ME 425: Aerodynamics

Size: px
Start display at page:

Download "ME 425: Aerodynamics"

Transcription

1 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/ oiqehasan@me.be.ac.bd Dr. A.B.M. Toiqe Hasan BUET L-4 T- Dep. o ME ME 45: Aerodnamics Jan Fndamenal principles in Aerodnamics Flid Mechanics: 1. Conseraion o mass. Conseraion o momenm 3. Conseraion o energ Dr. A.B.M. Toiqe Hasan BUET L-4 T- Dep. o ME ME 45: Aerodnamics Jan. 18 1

2 3/4/18 Mass can neiher be creaed nor desroed. Consider a small olme o space conrol olme hrogh hich a lid is loing. For simplici a D lo is considered and he conrol olme is bonded b he sraces and asshoninigre. Accordingohelahe 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 prodc o densi eloci componen normal o srace and he area o ha Conseraion o Mass The mass lo rae is eqal o he prodc o densi eloci componen normal o srace and he area o ha srace. In ecor orm ρ ρ da m s nˆ V A irs-order Talor series is sed o ealae he lo properies a he aces o he elemen since he properies are a ncion o posiion coninm approach. The ne olo o mass per ni o ime per ni deph is olo +e olo +e area olo +e olo +e inlo e Dr. A.B.M. Toiqe Hasan BUET 3 L-4 T- Dep. o ME ME 45: Aerodnamics Jan olo e inlo e inlo e area inlo e Conseraion o Mass hich ms be eqal he rae a hich he mass conained ihin he elemen decreases mass in de o decrease e 1 mass= densi olme Eqaing he aboe o epressions and diiding b - I -dimension is considered he dierenial orm o he aboe epression comes as Dr. A.B.M. Toiqe Hasan BUET 4 L-4 T- Dep. o ME ME 45: Aerodnamics Jan. 18 hich is knon as dierenial conini eqaion in ecor orm. V V operaor del and here

3 3/4/18 Conseraion o Mass In case o sead los he conini eqaion becomes as- V di V V div Compressible los Incompressible los Dr. A.B.M. Toiqe Hasan BUET L-4 T- Dep. o ME ME 45: Aerodnamics Jan Conseraion o Momenm Linear Momenm Eqaion The ne orce acing on a lid paricle is eqal o he ime rae o change o he linear momenm o he lid paricle. As lid elemen moes in space is eloci densi shape and olme ma change b is mass is consered. Conseraion o momenm can be rien as- F m DV D D direcion : F m D D direcion : F m D D direcion i : F m D V and F F F F 1 The eloci o a lid paricle is in general an eplici ncion o ime as ell as o is posiion. Frhermore he posiion coordinaes o he lid paricle are hemseles a ncion o ime. The deriaie in he aboe epression is reqenl ermed as paricle oal or sbsanial deriaie D/D o eloci. Dr. A.B.M. Toiqe Hasan BUET L-4 T- Dep. o ME ME 45: Aerodnamics Jan

4 3/4/18 4 Conseraion o Momenm Since conecie local oal D D D D D D D D Similarl Area=A A < A A 3 > A Dr. A.B.M. Toiqe Hasan BUET 7 L-4 T- Dep. o ME ME 45: Aerodnamics Jan. 18 Sead lo Veloci increases 1 o Veloci decreases o 3 a Conecie acceleraion Area=A 1 A < A 1 3 Conseraion o Momenm The principal 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 hepressre orces and shear orces. The sress ssem acing on an elemen o he srace is shon in igre: The properies o mos lids hae no preerred direcion in space ha is lids are isoropic. Asa resl Dr. A.B.M. Toiqe Hasan BUET 8 L-4 T- Dep. o ME ME 45: Aerodnamics Jan. 18

5 3/4/18 5 Conseraion o Momenm In general he arios sresses change rom poin o poin coninm approach. Ths he prodce ne orces on he lid paricle hich case i o accelerae. To simpli he illsraion o he orce balance on he lid paricle consider a D lo as indicaed in igre. The reslan orce in - direcion or a ni deph in he -direcion is here is he bod orce per ni mass in - direcion. Incldingloinhe-direcion he reslan orce in he -direcion- Dr. A.B.M. Toiqe Hasan BUET 9 L-4 T- Dep. o ME ME 45: Aerodnamics Jan. 18 F Conseraion o Momenm Use his epression in eqn. 1 or -direcion: D D D F Similarl or - and -direcions D d D d D Dr. A.B.M. Toiqe Hasan BUET 1 L-4 T- Dep. o ME ME 45: Aerodnamics Jan. 18 d These are he basic orm o Naier-Sokes eqaions.

