Optimal Path Planning for Flexible Redundant Robot Manipulators

Size: px
Start display at page:

Download "Optimal Path Planning for Flexible Redundant Robot Manipulators"

Transcription

1 25 WSEAS In. Conf. on DYNAMICAL SYSEMS and CONROL, Venice, Ialy, November 2-4, 25 (pp ) Opimal Pah Planning for Flexible Redundan Robo Manipulaors H. HOMAEI, M. KESHMIRI Deparmen of Mechanical Engineering Isfahan Universiy of echnology IRAN Absrac: - Vibraion is one of he mos imporan resources of error in moion of ip of flexible robo manipulaors. Alhough much work has been done in he design of conrollers for flexible manipulaors o follow a specified ip rajecory, i has been done a lile work in rajecory planning iself. For redundan robo manipulaors, rajecory planning can be accomplished wih he aim of opimizing some objecive funcions while racing along a given ip rajecory. In he presen work, he opimal rajecory-planning problem for a flexible redundan manipulaor will be formulaed as a wo poin boundary value problem (PBV) by globally minimizing he elasic deformaion of flexible links during he moion. Key-Words: Manipulaor - Redundan - Flexible - Vibraion - Opimizaion - Pah Planning 1 Inroducion Precise conrol of a robo manipulaor is an imporan aspec of robo performance. In he pas, his has led o he design of heavy and siff links and large moors. Hence mos exising manipulaors have very low payload o oal weigh raio. However, o increase produciviy by fas moion and o have less energy consumpion, robo arms are required o have ligh and consequenly flexible srucures. he main difficuly which arises from flexible srucures is vibraion. his vibraion leads o an error in moion of he manipulaor ip along a given rajecory and especially afer reaching he manipulaor o he desired end goal poin. Since his vibraion needs addiional seling ime before any ask can be begun, an effecive mehod should be employed o reduce he vibraion and srain energy of he robo manipulaor. Alhough here has been much work in he area of conrolling flexible manipulaors o follow a desired ip rajecory [1], lile work has been done in choosing he rajecory iself. Such a choice is necessary eiher for poin o poin moion or for resolving he redundancy of robos wih more degrees of freedom han necessary o follow he given ip rajecory. Meirowich and Chen used LQR conrol o reduce he elasic disurbance for a flexible redundan robo [2]. Eisler e al. considered join orque bounds and deermined minimum ime rajecories o minimize ip racking error for a flexible redundan robo [3]. However hese works have been based on minimizing a cos funcion independen of elasic deflecions and velociies. Redundancy, which is widely used in robo manipulaors o achieve addiional performance while racing a given end-effecor rajecory, can be used for vibraion reducion of flexible robo manipulaors. Shigang analyzed he effecs of iniial configuraion in vibraion reducion of flexible robos wih kinemaic redundancy [4]. Alhough he problem of opimizing he join moion for rigid, redundan manipulaors has already received much aenion from researchers, here has been a lile work concerning flexible redundan manipulaors. Opimal pah generaion by minimizing an objecive funcion evaluaed locally, "local opimizaion", involves less complexiy and requires less compuaional effor, while minimizing an objecive funcion evaluaed along he enire pah, "global opimizaion", resuls in more complexiy, bu more desirable manipulaor performance. In he previous works, some mehods have been developed on opimal pah generaion for flexible redundan manipulaors by local opimizaion of some objecive funcions [5], and in he presen work we will propose a mehod for opimal pah generaion by global minimizaion of elasic deformaion along a specified pah. he approach developed in his paper formulaes he rajecory planning problem for a flexible redundan manipulaor by a wo poin boundary value problem (PBV) where globally minimizes he elasic deformaion during he moion. he remainder of he paper is organized as follows. Firs, he equaions of moion for a general flexible robo manipulaor are briefly presened. he formulaion of opimal rajecory planning will be developed in he hird secion. hen differen numerical schemes for solving wo-poin boundary value problems will be defined and finally a numerical example will be solved by he presened formulaion a he end.

