NONLINEAR MODEL OF THE VEHICLE HYDROPNEUMATIC SUSPENSION UNIT
|
|
- Lucas Horton
- 5 years ago
- Views:
Transcription
1 Nuber, olue II, Deceber NONLINEAR MODEL OF THE EHICLE HYDROPNEUMATIC UPENION UNIT Libor Kuk ury: The lue reers oel of he hyroneuic susension uni n is verificion is escribe in he er. The relions effecive surfce n volue of he rubber bellows ir sring versus osiion n ressure n Bernoulli equion re use in he heicl oel of hyrulic r. The oil volue coression chnges re consiere negligible. The ibic se equion for he gs is use. The gs flow hrough he hroling injecor is consiere boh in uner n overcriicl coniions. The sic n ynic chrcerisics of he whole uni n is rs were esure. Key wors: hyroneuic susension uni, rubber bellows ir sring, heicl oel. INTRODUCTION The hyroneuic susension uni (fig. consiss of hyrulic n neuic rs. I is ossible o sere he hyrulic r for he esureen (,. Fig. Hyroneuic susension uni Ing. Libor Kuk, Ph.D., Universiy of Prubice, Fculy of Elecricl Engineering n Inforics, Deren of Process Conrol, náěsí Čs. legií 6, Prubice, Tel.: , Fx: , E-il: libor.kuk@uce.c Kuk: Nonliner Moel of he vehicle hyroneuic usension Uni 79
2 Nuber, olue II, Deceber The uni (see fig. consiss of: neuic rubber bellows ir sring (, seel chber (, neuic cuor n chnnels (, n, lower n uer rubber bellows sring (6 n 7, silicon oil fille, fixe chnnel (8, hyrulic cuor n chnnels (9,, seel ro ( n lerl guince syse of uer rubber bellows sring (.. NONLINEAR MATHEMATICAL MODEL. Hyrulic r The hyrulic r hs he chrcer of clssic er, bu i hs sll sring chrcer s well. Hyrulic r consiss of wo rubber bellows srings, which re connece wih ech oher hrough hroling bore n rllel hyrulic chnnels wih cuor. Fig. chee of he hyrulic r of he uni (, lower n uer rubber bellows srings, fixe oin of esureen equien, hroling bore, servo vlve The relions beween osiion n ressure of one rubber bellows sring n he effecive surfce were esure using lborory urose-buil esing equien. The relion volue versus osiion n ressure ws roxie wih funcion (. The volue roxiion funcion ws chosen in he following for (, e, ( where is volue, is osiion, is ressure, u o re coefficiens. The coefficiens n were eerine exerienlly fro he esureen on he sseble hyrulic r. The exlici exression = (, fro ( is e. ( The ressure insie e.g. lower rubber bellows sring s funcion of ie is escribe by Kuk: Nonliner Moel of he vehicle hyroneuic usension Uni 8
3 Nuber, olue II, Deceber. ( = / is oil volue flow ino he rubber bellows sring. = f (, [c ].8.6. [MP]. - - [c] Fig. D visuliion of he funcion = (, 8 rojecion of = f (, 6 [c ] [c] Fig. Projecion of cross secion curves of he funcion = (,, curves reer is ressure =. u o. MP Kuk: Nonliner Moel of he vehicle hyroneuic usension Uni 8
4 Nuber, olue II, Deceber Kuk: Nonliner Moel of he vehicle hyroneuic usension Uni 8 Le us coue he erivives / n / fro ( n subsiue he ino ( e e ( ( ( ( ( Le us esigne he ressures insie he lower n he uer bellows n ifference beween he, n = resecively. The following roxiion of he soluion of Bernoulli's equion ws use o coue h h e sign( R, ( R h is hyrulic resisnce n h is coefficien which ffecs he erivive /( for =. The force hef hef h F F F, (6 hef n hef re effecive surfces of he uer n lower bellows srings. The roxiion of he effecive surfce of bellows sring ws chosen in he following for e hef, (. (7 Fig. D visuliion of he roxiion hef = hef (, n esureens of n effecive surfce. Pneuic r The neuic r of he susension uni consiss of rubber bellows srings, seel chber n cuor hroling eleen (see fig. 6. The equion of ibic chnges in ir is kons, (8 where is ressure, is ensiy n =.. The ifferenil for of (8 is
5 Nuber, olue II, Deceber. (9 Fro (9 ( n. ( Mss conservion lw is kons ( n he ifferenil for of his lw is, ( is ss flow. Fig. 6 chee of he neuic r of he uni ( bellows ir sring, seel chber, fixe oin of esureen equien, hroling injecor, loss coefficien PT, servo vlve, loss coefficien P Kuk: Nonliner Moel of he vehicle hyroneuic usension Uni 8
6 Nuber, olue II, Deceber Kuk: Nonliner Moel of he vehicle hyroneuic usension Uni 8 The oificions of equion ( for boh rs of neuic uni re ( ( n (. ( Fro ( n (, (6 resecively. (7 Bernoulli equion is use for he ibic gs flow hrough he hroling injecor kons v v i i i i i i, (8 i, v i, i n i, v i, i re vribles, which escribe he flow in fron of n behin he hroling injecor. ince v i << v i, he relion beween flow velociies is i i i i i v. (9 For i, i n i, i fro (8 i i i i. ( The ss flow hrough he hroling injecor is i i v, ( is he secionl re of he hroling injecor. Afer subsiuion of (9 n ( ino ( n using he loss coefficien is i i i i i i. ( This equion is vli for uner-criicl (linr flow, in he cse of ir i ens for i / i.8. Le us esigne kri / i =.8. For over-criicl (urbulen flow, for i / i <.8 is i kri i kri i i. (
