The primal versus the dual approach to the optimal Ramsey tax problem

Size: px
Start display at page:

Download "The primal versus the dual approach to the optimal Ramsey tax problem"

Transcription

1 The primal versus he dual approah o he opimal Ramsey ax prolem y George Eonomides a, Aposolis Philippopoulos,, and Vangelis Vassilaos a Deparmen of Inernaional and European Eonomi Sudies, Ahens Universiy of Eonomis and Business, 76 Paission sree, Ahens 434, Greee. Deparmen of Eonomis, Ahens Universiy of Eonomis and Business, 76 Paission sree, Ahens 434, Greee. ESifo, Munih, Germany. April, 28 Asra: There are wo soluion approahes o he dynami opimal puli finane (also nown as Ramsey prolem: he primal and he dual. Mos papers ha have fully solved a Ramsey prolem (y full soluion, we also mean a quaniaive soluion of poliies and ouomes aross differen ax regimes have used he primal approah; his is eause i is simpler han he dual. This paper fully solves a Ramsey poliy prolem y applying oh approahes, and ompares hem. JEL: H2; O4. eywords: Dynami opimal axaion; Endogenous growh. orresponding auhor. Tel: Fax: aphil@aue.gr Anowledgemens: We han Marios Angeleos, evin Lansing, Theodore Palivos and Hyun Par for ommens. Any errors are ours.

2 . Inroduion The dynami opimal puli finane prolem, referred o as Ramsey prolem, is one of he mos fundamenal and influenial eonomi prolems. In his prolem, he governmen hooses is axde poliy mix o maximize he household s welfare y aing ino aoun he equilirium reaion of privae agens o he ax poliy. A eleraed resul is ha he ax rae on (apial inome should e high in he iniial periods and hen roughly zero (see hamley, 986, and Judd, 985. Two approahes have een used o solve his prolem: he primal and he dual. In he primal, we eliminae axes and pries, so ha he governmen an e hough as direly using he quaniies as onrols. In he dual, he governmen uses he ax raes or pries as onrols. Mos papers ha have fully solved he Ramsey prolem (y full soluion, we mean no only he aove eleraed qualiaive resul, u also a quaniaive soluion of poliies and ouomes aross differen ax regimes 2 have used he primal approah. We are no aware of a full soluion o a dual prolem. This is eause, as is widely reognized (see e.g. Jones e al., 997, p. 99, he primal is onsideraly simpler han he dual. 3 This paper fully solves a Ramsey ax poliy prolem y applying oh approahes, and ompares hem. To mae he analysis lear and raale, we hoose a simple seup. The model is as in he lieraure exep ha we use a single inome ax and a linear A produion ehnology. The former is no imporan eause an inome ax inheris he feaures of a apial inome ax. The A ehnology has he advanage ha here are no ransiion dynamis wihin eah ax poliy regime; his redues he omplexiy of he Ramsey prolem wihou affeing he ey poins. As is nown, here are hree ax poliy regimes: an iniial period during whih he ax rae is exogenously given; he period(s of relaively heavy hosen ax raes; and he laer period(s of hosen zero ax raes. We will herefore presen hree suses of equaions assoiaed wih hese hree regimes and show how he hree suses are ineronneed o give a sysem of equaions ha haraerizes he full Ramsey prolem. Beyond his, we will solve he Ramsey sysem numerially. We will do so under oh he primal and he dual approah. See e.g. Ljungqvis and Sargen (2, haper 2 for a reen review of he lieraure. The opimal long-run ax rae an e differen from zero if here are imperfeions. Bu he ey logi remains: i is opimal o heavily ax inelasially supplied inpus. 2 As Ljungqvis and Sargen (2, p. 349 poin ou, a qualiaive analysis provides imporan insighs u anno yield definie resuls. Wha is he value of he non-zero ax rae(s in he iniial period(s? Wha is for onsumpion, growh, e, aross differen ax regimes? These quesions have o e sudied numerially. 3 In he Ramsey prolem, irrespeively of he soluion approah used, one anno solve firs for he long run and in urn sudy he ransiion period, as is ypially he ase in growh models. Insead, one has o solve simulaneously for he long run and he whole opimal pah. hari e al. (994 were he firs ones who oained numerial resuls y applying he primal approah. Bu, as far as we now, here are no analogous resuls y applying he dual approah (hamley, 986, p. 68, has provided a seh of a full dual soluion.

3 The main resuls are as follows. The dual prolem is indeed more omplex o solve (in erms of equaions and unnowns. I is hene harder o find ranges of parameer values, iniial ondiions and exogenous governmen spending ha yield a dual soluion. The primal soluion is easier o oain. This an parly explain he la of full, numerial soluions o he dual prolem. Neverheless, given a soluion, he wo approahes give idenial resuls along he whole opimal pah as expeed. 4 The res of he paper is as follows. Seion 2 presens he eonomy and solves for is ompeiive equilirium. Seion 3 solves he Ramsey poliy prolem y using he primal approah, while Seion 4 uses he dual approah. Seion 5 onludes. 2. ompeiive equilirium 2. Desripion of he eonomy and how we are going o wor onsider a losed eonomy wih an individual agen and a governmen. The individual onsumes, saves in he form of apial and governmen onds, and produes a single good aording o a linear A produion ehnology. The governmen imposes an inome ax and issues onds o finane puli servies, where he laer ener he individual s uiliy funion. We assume disree ime, infinie ime-horizons and perfe foresigh. The governmen is enevolen and hooses he pah of he ax rae one-and-for-all a ime y aing ino aoun he ompeiive equilirium. 5 Afer we presen he ompeiive equilirium, we solve he primal prolem. The dual will follow nex. This is for onveniene. 2.2 Individuals Using for simpliiy a log-linear uiliy funion, he individual maximizes: β [ ν ln ( ν ln H ] ( where and H are respeively privae onsumpion and puli onsumpion a, < β < is he disoun rae and <ν < is he weigh given o privae relaive o puli onsumpion. The wihin-period udge onsrain is: 4 Solving he prolem also under he dual approah is no only for inelleual uriosiy. In addiion o he ig numer of papers ha have used he dual approah o ge qualiaive resuls, here are ases (in riher seups where i is no possile o redue he onsrains o he Ramsey prolem ino a simple implemenailiy (udge onsrain and a resoure equaion. 5 Following mos of he lieraure, we assume ha governmen expendiure is exogenous. Our main resuls do no hange if governmen expendiure is also hosen opimally (resuls are availale upon reques. 2

