PERIPHERAL SURFACE PROFILING OF THE HOB CUTTER FOR SCREW COMPRESSOR ROTORS COMPONENTS II. MALE ROTOR
|
|
- Charleen Atkinson
- 5 years ago
- Views:
Transcription
1 U.P.B. Sci. Bull., Series D, Vol. 75, Iss., ISS PERIPHERAL SURFACE PROFILIG OF THE HOB CUTTER FOR SCREW COMPRESSOR ROTORS COMPOETS II. MALE ROTOR Camelia POPA, icolae OACEA Profilarea suprafeţei periferice a sculei melc reciproc înfǎşurǎoare cu suprafeţele elicoidale ale flancurilor rooarelor compresorului elicoidal, consiuie o problemǎ de generare de speţa a II-a (referioare la suprafeţele reciproc înfǎşurǎoare cu conac punciform). În lucrare, pe baa eoremelor referioare la descompunerea unei mişcǎri elicoidale, se propune o meodǎ de profilare a suprafeţei periferice primare a sculei melc generaoare a roorului conducǎor din componenţa compresorului elicoidal. Sun preenae formele consrucive ale lobilor roorului conducǎor, forma cremalierei generaoare şi forma profilului aial al sculei melc, reciproc înfǎşurǎoare aceseia. De asemenea, pe baa unui produs sof dedica, se preinǎ eemple numerice ale formelor aiale ale sculelor melc generaoare penru roorul conducǎor penru un compresor cu rapor de ransmiere 4/6, respeciv /5. Peripheral surface profiling of he hob cuer represens a second degree generaion problem referring o poin conac surfaces. In his paper, according o heorems referring o he decomposiion of a helical moion, we propose a surface profiling mehod of he peripheral surface of he hob cuer for he male roor, screw compressor componen. The consrucive form of he male roor lobes, he shape of he generaing rack and he shape of he aial profile of he hob cuer are presened. Also, we presen fronal applicaions of he aial shapes of he hob cuer generaing for he male roor, screw compressor componen, gear raio 4/6, and /5 respecively. Keywords: helical surfaces, hob cuer, meshing surfaces. Inroducion Mehods of profiling ool drives, envelope a vore of surfaces associaed wih a couple in rolling aodes, are: Oliver II heorem, for enveloping surfaces wih conac poin, and Gohman heorem, hrough he inermediae surface; helical movemen decomposiion mehod, icolaev [],[],[4],[6],[8]. We also proposed D and D graphic soluions in order o solve hese problems [7], [9]. Assis, Deparmen of Machine Elemens and Graphics, Dunărea de Jos Universiy of Galai, Galai, Romania, lpopa@ugal.ro Prof., Deparmen of Manufacuring, Roboics and Welding Engineering,, Dunărea de Jos Universiy of Galai, Galai, Romania, noancea@ugal.ro
2 Camelia Popa, icolae Oancea Using Béier polynomials, surface represenaion is possible o be done, precisely enough. This is he soluion for he helical surfaces of screw compressor roors, male and female.. Coordinaes sysems; generaion moion In Fig., i is represened he aes sysem, and he absolue movemens of he reference sysems associaed o hese aes. The reference sysems are he following: - y is he global sysem wih ais, ais of roaion of he ais associaed o he generaing surfaces roller; - y he global sysem, wih ais y superposed o he primary peripheral surface ais of he hob cuer; - X Y Z he relaive sysem aached o he ais of he aode, A ; - ξζ he relaive sysem aached o he ais of he rack generaing (fla surface superposed o he plane ζ), A ; - X S Y S Z S he relaive sysem associaed o he peripheral surface of he hob cuer. Fig.. Coordinaes sysems; generaion moions The kinemaics of he generaion process is known as follow: roaion of he aode A (radius R rp ), ϕ angular moion parameer,
3 Peripheral surface profiling [...] for screw compressor roors componens; II.Male roor ( φ ) T = ω X. () displacemen of he aode A - l moion parameer, = ξ - a, R r p a = ; () roaion of he sysem X S Y S Z S around he ais Y, wih φ angular moion parameer, T ( φ ) =ω X S. () The following condiions are known: condiion of rolling of he aodes A and A, = Rr φ p ; (4) dependence generaed by he shape of he peripheral surface of he hob cuer (consan seep parallel-ype heli, wih p helical parameer), = pφcosω ; (5) ransformaion beween fied coordinaes sysems, A y = cosω sinω y, (6) sinω cosω where A is he disance beween he aes, respecively, of aode A and of he helical surface V. The relaive moion of he sysem aached o he aode A, of he generaing surface XYZ, compared wih he reference sysem associaed o he rack generaing space ξζ, is given by he ransformaion: ξ = ω T ( φ ) X - a. (7) The curren poin on he generaing surface, as a cylindrical helical surface is: X ( ) = X u ; Σ Y = Y ( u) ; (8) Z = p υ, for u discree variable known hrough a reduced number of values ( or 4 poins); υ angular roaion parameer around he ais Z ; p helical parameer of he conducive roor.