7 Nuber, olue II, Deceber The resuling force is F F F F G. ( The force F of he rubber bellows ir sring (fig. 7 is F. ( ef The eenences of effecive surfce ef n volue on osiion (see fig. 8 were roxie wih fifh egrees olynoils. Fig. 7 chee of he rubber bellows ir sring Ruben D -7 ef = f(, = f( ef ( ( 6 ef [c ] [c ] [c] Fig. 8 Effecive surfce n volue of he use bellows sring Ruben D -7 ( ef ef n Kuk: Nonliner Moel of he vehicle hyroneuic usension Uni 8
8 Nuber, olue II, Deceber. IMULATION The siulion oel ws cree in MATLAB iulink. Plos of n xil force F( cquire by nuericl siulion re in figs. 9 u o, he frequencies of he hronic signl were.6,. n. H, he liues were, n. Fig. 9 Corison of he oel n exerienl for frequency.6 H n liue (xil force F = F( Kuk: Nonliner Moel of he vehicle hyroneuic usension Uni 86
9 Nuber, olue II, Deceber 6 exerien oel F( F [kn] [c] Fig. Corison of he oel n exerienl for frequency.6 H n liue (xil force F = F( Fig. Corison of he oel n exerienl for frequency. H n liue (xil force F = F( Kuk: Nonliner Moel of he vehicle hyroneuic usension Uni 87
10 Nuber, olue II, Deceber 7 6 exerien oel F( F [kn] [c] Fig. Corison of he oel n exerienl for frequency. H n liue (xil force F = F( Fig. Corison of he oel n exerienl for frequency. H n liue (xil force F = F( Kuk: Nonliner Moel of he vehicle hyroneuic usension Uni 88
11 Nuber, olue II, Deceber 6 exerien oel F( F [kn] [c] Fig. Corison of he oel n exerienl for frequency. H n liue (xil force F = F( CONLUION The eveloen of hyroneuic susension uni (wih rubber bellows srings is escribe in he er. The siulion oel ws cree in MATLAB iulink. This oel ches he ynics of he hyroneuic uni uner consierion relively well. Prosecive licion of his uni is ruck bck xle susension. The sring n ing chrcerisics cn be chnge in he cse of sei-cive, or cive conrol. The conrol hs no been esigne ye. ACKNOWLEDGMENT The work hs been suore by he funs No. GFEI/ of he Universiy of Prubice, Cech Reublic. This suor is very grefully cknowlege. REFERENCE ( ŠKLÍBA, J.; BARBORA, J.; CIRKL, D. Hyroneuický člen s rlelní ření hyrulického neuického luení. In Proceeings of Inercion n Feebcks. Prgue: Insiue of Theroechnics A CR,.. 6. IBN ( BARBORA, J.; JANEČEK, B.; KUPKA, L.; ZŮBEK, T. Hyroneuic usension Rubber-bellows Uni. In Proceeings of Colloquiu Euroech on ei-acive ibrion uression [CD ROM]. Prgue: CTU,.. ( BAUER, W. Hyroneuic usensions yses. s e. Berlin Heielberg New York: ringer,. IBN Kuk: Nonliner Moel of he vehicle hyroneuic usension Uni 89
12 Nuber, olue II, Deceber ( HANUŠ, B.; OLEHLA, M.; MODRLÁK, O. Číslicová regulce echnologických rocesů: lgoriy, eicko-fyikální nlý, ienifikce, ce. Brno: BUT,. IBN 8--6-X. ( ETFÁLOÁ, M.; TŘEDA, I. Technická ynik lynů. Liberec: TU,. (6 KUPKA L.: yhonocení růběhů růokových chrkerisik elekroneuického servovenilu EF. [Reserch reor.] Liberec: TU,. Kuk: Nonliner Moel of he vehicle hyroneuic usension Uni 9
IDENTIFICATION OF STATIC CHARACTERISTICS OF A PNEUMATIC REGULATOR OF BRAKING FORCES IN VEHICLES. Jarosław Czaban, Mikołaj Miatluk
TEKA Ko. Mo. Energ. oln., 5, 5, 8-55 IENTIFICATION OF TATIC CHAACTEITIC OF A PNEUMATIC EGULATO OF BAKING FOCE IN VEHICLE Jarosław Czaban, Mikołaj Mialuk earen of Auooive Vehicle, earen of Auoaion Technique,
More informationt v a t area Dynamic Physics for Simulation and Game Programming F a m v v a t x x v t Discrete Dynamics
Dynic Physics for Siulion n Ge Progring F Discree Dynics. Force equls ss ies ccelerion (F=) v v v v Mike Biley This work is license uner Creive Coons Aribuion-NonCoercil- NoDerivives.0 Inernionl License
More informationφ p ( B) AR polynomial of B of order p, p Non-seasonal differencing operator = 1 B
ARIMA Noion The ARIMA roceure coues he reer esies for given sesonl or non-sesonl univrie ARIMA oel. I lso coues he fie vlues, forecsing vlues, n oher rele vribles for he oel. The following noion is use
More informationChapter 10. Simple Harmonic Motion and Elasticity. Goals for Chapter 10
Chper 0 Siple Hronic Moion nd Elsiciy Gols or Chper 0 o ollow periodic oion o sudy o siple hronic oion. o sole equions o siple hronic oion. o use he pendulu s prooypicl syse undergoing siple hronic oion.
