Numerical Optimization

Size: px
Start display at page:

Download "Numerical Optimization"

Transcription

1 Numerical Opimizaion A Workshop A Deparmen o Mahemaics Chiang Mai Universiy Augus 4-5, 9 Insrucor: Elecrical Engineering and Compuer Science Case Wesern Reserve Universiy Phone: , Fax: vira@case.edu Session: Opimizaion o Dynamic Sysems Case Wesern Reserve Universiy Elecrical Engineering and Compuer Science EECS.

2 Module Objecive o develop uncional knowledge and skills in modeling dynamic sysems and/or opimal conrol problems deermining a sae rajecory and/or a conrol o dynamic sysems ha opimizes a perormance uncional subjec o consrains on conrol and/or saes. 3 Module Highlighs wo pronged approach:. Focus on he wo radiional approaches or dealing wih dynamic opimizaion/opimal conrol problems he variaional approach based on calculus o variaions leading o he maximum principle he dynamic programming approach and is corresponding Hamilon-Jacobi-Bellman (HJB equaion. When applied o linear opimal conrol problem derivaion o similar resuls based on he concep o Lyapunov sabiliy will also be demonsraed.. Focus on numerical mehods or solving large real-world dynamic opimizaion and opimal conrol problems wih complex consrains. he wo numerical approaches are he indirec approach and he direc approach. MALAB will be used o implemen mehods discussed. Applicaions o engineering and economic problems will be illusraed hroughou 4

3 ex: Reerences Opimal Conrol heory, D.E. Kirk, Dover Publicaions, ISBN: , 4 Reerences:. Pracical Mehods or Opimal Conrol Using Nonlinear Programming, J.. Bes, SIAM, ISBN: ,. Applied Dynamic Programming or Opimizaion o Dynamical Sysems, R.D. Robine III, D.G. Wilson, G. Richard Eisler and J. E. Hurado, SIAM, ISBN: , 6 5 Dynamic Opimizaion ( n min J = gxx (,,.., x, d x: [, ] R ( n ( n subjec o, x( = x, ( =,.., x ( = x ( n ( n and possibly, x( = x, ( =,.., x ( = x Noe: he inal ime may or may no be speciied. I is speciied ixed-end-ime problem (or ixed-erminal-ime I is no speciied variable-end-ime problem ( or open-erminal-ime, open horizon I is speciied, and i x ( is also ixed ixed-end-poin problem x ( is consrained (i.e. x ( S consrained-erminal-poin problem x ( is no ixed or has no resricion ree-end-poin problem 6 3

4 Opimal Conrol Problems min J = h( x(, + g( x(, u(, d m u: [, ] R subjec o Sysem Dynamics: ( = a( x(, u(, ; where sae x: [, ] R Iniial condiions: x( = x erminal or inal condi ions: x( = x n Find a conrol u( o ake he sysem rom he iniial sae x( a he iniial ime o he inal sae x( a he inal ime. 7 Opimal Conrol Problems Possible addiional consrains: Conrains on conrol: u( U or all [, ] e.g. u u( u or all [, ] min max Conrains on sae: x( X or all [, ] e.g. xmin x( xmax or all [, ] 8 4

5 Noe: Opimal Conrol Problems As beore, may be speciied ( ixed-end-ime I is speciied, or may no speciied ( variable-end-ime or open erminalime x ( may be ixed ( ixed-end-poin or hard erminal consrain or consrained x ( S( so erminal consrain or no ixed or no resricion ( ree-end-poin 9 Various ypes o J : Opimal Conrol Problems g =, i.e. J = h( x(, Mayer Problem Special Mayer Problems: ( a J = cx( (Linear Mayer ( ( ( b J = x( - r( H x( - r( (erminal conrol problem h =, i.e. J = g( x(, u(, d lagrange Problem Special Lagrange Problems: (a g =, i.e. J = d = - (b g = u(, i.e. J = u( d (Minimum ime (Minimum uel (c g = u(, i.e. J = u( u( d (Minimum energy 5

6 (a racking problem: Opimal Conrol Problems J = h( x(, + g( x(, u(, d bolza Problems Special Bolza Problems: h = g = ( x( - r( H( x( - r( ( x(-( r Q( x(-( r + u( Ru( ( x r H( x r ( x r Q( J = ( -( ( - ( + (- ( x(-( r + u( Ru( d Noe: H, Q and R are w eighing marices (b Regulaor problem: h = x( Hx( g = x( Qx( + u( Ru( J = x( Hx( + x( Qx( + u( Ru( d Example : (Brachisochrome A bead o mass uni descends along a wire joining wo ixed poins (x,y and (x,y. We wish o ind he shape o he wire so ha he bead complees is slide in minimum ime. (x,y = (x,y 6

7 Example : (Brachisochrome Model: Dynamic Opimizaion Model: (x,y = y = y(x, y: [x,x ] R, y C ( x g y y( x (x,y min = subjec o yx ( = y yx ( x = y + y ( x dx Minimum ime Fixed erminal poin problem (Hard erminal consrain 3 (x,y = (, Example : (River-Crossing A boa ravels wih consan velociy V wih respec o he waer. In he region he velociy o he curren is parallel o x-axis bu varies wih y. Given he desinaion (x,y on he oher side o he river, ind he pah o be aken by he boa o minimize he ravel ime, y = V θ (x,y = v c (y Opimal Conrol Model: min = d + x Final condiions: x( = x ; y( = y Minimum ime Fixed erminal poin problem subjec o Dynamics (Equaion o Moion: = V cos θ + vc ( y y = V sinθ Iniial condiions: x( = x ; y( = y 4 7

