable online a www.jamonline.ne, ISSN 735-357, EISSN 735-3645. DOI:.8869/acadb.jam.73.39.6854 Modelisaion and Simlaion o Hea and Mass ransers dring
More informationPhysics 101: Lecture 03 Kinematics Today s lecture will cover Textbook Sections (and some Ch. 4)
Physics 101: Lecure 03 Kinemaics Today s lecure will coer Texbook Secions 3.1-3.3 (and some Ch. 4) Physics 101: Lecure 3, Pg 1 A Refresher: Deermine he force exered by he hand o suspend he 45 kg mass as
More informationDIRECT NUMERICAL SIMULATION OF FLOWS OVER A CAVITY WITH FLOW CONTROL USING A MOVING BOTTOM WALL
11h World Congress on Comuaional Mechanics (WCCM XI) 5h Euroean Conference on Comuaional Mechanics (ECCM V) 6h Euroean Conference on Comuaional Fluid Dynamics (ECFD VI) E. Oñae, J. Olier and A. Huera (Eds)
More informationTwo Dimensional Dynamics
Physics 11: Lecure 6 Two Dimensional Dynamics Today s lecure will coer Chaper 4 Saring Wed Sep 15, W-F oice hours will be in 3 Loomis. Exam I M oice hours will coninue in 36 Loomis Physics 11: Lecure 6,
More informationWell-posedness of the generalized Proudman-Johnson equation without viscosity. Hisashi Okamoto RIMS, Kyoto University
Well-posedness o he generalized Prodman-Johnson eqaion wiho viscosiy Hisashi Okamoo RIMS, Kyoo Universiy okamoo@krims.kyoo-.ac.jp Generalized Prodman-Johnson eqaion Proposed in by Zh and O. in order o
More informationTHERMOPHORESIS PARTICLE DEPOSITION ON FLAT SURFACES DUE TO FLUID FLOW IN DARCY-FORCHHEIMER POROUS MEDIUM
elfh Inernaional Waer echnolog onference, IW1 008 Aleandria, Egp 1 HERMOPHORESIS PARILE DEPOSIION ON FLA SRFAES DE O FLID FLOW IN DAR-FORHHEIMER POROS MEDIM Rebhi A. Damseh 1 and Kamel Alzboon 1 Mechanical
More informationDirac s hole theory and the Pauli principle: clearing up the confusion.
Dirac s hole heory and he Pauli rincile: clearing u he conusion. Dan Solomon Rauland-Borg Cororaion 8 W. Cenral Road Moun Prosec IL 656 USA Email: dan.solomon@rauland.com Absrac. In Dirac s hole heory
More informationPage 1 o 13 1. The brighes sar in he nigh sky is α Canis Majoris, also known as Sirius. I lies 8.8 ligh-years away. Express his disance in meers. ( ligh-year is he disance coered by ligh in one year. Ligh
More informationASTR415: Problem Set #5
ASTR45: Problem Se #5 Curran D. Muhlberger Universi of Marland (Daed: April 25, 27) Three ssems of coupled differenial equaions were sudied using inegraors based on Euler s mehod, a fourh-order Runge-Kua
More informationPlasma Astrophysics Chapter 3: Kinetic Theory. Yosuke Mizuno Institute of Astronomy National Tsing-Hua University
Plasma Asrophysics Chaper 3: Kineic Theory Yosuke Mizuno Insiue o Asronomy Naional Tsing-Hua Universiy Kineic Theory Single paricle descripion: enuous plasma wih srong exernal ields, imporan or gaining
More informationCH.7. PLANE LINEAR ELASTICITY. Continuum Mechanics Course (MMC) - ETSECCPB - UPC
CH.7. PLANE LINEAR ELASTICITY Coninuum Mechanics Course (MMC) - ETSECCPB - UPC Overview Plane Linear Elasici Theor Plane Sress Simplifing Hpohesis Srain Field Consiuive Equaion Displacemen Field The Linear
More informationPhys 221 Fall Chapter 2. Motion in One Dimension. 2014, 2005 A. Dzyubenko Brooks/Cole
