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Energy Efficiency and Rebound Effects: An Econometric Analysis of Energy Demand in the Commercial Building Sector

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Abstract

It is widely recognized that the adoption of energy saving innovations can induce an increase in the usage of the corresponding technologies and thus can possibly increase energy consumption. Among other concerns is that uncertainties regarding the magnitude of this “rebound effect” can deter policy makers from promoting energy efficiency. This paper analyzes the rebound effects of the adoption of energy efficient technologies in commercial buildings. Based upon a structural model of technology adoption and subsequent energy demand at the building level, the empirical results are that energy efficiency can reduce electricity use by about 35 % and natural gas consumption by about 50 %.

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Notes

  1. In this paper, I use EIA’s definition of commercial buildings: Commercial buildings include all buildings in which at least half of the floorspace is used for a purpose that is not residential, industrial, or agricultural, so they include building types that might not traditionally be considered “commercial,” such as schools, correctional institutions, and buildings used for religious worship.

  2. We will discuss in more detail in Sect. 5.1 why the technologies analyzed for electricity and natural gas uses are different.

  3. I treat the behaviors and decision makings of all the people in a commercial building as a whole. So when I say commercial buildings consume energy or make decisions in this paper, it is equivalent to say people in the commercial buildings consume energy or make decisions—similar to the concept of a firm’s behavior.”

  4. http://www.eia.gov/consumption/commercial/

  5. This range is not calculated from the 95 % confidence intervals of each coefficient. It is a range of the mean values calculated from the means of the coefficients.

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Correspondence to Yueming Qiu.

Additional information

This paper is modified from a chapter of my doctoral dissertation at Stanford University. I would like to thank the Precourt Energy Efficiency Center for the funding that made this research possible. I would also like to thank Matt Harding and Luigi Pistaferri from Stanford Department of Economics, Jim Sweeney from Stanford Department of Management Science and Engineering, Laura Diaz Anadon from Harvard Kenney School, Kenny Gillingham from Yale School of Forestry and Environmental Studies, and Yi David Wang from University of International Business and Economics for extremely useful suggestions, Shirley Neff and Joelle Michaels from US Energy Information Administration for providing advice on the Commercial Buildings Energy Consumption Survey data. Any remaining errors are my own responsibility.

Appendix: Derivation of the Modified Heckman Selection Model

Appendix: Derivation of the Modified Heckman Selection Model

The following is the modified Heckman selection model. The energy consumption of a building we can observe is a combination of two components:

$$\begin{aligned} Q_i =Q_i ^{1}T_i +Q_i ^{0}(1-T_i ), \end{aligned}$$

where \(Q_i ^{1}\) is the energy consumption of a building if it adopts an energy efficient technology; \(Q_i ^{0}\) is the consumption if a building does not adopt the technology. \(T_{i}=1\) means a building adopts the technology.

The expected value of the energy consumption is

$$\begin{aligned} E(Q_i )=E(Q_i \left| {T_i =1} \right. )\Pr (T_i =1)+E(Q_i \left| {T_i =0} \right. )\Pr (T_i =0) \end{aligned}$$

From equation \(Q_i =\mu +\beta \overline{p_i } +\gamma ngp_i +\delta X_i +\eta Y_{j(i)} +\theta _i T_i +\varepsilon _i \), we have

$$\begin{aligned} Q_i ^{1}&= \mu +\theta +\beta \overline{p_i } +\gamma ngp_i +\delta X_i +\eta Y_{j(i)} +\varepsilon _i +\nu _i\\&= \mu ^{1}+\beta \overline{p_i } +\gamma ngp_i +\delta X_i +\eta Y_{j(i)} +\varepsilon ^{1}_i\\ Q_i ^{0}&= \mu +\beta \overline{p_i } +\gamma ngp_i +\delta X_i +\eta Y_{j(i)} +\varepsilon _i =\mu ^{0}+\beta \overline{p_i } +\gamma ngp_i +\delta X_i +\eta Y_{j(i)} +\varepsilon ^{0}_i \end{aligned}$$

where \(\mu ^{1}=\mu +\theta ,\,\varepsilon ^{1}_i =\varepsilon _i +\nu _i ,\,\mu ^{0}=\mu ,\,\varepsilon ^{0}_i =\varepsilon _i \)

