Skip to main content

Advertisement

Log in

Quantifying the CO2 Permit Price Sensitivity

Quantifizierung der CO2-Zertifikate-Preis Sensitivität

  • Published:
Zeitschrift für Energiewirtschaft Aims and scope Submit manuscript

Abstract

Equilibrium models have been widely used in the literature with the aim of showing theoretical properties of emissions trading schemes. This paper applies equilibrium models to empirically study permit prices and to quantify the permit price sensitivity. In particular, we demonstrate that emission trading schemes both with and without banking are inherently prone to price jumps.

Zusammenfassung

Zur Untersuchung der theoretischen Eigenschaften von Emissionshandelssystemen wurden in der Literatur meist Gleichgewichtsmodelle genutzt. In diesem Artikel nutzen wir Gleichgewichtsmodelle zur empirischen Untersuchung von Zertifikatepreisen und ihren Sensitivitäten. Wir zeigen insbesondere, daß Emissionshandelssysteme (auch wenn Banking zugelassen ist) Preisprozesse generieren, die Sprünge enthalten.

This is a preview of subscription content, log in via an institution to check access.

Access this article

Subscribe and save

Springer+ Basic
$34.99 /Month
  • Get 10 units per month
  • Download Article/Chapter or eBook
  • 1 Unit = 1 Article or 1 Chapter
  • Cancel anytime
Subscribe now

Buy Now

Price excludes VAT (USA)
Tax calculation will be finalised during checkout.

Instant access to the full article PDF.

Fig. 1
Fig. 2
Fig. 3
Fig. 4
Fig. 5
Fig. 6
Fig. 7

Similar content being viewed by others

Notes

  1. An overview of the exact numerical computation methods for an integral over a geometric Brownian motion can be found in the book of Jeanblanc et al. (2009) in Sect. 6.6.

  2. The corresponding European-style call option pays off the maximum of zero and the difference between the asset price at maturity and the strike price, i.e. max(S T K,0). Asian-style options are popular because they are cheaper compared to European-style options as the averaging reduces the volatility.

  3. For a more detailed explanation see Chap. 3 in Grüll (2010).

  4. The trajectory of x t is based on (3), (4) and (7).

  5. The permit price trajectories are obtained by plugging the trajectory of x t (see Fig. 1) into the permit price formulae of Lemma 1.

  6. Lower and upper bounds are obtained by considering the permit prices of \(\mathbb {E}(q_{[0,t]} ) \pm c \sqrt{Var (q_{[0,t]} )}\) which is the confidence band for outstanding emissions.

  7. In phase I of the EU ETS the banking of permits was not allowed, i.e. permits that were not used in phase I (2005–2007) could not be handed in for compliance purposes in phase II (2008–2012). From phase II on the banking of permits is allowed.

  8. The derivation of this result is to be found in the Appendix.

  9. The volatility of the outstanding emissions of all regulated companies in the EU ETS is assumed to be smaller than 5 percent. This is motivated by the verified emissions data of the years 2005–2010. The annual percentage change remained in the confidence band [−10 %,+10 %] that is implied by our assumption.

References

  • Carmona R, Fehr M, Hinz J, Porchet A (2009) Market design for emission trading schemes. SIAM Rev 9(3):465–469

    MathSciNet  Google Scholar 

  • Chesney M, Taschini L (2008) The endogenous price dynamics of emission allowances and an application to CO2 option pricing. Preprint

  • Cronshaw M, Kruse J (1996) Regulated firms in pollution permit markets with banking. J Regul Econ 9(2):179–189

    Article  Google Scholar 

  • European Union (2006) EU emissions trading scheme delivers first verified emissions data for installations. Press release IP/06/612. Brussels

  • Grüll G (2010) Modelling CO2 permit prices. Universität Duisburg-Essen, Universitätsbibliothek

  • Grüll G, Taschini L (2011) Cap-and-trade properties under different hybrid scheme designs. J Environ Econ Manag 61(1):107–118

    Article  MATH  Google Scholar 

  • Hepburn C (2009) In: Helm D, Hepburn C (eds) Carbon taxes, emissions trading, and hybrid schemes. The economics and politics of climate change. Oxford University Press, London, pp 365–384

    Google Scholar 

  • Hitzemann S, Uhrig-Homburg M (2010) Understanding the price dynamics of emission permits: a model for multiple trading periods. Preprint

  • Jacoby HD, Ellerman AD (2004) The safety valve and climate policy. Energy Policy 32(4):481–491

    Article  Google Scholar 

  • Jeanblanc M, Yor M, Chesney M (2009) Mathematical methods for financial markets. Springer, Berlin

    Book  MATH  Google Scholar 

  • Kling C, Rubin J (1997) Bankable permits for the control of environmental pollution. J Public Econ Theory 64:101–115

    Google Scholar 

  • Milevsky MA, Posner SE (1998) Asian options, the sum of lognormals, and the reciprocal gamma distribution. J Financ Quant Anal 33(3):409–421

    Article  Google Scholar 

  • Murray BC, et al. (2009) Balancing cost and emissions certainty: an allowance reserve for cap-and-trade. Rev Environ Econ Policy 1(3):84–103

    Google Scholar 

  • Roberts MJ, Spence M (1976) Effluent charges and licenses under uncertainty. J Public Econ 3(5):193–208

    Article  Google Scholar 

  • Rubin J (1996) A model of intertemporal emission trading, banking and borrowing. J Environ Econ Manag 31:269–286

    Article  MATH  Google Scholar 

  • Seifert J, Uhrig-Homburg M, Wagner M (2008) Dynamic behavior of CO2 spot prices—theory and empirical evidence. J Environ Econ Manag 56(2):180–194

    Article  MATH  Google Scholar 

Download references

Author information

Authors and Affiliations

Authors

Corresponding author

Correspondence to Rüdiger Kiesel.

