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

Size: px
Start display at page:

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

Transcription

1 SZG Macro 2011 Lecure 3: Dynamic Programming SZG macro 2011 lecure 3 1

2 Background Our previous discussion of opimal consumpion over ime and of opimal capial accumulaion sugges sudying he general decision problems on he nex pages, where c = conrol (consumpion) k = sae x = exogenous variable In each case, we migh solve he dynamic opimizaion problem using a discree ime opimal conrol approach as in prior lecures. SZG macro 2011 lecure 3 2

3 Finie horizon problem T å { c},{ k} b uk x c = 0 max (,, ) u: momenary objecive s.. k - k = g( k, x, c ) g : sae law of moion + 1 k k 0 ³ b( x ) T+ 1 T+ 1 SZG macro 2011 lecure 3 3

4 Infinie horizon problem å { c},{ k} b uk x c = 0 max (,, ) s.. k + - k = g( k, x, c ) = 0,1,... 1 k 0 SZG macro 2011 lecure 3 4

5 We migh aack he finie horizon problem by forming L = T å = 0 T å = 0 b u( k, x, c ) + bl[ k + g( k, x, c )-k ] + 1 +Q [ k - b( x )] T SZG macro 2011 lecure 3 5

6 We migh aack he infinie horizon problem by forming L = å = 0 å = 0 b u( k, x, c ) + bl[ k + g( k, x, c )-k ] + 1 SZG macro 2011 lecure 3 6

7 Eiher case Oucome is sequence of opimal conrol {c }, opimal sae {k }, and opimal shadow prices { } ha saisfy FOCs and TC give he pah {x }. Desirable because we have boh real oucomes and a means of deriving supporing prices. SZG macro 2011 lecure 3 7

8 Why? We will sudy an alernaive, dynamic programming, nex Alernaive ool for oolki DP is beer for cerain problems wih uncerainy DP logic applied in oher, equilibrium conexs LS: he imperialism of recursive mehods SZG macro 2011 lecure 3 8

9 Ouline 1. Cerainy opimizaion problem used o illusrae: a. Resricions on exogenous variables {x } b. Value funcion c. Policy funcion d. The Bellman equaion and an associaed Lagrangian e. The envelope heorem f. The Euler equaion SZG macro 2011 lecure 3 9

10 Ouline Con d 2. Adding uncerainy 3. Applicaions opimal consumpion over ime opimal consumpion under uncerainy. SZG macro 2011 lecure 3 10

11 1. A cerainy dynamic problem and he DP approach Maximize å = 0 b uk (, x, c) Subjec o k+ 1 - k = g( k, x, c) conrolled sae and x = x( V ) exogenous variable V = m( V - 1) exogenous sae SZG macro 2011 lecure 3 11

12 Wha s differen from background seup? Immediae jump o infinie horizon problem, no essenial bu maches presenaion in LS chaper (noe differences in noaion, hough). The exogenous (x) variable(s) are now funcions of a vecor of exogenous sae variables, which evolve according o a difference equaion (perhaps nonlinear, perhaps in a vecor). The laer is a key par of he vision of Richard Bellman, he invenor of DP: his experience in oher areas (such as difference equaions) led him o hink in erms of describing dynamics in erms of sae variables. SZG macro 2011 lecure 3 12

13 Recursive policies Suppose conrols are funcions of saes, c ( k, ) policy funcion k 1 k g( k, x, c) k g( k, x( ), ( k, )) Then, he sae vecor evolves according o a recursion k 1 k g( k, x( ), ( k, )) s 1 M( s) 1 m( ) ha can be used o generae fuure saes from given iniial condiions SZG macro 2011 lecure 3 13

14 Evaluaing he objecive Under any recursive policy, we can see ha all of he erms which ener in he objecive are a funcion of he iniial sae (s 0 ) so ha he objecive is also a funcion of he iniial sae å b = 0 = 0 uk (, x, c) = b uk (, x( V ), p( k, x( V ))) = Wk (, V ) = Ws ( ) å SZG macro 2011 lecure 3 14

15 Recursion for objecive under arbirary recursive policy Ws ( ; p) = ws ( ; p) + bws ( ; p) ws ( ; p) = ukx (, ( V), p( kx, ( V))) s + 1 = M( s ) SZG macro 2011 lecure 3 15

16 Noice he swich Given ha here is a policy funcion ( ), he objecive is now a funcion of he sae vecor. We have made he change we are now hinking in erms of funcions raher han sequences. Bu we haven opimized ye! We could be calculaing he objecive wih a very bad policy. SZG macro 2011 lecure 3 16

17 Bellman s core idea Subdivide complicaed ineremporal problems ino many wo period problems, in which he rade-off is beween he presen now and laer. Specifically, he idea was o find he opimal conrol and sae now, aking as given ha laer behavior would iself be opimal. SZG macro 2011 lecure 3 17

18 The Principle of Opimaliy An opimal policy has he propery ha, whaever he sae and opimal firs decision may be, he remaining decisions consiue an opimal policy wih respec o he sae originaing from he firs decisions Bellman (1957, pg. 83) SZG macro 2011 lecure 3 18

19 Following he principle, The naural maximizaion problem is max{ uc (, k, x( V )) + bv( k, V )} c, k s.. k = k + g( k, x, c ) V = m( V ) Where he righ hand side is he curren momenary objecive (u) plus he consequences (V) for he discouned objecive of behaving opimally in he fuure. SZG macro 2011 lecure 3 19