4 Camelia Popa, icolae Oancea. Mehod of definiion for he shape of he generaing rack surface According o (7) and (8) we define: ξ cosφ ( ) R sinφ X u rp = sinφ cosφ Y ( u) Rr φ p. (9) ζ pυ The enveloping condiion is ' ' [ X X ( u) ] X [ Y Y ( u) ] - u - Yu =, () where: X = Rr cos φ ; p Y = Rr sin φ. p () Equaion () represens condiion of normal [] (R rp is he radius of he cylindrical aode A, (Fig. )). Fig.. Surface Σ, generaing surface known hrough 4 poins : A[X A,X A ], B[X B,X B ],C[X C,X C ], D[X D,X D ] We can accep ha, he direcri of he surface represening he cylindrical flank of he generaing rack, (equaions () (8)), can be subsiued by a Béier polynomial, given by he following equaions : ξ = Aξ ( ) Bξ ( ) Cξ ( ) Dξ ; I : () = A ( ) B ( ) C ( ) D. All he poins which deermine he direcri of he cylindrical surface (he flank of he blank) is given by: A[ A, y A ], B[ B, y B ], C[ C, y C ], D[ D,y D ], ( Fig. ).
5 Peripheral surface profiling [...] for screw compressor roors componens; II.Male roor 4. Peripheral surface profiling mehod for he hob cuer Knowing he surface of he generaing rack flank (in approimae shape, as Béier polynomial), we propose o deermine he characerisic (conac curve) using he mehod of decomposiion of he helical moion [5], (Fig. ). The helical movemen of peripheral surface of he hob cuer, (V, p) decomposes ino a sum of equivalen movemens: a ranslaion, upon he uni vecor of he generari of cylindrical surface of he flank rack and he roaion of he ais A. The disance: π a = p an ω, () represens he disance o he helical surface ais, V, ( Fig. ). Fig.. Helical movemen decomposiion mehod; coordinaes sysems The condiion o deermine he characerisic curve is provided as follows:. (4) The normal vecor o he cylindrical surface I, is always normal o is own generari; characerisic curve depends only on he roaion around he ais A. Therefore, he characerisic curve, during he helical movemen of ais V and he parameer p, is defined as he projecion ais A on he surface I.
6 4 Camelia Popa, icolae Oancea We define, see Fig. : - he ais A, in he y sysem, k sin j cos A ω ω =, (5) - he normal on he surface I, k j i j I =, (6) or : = k j y i k j y i I, (7) (see formula () flank surface of he ool-rack); - he vecor r i O O r i =, (8) where, r is he vecor of he cylindrical surface I. According (), he coordinae ransformaion y, d d r R y p β β ζ ξ cos sin =, (9) leads o he epression of surface shape of he rack I in he sysem y : ( ) ( ) ( ) ( ) ( ) ( ) = = =. cos ; sin ; d d r D C B A y R D C B A p β β ξ ξ ξ ξ () The sie of he parameer ω is, see Fig. 4: β d ω s ω =, () where: -ω s is he angle of hob cuer ais, in relaion o he fron plane of he male roor (righ screw); -β d - angle of he male roor heli, cylinder radius R rp ; -ω - il angle of he heli of hob cuer, wih he radius R rs, = lobs r r s cos R R arcsin ω s p β. ()
7 Peripheral surface profiling [...] for screw compressor roors componens; II.Male roor 5 Fig.4. Til ais of hob cuer The enveloping condiion is: ( A, I, r i ) =. () or, y ( ) ( ), a y, cos β d =. (4) cosω sinω The condiion (4) is a funcion of parameers and : q (, ) =, (5) where,. The equaions () and (5) are a locus surface I. The values of he parameers l and fulfilling (5), replaced in Béier form for rack flanks, deermine he mari: T C I = y, (6) i i i represening he coordinaes of he characerisic curve C I. Helical movemen (V,p) of he curve C I, generaes peripheral surface of he hob cuer. The coordinae ransformaion, see Fig. 4,
8 6 Camelia Popa, icolae Oancea X Y Z S S S = [ R R ] i r p i rs cosω sinω y, (7) i sinω cosω i=,...,n so ha, he helical movemen of (V,p) of he characerisic C I, becomes: X S = X [ ] S, y, φ ; i i i [, y, φ ]; Π YS = YS i i i= n. (8) i Z = Z [, y, φ ], S S i i i and represens he primary peripheral surface of he hob cuer - surface Π. Giving he surface Π he condiion Z S =, (9) he aial secion Π A is obained in he form: X [ ] S = X S, y,,φ ; i i i Π i= n, () Y = Y [, y,,φ ], S S i i i he variable [ φ ] represening he sie of he parameer corresponding o he aial secion, see (9). 5. umerical applicaions The profile of generaing rack of male roor (see also Fig. 5) has he following profile porions. ٠Firs applicaion (screw compressor, raio 4/6) Table The consrucive daes of he reference rack, version I ( Fig. 5) R r u ma ψ ma [ ] υ ma [ ] υ ma [ ] u ma L p Rr c Fig.5.Rack generaing profile
9 Peripheral surface profiling [...] for screw compressor roors componens; II.Male roor 7 Table and Fig. 6 describe numerically he aial secion coordinaes of he primary peripheral surface of he hob cuer. Table Aial secion of he primary peripheral surface of he hob cuer X S Y S X S Y S Fig. 6. The aial secion profile of he hob cuer Fig. 7. The relaive posiion beween he hob cuer and he male roor
10 8 Camelia Popa, icolae Oancea The Fig.7, represens he relaive posiion beween he hob cuer and he male roor. ٠Second applicaion (screw compressor, raio /5) Table The consrucive daes of he generaing rack ( Fig. ) R r u ma ψ ma [ ] υ ma [ ] υ ma [ ] u ma L p c Rr In Table 4, he aial secion coordinaes of he hob cuer peripheral surface are described. Table 4 The aial secion of he hob cuer s primary peripheral surface X Y X Y Fig. 9. The shape of he aial secion for he male hob cuer