Appendix: Derivation of Permit Price Formulae and Sensitivities

Appendix: Derivation of Permit Price Formulae and Sensitivities

The derivation of the permit prices for the different approximation approaches is split up into three parts. We start by presenting the first two moments of the outstanding emissions in the time period [t 1,t 2] denoted by \(q_{[t_{1},t_{2}]} = \int_{t_{1}}^{t_{2}} Q_{s} ds\) (see Sect. 6.1). Then, we derive the parameters of the random variables that are used to approximate the outstanding emissions (cf. Lemma 4 in Sect. 6.2). Finally, the permit price formulae are derived in Sect. 6.3.

1.1 6.1 Moments of Outstanding Emissions

Milevsky and Posner (1998) prove the following lemma for the integral over a geometric Brownian motion.

Lemma 3

(Moments of \(q_{[t_{1},t_{2}]}\))

Let \(Q_{s} = Q_{0} \exp \{ ( \mu- \frac{\sigma^{2}}{2} ) s + \sigma W_{s} \}\) be a geometric Brownian motion. Then the first two moments of \(q_{[t_{1},t_{2}]} = \int_{t_{1}}^{t_{2}} Q_{s} ds\) are given by

(16)
(17)

where

(18)
(19)

Lemma 3 shows that \(\alpha_{t_{2}-t_{1}}\) is approximately linear and that \(\beta_{t_{2}-t_{1}}\) is approximately a quadratic function for small μ and σ. Therefore, expected outstanding emissions are approximately linear.

1.2 6.2 Moment Matching/Determining Parameters of Approximating Random Variables

Lemma 4

(Overview on approximations)

Let τ=Tt and ZN(0,1). The outstanding emissions q [t,T] are approximated by the following random variables

  1. (a)

    Linear (interval length times GBM)

    (20)
  2. (b)

    Log-normal (moment matching)

    (21)

Proof

(a) Follows from (3) and (6).

(b) The parameters μ L (t,T) and σ L (t,T) are chosen such that the first two moments of \(q^{Log}_{[t,T]} = \log N(\mu_{L}(t,T), \sigma_{L}^{2}(t,T))\) match those of q [t,T].

Hence by Lemmas 3 and 5

Note that \(\sigma_{L}^{2}(t,T)\) is independent of Q t , μ L (t,T) not. □

1.3 6.3 Derivation of Permit Price Formulae

1.3.1 6.3.1 Proof of Lemma 2a (Linear Approximation Approach)

By (2) and (6) we have

Let ZN(0,1). Using (3) yields

1.4 6.4 Proof of Lemma 2b (Log-normal moment matching approach)

By (2) we have

Let ZN(0,1). Using (21) yields

Lemma 5

(Moments of log-normal random variable)

Let X∼logN(μ,σ 2). Then

  1. (a)

    The kth moment of X is given by

    $$\mu_k^{(X)} = e^{k\mu+ k^2 \frac{\sigma^2}{2}} $$
  2. (b)

    Let X∼logN(μ,σ 2) be a log-normal random variable with \(\mathbb {E}(X)=m_{1}\) and \(\mathbb {E}(X^{2})=m_{2}\). Then

Proof

(b) The first two moments of X∼logN(μ,σ 2) are given by

By assumption \(m_{2} = m^{2}_{1} e^{\sigma^{2}}\) and \(m_{1} = e^{\mu}\sqrt {e^{\sigma^{2}}}\). □

1.5 6.5 Proof of Lemma 3

As the proof for both approximation approaches is the same we only present the proof of part (a), i.e. (14). We assume that the observed permit prices \(\hat{S}_{t-\Delta}\) and \(\hat{S}_{t}\) can be described by the equilibrium price formula of the linear approximation approach given by (5) and Lemma 1, i.e.

Assuming that \(S_{t-\Delta}^{Lin} ( x_{t-\Delta} | \mu, \sigma ) \approx S_{t}^{Lin} ( x_{t-\Delta} | \mu, \sigma )\) implies

This yields

1.6 6.6 Proof that Price Drop Implies a Positive h (Implied Change in Permit Availability) Assuming that the Permit Price and the Share of Banking Value are Negatively Correlated

Without loss of generality the observed permit price at time t can be written as

$$\hat{S}_t = S_t + B_t := \gamma_t \hat{S}_t + (1-\gamma_t) \hat{S}_t $$

where γ t ∈(0,1). Especially, we have that

$$\frac{B_t}{\hat{S}_t} = 1 - \gamma_t $$

and

$$\hat{S}_t - B_t = \gamma_t \hat{S}_t $$

As Φ−1(⋅) is an increasing function, the implied change in permit availability h is positive if

$$\hat{S}_t - B_t < \hat{S}_{t-\Delta} - B_{t-\Delta} $$

which is equivalent to

(22)

By assumption a permit price drop coincides with an increase in the share of the banking value, i.e.

$$\frac{B_t}{\hat{S}_t} > \frac{B_{t-\Delta}}{\hat{S}_{t-\Delta}} $$

which is equivalent to

(23)

A decrease in the permit price and an increase in the share of the banking value imply that h is positive (cf. (22) and (23)):

Rights and permissions

Reprints and permissions

About this article

Cite this article

Grüll, G., Kiesel, R. Quantifying the CO2 Permit Price Sensitivity. Z Energiewirtsch 36, 101–111 (2012). https://doi.org/10.1007/s12398-012-0082-4

Download citation

  • Published:

  • Issue Date:

  • DOI: https://doi.org/10.1007/s12398-012-0082-4

Keywords

Navigation