ScienceDirect. Dynamic model of a mobile robot

Size: px
Start display at page:

Download "ScienceDirect. Dynamic model of a mobile robot"

Transcription

1 Avalable onlne at ScenceDect Poceda Engneeng 96 (014 ) Modellng of Mechancal and Mechatonc Systems MMaMS 014 Dynamc model of a moble obot Ján Kadoš* Faculty of Electcal Engneeng and Infomaton Technology, Slovak Unvesty of Technology, Ilkovčova 3, Batslava, Slovak Republc Abstact The contbuton pesents the dynamc model of a dffeental two-wheeled moble obot n the ont fame,.e. n the plane of angula poston of both the ght-hand sde wheel and the left-hand sde one. The am s to ceate an appopate MIMO plant model fo the pupose of the moble obot moton contol synthess. Based on the Lagangan fomalsm, the complete descpton of the second ode matx dffeental equaton (the dynamc model of the moble obot) s povded, ncludng the nfluence of netal couplng foces. A pa of wheel dvng toques epesents the nput of gven model. Addtonally, a decoupled dynamc model fo the obust moton contol mplementaton s pesented The The Authos. Authos. Publshed Publshed by Elseve by Elseve Ltd. Ths Ltd. s an open access atcle unde the CC BY-NC-ND lcense ( Pee-evew unde esponsblty of oganzng commttee of the Modellng of Mechancal and Mechatonc Systems MMaMS Pee-evew 014. unde esponsblty of oganzng commttee of the Modellng of Mechancal and Mechatonc Systems MMaMS 014 Keywods: Eule-Lagange s equaton; knetc enegy; nstantaneous cente of otaton; hozontal plane; decouplng 1. Intoducton The challengng ambton of a moble obot contol s the fast and accuate moton along the desed taectoy n the task plane gven by an actual applcaton (ndusty, agcultue, tanspot, household, posthetcs etc.). To keep both the hgh velocty of the moton and the elablty of the appled contol, t s nevtable to take the dynamcs of the movng mass of the moble obot nto account. The moton of the dffeental two-wheeled moble obot s pefomed by the wheel otaton descbed va the angula poston and t s tme devatves n the ont fame. On the othe hand, fom the use s pont of vew, the poston and velocty of the moble obot moton n the task fame (fo * Coespondng autho. Tel.: E-mal addess: an.kados@stuba.sk The Authos. Publshed by Elseve Ltd. Ths s an open access atcle unde the CC BY-NC-ND lcense ( Pee-evew unde esponsblty of oganzng commttee of the Modellng of Mechancal and Mechatonc Systems MMaMS 014 do: /.poeng

2 04 Ján Kadoš / Poceda Engneeng 96 ( 014 ) the smplcty, assume the moton wthn the hozontal plane) usually descbed by the plana Catesan coodnates s pefeed. The homogeneous tansfomaton [1] between the ont and task fames counts to tme ndependent (non-dynamc) tansfomatons esultng n non-lnea fowad and nvese knematcs (FKM fowad knematc model, IKM nvese knematc model) of the obot. Ths mples that the stuctue of the moble obot moton contol (as well as the moton contol of any knematc chan n geneal) can consst of the nne (dynamc) open contol loop (compsng the contol algothm and the contolled plant) pefomed n the ont fame, and the oute feedback loop wth the non-dynamc, non-lnea fowad and nvese tansfomatons between the task and ont fames (Fg. 1) []. In fgue, pr and p dr denote the poston and the desed poston vectos n the Catesan task fame, qr and q dr stand fo the angula poston and the desed angula poston vectos n the ont fame, and e qr epesents the eo vecto of the angula poston n the ont fame. Theefoe, the dynamc model of the moble obot n the ont fame (esultng n a contol-affne dynamc model [3, 4]) athe than n the task fame (non-lnea dynamc model) has to be syntheszed. Ths appoach allows avodng the poblem of nonunqueness and sngulaty [5] of the nvese knematcs soluton n the nne contol loop, tansfomng t to less complcated poblem of the desed taectoy fomng. Nomenclatue ICR nstantaneous cente of otaton of the moble obot C cente of gavty (cente of the obot body) 0 nstantaneous tunng adus of the obot taectoy θ C obot angula poston wth espect to ICR (obot oentaton) C angula velocty of the obot oentaton m C mass of the obot body C adus of the obot (cylndcal) body J C moment of neta of the obot body m mass of each of the obot wheels adus of each of the obot wheels J moment of neta of each of the obot wheels L dstance between the wheels (wheel spacng, bas) l C poston of the obot n the task plane v C velocty of the obot n the task plane l poston of the -th obot wheel n the task plane v velocty of the -th obot wheel n the task plane q angula poston of the -th obot wheel an element of the angula poston vecto q q angula velocty of the -th obot wheel an element of the angula velocty vecto q dvng toque fo the -th obot wheel an element of the dvng toque vecto τ τ p d q d e q Inne contol loop q p IKM FKM n the ont fame q IKM Fg. 1. Block dagam of the moton contol n the task fame.

3 Ján Kadoš / Poceda Engneeng 96 (014 ) l C, v C C,. C l, v l 1, v 1 ICR q,. q, τ 0 C m, J m C, J C m, J C q 1,. q 1, τ 1 L. Moble obot descpton Fg.. Schematc stuctue of the dffeental two-wheeled moble obot (top vew). Suppose the basc obot stuctue consstng of a cylndcal body and a pa of dffeentally dven sde wheels (Fg. ). Let = 1 denotes the ndex of the ght-hand sde wheel and = of the left-hand sde one. It s evdent, that the pa (l C, θ C) matches wth the numbe of degees of feedom of the moble obot n the task fame, and equally the pa (q 1, q ) descbes the obot DOFs n the ont fame. The uppe notaton yelds the basc expesson [6] fo the obot wheel poston L l q C, 0 C as well as the obot body poston and oentaton l C l l L l q (1) 1 1 q q, q q 1 l l C 1 () L L Consequently, we ae able to expess the coespondng veloctes of wheels v q 1, (3) and of the obot body v C v v 1 q q, 1 q q 1 v v C 1 (4) L L Undelne that expessons (3) and (4) ae the functons of elements q 1 and q of the angula velocty vecto q. Assumng the cylndcal shape of the moble obot body, ts moment of neta s gven by 1 JC mcc (5)