11 Peripheral surface profiling [...] for screw compressor roors componens; II.Male roor 9 In Fig. 9 is represened he aial secion shape of he hob cuer for he main roor. In Fig. is represened, in D modeling, he relaive posiion beween he hob cuer and he male roor. Fig.. The relaive posiion beween he hob cuer and he male roor 6. Conclusions. The helical surfaces ha edges he screw compressors componen roors, are comple surfaces (cylindrical helical surfaces and consan sep). Generaing his ype of surfaces is done wih a specific rack, whose ransverse profile is deermined from echnological and funcional consideraions in order o obain an opimum yield.. The male roor generaors can be epressed by simple analyical forms, or approimaion of Béier polynomials.. The hob cuer profiles are generaed according o he composiion and decomposiion of he helical moion, using he inermediae surfaces mehod. The mehods D of he ools primary peripheral surfaces were also represened. B I B L I O G R A P H Y [] Livin, F. L., 989, Theory of Gearing, ASA RP- (AVSCOM 88-C-5), Washingon, D.C.; [] Houson, R., Mavripilis, D., Oswald, F., Liu, Y.S., 994, A basis for solid modeling of gear eeh whih applicaion in design manufacure, Mech. Mach. Theory 9 (5):7-7; [] Oancea,., 4, Mehode numérique pour l éude des surfaces enveloppes, Mech. Mach. Theory (7): ; [4] Radevich, S.P., 8, «Kinemaic geomery of surface machining, CRC, Boca Raon, ISB ;
12 4 Camelia Popa, icolae Oancea [5] Teodor, V.,, Conribuion o he elaboraion of a mehod for profiling ools-ools which generae by enwrapping, Lamber Academic Publishing, ISB ; [6] Rodin, R., P., 99, Osnovy proekirovania rehushich insrumenov (Basics of desing of cuing ools) Vishcha Shkola, Kiev;(in Russian) [7] Veliko, I.,Gencho,., 998, Profiling of roaion ools for forming of helical surfaces, In.J. Mach Tools; manuf.8:5-48; [8] Liukshin, V., S.,968, Teoria vinovih poverhnosei, Mashinosroenie, Moskva; [9] Baicu, I., Oancea,., Profilarea sculelor prin modelare solida ( Profiling of ools using solid modelling) Ediura TEHICA-IFO,Chişinǎu,, ISB X. (in Romanian)
The motions of the celt on a horizontal plane with viscous friction
The h Join Inernaional Conference on Mulibody Sysem Dynamics June 8, 18, Lisboa, Porugal The moions of he cel on a horizonal plane wih viscous fricion Maria A. Munisyna 1 1 Moscow Insiue of Physics and
More informationBasilio Bona ROBOTICA 03CFIOR 1
Indusrial Robos Kinemaics 1 Kinemaics and kinemaic funcions Kinemaics deals wih he sudy of four funcions (called kinemaic funcions or KFs) ha mahemaically ransform join variables ino caresian variables
More informationKinematics and kinematic functions
Kinemaics and kinemaic funcions Kinemaics deals wih he sudy of four funcions (called kinemaic funcions or KFs) ha mahemaically ransform join variables ino caresian variables and vice versa Direc Posiion
More informationWeek 1 Lecture 2 Problems 2, 5. What if something oscillates with no obvious spring? What is ω? (problem set problem)
Week 1 Lecure Problems, 5 Wha if somehing oscillaes wih no obvious spring? Wha is ω? (problem se problem) Sar wih Try and ge o SHM form E. Full beer can in lake, oscillaing F = m & = ge rearrange: F =
More informationECE 2100 Circuit Analysis
ECE 1 Circui Analysis Lesson 35 Chaper 8: Second Order Circuis Daniel M. Liynski, Ph.D. ECE 1 Circui Analysis Lesson 3-34 Chaper 7: Firs Order Circuis (Naural response RC & RL circuis, Singulariy funcions,
More informationStructural Dynamics and Earthquake Engineering
Srucural Dynamics and Earhquae Engineering Course 1 Inroducion. Single degree of freedom sysems: Equaions of moion, problem saemen, soluion mehods. Course noes are available for download a hp://www.c.up.ro/users/aurelsraan/
More informationSome Basic Information about M-S-D Systems
Some Basic Informaion abou M-S-D Sysems 1 Inroducion We wan o give some summary of he facs concerning unforced (homogeneous) and forced (non-homogeneous) models for linear oscillaors governed by second-order,
More informationAn Introduction to Malliavin calculus and its applications
An Inroducion o Malliavin calculus and is applicaions Lecure 5: Smoohness of he densiy and Hörmander s heorem David Nualar Deparmen of Mahemaics Kansas Universiy Universiy of Wyoming Summer School 214
More informationDifferential Equations
Mah 21 (Fall 29) Differenial Equaions Soluion #3 1. Find he paricular soluion of he following differenial equaion by variaion of parameer (a) y + y = csc (b) 2 y + y y = ln, > Soluion: (a) The corresponding
More informationSolutions from Chapter 9.1 and 9.2
Soluions from Chaper 9 and 92 Secion 9 Problem # This basically boils down o an exercise in he chain rule from calculus We are looking for soluions of he form: u( x) = f( k x c) where k x R 3 and k is
More informationKinematics and kinematic functions
ROBOTICS 01PEEQW Basilio Bona DAUIN Poliecnico di Torino Kinemaic funcions Kinemaics and kinemaic funcions Kinemaics deals wih he sudy of four funcions(called kinemaic funcions or KFs) ha mahemaically
More informationNew effective moduli of isotropic viscoelastic composites. Part I. Theoretical justification
IOP Conference Series: Maerials Science and Engineering PAPE OPEN ACCESS New effecive moduli of isoropic viscoelasic composies. Par I. Theoreical jusificaion To cie his aricle: A A Sveashkov and A A akurov
More information3.1.3 INTRODUCTION TO DYNAMIC OPTIMIZATION: DISCRETE TIME PROBLEMS. A. The Hamiltonian and First-Order Conditions in a Finite Time Horizon
3..3 INRODUCION O DYNAMIC OPIMIZAION: DISCREE IME PROBLEMS A. he Hamilonian and Firs-Order Condiions in a Finie ime Horizon Define a new funcion, he Hamilonian funcion, H. H he change in he oal value of
More informationKinematics Vocabulary. Kinematics and One Dimensional Motion. Position. Coordinate System in One Dimension. Kinema means movement 8.