8 (x,y = (, Example 3: (River-Crossing A boa ravels wih consan velociy V wih respec o he waer. In he region he velociy o he curren is parallel o x-axis bu varies wih y. Given he inal ime, ind he pah o be aken by he boa o maximize he landing disance on he oher side o he river, y = V θ (x,y = v c (y x Opimal Conrol Model: max J = x( subjec o Dynamics (Equaion o Moion: = V cos θ + vc ( y y = V sinθ Iniial condiions: x( = x ; y( = y Final condiions: y ( = y Linear Mayer problem wih semi-hard erminal consrain 5 Example 4: (Braking and Acceleraion: Wan o move a car o mass m rom o x in minimum ime. Minimum ime α ( +β ( Opimal Conrol: Hard erminal consrain x( x( = x min J = = d wih bound consrains EOM: x( = α( + β ( subjec o Sae: s x ( = x( Dynamics (Equaion o Moion: x( = ( = ( = x( Compac Dynamics: = α( + β( = Ax( + Bu( Iniial condiio ns: x( = ; x( = A = erminal condiions: x ( = x; x ( =, B = Conrains: For each [, ] : x( u( α( x( =, u( = = On conrol: u( M; u( M x( u( β ( On sae: x ( x ; x ( x( = 6 8

9 y v β( Example 5: (aking-o An aircra o mass m (assumed poin mass is o be lied by a consan rus o reach he cruising aliude H a ime, a maximum speed (along x- direcion. = H Opimal Conrol Model: max J = x ( Dynamics (Equaion o Moion: = = = 3 4 cos β m = 4 = sin β g x m Iniial condiions: x ( = x( = x3( = x4( = EOM: mx ( = cos β ( Final condiions: x3( = H; x4( = my ( = sin β ( mg Consrains: On conrol u ( π /, [, ] Saes: x( = x(; x( = ( = ( On sae: xi (, i =,..4; x3 ( H x3( = y(; x4( = 3( = y ( Conrol u ( = β ( x Linear Mayer problem wih semi-hard erminal consrain x 7 Example 6: (Rover Conrol Wan o conrol he speed o a Mariner Mars rover a abou 5 mph using as lile energy as possible. he conroller is he oupu volage o a baeryoperaed volage regulaing sysem. Baery Volage Regulaing Sysem i e( R L I a (consan R a L a θ( Viscous ricion coeicien B di ( Dynamics: Ri ( + L = e( d λ( = Ki( orque λ( = I θ( + B θ( + λl ( Saes: x( = i ( ; x( = θ ( Conrols: u ( = e(; u ( = λ ( L λ( λ L ( 8 9

10 Example 6: (Rover Conrol Min J = ( kx ( ( 5 + wx( u ( d i Dynamics : Baery R Volage R = x( + u( Regulaing e( L L Sysem L K B = x( - x( u( I I I I a (consan Iniial condi ions: x( = x( = R a Final con diions: None Viscous ricion Consrai ns : L coeicien B a θ( On conrol: u( emax, [, ] u( λmax, [, ] λ( λ L ( On sae: x( Imax, [, ] Minimum energy problem wih ree erminal x( Ωmax, [, ] condiions bu wih bound consrains 9 u( 5gal ank A 8lb sal a = Example 7: (Mixure Wan o ind inlow rae o resh waer (conrol o he wo-ank sysem so ha he sal concenraion in anks A and B are equal using minimum amoun o resh waer. u( 5gal ank B Fresh waer a = u( Opimal Conrol Model: min J = u( d Dynamics: u ( Assume: Well-mixed a all ime = x( 5 Incompressible luid u ( u ( Saes: x ( = lbs o sal in A a ime = x( x( 5 5 x ( = lbs o sal in B a ime Iniial condiions: x( = 8; x( = Co nrols: u ( = gal/m o resh waer erminal condiions: x( - x( = passing hru a ime Conrains: For each : Minimum conrol eor wih On conrol: u ( umax, [, ] So erminal consrain and bound consrains On sae: x ( 8; x (

11 Opimizing Yeas or Ehanol Producion in a Bioreacor Bioreacors are large vessels ha serve as an environmen or biochemical reacions o occur. ypical uses include he growh o microorganisms and he breakdown o producs. Source: D. Moore, MS hesis,, 7 he environmen wihin he vessel is conrolled o opimize perormance. ypical conrol variables include nurien eed rae, oxygen air low rae, and emperaure. here is large economic incenive o develop conrol sraegies o maximize he producion o baker s yeas and ehanol, wo imporan commercial producs produced in bioreacors. Yeas is ypically grown o a soluion conaining glucose and oher nuriens essenial or cellular growh. When glucose concenraion in he medium is high or when here is a limied supply o oxygen, he yeas microorganism excrees ehanol. Opimizing Yeas or Ehanol Producion in a Bioreacor We wish o maximize producion o yeas, or ehanol or boh by conrolling he subsrae eed rae, airlow (O and emperaure Model o Growh Dynamics X = yeas concenraion (g/l S = subsrae (glucose concenraion (g/l E = ehanol concenraion (g/l O = dissolved oxygen (O concenraion (g/l C = dissolved carbon dioxide (CO concenraion (g/l V = liquid volume (l F in = Subsrae eed rae (l/h S in = Inluen Subsrae Concenraion (g/l D = F in /V = Diluion rae (/h OR = k L a(o S O = O ranser rae (g/l h - CER = k V k L ac = CO evoluion rae (g/l h - m = Mainenance erm (g o S /g o X h - 7-Aug-9

12 wo Ways o Solve Dynamic Opimizaion/Opimal Conrol Problems. Indirec Mehod: Solve he necessary condiions or opimaliy derived hrough variaional principles rooed in Calculus o Variaions ha is: Solve wo-poin boundary value problems (PBVP 3 wo Ways o Solve Dynamic Opimizaion/Opimal Conrol Problems. Direc Mehod: Opimize he uncional direcly as consrained opimizaion Require conversion o nonlinear programs hrough ranscripion o he ODEs (dynamics o sysem Oen possesses high sparsiy and special srucure 4