20 Noing ha ime does no ener in an essenial way We someimes wrie his as (wih meaning nex period) max{ uckx (,, ( V)) + bv( k', V')} ck, ' s.. k' = k + g( k, x( V), c) V' = m( V) So hen he Bellman equaion is wrien as ck, ' Vk (, V) = max{ uckx (,, ( V)) + bvk ( ', V')} s.. k' = k + g( k, x( V), c) V' = m( V) SZG macro 2011 lecure 3 20

21 Afer he maximizaion We know he opimal policy (which we will call as above, bu wih he proviso ha i is opimal) and can calculae he associaed value, so ha here is now a Bellman equaion of he form Vk (, V) = {((, up kv), kx, ()) V + bvk ( + gkx (, ( V), p( k, V)), V')} A funcional equaion is defined, colloquially, as an equaion whose unknowns are funcions. In our conex, he unknowns are he policy and value funcions. SZG macro 2011 lecure 3 21

22 How o do he opimizaion? You are free o choose, depending on he applicaion Someimes we ake he Euler roue, subsiuing in he consrain and maximizing direcly over k Oher imes we wan o use a Lagrange approach, puing a muliplier on he consrain governing k SZG macro 2011 lecure 3 22

23 The associaed Lagrangian Takes he form L { u( c, k, x( )) V( k', ')} [ k g( k, x( ), c) k'] The opimal policy, sae evoluion and relaed muliplier are obained by maximizing wih respec o c,k and minimizing wih respec o. Hence hese are all funcions of he sae variables. SZG macro 2011 lecure 3 23

24 For an opimum (off corners) We mus have L u(, c k, x()) g(, k x(),) c 0 c c c L V( k', ') 0 k' k' L [ k g( k, x( ), c) k'] 0 And, a he values which solve hese equaions, V=L SZG macro 2011 lecure 3 24

25 The envelope heorem (Benvenise-Scheinkman) Quesion: wha is he effec of an infiniessimal change in k on V? Answer: I is given by V u(, c k, x()) g(, k x(),) c [ 1] k k k when we evaluae a he opimal policy and he associaed muliplier. As in LS, his may also be wrien a form which does no involve V u( c, k, x( )) V( k', ') g( k, x( ), c) he muliplier, [ 1] k k k' k SZG macro 2011 lecure 3 25

26 Ouline of proof Nonrivial o show differeniabiliy of V Bu if we have his (as we will frequenly assume) hen V L u( c, k, x( )) c u( c, k, x( )) { } k k c k k V( k', ') k' k' k [ k g( k, x( ), c) k'] k g( kx, ( ), c) g( kx, ( ), c) c k' [1 ] [ ] k k k k While his looks ugly, all erms involving behavior are muliplied by coefficiens ha are se o zero by he FOCs. SZG macro 2011 lecure 3 26

27 Deails on ET V u( c, k, x( )) g( k, x( ), c) [1 ] k k k uckx (,, ( )) gckx (,, ( )) c { } c c k V( k', ') k' { } k' k { [ k g( k, x( ), c) k']} k SZG macro 2011 lecure 3 27

28 Ieraing on he Bellman Equaion Under specific condiions on he funcions u and g, he Bellman equaion has a unique, sricly concave (in k) soluion. Under hese condiions, i can be calculaed by considering he limi Vj 1 ( k, ) max c, k' { u( k, x( ), c) Vj( k', ')} s.. k' k g( k, x( ), c) These ieraions are inerpreable as calculaing he value funcions for a class of finie horizon problems, wih successively longer horizons. SZG macro 2011 lecure 3 28

29 3. A Sochasic dynamic problem and he DP approach Maximize å = 0 E{ b u( k, x, c )} ( k, V ) 0 0 Subjec o k+ 1 - k = g( k, x, c) and Markovian exogenous sae variables x = x( V ) (, V B) = prob( V Î B V = V) + 1 SZG macro 2011 lecure 3 29

30 Markov examples Markov chains (LS, Chaper 1) Linear sae space sysems Nonlinear difference equaions wih iid shocks, m(, e ) 1 1 We won be more explici unil necessary. Key poin: saes are enough o compue expecaions. SZG macro 2011 lecure 3 30

31 Bellman Equaion Uncerainy case is minor modificaion of cerainy case Vk (, V) = max{ uckx (,, ( V)) + bevk ( ', V') ( k, V)} ck, ' s.. k' = k + g( k, x( V), c) SZG macro 2011 lecure 3 31

32 Proceeding as above Lagrangian L {(, u c k, x()) EV( k', ') (, k )} [ k g( k, x( ), c) k'] FOCs ET is unchanged L u(, c k, x()) g(, k x(),) c c c c L EV( k', ') 0 k' k' L [ k g( k, x( ), c) k'] 0 0 SZG macro 2011 lecure 3 32

33 Implicaions for opimal policies Funcions of saes and sae evoluion c ( k, ) k k g( k, x( ), ( k, )) 1 ( k, ) Sae evoluion is now a larger Markov process. For example, s k k g( k, x( ), ( k, )) M( s, e ) m(, e 1) SZG macro 2011 lecure 3 33

34 Value Funcion Since c,k,x depend on saes, he value funcion also is V(s). I is he maximized RHS of he Bellman equaion. SZG macro 2011 lecure 3 34

