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Research Papers

Higher moments in the fundamental specification of electricity forward prices

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Pages 2063-2078 | Received 07 Jun 2022, Accepted 26 Aug 2022, Published online: 29 Sep 2022
 

Abstract

An extended specification for estimating the risk premia necessary for the forward pricing of wholesale electricity is developed in order to respond to the increasing need for more precise risk management of hedging positions in practice. Using Taylor expansions, we provide new specifications for the electricity forward premium including its dependency on all four moments of the expected wholesale price density as well as the higher moments of the demand density including skewness and kurtosis. Overall we argue that previous models have been underspecified and that the extended formulation proposed in this analysis is robust and worthwhile.

Disclosure statement

No potential conflict of interest was reported by the author(s).

Notes

1 We can arrive at (Equation3), just by taking the cubic Taylor approximation of a simpler function g(x)=(xb+1cPRxb) and multiplying it by (xμW).

2 For instance, consider h(x)=ex and the corresponding quartic Taylor polynomial (around x = 0): p4(x)=1+x+x2/2+x3/6+x4/24. If XN(0,1) we can compute E[eX]=e1/21.649 and E[p4(X)]=13/8=1.625 and we see that the quartic Taylor approximation holds reasonably well also for the expectations. However, if X has a Laplace distribution with parameter λ(0,1), that is X=λ(Y1Y2) where Y1 and Y2 are independent and exponentially distributed with mean 1, then we can compute E[eX]=(1λ2)1. Next, we have E[X]=E[X3]=0, E[X2]=2λ2 and E[X4]=24λ4, so that E[p4(X)]=1+λ2+λ4. We see that E[p4(X)] can be far away from E[eX] if λ is close to 1. For instance, if λ=0.9, then the former expectation is 5.26, while the latter one is just 2.47.

3 They show from a detailed analysis of German prices that these prices, under a wide range of market conditions, can be characterized by two-, three- and four-moment distributions.

4 In other words we consider the distributions left-truncated at 0, which is in line with van Koten (Citation2020). However, differently from him, we do not discard replicates outside the interval μ±5σ.

5 Convexity can be observed also in the case c = 2, 3 and λ=1.2 by widening suitably the range for σD. In figure we kept the range (1,40) for σD in order to ease the comparison with results in van Koten (Citation2020).

6 Data is from the website www.destatis.com accessed in February 2022.

7 Γ denotes the Gamma function.

Additional information

Funding

This work was supported by the Università Degli Studi di Modena e Reggio Emila [grant number FAR2021].

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