13 Direc Mehod or Dynamic Opimizaion Conver o nonlinear programs hrough direc ranscripion o he ODEs (dynamics o sysem or he corresponding DAEs Use nonlinear opimizer such SQP o solve he resuling nonlinear programs (Soware such as SNOP by Boeing, ec. Fine-une he resul hrough meshreinemen echniques 5 Direc Mehod: ranscripion mehods Euler: x = x + h a( x, u, Classical Runge-Kaa: x x s k+ k k k k k k+ = k + hk k where sk = ( k + k + k3 + k4 6 k = hka( xk, uk, k hk k = hka( xk + k, uk+, k + hk k3 = hka( xk + k, uk+, k + k4 = hka( xk + k3, uk+, k+ rapezoidal: xk+ = xk + hk a( xk, uk, k + a( xk + hka( xk, uk, k, uk+, k+ Hermi-Simpson: ( hk xk+ = xk + ( a( xk, uk, k + a( xk + hka( xk, uk, k, uk+, k+ + ak+ 6 hk where xk+ = xk + xk + hka( xk, uk, k + a( xk, uk, k a( xk + hka( xk, uk, k, uk+, k+ 8 hk and ak+ = a( xk+, uk+, k + ( ( 6 3

14 Direc Mehod: ranscripion mehods Band, Sair-case Srucure and Sparsiy o resuling marix: Employ special numerical ricks o ake advanage o he special srucure and sparsiy o he resuling problem 7 Indirec Mehod: Derivaion o Opimaliy Condiions Euler-Lagrange Equaions and all Boundary Condiions Hamilon-Jacobi Jacobi-Bellman Condiions Ponryagin s Minimum Principle 8 4

15 Indirec Mehod: Fundamenals Variaions o a Funcional: Pah opimizaion: Funcional J( y( x: where x [ x, x] and y:[ x, x] R Δ J( y*, δy = δj( y*, δy + ο( δy incremen variaion error erm where ο( δy as δy Opimal conrol: Funcion J ( x( or J( x(, : where [, ] and x:[, ] R Δ J( δx = δj( δx + ο( δx incremen variaion error erm Δ J(*, x δx, δ = δj(*, x δx, δ + ο( δx, δ incremen variaion error erm n n 9 J Key variaion ormular: δj ( x, δx = δx x J J J = δx + δx δx x ( n ( x( = (,,..,, For example: J g x x x d J J J ( n hen δj( x, δx = δx+ δ δx ( n ( n =.. δx+ δ + + δx ( n d erm like δ xd are deal wih hru inegraion by par i.e. Indirec Mehod: Fundamenals δxd = δx δ xd n n 3 5

16 3 Fundamenal heorem o Calculus o Variaions: x* is an exremal o J( x only i δj( δx = or all admissible δx. 4 Fundamenal Lemmas o Calculus o Variaions: a Le α( x C[ a, b]. a b I α( xhxdx ( = or all hx ( Cab [, ] wih ha ( = hb ( = hen α( x = or all x [ a, b] b Le α( x C a b [, ]. b I α( xh ( xd x= or all h( x C [ a, b] wih h( a = h( b = a hen α( x = c or all x [ a, b] x Indirec Mehod: Fundamenals C a b c Le α( and β(x [, ]. ( α β b I ( xhx ( + ( xh ( x dx= or all hx ( C[ ab, ] wih ha ( = hb ( = a hen β ( x = α( x or all x [ ab, ] 3 Indirec Mehod: Necessary Condiions Now consider J( x = g( x,, d, x:[, ] R a Case: and x( are ixed (ixed end poin x* is an exremal o Jx ( only i δ Jx ( *, δ x = or all admissible δ x. J J = δ J( δ x = δ x+ δ or all admissible δx x = or all admissible δx+ δ d δx = δx + δ x δx d (inegraion by par x = or all admissible δxd δx (since δx ( = and δx ( = g = (by Fundamenal Lemmas o Calculus o Variaions 4a his is Euler-Lagrange Equaion 3 6

17 Indirec Mehod: Necessary Condiions For J( x = g( x,, d, x: [, ] R wih and x( ixed (ixed end poin Necessary Condiions: Euler-Lagrange Equaion x* is an exremal o Jx ( only i = (second-order ODE wih -boundary poin x ( = x and x ( = x Solved by shooing mehod (or example 33 Indirec Mehod: Necessary Condiions Example: J x = x x d x R g( x, x π ( ( ( (, :[, ] wih x( =, x( π = (ixed end poin Euler-Lagrange Equaion = x ( = x+ x = x ( = ccos+ c sin Wih x( = and x( π = x ( = cos+ sin = sin Solved numerically by he shooing mehod 34 7

18 Indirec Mehod: Necessary Condiions For J( x = g( x,, d, x:[, ] R b Case: is ixed and x( is ree (ree end poin x* is an exremal o J ( x only i δj( δx, δ x = or all admissible ( δx, δ x. J J = δj( δx = δx+ δ or all admissible δx = or all admissible δx+ δ d δx = δ x + δ x δ x d (inegraion by par x = x δ x ( + δxd or all admissible δx, and δx( (since δx ( = and δx( = ( Euler-Lagrange = x ( = 35 Indirec Mehod: Necessary Condiions Now consider J( x, = g( x,, d, x:[, ] R and is ree (variable end ime, ree erminal ime or horizon a Case: x ( is ree and is independen o (ree erminal condiions =δ J( δx, δx, δ or all admissible ( δx, δx, δ + δ = δ gxx (,, d+ (*, *, or all admissible x, x and gx d δ δ δ = δ x( + δ x d + g(*,*, x δ x = ( δx - * ( δ + ( *, *, δ xd + g x x δ x x (since δx ( = δx - *( δ g g = δ x + δ xd g( x* ( + δ or all admissible δx, δx and δ = (Euler-Lagrange =, gx (*,*, *( =, and x ( = 36 8

19 Indirec Mehod: Necessary Condiions Now consider J( x, = g( x,, d, x:[, ] R and is ree (variable end ime, ree erminal ime or horizon b Case: x ( = x (Hard erminal conrain = (Euler-Lagrange x ( = x, gx ( *, *, *( =, and x ( = c Case: x ( = θ ( (So erminal conrain -- δ x = θ( δ = (Euler-Lagrange θ ( + g( *, * ( =, x*, x*, and x ( =, x ( = θ ( 37 Example Derivaion o Case (c Now consider J( x, = g( x,, d, x:[, ] R and is ree (variable end ime, ree erminal ime or horizon c Case: x( = θ ( (So erminal conrain =δj( δx, δx, δ or all admissible δ x + δ = δ gx ( *, *, d + ( *, *, or all admissible gx d δ x = δx ( + δ xd g( δ + x = ( δx - *( δ + ( *, *, δ xd+ g x δ x (since δx ( = δx - *( δ = δ x + δ xd+ g( x *( δ x or all admissible δx, δx and δ = (Euler-Lagrange =, g(*,*, x *( =, and x( = 38 9

