# ELECTRICITY REAL OPTIONS VALUATION

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1 Vol. 37 (6) ACTA PHYSICA POLONICA B No 11 ELECTRICITY REAL OPTIONS VALUATION Ewa Broszkiewicz-Suwaj Hugo Steinhaus Center, Institute of Mathematics and Computer Science Wrocław University of Technology Wyspiańskiego 7, 5-37 Wrocław, Poland (Received August 17, 6) In this paper a real option approach for the valuation of real assets is presented. Two continuous time models used for valuation are described: geometric Brownian motion model and interest rate model. The valuation for electricity spread option under Vasicek interest model is placed and the formulas for parameter estimators are calculated. The theoretical part is confronted with real data from electricity market. PACS numbers:.3.cj,.5.ey,.7. c 1. Introduction The liberalization of electricity market caused that modeling on this market became very important skill. It helps us to minimize loss and hedge our position. It is a very interesting fact that spread option could be used for valuation of some real assets as power plants or transmission lines. But before that we need to know the spread option price formula. Very popular model used for option valuation is the geometric Brownian motion model but it is not very efficient. In the 5 the idea of modeling domestic electricity market using interest rate model was introduced by Hinz, Grafenstein, Verschue and Wilhelm [1]. They valuated European call option written on power forward contract under Heath Jarrow Morton model and, in this way, created very interesting class of models. The aim of my work is the valuation and calibration of electricity spread option under interest rate model applied for electricity market. I start with assumption of Vasicek model and using martingale methodology [] valuate spread option. Using the maximum likelihood function methodology Presented at the nd Polish Symposium on Econo- and Sociophysics, Kraków, Poland, April 1, 6. (955)

3 Electricity Real Options Valuation 957 is moved from the place of lower price to the place of higher price and this is why the transaction is profitable. The whole transaction depends on the difference between the electricity prices and also on delivery costs and for hedging we could use options. This kind of instrument could be defined in following way [3]: An European call option on the locational spread between the location one and location two, with maturity T, gives its holder the right but not the obligation to pay the price of one unit of electricity at location one at time T and receive the price of K units of electricity at location two. Assume that P 1 and P are the electricity prices at the first location and second location, respectively. The payoff of the European locational spread call option is given by C L (P 1, P, T ) = max [P 1 (T ) KP (T ), ]. The put option is defined similar and the payoff of the European electricity fuel spread put option has the form P L (P 1, P, T ) = max [KP (T ) P 1 (T ), ]. 3. Real options Suppose that for describing the commodity we use three qualities (G, t, L): G the nature of good, t time when it is available, L location it is available. We could define [5] a real option as technology to physically convert one or more input commodities (G, t, L) into an output commodity (G, t, L ). For example, most of power plants are real option because they give us the right to convert fuel into electricity. The transmission line is also real option. It gives us the right to change the electricity in one location into electricity in second location. The works of Deng, Johnson and Sogomonian [3, 6] contain two formulas defining how to valuate generation and transmission assets. If we define that u F (t) is a one unit of the time-t right to use generation asset we could say that it is the value of just maturing, time-t call option on the spread between electricity and fuel prices C F (t) and the one unit value of capacity of power plant using some fuel F is given by V F = u F (t)dt = C F (t)dt, T is the length of power plant life. Similarly if we define that u AB L (t) is a one unit of the time-t right to convert one unit of electricity in location A into one unit of electricity in location B we could say that it is the value of just maturing, time-t call