Kinemaics Vocabulary Kinemaics and One Dimensional Moion 8.1 WD1 Kinema means movemen Mahemaical descripion of moion Posiion Time Inerval Displacemen Velociy; absolue value: speed Acceleraion Averages
More informationLet us start with a two dimensional case. We consider a vector ( x,
Roaion marices We consider now roaion marices in wo and hree dimensions. We sar wih wo dimensions since wo dimensions are easier han hree o undersand, and one dimension is a lile oo simple. However, our
More informationSolutions for homework 12
y Soluions for homework Secion Nonlinear sysems: The linearizaion of a nonlinear sysem Consider he sysem y y y y y (i) Skech he nullclines Use a disincive marking for each nullcline so hey can be disinguished
More informationOptimal Path Planning for Flexible Redundant Robot Manipulators
25 WSEAS In. Conf. on DYNAMICAL SYSEMS and CONROL, Venice, Ialy, November 2-4, 25 (pp363-368) Opimal Pah Planning for Flexible Redundan Robo Manipulaors H. HOMAEI, M. KESHMIRI Deparmen of Mechanical Engineering
More informationProgram: RFEM 5, RSTAB 8, RF-DYNAM Pro, DYNAM Pro. Category: Isotropic Linear Elasticity, Dynamics, Member
Verificaion Example Program: RFEM 5, RSTAB 8, RF-DYNAM Pro, DYNAM Pro Caegory: Isoropic Linear Elasiciy, Dynamics, Member Verificaion Example: 0104 Canilever Beam wih Periodic Exciaion 0104 Canilever Beam
More informationSolution: b All the terms must have the dimension of acceleration. We see that, indeed, each term has the units of acceleration
PHYS 54 Tes Pracice Soluions Spring 8 Q: [4] Knowing ha in he ne epression a is acceleraion, v is speed, is posiion and is ime, from a dimensional v poin of view, he equaion a is a) incorrec b) correc
More informationTraveling Waves. Chapter Introduction
Chaper 4 Traveling Waves 4.1 Inroducion To dae, we have considered oscillaions, i.e., periodic, ofen harmonic, variaions of a physical characerisic of a sysem. The sysem a one ime is indisinguishable from
More informationImproved Approximate Solutions for Nonlinear Evolutions Equations in Mathematical Physics Using the Reduced Differential Transform Method
Journal of Applied Mahemaics & Bioinformaics, vol., no., 01, 1-14 ISSN: 179-660 (prin), 179-699 (online) Scienpress Ld, 01 Improved Approimae Soluions for Nonlinear Evoluions Equaions in Mahemaical Physics
More informationLecture 2-1 Kinematics in One Dimension Displacement, Velocity and Acceleration Everything in the world is moving. Nothing stays still.
Lecure - Kinemaics in One Dimension Displacemen, Velociy and Acceleraion Everyhing in he world is moving. Nohing says sill. Moion occurs a all scales of he universe, saring from he moion of elecrons in
More informationCOMPLEMENTARY THEOREMS OF SURFACE ENWRAPPING EXPRESSED IN GRAPHICAL FORM
, TECHNOLOGIES IN MACHINE BUILDING, ISSN 1221-4566, 2014 COMPLEMENTARY THEOREMS OF SURFACE ENWRAPPING EXPRESSED IN GRAPHICAL FORM Virgil TEODOR 1, Silviu BERBINSCHI 2, Ioan BAICU 2, Nicuşor BAROIU 1, Nicolae
More informationLecture 10: Wave equation, solution by spherical means
Lecure : Wave equaion, soluion by spherical means Physical modeling eample: Elasodynamics u (; ) displacemen vecor in elasic body occupying a domain U R n, U, The posiion of he maerial poin siing a U in
More informationECE 2100 Circuit Analysis
ECE 1 Circui Analysis Lesson 37 Chaper 8: Second Order Circuis Discuss Exam Daniel M. Liynski, Ph.D. Exam CH 1-4: On Exam 1; Basis for work CH 5: Operaional Amplifiers CH 6: Capaciors and Inducor CH 7-8:
More informationPosition, Velocity, and Acceleration
rev 06/2017 Posiion, Velociy, and Acceleraion Equipmen Qy Equipmen Par Number 1 Dynamic Track ME-9493 1 Car ME-9454 1 Fan Accessory ME-9491 1 Moion Sensor II CI-6742A 1 Track Barrier Purpose The purpose
More information2.1: 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 informationTrajectory planning in Cartesian space
Roboics 1 Trajecory planning in Caresian space Prof. Alessandro De Luca Roboics 1 1 Trajecories in Caresian space in general, he rajecory planning mehods proposed in he join space can be applied also in
More informationRobotics I. April 11, The kinematics of a 3R spatial robot is specified by the Denavit-Hartenberg parameters in Tab. 1.