20 Indirec Mehod: Necessary Condiions Furher exensions: Piecewise Coninuous Soluion: Require addiional Weisrass Erdman Corner Condiions or ranversailiy Condiions Consrains on x( require he use o mulipliers Mos imporan cases are in opimal conrol problems: 39 Indirec Mehod: Necessary Condiions Opimal Conrol Problems: Opimize J ( xu,, = h( x(, + g( xu,, d s.. = a( x, u, Boundary condiions: x( = x Cas es: I is ixed and x( is ixed II is ixed and x( is ree III is ixed, and m( x( = IV is ree and x( is ree V is ree and x( is ixed VI is ree and x( = θ( VII is ree, and m( x( = VIII is ree, and m( x(, = 4

21 Indirec Mehod: Necessary Condiions Opimal Conrol Problems: Opimize J( xu,, = h( x(, + g( xu,, d s.. = a( x, u, Boundary condiions: x( = x Case IV: h( x(, = h ( x(, d + h( x(, ignored (consan H ( xup,,, Hamilonian h( x(, h( x(, = + d h( x(, h( x(, g a ( xxup,,,, = g( xu,, ++ p ( axu (,, + J ( xxup,,,, = g ( xxup,,,, d a a δja(*, x δx,*, u δu,*, p δp, δx, δ H * H * = d δu+ + p δx u h(*, x h( x *(, + p( δ x + g* + p a( u*, + = or all admissible δx, δu, δx, δ δ 4 Indirec Mehod: Necessary Condiions Necessary Condiions or Opimal Conrol Problems: Case IV: Free-end poin problems: ree and x( ree Hamilonian-Jacobi Condiions: ( u*is exremal, hen here exiss co-saes p*such ha: H * = ( u H * p = ( = a( x, u, (3 h(*, x h( x*(, p( δx + H* + δ = (4 and x( = x OHER CASES CAN BE SIMILARILY DERIVED 4

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

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

MA Study Guide #1

MA Study Guide #1 MA 66 Su Guide #1 (1) Special Tpes of Firs Order Equaions I. Firs Order Linear Equaion (FOL): + p() = g() Soluion : = 1 µ() [ ] µ()g() + C, where µ() = e p() II. Separable Equaion (SEP): dx = h(x) g()

More information

Solutions to Assignment 1

Solutions to Assignment 1 MA 2326 Differenial Equaions Insrucor: Peronela Radu Friday, February 8, 203 Soluions o Assignmen. Find he general soluions of he following ODEs: (a) 2 x = an x Soluion: I is a separable equaion as we

More information

Math Final Exam Solutions

Math Final Exam Solutions Mah 246 - Final Exam Soluions Friday, July h, 204 () Find explici soluions and give he inerval of definiion o he following iniial value problems (a) ( + 2 )y + 2y = e, y(0) = 0 Soluion: In normal form,

More information

Optimal Path Planning for Flexible Redundant Robot Manipulators

Optimal Path Planning for Flexible Redundant Robot Manipulators 25 WSEAS In. Conf. on DYNAMICAL SYSEMS and CONROL, Venice, Ialy, November 2-4, 25 (pp363-368) Opimal Pah Planning for Flexible Redundan Robo Manipulaors H. HOMAEI, M. KESHMIRI Deparmen of Mechanical Engineering

More 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

Math 333 Problem Set #2 Solution 14 February 2003

Math 333 Problem Set #2 Solution 14 February 2003 Mah 333 Problem Se #2 Soluion 14 February 2003 A1. Solve he iniial value problem dy dx = x2 + e 3x ; 2y 4 y(0) = 1. Soluion: This is separable; we wrie 2y 4 dy = x 2 + e x dx and inegrae o ge The iniial

More 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

u(x) = e x 2 y + 2 ) Integrate and solve for x (1 + x)y + y = cos x Answer: Divide both sides by 1 + x and solve for y. y = x y + cos x

u(x) = e x 2 y + 2 ) Integrate and solve for x (1 + x)y + y = cos x Answer: Divide both sides by 1 + x and solve for y. y = x y + cos x . 1 Mah 211 Homework #3 February 2, 2001 2.4.3. y + (2/x)y = (cos x)/x 2 Answer: Compare y + (2/x) y = (cos x)/x 2 wih y = a(x)x + f(x)and noe ha a(x) = 2/x. Consequenly, an inegraing facor is found wih

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

Instructor: Barry McQuarrie Page 1 of 5

Instructor: Barry McQuarrie Page 1 of 5 Procedure for Solving radical equaions 1. Algebraically isolae one radical by iself on one side of equal sign. 2. Raise each side of he equaion o an appropriae power o remove he radical. 3. Simplify. 4.

More information

Optima and Equilibria for Traffic Flow on a Network

Optima and Equilibria for Traffic Flow on a Network Opima and Equilibria for Traffic Flow on a Nework Albero Bressan Deparmen of Mahemaics, Penn Sae Universiy bressan@mah.psu.edu Albero Bressan (Penn Sae) Opima and equilibria for raffic flow 1 / 1 A Traffic

More information

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

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

1 Subdivide the optimization horizon [t 0,t f ] into n s 1 control stages,

1 Subdivide the optimization horizon [t 0,t f ] into n s 1 control stages, Opimal Conrol Formulaion Opimal Conrol Lecures 19-2: Direc Soluion Mehods Benoî Chachua Deparmen of Chemical Engineering Spring 29 We are concerned wih numerical soluion procedures for

More information

Math 221: Mathematical Notation

Math 221: Mathematical Notation Mah 221: Mahemaical Noaion Purpose: One goal in any course is o properly use he language o ha subjec. These noaions summarize some o he major conceps and more diicul opics o he uni. Typing hem helps you