2 25 WSEAS In. Conf. on DYNAMICAL SYSEMS and CONROL, Venice, Ialy, November 2-4, 25 (pp ) 2 Dynamic Modeling Dynamic equaions of a general flexible robo can be derived using differen mehods such as finie elemen or assumed mode mehods. I can be shown ha dynamic equaions for a flexible robo manipulaor can be wrien as: M ( θ,φ) & θ + M ( θ,φ) Φ&& + d ( θ,θ,φ & , Φ& ) = τ (1) M ( θ,φ) && θ + M ( θ,φ) Φ&& + d ( θ,θ,φ & , Φ& ) = (2) Where θ, θ & and & θ are vecors of join angles, velociies and acceleraion, Φ, Φ & and Φ & are vecors of generalized coordinaes, velociies and acceleraions describing deformaion behavior of he flexible links and τ is he acuaor orque vecor. d 1 and d 2 are erms involving damping, siffness, cenrifugal, corilois of rigid and flexible coupling, and graviaional effecs. 3 rajecory Opimizaion For redundan manipulaors he number of joins is more han he number of degrees of freedom ha is required o follow a desired ip rajecory. In opimal pah generaion approaches, he rajecory of joins is designed o opimize some objecive funcion along he enire rajecory. In his paper we will find he opimal rajecory of a redundan, flexible robo by globally minimizing a funcion of flexible coordinaes in he form of: g ( Φ) = Φ CΦ (3) where C is a posiive definie weigh marix. o minimize a funcion evaluaed along he enire pah, he sandard mehods of calculus of variaions such as Hamilonian approach for opimal conrol problems may be employed. Opimal rajecory of he manipulaor is deermined by globally minimizing g (Φ), subjec o some consrains. he firs consrain is he moion of he ip of he manipulaor along a specified rajecory: X e = X() (4) Also we can see ha (2) represens anoher consrain. Essenially his is a differenial consrain relaing rigid acceleraion & θ and elasic acceleraion Φ &. I should be noed ha for general manipulaors his consrain is non inegrable. In moion planning problems, (1) is no a consrain because he orque τ is no considered in hese problems, bu only he moion of joins is deermined for a specified ip rajecory and once he acceleraions and he curren sae are known, (1) may be employed o obain acuaor orques. I is apparen from (2) ha elasic coordinaes are no conrolled direcly. hus he problem of moion planning is o calculae join acceleraion vecor & θ which globally opimizes some objecive funcions such as (3), subjec o he differenial consrain (2), ip rajecory consrain (4) and suiable boundary condiions: s. 12 ( θ,φ) && θ + M 22( θ,φ) Φ&& + h2( θ,θ,φ &, Φ& ) = min J = Φ CΦ M, (5) X e = X() I should be noed ha he ip posiion of he manipulaor is a funcion of join angles; In oher words he consrain (4) can be wrien as: X e = h( θ) = X( ) (6) he sae of he manipulaor can be defined as: x = [ θ, θ&, Φ, Φ& ] (7) As can be seen, (2) is a differenial consrain of degree 2. We can sae he consrains (2) and (6) as a differenial consrain of degree 1 wih a suiable ransformaion. hen he consrains of he problem can be summarized by he sae dynamics equaion: x & = f ( x, (8) where (2) and (6) have been used o obain & θ and Φ & as funcions of x and a conrol vecor u. If he number of join angles is n, he number of elasic coordinaes is r and X e is a vecor of dimension s, (2) and (6) represen r + s consrain equaions. We can differeniae (6) wice o have: J ( θ) & θ = X&& ( ) J& ( θ ) θ& (9) where J is he Jacobian marix: h( θ) J( θ) = (1) θ I is clear ha (2) and (9) are linear wih respec o & θ and Φ &, and may be used o obain hem as funcions of x. I is eviden ha we have n + r unknowns bu r + s equaions, so if we define: u = [ && θ, && 1 θ2,..., & θ n s ] (11) where n s is he number of degrees of robo redundancy, by his definiion i will be possible o sae & θ and Φ & as funcions of x and u, and as a consequence he derivaive of he sae vecor x can be saed as a funcion of x and u as in (8). Anoher imporan problem ha we should consider is boundary condiions. In he presen problem we wan o obain he opimal join rajecory from known iniial condiions. In oher word he vecor x is assumed o be known a ime. herefore we can sae he problem by: f min J = F( x, d s. x & = f ( x,, x ( ) = x (12)

3 25 WSEAS In. Conf. on DYNAMICAL SYSEMS and CONROL, Venice, Ialy, November 2-4, 25 (pp ) I should be noed ha in he presen case he final ime f is fixed. Following he LQR heory developed for opimal conrol [6], we can choose a general form for F: F ( x, = x Qx + u Ru (13) Where Q and R are consan weighing marices, Q is a posiive semi-definie and R is a posiive definie marix. If our aim is minimizaion of some objecive funcion in he form of (5), we should define Q as he followings: Q = diag(,, C, ) (14) While if our aim is minimizing he join velociies along he enire pah we can choose: Q = diag(, C,, ) (15) o obain differenial equaions governing he opimal rajecory, he differenial consrain is incorporaed ino he problem formulaion by augmening F using he Lagrange muliplier mehod. So we can sae (12) by min J = f [ F( x, + λ ( f ( x, x& )] d (16) Where λ is he vecor of Lagrange mulipliers or cosaes. For an opimal rajecory we should have: δ J = (17) δ J can be derived from (16) and o obain differenial equaions and associaed boundary condiions we should have: f F (, ) = f x u δ J [( + λ + λ& ) δx + δλ x x F (, ) f x u f + ( + λ ) δu] d λ δx = ( f ( x, x& ) (18) hus he equaions governing he opimal rajecory will be developed as: f λ& F = λ x x (19) x & = f ( x, (2) F f ( x, u = λ f ( x, 2u R = λ (21) Conrol vecor u can be obained as a funcion of x and λ from he las equaion because R is a nonsingular marix and f is a linear funcion of u. So we can inegrae (19) and (2) o obain saes and cosaes from iniial ime o final ime f. Also he boundary condiions saisfy he expression: f λ δ x = (22) I should be noed ha he sae vecor x is unknown a final ime f, so (22) leads o: x ( ) = x, λ = (23) f As can be seen he problem of opimal rajecory planning for a flexible redundan robo manipulaor racing along a specified ip rajecory wih minimum elasic deflecions leaded o a wo-poin boundary value problem. he soluion of he wopoin boundary value problem defined by (19) and (2) associaed wih he given iniial and final condiions for saes and cosaes (23) will yield he opimal rajecory of he manipulaor. Noe ha by choosing R o be a posiive definie marix, we will have he posiive definie Hessian and consequenly he soluion derived by he aforemenioned scheme will be a unique global minimum. Also i should be noed ha when he aim is no minimizaion of u, as for he presen problem, R should no be made very large o affec he soluion. 4 Numerical Mehods here are some mehods for solving wo-poin boundary value problems. he finie-difference mehod, shooing mehod, Rayleigh-Riz mehod, collocaion mehod and dynamic programming [7] are some of hese mehods. he imporan difference beween hese mehods is in how well he differenial equaions and he boundary condiions of he problem can be saisfied. In finie-difference mehods he derivaives in he differenial equaions of he problem are approximaed by finie differences beween he soluion a discree imes [8]. In some problems as for he presen case o have an accurae soluion wih finie-difference mehod a very high number of discree imes may be required. In shooing mehods he differenial equaions of he problem are solved accuraely and he soluion is obained wihin inegraion olerances. his is done by iniially approximaing some of he boundary condiions and an ieraive mehod is used o updae he iniial approximaions o converge o a soluion which saisfies he given boundary condiions. he error in he known boundary condiions expressed as a funcion of he iniial approximaions can be used o modify he iniial approximaions of he boundary condiions and a nonlinear opimizaion mehod is used o updae he iniial guesses o reduce he error. In Rayleigh-Riz mehod he soluion of a problem is approximaed by a linear combinaion of some basis funcions [8], so a good experience in choosing he appropriae basis funcions is very essenial o obain an accurae soluion by his mehod. Collocaion mehod is a mehod similar o he Rayleigh-Riz mehod in which dynamics consrains are saisfied a discree imes. Comparing hese mehods, we employed collocaion mehod for solving he wo poin