Roboics I April 11, 017 Exercise 1 he kinemaics of a 3R spaial robo is specified by he Denavi-Harenberg parameers in ab 1 i α i d i a i θ i 1 π/ L 1 0 1 0 0 L 3 0 0 L 3 3 able 1: able of DH parameers of
More informationDistance Between Two Ellipses in 3D
Disance Beween Two Ellipses in 3D David Eberly Magic Sofware 6006 Meadow Run Cour Chapel Hill, NC 27516 eberly@magic-sofware.com 1 Inroducion An ellipse in 3D is represened by a cener C, uni lengh axes
More informationThis is an example to show you how SMath can calculate the movement of kinematic mechanisms.
Dec :5:6 - Kinemaics model of Simple Arm.sm This file is provided for educaional purposes as guidance for he use of he sofware ool. I is no guaraeed o be free from errors or ommissions. The mehods and
More informationFrom Particles to Rigid Bodies
Rigid Body Dynamics From Paricles o Rigid Bodies Paricles No roaions Linear velociy v only Rigid bodies Body roaions Linear velociy v Angular velociy ω Rigid Bodies Rigid bodies have boh a posiion and
More informationThe Paradox of Twins Described in a Three-dimensional Space-time Frame
The Paradox of Twins Described in a Three-dimensional Space-ime Frame Tower Chen E_mail: chen@uguam.uog.edu Division of Mahemaical Sciences Universiy of Guam, USA Zeon Chen E_mail: zeon_chen@yahoo.com
More informationDirectional Tubular Surfaces
Inernaional Journal of Algebra, Vol. 9, 015, no. 1, 57-535 HIKARI Ld, www.m-hikari.com hp://dx.doi.org/10.1988/ija.015.5174 Direcional Tubular Surfaces Musafa Dede Deparmen of Mahemaics, Faculy of Ars
More informationWEEK-3 Recitation PHYS 131. of the projectile s velocity remains constant throughout the motion, since the acceleration a x
WEEK-3 Reciaion PHYS 131 Ch. 3: FOC 1, 3, 4, 6, 14. Problems 9, 37, 41 & 71 and Ch. 4: FOC 1, 3, 5, 8. Problems 3, 5 & 16. Feb 8, 018 Ch. 3: FOC 1, 3, 4, 6, 14. 1. (a) The horizonal componen of he projecile
More informationVoltage/current relationship Stored Energy. RL / RC circuits Steady State / Transient response Natural / Step response
Review Capaciors/Inducors Volage/curren relaionship Sored Energy s Order Circuis RL / RC circuis Seady Sae / Transien response Naural / Sep response EE4 Summer 5: Lecure 5 Insrucor: Ocavian Florescu Lecure
More information3, so θ = arccos
Mahemaics 210 Professor Alan H Sein Monday, Ocober 1, 2007 SOLUTIONS This problem se is worh 50 poins 1 Find he angle beween he vecors (2, 7, 3) and (5, 2, 4) Soluion: Le θ be he angle (2, 7, 3) (5, 2,
More informationRoller-Coaster Coordinate System
Winer 200 MECH 220: Mechanics 2 Roller-Coaser Coordinae Sysem Imagine you are riding on a roller-coaer in which he rack goes up and down, wiss and urns. Your velociy and acceleraion will change (quie abruply),
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 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 informationAn Invariance for (2+1)-Extension of Burgers Equation and Formulae to Obtain Solutions of KP Equation
Commun Theor Phys Beijing, China 43 2005 pp 591 596 c Inernaional Academic Publishers Vol 43, No 4, April 15, 2005 An Invariance for 2+1-Eension of Burgers Equaion Formulae o Obain Soluions of KP Equaion
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 informationSUFFICIENT CONDITIONS FOR EXISTENCE SOLUTION OF LINEAR TWO-POINT BOUNDARY PROBLEM IN MINIMIZATION OF QUADRATIC FUNCTIONAL
HE PUBLISHING HOUSE PROCEEDINGS OF HE ROMANIAN ACADEMY, Series A, OF HE ROMANIAN ACADEMY Volume, Number 4/200, pp 287 293 SUFFICIEN CONDIIONS FOR EXISENCE SOLUION OF LINEAR WO-POIN BOUNDARY PROBLEM IN
More informationWall. x(t) f(t) x(t = 0) = x 0, t=0. which describes the motion of the mass in absence of any external forcing.
MECHANICS APPLICATIONS OF SECOND-ORDER ODES 7 Mechanics applicaions of second-order ODEs Second-order linear ODEs wih consan coefficiens arise in many physical applicaions. One physical sysems whose behaviour
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 informationMath Week 14 April 16-20: sections first order systems of linear differential equations; 7.4 mass-spring systems.