4 B B ( τ A( B (2 where is end-of-period apial, B is end-of-period onds, τ < is he ax rae a and A > is a parameer. We assume for simpliiy ha apial and onds pay he same gross reurn, A, and are axed a he same rae, τ. We also assume zero apial depreiaion. The iniial sos, and B, are given. The household hooses {, } B, < o maximize ( suje o ( Governmen udge onsrain To finane puli expendiure, H, he governmen axes all ypes of inome a a rae τ < < and issues onds. The wihin-period governmen udge onsrain is: B B H AB τ A( B (3 2.4 ompeiive equilirium (E Given he pahs of he independen poliy insrumens {, H } τ and iniial ondiions for and B, a E is an alloaion {, } B suh ha he individual s prolem is solved,, mares lear and udge onsrains are saisfied. There are wo equivalen ways of presening he E. In he firs, he E is summarized y he resoure onsrain holding in eah period and a single implemenailiy (udge onsrain in period (see Appendix A ha also ompares our implemenailiy onsrain (4 o he lieraure: 6 H A (4a [ ( τ β A ]( B (4 where, in (4a-(4, we have eliminaed pries and axes apar from τ, whih is exogenously given o mae he poliy prolem nonrivial (see elow for deails. Seondly, and equivalenly, he E an e summarized y he individual Euler equaion, he resoure onsrain and governmen udge onsrain in eah period (see Appendix A: 6 and B are exogenously given iniial sos, while period- onsumpion,, is endogenous. Thus, in our seup, follows from (4; see also elow. 3

5 ( β r (5a H A (5 B B H r B r A (5 where r ( τ A is he ne (afer ax reurn o asses. onerning he exogenous poliy insrumens, we assume ha he governmen ses is expendiure as an exogenous fraion of he eginning-of-period apial so, H h (his saisfies saionariy. For simpliiy, in he ompuaions elow, we will assume ha h h is onsan over ime. Also, he period- ax rae, τ <, will e aen as given; oherwise he governmen would use i as a lump-sum ax whih maes he poliy prolem firs-es and hene rivial (see e.g. Ljungqvis and Sargen, 2, pp The primal approah o he Ramsey prolem, In he primal approah, he governmen hooses he pahs of { } o maximize ( suje o (4a-(4. To mae our resuls easily omparale, we follow hari e al. (994 and Ljungqvis and Sargen (2, pp The Lagrangean is: β { ν ln ( νln H [ A H ] } ( B [ ( τ A] ξ (6 β where ξ is an aemporal muliplier assoiaed wih (4 and is a dynami muliplier assoiaed wih (4a. As is nown (see e.g. hari e. al, 994, p. 625, and Ljungqvis and Sargen, 2, p. 322, he period- alloaions differ from he same rules governing ehavior from period onward. This is eause he period- firs-order ondiions inlude erms relaed o he iniial so of asses, and B. Speifially, a he firs-order ondiions for and are: 7 Well-nown papers ha use he primal approah inlude Luas (99, hari e al. (994 and Jones e al. (997. 4

6 ν ξ ( B [ ( τ A] (7a 2 β ( A (7 while, a he firs-order ondiions for and are: ν (8a β ( A (8 In addiion, in all periods, he firs-order ondiions inlude he onsrains o he governmen s prolem, namely (4a-. 3. Qualiaive feaures In he asene of exogenous upper ounds on he ax rae, here an e one period only wih nonzero axaion, and his is a. 8 Aually, i is sraighforward o show y woring as in hari e al. (994, pp ha, in his lass of uiliy funions, he opimal ax rae is zero a 2 onward. Thus, here are hree ax poliy regimes ha orrespond o, and 2, where τ is exogenously given and τ for 2. All his is onfirmed elow. 3.2 The full Ramsey sysem We now presen he full sysem. We wor in wo seps. Firs, we omine he firs-order ondiions - equaions (7a-, (8a- and he onsrains (4a- - so as o saisfy oninuiy aross poliy regimes. Reall ha here are hree disin poliy regimes, whih orrespond o periods, and 2. Seond, sine he model allows for long-erm growh, we ransform he variales o mae hem saionary. In pariular, we define a all, whih is a jump variale. Thus, as in he asi A model, afer period 2 here are no ransiional dynamis; as soon as he zero ax rae regime sars a 2 wih given values of apial and onds, 2 and B 2, all saionary 8 If here are exogenous upper ounds on he ax rae, i is opimal o se he ax rae a is upper ound for as many periods as neessary and zero hereafer. See he disussion in hari e al. (994, p

7 variales jump o heir long-run values where all quaniies grow a he same onsan rae. 9 Therefore, we have (see Appendix B for deails: Γ A h ] βν ( Firs poliy regime, (9a [ A β ( A A h β ( A A h Seond poliy regime, (9 Third poliy regime, 2 (9 ν where Γ ξ [ ( τ A] 2. Throughou, numers in susrips denoe ime periods, while variales wihou ime susrips denoe long-run values (here he long run is reahed a 2. We also have he implemenailiy onsrain (4 rewrien in saionary form as: ( β [ ( τ A] (9d are (9a-d summarize he Ramsey prolem. We have four equaions in four unnowns whih B,,, ξ. This is given he pah of h, he iniially given and he period- ax rae, τ. In urn, he implied opimal ax rae ( τ for an follow from he individual s opimaliy ondiions (see Appendix B. This is a simple sysem ha an e solved even analyially. 3.3 Numerial soluion We solve (9a-d numerially o mae our resuls omparale o hose in seion 4 elow. As a aseline ase, we se he following values for parameers, ν. 85, A, β. 9 ; B iniial ondiions,. 25 ; and exogenous variales, τ. 4 and h H.667. Soluions are in Tale ha also repors he implied values of he ax rae, τ. 9 See hari e al. (994, pp for a riher model wih ransiion dynamis wihin poliy regimes. The values of and h are he means of he US eonomy. 6