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

I. OBJECTIVE OF THE EXPERIMENT.

I. OBJECTIVE OF THE EXPERIMENT. I. OBJECTIVE OF THE EXPERIMENT. Swissmero raels a high speeds hrough a unnel a low pressure. I will hereore undergo ricion ha can be due o: ) Viscosiy o gas (c. "Viscosiy o gas" eperimen) ) The air in

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

Solutions of Sample Problems for Third In-Class Exam Math 246, Spring 2011, Professor David Levermore

Solutions of Sample Problems for Third In-Class Exam Math 246, Spring 2011, Professor David Levermore Soluions of Sample Problems for Third In-Class Exam Mah 6, Spring, Professor David Levermore Compue he Laplace ransform of f e from is definiion Soluion The definiion of he Laplace ransform gives L[f]s

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

MA 366 Review - Test # 1

MA 366 Review - Test # 1 MA 366 Review - Tes # 1 Fall 5 () Resuls from Calculus: differeniaion formulas, implici differeniaion, Chain Rule; inegraion formulas, inegraion b pars, parial fracions, oher inegraion echniques. (1) Order

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

= ( ) ) 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

LAPLACE TRANSFORM AND TRANSFER FUNCTION

LAPLACE TRANSFORM AND TRANSFER FUNCTION CHBE320 LECTURE V LAPLACE TRANSFORM AND TRANSFER FUNCTION Professor Dae Ryook Yang Spring 2018 Dep. of Chemical and Biological Engineering 5-1 Road Map of he Lecure V Laplace Transform and Transfer funcions

More 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

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

Homogenization of random Hamilton Jacobi Bellman Equations

Homogenization of random Hamilton Jacobi Bellman Equations Probabiliy, Geomery and Inegrable Sysems MSRI Publicaions Volume 55, 28 Homogenizaion of random Hamilon Jacobi Bellman Equaions S. R. SRINIVASA VARADHAN ABSTRACT. We consider nonlinear parabolic equaions

More information

not to be republished NCERT MATHEMATICAL MODELLING Appendix 2 A.2.1 Introduction A.2.2 Why Mathematical Modelling?

not to be republished NCERT MATHEMATICAL MODELLING Appendix 2 A.2.1 Introduction A.2.2 Why Mathematical Modelling? 256 MATHEMATICS A.2.1 Inroducion In class XI, we have learn abou mahemaical modelling as an aemp o sudy some par (or form) of some real-life problems in mahemaical erms, i.e., he conversion of a physical

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

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

Suggested Practice Problems (set #2) for the Physics Placement Test

Suggested Practice Problems (set #2) for the Physics Placement Test Deparmen of Physics College of Ars and Sciences American Universiy of Sharjah (AUS) Fall 014 Suggesed Pracice Problems (se #) for he Physics Placemen Tes This documen conains 5 suggesed problems ha are

More information

x i v x t a dx dt t x

x i v x t a dx dt t x Physics 3A: Basic Physics I Shoup - Miderm Useful Equaions A y A sin A A A y an A y A A = A i + A y j + A z k A * B = A B cos(θ) A B = A B sin(θ) A * B = A B + A y B y + A z B z A B = (A y B z A z B y

More information

CHBE320 LECTURE IV MATHEMATICAL MODELING OF CHEMICAL PROCESS. Professor Dae Ryook Yang

CHBE320 LECTURE IV MATHEMATICAL MODELING OF CHEMICAL PROCESS. Professor Dae Ryook Yang CHBE320 LECTURE IV MATHEMATICAL MODELING OF CHEMICAL PROCESS Professor Dae Ryook Yang Spring 208 Dep. of Chemical and Biological Engineering CHBE320 Process Dynamics and Conrol 4- Road Map of he Lecure

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

Physics 3A: Basic Physics I Shoup Sample Midterm. Useful Equations. x f. x i v x. a x. x i. v xi v xf. 2a x f x i. y f. a r.

Physics 3A: Basic Physics I Shoup Sample Midterm. Useful Equations. x f. x i v x. a x. x i. v xi v xf. 2a x f x i. y f. a r. Physics 3A: Basic Physics I Shoup Sample Miderm Useful Equaions A y Asin A A x A y an A y A x A = A x i + A y j + A z k A * B = A B cos(θ) A x B = A B sin(θ) A * B = A x B x + A y B y + A z B z A x B =

More information

Math 2214 Solution Test 1B Fall 2017

Math 2214 Solution Test 1B Fall 2017 Mah 14 Soluion Tes 1B Fall 017 Problem 1: A ank has a capaci for 500 gallons and conains 0 gallons of waer wih lbs of sal iniiall. A soluion conaining of 8 lbsgal of sal is pumped ino he ank a 10 galsmin.

More information

1 st order ODE Initial Condition

1 st order ODE Initial Condition Mah-33 Chapers 1-1 s Order ODE Sepember 1, 17 1 1 s order ODE Iniial Condiion f, sandard form LINEAR NON-LINEAR,, p g differenial form M x dx N x d differenial form is equivalen o a pair of differenial

More information

In Game Theory and Applications, Volume X WITH MIGRATION: RESERVED TERRITORY APPROACH. Vladimir V. Mazalov. Anna N. Rettieva

In Game Theory and Applications, Volume X WITH MIGRATION: RESERVED TERRITORY APPROACH. Vladimir V. Mazalov. Anna N. Rettieva In Game Theory and Applicaions, Volume X Edied by L.A. Perosjan and V.V. Mazalov, pp.97{10 ISBN 1-59033-34-X c 004 Nova Science Publishers, Inc. A FISHERY GAME MODEL WITH MIGRATION: RESERVED TERRITORY

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

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

Kinematics Vocabulary. Kinematics and One Dimensional Motion. Position. Coordinate System in One Dimension. Kinema means movement 8.