Thus

$$\begin{aligned} Q_i&= \mu ^{0}+\beta \overline{p_i } +\gamma ngp_i +\delta X_i +\eta Y_{j(i)} +(\mu ^{1}-\mu ^{0})T_i +\varepsilon ^{0}_i +(\varepsilon ^{1}_i -\varepsilon ^{0}_i )T_i\\ E(Q_i \left| {T_i =1} \right. )&= \mu ^{1}+\beta \overline{p_i } +\gamma ngp_i +\delta X_i +\eta Y_{j(i)} +E(\varepsilon ^{1}_i \left| {T_i =1} \right. ) \\ E(Q_i \left| {T_i =0} \right. )&= \mu ^{0}+\beta \overline{p_i } +\gamma ngp_i +\delta X_i +\eta Y_{j(i)} +E(\varepsilon ^{0}_i \left| {T_i =0} \right. ) \end{aligned}$$

Assume that \(\varepsilon ^{1}_i ,\,\varepsilon ^{0}_i \) and \(\omega _i \) are all normally distributed random variables with mean zero and covariance matrix as follows:

$$\begin{aligned} \left[ {{\begin{array}{l@{\quad }l@{\quad }l} {\sigma _{\varepsilon ^{1}}^2 }&{} &{} \\ {\sigma _{\varepsilon ^{1}\varepsilon ^{0}} }&{} {\sigma _{\varepsilon ^{0}}^2 }&{} \\ {\sigma _{\varepsilon ^{1}\omega } }&{} {\sigma _{\varepsilon ^{0}\omega } }&{} {\sigma _\omega ^2 } \\ \end{array} }} \right] \end{aligned}$$

Then

$$\begin{aligned} E(\varepsilon _i^1 \left| {T_i =1} \right. )&= E\left( \varepsilon _i^1 \left| {\omega _i \ge -(\Psi _0 +\Psi _1 C_{j(i)} +\Psi _2 Z_{j(i)} +\Psi _3 X_i +\Psi _4 Y_{j(i)} +\Psi _5 U_i )} \right. \right) \\&= \sigma _{\varepsilon ^{1}\omega } \frac{\phi (\Psi _0 +\Psi _1 C_{j(i)} +\Psi _2 Z_{j(i)} +\Psi _3 X_i +\Psi _4 Y_{j(i)} +\Psi _5 U_i )}{\Phi (\Psi _0 +\Psi _1 C_{j(i)} +\Psi _2 Z_{j(i)} +\Psi _3 X_i +\Psi _4 Y_{j(i)} +\Psi _5 U_i )} \\ E(\varepsilon _i^o \left| {T_i =0} \right. )&= E\left( \varepsilon _i^0 \left| {\omega _i \le -(\Psi _0 +\Psi _1 C_{j(i)} +\Psi _2 Z_{j(i)} +\Psi _3 X_i +\Psi _4 Y_{j(i)} +\Psi _5 U_i )} \right. \right) \\&= -\sigma _{\varepsilon ^{0}\omega } \frac{\phi (\Psi _0 +\Psi _1 C_{j(i)} +\Psi _2 Z_{j(i)} +\Psi _3 X_i +\Psi _4 Y_{j(i)} +\Psi _5 U_i )}{1-\Phi (\Psi _0 +\Psi _1 C_{j(i)} +\Psi _2 Z_{j(i)} +\Psi _3 X_i +\Psi _4 Y_{j(i)} +\Psi _5 U_i )} \end{aligned}$$

Define

$$\begin{aligned} a_i&= 1-\Phi (\psi _0 +\psi _1 C_{j(i)} +\psi _2 Z_{j(i)} +\psi _3 X_i +\psi _4 Y_{j(i)} +\psi _5 U_i ) \\ b_i&= \Phi (\psi _0 +\psi _1 C_{j(i)} +\psi _2 Z_{j(i)} +\psi _3 X_i +\psi _4 Y_{j(i)} +\psi _5 U_i )=1-a_i \\ c_i&= \varphi (\psi _0 +\psi _1 C_{j(i)} +\psi _2 Z_{j(i)} +\psi _3 X_i +\psi _4 Y_{j(i)} +\psi _5 U_i ) \end{aligned}$$

where \( a_{i}\) is the probability that building \(i\) does not adopt the energy efficient technology; \(b_{i}\) is the probability that building \(i\) adopts the technology; \(c_{i}\) can be interpreted as the probability that the latent variable \(S_{i}\) takes on a certain value. These three variables are estimated from the probit model.