4 958 E. Broszkiewicz-Suwaj option on the spread between electricity prices in location A and B CL AB(t). The one unit value of such transmission asset is given by V L = u AB L (t)dt + u BA L (t)dt = T is the length of transmission network life. 4. Valuation methods CL AB (t)dt + C BA L (t)dt, In this section I present the widely known geometric Brownian motion model and valuate the call spread option for the new, interest rate model using martingale methodology. All calculations are described below Geometric Brownian motion model Suppose that the future prices of commodity are described by following stochastic differential equations dp 1 (t, T ) = µ 1 P 1 (t, T )dt + σ 1 P 1 (t, T )dw t,1, dp (t, T ) = µ P (t, T )dt + σ P (t, T )dw t,, W t,1 = ρw t, + 1 ρ W t, and W t,, W t, are i.i.d. Brownian motions. It is known fact [5], that the price of the spread call option with swap ratio K and time to maturity T, written on futures contract with maturity U < T is given by C 1 (t) = e r(t t) [P 1 (t, U)Φ(d + (t)) KP (t, U)Φ(d (t))], and d ± (t) = ln P 1(t,U) KP (t,u) ± σ (T t) σ, T t σ = σ 1 σ 1 ρσ + σ. 4.. Interest rate model For domestic currency, for example MWh, we denote two processes: p 1 (t, T ), p (t, T ) which are the future prices of one unit of commodity. The interest rate functions for such processes are, respectively: dr t,1 = (a 1 b 1 r t,1 )dt + σ 1 dw t,1,

5 Electricity Real Options Valuation 959 and dr t, = (a b r t, )dt + σ dw t,, W t,1 = ρw t, + 1 ρ W t, and W t,, W t, are i.i.d. Brownian motions. We assume that there exist the savings security N t (for example in USD), with constant interest rate r, for which P (t, T ) = p(t, T ) e rt N t is the USD price of future delivery of 1 unit of commodity. We know [1] that there exist a martingale measure P for which the discounted processes p 1 (t, T )/N t, p (t, T )/N t are martingales. We have C () = ( ) N E P (p 1 (T, U) Kp (T, U)) + N 1 T F e r. N We define the new discounting processes for i = 1, as db t,i = B t,i r t,i dt, B,i = 1. If we change the measure from P to P 1 dp dp 1 = N T B,1 N B T,1 we know that processes p 1 (t, T ) = p 1 (t, T )/B t,1, p (t, T ) = p (t, T )/B t,1 are P 1 -martingales. From interest rate theory we obtain d p 1 (t, T ) = p 1 (t, T )n 1 (t, T )dw t,1, n 1 (t, T ) = σ 1 b 1 ( 1 e b 1(T t) ). (1) If we change the measure again from P 1 to P dp 1 dp = B T,1B, B,1 B T, we know that ˆp (t, T ) = p (t, T )/B t, and ˆp 1 (t, T ) = p 1 (t, T )/B t, = p 1 (t, T )B t,1 /B t, are P -martingales and similar to the earlier situation, we have d ˆp (t, T ) = ˆp (t, T )n (t, T ) dw t,, ()

6 96 E. Broszkiewicz-Suwaj n (t, T ) = σ ( ) 1 e b (T t). (3) b After simple calculations we also have We also assume that d ˆp 1 (t, T ) = ˆp 1 (t, T )n 1 (t, T ) d W t,1, (4) W t,1 = ρw t, + 1 ρ W t,, W t, = W t, + r t,1 r t, n 1 (t, T ) 1 ρ t. d ˆN t = ˆN t vdv t, (5) V t = ρ 1 W t, + 1 ρ 1 W t,, and W t,, W t,, W t, are independent Wiener processes. For discounted processes following equation is true P i (t, T ) = p i(t, T ) e rt N t = ˆp i(t, T ) e rt ˆN t. (6) Having the necessary stochastic differential equations we could price the option. We change the measure from P to Q in the following way dp dq = B T,p (, U) B, p (T, U). Process X(t, T ) = p 1 (t, T )/p (t, T ) = From Itô Lemma we know that ˆp 1 (t, T )/ ˆp (t, T ) is Q-martingale. dx(t, T ) = X(t, T )(n 1 (t, T )dŵt,1 n (t, T )dw t, ), Ŵt,1 =ρw t, + 1 ρ Ŵ t, and Ŵt, = W t, + n (t,t ) n (t,t )ρn 1 (t,t ) t. n 1 (t,t ) 1 ρ Now, for calculation of the option price, we could use the Black Scholes formula ( C () = p (p1 (, U)e r ) ) (T, U) + E Q N p (T, U) K F = P (, U)E Q ( (P (T, U) P 1 (T, U) K ) + F ) = P (, U)E Q ((X(T, U) K) + F ) = P (, U)(X(, U)Φ(d + ) KΦ(d )) = P 1 (, U)Φ(d + ) KP (, U)Φ(d ),

