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ECON 4325 Monetary Policy Lecture 3 Martin Blomhoff Holm

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  • ECON 4325Monetary Policy

    Lecture 3

    Martin Blomhoff Holm

  • Outline

    1. Brief review of lecture 2.

    2. The firm problem without sticky prices.

    3. Monetary policy without sticky prices.

    Holm Monetary Policy, Lecture 3 1 / 27

  • Part I: Brief review of lecture 2.

    Holm Monetary Policy, Lecture 3 2 / 27

  • Let’s check what you remember from last time.

    Holm Monetary Policy, Lecture 3 3 / 27

  • Part II: Firm problem without sticky prices.

    Holm Monetary Policy, Lecture 3 4 / 27

  • The firm problem

    Assume that we have many firms denoted by i who produce according to

    Yi ,t = AtN1−αi ,t

    where Yi ,t is production by firm i , At is aggregate TFP, Ni ,t is labor infirm i , and α ∈ [0, 1) is the curvature of the production function.

    We further assume that aggregate TFP follows an AR(1) in logs:

    log(At) = ρa log(At−1) + �At

    at = ρaat−1 + �At

    Holm Monetary Policy, Lecture 3 5 / 27

  • The firm problem

    Let firm i maximize profits

    maxNi,t

    PtYi ,t −WtNi ,t

    maxNi,t

    PtAtN1−αi ,t −WtNi ,t

    The first order condition is

    WtPt

    = (1− α)AtN−αi ,t

    i.e. all firms choose the same level of labor.

    As a result, we can aggregate all firms to one representative firm. Fromnow on, we therefore remove the dependence on i .

    Holm Monetary Policy, Lecture 3 6 / 27

  • The first order condition

    WtPt

    = (1− α)AtN−αt

    What does it mean? Let us take logs on both sides and solve in terms oflabor demand.

    wt − pt = log(1− α) + at − αntor rearranged

    nt = −1

    α(wt − pt − at − log(1− α))

    Takeaways:

    I If wages increase, firms reduce labor demand by 1α of the percentagereduction in wages.

    I 1/α is the elasticity of labor demand to wage changes.

    I α = 0: firms adjust labor infinitely much in response to wage changes.

    I α→ 1 firms adjust one-for-one for any increase in wages.

    Holm Monetary Policy, Lecture 3 7 / 27

  • EquilibriumWe can now summarize the complete model by the following equations:

    Household side:

    C−σt = β(1 + it)Et

    {C−σt+1

    (PtPt+1

    )}WtPt

    = Cσt Nφt

    Firm side:

    Yt = AtN1−αt

    WtPt

    = (1− α)AtN−αt

    Market Clearing:

    Yt = Ct (supply = demand in goods market)

    Nt = Nt (supply = demand in labor market)

    Holm Monetary Policy, Lecture 3 8 / 27

  • Let’s log-linearize I: Consumption-Euler

    1 = Et

    {β(1 + it)

    (CtCt+1

    )σ PtPt+1

    }Step 1: Take exponential and logs of RHS

    1 = Et exp {it − ρ− σ(ct+1 − ct)− πt+1}

    Step 2: Taylor expansion of RHS (step on blackboard)

    Et{1 + (it − i)− σ(ct+1 − ct)− (πt+1 − π)}

    Step 3: Note that i = π + ρ in steady state such that and LHS = RHS

    1 = Et{1 + it − ρ− σ(ct+1 − ct)− πt+1}

    Step 4: Rearrange to obtain

    ct = Et{ct+1} −1

    σ(it − Et{πt+1} − ρ)

    Holm Monetary Policy, Lecture 3 9 / 27

  • Let’s log-linearize II: Labor supply

    WtPt

    = Cσt Nφt

    ωt = σct + φnt

    Holm Monetary Policy, Lecture 3 10 / 27

  • Let’s log-linearize III: Production

    Yt = AtN1−αt

    yt = at + (1− α)nt

    Holm Monetary Policy, Lecture 3 11 / 27

  • Let’s log-linearize IV: Labor demand

    WtPt

    = (1− α)AtN−αt

    ωt = log(1− α) + at − αnt

    Holm Monetary Policy, Lecture 3 12 / 27

  • Part III: Monetary policy without sticky prices.