Mah 2250-004 Week 4 April 6-20 secions 7.-7.3 firs order sysems of linear differenial equaions; 7.4 mass-spring sysems. Mon Apr 6 7.-7.2 Sysems of differenial equaions (7.), and he vecor Calculus we need
More informationCh.1. Group Work Units. Continuum Mechanics Course (MMC) - ETSECCPB - UPC
Ch.. Group Work Unis Coninuum Mechanics Course (MMC) - ETSECCPB - UPC Uni 2 Jusify wheher he following saemens are rue or false: a) Two sreamlines, corresponding o a same insan of ime, can never inersec
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 informationSignals and Systems Profs. Byron Yu and Pulkit Grover Fall Midterm 1 Solutions
8-90 Signals and Sysems Profs. Byron Yu and Pulki Grover Fall 07 Miderm Soluions Name: Andrew ID: Problem Score Max 0 8 4 6 5 0 6 0 7 8 9 0 6 Toal 00 Miderm Soluions. (0 poins) Deermine wheher he following
More informationMotion along a Straight Line
chaper 2 Moion along a Sraigh Line verage speed and average velociy (Secion 2.2) 1. Velociy versus speed Cone in he ebook: fer Eample 2. Insananeous velociy and insananeous acceleraion (Secions 2.3, 2.4)
More informationMATHEMATICAL MODELING OF THE TRACTOR-GRADER AGRICULTURAL SYSTEM CINEMATIC DURING LAND IMPROVING WORKS
Bullein of he Transilvania Universiy of Braşov Series II: Foresry Wood Indusry Agriculural Food Engineering Vol. 5 (54) No. 1-2012 MATHEMATICA MODEING OF THE TRACTOR-GRADER AGRICUTURA SYSTEM CINEMATIC
More informationSection 3.5 Nonhomogeneous Equations; Method of Undetermined Coefficients
Secion 3.5 Nonhomogeneous Equaions; Mehod of Undeermined Coefficiens Key Terms/Ideas: Linear Differenial operaor Nonlinear operaor Second order homogeneous DE Second order nonhomogeneous DE Soluion o homogeneous
More informationElements of Stochastic Processes Lecture II Hamid R. Rabiee
Sochasic Processes Elemens of Sochasic Processes Lecure II Hamid R. Rabiee Overview Reading Assignmen Chaper 9 of exbook Furher Resources MIT Open Course Ware S. Karlin and H. M. Taylor, A Firs Course
More informationOrdinary Differential Equations
Lecure 22 Ordinary Differenial Equaions Course Coordinaor: Dr. Suresh A. Karha, Associae Professor, Deparmen of Civil Engineering, IIT Guwahai. In naure, mos of he phenomena ha can be mahemaically described
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 informationPrinciple and Analysis of a Novel Linear Synchronous Motor with Half-Wave Rectified Self Excitation
Principle and Analysis of a Novel Linear Synchronous Moor wih Half-Wave Recified Self Exciaion Jun OYAMA, Tsuyoshi HIGUCHI, Takashi ABE, Shoaro KUBOTA and Tadashi HIRAYAMA Deparmen of Elecrical and Elecronic
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 information15. Vector Valued Functions
1. Vecor Valued Funcions Up o his poin, we have presened vecors wih consan componens, for example, 1, and,,4. However, we can allow he componens of a vecor o be funcions of a common variable. For example,
More informationth World Conference on Earthquake Engineering Vancouver, B.C., Canada August 1-6, 2004 Paper No. 3256
11111 1 h World Conference on Earhquake Engineering Vancouver, B.C., Canada Augus 1-6, 2004 Paper No. 256 TOUCHING ANALYSIS OF TWO BUILDINGS USING FINITE ELEMENT METHOD Mircea IEREMIA 1, Silviu GINJU 1,
More informationNumerical Dispersion
eview of Linear Numerical Sabiliy Numerical Dispersion n he previous lecure, we considered he linear numerical sabiliy of boh advecion and diffusion erms when approimaed wih several spaial and emporal
More information8. Basic RL and RC Circuits
8. Basic L and C Circuis This chaper deals wih he soluions of he responses of L and C circuis The analysis of C and L circuis leads o a linear differenial equaion This chaper covers he following opics
More informationFormulation of the Stress Distribution Due to a Concentrated Force Acting on the Boundary of Viscoelastic Half-Space
Formulaion of he Sress Disribuion Due o a Concenraed Force Acing on he Boundar of Viscoelasic Half-Space Yun eng and Debao Zhou Deparmen of Mechanical and Indusrial Engineering Universi of Minnesoa, Duluh
More informationVIRTUAL MACHINE FOR PROCESSING OF CUTTING TOOLS
7 h INTERNATIONAL MULTIDISCIPLINARY CONFERENCE Baia Mare, Romania, May 7-8, 2007 ISSN-224-3264 VIRTUAL MACHINE FOR PROCESSING OF CUTTING TOOLS Sandu Consanin, assoc. rofessor, Universiy POLITEHNICA of
More informationHomotopy Perturbation Method for Solving Some Initial Boundary Value Problems with Non Local Conditions
Proceedings of he World Congress on Engineering and Compuer Science 23 Vol I WCECS 23, 23-25 Ocober, 23, San Francisco, USA Homoopy Perurbaion Mehod for Solving Some Iniial Boundary Value Problems wih
More informationKINEMATICS IN ONE DIMENSION
KINEMATICS IN ONE DIMENSION PREVIEW Kinemaics is he sudy of how hings move how far (disance and displacemen), how fas (speed and velociy), and how fas ha how fas changes (acceleraion). We say ha an objec
More informationInteractions of magnetic particles in a rotational magnetic field
Bielefeld Universiy Deparmen of Physics Presened a he COMSOL Conference 2008 Hannover A. Weddemann, A. Auge, F. Wibrach, S. Herh, A. Hüen Ineracions of magneic paricles in a roaional magneic field D2 PHYSICS
More informationON THE DEGREES OF RATIONAL KNOTS
ON THE DEGREES OF RATIONAL KNOTS DONOVAN MCFERON, ALEXANDRA ZUSER Absrac. In his paper, we explore he issue of minimizing he degrees on raional knos. We se a bound on hese degrees using Bézou s heorem,
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 informationAt the end of this lesson, the students should be able to understand
Insrucional Objecives A he end of his lesson, he sudens should be able o undersand Sress concenraion and he facors responsible. Deerminaion of sress concenraion facor; experimenal and heoreical mehods.