4 25 WSEAS In. Conf. on DYNAMICAL SYSEMS and CONROL, Venice, Ialy, November 2-4, 25 (pp ) boundary value problem described in he previous secion. 5 Numerical Example As an example we consider opimal pah generaion for a wo degree of freedom planar manipulaor (Fig. 1) wih he aim of minimizaion of he elasic deflecions of he flexible links along he enire pah. he ip of he manipulaor is o move along a rajecory consrained by he equaion: x = 2cos() (24) he above consrain can be wrien in he form of (6) as: x = l1 cos( θ 1) + l2 cos( θ1 + θ2) = 2cos( ) (25) We have a wo degree of freedom manipulaor ha should move along a rajecory consrained by only one consrain, so we have a robo wih 1 degree of redundancy. Link 1 is a rigid link of lengh 2 m and link 2 is a flexible link of lengh 4 m, Young's modulus E=71 GPa and momen of ineria of he cross secion I= m 4. wo links have he same densiy of 271 kg/m 3. A dynamic model for his manipulaor can be developed using finie elemen or assumed mode mehod. Here, only ransverse displacemen of he flexible link 2 is considered in he model. In order o make a comparison beween he resuls, we have accomplished rajecory planning for wo differen problems. In he firs problem, an objecive cos funcion of elasic deflecions is used o minimize elasic vibraions along he enire pah, while in he second problem we have used a cos funcion of join velociies in he form of: f 2 2 min J = ( & θ & + ) d (26) y 1 θ2 θ 2 For he firs problem marix Q is obained from (14) and for he second problem i is obained from (15) and ideniy marix wih appropriae dimension may be subsiued for C in (14) and (15). In he presen example, vecor u is a one dimensional vecor, because we have one degree of redundancy. So he one dimensional weigh marix R is made posiive definie bu no large enough o affec he soluion. Here we consider: R= 1-6 (26) Now we should specify he iniial condiions x from which he opimal rajecory will be iniiaed, we consider: θ1() = π / 3 θ2() =.27 (27) θ & = Φ = Φ& = I is apparen ha he iniial condiions for join angles saisfy he consrain (25). Also he iniial join velociies, elasic deflecions and elasic raes are considered o be zero. For he firs problem he error in racking he specified pah (24) is shown in Fig. 2. I is seen ha he error is very small and he ip of he manipulaor moves along he specified pah wih an accepable accuracy. he elasic deflecion of he end poin of link 2 is shown in Fig. 3 and as is shown, he maximum ip deflecion is less han.4% of he lengh of he flexible link 2. Also he configuraions of he manipulaor as racing he specified rajecory are shown in Fig. 4. he amoun of he cos funcion of elasic deflecions (J 1 ) and he cos funcion of join velociies (J 2 ) calculaed in his problem are: J 1 = e-11 J 2 =.99 For he second problem he error in racking he specified pah (24) is shown in Fig. 5. I is seen ha he ip of he manipulaor moves along he specified pah wih a small error. he elasic deflecion of he end poin of link 2 is shown in Fig. 6. he maximum ip deflecion is more han 1% of he lengh of he link 2. he amoun of he cos funcion of elasic deflecions (J 1 ) and he cos funcion of join velociies (J 2 ) calculaed in his problem are: J 1 =.15 J 2 =.959 θ 1 Fig. 1 A wo link flexible manipulaor x

5 25 WSEAS In. Conf. on DYNAMICAL SYSEMS and CONROL, Venice, Ialy, November 2-4, 25 (pp ) 4 x x 1-8 racking error (m) racking error (m) ime (s) Fig. 2 Error in racking he desired pah (firs problem) ime (s) Fig. 5 Error in racking he desired pah (second problem) 5 x Elasic deflecion (m) -5-1 Elasic deflecion (m) ime (s) Fig. 3 Elasic deflecion of he end poin of link 2 (firs problem) y ime (s) Fig. 6 Elasic deflecion of he end poin of link 2 (second problem) I is apparen ha as we expeced J 1 calculaed in he firs problem is less han J 1 obained in he second problem, Also he amoun of he cos funcion J 2 in he second problem is less han J 2 obained in he firs problem x Fig. 4 Manipulaor configuraions (firs problem) 6 Conclusion An approach for solving he opimal pah planning problem for a flexible redundan robo manipulaor has been presened. he opimal pah has been generaed by globally minimizing an objecive cos funcion dependen on he elasic deformaions of he flexible links of he manipulaor. he presened mehodology leaded o a wo-poin boundary value problem and he collocaion mehod has been employed for solving his problem. he efficiency of he proposed approach has been shown by a simple numerical example of opimal pah planning for a wo degree of freedom manipulaor wih link flexi-

6 25 WSEAS In. Conf. on DYNAMICAL SYSEMS and CONROL, Venice, Ialy, November 2-4, 25 (pp ) biliy. his approach is applicable o a general flexible redundan manipulaor for minimizaion of differen objecive funcions. References: [1] W. J. Book. Srucural flexibiliy of moion sysems in he space environmen, IEEE ransacions on Roboics and Auomaion, vol. 9, no. 5, pp , Ocober [2] L. Meirowich and Y. Chen. rajecory and conrol opimizaion for flexible space robos, Journal of Guidance, Conrol, and Dynamics, vol. 18, no. 3, pp , May-June [3] G. R. Eisler, R. D. Robine, D. J. Segalman, and J. D. Feddema. Approximae opimal rajecories for flexible-link manipulaor slewing using recursive quadraic programming, ransacions of he ASME, Journal of Dynamic Sysems, Measuremen and conrol, vol. 115, pp , Sepember [4] Y. Shigang. Weak-vibraion configuraions for flexible robo manipulaors wih kinemaic redundancy, Journal of Mechanism and Machine heory, vol. 35, pp , 2. [5] X. Zhang, Y. Q. Yu. Moion conrol of flexible robo manipulaors via opimizing redundan configuraions. Journal of Mechanism and Machine heory, vol. 36, pp , 21. [6] S. M. Shinners. Modern Conrol Sysem heory and Design. John Wiley & Sons, 2nd ediion, [7] D. P. Bersekas. Dynamic Programming and Opimal Conrol. Ahena Scienific, 2nd ediion, [8] R. L. Burden and J. D. Faires. Numerical analysis. PWS-Ken Publishing, Boson, 6h ediion, 1997.