More informationConservation of Momentum. The purpose of this experiment is to verify the conservation of momentum in two dimensions.
Conseraion of Moenu Purose The urose of his exerien is o erify he conseraion of oenu in wo diensions. Inroducion and Theory The oenu of a body ( ) is defined as he roduc of is ass () and elociy ( ): When
More informationP441 Analytical Mechanics - I. Coupled Oscillators. c Alex R. Dzierba
Lecure 3 Mondy - Deceber 5, 005 Wrien or ls upded: Deceber 3, 005 P44 Anlyicl Mechnics - I oupled Oscillors c Alex R. Dzierb oupled oscillors - rix echnique In Figure we show n exple of wo coupled oscillors,
More information6. Gas dynamics. Ideal gases Speed of infinitesimal disturbances in still gas
6. Gs dynmics Dr. Gergely Krisóf De. of Fluid echnics, BE Februry, 009. Seed of infiniesiml disurbnces in sill gs dv d, dv d, Coninuiy: ( dv)( ) dv omenum r r heorem: ( ( dv) ) d 3443 4 q m dv d dv llievi
More information(b) 10 yr. (b) 13 m. 1.6 m s, m s m s (c) 13.1 s. 32. (a) 20.0 s (b) No, the minimum distance to stop = 1.00 km. 1.
Answers o Een Numbered Problems Chper. () 7 m s, 6 m s (b) 8 5 yr 4.. m ih 6. () 5. m s (b).5 m s (c).5 m s (d) 3.33 m s (e) 8. ().3 min (b) 64 mi..3 h. ().3 s (b) 3 m 4..8 mi wes of he flgpole 6. (b)
More informationPractice Problems - Week #4 Higher-Order DEs, Applications Solutions
Pracice Probles - Wee #4 Higher-Orer DEs, Applicaions Soluions 1. Solve he iniial value proble where y y = 0, y0 = 0, y 0 = 1, an y 0 =. r r = rr 1 = rr 1r + 1, so he general soluion is C 1 + C e x + C
More informationPhysics Worksheet Lesson 4: Linear Motion Section: Name:
Physics Workshee Lesson 4: Liner Moion Secion: Nme: 1. Relie Moion:. All moion is. b. is n rbirry coorine sysem wih reference o which he posiion or moion of somehing is escribe or physicl lws re formule.
More informationForms of Energy. Mass = Energy. Page 1. SPH4U: Introduction to Work. Work & Energy. Particle Physics:
SPH4U: Inroducion o ork ork & Energy ork & Energy Discussion Definiion Do Produc ork of consn force ork/kineic energy heore ork of uliple consn forces Coens One of he os iporn conceps in physics Alernive
More informationSTATE CONTROLLER DESIGN OF THE ACTIVELY CONTROLLED DRIVER S SEAT
STATE CONTROLLER DESIGN OF THE ACTIELY CONTROLLED DRIER S SEAT Libor K Smmry: In e er e inrocion sies o e se conroller esign o cive vibrion isolion sysem o e river se re resene. Te river se i e ir sring
More informationMotion. Part 2: Constant Acceleration. Acceleration. October Lab Physics. Ms. Levine 1. Acceleration. Acceleration. Units for Acceleration.