35 Wha we ve covered in his lecure Inroducion o DP under cerainy Bellman Equaion Associaed Lagrangian FOCs and he ET DP wih exogenous variables ha are funcions of a Markov process (exogenous sae vecor) Wha follows: Opimal consumpion over ime via dynamic programming: calculaion of policy and value funcions in a simple case Seing up opimal consumpion problem wih uncerain income SZG macro 2011 lecure 3 35

36 3A. Opimal consumpion over ime Simple case (no k,x in u) å = 0 uc ( ) Accumulaion of asses b a = Ra [ + y -c ] + 1 y = y + r( y -y) + 1 And R=1 (level consumpion) SZG macro 2011 lecure 3 36

37 Bellman Equaion V( a, y) max { u( c) V( a', y')} ca, ' s.. a' R[ a y c] y' y ( y y) SZG macro 2011 lecure 3 37

38 Taking an Euler Roue 1 V( a, y) max ca, '{ u( a y a') V( a', y')} R s.. y' y ( y y) 1 1 V( a', y') EE :0 uc( a y a ') R R a' V( a, y) 1 ET : uc ( a y a ') a R SZG macro 2011 lecure 3 38

39 Learning abou consumpion Updae ET and inser in EE o ge 1 1 uc( a y a') uc( a' y' a'') c c' R R Suppose here is a linear policy funcion c ( y y) a y a c' ( y' y) a' y ( y y) R[ a y c] y a a ( y y) R[ a y ( y y) a] y a y a SZG macro 2011 lecure 3 39

40 Requiring c=c, we have equaions ha resric undeermined coefficiens ( y y) a y a ( y y) R[ a ( y y) y ( y y) a] y a y a Ry ( ) a R(1 ) R/[1 R] y y a y y a a R 1 a ar[1 a] a ( ) R y y a 1 (1 ) R SZG macro 2011 lecure 3 40

41 Economic Rules Consume he normal level of income (y) Consume he ineres from asse sock, leaving he asse sock unchanged period o period (excep as noed nex) Consume based on he presen value of deviaions from normal income, reaing his as if i were anoher source of wealh; allow variaions in asse posiion on his basis. SZG macro 2011 lecure 3 41

42 Could have goen hese rules more direcly 1 j 1 j j ( ) c a ( ) [ y ( y y)] R R j 0 j c a y ( y y ) R R R R 1 1 c y [ a ( y y)] R 1 R SZG macro 2011 lecure 3 42

43 Quesions & Answers If we could have goen hem more easily, hen why do we need DP? Because here are many problems ha we canno solve so easily and DP is a procedure for solving hem. Wha is he value funcion? V ( a, y ) ( ( )) 1 u a 1 y y y 1 1 R Easy o deermine in his case because c is consan over ime; V inheris properies of u Check: ake his v, inser in Bellman equaion as v, show opimal form c has specified form, show v has his form. R SZG macro 2011 lecure 3 43

44 3B. Opimal consumpion wih flucuaing income: seing up a DP Simple case (no k,x in u) å = 0 E{ b u( c )} s Accumulaion of asses (don necessarily resric R) a+ 1 = Ra [ + y -c] 0 Income process y( V ) V : Markov SZG macro 2011 lecure 3 44

45 One version of he Bellman equaion V( a, ) max {( u( c) EV( a', ')} ca, ' 1 s..[ a y( ) c a'] 0 R SZG macro 2011 lecure 3 45

46 FOCs and ET Make sure you can work hese ou following he recipe above, c: u ( c) 0 c 1 EV ( a ', ') a': E{ } 0 R a' 1 : [ a y( ) c a'] 0 R ET : EV ( a, ) a SZG macro 2011 lecure 3 46

47 Implicaions for policies Opimal consumpion depends on (a) wealh; and (b) he variables ha are useful for forecasing fuure income. ca (, ) Bu solving for his funcion is no longer easy. Raionalizes SL s discussion of numerical mehods, a opic ha we will consider furher laer. SZG macro 2011 lecure 3 47

48 Implicaion for value funcion Value funcion is objecive evaluaed a opimal consumpion policy, which is a funcion of a Markov process, so ha 0 V0 = å b p V 0 V0 = 0 Va (, ) E{ u( ( a, ))} ( a, ) Value funcion saisfies he Bellman funcional equaion. Va (, V) = max {( uc ( ) + EVa ( ', V')} ca, ' 1 s..[ a + y( V) -c- a' = 0] R = ( u( p( a, V)) + EV( Ra [ + y( V) -p( a, V)], V') ( a, V) SZG macro 2011 lecure 3 48

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

Essential Microeconomics : OPTIMAL CONTROL 1. Consider the following class of optimization problems

Essential Microeconomics : OPTIMAL CONTROL 1. Consider the following class of optimization problems Essenial Microeconomics -- 6.5: OPIMAL CONROL Consider he following class of opimizaion problems Max{ U( k, x) + U+ ( k+ ) k+ k F( k, x)}. { x, k+ } = In he language of conrol heory, he vecor k is he vecor

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

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

This document was generated at 7:34 PM, 07/27/09 Copyright 2009 Richard T. Woodward

This document was generated at 7:34 PM, 07/27/09 Copyright 2009 Richard T. Woodward his documen was generaed a 7:34 PM, 07/27/09 Copyrigh 2009 Richard. Woodward 15. Bang-bang and mos rapid approach problems AGEC 637 - Summer 2009 here are some problems for which he opimal pah does no