Kinematics Vocabulary. Kinematics and One Dimensional Motion. Position. Coordinate System in One Dimension. Kinema means movement 8. Kinemaics Vocabulary Kinemaics and One Dimensional Moion 8.1 WD1 Kinema means movemen Mahemaical descripion of moion Posiion Time Inerval Displacemen Velociy; absolue value: speed Acceleraion Averages

More information

Module 2 F c i k c s la l w a s o s f dif di fusi s o i n

Module 2 F c i k c s la l w a s o s f dif di fusi s o i n Module Fick s laws of diffusion Fick s laws of diffusion and hin film soluion Adolf Fick (1855) proposed: d J α d d d J (mole/m s) flu (m /s) diffusion coefficien and (mole/m 3 ) concenraion of ions, aoms

More information

Chapter 1 Fundamental Concepts

Chapter 1 Fundamental Concepts Chaper 1 Fundamenal Conceps 1 Signals A signal is a paern of variaion of a physical quaniy, ofen as a funcion of ime (bu also space, disance, posiion, ec). These quaniies are usually he independen variables

More information

CHE302 LECTURE IV MATHEMATICAL MODELING OF CHEMICAL PROCESS. Professor Dae Ryook Yang

CHE302 LECTURE IV MATHEMATICAL MODELING OF CHEMICAL PROCESS. Professor Dae Ryook Yang CHE302 LECTURE IV MATHEMATICAL MODELING OF CHEMICAL PROCESS Professor Dae Ryook Yang Fall 200 Dep. of Chemical and Biological Engineering Korea Universiy CHE302 Process Dynamics and Conrol Korea Universiy

More information

Fractional Method of Characteristics for Fractional Partial Differential Equations

Fractional Method of Characteristics for Fractional Partial Differential Equations Fracional Mehod of Characerisics for Fracional Parial Differenial Equaions Guo-cheng Wu* Modern Teile Insiue, Donghua Universiy, 188 Yan-an ilu Road, Shanghai 51, PR China Absrac The mehod of characerisics

More information

Math 2214 Solution Test 1A Spring 2016

Math 2214 Solution Test 1A Spring 2016 Mah 14 Soluion Tes 1A Spring 016 sec Problem 1: Wha is he larges -inerval for which ( 4) = has a guaraneed + unique soluion for iniial value (-1) = 3 according o he Exisence Uniqueness Theorem? Soluion

More information

6.003 Homework 1. Problems. Due at the beginning of recitation on Wednesday, February 10, 2010.

6.003 Homework 1. Problems. Due at the beginning of recitation on Wednesday, February 10, 2010. 6.003 Homework Due a he beginning of reciaion on Wednesday, February 0, 200. Problems. Independen and Dependen Variables Assume ha he heigh of a waer wave is given by g(x v) where x is disance, v is velociy,

More information

04. Kinetics of a second order reaction

04. Kinetics of a second order reaction 4. Kineics of a second order reacion Imporan conceps Reacion rae, reacion exen, reacion rae equaion, order of a reacion, firs-order reacions, second-order reacions, differenial and inegraed rae laws, Arrhenius

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

Ch.1. Group Work Units. Continuum Mechanics Course (MMC) - ETSECCPB - UPC

Ch.1. Group Work Units. Continuum Mechanics Course (MMC) - ETSECCPB - UPC Ch.. Group Work Unis Coninuum Mechanics Course (MMC) - ETSECCPB - UPC Uni 2 Jusify wheher he following saemens are rue or false: a) Two sreamlines, corresponding o a same insan of ime, can never inersec

More 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

( ) 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

Physics Notes - Ch. 2 Motion in One Dimension

Physics Notes - Ch. 2 Motion in One Dimension Physics Noes - Ch. Moion in One Dimension I. The naure o physical quaniies: scalars and ecors A. Scalar quaniy ha describes only magniude (how much), NOT including direcion; e. mass, emperaure, ime, olume,

More information

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

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

MA 214 Calculus IV (Spring 2016) Section 2. Homework Assignment 1 Solutions

MA 214 Calculus IV (Spring 2016) Section 2. Homework Assignment 1 Solutions MA 14 Calculus IV (Spring 016) Secion Homework Assignmen 1 Soluions 1 Boyce and DiPrima, p 40, Problem 10 (c) Soluion: In sandard form he given firs-order linear ODE is: An inegraing facor is given by

More information

di Bernardo, M. (1995). A purely adaptive controller to synchronize and control chaotic systems.

di Bernardo, M. (1995). A purely adaptive controller to synchronize and control chaotic systems. di ernardo, M. (995). A purely adapive conroller o synchronize and conrol chaoic sysems. hps://doi.org/.6/375-96(96)8-x Early version, also known as pre-prin Link o published version (if available):.6/375-96(96)8-x

More information

The fundamental mass balance equation is ( 1 ) where: I = inputs P = production O = outputs L = losses A = accumulation

The fundamental mass balance equation is ( 1 ) where: I = inputs P = production O = outputs L = losses A = accumulation Hea (iffusion) Equaion erivaion of iffusion Equaion The fundamenal mass balance equaion is I P O L A ( 1 ) where: I inpus P producion O oupus L losses A accumulaion Assume ha no chemical is produced or

More information

EECE251. Circuit Analysis I. Set 4: Capacitors, Inductors, and First-Order Linear Circuits

EECE251. Circuit Analysis I. Set 4: Capacitors, Inductors, and First-Order Linear Circuits EEE25 ircui Analysis I Se 4: apaciors, Inducors, and Firs-Order inear ircuis Shahriar Mirabbasi Deparmen of Elecrical and ompuer Engineering Universiy of Briish olumbia shahriar@ece.ubc.ca Overview Passive

More information

Signal and System (Chapter 3. Continuous-Time Systems)

Signal and System (Chapter 3. Continuous-Time Systems) Signal and Sysem (Chaper 3. Coninuous-Time Sysems) Prof. Kwang-Chun Ho kwangho@hansung.ac.kr Tel: 0-760-453 Fax:0-760-4435 1 Dep. Elecronics and Informaion Eng. 1 Nodes, Branches, Loops A nework wih b

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

v x + v 0 x v y + a y + v 0 y + 2a y + v y Today: Projectile motion Soccer problem Firefighter example

v x + v 0 x v y + a y + v 0 y + 2a y + v y Today: Projectile motion Soccer problem Firefighter example Thurs Sep 10 Assign 2 Friday SI Sessions: Moron 227 Mon 8:10-9:10 PM Tues 8:10-9:10 PM Thur 7:05-8:05 PM Read Read Draw/Image lay ou coordinae sysem Wha know? Don' know? Wan o know? Physical Processes?