8 Tale : Soluion of he primal prolem endogenous variales ax poliy regimes τ ξ (se Noe: We use Mala 7.. All values mae sense. For insane, he ax rae in he firs period is posiive, τ.7, while i is zero in he long run (a 2. The value of he aemporal muliplier assoiaed wih he implemenailiy onsrain, ξ, is posiive. I is worh poining ou ha, exep for he ax rae, all oher variales jump o heir long run values in he firs period (his is proaly a propery of he A model. We repor ha omparaive sai exerises give inuiive resuls. For insane, a higher τ leads o a fall in τ and an inrease in he growh rae of onsumpion and apial in period onward. A higher leads o opposie effes. We finally repor ha our resuls are rous o hanges in he values of parameers, iniial ondiions and exogenous variales. 4. The dual approah o he Ramsey prolem τ,,, B o maximize ( suje o (5a- (5. We now follow hamley (986 and Ljungqvis and Sargen (2, p. 36. Sine τ < is In he dual approah, he governmen hooses { } aen as given o mae he poliy prolem nonrivial, he governmen an hoose,, B only a. Afer his period,, he governmen hooses τ,,, B, or equivalenly r,,, B, where r ( τ A. The Lagrangean is: { β ν ln ( ν ln H A H ] [ [ H ( r B B r A ] β ( r ]} [ ( 7

9 where, and are dynami mulipliers assoiaed wih (5a, (5 and (5 respeively. The period- firs-order ondiions again differ from he same rules governing ehavior from period onward. Speifially, a he firs-order ondiions for,, B are respeively: ν β r ( (a β A β ( r ( ( A β ( r ( while, a he firs-order ondiions for r,,, B are respeively: B (2a ( ν β ( r β (2 β ( A β ( r A (2 β ( r (2d In addiion, in all periods, he firs-order ondiions inlude he onsrains o he governmen s prolem, namely (5a-. 4. Qualiaive feaures In addiion o he feaures disussed in he primal approah (see suseion 3., noe ha equaion (5a is linearly dependen wih equaions ( and (2d. In pariular, a any ime,..., whih means ha φ is onsan over ime as in hamley 2 2 (986, equaion 34. eep in mind ha φ is a new endogenous variale. Following hamley (986, φ p. 68, in wha follows, we use o susiue ou (he sign of φ is he sign of, whih is expeed o e negaive in a seond-es prolem and omi ( and (2d from he sysem. All 8

10 his also onfirms ha one has o solve simulaneously for he long run and he ransiion pah inluding period, as was oviously he ase in he primal approah (see elow. 4.2 The full Ramsey sysem We now presen he full sysem woring as in he primal approah. Thus, we firs omine he firs-order ondiions - equaions (a-, (2a-d and he onsrains (5a- - so as o saisfy oninuiy aross he hree poliy regimes. In urn, we ransform he variales o mae hem saionary; in pariular, we define, m Λ, Λ a all, whih are, B all jump variales. 2 Therefore, we have (see Appendix for deails: Firs poliy regime, β ( r A h m β ( r m mh m m r A βφ Λ ( A h β Λ( A ( r (3 A (3a (3 ν Λ Λ β ( r (3d Seond poliy regime, β ( r A h m β ( r m mh m m r A (4a (4 βφ Λ [ A h ] β Λ ( A ( r A (4 φ φ Λ (4d m While he need o solve simulaneously for he long run and he ransiion pah is, y onsruion, he ase in he primal approah, in he dual approah we ould solve for he long run independenly if here were no puli de (i.e. he governmen udge is alaned; see e.g. Par and Philippopoulos (24 and Eonomides and Philippopoulos (28. 2 We repor ha he soluion is rous o he ransformaions used. 9

11 ν Λ Λβ ( r Λ [ A β h ] (4e Third poliy regime, 2 3 β ( r A h β ( r mh m m r A (5a (5 βφ Λ [ A h ] β Λ ( A ( r A (5 φ φ Λ (5d m ν Λ Λ β ( r Λ[ A β h ] (5e Equaions (3a-d, (4a-e, (5a-e and m summarize he Ramsey prolem. B B We have fifeen equaions in fifeen unnowns whih are,,, r, r,,, Λ Λ Λ,,, Λ Λ Λ, m, m, m,φ. This is given he pah of h, iniial ondiions for and B, and he period- ax rae, τ. In erms of he numer of equaions and unnowns, his is a more omplex sysem o solve han he one in he primal approah (see (9a-d aove. 4.3 Numerial soluion To solve he aove sysem, we use he same parameer values used in seion 3. Aually, i was harder o find ranges of parameer values, iniial ondiions and exogenous variales ha yield a dual soluion; a soluion o he primal prolem was muh easier o oain. We hus sared our searh for a soluion from he dual. Numerial resuls for all endogenous variales are presened in Tale 2. We also repor he implied values of B m and he ax raes, τ. 3 As in he primal soluion, sine all ransformed variales are jump, he eonomy is a is long run a 2.

12 Tale 2: Soluion of he dual prolem endogenous variales ax poliy regimes m Λ Λ r τ φ (se Noe: We use Mala 7.. The soluions of and τ are he same as in Tale. In addiion, here we have soluions for Λ, Λ and he onsan value of φ, whih are presen in he dual prolem only. All endogenous variales have he righ sign. Regarding he soluion for, he idea is ha i is opimal for he governmen o raise all ax revenue hrough a ime- apial levy, lend he proeeds o he privae seor and finane governmen expendiure y using he ineres from he loan (hene he negaive value of m, 5. onlusions We solved he dynami opimal puli finane (Ramsey prolem y applying he dual and primal approah. As expeed, hey yield he same resuls for poliies and alloaions.