ME 425: Aerodynamics

ME 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 information

ME 321: FLUID MECHANICS-I

ME 321: FLUID MECHANICS-I 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

More information

Atmospheric Dynamics 11:670:324. Class Time: Tuesdays and Fridays 9:15-10:35

Atmospheric 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 information

INTERMEDIATE FLUID MECHANICS

INTERMEDIATE 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 information

RTT relates between the system approach with finite control volume approach for a system property:

RTT 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 information

Vorticity equation 2. Why did Charney call it PV?

Vorticity 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 information

Integration of the equation of motion with respect to time rather than displacement leads to the equations of impulse and momentum.

Integration 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 information

ME 3560 Fluid Mechanics

ME 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 information

ATMS 310 The Vorticity Equation. The Vorticity Equation describes the factors that can alter the magnitude of the absolute vorticity with time.

ATMS 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 information

Kinematics in two dimensions

Kinematics 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 information

Velocity is a relative quantity

Velocity 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 information

We may write the basic equation of motion for the particle, as

We 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 information

CSE 5365 Computer Graphics. Take Home Test #1

CSE 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 information

Kinematics in two Dimensions

Kinematics 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 information

Physics Notes - Ch. 2 Motion in One Dimension

Physics 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 information

CSE-4303/CSE-5365 Computer Graphics Fall 1996 Take home Test

CSE-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 information

ME 321: FLUID MECHANICS-I

ME 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 information

M E FLUID MECHANICS II

M 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 information

CFD Modelling of Indoor Air Quality and Thermal Comfort

CFD 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 information

Theory of! Partial Differential Equations!

Theory 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 information

Method of Moment Area Equations

Method 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 information

Chapter 12: Velocity, acceleration, and forces

Chapter 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 information

AP Calculus BC Chapter 10 Part 1 AP Exam Problems

AP Calculus BC Chapter 10 Part 1 AP Exam Problems AP Calculus BC Chaper Par AP Eam Problems All problems are NO CALCULATOR unless oherwise indicaed Parameric Curves and Derivaives In he y plane, he graph of he parameric equaions = 5 + and y= for, is a

More information

1. The 200-kg lunar lander is descending onto the moon s surface with a velocity of 6 m/s when its retro-engine is fired. If the engine produces a

1. The 200-kg lunar lander is descending onto the moon s surface with a velocity of 6 m/s when its retro-engine is fired. If the engine produces a PROBLEMS. The -kg lunar lander is descending ono he moon s surface wih a eloci of 6 m/s when is rero-engine is fired. If he engine produces a hrus T for 4 s which aries wih he ime as shown and hen cus

More information

Course II. Lesson 7 Applications to Physics. 7A Velocity and Acceleration of a Particle

Course II. Lesson 7 Applications to Physics. 7A Velocity and Acceleration of a Particle Course II Lesson 7 Applicaions o Physics 7A Velociy and Acceleraion of a Paricle Moion in a Sraigh Line : Velociy O Aerage elociy Moion in he -ais + Δ + Δ 0 0 Δ Δ Insananeous elociy d d Δ Δ Δ 0 lim [ m/s

More information

a. Show that these lines intersect by finding the point of intersection. b. Find an equation for the plane containing these lines.

a. Show that these lines intersect by finding the point of intersection. b. Find an equation for the plane containing these lines. Mah A Final Eam Problems for onsideraion. Show all work for credi. Be sure o show wha you know. Given poins A(,,, B(,,, (,, 4 and (,,, find he volume of he parallelepiped wih adjacen edges AB, A, and A.

More information

Giambattista, Ch 3 Problems: 9, 15, 21, 27, 35, 37, 42, 43, 47, 55, 63, 76

Giambattista, Ch 3 Problems: 9, 15, 21, 27, 35, 37, 42, 43, 47, 55, 63, 76 Giambaisa, Ch 3 Problems: 9, 15, 21, 27, 35, 37, 42, 43, 47, 55, 63, 76 9. Sraeg Le be direced along he +x-axis and le be 60.0 CCW from Find he magniude of 6.0 B 60.0 4.0 A x 15. (a) Sraeg Since he angle

More information

Theory of! Partial Differential Equations-I!