More information

Macroeconomic Theory Ph.D. Qualifying Examination Fall 2005 ANSWER EACH PART IN A SEPARATE BLUE BOOK. PART ONE: ANSWER IN BOOK 1 WEIGHT 1/3

Macroeconomic Theory Ph.D. Qualifying Examination Fall 2005 ANSWER EACH PART IN A SEPARATE BLUE BOOK. PART ONE: ANSWER IN BOOK 1 WEIGHT 1/3 Macroeconomic Theory Ph.D. Qualifying Examinaion Fall 2005 Comprehensive Examinaion UCLA Dep. of Economics You have 4 hours o complee he exam. There are hree pars o he exam. Answer all pars. Each par has

More information

Online Appendix to Solution Methods for Models with Rare Disasters

Online Appendix to Solution Methods for Models with Rare Disasters Online Appendix o Soluion Mehods for Models wih Rare Disasers Jesús Fernández-Villaverde and Oren Levinal In his Online Appendix, we presen he Euler condiions of he model, we develop he pricing Calvo block,

More information

E β t log (C t ) + M t M t 1. = Y t + B t 1 P t. B t 0 (3) v t = P tc t M t Question 1. Find the FOC s for an optimum in the agent s problem.

E β t log (C t ) + M t M t 1. = Y t + B t 1 P t. B t 0 (3) v t = P tc t M t Question 1. Find the FOC s for an optimum in the agent s problem. Noes, M. Krause.. Problem Se 9: Exercise on FTPL Same model as in paper and lecure, only ha one-period govenmen bonds are replaced by consols, which are bonds ha pay one dollar forever. I has curren marke

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

THE BELLMAN PRINCIPLE OF OPTIMALITY

THE BELLMAN PRINCIPLE OF OPTIMALITY THE BELLMAN PRINCIPLE OF OPTIMALITY IOANID ROSU As I undersand, here are wo approaches o dynamic opimizaion: he Ponrjagin Hamilonian) approach, and he Bellman approach. I saw several clear discussions

More information

ANSWERS TO EVEN NUMBERED EXERCISES IN CHAPTER 6 SECTION 6.1: LIFE CYCLE CONSUMPTION AND WEALTH T 1. . Let ct. ) is a strictly concave function of c

ANSWERS TO EVEN NUMBERED EXERCISES IN CHAPTER 6 SECTION 6.1: LIFE CYCLE CONSUMPTION AND WEALTH T 1. . Let ct. ) is a strictly concave function of c John Riley December 00 S O EVEN NUMBERED EXERCISES IN CHAPER 6 SECION 6: LIFE CYCLE CONSUMPION AND WEALH Eercise 6-: Opimal saving wih more han one commodiy A consumer has a period uiliy funcion δ u (

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

RANDOM LAGRANGE MULTIPLIERS AND TRANSVERSALITY

RANDOM LAGRANGE MULTIPLIERS AND TRANSVERSALITY ECO 504 Spring 2006 Chris Sims RANDOM LAGRANGE MULTIPLIERS AND TRANSVERSALITY 1. INTRODUCTION Lagrange muliplier mehods are sandard fare in elemenary calculus courses, and hey play a cenral role in economic

More information

The Brock-Mirman Stochastic Growth Model

The Brock-Mirman Stochastic Growth Model c December 3, 208, Chrisopher D. Carroll BrockMirman The Brock-Mirman Sochasic Growh Model Brock and Mirman (972) provided he firs opimizing growh model wih unpredicable (sochasic) shocks. The social planner

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

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

Problem Set 5. Graduate Macro II, Spring 2017 The University of Notre Dame Professor Sims

Problem Set 5. Graduate Macro II, Spring 2017 The University of Notre Dame Professor Sims Problem Se 5 Graduae Macro II, Spring 2017 The Universiy of Nore Dame Professor Sims Insrucions: You may consul wih oher members of he class, bu please make sure o urn in your own work. Where applicable,

More information

Midterm Exam. Macroeconomic Theory (ECON 8105) Larry Jones. Fall September 27th, Question 1: (55 points)

Midterm Exam. Macroeconomic Theory (ECON 8105) Larry Jones. Fall September 27th, Question 1: (55 points) Quesion 1: (55 poins) Macroeconomic Theory (ECON 8105) Larry Jones Fall 2016 Miderm Exam Sepember 27h, 2016 Consider an economy in which he represenaive consumer lives forever. There is a good in each

More information

Linear Dynamic Models

Linear Dynamic Models Linear Dnamic Models and Forecasing Reference aricle: Ineracions beween he muliplier analsis and he principle of acceleraion Ouline. The sae space ssem as an approach o working wih ssems of difference

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

23.2. Representing Periodic Functions by Fourier Series. Introduction. Prerequisites. Learning Outcomes

23.2. Representing Periodic Functions by Fourier Series. Introduction. Prerequisites. Learning Outcomes Represening Periodic Funcions by Fourier Series 3. Inroducion In his Secion we show how a periodic funcion can be expressed as a series of sines and cosines. We begin by obaining some sandard inegrals

More information

Reserves measures have an economic component eg. what could be extracted at current prices?