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

f t te e = possesses a Laplace transform. Exercises for Module-III (Transform Calculus)

f t te e = possesses a Laplace transform. Exercises for Module-III (Transform Calculus) Exercises for Module-III (Transform Calculus) ) Discuss he piecewise coninuiy of he following funcions: =,, +, > c) e,, = d) sin,, = ) Show ha he funcion ( ) sin ( ) f e e = possesses a Laplace ransform.

More information

In this chapter the model of free motion under gravity is extended to objects projected at an angle. When you have completed it, you should

In this chapter the model of free motion under gravity is extended to objects projected at an angle. When you have completed it, you should Cambridge Universiy Press 978--36-60033-7 Cambridge Inernaional AS and A Level Mahemaics: Mechanics Coursebook Excerp More Informaion Chaper The moion of projeciles In his chaper he model of free moion

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

University of Cyprus Biomedical Imaging and Applied Optics. Appendix. DC Circuits Capacitors and Inductors AC Circuits Operational Amplifiers

University of Cyprus Biomedical Imaging and Applied Optics. Appendix. DC Circuits Capacitors and Inductors AC Circuits Operational Amplifiers Universiy of Cyprus Biomedical Imaging and Applied Opics Appendix DC Circuis Capaciors and Inducors AC Circuis Operaional Amplifiers Circui Elemens An elecrical circui consiss of circui elemens such as

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

Optimizing heat exchangers

Optimizing heat exchangers Opimizing hea echangers Jean-Luc Thiffeaul Deparmen of Mahemaics, Universiy of Wisconsin Madison, 48 Lincoln Dr., Madison, WI 5376, USA wih: Florence Marcoe, Charles R. Doering, William R. Young (Daed:

More information

The motions of the celt on a horizontal plane with viscous friction

The motions of the celt on a horizontal plane with viscous friction The h Join Inernaional Conference on Mulibody Sysem Dynamics June 8, 18, Lisboa, Porugal The moions of he cel on a horizonal plane wih viscous fricion Maria A. Munisyna 1 1 Moscow Insiue of Physics and

More information

Sliding Mode Controller for Unstable Systems

Sliding Mode Controller for Unstable Systems S. SIVARAMAKRISHNAN e al., Sliding Mode Conroller for Unsable Sysems, Chem. Biochem. Eng. Q. 22 (1) 41 47 (28) 41 Sliding Mode Conroller for Unsable Sysems S. Sivaramakrishnan, A. K. Tangirala, and M.

More information

Wall. x(t) f(t) x(t = 0) = x 0, t=0. which describes the motion of the mass in absence of any external forcing.

Wall. x(t) f(t) x(t = 0) = x 0, t=0. which describes the motion of the mass in absence of any external forcing. MECHANICS APPLICATIONS OF SECOND-ORDER ODES 7 Mechanics applicaions of second-order ODEs Second-order linear ODEs wih consan coefficiens arise in many physical applicaions. One physical sysems whose behaviour

More information

Chapter 2. Motion in One-Dimension I

Chapter 2. Motion in One-Dimension I Chaper 2. Moion in One-Dimension I Level : AP Physics Insrucor : Kim 1. Average Rae of Change and Insananeous Velociy To find he average velociy(v ) of a paricle, we need o find he paricle s displacemen

More information

ECE Spring Prof. David R. Jackson ECE Dept. Notes 20

ECE Spring Prof. David R. Jackson ECE Dept. Notes 20 ECE 6345 Spring 5 Prof. David R. Jacson ECE Dep. Noes Overview In his se of noes we apply he SDI mehod o invesigae he fields produced by a pach curren. We calculae he field due o a recangular pach on op

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

Silicon Controlled Rectifiers UNIT-1

Silicon Controlled Rectifiers UNIT-1 Silicon Conrolled Recifiers UNIT-1 Silicon Conrolled Recifier A Silicon Conrolled Recifier (or Semiconducor Conrolled Recifier) is a four layer solid sae device ha conrols curren flow The name silicon

More information

Economics 8105 Macroeconomic Theory Recitation 6

Economics 8105 Macroeconomic Theory Recitation 6 Economics 8105 Macroeconomic Theory Reciaion 6 Conor Ryan Ocober 11h, 2016 Ouline: Opimal Taxaion wih Governmen Invesmen 1 Governmen Expendiure in Producion In hese noes we will examine a model in which

More information

CONTROL SYSTEMS, ROBOTICS AND AUTOMATION Vol. XI Control of Stochastic Systems - P.R. Kumar

CONTROL SYSTEMS, ROBOTICS AND AUTOMATION Vol. XI Control of Stochastic Systems - P.R. Kumar CONROL OF SOCHASIC SYSEMS P.R. Kumar Deparmen of Elecrical and Compuer Engineering, and Coordinaed Science Laboraory, Universiy of Illinois, Urbana-Champaign, USA. Keywords: Markov chains, ransiion probabiliies,

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

ADVANCED MATHEMATICS FOR ECONOMICS /2013 Sheet 3: Di erential equations

ADVANCED MATHEMATICS FOR ECONOMICS /2013 Sheet 3: Di erential equations ADVANCED MATHEMATICS FOR ECONOMICS - /3 Shee 3: Di erenial equaions Check ha x() =± p ln(c( + )), where C is a posiive consan, is soluion of he ODE x () = Solve he following di erenial equaions: (a) x

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

CSE 3802 / ECE Numerical Methods in Scientific Computation. Jinbo Bi. Department of Computer Science & Engineering