    Holm Monetary Policy, Lecture 3 13 / 27

  • Equilibrium Definition

    1. Households maximize the discounted stream of utility

    2. Firms maximize profits

    3. Market clearing: Yt = Ct and NDt = N

    St

    Holm Monetary Policy, Lecture 3 14 / 27

  • The Model Equations

    ωt = σct + φnt (1)

    ct = Etct+1 −1

    σ(it − Etπt+1 − ρ) (2)

    yt = at + (1− α)nt (3)ωt = at − αnt + log(1− α) (4)yt = ct (5)

    Holm Monetary Policy, Lecture 3 15 / 27

  • Five Steps to Solve the Model

    1. Combine (1) and (4) to solve for nt .

    2. Use the solution for nt to solve for yt(= ct) using (3).

    3. Solve for the equilibrium real interest rate using the Euler-equation(2). Remember that rt = it − Etπt+1.

    4. Use the solution for yt in step 2 to find nt from the solution in step 1.

    5. Use either (1) or (4) to solve for ωt .

    Holm Monetary Policy, Lecture 3 16 / 27

  • DO IT!

    Holm Monetary Policy, Lecture 3 17 / 27

  • DO IT!

    Holm Monetary Policy, Lecture 3 18 / 27

  • The Solution

    ct = yt

    yt =1 + φ

    σ(1− α) + φ+ αat +

    (1− α) log(1− α)σ(1− α) + φ+ α

    = ψyaat + ξy

    rt = ρ+ σψyaEt{∆at+1}

    nt =1− σ

    σ(1− α) + φ+ αat +

    log(1− α)σ(1− α) + φ+ α

    = ψnaat + ξn

    ωt =σ + φ

    σ(1− α) + φ+ αat +

    [σ(1− α) + φ] log(1− α)σ(1− α) + φ+ α

    = ψωaat + ξω

    Holm Monetary Policy, Lecture 3 19 / 27

  • Interpretations

    Holm Monetary Policy, Lecture 3 20 / 27

  • Result: The Classical Dichotomy

    I All real variables (real wage, output, consumption, and labor hours)are independent of monetary policy: monetary policy neutrality

    I Technology is the only driving force of real variables

    I Nominal variables (inflation, nominal interest rate) are not uniquelydetermined

    I We need one more equation to specify how monetary policy isconducted

    Holm Monetary Policy, Lecture 3 21 / 27

  • Equilibrium behavior of nominal variables I

    I The real interest rate is entirely determined by the real side of theeconomy. The nominal interest rate and expected inflation is thendetermined by the Fisher equation

    it = Etπt+1 + rt

    I Since we have one equation with two unknowns. The inflation andnominal interest rate is indeterminate. Give me any path of prices andI can specify the right path of nominal interest rate, and opposite.

    Holm Monetary Policy, Lecture 3 22 / 27

  • Equilibrium behavior of nominal variables II

    I Example: The Taylor rule:

    it = ρ+ φππt

    With this equation, we also know the path of πt and it .

    I However, the model has two predictions that are in sharp contrast toempirical evidence:

    1. Prices respond instantaneously to any shock.2. Since rt is fixed, a higher nominal interest rate will result in higher

    expected inflation.

    Holm Monetary Policy, Lecture 3 23 / 27

  • Recall for example from lecture 1

    Romer-Romer 2004Holm Monetary Policy, Lecture 3 24 / 27

  • What is needed?

    I For nominal interest rate changes to have to real effects, we need tointroduce a friction.

    I In the canonical New-Keynesian model and in this class, we introducesticky prices and monopolistic competition.

    I But remember! There are many ways to non-neutralityI Wage rigidities, information frictions ...

    Holm Monetary Policy, Lecture 3 25 / 27

  • Short Summary

    Today we’ve covered:

    I Firm problem w/o sticky prices

    I Monetary policy in a model w/o frictions

    You should know how to:

    I Solve the first-order conditions of the firm problem.

    I Interpret the first-order conditions.

    I Interpret α in the firm problem.

    I Solve the model without sticky prices.

    ... and understand why we need to add frictions to the RBC model to getshort-run monetary policy non-neutrality.

    Holm Monetary Policy, Lecture 3 26 / 27

  • Next week

    I The firm problem with sticky prices.

    Holm Monetary Policy, Lecture 3 27 / 27