Moion Accelerion Pr : Consn Accelerion Accelerion Accelerion Accelerion is he re of chnge of velociy. = v - vo = Δv Δ ccelerion = = v - vo chnge of velociy elpsed ime Accelerion is vecor, lhough in one-dimensionl
More informationHomework 2 Solutions
Mah 308 Differenial Equaions Fall 2002 & 2. See he las page. Hoework 2 Soluions 3a). Newon s secon law of oion says ha a = F, an we know a =, so we have = F. One par of he force is graviy, g. However,
More informationOur main purpose in this section is to undertake an examination of the stock
3. Caial gains ax and e sock rice volailiy Our main urose in is secion is o underake an examinaion of e sock rice volailiy by considering ow e raional seculaor s olding canges afer e ax rae on caial gains
More informationProblems on transformer main dimensions and windings
Probles_Trn_winding Probles on rnsforer in diensions nd windings. Deerine he in diensions of he core nd window for 500 ka, /400, 50Hz, Single phse core ype, oil iersed, self cooled rnsforer. Assue: Flux
More informationImproved Analysis of the Coupling of Optical Waves into Multimode Waveguides Using Overlap Integrals
464 rogress In Elecrogneics Reserch Syosiu 5, Hngzhou, Chin, Augus -6 Iroved Anlysis of he Couling of Oicl Wves ino Muliode Wveguides Using Overl Inegrls M Sllein, C Kollec, nd G Mrozynsi Universiy of
More informationCharacteristic Function for the Truncated Triangular Distribution., Myron Katzoff and Rahul A. Parsa
Secion on Survey Reserch Mehos JSM 009 Chrcerisic Funcion for he Trunce Tringulr Disriuion Jy J. Kim 1 1, Myron Kzoff n Rhul A. Prs 1 Nionl Cener for Helh Sisics, 11Toleo Ro, Hysville, MD. 078 College
More informationELEC-E8417 Switched-Mode Power Supplies Exam
ELE-E847 Swiche-Moe Power Supplies Exa 7..06 Quesion. n sep-up converer (Boos) he oupu volage o = 48 V an supply volage changes beween 0 V 5 V. upu power P o 5 W an swiching frequency ƒ s = 0 khz, = 47
More informationAn object moving with speed v around a point at distance r, has an angular velocity. m/s m
Roion The mosphere roes wih he erh n moions wihin he mosphere clerly follow cure phs (cyclones, nicyclones, hurricnes, ornoes ec.) We nee o epress roion quniiely. For soli objec or ny mss h oes no isor
More informationAN ANALYSIS OF TRANSIENT PROCESSES IN PNEUMATIC BRAKE SYSTEM WITH AUTOMATIC REGULATOR OF BRAKE FORCES OF AUTOMOTIVE VEHICLES 1
TEK Ko. Mo. Energ. Roln.,,, 8 9 N NLYSIS OF TRNSIENT PROCESSES IN PNEUMTIC BRKE SYSTEM WITH UTOMTIC REGULTOR OF BRKE FORCES OF UTOMOTIE EHICLES Mikołaj Mialuk, Jarosław Czaban Dearen of uoaion Technique
More information4.8 Improper Integrals
4.8 Improper Inegrls Well you ve mde i hrough ll he inegrion echniques. Congrs! Unforunely for us, we sill need o cover one more inegrl. They re clled Improper Inegrls. A his poin, we ve only del wih inegrls
More informationContraction Mapping Principle Approach to Differential Equations
epl Journl of Science echnology 0 (009) 49-53 Conrcion pping Principle pproch o Differenil Equions Bishnu P. Dhungn Deprmen of hemics, hendr Rn Cmpus ribhuvn Universiy, Khmu epl bsrc Using n eension of
More informationRESPONSE UNDER A GENERAL PERIODIC FORCE. When the external force F(t) is periodic with periodτ = 2π
RESPONSE UNDER A GENERAL PERIODIC FORCE When he exernl force F() is periodic wih periodτ / ω,i cn be expnded in Fourier series F( ) o α ω α b ω () where τ F( ) ω d, τ,,,... () nd b τ F( ) ω d, τ,,... (3)
More informationPHYSICS 1210 Exam 1 University of Wyoming 14 February points
PHYSICS 1210 Em 1 Uniersiy of Wyoming 14 Februry 2013 150 poins This es is open-noe nd closed-book. Clculors re permied bu compuers re no. No collborion, consulion, or communicion wih oher people (oher
More informationPhysics 2A HW #3 Solutions
Chper 3 Focus on Conceps: 3, 4, 6, 9 Problems: 9, 9, 3, 41, 66, 7, 75, 77 Phsics A HW #3 Soluions Focus On Conceps 3-3 (c) The ccelerion due o grvi is he sme for boh blls, despie he fc h he hve differen
More informationMEI 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 informationHow to Prove the Riemann Hypothesis Author: Fayez Fok Al Adeh.
How o Prove he Riemnn Hohesis Auhor: Fez Fok Al Adeh. Presiden of he Srin Cosmologicl Socie P.O.Bo,387,Dmscus,Sri Tels:963--77679,735 Emil:hf@scs-ne.org Commens: 3 ges Subj-Clss: Funcionl nlsis, comle
More informationAverage & instantaneous velocity and acceleration Motion with constant acceleration
Physics 7: Lecure Reminders Discussion nd Lb secions sr meeing ne week Fill ou Pink dd/drop form if you need o swich o differen secion h is FULL. Do i TODAY. Homework Ch. : 5, 7,, 3,, nd 6 Ch.: 6,, 3 Submission
More informationSeptember 20 Homework Solutions
College of Engineering nd Compuer Science Mechnicl Engineering Deprmen Mechnicl Engineering A Seminr in Engineering Anlysis Fll 7 Number 66 Insrucor: Lrry Creo Sepember Homework Soluions Find he specrum
More informationSolutions to Problems from Chapter 2
Soluions o Problems rom Chper Problem. The signls u() :5sgn(), u () :5sgn(), nd u h () :5sgn() re ploed respecively in Figures.,b,c. Noe h u h () :5sgn() :5; 8 including, bu u () :5sgn() is undeined..5
More informationd 1 = c 1 b 2 - b 1 c 2 d 2 = c 1 b 3 - b 1 c 3
and d = c b - b c c d = c b - b c c This process is coninued unil he nh row has been compleed. The complee array of coefficiens is riangular. Noe ha in developing he array an enire row may be divided or
More informationConservation Law. Chapter Goal. 6.2 Theory
Chpter 6 Conservtion Lw 6.1 Gol Our long term gol is to unerstn how mthemticl moels re erive. Here, we will stuy how certin quntity chnges with time in given region (sptil omin). We then first erive the
More informationBoundary layer problem for system of first order of ordinary differential equations with linear non-local boundary conditions
IJS 3 37A3 Secil issue-mheics: 389-396 Irnin Journl of Science & echnology h://ijssshirzucir Boundry lyer role for syse of firs order of ordinry differenil euions wih liner non-locl oundry condiions M
More informationET 438a Automatic Control Systems Technology. After this presentation you will be able to:
8/7/5 ESSON 8: MODEING PHYSI SYSEMS WIH INE DIFFEENI EQUIONS E 438a uoaic onrol Syses echnology earng Objecives fer his presenaion you will be able o: Expla wha a ifferenial equaion is an how i can represen
More informationHW #1 Solutions. Lewis Structures: Using the above rules, determine the molecular structure for Cl2CO. Hint: C is at the center.