Theory 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 information

Mat 267 Engineering Calculus III Updated on 04/30/ x 4y 4z 8x 16y / 4 0. x y z x y. 4x 4y 4z 24x 16y 8z.

Mat 267 Engineering Calculus III Updated on 04/30/ x 4y 4z 8x 16y / 4 0. x y z x y. 4x 4y 4z 24x 16y 8z. Ma 67 Engineering Calcls III Updaed on 04/0/0 r. Firoz Tes solion:. a) Find he cener and radis of he sphere 4 4 4z 8 6 0 z ( ) ( ) z / 4 The cener is a (, -, 0), and radis b) Find he cener and radis of

More information

ASTR415: Problem Set #5

ASTR415: 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 information

Physics 101: Lecture 03 Kinematics Today s lecture will cover Textbook Sections (and some Ch. 4)

Physics 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 information

Math 2214 Solution Test 1 B Spring 2016

Math 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 information

Concept of Stress at a Point

Concept 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 information

3D Coordinate Systems. 3D Geometric Transformation Chapt. 5 in FVD, Chapt. 11 in Hearn & Baker. Right-handed coordinate system:

3D 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 information

and v y . The changes occur, respectively, because of the acceleration components a x and a y

and 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 information

Cartesian tensors. Order (rank) Scalar. Vector. 3x3 matrix

Cartesian tensors. Order (rank) Scalar. Vector. 3x3 matrix Caresan ensors Order (rank) 0 1 3 a b c d k Scalar ecor 33 mar Caresan ensors Kronecker dela δ = 1 f = 0 f Le- Ca epslon ε k = 1 f,, k are cclc 1 f,, k are ancclc 0 oherse Smmaon conenon (o eqal ncces

More information

Equations of motion for constant acceleration

Equations 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 information

LAB # 2 - Equilibrium (static)

LAB # 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 information

Page 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 information

Study on convection improvement of standard vacuum tube

Study 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 information

MEI Mechanics 1 General motion. Section 1: Using calculus

MEI Mechanics 1 General motion. Section 1: Using calculus Soluions o Exercise MEI Mechanics General moion Secion : Using calculus. s 4 v a 6 4 4 When =, v 4 a 6 4 6. (i) When = 0, s = -, so he iniial displacemen = - m. s v 4 When = 0, v = so he iniial velociy

More information

Unit 1 Test Review Physics Basics, Movement, and Vectors Chapters 1-3

Unit 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 information

Research on Eddy Air-Curtain Dust Controlled Flow Field in Hard Rock Mechanized Driving Face

Research on Eddy Air-Curtain Dust Controlled Flow Field in Hard Rock Mechanized Driving Face JOURNAL OF NETWORKS, VOL. 8, NO., FEBRUARY 013 453 Research on Edd Air-Crain Ds Conrolled Flo Field in Hard Roc Mechanied Driing Face Wei-min Cheng 1,, Wen Nie 1,, Gang Zho 1, 1,, Jn-lei Yang 1. College

More information

UNIT # 01 (PART I) BASIC MATHEMATICS USED IN PHYSICS, UNIT & DIMENSIONS AND VECTORS. 8. Resultant = R P Q, R P 2Q

UNIT # 01 (PART I) BASIC MATHEMATICS USED IN PHYSICS, UNIT & DIMENSIONS AND VECTORS. 8. Resultant = R P Q, R P 2Q J-Phsics UNI # 0 (PAR I) ASIC MAHMAICS USD IN PHYSICS, UNI & DIMNSIONS AND VCORS XRCIS I. nclosed area : A r so da dr r Here r 8 cm, dr da 5 cm/s () (8) (5) 80 cm /s. Slope d d 6 9 if angen is parallel

More information

AP CALCULUS AB 2003 SCORING GUIDELINES (Form B)

AP CALCULUS AB 2003 SCORING GUIDELINES (Form B) SCORING GUIDELINES (Form B) Quesion A blood vessel is 6 millimeers (mm) long Disance wih circular cross secions of varying diameer. x (mm) 6 8 4 6 Diameer The able above gives he measuremens of he B(x)

More information

PHYSICS 220 Lecture 02 Motion, Forces, and Newton s Laws Textbook Sections

PHYSICS 220 Lecture 02 Motion, Forces, and Newton s Laws Textbook Sections PHYSICS 220 Lecure 02 Moion, Forces, and Newon s Laws Texbook Secions 2.2-2.4 Lecure 2 Purdue Universiy, Physics 220 1 Overview Las Lecure Unis Scienific Noaion Significan Figures Moion Displacemen: Δx

