電力期權(quán)的定價(jià)
[Abstract]:In recent years, with the reform of the power industry market and the further development of the power derivatives market, many ordinary power options and some strange options have emerged, so the pricing of these options has become an urgent problem. Electricity is a kind of common resource, which can not be stored. This characteristic excludes the traditional spot market pricing method based on storage and the traditional method of pricing power option based on no arbitrage principle. Therefore, it is necessary to copy the electricity derivatives with electricity futures as the target. In this paper, two kinds of power options are described, one is heat rate dependent option (spark spread option), and the other is regional transmission option (locational spread option),. These two kinds of options are subjected to both geometric Brownian motion and mean recovery process. In this paper, the partial differential equation based on power futures and risk-free assets is established, and the pricing formulas of heat ratio related options and regional transmission options are obtained through unit conversion. In addition, a new numerical method is proposed to solve the partial differential equations of call options related to the heat rate by using the finite element method in the space direction and the finite difference method in the time direction. Finally, the numerical solution of Euclidean heat ratio dependent call option under geometric Brownian motion is obtained, and the error order between finite element solution and true solution of heat rate dependent call option is obtained by using spatial approximation discontinuity. The error order tends to be 2. The final conclusion shows that the numerical solution and the true solution obtained by the finite element method can be approximated and can be replaced each other, thus reflecting the importance of the numerical method mentioned in this paper.
【學(xué)位授予單位】:天津財(cái)經(jīng)大學(xué)
【學(xué)位級(jí)別】:碩士
【學(xué)位授予年份】:2013
【分類號(hào)】:F830.9;F224;O241.82
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