Four equations describe the dynamic solution to RBC model. Consumption-leisure efficiency condition. Consumption-investment efficiency condition

Similar documents
LINEAR APPROXIMATION OF THE BASELINE RBC MODEL SEPTEMBER 17, 2013

LINEAR APPROXIMATION OF THE BASELINE RBC MODEL JANUARY 29, 2013

Four equations describe the dynamic solution to RBC model. Consumption-leisure efficiency condition. Consumption-investment efficiency condition

1. Solve by the method of undetermined coefficients and by the method of variation of parameters. (4)

State and Parameter Estimation of The Lorenz System In Existence of Colored Noise

Comparison between Fourier and Corrected Fourier Series Methods

Approximating Solutions for Ginzburg Landau Equation by HPM and ADM

Using Linnik's Identity to Approximate the Prime Counting Function with the Logarithmic Integral

Available online at J. Math. Comput. Sci. 4 (2014), No. 4, ISSN:

Electrical Engineering Department Network Lab.

The Eigen Function of Linear Systems

The Solution of the One Species Lotka-Volterra Equation Using Variational Iteration Method ABSTRACT INTRODUCTION

REDUCED DIFFERENTIAL TRANSFORM METHOD FOR GENERALIZED KDV EQUATIONS. Yıldıray Keskin and Galip Oturanç

F D D D D F. smoothed value of the data including Y t the most recent data.

Ideal Amplifier/Attenuator. Memoryless. where k is some real constant. Integrator. System with memory

10.3 Autocorrelation Function of Ergodic RP 10.4 Power Spectral Density of Ergodic RP 10.5 Normal RP (Gaussian RP)

Calculus BC 2015 Scoring Guidelines

MODERN CONTROL SYSTEMS

Math-303 Chapter 7 Linear systems of ODE November 16, Chapter 7. Systems of 1 st Order Linear Differential Equations.

Economics 8723 Macroeconomic Theory Problem Set 3 Sketch of Solutions Professor Sanjay Chugh Spring 2017

Clock Skew and Signal Representation

Solutions Manual 4.1. nonlinear. 4.2 The Fourier Series is: and the fundamental frequency is ω 2π

Additional Tables of Simulation Results

Homotopy Analysis Method for Solving Fractional Sturm-Liouville Problems

A Novel Approach for Solving Burger s Equation

14.02 Principles of Macroeconomics Fall 2005

Linear System Theory

Paper 3A3 The Equations of Fluid Flow and Their Numerical Solution Handout 1

Economics 8723 Macroeconomic Theory Problem Set 2 Professor Sanjay Chugh Spring 2017

INVESTMENT PROJECT EFFICIENCY EVALUATION

Problems and Solutions for Section 3.2 (3.15 through 3.25)

F.Y. Diploma : Sem. II [AE/CH/FG/ME/PT/PG] Applied Mathematics

EE757 Numerical Techniques in Electromagnetics Lecture 8

APPROXIMATE SOLUTION OF FRACTIONAL DIFFERENTIAL EQUATIONS WITH UNCERTAINTY

Supplement for SADAGRAD: Strongly Adaptive Stochastic Gradient Methods"

VIM for Determining Unknown Source Parameter in Parabolic Equations

ANALYSIS OF THE CHAOS DYNAMICS IN (X n,x n+1) PLANE

Samuel Sindayigaya 1, Nyongesa L. Kennedy 2, Adu A.M. Wasike 3

Hadamard matrices from the Multiplication Table of the Finite Fields

Affine term structure models

ODEs II, Supplement to Lectures 6 & 7: The Jordan Normal Form: Solving Autonomous, Homogeneous Linear Systems. April 2, 2003

Optimization of Rotating Machines Vibrations Limits by the Spring - Mass System Analysis

ECE-314 Fall 2012 Review Questions

Lecture 15 First Properties of the Brownian Motion

BEST LINEAR FORECASTS VS. BEST POSSIBLE FORECASTS

TAKA KUSANO. laculty of Science Hrosh tlnlersty 1982) (n-l) + + Pn(t)x 0, (n-l) + + Pn(t)Y f(t,y), XR R are continuous functions.