Phys 221 Fall 2014 Chaper 2 Moion in One Dimension 2014, 2005 A. Dzyubenko 2004 Brooks/Cole 1 Kinemaics Kinemaics, a par of classical mechanics: Describes moion in erms of space and ime Ignores he agen
More informationChapter 6 Differential Analysis of Fluid Flow
57:00 Mechanics of Flids and Transpor Processes Chaper 6 Professor Fred Sern Fall 006 1 Chaper 6 Differenial Analysis of Flid Flow Flid Elemen Kinemaics Flid elemen moion consiss of ranslaion, linear deformaion,
More informationSOLVING AN OPTIMAL CONTROL PROBLEM WITH MATLAB
SOLVING AN OPIMAL CONROL PROBLEM WIH MALAB RGeeharamani, SSviha Assisan Proessor, Researh Sholar KG College O Ars and Siene Absra: In his paper, we presens a Ponryagin Priniple or Bolza problem he proedre
More informationStudy on convection improvement of standard vacuum tube
IOP Conference Series: Earh and Enironmenal Science PAPER OPEN ACCESS Sd on conecion improemen of sandard acm be To cie his aricle: J H He e al 017 IOP Conf. Ser.: Earh Eniron. Sci. 93 0100 View he aricle
More informationConservation Laws and Hamiltonian Symmetries of Whitham-Broer-Kaup Equations
Indian Jornal of Science and Technology Vol 8( 78 84 Janary 05 ISSN (Prin : 0974-84 ISSN (Online : 0974-545 DOI : 0.7485/ijs/05/8i/47809 Conseraion Laws and Hamilonian Symmeries of Whiham-Broer-Kap Eqaions
More informationSpace-Time Electrodynamics, and Magnetic Monopoles
Gauge Insiue Journal Space-Time lecrodnamics and Magneic Monopoles vic0@comcas.ne June 203 Absrac Mawell s lecrodnamics quaions for he 3- Space Vecor Fields disallow magneic monopoles. Those equaions could
More informationChapter 3 Common Families of Distributions
Chaer 3 Common Families of Disribuions Secion 31 - Inroducion Purose of his Chaer: Caalog many of common saisical disribuions (families of disribuions ha are indeed by one or more arameers) Wha we should
More informationLAB # 2 - Equilibrium (static)
AB # - Equilibrium (saic) Inroducion Isaac Newon's conribuion o physics was o recognize ha despie he seeming compleiy of he Unierse, he moion of is pars is guided by surprisingly simple aws. Newon's inspiraion
More information4.2 Continuous-Time Systems and Processes Problem Definition Let the state variable representation of a linear system be
4 COVARIANCE ROAGAION 41 Inrodcion Now ha we have compleed or review of linear sysems and random processes, we wan o eamine he performance of linear sysems ecied by random processes he sandard approach
More informationVI. Computational Fluid Dynamics 1. Examples of numerical simulation
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
More informationME 321: FLUID MECHANICS-I
6/07/08 ME 3: LUID MECHANI-I Dr. A.B.M. Toufique Hasan Professor Department of Mechanical Engineering Bangladesh Universit of Engineering & Technolog (BUET), Dhaka Lecture- 4/07/08 Momentum Principle teacher.buet.ac.bd/toufiquehasan/
More information27.1 The Heisenberg uncertainty principles
7.1 Te Heisenberg uncerainy rinciles Naure is bilaeral: aricles are waves and waves are aricles.te aricle asec carries wi i e radiional conces of osiion and momenum; Te wave asec carries wi i e conces
More informationPhysics 235 Chapter 2. Chapter 2 Newtonian Mechanics Single Particle
Chaper 2 Newonian Mechanics Single Paricle In his Chaper we will review wha Newon s laws of mechanics ell us abou he moion of a single paricle. Newon s laws are only valid in suiable reference frames,
