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The Model with Input Complementarity

In document Essays in Applied Macroeconomics (Page 138-144)

In this section, we present a simple dynamic stochastic general equilibrium model with the normalized Translog production function. We make three deviations from the canonical real business cycle models: (i) we use the normalized Translog production function that generates complementarity-induced procyclical returns to scale ; (ii) we explicitly consider energy as an input and allow complementarity with labor to reflect our empirical findings ; (iii) we cast the model in a monopolistic competitive framework (as in conventional internal increasing returns to scale model) in which final goods firms

aggregate differentiated intermediate goods and sell them to households.24

In Figure 3.2, we plot the time series of labor and energy inputs in the United States. There is a strong positive comovements of these variables. Positive comovement of labor and energy, combined with our complementarity parameter βel > 0 will induce procyclical returns to scale under the normalized Translog production function.

3.4.1 Households

The economy is populated by a large number of identical infinitely lived households.

The representative household chooses sequence of consumption Ct, labor supplied Lt, investment It, capital stock Kt, and borrowing Bt to solve

Ct,Lmaxt,It,Kt,Bt

E0

X

t=0

βtU (Ct, Lt)

subject to the following budget constraint Ct+ It+Bt

Rt + Tt = RktKt−1+ Bt−1+ WtLt+ Πt+ Πet

24Since the returns to scale is procyclical, the production function could feature increasing returns to scale (in the boom periods). Thus, as in internal increasing returns to scale model, we need to have some mild degree of markups to make the model well-defined. Alternatively, we could cast the model in perfect competition with additional assumption that the production function features decreasing returns to scale at the steady state.

Then as long as the returns to scale parameter (which is determined endogenously) has value less than one, the model is well-defined.

Figure 3.2: Positive Comovement of Labor and Energy (HP filtered

Note. Data source : FRED and US Energy Information Administration. Labor is measured by log of hours per captia, and energy input is measured by log of total energy consumed by the industrial sector (measured in Btu) divided by population. We plot the HP filtered variables at the quarterly level. Y axis represents a percent deviation from the trend defined by the HP filter.

and the law of motion of capital

Kt = It+ (1 − δ) Kt−1 (3.4.1)

where R is a (gross) risk-free rate, Rk is real rental rate of capital, W is real wages, T is tax paid by the household in terms of consumption units, Π is the dividend paid to the households by the intermediate goods firms, and Πe is the dividend paid by the energy firms. We assume UC,t > 0, UCC,t ≤ 0, UL,t≤ 0, ULL,t ≤ 0.

The FOCs are given by

UC(Ct, Lt) = βEt UC(Ct+1, Lt+1)Rt+1k + 1 − δ 

(3.4.2) Wt= −UL(Ct, Lt)

UC(Ct, Lt) (3.4.3)

UC(Ct, Lt) = βRtEt[UC(Ct+1, Lt+1)] (3.4.4)

3.4.2 Final Goods Producers

The final goods producers purchase differentiated intermediate goods products and aggregate them using the Dixit-Stiglitz CES technology. We assume that the final goods sector is perfectlyd competitive. Each final goods producer solves

maxYt,Yit

Yt− Z 1

0

PitYitdi subject to

Yt=

Z 1 0

Yitλdi

1/λ

where Yt, Yit are the final and intermediate goods, respectively, and Pti is intermediate goods price. λ is the inverse of markup.

The optimality implies

Yit= Yt· Pit1/(λ−1) (3.4.5)

3.4.3 Intermediate Goods Producers

We assume a monopolistic competitive intermediate goods sector. The intermediate goods producers have technology characterized by the normalized Translog production function characterized by (3.3.1) and (3.3.4):

Yit= εat [(Kits)αkLαitlEitαe] ·

Here, Yit is intermediate goods output, Kits is capital services used in production, Lit is labor input, and Eit is energy input. ˜Lt and ˜Et are the aggregate labor and energy, which individual firms take as given. In the equilibrium, ˜Lt = Lt and ˜Et = Et hold.

Total factor productivity εat follows

log εat = ρalog εat−1+ ηta, ηta∼ N (0, σa2) (3.4.7) Each intermediate goods producer’s periodic profit is given by

Πit = PitYit− WtLit− RktKits − PteEit (3.4.8) where Wt, Rkt, and Pte are the aggregate real wage, the real rental rate of capital, and real energy price, respectively. Note that because there is no price rigidity, we are using the final good as a numeraire.