Physics 235 Chapter 2. Chapter 2 Newtonian Mechanics Single Particle

Physics 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 information

3.1.3 INTRODUCTION TO DYNAMIC OPTIMIZATION: DISCRETE TIME PROBLEMS. A. The Hamiltonian and First-Order Conditions in a Finite Time Horizon

3.1.3 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 information

Lecture 20: Riccati Equations and Least Squares Feedback Control

Lecture 20: Riccati Equations and Least Squares Feedback Control 34-5 LINEAR SYSTEMS Lecure : Riccai Equaions and Leas Squares Feedback Conrol 5.6.4 Sae Feedback via Riccai Equaions A recursive approach in generaing he marix-valued funcion W ( ) equaion for i for he

More information

where the coordinate X (t) describes the system motion. X has its origin at the system static equilibrium position (SEP).

where 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 information

Structural Dynamics and Earthquake Engineering

Structural 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 information

4.6 One Dimensional Kinematics and Integration

4.6 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 information

Finite Element Analysis of Structures

Finite 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 information

Notes on Kalman Filtering

Notes on Kalman Filtering Noes on Kalman Filering Brian Borchers and Rick Aser November 7, Inroducion Daa Assimilaion is he problem of merging model predicions wih acual measuremens of a sysem o produce an opimal esimae of he curren

More information

10. State Space Methods

10. 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 information

Simulation-Solving Dynamic Models ABE 5646 Week 2, Spring 2010

Simulation-Solving Dynamic Models ABE 5646 Week 2, Spring 2010 Simulaion-Solving Dynamic Models ABE 5646 Week 2, Spring 2010 Week Descripion Reading Maerial 2 Compuer Simulaion of Dynamic Models Finie Difference, coninuous saes, discree ime Simple Mehods Euler Trapezoid

More information

Some Basic Information about M-S-D Systems

Some 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 information

WEEK-3 Recitation PHYS 131. of the projectile s velocity remains constant throughout the motion, since the acceleration a x

WEEK-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 information

Differential Equations

Differential 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 information

Class Meeting # 10: Introduction to the Wave Equation

Class Meeting # 10: Introduction to the Wave Equation MATH 8.5 COURSE NOTES - CLASS MEETING # 0 8.5 Inroducion o PDEs, Fall 0 Professor: Jared Speck Class Meeing # 0: Inroducion o he Wave Equaion. Wha is he wave equaion? The sandard wave equaion for a funcion

More information

v A Since the axial rigidity k ij is defined by P/v A, we obtain Pa 3

v 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 information

Modal identification of structures from roving input data by means of maximum likelihood estimation of the state space model

Modal identification of structures from roving input data by means of maximum likelihood estimation of the state space model Modal idenificaion of srucures from roving inpu daa by means of maximum likelihood esimaion of he sae space model J. Cara, J. Juan, E. Alarcón Absrac The usual way o perform a forced vibraion es is o fix

More information

SZG Macro 2011 Lecture 3: Dynamic Programming. SZG macro 2011 lecture 3 1

SZG Macro 2011 Lecture 3: Dynamic Programming. SZG macro 2011 lecture 3 1 SZG Macro 2011 Lecure 3: Dynamic Programming SZG macro 2011 lecure 3 1 Background Our previous discussion of opimal consumpion over ime and of opimal capial accumulaion sugges sudying he general decision

More information

SUFFICIENT CONDITIONS FOR EXISTENCE SOLUTION OF LINEAR TWO-POINT BOUNDARY PROBLEM IN MINIMIZATION OF QUADRATIC FUNCTIONAL

SUFFICIENT 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 information

Unsteady Flow Problems

Unsteady Flow Problems School of Mechanical Aerospace and Civil Engineering Unseady Flow Problems T. J. Craf George Begg Building, C41 TPFE MSc CFD-1 Reading: J. Ferziger, M. Peric, Compuaional Mehods for Fluid Dynamics H.K.

More information

Navneet Saini, Mayank Goyal, Vishal Bansal (2013); Term Project AML310; Indian Institute of Technology Delhi

Navneet Saini, Mayank Goyal, Vishal Bansal (2013); Term Project AML310; Indian Institute of Technology Delhi Creep in Viscoelasic Subsances Numerical mehods o calculae he coefficiens of he Prony equaion using creep es daa and Herediary Inegrals Mehod Navnee Saini, Mayank Goyal, Vishal Bansal (23); Term Projec

More information

From Particles to Rigid Bodies

From 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 information

Vehicle Arrival Models : Headway

Vehicle Arrival Models : Headway Chaper 12 Vehicle Arrival Models : Headway 12.1 Inroducion Modelling arrival of vehicle a secion of road is an imporan sep in raffic flow modelling. I has imporan applicaion in raffic flow simulaion where

More information

Optimal Control of Dc Motor Using Performance Index of Energy

Optimal Control of Dc Motor Using Performance Index of Energy American Journal of Engineering esearch AJE 06 American Journal of Engineering esearch AJE e-issn: 30-0847 p-issn : 30-0936 Volume-5, Issue-, pp-57-6 www.ajer.org esearch Paper Open Access Opimal Conrol

More information

BU Macro BU Macro Fall 2008, Lecture 4

BU Macro BU Macro Fall 2008, Lecture 4 Dynamic Programming BU Macro 2008 Lecure 4 1 Ouline 1. Cerainy opimizaion problem used o illusrae: a. Resricions on exogenous variables b. Value funcion c. Policy funcion d. The Bellman equaion and an