4 06 Ján Kadoš / Poceda Engneeng 96 ( 014 ) and smlaly s the moment of neta of each of the obot wheels 1 J m (6) We ae now eady to get the dynamc model of moble obot n the ont fame. 3. Dynamc model of the moble obot In MIMO dynamc system s analyss, the staghtfowad and poweful tool fo the dynamc model synthess epesents the Eule-Lagange method [1, 7] based on the system s total knetc and potental enegy concept. Lagange s enegy functon L stands fo the dffeence between the total knetc enegy E K and total potental enegy E P. Due to above mentoned smplfcaton moton wthn the hozontal plane (.e. the constant potental enegy) only the knetc enegy of a movng obot should be taken nto consdeaton. Futhemoe, the total knetc enegy E K of the dffeentally-dven moble obot s ndependent of ts poston n the task plane lkewse n the ont fame. Thus, fo the moble obot dynamcs descpton, the educed veson of the Eule-Lagange s equaton fo the -th ont coodnate q s gven by d dt E dq K Q (7) whee Q stands fo the genealzed non-consevatve (extenal) foce n the decton of the -th coodnate. Ths foce compses the dvng toque τ and the sum of load foces τ L (.e. dsspatve foces lke vscous fcton and ollng fcton). The esultant genealzed foce s then expessed by the dffeence Q (8) L The total knetc enegy of moble obot conssts of enegy of both the tanslatonal and the otatonal moton of the obot body and the obot wheels E K mcvc mv1 mv JC C Jq 1 Jq (9) Substtutng expessons (1) (6) to (9) yelds E K 3 m q q C m q q q q 1 C 1 1 (10) 4 L As mentoned above, the total knetc enegy of the moble obot s ndependent of the angula poston vecto q. Eule-Lagange s equaton (7) should be solved fo both degees of feedom,.e. fo q 1 and q, gvng the esultant system of two dffeental equatons of second ode 11q 1 1q 1 q q 1 1 L1 L (11) whee

5 Ján Kadoš / Poceda Engneeng 96 (014 ) C m mc, 1, (1) L epesents the moment of neta of the -th degee of feedom, C m 1 C,, 1,, L (13) s the couplng moment of neta between the DOFs (the poduct netal couplng foces Eule s foces), and coesponds to the undesable mutual q dq q dt d q, dt 1, (14) stands fo the angula acceleaton n the -th DOF. The angula poston q and angula velocty q ae the elements of the -th DOF s phase vecto q. Denote J R (15) the netal matx of the moble obot. Now, the system of equatons (11) can be ewtten n the fom of matx dffeental equaton of second ode Jq L (16) System of dffeental equatons (11) o (16) stands fo the contol-affne [3, 4] dynamc model of the moble obot n the ont fame. The soluton of ths system yelds the behavo of the obot wheel s angula poston n tme. To assue the desed taectoy of the moble obot, any contol algothm should geneate the coespondng dvng toque vecto τ. 4. Decoupled dynamc model To guaantee the desed behavo (pefect accuacy and fast dynamcs) of moble obot n pesence of load foces and vaable netal couplng foces (sgnal dstubances), the obust contol technques should be taken nto account. In geneal, the am of the obust contol s to keep the qualty of the contolled pocess despte the paametc and sgnal dstubances [8], pefeably wthout any adaptaton o on-lne dentfcaton. The only nfomaton about the dstubances s the estmated o computed ampltude (maxmal value). In the case of moble obot, the combnaton of the load toque and the netal couplng foce acts aganst the dvng toque. Denote τ Lmax the maxmal value of ths combnaton n the moble obot wokng plane. Ths maxmal value s dentcal also n the ont space L max max q const. q, q, q L (17) The constant (ndependent of the system s ont vaables) maxmal value n (17) mples, that usng (11) and (17), the decoupled dynamc model [9, 10, 11] of the moble obot fo the pupose of the obust contol algothm synthess can be ceated

6 08 Ján Kadoš / Poceda Engneeng 96 ( 014 ) q 1 1 q L1max L max (18) povded that once desgned fo the decoupled dynamc model (18), the esultant obust contol [9, 10, 11] guaantees the desed qualty of the eal moton contol system fo any combnaton of sgnal dstubances unde the condton L q Lmax (19) egadless of the fequency specta o the tme hstoy of dstubances. We can conclude that fom the pont of vew of the obust contol desgn, the dynamc model of a moble obot can be teated as a system of the pa of mutually ndependent double ntegatos (18). Smla appoach to the dynamc system analyss has been appled also n [1] and [13]. 5. Conclusons The pape shows two specfc featues of the moble obot dynamc model synthess, the desgne of the moton contol algothm should take nto account. The fst featue s that fo the moton contol n the task fame, the dynamc model n the ont fame can be appled. Ths yelds the contol-affne MIMO dynamc model n the fom of the system of two dffeental equatons of second ode. The second featue deals wth the decouplng of ths MIMO model to the pa of ndependent (SISO) double ntegato models, povded that the obust contol algothm fo the moble obot moton s unde consdeaton. The outcome of ths contbuton can essentally smplfy the desgn of a elable obust contol algothm n ognally complex and ntcate non-lnea MIMO contol task. Acknowledgements The wok pesented n ths contbuton has been suppoted by the Slovak Reseach and Development Agency unde the Gant No. APVV Refeences [1] A.J. Kovo, Fundamentals fo Contol of Robotc Manpulatos, Wley & Sons, New Yok, [] J. Kadoš, Specfc poblems of the obot moton contol n the task fame (n Slovak), Jounal EE 18 (01) 6 7. [3] A. Isdo, Nonlnea Contol Systems, thd ed., Spnge, London, [4] S. Sasty, Nonlnea Systems: Analyss, Stablty, and Contol, Spnge, New Yok, [5] M,W. Spong, M. Vdyasaga, Robot Dynamcs and Contol, Wley & Sons, Sngapoe, [6] G. Cook, Moble Robots (Navgaton, Contol and Remote Sensng), Wley & Sons, New Jesey, 011. [7] J. Kadoš, The smplfed dynamc model of a obot manpulato, 18 th Intenatonal Confeence Techncal Computng, Batslava, 010. [8] V.I. Utkn, Fst Stage of VSS: People and events, n: X. Yu, J.X. Xu (Eds.), Vaable Stuctue Systems: Towads the 1 st Centuy, Spnge, Beln, 00, pp [9] J. Kadoš, Smplfed obust contol of an anthopomophc leg, Poceedngs of the 19 th Intenatonal Confeence on Pocess Contol, Štbské Pleso, 013, pp [10] J. Kadoš, Robust command followng contol n the obot ont space, Poceedngs of the Intenatonal Confeence on Innovatve Technologes, In-Tech 01, Reka, 01, pp [11] J. Kadoš, Robust contol of a manpulato n the task space, 10 th Intenatonal Confeence Pocess Contol, Kouty nad Desnou, 01, pp. C014a-1 C014a-9. [1] M. Huba, P. Bsták, Z. Skachová, K. Žáková, Pedctve antwndup PI and PID-contolles based on I1 and I models wth dead tme, Poceedngs of the 6 th IEEE Medteanean Confeence on Contol and Systems, Algheo, 1998, pp [13] J. Han, Fom PID to actve dstubance eecton contol, IEEE Tansactons on Industal Electoncs, 56 (009)

PHYS 705: Classical Mechanics. Derivation of Lagrange Equations from D Alembert s Principle

PHYS 705: Classical Mechanics. Derivation of Lagrange Equations from D Alembert s Principle 1 PHYS 705: Classcal Mechancs Devaton of Lagange Equatons fom D Alembet s Pncple 2 D Alembet s Pncple Followng a smla agument fo the vtual dsplacement to be consstent wth constants,.e, (no vtual wok fo

More information

Energy in Closed Systems

Energy in Closed Systems Enegy n Closed Systems Anamta Palt palt.anamta@gmal.com Abstact The wtng ndcates a beakdown of the classcal laws. We consde consevaton of enegy wth a many body system n elaton to the nvese squae law and

More information

Part V: Velocity and Acceleration Analysis of Mechanisms

Part V: Velocity and Acceleration Analysis of Mechanisms Pat V: Velocty an Acceleaton Analyss of Mechansms Ths secton wll evew the most common an cuently pactce methos fo completng the knematcs analyss of mechansms; escbng moton though velocty an acceleaton.