xp (X = x) = P (X = 1) = θ. Hence, the method of moments estimator of θ is

Numerical Method for Ordinary Differential Equation

The Central Limit Theorem

SOLVING OF THE FRACTIONAL NON-LINEAR AND LINEAR SCHRÖDINGER EQUATIONS BY HOMOTOPY PERTURBATION METHOD

A note on deviation inequalities on {0, 1} n. by Julio Bernués*

2 f(x) dx = 1, 0. 2f(x 1) dx d) 1 4t t6 t. t 2 dt i)

A Note on Prediction with Misspecified Models

Basic Results in Functional Analysis

BE.430 Tutorial: Linear Operator Theory and Eigenfunction Expansion

Time Dependent Queuing

Calculus Limits. Limit of a function.. 1. One-Sided Limits...1. Infinite limits 2. Vertical Asymptotes...3. Calculating Limits Using the Limit Laws.

A Complex Neural Network Algorithm for Computing the Largest Real Part Eigenvalue and the corresponding Eigenvector of a Real Matrix

SUMMATION OF INFINITE SERIES REVISITED

Online Appendix to Solution Methods for Models with Rare Disasters

Math 6710, Fall 2016 Final Exam Solutions

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

Decentralized Double Stochastic Averaging Gradient

Mean Square Convergent Finite Difference Scheme for Stochastic Parabolic PDEs

Section 8 Convolution and Deconvolution

Energy Density / Energy Flux / Total Energy in 1D. Key Mathematics: density, flux, and the continuity equation.

Lecture 15: Three-tank Mixing and Lead Poisoning

S n. = n. Sum of first n terms of an A. P is

Online Supplement to Reactive Tabu Search in a Team-Learning Problem

Comparison of Adomian Decomposition Method and Taylor Matrix Method in Solving Different Kinds of Partial Differential Equations

The Moment Approximation of the First Passage Time for the Birth Death Diffusion Process with Immigraton to a Moving Linear Barrier

ME 321 Kinematics and Dynamics of Machines S. Lambert Winter 2002

CLOSED FORM EVALUATION OF RESTRICTED SUMS CONTAINING SQUARES OF FIBONOMIAL COEFFICIENTS

Vibration 2-1 MENG331

Additional Methods for Solving DSGE Models

Chapter 2: Time-Domain Representations of Linear Time-Invariant Systems. Chih-Wei Liu

When both wages and prices are sticky

1 Notes on Little s Law (l = λw)

Numerical Solution of Parabolic Volterra Integro-Differential Equations via Backward-Euler Scheme

Advection! Discontinuous! solutions shocks! Shock Speed! ! f. !t + U!f. ! t! x. dx dt = U; t = 0

INTEGER INTERVAL VALUE OF NEWTON DIVIDED DIFFERENCE AND FORWARD AND BACKWARD INTERPOLATION FORMULA

A Generalized Cost Malmquist Index to the Productivities of Units with Negative Data in DEA

David Randall. ( )e ikx. k = u x,t. u( x,t)e ikx dx L. x L /2. Recall that the proof of (1) and (2) involves use of the orthogonality condition.

ME 3210 Mechatronics II Laboratory Lab 6: Second-Order Dynamic Response

Review Exercises for Chapter 9

Inference of the Second Order Autoregressive. Model with Unit Roots

Supplementary Information for Thermal Noises in an Aqueous Quadrupole Micro- and Nano-Trap

Research Article A Generalized Nonlinear Sum-Difference Inequality of Product Form

Big O Notation for Time Complexity of Algorithms

Development of Kalman Filter and Analogs Schemes to Improve Numerical Weather Predictions

Moment Generating Function

L-functions and Class Numbers

Prakash Chandra Rautaray 1, Ellipse 2

Math 2414 Homework Set 7 Solutions 10 Points

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

N! AND THE GAMMA FUNCTION

FRACTIONAL VARIATIONAL ITERATION METHOD FOR TIME-FRACTIONAL NON-LINEAR FUNCTIONAL PARTIAL DIFFERENTIAL EQUATION HAVING PROPORTIONAL DELAYS