More information

Detecting Movement SINA 07/08

Detecting 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 information

Review Equations. Announcements 9/8/09. Table Tennis

Review Equations. Announcements 9/8/09. Table Tennis Announcemens 9/8/09 1. Course homepage ia: phsics.bu.edu Class web pages Phsics 105 (Colon J). (Class-wide email sen) Iclicker problem from las ime scores didn ge recorded. Clicker quizzes from lecures

More information

Chapter 5: Control Volume Approach and Continuity Principle Dr Ali Jawarneh

Chapter 5: Control Volume Approach and Continuity Principle Dr Ali Jawarneh Chaper 5: Conrol Volume Approach and Coninuiy Principle By Dr Ali Jawarneh Deparmen of Mechanical Engineering Hashemie Universiy 1 Ouline Rae of Flow Conrol volume approach. Conservaion of mass he coninuiy

More information

NEWTON S SECOND LAW OF MOTION

NEWTON 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 information

Q2.1 This is the x t graph of the motion of a particle. Of the four points P, Q, R, and S, the velocity v x is greatest (most positive) at

Q2.1 This is the x t graph of the motion of a particle. Of the four points P, Q, R, and S, the velocity v x is greatest (most positive) at Q2.1 This is he x graph of he moion of a paricle. Of he four poins P, Q, R, and S, he velociy is greaes (mos posiive) a A. poin P. B. poin Q. C. poin R. D. poin S. E. no enough informaion in he graph o

More information

Numerical Modeling of the Effect of Fine Water Mist on the Small Scale Flame Spreading Over Solid Combustibles

Numerical 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 information

Mesoscale Meteorology: Supercell Dynamics 25, 27 April 2017 Overview Supercell thunderstorms are long-lived single-cell thunderstorms, with

Mesoscale 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 information

A B C D September 25 Exam I Physics 105. Circle the letter of the single best answer. Each question is worth 1 point

A B C D September 25 Exam I Physics 105. Circle the letter of the single best answer. Each question is worth 1 point 2012 Sepember 25 Eam I Physics 105 Circle he leer of he single bes answer. Each uesion is worh 1 poin Physical Consans: Earh s free-fall acceleraion = g = 9.80 m/s 2 3. (Mark wo leers!) The below graph

More information

Heat and Mass Transfer on the Unsteady MHD Flow of Chemically Reacting Micropolar Fluid with Radiation and Joule Heating

Heat 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 information

A numerical solution of the NS equations based on the mean value theorem with applications to aerothermodynamics

A 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 information

One-Dimensional Kinematics

One-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 information

The Pressure Perturbation Equation: Exposed!

The 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 information

2.1: What is physics? Ch02: Motion along a straight line. 2.2: Motion. 2.3: Position, Displacement, Distance

2.1: What is physics? Ch02: Motion along a straight line. 2.2: Motion. 2.3: Position, Displacement, Distance Ch: Moion along a sraigh line Moion Posiion and Displacemen Average Velociy and Average Speed Insananeous Velociy and Speed Acceleraion Consan Acceleraion: A Special Case Anoher Look a Consan Acceleraion

More information

Rectilinear Kinematics

Rectilinear Kinematics Recilinear Kinemaic Coninuou Moion Sir Iaac Newon Leonard Euler Oeriew Kinemaic Coninuou Moion Erraic Moion Michael Schumacher. 7-ime Formula 1 World Champion Kinemaic The objecie of kinemaic i o characerize

More information

Phys 221 Fall Chapter 2. Motion in One Dimension. 2014, 2005 A. Dzyubenko Brooks/Cole

Phys 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 information

SMS-618, Particle Dynamics, Fall 2003 (E. Boss, last updated: 10/8/2003) Conservation equations in fluids

SMS-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 information

PH2130 Mathematical Methods Lab 3. z x

PH2130 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 information

Ch1: Introduction and Review

Ch1: Introduction and Review //6 Ch: Inroducion and Review. Soli and flui; Coninuum hypohesis; Transpor phenomena (i) Solid vs. Fluid No exernal force : An elemen of solid has a preferred shape; fluid does no. Under he acion of a