More information

PHY126 Summer Session I, 2008

PHY126 Summer Session I, 2008 PHY6 Summe Sesson I, 8 Most of nfomaton s avalable at: http://nngoup.phscs.sunsb.edu/~chak/phy6-8 ncludng the sllabus and lectue sldes. Read sllabus and watch fo mpotant announcements. Homewok assgnment

More information

COMPLEMENTARY ENERGY METHOD FOR CURVED COMPOSITE BEAMS

COMPLEMENTARY ENERGY METHOD FOR CURVED COMPOSITE BEAMS ultscence - XXX. mcocd Intenatonal ultdscplnay Scentfc Confeence Unvesty of skolc Hungay - pl 06 ISBN 978-963-358-3- COPLEENTRY ENERGY ETHOD FOR CURVED COPOSITE BES Ákos József Lengyel István Ecsed ssstant

More information

Rotary motion

Rotary motion ectue 8 RTARY TN F THE RGD BDY Notes: ectue 8 - Rgd bod Rgd bod: j const numbe of degees of feedom 6 3 tanslatonal + 3 ota motons m j m j Constants educe numbe of degees of feedom non-fee object: 6-p

More information

EFFICIENT COMPUTATION OF THE GENERALIZED INERTIAL TENSOR OF ROBOTS BY USING THE GIBBS- APPELL EQUATIONS

EFFICIENT COMPUTATION OF THE GENERALIZED INERTIAL TENSOR OF ROBOTS BY USING THE GIBBS- APPELL EQUATIONS EFFICIEN CMPUAIN F HE ENERALIZED INERIAL ENSR F RBS BY USIN HE IBBS- APPELL EQUAINS Povenzano S. (*) Mata V.(**) Ceccaell M.(***) and Suñe J.L. (**) (*) Escuela de Ingeneía Mecánca Unvesdad de Los Andes

More information

Scalars and Vectors Scalar

Scalars and Vectors Scalar Scalas and ectos Scala A phscal quantt that s completel chaacteed b a eal numbe (o b ts numecal value) s called a scala. In othe wods a scala possesses onl a magntude. Mass denst volume tempeatue tme eneg

More information

Potential Fields in Cooperative Motion Control and Formations

Potential Fields in Cooperative Motion Control and Formations Pepaed by F.L. Lews and E. Stngu Updated: Satuday, Febuay 0, 03 Potental Felds n Coopeatve Moton Contol and Fomatons Add dscusson. Refe to efs.. Potental Felds Equaton Chapte Secton The potental s a scala

More information

Dynamics of Rigid Bodies

Dynamics of Rigid Bodies Dynamcs of Rgd Bodes A gd body s one n whch the dstances between consttuent patcles s constant thoughout the moton of the body,.e. t keeps ts shape. Thee ae two knds of gd body moton: 1. Tanslatonal Rectlnea

More information

Rigid Bodies: Equivalent Systems of Forces

Rigid Bodies: Equivalent Systems of Forces Engneeng Statcs, ENGR 2301 Chapte 3 Rgd Bodes: Equvalent Sstems of oces Intoducton Teatment of a bod as a sngle patcle s not alwas possble. In geneal, the se of the bod and the specfc ponts of applcaton

More information

DYNAMICS VECTOR MECHANICS FOR ENGINEERS: Kinematics of Rigid Bodies in Three Dimensions. Seventh Edition CHAPTER

DYNAMICS VECTOR MECHANICS FOR ENGINEERS: Kinematics of Rigid Bodies in Three Dimensions. Seventh Edition CHAPTER Edton CAPTER 8 VECTOR MECANCS FOR ENGNEERS: DYNAMCS Fednand P. Bee E. Russell Johnston, J. Lectue Notes: J. Walt Ole Teas Tech Unvest Knematcs of Rgd Bodes n Thee Dmensons 003 The McGaw-ll Companes, nc.

More information

Capítulo. Three Dimensions

Capítulo. Three Dimensions Capítulo Knematcs of Rgd Bodes n Thee Dmensons Mecánca Contents ntoducton Rgd Bod Angula Momentum n Thee Dmensons Pncple of mpulse and Momentum Knetc Eneg Sample Poblem 8. Sample Poblem 8. Moton of a Rgd

More information

Minimising Energy Consumption for Robot Arm Movement

Minimising Energy Consumption for Robot Arm Movement Mnmsng Enegy Consumpton fo obot Am Movement Abdullah Mohammed, Benad Schmdt, Lhu Wang, Lang Gao KH oyal Insttute of echnology, Bnellvägen 8, Stockholm, SE- Sweden, E-Mal: abdullah.mohammed@tm.kth.se, lhu.wang@p.kth.se

More information

Integral Vector Operations and Related Theorems Applications in Mechanics and E&M

Integral Vector Operations and Related Theorems Applications in Mechanics and E&M Dola Bagayoko (0) Integal Vecto Opeatons and elated Theoems Applcatons n Mechancs and E&M Ι Basc Defnton Please efe to you calculus evewed below. Ι, ΙΙ, andιιι notes and textbooks fo detals on the concepts

More information

1. A body will remain in a state of rest, or of uniform motion in a straight line unless it

1. A body will remain in a state of rest, or of uniform motion in a straight line unless it Pncples of Dnamcs: Newton's Laws of moton. : Foce Analss 1. A bod wll eman n a state of est, o of unfom moton n a staght lne unless t s acted b etenal foces to change ts state.. The ate of change of momentum

More information

3. A Review of Some Existing AW (BT, CT) Algorithms

3. A Review of Some Existing AW (BT, CT) Algorithms 3. A Revew of Some Exstng AW (BT, CT) Algothms In ths secton, some typcal ant-wndp algothms wll be descbed. As the soltons fo bmpless and condtoned tansfe ae smla to those fo ant-wndp, the pesented algothms

More information

Physics 1: Mechanics

Physics 1: Mechanics Physcs : Mechancs Đào Ngọc Hạnh Tâm Offce: A.503, Emal: dnhtam@hcmu.edu.vn HCMIU, Vetnam Natonal Unvesty Acknowledgment: Sldes ae suppoted by Pof. Phan Bao Ngoc Contents of Physcs Pat A: Dynamcs of Mass

More information

An Approach to Inverse Fuzzy Arithmetic

An Approach to Inverse Fuzzy Arithmetic An Appoach to Invese Fuzzy Athmetc Mchael Hanss Insttute A of Mechancs, Unvesty of Stuttgat Stuttgat, Gemany mhanss@mechaun-stuttgatde Abstact A novel appoach of nvese fuzzy athmetc s ntoduced to successfully