13 APPENDIX Appendix A: ompeiive equilirium The firs-order ondiions of he individual s prolem inlude (2 and he Euler equaion (5a. Using he governmen s udge onsrain (3 ino he individual s udge onsrain (2, we ge he resoure onsrain, (4a or (5. Equaion (5 is equaion (3 rewrien as in hamley (986, equaion 2. To ge he implemenailiy onsrain (4, one an wor as in Ljungqvis and Sargen (2, haper 2. Aually, our model wih a log-linear uiliy funion and an A produion ehnology is a speial ase of equaions (2.3 and 2.32 in Ljungqvis and Sargen if: (i we se u( (ii we ignore heir laor supply erms (iii sine here apial and onds are axed a he same rae and earn he same reurn, we use [ ( τ A ]( B on he righ-hand side of (2.32. This gives [ ( τ A]( β B, whih is (4. Appendix B: Primal soluion o he Ramsey prolem onsider ondiions a. If we use (7a for and (8a for ino (7, we have ( A ν βν ξ [ ] τ 2 B ( A Γ, where H A from (4a. This gives (9a. onsider ondiions a. Equaions (8a-(8 imply β ( A or ( A H β ( A β, where A from (4a. Thus, a,. A h When we are in he seond poliy regime a, whih also means ha a 2 he eonomy will e on is alaned growh pah where variales remain onsan and are denoed wihou a ime susrip, his is wrien as β ( A A h β ( A growh pah, so his is wrien as, whih is (9. A h Equaion (9d is equaion (4 rewrien in saionary form., whih is (9. A 2, we are on he alaned 2

14 Finally, given he (primal soluion, he gross growh rae of onsumpion is ( A β a, while a we have ( A βν. Also, a any, he gross Γ growh rae of apial follows from he resoure onsrain, A h. Having solved for, he ax rae an follow from β [ ( τ ] A. Appendix : Dual soluion o he Ramsey prolem ν onsider (a whih holds a only. This is wrien as β ( r, whih is (3d. onsider (2a and (2 whih hold a only. Equaion (2a is rewrien as B or, y using B φ φb. This, as B gives (4d a and (5d a 2. Equaion (2 is rewrien as ν β( r, where β A H from (5. This gives (4e a and (5e a 2. onsider now hose ondiions ha hold a any ime,. The Euler ondiion, (5a, and he resoure onsrain, (5, imply β ( r A h. This gives (3a a, (4a a and (5a a 2. The governmen udge onsrain, (5, joinly wih he Euler ondiion, m B β ( r (5a, imply. This gives (3 a, (4 a m B mh m m r A and (5 a 2. Finally, he Euler ondiions for apial, ( or (2, imply ha a any β ( A β ( r A, where This gives (3 a, (4 a and (5 a 2. φ and A H. 3

15 REFERENES Ainson A. and J. Sigliz (98: Leurers on Puli Eonomis. MGraw Hill, London. hamley. (986: Opimal axaion of apial inome in general equilirium wih infinie lives, Eonomeria, 54, hari V.V., L. hrisiano and P. ehoe (994: Opimal fisal poliy in a usiness yle model, Journal of Poliial Eonomy, 2, Eonomides G. and A. Philippopoulos (28: Growh enhaning poliy is he means o susain he environmen, Review of Eonomi Dynamis,, Jones L., R. Manuelli and P. Rossi (997: On he opimal axaion of apial inome, Journal of Eonomi Theory, 73, Judd. (985: Redisriuive axaion in a simple perfe foresigh model, Journal of Puli Eonomis, 28, Ljungqvis L. and T. Sargen (2: Reursive Maroeonomi Theory. The MIT Press, amridge, Mass. Firs ediion. Luas R. E. (99: Supply-side eonomis: An analyial review, Oxford Eonomi Papers, 42, Par H. and A. Philippopoulos (24: Indeerminay and fisal poliies in a growing eonomy, Journal of Eonomi Dynamis and onrol, 28,

The primal versus the dual approach to the Ramsey tax problem: A note

The primal versus the dual approach to the Ramsey tax problem: A note The primal versus he dual approah o he Ramsey ax prolem: A noe y George Eonomides a,, Aposolis Philippopoulos,, and Vangelis Vassilaos a Deparmen of Inernaional and European Eonomi Sudies, Ahens Universiy

More information

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

Problem 1 / 25 Problem 2 / 10 Problem 3 / 15 Problem 4 / 30 Problem 5 / 20 TOTAL / 100 Deparmen of Applied Eonomis Johns Hopkins Universiy Eonomis 60 Maroeonomi Theory and Poliy Miderm Exam Suggesed Soluions Professor Sanjay Chugh Summer 0 NAME: The Exam has a oal of five (5) problems and

More information

Mathematical Foundations -1- Choice over Time. Choice over time. A. The model 2. B. Analysis of period 1 and period 2 3

Mathematical Foundations -1- Choice over Time. Choice over time. A. The model 2. B. Analysis of period 1 and period 2 3 Mahemaial Foundaions -- Choie over Time Choie over ime A. The model B. Analysis of period and period 3 C. Analysis of period and period + 6 D. The wealh equaion 0 E. The soluion for large T 5 F. Fuure

More information

Economics 202 (Section 05) Macroeconomic Theory Practice Problem Set 7 Suggested Solutions Professor Sanjay Chugh Fall 2013

Economics 202 (Section 05) Macroeconomic Theory Practice Problem Set 7 Suggested Solutions Professor Sanjay Chugh Fall 2013 Deparmen of Eonomis Boson College Eonomis 0 (Seion 05) Maroeonomi Theory Praie Problem Se 7 Suggesed Soluions Professor Sanjay Chugh Fall 03. Lags in Labor Hiring. Raher han supposing ha he represenaive

More information

Problem Set 9 Due December, 7

Problem Set 9 Due December, 7 EE226: Random Proesses in Sysems Leurer: Jean C. Walrand Problem Se 9 Due Deember, 7 Fall 6 GSI: Assane Gueye his problem se essenially reviews Convergene and Renewal proesses. No all exerises are o be

More information

Fall 2017 Social Sciences 7418 University of Wisconsin-Madison Problem Set 1 Answers

Fall 2017 Social Sciences 7418 University of Wisconsin-Madison Problem Set 1 Answers Eonomis 435 enzie D. Cinn Fall 7 Soial Sienes 748 Universiy of Wisonsin-adison rolem Se Answers Due in leure on Wednesday, Sepemer. Be sure o pu your name on your prolem se. u oxes around your answers

More information

Online Appendix to Fiscal Consolidation in an Open Economy with Sovereign Premia and without Monetary Policy Independence

Online Appendix to Fiscal Consolidation in an Open Economy with Sovereign Premia and without Monetary Policy Independence Online Appendix o Fisal Consolidaion in an Open Eonomy wih Sovereign Premia and wihou Moneary Poliy Independene Aposolis Philippopoulos, a,b Peros Varhaliis, and Vanghelis Vassilaos a a Ahens Universiy

More information

Linear Quadratic Regulator (LQR) - State Feedback Design

Linear Quadratic Regulator (LQR) - State Feedback Design Linear Quadrai Regulaor (LQR) - Sae Feedbak Design A sysem is expressed in sae variable form as x = Ax + Bu n m wih x( ) R, u( ) R and he iniial ondiion x() = x A he sabilizaion problem using sae variable