More information

4.1.1 Mindlin plates: Bending theory and variational formulation

4.1.1 Mindlin plates: Bending theory and variational formulation Chaper 4 soropic fla shell elemens n his chaper, fia shell elemens are formulaed hrough he assembly of membrane and plae elemens. The exac soluion of a shell approximaed by fia faces compared o he exac

More information

EXPLICIT TIME INTEGRATORS FOR NONLINEAR DYNAMICS DERIVED FROM THE MIDPOINT RULE

EXPLICIT TIME INTEGRATORS FOR NONLINEAR DYNAMICS DERIVED FROM THE MIDPOINT RULE Version April 30, 2004.Submied o CTU Repors. EXPLICIT TIME INTEGRATORS FOR NONLINEAR DYNAMICS DERIVED FROM THE MIDPOINT RULE Per Krysl Universiy of California, San Diego La Jolla, California 92093-0085,

More information

4.5 Constant Acceleration

4.5 Constant Acceleration 4.5 Consan Acceleraion v() v() = v 0 + a a() a a() = a v 0 Area = a (a) (b) Figure 4.8 Consan acceleraion: (a) velociy, (b) acceleraion When he x -componen of he velociy is a linear funcion (Figure 4.8(a)),

More information

KINEMATICS IN ONE DIMENSION

KINEMATICS 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 information

Summary of shear rate kinematics (part 1)

Summary 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 information

Chapter 3 Boundary Value Problem

Chapter 3 Boundary Value Problem Chaper 3 Boundary Value Problem A boundary value problem (BVP) is a problem, ypically an ODE or a PDE, which has values assigned on he physical boundary of he domain in which he problem is specified. Le

More information

System of Linear Differential Equations

System 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 information

Single and Double Pendulum Models

Single and Double Pendulum Models Single and Double Pendulum Models Mah 596 Projec Summary Spring 2016 Jarod Har 1 Overview Differen ypes of pendulums are used o model many phenomena in various disciplines. In paricular, single and double

More information

ψ(t) = V x (0)V x (t)

ψ(t) = V x (0)V x (t) .93 Home Work Se No. (Professor Sow-Hsin Chen Spring Term 5. Due March 7, 5. This problem concerns calculaions of analyical expressions for he self-inermediae scaering funcion (ISF of he es paricle in

More information

Basilio Bona ROBOTICA 03CFIOR 1

Basilio 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 information

Appendix 14.1 The optimal control problem and its solution using

Appendix 14.1 The optimal control problem and its solution using 1 Appendix 14.1 he opimal conrol problem and is soluion using he maximum principle NOE: Many occurrences of f, x, u, and in his file (in equaions or as whole words in ex) are purposefully in bold in order

More information

STATE-SPACE MODELLING. A mass balance across the tank gives:

STATE-SPACE MODELLING. A mass balance across the tank gives: B. Lennox and N.F. Thornhill, 9, Sae Space Modelling, IChemE Process Managemen and Conrol Subjec Group Newsleer STE-SPACE MODELLING Inroducion: Over he pas decade or so here has been an ever increasing

More information

The Contradiction within Equations of Motion with Constant Acceleration

The Contradiction within Equations of Motion with Constant Acceleration The Conradicion wihin Equaions of Moion wih Consan Acceleraion Louai Hassan Elzein Basheir (Daed: July 7, 0 This paper is prepared o demonsrae he violaion of rules of mahemaics in he algebraic derivaion

More information

3, so θ = arccos

3, 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 information

On-line Adaptive Optimal Timing Control of Switched Systems

On-line Adaptive Optimal Timing Control of Switched Systems On-line Adapive Opimal Timing Conrol of Swiched Sysems X.C. Ding, Y. Wardi and M. Egersed Absrac In his paper we consider he problem of opimizing over he swiching imes for a muli-modal dynamic sysem when

More information

IMPLICIT AND INVERSE FUNCTION THEOREMS PAUL SCHRIMPF 1 OCTOBER 25, 2013

IMPLICIT AND INVERSE FUNCTION THEOREMS PAUL SCHRIMPF 1 OCTOBER 25, 2013 IMPLICI AND INVERSE FUNCION HEOREMS PAUL SCHRIMPF 1 OCOBER 25, 213 UNIVERSIY OF BRIISH COLUMBIA ECONOMICS 526 We have exensively sudied how o solve sysems of linear equaions. We know how o check wheher

More information

Sliding Mode Extremum Seeking Control for Linear Quadratic Dynamic Game

Sliding Mode Extremum Seeking Control for Linear Quadratic Dynamic Game Sliding Mode Exremum Seeking Conrol for Linear Quadraic Dynamic Game Yaodong Pan and Ümi Özgüner ITS Research Group, AIST Tsukuba Eas Namiki --, Tsukuba-shi,Ibaraki-ken 5-856, Japan e-mail: pan.yaodong@ais.go.jp

More information

Physics 127b: Statistical Mechanics. Fokker-Planck Equation. Time Evolution

Physics 127b: Statistical Mechanics. Fokker-Planck Equation. Time Evolution Physics 7b: Saisical Mechanics Fokker-Planck Equaion The Langevin equaion approach o he evoluion of he velociy disribuion for he Brownian paricle migh leave you uncomforable. A more formal reamen of his

More information

Trajectory planning in Cartesian space

Trajectory 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 information

Let us start with a two dimensional case. We consider a vector ( x,

Let 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 information

Robotics I. April 11, The kinematics of a 3R spatial robot is specified by the Denavit-Hartenberg parameters in Tab. 1.

Robotics 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 information

At the end of this lesson, the students should be able to understand

At 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 information

Program: RFEM 5, RSTAB 8, RF-DYNAM Pro, DYNAM Pro. Category: Isotropic Linear Elasticity, Dynamics, Member

Program: 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 information

15. Vector Valued Functions

15. 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 information

The expectation value of the field operator.