More information

Vibration Input Identification using Dynamic Strain Measurement

Vibration Input Identification using Dynamic Strain Measurement Vbaton Input Identfcaton usng Dynamc Stan Measuement Takum ITOFUJI 1 ;TakuyaYOSHIMURA ; 1, Tokyo Metopoltan Unvesty, Japan ABSTRACT Tansfe Path Analyss (TPA) has been conducted n ode to mpove the nose

More information

Chapter 8. Linear Momentum, Impulse, and Collisions

Chapter 8. Linear Momentum, Impulse, and Collisions Chapte 8 Lnea oentu, Ipulse, and Collsons 8. Lnea oentu and Ipulse The lnea oentu p of a patcle of ass ovng wth velocty v s defned as: p " v ote that p s a vecto that ponts n the sae decton as the velocty

More information

INVERSE DYNAMICS OF THE CINCINNATI-MILACRON WRIST ROBOT

INVERSE DYNAMICS OF THE CINCINNATI-MILACRON WRIST ROBOT INVERSE DYNMIS OF THE ININNTI-MILRON WRIST ROOT ŞTEFN STIU * Recusve matx elatons n dynamcs of the ncnnat-mlacon wst obot ae establshed n ths pape. The pototype of ths mechansm s a thee-degees-offeedom

More information

A New Approach for Deriving the Instability Potential for Plates Based on Rigid Body and Force Equilibrium Considerations

A New Approach for Deriving the Instability Potential for Plates Based on Rigid Body and Force Equilibrium Considerations Avalable onlne at www.scencedect.com Poceda Engneeng 4 (20) 4 22 The Twelfth East Asa-Pacfc Confeence on Stuctual Engneeng and Constucton A New Appoach fo Devng the Instablty Potental fo Plates Based on

More information

Exact Simplification of Support Vector Solutions

Exact Simplification of Support Vector Solutions Jounal of Machne Leanng Reseach 2 (200) 293-297 Submtted 3/0; Publshed 2/0 Exact Smplfcaton of Suppot Vecto Solutons Tom Downs TD@ITEE.UQ.EDU.AU School of Infomaton Technology and Electcal Engneeng Unvesty

More information

Modeling and Adaptive Control of a Coordinate Measuring Machine

Modeling and Adaptive Control of a Coordinate Measuring Machine Modelng and Adaptve Contol of a Coodnate Measung Machne Â. Yudun Obak, Membe, IEEE Abstact Although tadtonal measung nstuments can povde excellent solutons fo the measuement of length, heght, nsde and

More information

Review. Physics 231 fall 2007

Review. Physics 231 fall 2007 Reew Physcs 3 all 7 Man ssues Knematcs - moton wth constant acceleaton D moton, D pojectle moton, otatonal moton Dynamcs (oces) Enegy (knetc and potental) (tanslatonal o otatonal moton when detals ae not

More information

Design and Simulation of a Three-Phase Electrostatic Cylindrical Rotary Micromotor

Design and Simulation of a Three-Phase Electrostatic Cylindrical Rotary Micromotor Intenatonal Jounal of Advanced Botechnology and Reseach (IJBR) ISSN 0976-61, Onlne ISSN 78 599X, Vol-7, Specal Issue-Numbe5-July, 016, pp917-91 http://www.bpublcaton.com Reseach Atcle Desgn and Smulaton

More information

Mechanics Physics 151

Mechanics Physics 151 Mechancs Physcs 151 Lectue 18 Hamltonan Equatons of Moton (Chapte 8) What s Ahead We ae statng Hamltonan fomalsm Hamltonan equaton Today and 11/6 Canoncal tansfomaton 1/3, 1/5, 1/10 Close lnk to non-elatvstc

More information

Modelling of tangential vibrations in cylindrical grinding contact with regenerative chatter

Modelling of tangential vibrations in cylindrical grinding contact with regenerative chatter Modellng of tangental vbatons n cylndcal gndng contact wth egeneatve chatte Vel-Matt ävenpää, Lhong Yuan, Hessam Kalbas Shavan and asal Mehmood ampee Unvesty of echnology epatment of Engneeng esgn P.O.Bo

More information

Engineering Mechanics. Force resultants, Torques, Scalar Products, Equivalent Force systems

Engineering Mechanics. Force resultants, Torques, Scalar Products, Equivalent Force systems Engneeng echancs oce esultants, Toques, Scala oducts, Equvalent oce sstems Tata cgaw-hll Companes, 008 Resultant of Two oces foce: acton of one bod on anothe; chaacteed b ts pont of applcaton, magntude,

More information

Chapter I Matrices, Vectors, & Vector Calculus 1-1, 1-9, 1-10, 1-11, 1-17, 1-18, 1-25, 1-27, 1-36, 1-37, 1-41.

Chapter I Matrices, Vectors, & Vector Calculus 1-1, 1-9, 1-10, 1-11, 1-17, 1-18, 1-25, 1-27, 1-36, 1-37, 1-41. Chapte I Matces, Vectos, & Vecto Calculus -, -9, -0, -, -7, -8, -5, -7, -36, -37, -4. . Concept of a Scala Consde the aa of patcles shown n the fgue. he mass of the patcle at (,) can be epessed as. M (,

More information

19 The Born-Oppenheimer Approximation

19 The Born-Oppenheimer Approximation 9 The Bon-Oppenheme Appoxmaton The full nonelatvstc Hamltonan fo a molecule s gven by (n a.u.) Ĥ = A M A A A, Z A + A + >j j (883) Lets ewte the Hamltonan to emphasze the goal as Ĥ = + A A A, >j j M A

More information

On Maneuvering Target Tracking with Online Observed Colored Glint Noise Parameter Estimation

On Maneuvering Target Tracking with Online Observed Colored Glint Noise Parameter Estimation Wold Academy of Scence, Engneeng and Technology 6 7 On Maneuveng Taget Tacng wth Onlne Obseved Coloed Glnt Nose Paamete Estmaton M. A. Masnad-Sha, and S. A. Banan Abstact In ths pape a compehensve algothm

More information

Rotational Kinematics. Rigid Object about a Fixed Axis Western HS AP Physics 1

Rotational Kinematics. Rigid Object about a Fixed Axis Western HS AP Physics 1 Rotatonal Knematcs Rgd Object about a Fxed Axs Westen HS AP Physcs 1 Leanng Objectes What we know Unfom Ccula Moton q s Centpetal Acceleaton : Centpetal Foce: Non-unfom a F c c m F F F t m ma t What we

More information

Amplifier Constant Gain and Noise

Amplifier Constant Gain and Noise Amplfe Constant Gan and ose by Manfed Thumm and Wene Wesbeck Foschungszentum Kalsuhe n de Helmholtz - Gemenschaft Unvestät Kalsuhe (TH) Reseach Unvesty founded 85 Ccles of Constant Gan (I) If s taken to

More information

CSU ATS601 Fall Other reading: Vallis 2.1, 2.2; Marshall and Plumb Ch. 6; Holton Ch. 2; Schubert Ch r or v i = v r + r (3.