HW # Soluions Cron Mss Prolem: ssuming n erge surfce pressure of m, n erge ropospheric emperure of 55 K, n glol CO mixing rio of 385 ppm, wh is he curren mospheric Cron reseroir (in unis of g m -? Compre
More informationA 1.3 m 2.5 m 2.8 m. x = m m = 8400 m. y = 4900 m 3200 m = 1700 m
PHYS : Soluions o Chper 3 Home Work. SSM REASONING The displcemen is ecor drwn from he iniil posiion o he finl posiion. The mgniude of he displcemen is he shores disnce beween he posiions. Noe h i is onl
More information1 Radian Measures. Exercise 1. A --- 1Vc. MAT Worksheet 10 Sections 7.1, 8.1 Name:
MAT 012 55218 1 Radian Measures Consider he following figure. corresponding o he angle 0. Exercise 1 The shaded porion of he circle is called he secor of he circle K V 1. Suppose know he radian measure
More informationModule 4: Time Response of discrete time systems Lecture Note 2
Module 4: Time Response of discree ime sysems Lecure Noe 2 1 Prooype second order sysem The sudy of a second order sysem is imporan because many higher order sysem can be approimaed by a second order model
More informationChapter Three Systems of Linear Differential Equations
Chaper Three Sysems of Linear Differenial Equaions In his chaper we are going o consier sysems of firs orer orinary ifferenial equaions. These are sysems of he form x a x a x a n x n x a x a x a n x n
More information3 Motion with constant acceleration: Linear and projectile motion
3 Moion wih consn ccelerion: Liner nd projecile moion cons, In he precedin Lecure we he considered moion wih consn ccelerion lon he is: Noe h,, cn be posiie nd neie h leds o rie of behiors. Clerl similr
More informationThe solution is often represented as a vector: 2xI + 4X2 + 2X3 + 4X4 + 2X5 = 4 2xI + 4X2 + 3X3 + 3X4 + 3X5 = 4. 3xI + 6X2 + 6X3 + 3X4 + 6X5 = 6.
[~ o o :- o o ill] i 1. Mrices, Vecors, nd Guss-Jordn Eliminion 1 x y = = - z= The soluion is ofen represened s vecor: n his exmple, he process of eliminion works very smoohly. We cn elimine ll enries
More informationHall effect. Formulae :- 1) Hall coefficient RH = cm / Coulumb. 2) Magnetic induction BY 2
Page of 6 all effec Aim :- ) To deermine he all coefficien (R ) ) To measure he unknown magneic field (B ) and o compare i wih ha measured by he Gaussmeer (B ). Apparaus :- ) Gauss meer wih probe ) Elecromagne
More informationCHAPTER 12 DIRECT CURRENT CIRCUITS
CHAPTER 12 DIRECT CURRENT CIUITS DIRECT CURRENT CIUITS 257 12.1 RESISTORS IN SERIES AND IN PARALLEL When wo resisors are conneced ogeher as shown in Figure 12.1 we said ha hey are conneced in series. As
More informationON THE PROBLEM OF HEIGHT ADJUSTMENT OF THE ACTIVELY CONTROLLED DRIVER S SEAT VIBRATION ISOLATION STAND
Number 5, Volume VI, December 0 ON THE POBLEM OF HEIGHT ADJUSTMENT OF THE ACTIVELY CONTOLLED DIVE S SEAT VIBATION ISOLATION STAND Libor Kupka Summary: Every driver s seat vibration isolation stand is supplied
More informationOn Customized Goods, Standard Goods, and Competition
On Cusomize Goos, Sanar Goos, an Compeiion Nilari. Syam C. T. auer College of usiness Universiy of Houson 85 Melcher Hall, Houson, TX 7704 Email: nbsyam@uh.eu Phone: (71 74 4568 Fax: (71 74 457 Nana Kumar
More informationMOMENTUM CONSERVATION LAW
1 AAST/AEDT AP PHYSICS B: Impulse and Momenum Le us run an experimen: The ball is moving wih a velociy of V o and a force of F is applied on i for he ime inerval of. As he resul he ball s velociy changes
More informationA Kalman filtering simulation
A Klmn filering simulion The performnce of Klmn filering hs been esed on he bsis of wo differen dynmicl models, ssuming eiher moion wih consn elociy or wih consn ccelerion. The former is epeced o beer
More informationChapter 9 Sinusoidal Steady State Analysis
Chaper 9 Sinusoidal Seady Sae Analysis 9.-9. The Sinusoidal Source and Response 9.3 The Phasor 9.4 pedances of Passive Eleens 9.5-9.9 Circui Analysis Techniques in he Frequency Doain 9.0-9. The Transforer
More informationModeling and Stabilizing Control of an UAV for Easy Taking-off and Hovering.