More information4.5 Constant Acceleration
4.5 Consan Acceleraion v() v() = v 0 + a a() a a() = a v 0 Area = a (a) (b) Figure 4.8 Consan acceleraion: (a) velociy, (b) acceleraion When he x -componen of he velociy is a linear funcion (Figure 4.8(a)),
More informationA numerical solution of the NS equations based on the mean value theorem with applications to aerothermodynamics
Adanced Compaional Mehod in Hea ranfer IX 97 A nmerical olion of he NS eqaion baed on he mean ale heorem wih applicaion o aerohermodnamic F. Fergon & G. Elamin Deparmen of Mechanical Engineering, Norh
More informationPhysics Unit Workbook Two Dimensional Kinematics
Name: Per: L o s A l o s H i g h S c h o o l Phsics Uni Workbook Two Dimensional Kinemaics Mr. Randall 1968 - Presen adam.randall@mla.ne www.laphsics.com a o 1 a o o ) ( o o a o o ) ( 1 1 a o g o 1 g o
More informationA Mathematical model to Solve Reaction Diffusion Equation using Differential Transformation Method
Inernaional Jornal of Mahemaics Trends and Technology- Volme Isse- A Mahemaical model o Solve Reacion Diffsion Eqaion sing Differenial Transformaion Mehod Rahl Bhadaria # A.K. Singh * D.P Singh # #Deparmen
More informationNon-uniform circular motion *
OpenSax-CNX module: m14020 1 Non-uniform circular moion * Sunil Kumar Singh This work is produced by OpenSax-CNX and licensed under he Creaive Commons Aribuion License 2.0 Wha do we mean by non-uniform
More information10. Euler's equation (differential momentum equation)
3 Ele's eqaion (iffeenial momenm eqaion) Inisci flo: µ eslan of foces mass acceleaion Inisci flo: foces case b he esse an fiel of foce In iecion: ) ( a o a If (), ) ( a a () If cons he nknon aiables ae:,,,
More information0.1 MAXIMUM LIKELIHOOD ESTIMATION EXPLAINED
0.1 MAXIMUM LIKELIHOOD ESTIMATIO EXPLAIED Maximum likelihood esimaion is a bes-fi saisical mehod for he esimaion of he values of he parameers of a sysem, based on a se of observaions of a random variable
More informationPracticing Problem Solving and Graphing
Pracicing Problem Solving and Graphing Tes 1: Jan 30, 7pm, Ming Hsieh G20 The Bes Ways To Pracice for Tes Bes If need more, ry suggesed problems from each new opic: Suden Response Examples A pas opic ha
More informationChapters 2 Kinematics. Position, Distance, Displacement
Chapers Knemacs Poson, Dsance, Dsplacemen Mechancs: Knemacs and Dynamcs. Knemacs deals wh moon, bu s no concerned wh he cause o moon. Dynamcs deals wh he relaonshp beween orce and moon. The word dsplacemen
More informationTHE DARBOUX TRIHEDRONS OF REGULAR CURVES ON A REGULAR TIME-LIKE SURFACE. Emin Özyilmaz
Mahemaical and Compaional Applicaions, Vol. 9, o., pp. 7-8, 04 THE DARBOUX TRIHEDROS OF REULAR CURVES O A REULAR TIME-LIKE SURFACE Emin Özyilmaz Deparmen of Mahemaics, Facly of Science, Ee Uniersiy, TR-500
More informationLearning from a Golf Ball
Session 1566 Learning from a Golf Ball Alireza Mohammadzadeh Padnos School of Engineering Grand Valley Sae Uniersiy Oeriew Projecile moion of objecs, in he absence of air fricion, is sdied in dynamics
More informationFinite Strain Consolidation Numerical Methods in Geotechnical Engineering. Murray Fredlund June 7, 1995