More information

Physics 221 Fall 2008 Homework #2 Solutions Ch. 2 Due Tues, Sept 9, 2008

Physics 221 Fall 2008 Homework #2 Solutions Ch. 2 Due Tues, Sept 9, 2008 Physics 221 Fall 28 Homework #2 Soluions Ch. 2 Due Tues, Sep 9, 28 2.1 A paricle moving along he x-axis moves direcly from posiion x =. m a ime =. s o posiion x = 1. m by ime = 1. s, and hen moves direcly

More information

International Journal of Pure and Applied Sciences and Technology

International 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 information

Vector Calculus. Chapter 2

Vector Calculus. Chapter 2 Chaper Vecor Calculus. Elemenar. Vecor Produc. Differeniaion of Vecors 4. Inegraion of Vecors 5. Del Operaor or Nabla (Smbol 6. Polar Coordinaes Chaper Coninued 7. Line Inegral 8. Volume Inegral 9. Surface

More information

1. The graph below shows the variation with time t of the acceleration a of an object from t = 0 to t = T. a

1. The graph below shows the variation with time t of the acceleration a of an object from t = 0 to t = T. a Kinemaics Paper 1 1. The graph below shows he ariaion wih ime of he acceleraion a of an objec from = o = T. a T The shaded area under he graph represens change in A. displacemen. B. elociy. C. momenum.

More information

Plasma Astrophysics Chapter 3: Kinetic Theory. Yosuke Mizuno Institute of Astronomy National Tsing-Hua University

Plasma 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 information

6.2 The Moment-Curvature Equations

6.2 The Moment-Curvature Equations Secio 6. 6. The ome-crare Eqaios 6.. From Beam Theor o Plae Theor I he beam heor based o he assmpios of plae secios remaiig plae ad ha oe ca eglec he raserse srai he srai aries liearl hrogh he hickess.

More information

Chapters 2 Kinematics. Position, Distance, Displacement

Chapters 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 information

Chapter 3 Kinematics in Two Dimensions

Chapter 3 Kinematics in Two Dimensions Chaper 3 KINEMATICS IN TWO DIMENSIONS PREVIEW Two-dimensional moion includes objecs which are moing in wo direcions a he same ime, such as a projecile, which has boh horizonal and erical moion. These wo

More information

AP CALCULUS AB 2003 SCORING GUIDELINES (Form B)

AP CALCULUS AB 2003 SCORING GUIDELINES (Form B) SCING GUIDELINES (Form B) Quesion 4 A paricle moves along he x-axis wih velociy a ime given by v( ) = 1 + e1. (a) Find he acceleraion of he paricle a ime =. (b) Is he speed of he paricle increasing a ime

More information

Lecture 5. Differential Analysis of Fluid Flow Navier-Stockes equation

Lecture 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 information

(π 3)k. f(t) = 1 π 3 sin(t)

(π 3)k. f(t) = 1 π 3 sin(t) Mah 6 Fall 6 Dr. Lil Yen Tes Show all our work Name: Score: /6 No Calculaor permied in his par. Read he quesions carefull. Show all our work and clearl indicae our final answer. Use proper noaion. Problem

More information

INSTANTANEOUS VELOCITY

INSTANTANEOUS 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 information

Work Power Energy. For conservaive orce ) Work done is independen o he pah ) Work done in a closed loop is zero ) Work done agains conservaive orce is sored is he orm o poenial energy 4) All he above.

More information

Chapter 6 Differential Analysis of Fluid Flow

Chapter 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 information

THE DARBOUX TRIHEDRONS OF REGULAR CURVES ON A REGULAR TIME-LIKE SURFACE. Emin Özyilmaz

THE 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 information

Midterm Exam Review Questions Free Response Non Calculator

Midterm Exam Review Questions Free Response Non Calculator Name: Dae: Block: Miderm Eam Review Quesions Free Response Non Calculaor Direcions: Solve each of he following problems. Choose he BEST answer choice from hose given. A calculaor may no be used. Do no

More information

Learning from a Golf Ball

Learning 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 information

0.1 MAXIMUM LIKELIHOOD ESTIMATION EXPLAINED

0.1 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 information

3.3 Internal Stress. Cauchy s Concept of Stress

3.3 Internal Stress. Cauchy s Concept of Stress INTERNL TRE 3.3 Inernal ress The idea of sress considered in 3.1 is no difficul o concepualise since objecs ineracing wih oher objecs are encounered all around us. more difficul concep is he idea of forces

More information

Homework 2: Kinematics and Dynamics of Particles Due Friday Feb 8, 2019

Homework 2: Kinematics and Dynamics of Particles Due Friday Feb 8, 2019 EN4: Dynamics and Vibraions Homework : Kinemaics and Dynamics of Paricles Due Friday Feb 8, 19 School of Engineering Brown Universiy 1. Sraigh Line Moion wih consan acceleraion. Virgin Hyperloop One is

More information

Section 2.2 Charge and Current 2.6 b) The current direction is designated as the direction of the movement of positive charges.