7 σ (t, T ) = t Electricity Real Options Valuation 961 d ± = ln X(,U) K σ(, U) ± σ (,U) ( n 1 (u, T ) n (u, T )ρn 1 (u, T ) + n (u, T ) ) du, and Φ is the normal cumulative distribution function. For every time point t T the option price with swap ratio K and time to maturity T, written on futures contract with maturity U < T is given by C (t) = P 1 (t, U)Φ(d + (t)) KP (t, U)Φ(d (t)), d ± (t) = ln P 1(t,U) KP (t,u) ± σ (t,u). σ(t, U) This methodology could be used directly for locational spread options and also for fuel electricity spread options if we assume that the swap ratio between MWh and unit of fuel is one. 5. Historical calibration In this section we describe how to fit our models for real, historical data. At the beginning we assume that we are given historical prices of future contracts P 1 (t k, T j ) and P (t k, T j ), k =,..., n, j =,..., m, in discrete time points t < t 1 <... < t n and T < T 1 <... < T m, t k+1 t k = dt and T j+1 T j = T. For geometric Brownian motion model the calibration methodology is not very complicated. We analyze the returns of future prices of instrument and µ is its mean, σ is its variance and correlation parameter is simply the correlation between returns of two instruments. But for interest rate model the calibration is quite complicated, especially for multidimensional HJM model [7]. Calibration for discussed Vasicek model is presented below. Let us consider the following process From Itô Lemma we know that η i (t, T j ) = ˆp i(t, T j ) ˆp i (t, T j+1 ) = P i(t, T j ) P i (t, T j+1 ). (n dη i (t, T j ) = η i (t, T j )[ i (t, T j+1 ) n i (t, T j+1 )n i (t, T j ) ) dt ] + (n i (t, T j ) n i (t, T j+1 )) dw t,i.,

8 96 E. Broszkiewicz-Suwaj We could write that n i (t, T ) = n i (T t) because this function depends only on the difference between the maturity time T and the time point t. If we then consider the process s i (T t) = dη i(t, T ) η i (t, T ), we know that s i (T t) is normally distributed with mean and variance α i (T t) = ( n i (T + T t) n i(t + T t)n i (T t) ) dt β i (T t) = (n i(t t) n i (T + T t)) dt. Knowing the form of functions n i (T t) (1), (3) we see that and β i (T t) = ( ) σi e b i(t t) [1 e bi T ] dt (7) b i βi (T t) βi (T t + dt) = eb idt. (8) After discretization and for assumption that dt = T = 1, T t = p T and j = 1,..., m we could say that the estimator of β has the form ˆβ i (p T ) = 1 m m ( ) s i,j (p T ) s i,j (p T ) s i, j=1 and we put s i = 1 m m s i,j (p T ) j=1 s i,j (p T ) = So using (7), (8) we have P i (T j p T,T j ) P i (T j p T,T j + T ) P i(t j (p+1) T,T j ) P i (T j (p+1) T,T j + T ). P i (T j p T,T j ) P i (T j p T,T j + T ) ˆbi = 1 T ln ˆβi (p T ) ˆβ i ((p + 1) T ),