CSE 3802 / ECE Numerical Methods in Scientific Computation. Jinbo Bi. Department of Computer Science & Engineering CSE 3802 / ECE 3431 Numerical Mehods in Scienific Compuaion Jinbo Bi Deparmen of Compuer Science & Engineering hp://www.engr.uconn.edu/~jinbo 1 Ph.D in Mahemaics The Insrucor Previous professional experience:

More information

Order Reduction of Large Scale DAE Models. J.D. Hedengren and T. F. Edgar Department of Chemical Engineering The University of Texas at Austin

Order Reduction of Large Scale DAE Models. J.D. Hedengren and T. F. Edgar Department of Chemical Engineering The University of Texas at Austin Order Reducion of Large Scale DAE Models J.D. Hedengren and T. F. Edgar Deparmen of Chemical Engineering The Universiy of Teas a Ausin 1 Ouline Moivaion Two Sep Process for DAE Model Reducion 1. Reducion

More information

t dt t SCLP Bellman (1953) CLP (Dantzig, Tyndall, Grinold, Perold, Anstreicher 60's-80's) Anderson (1978) SCLP

t dt t SCLP Bellman (1953) CLP (Dantzig, Tyndall, Grinold, Perold, Anstreicher 60's-80's) Anderson (1978) SCLP Coninuous Linear Programming. Separaed Coninuous Linear Programming Bellman (1953) max c () u() d H () u () + Gsusds (,) () a () u (), < < CLP (Danzig, yndall, Grinold, Perold, Ansreicher 6's-8's) Anderson

More information

Vanishing Viscosity Method. There are another instructive and perhaps more natural discontinuous solutions of the conservation law

Vanishing Viscosity Method. There are another instructive and perhaps more natural discontinuous solutions of the conservation law Vanishing Viscosiy Mehod. There are anoher insrucive and perhaps more naural disconinuous soluions of he conservaion law (1 u +(q(u x 0, he so called vanishing viscosiy mehod. This mehod consiss in viewing

More information

Theory of! Partial Differential Equations-I!

Theory of! Partial Differential Equations-I! hp://users.wpi.edu/~grear/me61.hml! Ouline! Theory o! Parial Dierenial Equaions-I! Gréar Tryggvason! Spring 010! Basic Properies o PDE!! Quasi-linear Firs Order Equaions! - Characerisics! - Linear and

More information

Math 115 Final Exam December 14, 2017

Math 115 Final Exam December 14, 2017 On my honor, as a suden, I have neiher given nor received unauhorized aid on his academic work. Your Iniials Only: Iniials: Do no wrie in his area Mah 5 Final Exam December, 07 Your U-M ID # (no uniqname):

More information

Math 4600: Homework 11 Solutions

Math 4600: Homework 11 Solutions Mah 46: Homework Soluions Gregory Handy [.] One of he well-known phenomenological (capuring he phenomena, bu no necessarily he mechanisms) models of cancer is represened by Gomperz equaion dn d = bn ln(n/k)

More information

AP CALCULUS AB 2003 SCORING GUIDELINES (Form B)

AP CALCULUS AB 2003 SCORING GUIDELINES (Form B) SCORING GUIDELINES (Form B) Quesion A ank conains 15 gallons of heaing oil a ime =. During he ime inerval 1 hours, heaing oil is pumped ino he ank a he rae 1 H ( ) = + ( 1 + ln( + 1) ) gallons per hour.

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

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

Electrical Circuits. 1. Circuit Laws. Tools Used in Lab 13 Series Circuits Damped Vibrations: Energy Van der Pol Circuit

Electrical Circuits. 1. Circuit Laws. Tools Used in Lab 13 Series Circuits Damped Vibrations: Energy Van der Pol Circuit V() R L C 513 Elecrical Circuis Tools Used in Lab 13 Series Circuis Damped Vibraions: Energy Van der Pol Circui A series circui wih an inducor, resisor, and capacior can be represened by Lq + Rq + 1, a

More information

Math 23 Spring Differential Equations. Final Exam Due Date: Tuesday, June 6, 5pm

Math 23 Spring Differential Equations. Final Exam Due Date: Tuesday, June 6, 5pm Mah Spring 6 Differenial Equaions Final Exam Due Dae: Tuesday, June 6, 5pm Your name (please prin): Insrucions: This is an open book, open noes exam. You are free o use a calculaor or compuer o check your

More information

R.#W.#Erickson# Department#of#Electrical,#Computer,#and#Energy#Engineering# University#of#Colorado,#Boulder#

R.#W.#Erickson# Department#of#Electrical,#Computer,#and#Energy#Engineering# University#of#Colorado,#Boulder# .#W.#Erickson# Deparmen#of#Elecrical,#Compuer,#and#Energy#Engineering# Universiy#of#Colorado,#Boulder# Chaper 2 Principles of Seady-Sae Converer Analysis 2.1. Inroducion 2.2. Inducor vol-second balance,

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

PROBLEMS FOR MATH 162 If a problem is starred, all subproblems are due. If only subproblems are starred, only those are due. SLOPES OF TANGENT LINES

PROBLEMS FOR MATH 162 If a problem is starred, all subproblems are due. If only subproblems are starred, only those are due. SLOPES OF TANGENT LINES PROBLEMS FOR MATH 6 If a problem is sarred, all subproblems are due. If onl subproblems are sarred, onl hose are due. 00. Shor answer quesions. SLOPES OF TANGENT LINES (a) A ball is hrown ino he air. Is

More information

Optimal Control. Lecture 5. Prof. Daniela Iacoviello

Optimal Control. Lecture 5. Prof. Daniela Iacoviello Opimal Conrol ecre 5 Pro. Daniela Iacoviello THESE SIDES ARE NOT SUFFICIENT FOR THE EXAM: YOU MUST STUDY ON THE BOOKS Par o he slides has been aken rom he Reerences indicaed below Pro. D.Iacoviello - Opimal

More information

Math 116 Second Midterm March 21, 2016

Math 116 Second Midterm March 21, 2016 Mah 6 Second Miderm March, 06 UMID: EXAM SOLUTIONS Iniials: Insrucor: Secion:. Do no open his exam unil you are old o do so.. Do no wrie your name anywhere on his exam. 3. This exam has pages including

More information