CSU ATS601 Fall Other reading: Vallis 2.1, 2.2; Marshall and Plumb Ch. 6; Holton Ch. 2; Schubert Ch r or v i = v r + r (3. 3 Eath s Rotaton 3.1 Rotatng Famewok Othe eadng: Valls 2.1, 2.2; Mashall and Plumb Ch. 6; Holton Ch. 2; Schubet Ch. 3 Consde the poston vecto (the same as C n the fgue above) otatng at angula velocty.

More information

Review of Vector Algebra and Vector Calculus Operations

Review of Vector Algebra and Vector Calculus Operations Revew of Vecto Algeba and Vecto Calculus Opeatons Tpes of vaables n Flud Mechancs Repesentaton of vectos Dffeent coodnate sstems Base vecto elatons Scala and vecto poducts Stess Newton s law of vscost

More information

Fundamental principles

Fundamental principles JU 07/HL Dnacs and contol of echancal sstes Date Da (0/08) Da (03/08) Da 3 (05/08) Da 4 (07/08) Da 5 (09/08) Da 6 (/08) Content Reve of the bascs of echancs. Kneatcs of gd bodes coodnate tansfoaton, angula

More information

Set of square-integrable function 2 L : function space F

Set of square-integrable function 2 L : function space F Set of squae-ntegable functon L : functon space F Motvaton: In ou pevous dscussons we have seen that fo fee patcles wave equatons (Helmholt o Schödnge) can be expessed n tems of egenvalue equatons. H E,

More information

Khintchine-Type Inequalities and Their Applications in Optimization

Khintchine-Type Inequalities and Their Applications in Optimization Khntchne-Type Inequaltes and The Applcatons n Optmzaton Anthony Man-Cho So Depatment of Systems Engneeng & Engneeng Management The Chnese Unvesty of Hong Kong ISDS-Kolloquum Unvestaet Wen 29 June 2009

More information

Chapter 23: Electric Potential

Chapter 23: Electric Potential Chapte 23: Electc Potental Electc Potental Enegy It tuns out (won t show ths) that the tostatc foce, qq 1 2 F ˆ = k, s consevatve. 2 Recall, fo any consevatve foce, t s always possble to wte the wok done

More information

A Study about One-Dimensional Steady State. Heat Transfer in Cylindrical and. Spherical Coordinates

A Study about One-Dimensional Steady State. Heat Transfer in Cylindrical and. Spherical Coordinates Appled Mathematcal Scences, Vol. 7, 03, no. 5, 67-633 HIKARI Ltd, www.m-hka.com http://dx.do.og/0.988/ams.03.38448 A Study about One-Dmensonal Steady State Heat ansfe n ylndcal and Sphecal oodnates Lesson

More information

Some Approximate Analytical Steady-State Solutions for Cylindrical Fin

Some Approximate Analytical Steady-State Solutions for Cylindrical Fin Some Appoxmate Analytcal Steady-State Solutons fo Cylndcal Fn ANITA BRUVERE ANDRIS BUIIS Insttute of Mathematcs and Compute Scence Unvesty of Latva Rana ulv 9 Rga LV459 LATVIA Astact: - In ths pape we

More information

Thermodynamics of solids 4. Statistical thermodynamics and the 3 rd law. Kwangheon Park Kyung Hee University Department of Nuclear Engineering

Thermodynamics of solids 4. Statistical thermodynamics and the 3 rd law. Kwangheon Park Kyung Hee University Department of Nuclear Engineering Themodynamcs of solds 4. Statstcal themodynamcs and the 3 d law Kwangheon Pak Kyung Hee Unvesty Depatment of Nuclea Engneeng 4.1. Intoducton to statstcal themodynamcs Classcal themodynamcs Statstcal themodynamcs

More information

Test 1 phy What mass of a material with density ρ is required to make a hollow spherical shell having inner radius r i and outer radius r o?

Test 1 phy What mass of a material with density ρ is required to make a hollow spherical shell having inner radius r i and outer radius r o? Test 1 phy 0 1. a) What s the pupose of measuement? b) Wte all fou condtons, whch must be satsfed by a scala poduct. (Use dffeent symbols to dstngush opeatons on ectos fom opeatons on numbes.) c) What

More information

One-dimensional kinematics

One-dimensional kinematics Phscs 45 Fomula Sheet Eam 3 One-dmensonal knematcs Vectos dsplacement: Δ total dstance taveled aveage speed total tme Δ aveage veloct: vav t t Δ nstantaneous veloct: v lm Δ t v aveage acceleaton: aav t

More information

New Condition of Stabilization of Uncertain Continuous Takagi-Sugeno Fuzzy System based on Fuzzy Lyapunov Function

New Condition of Stabilization of Uncertain Continuous Takagi-Sugeno Fuzzy System based on Fuzzy Lyapunov Function I.J. Intellgent Systems and Applcatons 4 9-5 Publshed Onlne Apl n MCS (http://www.mecs-pess.og/) DOI:.585/sa..4. New Condton of Stablzaton of Uncetan Contnuous aag-sugeno Fuzzy System based on Fuzzy Lyapunov

More information

Asymptotic Solutions of the Kinetic Boltzmann Equation and Multicomponent Non-Equilibrium Gas Dynamics

Asymptotic Solutions of the Kinetic Boltzmann Equation and Multicomponent Non-Equilibrium Gas Dynamics Jounal of Appled Mathematcs and Physcs 6 4 687-697 Publshed Onlne August 6 n ScRes http://wwwscpog/jounal/jamp http://dxdoog/436/jamp64877 Asymptotc Solutons of the Knetc Boltzmann Equaton and Multcomponent

More information

A NOVEL DWELLING TIME DESIGN METHOD FOR LOW PROBABILITY OF INTERCEPT IN A COMPLEX RADAR NETWORK

A NOVEL DWELLING TIME DESIGN METHOD FOR LOW PROBABILITY OF INTERCEPT IN A COMPLEX RADAR NETWORK Z. Zhang et al., Int. J. of Desgn & Natue and Ecodynamcs. Vol. 0, No. 4 (205) 30 39 A NOVEL DWELLING TIME DESIGN METHOD FOR LOW PROBABILITY OF INTERCEPT IN A COMPLEX RADAR NETWORK Z. ZHANG,2,3, J. ZHU

More information

Research Article A Robust Longitudinal Control Strategy for Safer and Comfortable Automotive Driving

Research Article A Robust Longitudinal Control Strategy for Safer and Comfortable Automotive Driving Reseach Jounal of Appled Scences, Engneeng and Technology 7(3): 506-5033, 014 DOI:10.1906/jaset.7.896 ISSN: 040-7459; e-issn: 040-7467 014 Mawell Scentfc Publcaton Cop. Submtted: Febuay 18, 014 Accepted:

More information

Distinct 8-QAM+ Perfect Arrays Fanxin Zeng 1, a, Zhenyu Zhang 2,1, b, Linjie Qian 1, c

Distinct 8-QAM+ Perfect Arrays Fanxin Zeng 1, a, Zhenyu Zhang 2,1, b, Linjie Qian 1, c nd Intenatonal Confeence on Electcal Compute Engneeng and Electoncs (ICECEE 15) Dstnct 8-QAM+ Pefect Aays Fanxn Zeng 1 a Zhenyu Zhang 1 b Lnje Qan 1 c 1 Chongqng Key Laboatoy of Emegency Communcaton Chongqng