Reserves measures have an economic component eg. what could be extracted at current prices? 3.2 Non-renewable esources A. Are socks of non-renewable resources fixed? eserves measures have an economic componen eg. wha could be exraced a curren prices? - Locaion and quaniies of reserves of resources

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 :37 PM, 1/11/018 Copyrigh 018 Richard T. Woodward 1. An inroducion o dynamic opimiaion -- Opimal Conrol and Dynamic Programming AGEC 64-018 I. Overview of opimiaion Opimiaion

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

( ) 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

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

FINM 6900 Finance Theory

FINM 6900 Finance Theory FINM 6900 Finance Theory Universiy of Queensland Lecure Noe 4 The Lucas Model 1. Inroducion In his lecure we consider a simple endowmen economy in which an unspecified number of raional invesors rade asses

More information

Section 7.4 Modeling Changing Amplitude and Midline

Section 7.4 Modeling Changing Amplitude and Midline 488 Chaper 7 Secion 7.4 Modeling Changing Ampliude and Midline While sinusoidal funcions can model a variey of behaviors, i is ofen necessary o combine sinusoidal funcions wih linear and exponenial curves

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

O Q L N. Discrete-Time Stochastic Dynamic Programming. I. Notation and basic assumptions. ε t : a px1 random vector of disturbances at time t.

O Q L N. Discrete-Time Stochastic Dynamic Programming. I. Notation and basic assumptions. ε t : a px1 random vector of disturbances at time t. Econ. 5b Spring 999 C. Sims Discree-Time Sochasic Dynamic Programming 995, 996 by Chrisopher Sims. This maerial may be freely reproduced for educaional and research purposes, so long as i is no alered,

More information

Introduction D P. r = constant discount rate, g = Gordon Model (1962): constant dividend growth rate.

Introduction D P. r = constant discount rate, g = Gordon Model (1962): constant dividend growth rate. Inroducion Gordon Model (1962): D P = r g r = consan discoun rae, g = consan dividend growh rae. If raional expecaions of fuure discoun raes and dividend growh vary over ime, so should he D/P raio. Since

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

Section 3.5 Nonhomogeneous Equations; Method of Undetermined Coefficients

Section 3.5 Nonhomogeneous Equations; Method of Undetermined Coefficients Secion 3.5 Nonhomogeneous Equaions; Mehod of Undeermined Coefficiens Key Terms/Ideas: Linear Differenial operaor Nonlinear operaor Second order homogeneous DE Second order nonhomogeneous DE Soluion o homogeneous

More information

Seminar 4: Hotelling 2

Seminar 4: Hotelling 2 Seminar 4: Hoelling 2 November 3, 211 1 Exercise Par 1 Iso-elasic demand A non renewable resource of a known sock S can be exraced a zero cos. Demand for he resource is of he form: D(p ) = p ε ε > A a

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

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

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

Solutions Problem Set 3 Macro II (14.452)

Solutions Problem Set 3 Macro II (14.452) Soluions Problem Se 3 Macro II (14.452) Francisco A. Gallego 04/27/2005 1 Q heory of invesmen in coninuous ime and no uncerainy Consider he in nie horizon model of a rm facing adjusmen coss o invesmen.

More information

Graduate Macro Theory II: Notes on Neoclassical Growth Model

Graduate Macro Theory II: Notes on Neoclassical Growth Model Graduae Macro Theory II: Noes on Neoclassical Growh Model Eric Sims Universiy of Nore Dame Spring 2015 1 Basic Neoclassical Growh Model The economy is populaed by a large number of infiniely lived agens.

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

Diebold, Chapter 7. Francis X. Diebold, Elements of Forecasting, 4th Edition (Mason, Ohio: Cengage Learning, 2006). Chapter 7. Characterizing Cycles

Diebold, Chapter 7. Francis X. Diebold, Elements of Forecasting, 4th Edition (Mason, Ohio: Cengage Learning, 2006). Chapter 7. Characterizing Cycles Diebold, Chaper 7 Francis X. Diebold, Elemens of Forecasing, 4h Ediion (Mason, Ohio: Cengage Learning, 006). Chaper 7. Characerizing Cycles Afer compleing his reading you should be able o: Define covariance

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

1 Answers to Final Exam, ECN 200E, Spring

1 Answers to Final Exam, ECN 200E, Spring 1 Answers o Final Exam, ECN 200E, Spring 2004 1. A good answer would include he following elemens: The equiy premium puzzle demonsraed ha wih sandard (i.e ime separable and consan relaive risk aversion)

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

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

Inventory Analysis and Management. Multi-Period Stochastic Models: Optimality of (s, S) Policy for K-Convex Objective Functions

Inventory Analysis and Management. Multi-Period Stochastic Models: Optimality of (s, S) Policy for K-Convex Objective Functions Muli-Period Sochasic Models: Opimali of (s, S) Polic for -Convex Objecive Funcions Consider a seing similar o he N-sage newsvendor problem excep ha now here is a fixed re-ordering cos (> 0) for each (re-)order.

More information

Lecture Notes 3: Quantitative Analysis in DSGE Models: New Keynesian Model

Lecture Notes 3: Quantitative Analysis in DSGE Models: New Keynesian Model Lecure Noes 3: Quaniaive Analysis in DSGE Models: New Keynesian Model Zhiwei Xu, Email: xuzhiwei@sju.edu.cn The moneary policy plays lile role in he basic moneary model wihou price sickiness. We now urn

More information

Chapter #1 EEE8013 EEE3001. Linear Controller Design and State Space Analysis

Chapter #1 EEE8013 EEE3001. Linear Controller Design and State Space Analysis Chaper EEE83 EEE3 Chaper # EEE83 EEE3 Linear Conroller Design and Sae Space Analysis Ordinary Differenial Equaions.... Inroducion.... Firs Order ODEs... 3. Second Order ODEs... 7 3. General Maerial...