Moeling n Sbilizing Conrol of n UAV for Esy Tking-off n Hovering. NASR Slh CEM-Lb ENIS Sfx, Nionl Engineering School of Sousse, Universiy of Sousse, Tunisi. nsrslh.oc@gil.co BOUALLEGUE Kis Depren of Elecricl
More informationCollision Detection and Bouncing
Collision Deecion nd Bouncing Collisions re Hndled in Two Prs. Deecing he collision Mike Biley mj@cs.oregonse.edu. Hndling he physics of he collision collision-ouncing.ppx If You re Lucky, You Cn Deec
More informationChapter Direct Method of Interpolation
Chper 5. Direc Mehod of Inerpolion Afer reding his chper, you should be ble o:. pply he direc mehod of inerpolion,. sole problems using he direc mehod of inerpolion, nd. use he direc mehod inerpolns o
More informationPhysics 218 Exam 1. with Solutions Fall 2010, Sections Part 1 (15) Part 2 (20) Part 3 (20) Part 4 (20) Bonus (5)
Physics 18 Exam 1 wih Soluions Fall 1, Secions 51-54 Fill ou he informaion below bu o no open he exam unil insruce o o so! Name Signaure Suen ID E-mail Secion # ules of he exam: 1. You have he full class
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 informationMotion in a Straight Line
Moion in Srigh Line. Preei reched he mero sion nd found h he esclor ws no working. She wlked up he sionry esclor in ime. On oher dys, if she remins sionry on he moing esclor, hen he esclor kes her up in
More informationTEST - 4 (Paper-I) ANSWERS PHYSICS CHEMISTRY MATHEMATICS
TEST - 4 (Pper-I) NSWERS PHYSICS CHEMISTRY MTHEMTICS. (4). (). () 4. () 5. () 6. (4) 7. () 8. () 9. (). (). (). (). () 4. () 5. () 6. (4) 7. () 8. (4) 9. (). (). (). (). () 4. (4) 5. (4) 6. () 7. () 8.
More information1. VELOCITY AND ACCELERATION
1. VELOCITY AND ACCELERATION 1.1 Kinemaics Equaions s = u + 1 a and s = v 1 a s = 1 (u + v) v = u + as 1. Displacemen-Time Graph Gradien = speed 1.3 Velociy-Time Graph Gradien = acceleraion Area under
More informationMaterial Resistance and Friction in Cold Rolling
h World Congresses of Srucural and Mulidiscilinary Oimizaion Rio de Janeiro, 30 May - 03 June 200, Brazil Maerial Resisance and Fricion in Cold Rolling A.K. Tieu, C. You, H.T. Zhu, C. Lu, Z.Y. Jiang and
More informationMore on Magnetically C Coupled Coils and Ideal Transformers
Appenix ore on gneiclly C Couple Coils Iel Trnsformers C. Equivlen Circuis for gneiclly Couple Coils A imes, i is convenien o moel mgneiclly couple coils wih n equivlen circui h oes no involve mgneic coupling.
More informationSTUDY OF THERMAL PROPERTIES OF POROUS MATERIALS
SUY OF HRMAL PROPRIS OF POROUS MARIALS Oldři Zeškl, Pvl Šefková Insiue of Pysil nd Alied Ceisry, Fuly of Ceisry, Brno Universiy of enology, Purkyňov 118, CZ-61 Brno, Cze Reubli il: zeskl@f.vubr.z, sefkov@f.vubr.z
More informationDVC. VARIZON Displacement unit with adjustable spread pattern QUICK FACTS
VARIZON Dislacemen uni wih adjusable sread aern QUICK FACTS Adjusable sread aern and affeced zone Suiable for all yes of rooms Air volume measuring oin Cleanable Concealed fasening Sandard colour Whie
More informationMagnetostatics Bar Magnet. Magnetostatics Oersted s Experiment
Mgneosics Br Mgne As fr bck s 4500 yers go, he Chinese discovered h cerin ypes of iron ore could rc ech oher nd cerin mels. Iron filings "mp" of br mgne s field Crefully suspended slivers of his mel were
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 informationMA 214 Calculus IV (Spring 2016) Section 2. Homework Assignment 1 Solutions
MA 14 Calculus IV (Spring 016) Secion Homework Assignmen 1 Soluions 1 Boyce and DiPrima, p 40, Problem 10 (c) Soluion: In sandard form he given firs-order linear ODE is: An inegraing facor is given by
More informationThink of the Relationship Between Time and Space Again
Repor nd Opinion, 1(3),009 hp://wwwsciencepubne sciencepub@gmilcom Think of he Relionship Beween Time nd Spce Agin Yng F-cheng Compny of Ruid Cenre in Xinjing 15 Hongxing Sree, Klmyi, Xingjing 834000,
More informationHow to prove the Riemann Hypothesis
Scholrs Journl of Phsics, Mhemics nd Sisics Sch. J. Phs. Mh. S. 5; (B:5-6 Scholrs Acdemic nd Scienific Publishers (SAS Publishers (An Inernionl Publisher for Acdemic nd Scienific Resources *Corresonding
More informationM r. d 2. R t a M. Structural Mechanics Section. Exam CT5141 Theory of Elasticity Friday 31 October 2003, 9:00 12:00 hours. Problem 1 (3 points)
Delf Universiy of Technology Fculy of Civil Engineering nd Geosciences Srucurl echnics Secion Wrie your nme nd sudy numer he op righ-hnd of your work. Exm CT5 Theory of Elsiciy Fridy Ocoer 00, 9:00 :00
More informationY 0.4Y 0.45Y Y to a proper ARMA specification.