More information

A. Thicknesses and Densities

A. Thicknesses and Densities 10 Lab0 The Eath s Shells A. Thcknesses and Denstes Any theoy of the nteo of the Eath must be consstent wth the fact that ts aggegate densty s 5.5 g/cm (ecall we calculated ths densty last tme). In othe

More information

Chapter 10 and elements of 11, 12 Rotation of Rigid Bodies

Chapter 10 and elements of 11, 12 Rotation of Rigid Bodies Chapte 10 and elements of 11, 1 Rotaton of Rgd Bodes What s a Rgd Body? Rotatonal Knematcs Angula Velocty ω and Acceleaton α Rotaton wth Constant Acceleaton Angula vs. Lnea Knematcs Enegy n Rotatonal Moton:

More information

2/24/2014. The point mass. Impulse for a single collision The impulse of a force is a vector. The Center of Mass. System of particles

2/24/2014. The point mass. Impulse for a single collision The impulse of a force is a vector. The Center of Mass. System of particles /4/04 Chapte 7 Lnea oentu Lnea oentu of a Sngle Patcle Lnea oentu: p υ It s a easue of the patcle s oton It s a vecto, sla to the veloct p υ p υ p υ z z p It also depends on the ass of the object, sla

More information

Correspondence Analysis & Related Methods

Correspondence Analysis & Related Methods Coespondence Analyss & Related Methods Ineta contbutons n weghted PCA PCA s a method of data vsualzaton whch epesents the tue postons of ponts n a map whch comes closest to all the ponts, closest n sense

More information

Optimal System for Warm Standby Components in the Presence of Standby Switching Failures, Two Types of Failures and General Repair Time

Optimal System for Warm Standby Components in the Presence of Standby Switching Failures, Two Types of Failures and General Repair Time Intenatonal Jounal of ompute Applcatons (5 ) Volume 44 No, Apl Optmal System fo Wam Standby omponents n the esence of Standby Swtchng Falues, Two Types of Falues and Geneal Repa Tme Mohamed Salah EL-Shebeny

More information

Thermoelastic Problem of a Long Annular Multilayered Cylinder

Thermoelastic Problem of a Long Annular Multilayered Cylinder Wold Jounal of Mechancs, 3, 3, 6- http://dx.do.og/.436/w.3.35a Publshed Onlne August 3 (http://www.scp.og/ounal/w) Theoelastc Poble of a Long Annula Multlayeed Cylnde Y Hsen Wu *, Kuo-Chang Jane Depatent

More information

Design and Analysis of a Three Degrees of Freedom Parallel Kinematic Machine

Design and Analysis of a Three Degrees of Freedom Parallel Kinematic Machine Desgn and Analyss of a Thee Degees of Feedom Paallel Knematc Machne by Xaoln Hu A Thess Submtted n Patal Fulfllment of the Requements fo the Degee of Maste of Appled Scence n The Faculty of Engneeng and

More information

The Forming Theory and the NC Machining for The Rotary Burs with the Spectral Edge Distribution

The Forming Theory and the NC Machining for The Rotary Burs with the Spectral Edge Distribution oden Appled Scence The Fomn Theoy and the NC achnn fo The Rotay us wth the Spectal Ede Dstbuton Huan Lu Depatment of echancal Enneen, Zhejan Unvesty of Scence and Technoloy Hanzhou, c.y. chan, 310023,

More information

1. Physics for Scientists and Engineers by Serway and Jewett. V.1, 9 th ed. Chapter 11.5, pp

1. Physics for Scientists and Engineers by Serway and Jewett. V.1, 9 th ed. Chapter 11.5, pp Page of 6 THE GYROSCOPE The setup s not connected to a compute. You cannot get measued values dectly fom the compute o ente them nto the lab PC. Make notes dung the sesson to use them late fo composng

More information

CSJM University Class: B.Sc.-II Sub:Physics Paper-II Title: Electromagnetics Unit-1: Electrostatics Lecture: 1 to 4

CSJM University Class: B.Sc.-II Sub:Physics Paper-II Title: Electromagnetics Unit-1: Electrostatics Lecture: 1 to 4 CSJM Unvesty Class: B.Sc.-II Sub:Physcs Pape-II Ttle: Electomagnetcs Unt-: Electostatcs Lectue: to 4 Electostatcs: It deals the study of behavo of statc o statonay Chages. Electc Chage: It s popety by

More information

Physics 207 Lecture 16

Physics 207 Lecture 16 Physcs 07 Lectue 6 Goals: Lectue 6 Chapte Extend the patcle odel to gd-bodes Undestand the equlbu of an extended object. Analyze ollng oton Undestand otaton about a fxed axs. Eploy consevaton of angula

More information

Multistage Median Ranked Set Sampling for Estimating the Population Median

Multistage Median Ranked Set Sampling for Estimating the Population Median Jounal of Mathematcs and Statstcs 3 (: 58-64 007 ISSN 549-3644 007 Scence Publcatons Multstage Medan Ranked Set Samplng fo Estmatng the Populaton Medan Abdul Azz Jeman Ame Al-Oma and Kamaulzaman Ibahm

More information

MHD Oscillatory Flow in a Porous Plate

MHD Oscillatory Flow in a Porous Plate Global Jounal of Mathematcal Scences: Theoy and Pactcal. ISSN 97-3 Volume, Numbe 3 (), pp. 3-39 Intenatonal Reseach Publcaton House http://www.phouse.com MHD Oscllatoy Flow n a Poous Plate Monka Kala and

More information

Physics 2A Chapter 11 - Universal Gravitation Fall 2017

Physics 2A Chapter 11 - Universal Gravitation Fall 2017 Physcs A Chapte - Unvesal Gavtaton Fall 07 hese notes ae ve pages. A quck summay: he text boxes n the notes contan the esults that wll compse the toolbox o Chapte. hee ae thee sectons: the law o gavtaton,

More information

Chapter 12 Equilibrium and Elasticity

Chapter 12 Equilibrium and Elasticity Chapte 12 Equlbum and Elastcty In ths chapte we wll defne equlbum and fnd the condtons needed so that an object s at equlbum. We wll then apply these condtons to a vaety of pactcal engneeng poblems of

More information

Formation Control with Leadership Alternation for Obstacle Avoidance

Formation Control with Leadership Alternation for Obstacle Avoidance Pepnts of the 8th IFAC Wold Congess Mlano (Italy) August 8 - Septembe, Fomaton Contol wth Leadeshp Altenaton fo Obstacle Avodance Jose M. V. Vlca Maco H. Tea Vald Gass J. Depatment of Electcal Engneeng,

More information

Contact, information, consultations

Contact, information, consultations ontact, nfomaton, consultatons hemsty A Bldg; oom 07 phone: 058-347-769 cellula: 664 66 97 E-mal: wojtek_c@pg.gda.pl Offce hous: Fday, 9-0 a.m. A quote of the week (o camel of the week): hee s no expedence