Finie Srain Consolidaion Numerical Mehods in Geoechnical Engineering Murra Fredlund June 7, 1995 Finie Srain Consolidaion Page Murra Fredlund Table of Conens 1. INTRODUCTION... 4. THEORY... 5.1 Coordinae
More informationSIMPLIFIED METHOD ON MATHEMATICAL MODEL OF TRANSONIC AXIAL COMPRESSORS
ICAS CONRESS SIMPLIIED MEHOD ON MAHEMAICAL MODEL O RANSONIC AXIAL COMPRESSORS Árád ERESS Ph. D. sdn BDAPES NIERSIY O ECHNOLOY AND ECONOMICS Darmn o Aircra and Shis Kords: CD, rbomachinar, C, C, ini olm
More informationThe Bloch Space of Analytic functions
Inernaional OPEN ACCESS Jornal O Modern Engineering Research (IJMER) The Bloch Space o Analyic ncions S Nagendra, Pro E Keshava Reddy Deparmen o Mahemaics, Governmen Degree College, Pormamilla Deparmen
More informations in boxe wers ans Put
Pu answers in boxes Main Ideas in Class Toda Inroducion o Falling Appl Old Equaions Graphing Free Fall Sole Free Fall Problems Pracice:.45,.47,.53,.59,.61,.63,.69, Muliple Choice.1 Freel Falling Objecs
More informationUnit 1 Test Review Physics Basics, Movement, and Vectors Chapters 1-3
A.P. Physics B Uni 1 Tes Reiew Physics Basics, Moemen, and Vecors Chapers 1-3 * In sudying for your es, make sure o sudy his reiew shee along wih your quizzes and homework assignmens. Muliple Choice Reiew:
More informationMaxwell s Equations and Electromagnetic Waves
Phsics 36: Waves Lecure 3 /9/8 Maxwell s quaions and lecromagneic Waves Four Laws of lecromagneism. Gauss Law qenc all da ρdv Inegral From From he vecor ideni da dv Therefore, we ma wrie Gauss Law as ρ
More informationAsymptotic Solution of the Anti-Plane Problem for a Two-Dimensional Lattice
Asympoic Solion of he Ani-Plane Problem for a Two-Dimensional Laice N.I. Aleksandrova N.A. Chinakal Insie of Mining, Siberian Branch, Rssian Academy of Sciences, Krasnyi pr. 91, Novosibirsk, 6391 Rssia,
More informationCORRELATION. two variables may be related. SAT scores, GPA hours in therapy, self-esteem grade on homeworks, grade on exams
Inrodcion o Saisics in sychology SY 1 rofessor Greg Francis Lecre 1 correlaion Did I damage my dagher s eyes? CORRELATION wo ariables may be relaed SAT scores, GA hors in herapy, self-eseem grade on homeworks,
More informationwhere the coordinate X (t) describes the system motion. X has its origin at the system static equilibrium position (SEP).
Appendix A: Conservaion of Mechanical Energy = Conservaion of Linear Momenum Consider he moion of a nd order mechanical sysem comprised of he fundamenal mechanical elemens: ineria or mass (M), siffness
More informationVISUALIZED DEVELOPMENT OF ONSET FLOW BETWEEN TWO ROTATING CYLINDERS
ISFV14-14 h Inernaional Symposim on Flo Visalizaion Jne 1-4, 1, EXCO Daeg, Korea VISUALIZED DEVELOPMENT OF ONSET FLOW BETWEEN TWO ROTATING CYLINDERS Takashi Waanabe.*, Yorinob Toya**, Shohei Fjisaa* *Gradae
More informationDetecting Movement SINA 07/08
Deecing Moemen How do we perceie moemen? This is no a simple qesion becase we are neer saionar obserers (ees and head moe An imporan isse is how we discriminae he moion of he eernal world from he moion
More informationProbabilistic Robotics Sebastian Thrun-- Stanford
robabilisic Roboics Sebasian Thrn-- Sanford Inrodcion robabiliies Baes rle Baes filers robabilisic Roboics Ke idea: Eplici represenaion of ncerain sing he calcls of probabili heor ercepion sae esimaion
More information