Follow links for Class Use and other Permissions. For more information send to:

K3 p K2 p Kp 0 p 2 p 3 p

Lecture 9: Polynomial Approximations

Transcription:

LINEAR APPROXIMATION OF THE BASELINE RBC MODEL FEBRUARY, 202 Iroducio For f(, y, z ), mulivariable Taylor liear epasio aroud (, yz, ) f (, y, z) f(, y, z) + f (, y, z)( ) + f (, y, z)( y y) + f (, y, z)( z z) Four equaios describe he dyamic soluio o RBC model Cosumpio-leisure efficiecy codiio u( c, ) = zm ( k, ) uc( c, ) Cosumpio-ivesme efficiecy codiio Aggregae resource cosrai y z c + k+ ( δ ) k = zm ( k, ) Law of moio for TFP z l z = ( ρ )l z + ρ l z + ε ( δ ) u ( c, ) = βe u ( c, ) + z m ( k, c c + + + k + + + z z + February, 202 2

Iroducio STEADY STATE Deermiisic seady sae he aural local poi of approimaio Shu dow all shocks ad se eogeous variables a heir meas The Idea: Le ecoomy ru for may (ifiie) periods Time eveually does maer ay more Drop all ime idices u( c, ) = zm ( k, ) u ( c, ) c uc( c, ) = βuc( c, ) mk( k, ) + δ c + δ k = zm( k, ) l z = ( ρ )l z + ρ l z z = z (a parameer of he model) z z Give fucioal forms ad parameer values, solve for (c,, k) The seady sae of he model Taylor epasio aroud his poi February, 202 3 LINEARIZATION ALGORITHMS Schmi-Grohe ad Uribe (2004 JEDC) A perurbaio algorihm A class of mehods used o fid a approimae soluio o a problem ha cao be solved eacly, by sarig from he eac soluio of a relaed problem Applicable if he problem ca be formulaed by addig a small erm o he descripio of he eacly-solvable problem Malab code available hrough Columbia Dep. of Ecoomics web sie Uhlig (999, chaper i Compuaioal Mehods for he Sudy of Dyamic Ecoomies) Uses a geeralized eige-decomposiio Typically implemeed wih Schur decomposiio (Sims algorihm) Malab code available a hp://www2.wiwi.hu-berli.de/isiue/wpol/hml/oolki.hm Iroducio February, 202 4 2

Iroducio Defie co-sae vecor ad sae vecor y = k = z February, 202 5 Defie co-sae vecor ad sae vecor SGU Deails y = k = z Order model s dyamic equaios i a vecor Cosumpio-leisure efficiecy codiio Cosumpio-ivesme efficiecy codiio Aggregae resource cosrai Law of moio for TFP February, 202 6 f( y, y,, ) + + 3

SGU Deails Need four marices of derivaives. Differeiae f ( y, y,, ) wih respec o (elemes of) y + + + Firs derivaives wih respec o: c + + Cosumpio-leisure efficiecy codiio Cosumpio-ivesme efficiecy codiio Aggregae resource cosrai Law of moio for TFP = f y + February, 202 7 Need four marices of derivaives 2. Differeiae f ( y, y,, ) wih respec o (elemes of) y + + SGU Deails Firs derivaives wih respec o: Cosumpio-leisure efficiecy codiio Cosumpio-ivesme efficiecy codiio Aggregae resource cosrai Law of moio for TFP c = f y February, 202 8 4

SGU Deails Need four marices of derivaives 3. Differeiae f ( y, y,, ) wih respec o (elemes of) + + + Firs derivaives wih respec o: k + z + Cosumpio-leisure efficiecy codiio Cosumpio-ivesme efficiecy codiio Aggregae resource cosrai Law of moio for TFP = f + February, 202 9 Need four marices of derivaives 4. Differeiae f ( y, y,, ) wih respec o (elemes of) + + SGU Deails Firs derivaives wih respec o: Cosumpio-leisure efficiecy codiio Cosumpio-ivesme efficiecy codiio Aggregae resource cosrai Law of moio for TFP k z = f February, 202 0 5