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

A Dynamic Model of Economic Fluctuations

A Dynamic Model of Economic Fluctuations CHAPTER 15 A Dynamic Model of Economic Flucuaions Modified for ECON 2204 by Bob Murphy 2016 Worh Publishers, all righs reserved IN THIS CHAPTER, OU WILL LEARN: how o incorporae dynamics ino he AD-AS model

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

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

Chapter 6. Systems of First Order Linear Differential Equations

Chapter 6. Systems of First Order Linear Differential Equations Chaper 6 Sysems of Firs Order Linear Differenial Equaions We will only discuss firs order sysems However higher order sysems may be made ino firs order sysems by a rick shown below We will have a sligh

More information

Chapter 4 Introduction to Dynamic Programming

Chapter 4 Introduction to Dynamic Programming Chaper 4 Inroducion o Dynamic Programming An approach o solving dynamic opimizaion problems alernaive o opimal conrol was pioneered by Richard Bellman beginning in he lae 1950s Bellman emphasized he economic

More information

Policy regimes Theory

Policy regimes Theory Advanced Moneary Theory and Policy EPOS 2012/13 Policy regimes Theory Giovanni Di Barolomeo giovanni.dibarolomeo@uniroma1.i The moneary policy regime The simple model: x = - s (i - p e ) + x e + e D p

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

Introduction to choice over time

Introduction to choice over time Microeconomic Theory -- Choice over ime Inroducion o choice over ime Individual choice Income and subsiuion effecs 7 Walrasian equilibrium ineres rae 9 pages John Riley Ocober 9, 08 Microeconomic Theory

More information

Application of a Stochastic-Fuzzy Approach to Modeling Optimal Discrete Time Dynamical Systems by Using Large Scale Data Processing

Application of a Stochastic-Fuzzy Approach to Modeling Optimal Discrete Time Dynamical Systems by Using Large Scale Data Processing Applicaion of a Sochasic-Fuzzy Approach o Modeling Opimal Discree Time Dynamical Sysems by Using Large Scale Daa Processing AA WALASZE-BABISZEWSA Deparmen of Compuer Engineering Opole Universiy of Technology

More information

ODEs II, Lecture 1: Homogeneous Linear Systems - I. Mike Raugh 1. March 8, 2004

ODEs II, Lecture 1: Homogeneous Linear Systems - I. Mike Raugh 1. March 8, 2004 ODEs II, Lecure : Homogeneous Linear Sysems - I Mike Raugh March 8, 4 Inroducion. In he firs lecure we discussed a sysem of linear ODEs for modeling he excreion of lead from he human body, saw how o ransform

More information

Problem Set on Differential Equations

Problem Set on Differential Equations Problem Se on Differenial Equaions 1. Solve he following differenial equaions (a) x () = e x (), x () = 3/ 4. (b) x () = e x (), x (1) =. (c) xe () = + (1 x ()) e, x () =.. (An asse marke model). Le p()

More information

UNIVERSITY OF OSLO DEPARTMENT OF ECONOMICS

UNIVERSITY OF OSLO DEPARTMENT OF ECONOMICS UNIVERSITY OF OSLO DEPARTMENT OF ECONOMICS Exam: ECON4325 Moneary Policy Dae of exam: Tuesday, May 24, 206 Grades are given: June 4, 206 Time for exam: 2.30 p.m. 5.30 p.m. The problem se covers 5 pages

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

2.7. Some common engineering functions. Introduction. Prerequisites. Learning Outcomes

2.7. Some common engineering functions. Introduction. Prerequisites. Learning Outcomes Some common engineering funcions 2.7 Inroducion This secion provides a caalogue of some common funcions ofen used in Science and Engineering. These include polynomials, raional funcions, he modulus funcion

More information

1 Consumption and Risky Assets

1 Consumption and Risky Assets Soluions o Problem Se 8 Econ 0A - nd Half - Fall 011 Prof David Romer, GSI: Vicoria Vanasco 1 Consumpion and Risky Asses Consumer's lifeime uiliy: U = u(c 1 )+E[u(c )] Income: Y 1 = Ȳ cerain and Y F (

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

23.5. Half-Range Series. Introduction. Prerequisites. Learning Outcomes

23.5. Half-Range Series. Introduction. Prerequisites. Learning Outcomes Half-Range Series 2.5 Inroducion In his Secion we address he following problem: Can we find a Fourier series expansion of a funcion defined over a finie inerval? Of course we recognise ha such a funcion

More information

Chapter 15: Phenomena. Chapter 15 Chemical Kinetics. Reaction Rates. Reaction Rates R P. Reaction Rates. Rate Laws

Chapter 15: Phenomena. Chapter 15 Chemical Kinetics. Reaction Rates. Reaction Rates R P. Reaction Rates. Rate Laws Chaper 5: Phenomena Phenomena: The reacion (aq) + B(aq) C(aq) was sudied a wo differen emperaures (98 K and 35 K). For each emperaure he reacion was sared by puing differen concenraions of he 3 species