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 informationFinite Element Analysis of Structures
KAIT OE5 Finie Elemen Analysis of rucures Mid-erm Exam, Fall 9 (p) m. As shown in Fig., we model a russ srucure of uniform area (lengh, Area Am ) subjeced o a uniform body force ( f B e x N / m ) using
More informationAN ANALYSIS OF THE EFFECT OF THE APPLICATION OF HELICAL MOTION AND ASSEMBLY ERRORS ON THE MESHING OF A SPIRAL BEVEL GEAR USING DUPLEX HELICAL METHOD
ADVANCES IN MANUFACTURING SCIENCE AND TECHNOLOGY Vol. 40, No. 1, 2016 DOI: 10.2478/ams-2016-0002 AN ANALYSIS OF THE EFFECT OF THE APPLICATION OF HELICAL MOTION AND ASSEMBLY ERRORS ON THE MESHING OF A SPIRAL
More informationtranslational component of a rigid motion appear to originate.
!"#$%&'()(!"##$%&'(&')*+&'*',*-&.*'/)*/'0%'"1&.3$013'*'#".&45'/.*1%4*/0$1*4'-$/0$16'*1'/)*/' /)&',*-&.*6'(0/)'*'7$,*4'4&13/)'$7'8996'0%'-$+013'(0/)'+&4$,0/5'' :;6'?':@96'A96'B9>C' *>'D&1&.*4456'()*/'0%'/)&'7$,"%'$7'&E#*1%0$1'7$.'*'-$+013',*-&.*F'
More informationv A Since the axial rigidity k ij is defined by P/v A, we obtain Pa 3
The The rd rd Inernaional Conference on on Design Engineering and Science, ICDES 14 Pilsen, Czech Pilsen, Republic, Czech Augus Republic, 1 Sepember 1-, 14 In-plane and Ou-of-plane Deflecion of J-shaped
More informationarxiv: v1 [math.fa] 3 Jan 2019
DAMPED AND DIVERGENCE EXACT SOLUTIONS FOR THE DUFFING EQUATION USING LEAF FUNCTIONS AND HYPERBOLIC LEAF FUNCTIONS A PREPRINT arxiv:9.66v [mah.fa] Jan 9 Kazunori Shinohara Deparmen of Mechanical Sysems
More informationSolitons Solutions to Nonlinear Partial Differential Equations by the Tanh Method
IOSR Journal of Mahemaics (IOSR-JM) e-issn: 7-7,p-ISSN: 319-7X, Volume, Issue (Sep. - Oc. 13), PP 1-19 Solions Soluions o Nonlinear Parial Differenial Equaions by he Tanh Mehod YusurSuhail Ali Compuer
More informationSystem of Linear Differential Equations
Sysem of Linear Differenial Equaions In "Ordinary Differenial Equaions" we've learned how o solve a differenial equaion for a variable, such as: y'k5$e K2$x =0 solve DE yx = K 5 2 ek2 x C_C1 2$y''C7$y
More informationChapters 6 & 7: Trigonometric Functions of Angles and Real Numbers. Divide both Sides by 180
Algebra Chapers & : Trigonomeric Funcions of Angles and Real Numbers Chapers & : Trigonomeric Funcions of Angles and Real Numbers - Angle Measures Radians: - a uni (rad o measure he size of an angle. rad
More informationLAPLACE TRANSFORM AND TRANSFER FUNCTION
CHBE320 LECTURE V LAPLACE TRANSFORM AND TRANSFER FUNCTION Professor Dae Ryook Yang Spring 2018 Dep. of Chemical and Biological Engineering 5-1 Road Map of he Lecure V Laplace Transform and Transfer funcions
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 informationInvolute Gear Tooth Bending Stress Analysis
Involue Gear Tooh Bending Sress Analysis Lecure 21 Engineering 473 Machine Design Gear Ineracion Line of Ceners Line Tangen o s Line Normal o Line of Ceners 1 s Close Up of Meshed Teeh Line of Conac W
More informationApplication of a Stochastic-Fuzzy Approach to Modeling Optimal Discrete Time Dynamical Systems by Using Large Scale Data Processing
Applicaion of a Sochasic-Fuzzy Approach o Modeling Opimal Discree Time Dynamical Sysems by Using Large Scale Daa Processing AA WALASZE-BABISZEWSA Deparmen of Compuer Engineering Opole Universiy of Technology
More informationSummary of shear rate kinematics (part 1)
InroToMaFuncions.pdf 4 CM465 To proceed o beer-designed consiuive equaions, we need o know more abou maerial behavior, i.e. we need more maerial funcions o predic, and we need measuremens of hese maerial
More informationLab #2: Kinematics in 1-Dimension
Reading Assignmen: Chaper 2, Secions 2-1 hrough 2-8 Lab #2: Kinemaics in 1-Dimension Inroducion: The sudy of moion is broken ino wo main areas of sudy kinemaics and dynamics. Kinemaics is he descripion
More informationMETHOD OF CHARACTERISTICS AND GLUON DISTRIBUTION FUNCTION
METHOD OF CHARACTERISTICS AND GLUON DISTRIBUTION FUNCTION Saiful Islam and D. K. Choudhury Dep. Of Physics Gauhai Universiy, Guwahai, Assam, India. Email : saiful.66@rediffmail.com ; dkc_phys@yahoo.co.in