Section 2.2 Charge and Current 2.6 b) The current direction is designated as the direction of the movement of positive charges. Chaper Soluions Secion. Inroducion. Curren source. Volage source. esisor.4 Capacior.5 Inducor Secion. Charge and Curren.6 b) The curren direcion is designaed as he direcion of he movemen of posiive charges..7

More information

THERMOPHORESIS PARTICLE DEPOSITION ON FLAT SURFACES DUE TO FLUID FLOW IN DARCY-FORCHHEIMER POROUS MEDIUM

THERMOPHORESIS 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 information

Q2.4 Average velocity equals instantaneous velocity when the speed is constant and motion is in a straight line.

Q2.4 Average velocity equals instantaneous velocity when the speed is constant and motion is in a straight line. CHAPTER MOTION ALONG A STRAIGHT LINE Discussion Quesions Q. The speedomeer measures he magniude of he insananeous eloci, he speed. I does no measure eloci because i does no measure direcion. Q. Graph (d).

More information

Physics Unit Workbook Two Dimensional Kinematics

Physics 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 information

Flow-Induced Vibration Analysis of Supported Pipes with a Crack

Flow-Induced Vibration Analysis of Supported Pipes with a Crack Flow-Induced Vibraion Analsis of Suppored Pipes wih a Crack Jin-Huk Lee, Samer Masoud Al-Said Deparmen of Mechanical Engineering American Universi of Sharjah, UAE Ouline Inroducion and Moivaion Aeroacousicall

More information

Welcome Back to Physics 215!

Welcome Back to Physics 215! Welcome Back o Physics 215! (General Physics I) Thurs. Jan 19 h, 2017 Lecure01-2 1 Las ime: Syllabus Unis and dimensional analysis Today: Displacemen, velociy, acceleraion graphs Nex ime: More acceleraion

More information

Dynamics of the Atmosphere 11:670:324. Class Time: Tuesdays and Fridays 9:15-10:35

Dynamics of the Atmosphere 11:670:324. Class Time: Tuesdays and Fridays 9:15-10:35 Dnamics o the Atmosphere 11:67:34 Class Time: Tesdas and Fridas 9:15-1:35 Instrctors: Dr. Anthon J. Broccoli (ENR 9) broccoli@ensci.rtgers.ed 73-93-98 6 Dr. Benjamin Lintner (ENR 5) lintner@ensci.rtgers.ed

More information

Finite Strain Consolidation Numerical Methods in Geotechnical Engineering. Murray Fredlund June 7, 1995

Finite 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 information

2. VECTORS. R Vectors are denoted by bold-face characters such as R, V, etc. The magnitude of a vector, such as R, is denoted as R, R, V

2. VECTORS. R Vectors are denoted by bold-face characters such as R, V, etc. The magnitude of a vector, such as R, is denoted as R, R, V ME 352 VETS 2. VETS Vecor algebra form he mahemaical foundaion for kinemaic and dnamic. Geomer of moion i a he hear of boh he kinemaic and dnamic of mechanical em. Vecor anali i he imehonored ool for decribing

More information

Today in Physics 218: radiation reaction

Today in Physics 218: radiation reaction Today in Physics 18: radiaion reacion Radiaion reacion The Abraham-Lorenz formula; radiaion reacion force The pah of he elecron in oday s firs example (radial decay grealy exaggeraed) 6 March 004 Physics

More information

Q2. The velocity field in a fluid flow is given by

Q2. The velocity field in a fluid flow is given by Kinematics of Flid Q. Choose the correct anser (i) streamline is a line (a) hich is along the path of a particle (b) dran normal to the elocit ector at an point (c) sch that the streamlines diide the passage

More information

Department of Chemical Engineering University of Tennessee Prof. David Keffer. Course Lecture Notes SIXTEEN

Department 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 information

Maxwell s Equations and Electromagnetic Waves

Maxwell 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 information

4.5 Constant Acceleration

4.5 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 information

SOLVING AN OPTIMAL CONTROL PROBLEM WITH MATLAB

SOLVING 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 information