More information

Teacher Quality Policy When Supply Matters: Online Appendix

Teacher Quality Policy When Supply Matters: Online Appendix Teaher Qualiy Poliy When Supply Maers: Online Appendix Jesse Rohsein July 24, 24 A Searh model Eah eaher draws a single ouside job offer eah year. If she aeps he offer, she exis eahing forever. The ouside

More information

Amit Mehra. Indian School of Business, Hyderabad, INDIA Vijay Mookerjee

Amit Mehra. Indian School of Business, Hyderabad, INDIA Vijay Mookerjee RESEARCH ARTICLE HUMAN CAPITAL DEVELOPMENT FOR PROGRAMMERS USING OPEN SOURCE SOFTWARE Ami Mehra Indian Shool of Business, Hyderabad, INDIA {Ami_Mehra@isb.edu} Vijay Mookerjee Shool of Managemen, Uniersiy

More information

The Role of Money: Credible Asset or Numeraire? Masayuki Otaki (Institute of Social Science, University of Tokyo)

The Role of Money: Credible Asset or Numeraire? Masayuki Otaki (Institute of Social Science, University of Tokyo) DBJ Disussion Paper Series, No.04 The Role of Money: Credible Asse or Numeraire? Masayuki Oaki (Insiue of Soial Siene, Universiy of Tokyo) January 0 Disussion Papers are a series of preliminary maerials

More information

Neoclassical Growth Model

Neoclassical Growth Model Neolaial Growh Model I. Inroduion As disued in he las haper, here are wo sandard ways o analyze he onsumpion-savings deision. They are. The long bu finie-lived people who leave heir hildren no beque. 2.

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

5. An economic understanding of optimal control as explained by Dorfman (1969) AGEC

5. An economic understanding of optimal control as explained by Dorfman (1969) AGEC This doumen was generaed a 1:27 PM, 09/17/15 Copyrigh 2015 Rihard T Woodward 5 An eonomi undersanding of opimal onrol as explained by Dorfman (1969) AGEC 642-2015 The purpose of his leure and he nex is

More information

The role of international public goods in tax cooperation

The role of international public goods in tax cooperation MPRA Munih Personal RePE Arhive The role of inernaional publi goods in ax ooperaion Panelis Kammas and Aposolis Philippopoulos Deparmen of Eonomis, Universiy of Ioannina, Deparmen of Eonomis, Ahens Universiy

More information

New Oscillation Criteria For Second Order Nonlinear Differential Equations

New Oscillation Criteria For Second Order Nonlinear Differential Equations Researh Inveny: Inernaional Journal Of Engineering And Siene Issn: 78-47, Vol, Issue 4 (Feruary 03), Pp 36-4 WwwResearhinvenyCom New Osillaion Crieria For Seond Order Nonlinear Differenial Equaions Xhevair

More information

mywbut.com Lesson 11 Study of DC transients in R-L-C Circuits

mywbut.com Lesson 11 Study of DC transients in R-L-C Circuits mywbu.om esson Sudy of DC ransiens in R--C Ciruis mywbu.om Objeives Be able o wrie differenial equaion for a d iruis onaining wo sorage elemens in presene of a resisane. To develop a horough undersanding

More information

An Inventory Model for Weibull Time-Dependence. Demand Rate with Completely Backlogged. Shortages

An Inventory Model for Weibull Time-Dependence. Demand Rate with Completely Backlogged. Shortages Inernaional Mahemaial Forum, 5, 00, no. 5, 675-687 An Invenory Model for Weibull Time-Dependene Demand Rae wih Compleely Baklogged Shorages C. K. Tripahy and U. Mishra Deparmen of Saisis, Sambalpur Universiy

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

ECON Lecture 4 (OB), Sept. 14, 2010

ECON Lecture 4 (OB), Sept. 14, 2010 ECON4925 21 Leure 4 (OB), Sep. 14, 21 Exraion under imperfe ompeiion: monopoly, oligopoly and he arel-fringe model Perman e al. (23), Ch. 15.6; Salan (1976) 2 MONOPOLISTIC EXPLOITATION OF A NATURAL RESOURCE

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

Optimal Transform: The Karhunen-Loeve Transform (KLT)

Optimal Transform: The Karhunen-Loeve Transform (KLT) Opimal ransform: he Karhunen-Loeve ransform (KL) Reall: We are ineresed in uniary ransforms beause of heir nie properies: energy onservaion, energy ompaion, deorrelaion oivaion: τ (D ransform; assume separable)

More information

Optimal scal and monetary policy action in a closed economy

Optimal scal and monetary policy action in a closed economy Opimal sal and moneary poliy aion in a losed eonomy Aposolis Philippopoulos y Ahens Universiy of Eonomis and Business, and CESifo Peros Varhaliis Ahens Universiy of Eonomis and Business Vanghelis Vassilaos

More information

The Trade-off between Intra- and Intergenerational Equity in Climate Policy

The Trade-off between Intra- and Intergenerational Equity in Climate Policy The Trade-off beween Inra- and Inergeneraional Equiy in Climae Poliy Kverndokk S. E. Nævdal and L. Nøsbakken Posprin version This is a pos-peer-review pre-opyedi version of an arile published in: European

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

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

A state space approach to calculating the Beveridge Nelson decomposition

A state space approach to calculating the Beveridge Nelson decomposition Eonomis Leers 75 (00) 3 7 www.elsevier.om/ loae/ eonbase A sae spae approah o alulaing he Beveridge Nelson deomposiion James C. Morley* Deparmen of Eonomis, Washingon Universiy, Campus Box 08, Brookings

More information

3. Differential Equations

3. Differential Equations 3. Differenial Equaions 3.. inear Differenial Equaions of Firs rder A firs order differenial equaion is an equaion of he form d() d ( ) = F ( (),) (3.) As noed above, here will in general be a whole la

More information

Generalized electromagnetic energy-momentum tensor and scalar curvature of space at the location of charged particle

Generalized electromagnetic energy-momentum tensor and scalar curvature of space at the location of charged particle Generalized eleromagnei energy-momenum ensor and salar urvaure of spae a he loaion of harged parile A.L. Kholmeskii 1, O.V. Missevih and T. Yarman 3 1 Belarus Sae Universiy, Nezavisimosi Avenue, 0030 Minsk,