More information

Machine Learning 4771

Machine Learning 4771 Machne Leanng 4771 Instucto: Tony Jebaa Topc 6 Revew: Suppot Vecto Machnes Pmal & Dual Soluton Non-sepaable SVMs Kenels SVM Demo Revew: SVM Suppot vecto machnes ae (n the smplest case) lnea classfes that

More information

(8) Gain Stage and Simple Output Stage

(8) Gain Stage and Simple Output Stage EEEB23 Electoncs Analyss & Desgn (8) Gan Stage and Smple Output Stage Leanng Outcome Able to: Analyze an example of a gan stage and output stage of a multstage amplfe. efeence: Neamen, Chapte 11 8.0) ntoducton

More information

COLLEGE OF FOUNDATION AND GENERAL STUDIES PUTRAJAYA CAMPUS FINAL EXAMINATION TRIMESTER /2017

COLLEGE OF FOUNDATION AND GENERAL STUDIES PUTRAJAYA CAMPUS FINAL EXAMINATION TRIMESTER /2017 COLLEGE OF FOUNDATION AND GENERAL STUDIES PUTRAJAYA CAMPUS FINAL EXAMINATION TRIMESTER 1 016/017 PROGRAMME SUBJECT CODE : Foundaton n Engneeng : PHYF115 SUBJECT : Phscs 1 DATE : Septembe 016 DURATION :

More information

1. Starting with the local version of the first law of thermodynamics q. derive the statement of the first law of thermodynamics for a control volume

1. Starting with the local version of the first law of thermodynamics q. derive the statement of the first law of thermodynamics for a control volume EN10: Contnuum Mechancs Homewok 5: Alcaton of contnuum mechancs to fluds Due 1:00 noon Fda Febua 4th chool of Engneeng Bown Unvest 1. tatng wth the local veson of the fst law of themodnamcs q jdj q t and

More information

TEST-03 TOPIC: MAGNETISM AND MAGNETIC EFFECT OF CURRENT Q.1 Find the magnetic field intensity due to a thin wire carrying current I in the Fig.

TEST-03 TOPIC: MAGNETISM AND MAGNETIC EFFECT OF CURRENT Q.1 Find the magnetic field intensity due to a thin wire carrying current I in the Fig. TEST-03 TPC: MAGNETSM AND MAGNETC EFFECT F CURRENT Q. Fnd the magnetc feld ntensty due to a thn we cayng cuent n the Fg. - R 0 ( + tan) R () 0 ( ) R 0 ( + ) R 0 ( + tan ) R Q. Electons emtted wth neglgble

More information

Unconventional double-current circuit accuracy measures and application in twoparameter

Unconventional double-current circuit accuracy measures and application in twoparameter th IMEKO TC Wokshop on Techncal Dagnostcs dvanced measuement tools n techncal dagnostcs fo systems elablty and safety June 6-7 Wasaw Poland nconventonal double-cuent ccut accuacy measues and applcaton

More information

Course Outline. 1. MATLAB tutorial 2. Motion of systems that can be idealized as particles

Course Outline. 1. MATLAB tutorial 2. Motion of systems that can be idealized as particles Couse Outlne. MATLAB tutoal. Moton of systems that can be dealzed as patcles Descpton of moton, coodnate systems; Newton s laws; Calculatng foces equed to nduce pescbed moton; Devng and solvng equatons

More information

If there are k binding constraints at x then re-label these constraints so that they are the first k constraints.

If there are k binding constraints at x then re-label these constraints so that they are the first k constraints. Mathematcal Foundatons -1- Constaned Optmzaton Constaned Optmzaton Ma{ f ( ) X} whee X {, h ( ), 1,, m} Necessay condtons fo to be a soluton to ths mamzaton poblem Mathematcally, f ag Ma{ f ( ) X}, then

More information

Physics 11b Lecture #2. Electric Field Electric Flux Gauss s Law

Physics 11b Lecture #2. Electric Field Electric Flux Gauss s Law Physcs 11b Lectue # Electc Feld Electc Flux Gauss s Law What We Dd Last Tme Electc chage = How object esponds to electc foce Comes n postve and negatve flavos Conseved Electc foce Coulomb s Law F Same

More information

A Method of Reliability Target Setting for Electric Power Distribution Systems Using Data Envelopment Analysis

A Method of Reliability Target Setting for Electric Power Distribution Systems Using Data Envelopment Analysis 27 กก ก 9 2-3 2554 ก ก ก A Method of Relablty aget Settng fo Electc Powe Dstbuton Systems Usng Data Envelopment Analyss ก 2 ก ก ก ก ก 0900 2 ก ก ก ก ก 0900 E-mal: penjan262@hotmal.com Penjan Sng-o Psut

More information

iclicker Quiz a) True b) False Theoretical physics: the eternal quest for a missing minus sign and/or a factor of two. Which will be an issue today?

iclicker Quiz a) True b) False Theoretical physics: the eternal quest for a missing minus sign and/or a factor of two. Which will be an issue today? Clce Quz I egsteed my quz tansmtte va the couse webste (not on the clce.com webste. I ealze that untl I do so, my quz scoes wll not be ecoded. a Tue b False Theoetcal hyscs: the etenal quest fo a mssng

More information

Analytical and Numerical Solutions for a Rotating Annular Disk of Variable Thickness

Analytical and Numerical Solutions for a Rotating Annular Disk of Variable Thickness Appled Mathematcs 00 43-438 do:0.436/am.00.5057 Publshed Onlne Novembe 00 (http://www.scrp.og/jounal/am) Analytcal and Numecal Solutons fo a Rotatng Annula Ds of Vaable Thcness Abstact Ashaf M. Zenou Daoud

More information

Remember: When an object falls due to gravity its potential energy decreases.

Remember: When an object falls due to gravity its potential energy decreases. Chapte 5: lectc Potental As mentoned seveal tmes dung the uate Newton s law o gavty and Coulomb s law ae dentcal n the mathematcal om. So, most thngs that ae tue o gavty ae also tue o electostatcs! Hee

More information

24-2: Electric Potential Energy. 24-1: What is physics

24-2: Electric Potential Energy. 24-1: What is physics D. Iyad SAADEDDIN Chapte 4: Electc Potental Electc potental Enegy and Electc potental Calculatng the E-potental fom E-feld fo dffeent chage dstbutons Calculatng the E-feld fom E-potental Potental of a

More information

The Poisson bracket and magnetic monopoles

The Poisson bracket and magnetic monopoles FYST420 Advanced electodynamics Olli Aleksante Koskivaaa Final poject ollikoskivaaa@gmail.com The Poisson backet and magnetic monopoles Abstact: In this wok magnetic monopoles ae studied using the Poisson

More information

Event Shape Update. T. Doyle S. Hanlon I. Skillicorn. A. Everett A. Savin. Event Shapes, A. Everett, U. Wisconsin ZEUS Meeting, October 15,

Event Shape Update. T. Doyle S. Hanlon I. Skillicorn. A. Everett A. Savin. Event Shapes, A. Everett, U. Wisconsin ZEUS Meeting, October 15, Event Shape Update A. Eveett A. Savn T. Doyle S. Hanlon I. Skllcon Event Shapes, A. Eveett, U. Wsconsn ZEUS Meetng, Octobe 15, 2003-1 Outlne Pogess of Event Shapes n DIS Smla to publshed pape: Powe Coecton

More information

V. Principles of Irreversible Thermodynamics. s = S - S 0 (7.3) s = = - g i, k. "Flux": = da i. "Force": = -Â g a ik k = X i. Â J i X i (7.