More information

8. Basic RL and RC Circuits

8. Basic RL and RC Circuits 8. Basic L and C Circuis This chaper deals wih he soluions of he responses of L and C circuis The analysis of C and L circuis leads o a linear differenial equaion This chaper covers he following opics

More 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

T L. t=1. Proof of Lemma 1. Using the marginal cost accounting in Equation(4) and standard arguments. t )+Π RB. t )+K 1(Q RB

T L. t=1. Proof of Lemma 1. Using the marginal cost accounting in Equation(4) and standard arguments. t )+Π RB. t )+K 1(Q RB Elecronic Companion EC.1. Proofs of Technical Lemmas and Theorems LEMMA 1. Le C(RB) be he oal cos incurred by he RB policy. Then we have, T L E[C(RB)] 3 E[Z RB ]. (EC.1) Proof of Lemma 1. Using he marginal

More information

Lecture Notes 2. The Hilbert Space Approach to Time Series

Lecture Notes 2. The Hilbert Space Approach to Time Series Time Series Seven N. Durlauf Universiy of Wisconsin. Basic ideas Lecure Noes. The Hilber Space Approach o Time Series The Hilber space framework provides a very powerful language for discussing he relaionship

More information

Cooperative Ph.D. Program in School of Economic Sciences and Finance QUALIFYING EXAMINATION IN MACROECONOMICS. August 8, :45 a.m. to 1:00 p.m.

Cooperative Ph.D. Program in School of Economic Sciences and Finance QUALIFYING EXAMINATION IN MACROECONOMICS. August 8, :45 a.m. to 1:00 p.m. Cooperaive Ph.D. Program in School of Economic Sciences and Finance QUALIFYING EXAMINATION IN MACROECONOMICS Augus 8, 213 8:45 a.m. o 1: p.m. THERE ARE FIVE QUESTIONS ANSWER ANY FOUR OUT OF FIVE PROBLEMS.

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

Problem 1 / 25 Problem 2 / 20 Problem 3 / 10 Problem 4 / 15 Problem 5 / 30 TOTAL / 100

Problem 1 / 25 Problem 2 / 20 Problem 3 / 10 Problem 4 / 15 Problem 5 / 30 TOTAL / 100 eparmen of Applied Economics Johns Hopkins Universiy Economics 602 Macroeconomic Theory and Policy Miderm Exam Suggesed Soluions Professor Sanjay hugh Fall 2008 NAME: The Exam has a oal of five (5) problems

More information

Math 2142 Exam 1 Review Problems. x 2 + f (0) 3! for the 3rd Taylor polynomial at x = 0. To calculate the various quantities:

Math 2142 Exam 1 Review Problems. x 2 + f (0) 3! for the 3rd Taylor polynomial at x = 0. To calculate the various quantities: Mah 4 Eam Review Problems Problem. Calculae he 3rd Taylor polynomial for arcsin a =. Soluion. Le f() = arcsin. For his problem, we use he formula f() + f () + f ()! + f () 3! for he 3rd Taylor polynomial

More information

Suggested Solutions to Assignment 4 (REQUIRED) Submisson Deadline and Location: March 27 in Class

Suggested Solutions to Assignment 4 (REQUIRED) Submisson Deadline and Location: March 27 in Class EC 450 Advanced Macroeconomics Insrucor: Sharif F Khan Deparmen of Economics Wilfrid Laurier Universiy Winer 2008 Suggesed Soluions o Assignmen 4 (REQUIRED) Submisson Deadline and Locaion: March 27 in

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

Solutions from Chapter 9.1 and 9.2

Solutions from Chapter 9.1 and 9.2 Soluions from Chaper 9 and 92 Secion 9 Problem # This basically boils down o an exercise in he chain rule from calculus We are looking for soluions of he form: u( x) = f( k x c) where k x R 3 and k is

More information

CHAPTER 12 DIRECT CURRENT CIRCUITS

CHAPTER 12 DIRECT CURRENT CIRCUITS CHAPTER 12 DIRECT CURRENT CIUITS DIRECT CURRENT CIUITS 257 12.1 RESISTORS IN SERIES AND IN PARALLEL When wo resisors are conneced ogeher as shown in Figure 12.1 we said ha hey are conneced in series. As

More 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

Announcements: Warm-up Exercise:

Announcements: Warm-up Exercise: Fri Apr 13 7.1 Sysems of differenial equaions - o model muli-componen sysems via comparmenal analysis hp//en.wikipedia.org/wiki/muli-comparmen_model Announcemens Warm-up Exercise Here's a relaively simple

More information

Two Popular Bayesian Estimators: Particle and Kalman Filters. McGill COMP 765 Sept 14 th, 2017

Two Popular Bayesian Estimators: Particle and Kalman Filters. McGill COMP 765 Sept 14 th, 2017 Two Popular Bayesian Esimaors: Paricle and Kalman Filers McGill COMP 765 Sep 14 h, 2017 1 1 1, dx x Bel x u x P x z P Recall: Bayes Filers,,,,,,, 1 1 1 1 u z u x P u z u x z P Bayes z = observaion u =

More information

EE 315 Notes. Gürdal Arslan CLASS 1. (Sections ) What is a signal?