The expectation value of the field operator. The expecaion value of he field operaor. Dan Solomon Universiy of Illinois Chicago, IL dsolom@uic.edu June, 04 Absrac. Much of he mahemaical developmen of quanum field heory has been in suppor of deermining

More information

= ( ) ) or a system of differential equations with continuous parametrization (T = R

= ( ) ) or a system of differential equations with continuous parametrization (T = R XIII. DIFFERENCE AND DIFFERENTIAL EQUATIONS Ofen funcions, or a sysem of funcion, are paramerized in erms of some variable, usually denoed as and inerpreed as ime. The variable is wrien as a funcion of

More information

dt = C exp (3 ln t 4 ). t 4 W = C exp ( ln(4 t) 3) = C(4 t) 3.

dt = C exp (3 ln t 4 ). t 4 W = C exp ( ln(4 t) 3) = C(4 t) 3. Mah Rahman Exam Review Soluions () Consider he IVP: ( 4)y 3y + 4y = ; y(3) = 0, y (3) =. (a) Please deermine he longes inerval for which he IVP is guaraneed o have a unique soluion. Soluion: The disconinuiies

More information

Chapter 2. First Order Scalar Equations

Chapter 2. First Order Scalar Equations Chaper. Firs Order Scalar Equaions We sar our sudy of differenial equaions in he same way he pioneers in his field did. We show paricular echniques o solve paricular ypes of firs order differenial equaions.

More information

Course Notes for EE227C (Spring 2018): Convex Optimization and Approximation

Course Notes for EE227C (Spring 2018): Convex Optimization and Approximation Course Noes for EE7C Spring 018: Convex Opimizaion and Approximaion Insrucor: Moriz Hard Email: hard+ee7c@berkeley.edu Graduae Insrucor: Max Simchowiz Email: msimchow+ee7c@berkeley.edu Ocober 15, 018 3

More information

Mean-square Stability Control for Networked Systems with Stochastic Time Delay

Mean-square Stability Control for Networked Systems with Stochastic Time Delay JOURNAL OF SIMULAION VOL. 5 NO. May 7 Mean-square Sabiliy Conrol for Newored Sysems wih Sochasic ime Delay YAO Hejun YUAN Fushun School of Mahemaics and Saisics Anyang Normal Universiy Anyang Henan. 455

More information

Kinematics and kinematic functions

Kinematics 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 information

Predator - Prey Model Trajectories and the nonlinear conservation law

Predator - Prey Model Trajectories and the nonlinear conservation law Predaor - Prey Model Trajecories and he nonlinear conservaion law James K. Peerson Deparmen of Biological Sciences and Deparmen of Mahemaical Sciences Clemson Universiy Ocober 28, 213 Ouline Drawing Trajecories

More information

Lecture 2-1 Kinematics in One Dimension Displacement, Velocity and Acceleration Everything in the world is moving. Nothing stays still.

Lecture 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 information

Ordinary Differential Equations

Ordinary Differential Equations Ordinary Differenial Equaions 5. Examples of linear differenial equaions and heir applicaions We consider some examples of sysems of linear differenial equaions wih consan coefficiens y = a y +... + a

More information

2.3 SCHRÖDINGER AND HEISENBERG REPRESENTATIONS

2.3 SCHRÖDINGER AND HEISENBERG REPRESENTATIONS Andrei Tokmakoff, MIT Deparmen of Chemisry, 2/22/2007 2-17 2.3 SCHRÖDINGER AND HEISENBERG REPRESENTATIONS The mahemaical formulaion of he dynamics of a quanum sysem is no unique. So far we have described

More information

Non-uniform circular motion *

Non-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 information

(1) (2) Differentiation of (1) and then substitution of (3) leads to. Therefore, we will simply consider the second-order linear system given by (4)

(1) (2) Differentiation of (1) and then substitution of (3) leads to. Therefore, we will simply consider the second-order linear system given by (4) Phase Plane Analysis of Linear Sysems Adaped from Applied Nonlinear Conrol by Sloine and Li The general form of a linear second-order sysem is a c b d From and b bc d a Differeniaion of and hen subsiuion

More information

Linear Response Theory: The connection between QFT and experiments

Linear Response Theory: The connection between QFT and experiments Phys540.nb 39 3 Linear Response Theory: The connecion beween QFT and experimens 3.1. Basic conceps and ideas Q: How do we measure he conduciviy of a meal? A: we firs inroduce a weak elecric field E, and

More information

1. An introduction to dynamic optimization -- Optimal Control and Dynamic Programming AGEC

1. An introduction to dynamic optimization -- Optimal Control and Dynamic Programming AGEC This documen was generaed a :45 PM 8/8/04 Copyrigh 04 Richard T. Woodward. An inroducion o dynamic opimizaion -- Opimal Conrol and Dynamic Programming AGEC 637-04 I. Overview of opimizaion Opimizaion is

More information

This document was generated at 1:04 PM, 09/10/13 Copyright 2013 Richard T. Woodward. 4. End points and transversality conditions AGEC

This document was generated at 1:04 PM, 09/10/13 Copyright 2013 Richard T. Woodward. 4. End points and transversality conditions AGEC his documen was generaed a 1:4 PM, 9/1/13 Copyrigh 213 Richard. Woodward 4. End poins and ransversaliy condiions AGEC 637-213 F z d Recall from Lecure 3 ha a ypical opimal conrol problem is o maimize (,,

More information

arxiv:quant-ph/ v1 5 Jul 2004

arxiv:quant-ph/ v1 5 Jul 2004 Numerical Mehods for Sochasic Differenial Equaions Joshua Wilkie Deparmen of Chemisry, Simon Fraser Universiy, Burnaby, Briish Columbia V5A 1S6, Canada Sochasic differenial equaions (sdes) play an imporan

More information

!!"#"$%&#'()!"#&'(*%)+,&',-)./0)1-*23)

!!#$%&#'()!#&'(*%)+,&',-)./0)1-*23) "#"$%&#'()"#&'(*%)+,&',-)./)1-*) #$%&'()*+,&',-.%,/)*+,-&1*#$)()5*6$+$%*,7&*-'-&1*(,-&*6&,7.$%$+*&%'(*8$&',-,%'-&1*(,-&*6&,79*(&,%: ;..,*&1$&$.$%&'()*1$$.,'&',-9*(&,%)?%*,('&5