More informationInstitute for Mathematical Methods in Economics. University of Technology Vienna. Singapore, May Manfred Deistler
MULTIVARIATE TIME SERIES ANALYSIS AND FORECASTING Manfred Deisler E O S Economerics and Sysems Theory Insiue for Mahemaical Mehods in Economics Universiy of Technology Vienna Singapore, May 2004 Inroducion
More informationProblemas das Aulas Práticas
Mesrado Inegrado em Engenharia Elecroécnica e de Compuadores Conrolo em Espaço de Esados Problemas das Aulas Práicas J. Miranda Lemos Fevereiro de 3 Translaed o English by José Gaspar, 6 J. M. Lemos, IST
More informationNONLINEAR DYNAMICAL SYSTEMS IN VARIOUS SPACE-TIME DIMENSIONS
NONLINEAR DYNAMICAL SYSTEMS IN VARIOUS SPACE-TIME DIMENSIONS R. CIMPOIASU, V. CIMPOIASU, R. CONSTANTINESCU Universiy of Craiova, 3 A.I. Cuza, 00585 Craiova, Romania Received January, 009 The paper invesigaes
More information4.6 One Dimensional Kinematics and Integration
4.6 One Dimensional Kinemaics and Inegraion When he acceleraion a( of an objec is a non-consan funcion of ime, we would like o deermine he ime dependence of he posiion funcion x( and he x -componen of
More informationChapter 5 Kinematics
Chaper 5 Kinemaics In he firs place, wha do we mean b ime and space? I urns ou ha hese deep philosophical quesions have o be analzed ver carefull in phsics, and his is no eas o do. The heor of relaivi
More informationTime Domain Transfer Function of the Induction Motor
Sudies in Engineering and Technology Vol., No. ; Augus 0 ISSN 008 EISSN 006 Published by Redfame Publishing URL: hp://se.redfame.com Time Domain Transfer Funcion of he Inducion Moor N N arsoum Correspondence:
More informationExtremal problem on (2n, 2m 1)-system points on the rays.
DOI: 0.55/auom-06-0043 An. Ş. Univ. Ovidius Consanţa Vol. 4,06, 83 99 Exremal problem on n, m -sysem poins on he rays. Targonskii A. Absrac In his work derivaion of accurae esimae he producion inner radius
More informationMatlab and Python programming: how to get started
Malab and Pyhon programming: how o ge sared Equipping readers he skills o wrie programs o explore complex sysems and discover ineresing paerns from big daa is one of he main goals of his book. In his chaper,
More information10. State Space Methods
. Sae Space Mehods. Inroducion Sae space modelling was briefly inroduced in chaper. Here more coverage is provided of sae space mehods before some of heir uses in conrol sysem design are covered in he
More informationA New Perturbative Approach in Nonlinear Singularity Analysis
Journal of Mahemaics and Saisics 7 (: 49-54, ISSN 549-644 Science Publicaions A New Perurbaive Approach in Nonlinear Singulariy Analysis Ta-Leung Yee Deparmen of Mahemaics and Informaion Technology, The
More informationProbabilistic Robotics SLAM
Probabilisic Roboics SLAM The SLAM Problem SLAM is he process by which a robo builds a map of he environmen and, a he same ime, uses his map o compue is locaion Localizaion: inferring locaion given a map
More informationOscillation of an Euler Cauchy Dynamic Equation S. Huff, G. Olumolode, N. Pennington, and A. Peterson
PROCEEDINGS OF THE FOURTH INTERNATIONAL CONFERENCE ON DYNAMICAL SYSTEMS AND DIFFERENTIAL EQUATIONS May 4 7, 00, Wilmingon, NC, USA pp 0 Oscillaion of an Euler Cauchy Dynamic Equaion S Huff, G Olumolode,
More informationPhysics for Scientists and Engineers I
Physics for Scieniss and Engineers I PHY 48, Secion 4 Dr. Beariz Roldán Cuenya Universiy of Cenral Florida, Physics Deparmen, Orlando, FL Chaper - Inroducion I. General II. Inernaional Sysem of Unis III.
More informationComputer-Aided Analysis of Electronic Circuits Course Notes 3
Gheorghe Asachi Technical Universiy of Iasi Faculy of Elecronics, Telecommunicaions and Informaion Technologies Compuer-Aided Analysis of Elecronic Circuis Course Noes 3 Bachelor: Telecommunicaion Technologies
More informationA. Using Newton s second law in one dimension, F net. , write down the differential equation that governs the motion of the block.
Simple SIMPLE harmonic HARMONIC moion MOTION I. Differenial equaion of moion A block is conneced o a spring, one end of which is aached o a wall. (Neglec he mass of he spring, and assume he surface is
More information