SGU Deails The model s dyamic epecaioal equaios f ( y, y,, ) + + Cosumpio-leisure efficiecy codiio 2 f ( y, y,, ) E[ f( y, y,, ) ] E + + Cosumpio-ivesme efficiecy codiio + + = f 3 ( y, y,, ) + + Aggregae resource cosrai 4 f ( y+, y, +, ) Law of moio for TFP February, 202 SGU Deails The model s dyamic epecaioal equaios f ( y, y,, ) + + Cosumpio-leisure efficiecy codiio 2 f ( y, y,, ) E[ f( y, y,, ) ] E + + Cosumpio-ivesme efficiecy codiio + + = f 3 ( y, y,, ) + + Aggregae resource cosrai 4 f ( y+, y, +, ) Law of moio for TFP Cojecure equilibrium decisio rules Noe: g(.) ad h(.) are ime ivaria fucios! Perurbaio parameer : y = g(, ) govers size of shocks = h(, ) + ηε Subsiue decisio rules io dyamic equaios + + Mari of sadard deviaios of sae variables February, 202 2 6

SGU Deails The model s dyamic epecaioal equaios [ ( +,, +, )] = E[ f( g ( +, ), g (, ), h (, ) + ηε+, ] = E [ f( g( h(, ) + ηε, ), g(, ), h(, ) + ηε, ] E f y y + + F(, ) F (, ) F (, ) February, 202 3 The model s dyamic epecaioal equaios E[ f( y+, y, +, ) ] = E[ f( g ( +, ), g (, ), h (, ) + ηε+, ] = E f( g( h(, ) + ηε+, ), g(, ), h(, ) + ηε+, F(, ) [ ] Usig chai rule ad suppressig argumes F f f (, ) = fy g h + fy g + h + + + SGU Deails February, 202 4 7

SGU Deails The model s dyamic epecaioal equaios E[ f( y+, y, +, ) ] = E[ f( g ( +, ), g (, ), h (, ) + ηε+, ] = E f( g( h(, ) + ηε+, ), g(, ), h(, ) + ηε+, F(, ) Usig chai rule ad suppressig argumes [ ] F (, ) f f = y g h + y g + f h + f + + February, 202 5 The model s dyamic epecaioal equaios E[ f( y+, y, +, ) ] = E[ f( g ( +, ), g (, ), h (, ) + ηε+, ] = E f( g( h(, ) + ηε+, ), g(, ), h(, ) + ηε+, F(, ) Usig chai rule ad suppressig argumes [ ] F (, ) f f = y g h + y g + f h + f + + Holds, i paricular, a he deermiisic seady sae (,0) F (,0) = f g h + f g + f h + f y+ y + Seig shus dow shocks February, 202 6 SGU Deails Each erm is evaluaed a he seady sae jus as Taylor heorem requires 8

SGU Deails A quadraic equaio i he elemes of g ad h evaluaed a he seady sae F (,0) = f (,0) g (,0) h (,0) + f (, 0) g (,0) + f (,0) h (, 0) + f (,0) y+ y + Solve umerically for he elemes of g ad h (use fsolve i Malab) Recall cojecured equilibrium decisio rules y = g(, ) = h(, ) + ηε + + February, 202 7 A quadraic equaio i he elemes of g ad h evaluaed a he seady sae y+ y + Solve umerically for he elemes of g ad h (use fsolve i Malab) Recall cojecured equilibrium decisio rules Firs-order approimaio is y = g(, ) g(,0) + g (,0)( ) + g (,0) = h(, ) h(,0) + h (,0)( ) + h (,0) + SGU Deails F (,0) = f (,0) g (,0) h (,0) + f (, 0) g (,0) + f (,0) h (, 0) + f (,0) y = g(, ) = h(, ) + ηε + + SGU Theorem : g ad h DONE!!! Now coduc impulse resposes, abulae busiess cycle momes, wrie paper February, 202 8 9