More information

EE363 homework 1 solutions

EE363 homework 1 solutions EE363 Prof. S. Boyd EE363 homework 1 soluions 1. LQR for a riple accumulaor. We consider he sysem x +1 = Ax + Bu, y = Cx, wih 1 1 A = 1 1, B =, C = [ 1 ]. 1 1 This sysem has ransfer funcion H(z) = (z 1)

More information

Dynamic Analysis of Loads Moving Over Structures

Dynamic Analysis of Loads Moving Over Structures h Inernaional ongress of roaian ociey of echanics epember, 18-, 3 Bizovac, roaia ynamic nalysis of Loads oving Over rucures Ivica Kožar, Ivana Šimac Keywords: moving load, direc acceleraion mehod 1. Inroducion

More information

Finite element method for structural dynamic and stability analyses

Finite element method for structural dynamic and stability analyses Finie elemen mehod for srucural dynamic and sabiliy analyses Module- Nonlinear FE Models Lecure-39 Toal and updaed Lagrangian formulaions Prof C Manohar Deparmen of Civil Engineering IIc, Bangalore 56

More information

A Primal-Dual Type Algorithm with the O(1/t) Convergence Rate for Large Scale Constrained Convex Programs

A Primal-Dual Type Algorithm with the O(1/t) Convergence Rate for Large Scale Constrained Convex Programs PROC. IEEE CONFERENCE ON DECISION AND CONTROL, 06 A Primal-Dual Type Algorihm wih he O(/) Convergence Rae for Large Scale Consrained Convex Programs Hao Yu and Michael J. Neely Absrac This paper considers

More information

Zürich. ETH Master Course: L Autonomous Mobile Robots Localization II

Zürich. ETH Master Course: L Autonomous Mobile Robots Localization II Roland Siegwar Margaria Chli Paul Furgale Marco Huer Marin Rufli Davide Scaramuzza ETH Maser Course: 151-0854-00L Auonomous Mobile Robos Localizaion II ACT and SEE For all do, (predicion updae / ACT),

More information

Math Week 14 April 16-20: sections first order systems of linear differential equations; 7.4 mass-spring systems.

Math 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 information

Magnetic Field Synthesis in an Open-Boundary Region Exploiting Thévenin Equivalent Conditions

Magnetic Field Synthesis in an Open-Boundary Region Exploiting Thévenin Equivalent Conditions Magneic Field Synhesis in an Open-Boundary Region Exploiing Thévenin Equivalen Condiions Paolo DI BARBA, PhD Dep of Indusrial and Informaion Engineering Universiy of Pavia, Ialy paolo.dibarba@unipv.i Ouline

More information

Two Coupled Oscillators / Normal Modes

Two Coupled Oscillators / Normal Modes Lecure 3 Phys 3750 Two Coupled Oscillaors / Normal Modes Overview and Moivaion: Today we ake a small, bu significan, sep owards wave moion. We will no ye observe waves, bu his sep is imporan in is own

More information

Modified Iterative Method For the Solution of Fredholm Integral Equations of the Second Kind via Matrices

Modified Iterative Method For the Solution of Fredholm Integral Equations of the Second Kind via Matrices Modified Ieraive Mehod For he Soluion of Fredholm Inegral Equaions of he Second Kind via Marices Shoukralla, E. S 1, Saber. Nermein. A 2 and EL-Serafi, S. A. 3 1s Auhor, Prof. Dr, faculy of engineering

More information

Particle Swarm Optimization Combining Diversification and Intensification for Nonlinear Integer Programming Problems

Particle Swarm Optimization Combining Diversification and Intensification for Nonlinear Integer Programming Problems Paricle Swarm Opimizaion Combining Diversificaion and Inensificaion for Nonlinear Ineger Programming Problems Takeshi Masui, Masaoshi Sakawa, Kosuke Kao and Koichi Masumoo Hiroshima Universiy 1-4-1, Kagamiyama,

More information

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

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

More information

Week 1 Lecture 2 Problems 2, 5. What if something oscillates with no obvious spring? What is ω? (problem set problem)

Week 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 information

Homework 10 (Stats 620, Winter 2017) Due Tuesday April 18, in class Questions are derived from problems in Stochastic Processes by S. Ross.

Homework 10 (Stats 620, Winter 2017) Due Tuesday April 18, in class Questions are derived from problems in Stochastic Processes by S. Ross. Homework (Sas 6, Winer 7 Due Tuesday April 8, in class Quesions are derived from problems in Sochasic Processes by S. Ross.. A sochasic process {X(, } is said o be saionary if X(,..., X( n has he same

More information

CONTROL BY INTERCONNECTION OF THE TIMOSHENKO BEAM. DEIS, University of Bologna, viale Risorgimento 2, Bologna (Italy)

CONTROL BY INTERCONNECTION OF THE TIMOSHENKO BEAM. DEIS, University of Bologna, viale Risorgimento 2, Bologna (Italy) CONTROL BY INTERCONNECTION OF THE TIMOSHENKO BEAM Alessandro Macchelli Claudio Melchiorri EIS, Universiy of Bologna, viale Risorgimeno 2, 4036 Bologna Ialy email: {amacchelli, cmelchiorri}@deis.unio.i

More information

Recursive Least-Squares Fixed-Interval Smoother Using Covariance Information based on Innovation Approach in Linear Continuous Stochastic Systems

Recursive Least-Squares Fixed-Interval Smoother Using Covariance Information based on Innovation Approach in Linear Continuous Stochastic Systems 8 Froniers in Signal Processing, Vol. 1, No. 1, July 217 hps://dx.doi.org/1.2266/fsp.217.112 Recursive Leas-Squares Fixed-Inerval Smooher Using Covariance Informaion based on Innovaion Approach in Linear

More information

Ground Rules. PC1221 Fundamentals of Physics I. Kinematics. Position. Lectures 3 and 4 Motion in One Dimension. A/Prof Tay Seng Chuan

Ground Rules. PC1221 Fundamentals of Physics I. Kinematics. Position. Lectures 3 and 4 Motion in One Dimension. A/Prof Tay Seng Chuan Ground Rules PC11 Fundamenals of Physics I Lecures 3 and 4 Moion in One Dimension A/Prof Tay Seng Chuan 1 Swich off your handphone and pager Swich off your lapop compuer and keep i No alking while lecure