HG Jan 04 ECON 50 Exercises II - 0 Feb 04 (wih answers Exercise. Read secion 8 in lecure noes 3 (LN3 on he common facor problem in ARMA-processes. Consider he following process Y 0.4Y 0.45Y 0.5 ( where
More informationArea A 0 level is h 0, assuming the pipe flow to be laminar. D, L and assuming the pipe flow to be highly turbulent.
Pipe Flows (ecures 5 o 7). Choose he crec answer (i) While deriving an expression f loss of head due o a sudden expansion in a pipe, in addiion o he coninuiy and impulse-momenum equaions, one of he following
More informationMeasurement of the Equivalent Thermal Resistance of Rooftop Lawns in a. Hot-Climate Wind Tunnel 1
ICEBO006, Shenzhen, China Envelope Technologies for Builing Energy Efficiency Vol.II-4- Measuremen of he Equivalen Thermal Resisance of Roofop Lawns in a Ho-Climae Win Tunnel Qinglin Meng Yu Zhang Lei
More informationMathematical Modeling
ME pplie Engineering nlsis Chper Mhemicl Moeling Professor Ti-Rn Hsu, Ph.D. Deprmen of Mechnicl n erospce Engineering Sn Jose Se Universi Sn Jose, Cliforni, US Jnur Chper Lerning Ojecives Mhemicl moeling
More informationMTH 146 Class 11 Notes
8.- Are of Surfce of Revoluion MTH 6 Clss Noes Suppose we wish o revolve curve C round n is nd find he surfce re of he resuling solid. Suppose f( ) is nonnegive funcion wih coninuous firs derivive on he
More informationLecture 28: Single Stage Frequency response. Context
Lecure 28: Single Sage Frequency response Prof J. S. Sih Conex In oday s lecure, we will coninue o look a he frequency response of single sage aplifiers, saring wih a ore coplee discussion of he CS aplifier,
More informationEXPONENTIAL PROBABILITY DISTRIBUTION
MTH/STA 56 EXPONENTIAL PROBABILITY DISTRIBUTION As discussed in Exaple (of Secion of Unifor Probabili Disribuion), in a Poisson process, evens are occurring independenl a rando and a a unifor rae per uni
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 informationChickens vs. Eggs: Replicating Thurman and Fisher (1988) by Arianto A. Patunru Department of Economics, University of Indonesia 2004
Chicens vs. Eggs: Relicaing Thurman and Fisher (988) by Ariano A. Paunru Dearmen of Economics, Universiy of Indonesia 2004. Inroducion This exercise lays ou he rocedure for esing Granger Causaliy as discussed
More informationSome Inequalities variations on a common theme Lecture I, UL 2007
Some Inequliies vriions on common heme Lecure I, UL 2007 Finbrr Hollnd, Deprmen of Mhemics, Universiy College Cork, fhollnd@uccie; July 2, 2007 Three Problems Problem Assume i, b i, c i, i =, 2, 3 re rel
More informationf t f a f x dx By Lin McMullin f x dx= f b f a. 2
Accumulion: Thoughs On () By Lin McMullin f f f d = + The gols of he AP* Clculus progrm include he semen, Sudens should undersnd he definie inegrl s he ne ccumulion of chnge. 1 The Topicl Ouline includes
More informationReading. Lecture 28: Single Stage Frequency response. Lecture Outline. Context
Reading Lecure 28: Single Sage Frequency response Prof J. S. Sih Reading: We are discussing he frequency response of single sage aplifiers, which isn reaed in he ex unil afer uli-sae aplifiers (beginning
More information19. Oscillations. Objectives. By Liew Sau Poh. Outcomes. Outcomes. Periodic Motion Characteristics of SHM. Position VS.