Macro Fudameals CERTAINTY EQUIVALENCE Displayed by a model if decisio rules do o deped o he sadard deviaio of eogeous uceraiy e.g., PRECAUTIONARY SAVINGS! For sochasic problems wih quadraic objecive fucio ad liear cosrais, he decisio rules are ideical o hose of he osochasic problem Here, we have y = g(, ) g(,0) + g(,0)( ) + g (,0) = h(, ) h(,0) + h (,0)( ) + h (,0) + SGU Theorem : g ad h Firs-order approimaed decisio rules do o deped o he size of he shocks, which is govered by No he same hig as eac CE, bu refer o i as CE February, 202 9 LINEARIZING THE RBC MODEL Assume uc (, ) = lc ψ l ad mk (, ) = k α cosumpio-leisure efficiecy codiio is (Parial) Eample k Le f ( y+, y, +, ) = ( α) zk (ad recall y = ) = z ( α) zk February, 202 20 0

(Parial) Eample LINEARIZING THE RBC MODEL Assume uc (, ) = lc ψ l ad mk (, ) = k α cosumpio-leisure efficiecy codiio is k Le f ( y+, y, +, ) = ( α) zk (ad recall y = ) = z ( α) zk Compue firs row of mari f y+ c + + Cosumpio-leisure efficiecy codiio Cosumpio-ivesme efficiecy codiio Aggregae resource cosrai Law of moio for TFP February, 202 2 LINEARIZING THE RBC MODEL Assume uc (, ) = lc ψ l ad mk (, ) = k α cosumpio-leisure efficiecy codiio is (Parial) Eample k Le f ( y+, y, +, ) = ( α) zk (ad recall y = ) = z ( α) zk Compue firs row of mari f y+ c + + Cosumpio-leisure efficiecy codiio Cosumpio-ivesme efficiecy codiio Aggregae resource cosrai Law of moio for TFP 0 0 February, 202 22

(Parial) Eample LINEARIZING THE RBC MODEL Assume uc (, ) = lc ψ l ad mk (, ) = k α cosumpio-leisure efficiecy codiio is k Le f ( y+, y, +, ) = ( α) zk (ad recall y = ) = z ( α) zk Compue firs row of mari f y Cosumpio-leisure efficiecy codiio Cosumpio-ivesme efficiecy codiio Aggregae resource cosrai Law of moio for TFP c ψ + α ( α ) z k 2 α α February, 202 23 LINEARIZING THE RBC MODEL Assume uc (, ) = lc ψ l ad mk (, ) = k α cosumpio-leisure efficiecy codiio is (Parial) Eample k Le f ( y+, y, +, ) = ( α) zk (ad recall y = ) = z ( α) zk Compue firs row of mari f + k + z + Cosumpio-leisure efficiecy codiio Cosumpio-ivesme efficiecy codiio Aggregae resource cosrai Law of moio for TFP 0 0 February, 202 24 2

(Parial) Eample LINEARIZING THE RBC MODEL Assume uc (, ) = lc ψ l ad mk (, ) = k α cosumpio-leisure efficiecy codiio is k Le f ( y+, y, +, ) = ( α) zk (ad recall y = ) = z ( α) zk Compue firs row of mari f k z Cosumpio-leisure efficiecy codiio α k k α ( α ) z ( α ) α Cosumpio-ivesme efficiecy codiio Aggregae resource cosrai Law of moio for TFP α α + February, 202 25 LINEARIZING THE RBC MODEL I deermiisic seady sae, he firs rows of f y+, f y, f +, f are f y+ 0 0 (Parial) Eample f y f + ψ + α( α) zk 2 0 0 α k α( α) z ( ) k α f α α α + How o compue derivaives f y+, f y, f +, f? By had (feasible for small models) Schmi-Grohe ad Uribe Malab aalyical rouies Your ow Maple or Mahemaica programs Dyare package February, 202 26 3

CALIBRATION? Solvig for he seady sae? Choosig parameer values? Ne: calibraio of he baselie represeaive-age (RBC + growh) model February, 202 27 4