More information

AN INVENTORY MODEL FOR DETERIORATING ITEMS WITH EXPONENTIAL DECLINING DEMAND AND PARTIAL BACKLOGGING

AN INVENTORY MODEL FOR DETERIORATING ITEMS WITH EXPONENTIAL DECLINING DEMAND AND PARTIAL BACKLOGGING Yugoslav Journal of Operaions Researh 5 (005) Number 77-88 AN INVENTORY MODEL FOR DETERIORATING ITEMS WITH EXPONENTIAL DECLINING DEMAND AND PARTIAL BACKLOGGING Liang-Yuh OUYANG Deparmen of Managemen Sienes

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

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

LIGHT and SPECIAL RELATIVITY

LIGHT and SPECIAL RELATIVITY VISUAL PHYSICS ONLINE MODULE 7 NATURE OF LIGHT LIGHT and SPECIAL RELATIVITY LENGTH CONTRACTION RELATIVISTIC ADDITION OF VELOCITIES Time is a relaie quaniy: differen obserers an measuremen differen ime

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

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

Advanced and Contemporary Topics in Macroeconomics I

Advanced and Contemporary Topics in Macroeconomics I Advaned and Conemporary Topis in Maroeonomis I Alemayehu Geda Email: ag2526@gmail.om Web Page: www.alemayehu.om Class Leure Noe 2 Neolassial Growh Theory wih Endogenous Saving Ramsey-Cass-Koopmans & OLG

More information

Boyce/DiPrima 9 th ed, Ch 6.1: Definition of. Laplace Transform. In this chapter we use the Laplace transform to convert a

Boyce/DiPrima 9 th ed, Ch 6.1: Definition of. Laplace Transform. In this chapter we use the Laplace transform to convert a Boye/DiPrima 9 h ed, Ch 6.: Definiion of Laplae Transform Elemenary Differenial Equaions and Boundary Value Problems, 9 h ediion, by William E. Boye and Rihard C. DiPrima, 2009 by John Wiley & Sons, In.

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

(Radiation Dominated) Last Update: 21 June 2006

(Radiation Dominated) Last Update: 21 June 2006 Chaper Rik s Cosmology uorial: he ime-emperaure Relaionship in he Early Universe Chaper he ime-emperaure Relaionship in he Early Universe (Radiaion Dominaed) Las Updae: 1 June 006 1. Inroduion n In Chaper

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

Physics 235 Chapter 2. Chapter 2 Newtonian Mechanics Single Particle

Physics 235 Chapter 2. Chapter 2 Newtonian Mechanics Single Particle Chaper 2 Newonian Mechanics Single Paricle In his Chaper we will review wha Newon s laws of mechanics ell us abou he moion of a single paricle. Newon s laws are only valid in suiable reference frames,

More information

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

3.1.3 INTRODUCTION TO DYNAMIC OPTIMIZATION: DISCRETE TIME PROBLEMS. A. The Hamiltonian and First-Order Conditions in a Finite Time Horizon 3..3 INRODUCION O DYNAMIC OPIMIZAION: DISCREE IME PROBLEMS A. he Hamilonian and Firs-Order Condiions in a Finie ime Horizon Define a new funcion, he Hamilonian funcion, H. H he change in he oal value of

More information

Energy Momentum Tensor for Photonic System

Energy Momentum Tensor for Photonic System 018 IJSST Volume 4 Issue 10 Prin ISSN : 395-6011 Online ISSN : 395-60X Themed Seion: Siene and Tehnology Energy Momenum Tensor for Phooni Sysem ampada Misra Ex-Gues-Teaher, Deparmens of Eleronis, Vidyasagar

More information

Welfare Maximizing Operational Monetary and Fiscal Policy Rules

Welfare Maximizing Operational Monetary and Fiscal Policy Rules Welfare Maximizing Operaional Moneary and Fisal Poliy Rules Rober Kollmann (*) eparmen of Eonomis, Universiy of Bonn 24-42 Adenauerallee, -533 Bonn, Germany Cenre for Eonomi Poliy Researh, UK Firs draf:

More information

Second-Order Boundary Value Problems of Singular Type

Second-Order Boundary Value Problems of Singular Type JOURNAL OF MATEMATICAL ANALYSIS AND APPLICATIONS 226, 4443 998 ARTICLE NO. AY98688 Seond-Order Boundary Value Probles of Singular Type Ravi P. Agarwal Deparen of Maheais, Naional Uniersiy of Singapore,

More information

On economic growth and minimum wages

On economic growth and minimum wages MPRA Munih Personal RePE Arhive On eonomi growh and minimum wages Luiano Fani and Lua Gori Deparmen of Eonomis, Universiy of Pisa, Deparmen of Eonomis, Universiy of Pisa 2. Oober 200 Online a hps://mpra.ub.uni-muenhen.de/25842/

More information

The Macroeconomic Consequences of Remittances

The Macroeconomic Consequences of Remittances The aroeonomi Consequenes of Remianes Diego Vaaflores June 5, 29 Asra: We sudy he impa of remianes on a small open eonomy wih a sohasi limied pariipaion model wih ash in advane onsrains and osly adjusmen

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

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

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

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

A New Formulation of Electrodynamics

A New Formulation of Electrodynamics . Eleromagnei Analysis & Appliaions 1 457-461 doi:1.436/jemaa.1.86 Published Online Augus 1 hp://www.sirp.org/journal/jemaa A New Formulaion of Elerodynamis Arbab I. Arbab 1 Faisal A. Yassein 1 Deparmen

More information

Mass Transfer Coefficients (MTC) and Correlations I

Mass Transfer Coefficients (MTC) and Correlations I Mass Transfer Mass Transfer Coeffiiens (MTC) and Correlaions I 7- Mass Transfer Coeffiiens and Correlaions I Diffusion an be desribed in wo ways:. Deailed physial desripion based on Fik s laws and he diffusion

More information

5. Stochastic processes (1)

5. Stochastic processes (1) Lec05.pp S-38.45 - Inroducion o Teleraffic Theory Spring 2005 Conens Basic conceps Poisson process 2 Sochasic processes () Consider some quaniy in a eleraffic (or any) sysem I ypically evolves in ime randomly

More information

On the Distribution of the Break-Date Estimator Implied by the Perron-Type Statistics When the Form of Break is Misspecified