9. Oscillions By iew Su Poh Ojecies 9. Chrcerisics of siple hronic oion 9. Kineics of siple hronic oion 9.3 Enery in siple hronic oion 9.4 Syses in siple hronic oion 9.5 Dpe oscillions 9.6 Force oscillions
More informationFuji Power MOSFET Power calculation method
Fuji Power MOSFE Power clculi mehod Design ool Cher. Overview is necessry o check wheher he ower loss hs no exceeded he Asolue Mximum Rings for using MOSFE. Since he MOSFE loss cnno e mesured using ower
More informationLecture 23 Damped Motion
Differenial Equaions (MTH40) Lecure Daped Moion In he previous lecure, we discussed he free haronic oion ha assues no rearding forces acing on he oving ass. However No rearding forces acing on he oving
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 informationChapter 2. Motion along a straight line. 9/9/2015 Physics 218
Chper Moion long srigh line 9/9/05 Physics 8 Gols for Chper How o describe srigh line moion in erms of displcemen nd erge elociy. The mening of insnneous elociy nd speed. Aerge elociy/insnneous elociy
More information22.615, MHD Theory of Fusion Systems Prof. Freidberg Lecture 10: The High Beta Tokamak Con d and the High Flux Conserving Tokamak.
.615, MHD Theory of Fusion Sysems Prof. Freidberg Lecure 1: The High Be Tokmk Con d nd he High Flux Conserving Tokmk Proeries of he High Tokmk 1. Evlue he MHD sfey fcor: ψ B * ( ) 1 3 ρ 1+ ν ρ ρ cosθ *
More informationLecture 15: Differential Pairs (Part 2)
Lecure 5: ifferenial Pairs (Par ) Gu-Yeon Wei ivision of Enineerin and Applied Sciences Harvard Universiy uyeon@eecs.harvard.edu Wei Overview eadin S&S: Chaper 6.6 Suppleenal eadin S&S: Chaper 6.9 azavi,
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 informationJOY: The Journal of Yoga Summer 2008, Volume 7, Number 2
JOY: The Journal o Yoga Summer 008, Volume 7, Number The Mahemaical modeling o Pranic Body Saria*, VKKaiyar**, PPradhan * *Dearmen o Mahemaics & Saisics Gurukul kangri Univerisiy, aridwar, Uarakhand India
More informationA NUMERICAL STUDY ON MULTI-CHAMBER OSCILLATING WATER COLUMNS
Journl of JSCE, Vol. 3, 93-4, 5 A UMERICAL STUDY O MULTI-CAMBER OSCILLATIG WATER COLUMS Pllv KOIRALA, Shuichi AGATA, Ysuk IMAI 3, Tengen MURAKAMI 4 nd Toshiki SETOGUCI 5 Posdocorl Resercher, Insiue of
More informationTHEORY OF CUMULATIVE FUEL CONSUMPTION BY LPG POWERED CARS
Journal of KONES Powerrain an Transor, Vol. 22, No. 4 205 THEORY OF CUMULATIVE FUEL CONSUMPTION BY LPG POWERED CARS Lech Jerzy Sinik Wroclaw Universiy of Technology Faculy of Mechanical Engineering Wysianskiego
More informationMath 333 Problem Set #2 Solution 14 February 2003
Mah 333 Problem Se #2 Soluion 14 February 2003 A1. Solve he iniial value problem dy dx = x2 + e 3x ; 2y 4 y(0) = 1. Soluion: This is separable; we wrie 2y 4 dy = x 2 + e x dx and inegrae o ge The iniial
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 information3. Renewal Limit Theorems
Virul Lborories > 14. Renewl Processes > 1 2 3 3. Renewl Limi Theorems In he inroducion o renewl processes, we noed h he rrivl ime process nd he couning process re inverses, in sens The rrivl ime process
More informationI. Define the Situation
I. efine he Siuaion This exam explores he relaionship beween he applied volage o a permanen magne C moond he linear velociy (speed) of he elecric vehicle (EV) he moor drives. The moor oupu is fed ino a
More informationFM Applications of Integration 1.Centroid of Area
FM Applicions of Inegrion.Cenroid of Are The cenroid of ody is is geomeric cenre. For n ojec mde of uniform meril, he cenroid coincides wih he poin which he ody cn e suppored in perfecly lnced se ie, is
More informationON THE BEAT PHENOMENON IN COUPLED SYSTEMS
8 h ASCE Specialy Conference on Probabilisic Mechanics and Srucural Reliabiliy PMC-38 ON THE BEAT PHENOMENON IN COUPLED SYSTEMS S. K. Yalla, Suden Member ASCE and A. Kareem, M. ASCE NaHaz Modeling Laboraory,
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 informationMathematical Modeling of Hydroelastic Oscillations of the Stamp and the Plate, Resting on Pasternak Foundation
Jornl o Physics: onerence Series PAPER OPEN AESS Mheicl Moeling o Hyroelsic Oscillions o he S n he Ple Resing on Psern Fonion To cie his ricle: L I Mogilevich e l 8 J. Phys.: on. Ser. 9 8 Vie he ricle
More informationTax Audit and Vertical Externalities
T Audi nd Vericl Eernliies Hidey Ko Misuyoshi Yngihr Ngoy Keizi Universiy Ngoy Universiy 1. Inroducion The vericl fiscl eernliies rise when he differen levels of governmens, such s he federl nd se governmens,
More informationtotal distance cov ered time int erval v = average speed (m/s)
Physics Suy Noes Lesson 4 Linear Moion 1 Change an Moion a. A propery common o eeryhing in he unierse is change. b. Change is so imporan ha he funamenal concep of ime woul be meaningless wihou i. c. Since
More information