The expectation of the energy demand we observe is

$$\begin{aligned} E(Q_i )&= E(Q_i \left| {T_i =1} \right. )\Pr (T_i =1)+E(Q_i \left| {T_i =0} \right. )\Pr (T_i =0) \\&= \mu ^{1}b_i +(\beta \overline{p_i } +\gamma ngp_i +\delta X_i +\eta Y_{j(i)} )b_i +\sigma _{\varepsilon ^{1}\omega } c_i +\mu ^{0}a_i \\&\quad +\,(\beta \overline{p_i }+\,\gamma ngp_i +\delta X_i +\eta Y_{j(i)} )a_i -\sigma _{\varepsilon ^{0}\omega } c_i \end{aligned}$$

Because \(a_i +b_i =1\)

$$\begin{aligned} E(Q_i )=\mu ^{0}+(\mu ^{1}-\mu ^{0})b_i +(\sigma _{\varepsilon ^{1}\omega } -\sigma _{\varepsilon ^{0}\omega } )c_i +\beta \overline{p_i } +\gamma ngp_i +\delta X_i +\eta Y_{j(i)} \end{aligned}$$

Thus the final form of the modified Heckman selection model that estimates the average of the price elasticties across all buildings is

$$\begin{aligned} E(Q_i )=\mu ^{0}+\theta b_i +(\sigma _{\varepsilon ^{1}\omega } -\sigma _{\varepsilon ^{0}\omega } )c_i +\beta \overline{p_i } +\gamma ngp_i +\delta X_i +\eta Y_{j(i)} \end{aligned}$$

Now let us look at the model that can allow the estimation of two price elasticities: one average elasticity for buildings that adopt energy efficient technologies and one for buildings that do not.

Assume that \(\beta \) in Eqs. (9) and (10) are different:

$$\begin{aligned} Q_i ^{1}&= \mu ^{1}+\beta ^{1}\overline{p_i } +\gamma ngp_i +\delta X_i +\eta Y_{j(i)} +\varepsilon ^{1}_i\\ Q_i ^{0}&= \mu ^{0}+\beta ^{0}\overline{p_i } +\gamma ngp_i +\delta X_i +\eta Y_{j(i)} +\varepsilon ^{0}_i \end{aligned}$$

Then

$$\begin{aligned} E(Q_i )&= E(Q_i \left| {T_i =1} \right. )\Pr (T_i =1)+E(Q_i \left| {T_i =0} \right. )\Pr (T_i =0) \\ \!&= \!\left[ \mu ^{1}\!+\!\beta ^{1}\overline{p_i } \!+\!\gamma ngp_i \!+\!\delta X_i \!+\!\eta Y_{j(i)} \!+\!\sigma _{\varepsilon ^{1}\omega } \frac{c_i }{b_i }\right] b_i \!+\!\left[ \mu ^{0}\!+\!\beta ^{0}\overline{p_i } \!+\!\gamma ngp_i \!+\!\delta X_i \right. \\&\quad \left. +\,\eta Y_{j(i)} -\sigma _{\varepsilon ^{0}\omega } \frac{c_i }{a_i }\right] a_i \end{aligned}$$

Thus the final form of the modified Heckman selection model which allows estimating two price elasticities is

$$\begin{aligned} E(Q_i )=\mu ^{0}+\theta b_i +(\sigma _{\varepsilon ^{1}\omega } -\sigma _{\varepsilon ^{0}\omega } )c_i +\beta ^{1}\overline{p_i } b_i +\beta ^{0}\overline{p_i } a_i +\gamma ngp_i +\delta X_i +\eta Y_{j(i)} \end{aligned}$$

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Qiu, Y. Energy Efficiency and Rebound Effects: An Econometric Analysis of Energy Demand in the Commercial Building Sector. Environ Resource Econ 59, 295–335 (2014). https://doi.org/10.1007/s10640-013-9729-9

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