On the Distribution of the Break-Date Estimator Implied by the Perron-Type Statistics When the Form of Break is Misspecified Xavier Universiy Exhii Fauly Sholarship Eonomis 1-24-27 On he Disriuion of he Break-Dae Esimaor Implied y he Perron-ype Saisis When he Form of Break is Misspeified Ami Sen Xavier Universiy - Cininnai Follow

More information

Jang-Ting Guo Lecture 1-1. Introduction and Some Basics. The building blocks of modern macroeconomics are

Jang-Ting Guo Lecture 1-1. Introduction and Some Basics. The building blocks of modern macroeconomics are Jang-Ting Guo Leure - Inroduion and Some Basis The building bloks of modern maroeonomis are () Solow (Neolassial) growh model Opimal (Ramse) growh model Real business le (RBC) model () Overlapping generaions

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

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

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

5. The Lucas Critique and Monetary Policy

5. The Lucas Critique and Monetary Policy 5. The Luas Criique and Monear Poli John B. Talor, Ma 6, 013 Eonomeri Poli Evaluaion: A Criique Highl influenial (Nobel Prize Adds o he ase for oli rules Shows diffiulies of eonomeri oli evaluaion when

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

Durham Research Online

Durham Research Online Durham Researh Online Deposied in DRO: 19 July 211 Version of aahed le: Aeped Version Peer-review saus of aahed le: Peer-reviewed Ciaion for published iem: Rensr om, T.I. and Spaaro, L. (211) 'The opimum

More information

SIMULATION STUDY OF STOCHASTIC CHANNEL REDISTRIBUTION

SIMULATION STUDY OF STOCHASTIC CHANNEL REDISTRIBUTION Developmens in Business Simulaion and Experienial Learning, Volume 3, 3 SIMULATIO STUDY OF STOCHASTIC CHAEL REDISTRIBUTIO Yao Dong-Qing Towson Universiy dyao@owson.edu ABSTRACT In his paper, we invesigae

More information

How Should Environmental Policy Respond to Business Cycles? Optimal Policy under Persistent Productivity Shocks

How Should Environmental Policy Respond to Business Cycles? Optimal Policy under Persistent Productivity Shocks How Should Environmenal Poliy Respond o Business Cyles? Opimal Poliy under Persisen Produiviy Shos Garh Heuel Harvard Kennedy Shool 79 JFK Sree, Mailbo 84 Cambridge, MA 038 heuel@fas.harvard.edu Deember

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

Lorentz Transformation Properties of Currents for the Particle-Antiparticle Pair Wave Functions

Lorentz Transformation Properties of Currents for the Particle-Antiparticle Pair Wave Functions Open Aess Library Journal 17, Volume 4, e373 ISSN Online: 333-971 ISSN Prin: 333-975 Lorenz Transformaion Properies of Currens for he Parile-Aniparile Pair Wave Funions Raja Roy Deparmen of Eleronis and

More information

1 Differential Equation Investigations using Customizable

1 Differential Equation Investigations using Customizable Differenial Equaion Invesigaions using Cusomizable Mahles Rober Decker The Universiy of Harford Absrac. The auhor has developed some plaform independen, freely available, ineracive programs (mahles) for

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

SOLUTIONS TO ECE 3084

SOLUTIONS TO ECE 3084 SOLUTIONS TO ECE 384 PROBLEM 2.. For each sysem below, specify wheher or no i is: (i) memoryless; (ii) causal; (iii) inverible; (iv) linear; (v) ime invarian; Explain your reasoning. If he propery is no

More information

Ramsey Policy with Endogenous Government Spending: the Gains from Taxing Consumption

Ramsey Policy with Endogenous Government Spending: the Gains from Taxing Consumption Ramsey Poliy wih Endogenous Governmen Spending: he Gains from Taxing Consumpion Giorgio Moa Lanaser Universiy Raffaele Rossi Lanaser Universiy February 5, 203 Absra We sudy he Ramsey moneary and fisal

More information

Online Supplement for The Value of Bespoke : Demand Learning, Preference Learning, and Customer Behavior

Online Supplement for The Value of Bespoke : Demand Learning, Preference Learning, and Customer Behavior Online Supplemen for The Value of Bespoke : Demand Learning, Preferene Learning, and Cusomer Behavior Tingliang Huang Carroll Shool of Managemen, Boson College, Chesnu Hill, Massahuses 0467, inglianghuang@bedu

More information

Chapter 8 The Complete Response of RL and RC Circuits

Chapter 8 The Complete Response of RL and RC Circuits Chaper 8 The Complee Response of RL and RC Circuis Seoul Naional Universiy Deparmen of Elecrical and Compuer Engineering Wha is Firs Order Circuis? Circuis ha conain only one inducor or only one capacior

More information

Economics 6130 Cornell University Fall 2016 Macroeconomics, I - Part 2

Economics 6130 Cornell University Fall 2016 Macroeconomics, I - Part 2 Economics 6130 Cornell Universiy Fall 016 Macroeconomics, I - Par Problem Se # Soluions 1 Overlapping Generaions Consider he following OLG economy: -period lives. 1 commodiy per period, l = 1. Saionary

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

PHYS-3301 Lecture 5. Chapter 2. Announcement. Sep. 12, Special Relativity. What about y and z coordinates? (x - direction of motion)

PHYS-3301 Lecture 5. Chapter 2. Announcement. Sep. 12, Special Relativity. What about y and z coordinates? (x - direction of motion) Announemen Course webpage hp://www.phys.u.edu/~slee/33/ Tebook PHYS-33 Leure 5 HW (due 9/4) Chaper, 6, 36, 4, 45, 5, 5, 55, 58 Sep., 7 Chaper Speial Relaiiy. Basi Ideas. Consequenes of Einsein s Posulaes

More information

Oscillation of an Euler Cauchy Dynamic Equation S. Huff, G. Olumolode, N. Pennington, and A. Peterson

Oscillation of an Euler Cauchy Dynamic Equation S. Huff, G. Olumolode, N. Pennington, and A. Peterson PROCEEDINGS OF THE FOURTH INTERNATIONAL CONFERENCE ON DYNAMICAL SYSTEMS AND DIFFERENTIAL EQUATIONS May 4 7, 00, Wilmingon, NC, USA pp 0 Oscillaion of an Euler Cauchy Dynamic Equaion S Huff, G Olumolode,