9 Electricity Real Options Valuation 963 ˆσ i = ˆβ i (p T )ˆbi e ˆb i (p T ) [1 e ˆb i T ]. It is easy to notice that the correlation parameter between processes s 1 (T t) and s (T t) is ρ, so we have m j=1 ˆρ = (s 1,j(p T ) s 1 )(s,j (p T ) s ) m j=1 (s m. 1,j(p T ) s 1 ) j=1 (s,j(p T ) s ) At the end we should calculate also parameters connected with process N t. From equation (6) we know that for i = 1, ξ i (t, T ) = ˆp i(t, T ) ˆN t = e rt P i (t, T ). Using Itô Lemma and formulas (5), (4), () we could calculate following dynamic dξ (t, T ) = ξ (t, T ) [ v ] vn (t, T )ρ 1 dt [ + ξ (t, T ) (n (t, T ) vρ 1 )dw t, v 1 ρ 1 ] dw t,. We know that the process y(t t) = dξ (t, T ) ξ (t, T ) is normally distributed with mean (v vn (t, T )ρ 1 )dt and variance (n (t, T ) vn (t, T )ρ 1 + v )dt so we have that for dt = 1 and and m ˆv = ˆn (p T ) + ȳ j=1 (y j(p T ) ȳ) m m j=1 (y j(p T ) ȳ), ˆρ 1 = ˆv ȳ ˆvˆn (p T ), y j (p T ) = e r T P i (T j p T, T j ) P i (T j (p + 1) T, T j ) P i (T j (p + 1) T, T j ) T ȳ = 1 m m y j (p T ). j=1,

10 964 E. Broszkiewicz-Suwaj 6. Simulation and conclusion For simulation I used the data from New York Mercantile Exchange (NYMEX). I considered historical quotation of future natural gas (Henry Hub) and electricity (PJM) contracts since January 4 until March 6. The parameters were calculated using calibration methods described before. All estimated parameters are presented in Table I. I assumed that the constant interest rate is r =.5. For valuation of gas fired power plant I assumed that the life-time of the power plant is T = 15 years and P E, = USD, P F, = 6.38 USD. TABLE I Estimated parameters for GBM model and for interest rate model using historical data from New York Mercantile Exchange. Geometric Brownian Motion Interest Rate Model σ e σ e.678 σ g σ g.4 µ e b e µ g b g 1.85 ρ.8688 ρ.189 ρ v.668 In Fig. 1 we see the value of power plant for the heat rate ranging from 5 to 15 for both presented models. We could notice that there is difference in changes dynamic for analyzed models. The value of power plant for interest rate model is much more smaller than for GBM model and it tends to zero when the heat rate goes up. It is a very good feature, because in reality the value of power plant for heat rate greater than P E, /P F, 9 should be close to zero. Looking at work of Deng we could say, that the value of power plant under GBM model is usually too high, so also in this aspect the interest rate model gives better results.

11 Electricity Real Options Valuation Gas MMBtu Electricity MWh Future Price Time to maturity (weeks) Power plant price GBM Interest Rate Heat Rate Fig. 1. Top panel: Future prices of natural gas and electricity for contract maturing in March, 6. Bottom panel: Simulated unit value of gas fired power plant, with life length 15 years, for both models. REFERENCES [1] J. Hinz, L. Grafenstein, M. Verschuere, M. Wilhelm, Quantitative Finance 5, 49, (5). [] M. Musiela, M. Rutkowski, Martingale Methods in Financial Modelling, Springer, [3] S. Deng, B. Johnson, A. Sogomonian, Proceedings of the Chicago Risk Management Conference, [4] A. Weron, R. Weron, Power Exchange: Tools for Risk Management, CIRE, Wrocław,. [5] E. Ronn, Real Option and Energy Management: Using Options Methodology to Enhance Capital Budgeting Decisions, Risk Books, 4. [6] S. Deng, Stochastic Models of Energy Commodity Prices and Their Applications: Mean-reversion with Jumps and Spikes, POWER papers,. [7] E. Broszkiewicz-Suwaj, A. Weron, Acta Phys. Pol. B 37, 1455 (6).

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