Each intermediate goods producer maximizes (3.4.8) subject to the demand for its output (3.4.5) and the technology (3.4.6). The FOCs, after dropping subscript i’s, are given by

Although we explicitly introduce energy as a factor inputy, we abstract from modeling the energy sector separately, following Rotemberg and Woodford (1996). In other words, there are no resource costs associated with energy production. As in

Rotemberg and Woodford (1996), energy is freely available at no cost to the oligopolistic firms that sell it, and the exogenous variations in Pte represent variations in the degree to which they succeed in colluding to keep the price of energy where they want it (here taken as given rather than modeled). Thus, the intermediate goods producers pay Pte to get energy input Et(i), and

Πet ≡ Pte Z 1

0

Eitdi = PteEt

directly becomes the profit of (implicit) energy firms. These profits are distributed to the shareholders, who are representative households in our model. We assume that energy price follows an exogenous process

log Pte= (1 − ρe) log Psse + ρelog Pt−1e + ηte, ηte ∼ N (0, σ2e) (3.4.12) In the Appendix C.2, we provide a model with the energy producing sector and make the energy price endogenous.25 The results are robust to this alternative specification.

3.4.4 Government

The government budget constraint is given by

Gt+ Bt−1= Tt+Bt

Rt (3.4.13)

where Gtis government spending, Ttis lump-sum taxes (or subsidies). We define gt = YGt

ss, where Yssis the steady-state value of output, and assume gt follows an exogenous process

log gt = (1 − ρg) log gss+ ρglog gt−1+ ηtg, ηgt ∼ N (0, σg2) (3.4.14) In the model, the government spending shock will be the source of exogenous demand shock. Yet, the implications hold to other types of demand shocks such as preference shock affecting marginal utility of consumption or shock on discount factor.

25See Kilian (2008) for discussion on energy price endogeneity.

3.4.5 Resource Constraints

The market clearing of capital implies Kts = Kt−1. Additionally, the social resource constraint can be written as

Yt= Ct+ Kt− (1 − δ)Kt−1+ Gt

The full description of the equilibrium conditions can be found in Appendix C.1.

3.4.6 Functional Form

To simulate the model, we impose the following functional form of the utility function, which is widely used in the literature.

U (C, L) = 1

Following the existing literature, we calibrate the model by setting the time interval as a quarter. We set the discount factor β = 0.99 and the degree of relative risk aversion σ = 1. We let the labor share αl = 0.7, the capital share αk = 0.24, and the energy share αe = 0.06, which are within the range of widely used values in the literature.26 Additionally, we set the steady state government spending to output ratio as g = 0.2, which is consistent with post-war U.S. data. The parameter governing labor disutility ψ is calibrated so that the steady state of L matches 1/3, which means that people work approximately one-third of the time. We calibrate 1/φ = 3.31, which is the average Frisch elasticity used in the RBC literature (Chetty et al. (2013)).

To calibrate the input complementarity parameter between labor and energy, βel, we bring the value from our micro-estimate. The first order condition with respect to energy input can be written as follows:

λYt

26Depending on the data source and the definition of value added, the energy share varies from 0.04 to 0.08.

We use an average of these values.

Defining the energy share as ΘetPtYeEt

t and log-linearizing the above equation yields:

Θˆet = ˜βelt (3.4.16) where ˜βel ≡ βele. Note that the equation (3.4.16) is the theoretical counterpart of equations (3.2.5) and (3.2.7) in our empirical analysis. Thus, our micro-estimate β˜el = 1.69 implies βel = 0.10, given the energy share αe= 0.06.

Recall that individual firms take the returns to scale of the economy as given. This means that under boom (bust) periods, individual firms face increasing (decreasing) returns to scale as long as labor and energy inputs are procyclical and βel > 0. As individual firms face increasing returns to scale in periods outside the steady state (especially during the boom), this requires positive markups as in typical internal increasing returns to scale model with monopolistic competition. We impose minimal degree of markup that makes the model well-defined, given the historical fluctuation of labor and energy which in turn affects the returns to scale defined by (3.3.5). As can be seen in Figure 3.2, the observed fluctuation of energy and labor inputs around long-run trend in the United States economy is in general less than 10%.27 Thus, by combining βel = 0.10 and the expression of returns to scale RT St in (3.3.5), we get the maximal returns to scale plausible in the US economy as RT St = 1 + 0.10 × (0.10 + 0.10) = 1.02.

Thus, 2% of markup is sufficient to make our model well-defined, which implies 1/λ = 1.02. Quantitatively, this makes no difference in a perfect competitive model. Thus we can interpret our calibrated model as an approximation of a perfect competitive economy, making the model directly comparable with standard RBC models.

We summarize our calibration strategy in Table 3.3.

In document Essays in Applied Macroeconomics (Page 138-144)