More information

Mahgoub Transform Method for Solving Linear Fractional Differential Equations

Mahgoub Transform Method for Solving Linear Fractional Differential Equations Mahgoub Transform Mehod for Solving Linear Fraional Differenial Equaions A. Emimal Kanaga Puhpam 1,* and S. Karin Lydia 2 1* Assoiae Professor&Deparmen of Mahemais, Bishop Heber College Tiruhirappalli,

More information

Solutions to Exercises in Chapter 5

Solutions to Exercises in Chapter 5 in 5. (a) The required inerval is b ± se( ) b where b = 4.768, =.4 and se( b ) =.39. Tha is 4.768 ±.4.39 = ( 4.4, 88.57) We esimae ha β lies beween 4.4 and 85.57. In repeaed samples 95% of similarly onsrued

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

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

15. Vector Valued Functions

15. Vector Valued Functions 1. Vecor Valued Funcions Up o his poin, we have presened vecors wih consan componens, for example, 1, and,,4. However, we can allow he componens of a vecor o be funcions of a common variable. For example,

More information

The Arcsine Distribution

The Arcsine Distribution The Arcsine Disribuion Chris H. Rycrof Ocober 6, 006 A common heme of he class has been ha he saisics of single walker are ofen very differen from hose of an ensemble of walkers. On he firs homework, we

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

Idealize Bioreactor CSTR vs. PFR... 3 Analysis of a simple continuous stirred tank bioreactor... 4 Residence time distribution... 4 F curve:...

Idealize Bioreactor CSTR vs. PFR... 3 Analysis of a simple continuous stirred tank bioreactor... 4 Residence time distribution... 4 F curve:... Idealize Bioreaor CSTR vs. PFR... 3 Analysis of a simple oninuous sirred ank bioreaor... 4 Residene ime disribuion... 4 F urve:... 4 C urve:... 4 Residene ime disribuion or age disribuion... 4 Residene

More information

Jae Kim Monash University. Abstract

Jae Kim Monash University. Abstract ias Correed oosrap Inferene for Regression Models wih Auoorrelaed Errors ae Kim Monash Universiy Absra A boosrap bias orreion mehod is applied o saisial inferene in he regression model wih auoorrelaed

More information

6.2 Transforms of Derivatives and Integrals.

6.2 Transforms of Derivatives and Integrals. SEC. 6.2 Transforms of Derivaives and Inegrals. ODEs 2 3 33 39 23. Change of scale. If l( f ()) F(s) and c is any 33 45 APPLICATION OF s-shifting posiive consan, show ha l( f (c)) F(s>c)>c (Hin: In Probs.

More information

Chapter 8 The Complete Response of RL and RC Circuits

Chapter 8 The Complete Response of RL and RC Circuits Chaper 8 he Complee Response of R and RC Ciruis Exerises Ex 8.3-1 Before he swih loses: Afer he swih loses: 2 = = 8 Ω so = 8 0.05 = 0.4 s. 0.25 herefore R ( ) Finally, 2.5 ( ) = o + ( (0) o ) = 2 + V for

More information

Cross Layer Adaptive Control for Wireless Mesh Networks

Cross Layer Adaptive Control for Wireless Mesh Networks AD HOC NTWORKS (LSVIR), VOL. 5, NO. 6, PP. 719-743, AUGUST 2007 1 Cross Layer Adapive Conrol for Wireless Mesh Neworks Mihael J. Neely, Rahul Urgaonkar Asra This paper invesigaes opimal rouing and adapive

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

Generalized The General Relativity Using Generalized Lorentz Transformation

Generalized The General Relativity Using Generalized Lorentz Transformation P P P P IJISET - Inernaional Journal of Innoaie Siene, Engineering & Tehnology, Vol. 3 Issue 4, April 6. www.ijise.om ISSN 348 7968 Generalized The General Relaiiy Using Generalized Lorenz Transformaion

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

Continuous versus Discrete-time Modeling: Does it make a Difference? *

Continuous versus Discrete-time Modeling: Does it make a Difference? * Coninuous versus Disree-ime Modeling: Does i make a Differene? * Charles T. Carlsrom and Timohy S. Fuers Federal Reserve Bank of Cleveland, Cleveland, OH, S. Bowling Green Sae niversiy, Bowling Green,

More information

What Ties Return Volatilities to Price Valuations and Fundamentals? On-Line Appendix

What Ties Return Volatilities to Price Valuations and Fundamentals? On-Line Appendix Wha Ties Reurn Volailiies o Price Valuaions and Fundamenals? On-Line Appendix Alexander David Haskayne School of Business, Universiy of Calgary Piero Veronesi Universiy of Chicago Booh School of Business,

More information

Faster and Simpler Algorithms for Multicommodity Flow and other Fractional Packing Problems

Faster and Simpler Algorithms for Multicommodity Flow and other Fractional Packing Problems Faser and Simpler Algorihms for Muliommodiy Flow and oher Fraional Paking Problems aveen Garg Compuer Siene and Engineering Indian Insiue of Tehnology, ew Delhi, India Johen Könemann GSIA, Carnegie Mellon

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

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

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

Preliminary version Please do not quote

Preliminary version Please do not quote Feriliy-relaed pensions, ax-um-subsidy and Α Pareo effiieny Luiano Fani * and Lua Gori ** Deparmen of Eonomis, Universiy of Pisa, Via Cosimo Ridolfi, 0, I 5624 Pisa (PI), Ialy Deparmen of Law, Universiy

More information

Notes for Lecture 17-18

Notes for Lecture 17-18 U.C. Berkeley CS278: Compuaional Complexiy Handou N7-8 Professor Luca Trevisan April 3-8, 2008 Noes for Lecure 7-8 In hese wo lecures we prove he firs half of he PCP Theorem, he Amplificaion Lemma, up

More information

Concourse Math Spring 2012 Worked Examples: Matrix Methods for Solving Systems of 1st Order Linear Differential Equations

Concourse Math Spring 2012 Worked Examples: Matrix Methods for Solving Systems of 1st Order Linear Differential Equations Concourse Mah 80 Spring 0 Worked Examples: Marix Mehods for Solving Sysems of s Order Linear Differenial Equaions The Main Idea: Given a sysem of s order linear differenial equaions d x d Ax wih iniial

More information