V. Principles of Irreversible Thermodynamics. s = S - S 0 (7.3) s = = - g i, k. Flux: = da i. Force: = -Â g a ik k = X i. Â J i X i (7. Themodynamcs and Knetcs of Solds 71 V. Pncples of Ievesble Themodynamcs 5. Onsage s Teatment s = S - S 0 = s( a 1, a 2,...) a n = A g - A n (7.6) Equlbum themodynamcs detemnes the paametes of an equlbum

More information

Chapter Fifiteen. Surfaces Revisited

Chapter Fifiteen. Surfaces Revisited Chapte Ffteen ufaces Revsted 15.1 Vecto Descpton of ufaces We look now at the vey specal case of functons : D R 3, whee D R s a nce subset of the plane. We suppose s a nce functon. As the pont ( s, t)

More information

Physics Exam 3

Physics Exam 3 Physcs 114 1 Exam 3 The numbe of ponts fo each secton s noted n backets, []. Choose a total of 35 ponts that wll be gaded that s you may dop (not answe) a total of 5 ponts. Clealy mak on the cove of you

More information

Chapter IV Vector and Tensor Analysis IV.2 Vector and Tensor Analysis September 29,

Chapter IV Vector and Tensor Analysis IV.2 Vector and Tensor Analysis September 29, hapte I ecto and Tenso Analyss I. ecto and Tenso Analyss eptembe 9, 08 47 hapte I ecto and Tenso Analyss I. ecto and Tenso Analyss eptembe 9, 08 48 I. ETOR AND TENOR ANALYI I... Tenso functon th Let A

More information

COMPUTATIONAL METHODS AND ALGORITHMS Vol. I - Methods of Potential Theory - V.I. Agoshkov, P.B. Dubovski

COMPUTATIONAL METHODS AND ALGORITHMS Vol. I - Methods of Potential Theory - V.I. Agoshkov, P.B. Dubovski METHODS OF POTENTIAL THEORY.I. Agoshkov and P.B. Dubovsk Insttute of Numecal Mathematcs, Russan Academy of Scences, Moscow, Russa Keywods: Potental, volume potental, Newton s potental, smple laye potental,

More information

Rotating Disk Electrode -a hydrodynamic method

Rotating Disk Electrode -a hydrodynamic method Rotatng Dsk Electode -a hdodnamc method Fe Lu Ma 3, 0 ente fo Electochemcal Engneeng Reseach Depatment of hemcal and Bomolecula Engneeng Rotatng Dsk Electode A otatng dsk electode RDE s a hdodnamc wokng

More information

Transport Coefficients For A GaAs Hydro dynamic Model Extracted From Inhomogeneous Monte Carlo Calculations

Transport Coefficients For A GaAs Hydro dynamic Model Extracted From Inhomogeneous Monte Carlo Calculations Tanspot Coeffcents Fo A GaAs Hydo dynamc Model Extacted Fom Inhomogeneous Monte Calo Calculatons MeKe Ieong and Tngwe Tang Depatment of Electcal and Compute Engneeng Unvesty of Massachusetts, Amhest MA

More information

Physics 111 Lecture 11

Physics 111 Lecture 11 Physcs 111 ectue 11 Angula Momentum SJ 8th Ed.: Chap 11.1 11.4 Recap and Ovevew Coss Poduct Revsted Toque Revsted Angula Momentum Angula Fom o Newton s Second aw Angula Momentum o a System o Patcles Angula

More information

Please initial the statement below to show that you have read it

Please initial the statement below to show that you have read it EN40: Dynacs and Vbatons Fnal Exanaton Wednesday May 18 011 School of Engneeng own Unvesty NAME: Geneal Instuctons No collaboaton of any knd s petted on ths exanaton. You ay use double sded pages of efeence

More information

Chapter IV Vector and Tensor Analysis IV.2 Vector and Tensor Analysis September 23,

Chapter IV Vector and Tensor Analysis IV.2 Vector and Tensor Analysis September 23, hapte I ecto and Tenso Analyss I. ecto and Tenso Analyss eptembe, 07 47 hapte I ecto and Tenso Analyss I. ecto and Tenso Analyss eptembe, 07 48 I. ETOR AND TENOR ANALYI I... Tenso functon th Let A n n

More information

P 365. r r r )...(1 365

P 365. r r r )...(1 365 SCIENCE WORLD JOURNAL VOL (NO4) 008 www.scecncewoldounal.og ISSN 597-64 SHORT COMMUNICATION ANALYSING THE APPROXIMATION MODEL TO BIRTHDAY PROBLEM *CHOJI, D.N. & DEME, A.C. Depatment of Mathematcs Unvesty

More information

Advanced Robust PDC Fuzzy Control of Nonlinear Systems

Advanced Robust PDC Fuzzy Control of Nonlinear Systems Advanced obust PDC Fuzzy Contol of Nonlnea Systems M Polanský Abstact hs pape ntoduces a new method called APDC (Advanced obust Paallel Dstbuted Compensaton) fo automatc contol of nonlnea systems hs method

More information

Learning the structure of Bayesian belief networks

Learning the structure of Bayesian belief networks Lectue 17 Leanng the stuctue of Bayesan belef netwoks Mlos Hauskecht mlos@cs.ptt.edu 5329 Sennott Squae Leanng of BBN Leanng. Leanng of paametes of condtonal pobabltes Leanng of the netwok stuctue Vaables:

More information

Unknown Input Based Observer Synthesis for a Polynomial T-S Fuzzy Model System with Uncertainties

Unknown Input Based Observer Synthesis for a Polynomial T-S Fuzzy Model System with Uncertainties Unknown Input Based Obseve Synthess fo a Polynomal -S Fuzzy Model System wth Uncetantes Van-Phong Vu Wen-June Wang Fellow IEEE Hsang-heh hen Jacek M Zuada Lfe Fellow IEEE Abstact hs pape poposes a new

More information

4 Recursive Linear Predictor

4 Recursive Linear Predictor 4 Recusve Lnea Pedcto The man objectve of ths chapte s to desgn a lnea pedcto wthout havng a po knowledge about the coelaton popetes of the nput sgnal. In the conventonal lnea pedcto the known coelaton

More information

Observer Design for Takagi-Sugeno Descriptor System with Lipschitz Constraints

Observer Design for Takagi-Sugeno Descriptor System with Lipschitz Constraints Intenatonal Jounal of Instumentaton and Contol Systems (IJICS) Vol., No., Apl Obseve Desgn fo akag-sugeno Descpto System wth Lpschtz Constants Klan Ilhem,Jab Dalel, Bel Hadj Al Saloua and Abdelkm Mohamed

More information