More information

( ) a system of differential equations with continuous parametrization ( T = R + These look like, respectively:

( ) a system of differential equations with continuous parametrization ( T = R + These look like, respectively: XIII. DIFFERENCE AND DIFFERENTIAL EQUATIONS Ofen funcions, or a sysem of funcion, are paramerized in erms of some variable, usually denoed as and inerpreed as ime. The variable is wrien as a funcion of

More information

CH.7. PLANE LINEAR ELASTICITY. Continuum Mechanics Course (MMC) - ETSECCPB - UPC

CH.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 information

Lab #2: Kinematics in 1-Dimension

Lab #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 information

Final Spring 2007

Final Spring 2007 .615 Final Spring 7 Overview The purpose of he final exam is o calculae he MHD β limi in a high-bea oroidal okamak agains he dangerous n = 1 exernal ballooning-kink mode. Effecively, his corresponds o

More information

THE MYSTERY OF STOCHASTIC MECHANICS. Edward Nelson Department of Mathematics Princeton University

THE MYSTERY OF STOCHASTIC MECHANICS. Edward Nelson Department of Mathematics Princeton University THE MYSTERY OF STOCHASTIC MECHANICS Edward Nelson Deparmen of Mahemaics Princeon Universiy 1 Classical Hamilon-Jacobi heory N paricles of various masses on a Euclidean space. Incorporae he masses in he

More information

AP Calculus BC Chapter 10 Part 1 AP Exam Problems

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

More information

Sterilization D Values

Sterilization D Values Seriliaion D Values Seriliaion by seam consis of he simple observaion ha baceria die over ime during exposure o hea. They do no all live for a finie period of hea exposure and hen suddenly die a once,

More information

EXERCISES FOR SECTION 1.5

EXERCISES FOR SECTION 1.5 1.5 Exisence and Uniqueness of Soluions 43 20. 1 v c 21. 1 v c 1 2 4 6 8 10 1 2 2 4 6 8 10 Graph of approximae soluion obained using Euler s mehod wih = 0.1. Graph of approximae soluion obained using Euler

More information

Combined Bending with Induced or Applied Torsion of FRP I-Section Beams

Combined Bending with Induced or Applied Torsion of FRP I-Section Beams Combined Bending wih Induced or Applied Torsion of FRP I-Secion Beams MOJTABA B. SIRJANI School of Science and Technology Norfolk Sae Universiy Norfolk, Virginia 34504 USA sirjani@nsu.edu STEA B. BONDI

More information

Computation of the Effect of Space Harmonics on Starting Process of Induction Motors Using TSFEM

Computation of the Effect of Space Harmonics on Starting Process of Induction Motors Using TSFEM Journal of elecrical sysems Special Issue N 01 : November 2009 pp: 48-52 Compuaion of he Effec of Space Harmonics on Saring Process of Inducion Moors Using TSFEM Youcef Ouazir USTHB Laboraoire des sysèmes

More information

Integration Over Manifolds with Variable Coordinate Density

Integration Over Manifolds with Variable Coordinate Density Inegraion Over Manifolds wih Variable Coordinae Densiy Absrac Chrisopher A. Lafore clafore@gmail.com In his paper, he inegraion of a funcion over a curved manifold is examined in he case where he curvaure

More information

IB Physics Kinematics Worksheet

IB Physics Kinematics Worksheet IB Physics Kinemaics Workshee Wrie full soluions and noes for muliple choice answers. Do no use a calculaor for muliple choice answers. 1. Which of he following is a correc definiion of average acceleraion?

More information

Math 10B: Mock Mid II. April 13, 2016

Math 10B: Mock Mid II. April 13, 2016 Name: Soluions Mah 10B: Mock Mid II April 13, 016 1. ( poins) Sae, wih jusificaion, wheher he following saemens are rue or false. (a) If a 3 3 marix A saisfies A 3 A = 0, hen i canno be inverible. True.

More information

m = 41 members n = 27 (nonfounders), f = 14 (founders) 8 markers from chromosome 19

m = 41 members n = 27 (nonfounders), f = 14 (founders) 8 markers from chromosome 19 Sequenial Imporance Sampling (SIS) AKA Paricle Filering, Sequenial Impuaion (Kong, Liu, Wong, 994) For many problems, sampling direcly from he arge disribuion is difficul or impossible. One reason possible

More information

k 1 k 2 x (1) x 2 = k 1 x 1 = k 2 k 1 +k 2 x (2) x k series x (3) k 2 x 2 = k 1 k 2 = k 1+k 2 = 1 k k 2 k series

k 1 k 2 x (1) x 2 = k 1 x 1 = k 2 k 1 +k 2 x (2) x k series x (3) k 2 x 2 = k 1 k 2 = k 1+k 2 = 1 k k 2 k series Final Review A Puzzle... Consider wo massless springs wih spring consans k 1 and k and he same equilibrium lengh. 1. If hese springs ac on a mass m in parallel, hey would be equivalen o a single spring

More information

CHAPTER 10 VALIDATION OF TEST WITH ARTIFICAL NEURAL NETWORK

CHAPTER 10 VALIDATION OF TEST WITH ARTIFICAL NEURAL NETWORK 175 CHAPTER 10 VALIDATION OF TEST WITH ARTIFICAL NEURAL NETWORK 10.1 INTRODUCTION Amongs he research work performed, he bes resuls of experimenal work are validaed wih Arificial Neural Nework. From he

More information

Variational Iteration Method for Solving System of Fractional Order Ordinary Differential Equations

Variational Iteration Method for Solving System of Fractional Order Ordinary Differential Equations IOSR Journal of Mahemaics (IOSR-JM) e-issn: 2278-5728, p-issn: 2319-765X. Volume 1, Issue 6 Ver. II (Nov - Dec. 214), PP 48-54 Variaional Ieraion Mehod for Solving Sysem of Fracional Order Ordinary Differenial

More information