EE 315 Notes. Gürdal Arslan CLASS 1. (Sections ) What is a signal? EE 35 Noes Gürdal Arslan CLASS (Secions.-.2) Wha is a signal? In his class, a signal is some funcion of ime and i represens how some physical quaniy changes over some window of ime. Examples: velociy of

More information

This document was generated at 4:25 PM, 03/29/18 Copyright 2018 Richard T. Woodward

This document was generated at 4:25 PM, 03/29/18 Copyright 2018 Richard T. Woodward his documen was generaed a 4:25 PM, 3/29/8 Copyrigh 28 Richard. Woodward 4. Opimal conrol wih consrains and MRAP problems AGEC 642-28 We now reurn o an opimal conrol approach o dynamic opimizaion. his

More information

Chapter #1 EEE8013 EEE3001. Linear Controller Design and State Space Analysis

Chapter #1 EEE8013 EEE3001. Linear Controller Design and State Space Analysis Chaper EEE83 EEE3 Chaper # EEE83 EEE3 Linear Conroller Design and Sae Space Analysis Ordinary Differenial Equaions.... Inroducion.... Firs Order ODEs... 3. Second Order ODEs... 7 3. General Maerial...

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

Hamilton- J acobi Equation: Explicit Formulas In this lecture we try to apply the method of characteristics to the Hamilton-Jacobi equation: u t

Hamilton- J acobi Equation: Explicit Formulas In this lecture we try to apply the method of characteristics to the Hamilton-Jacobi equation: u t M ah 5 2 7 Fall 2 0 0 9 L ecure 1 0 O c. 7, 2 0 0 9 Hamilon- J acobi Equaion: Explici Formulas In his lecure we ry o apply he mehod of characerisics o he Hamilon-Jacobi equaion: u + H D u, x = 0 in R n

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

Reading from Young & Freedman: For this topic, read sections 25.4 & 25.5, the introduction to chapter 26 and sections 26.1 to 26.2 & 26.4.

Reading from Young & Freedman: For this topic, read sections 25.4 & 25.5, the introduction to chapter 26 and sections 26.1 to 26.2 & 26.4. PHY1 Elecriciy Topic 7 (Lecures 1 & 11) Elecric Circuis n his opic, we will cover: 1) Elecromoive Force (EMF) ) Series and parallel resisor combinaions 3) Kirchhoff s rules for circuis 4) Time dependence

More information

t is a basis for the solution space to this system, then the matrix having these solutions as columns, t x 1 t, x 2 t,... x n t x 2 t...

t is a basis for the solution space to this system, then the matrix having these solutions as columns, t x 1 t, x 2 t,... x n t x 2 t... Mah 228- Fri Mar 24 5.6 Marix exponenials and linear sysems: The analogy beween firs order sysems of linear differenial equaions (Chaper 5) and scalar linear differenial equaions (Chaper ) is much sronger

More information

Y 0.4Y 0.45Y Y to a proper ARMA specification.

Y 0.4Y 0.45Y Y to a proper ARMA specification. HG Jan 04 ECON 50 Exercises II - 0 Feb 04 (wih answers Exercise. Read secion 8 in lecure noes 3 (LN3 on he common facor problem in ARMA-processes. Consider he following process Y 0.4Y 0.45Y 0.5 ( where

More 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

1. Consider a pure-exchange economy with stochastic endowments. The state of the economy

1. Consider a pure-exchange economy with stochastic endowments. The state of the economy Answer 4 of he following 5 quesions. 1. Consider a pure-exchange economy wih sochasic endowmens. The sae of he economy in period, 0,1,..., is he hisory of evens s ( s0, s1,..., s ). The iniial sae is given.

More information

The Brock-Mirman Stochastic Growth Model

The Brock-Mirman Stochastic Growth Model c November 20, 207, Chrisopher D. Carroll BrockMirman The Brock-Mirman Sochasic Growh Model Brock and Mirman (972) provided he firs opimizing growh model wih unpredicable (sochasic) shocks. The social

More information

Math 334 Fall 2011 Homework 11 Solutions

Math 334 Fall 2011 Homework 11 Solutions Dec. 2, 2 Mah 334 Fall 2 Homework Soluions Basic Problem. Transform he following iniial value problem ino an iniial value problem for a sysem: u + p()u + q() u g(), u() u, u () v. () Soluion. Le v u. Then

More information

) were both constant and we brought them from under the integral.

) were both constant and we brought them from under the integral. YIELD-PER-RECRUIT (coninued The yield-per-recrui model applies o a cohor, bu we saw in he Age Disribuions lecure ha he properies of a cohor do no apply in general o a collecion of cohors, which is wha

More information

d 1 = c 1 b 2 - b 1 c 2 d 2 = c 1 b 3 - b 1 c 3

d 1 = c 1 b 2 - b 1 c 2 d 2 = c 1 b 3 - b 1 c 3 and d = c b - b c c d = c b - b c c This process is coninued unil he nh row has been compleed. The complee array of coefficiens is riangular. Noe ha in developing he array an enire row may be divided or

More information

Echocardiography Project and Finite Fourier Series

Echocardiography Project and Finite Fourier Series Echocardiography Projec and Finie Fourier Series 1 U M An echocardiagram is a plo of how a porion of he hear moves as he funcion of ime over he one or more hearbea cycles If he hearbea repeas iself every

More information

Seminar 5 Sustainability

Seminar 5 Sustainability Seminar 5 Susainabiliy Soluions Quesion : Hyperbolic Discouning -. Suppose a faher inheris a family forune of 0 million NOK an he wans o use some of i for himself (o be precise, he share ) bu also o beques

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