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ANALYSES OF THE CHAOTIC BEHAVIOR OF THE ELECTRICITY PRICE SERIES

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1 ANALYSES OF THE CHAOTIC BEHAVIOR OF THE ELECTRICITY PRICE SERIES
Radko Kříž University of Hradec Kralove Faculty of Science

2 Content Introduction Input data Methodology Results Conclusions

3 Introduction Is the world stochastic or deterministic

4 Input data EPEX (European Power Exchange) Phelix hourly spot prices
in EUR/MWh between to more then samples high volatility rate

5 Electricity spot prices

6 Descriptive statistics of the spot prices
Mean Median Std dev Skewness Kurtosis Min Max 25% qtl 75% qtl 42,5 39,3 25,8 -2,43 16,67 500,0 2436,6 34,3 53,1

7 Phase space reconstruction
A point in the phase space is given as:  is the time delay m is the embedding dimension How can we determine optimal  and m?

8 Optimal time delay Very small   near-linear reconstructions Very large   obscure the deterministic structure the mutual information between xn and xn+ Mutual information function:

9 Mutual information

10 Optimal embedding dimension
false nearest neighbors (FNN) This method measures the percentage of close neighboring points in a given dimension that remain so in the next highest dimension.

11 Nearest neighbors

12 The largest Lyapunov exponent
Z0 Zt The largest Lyapunov exponent:

13 Rosenstein algorithm dj(i) is distance from the j point to its nearest neighbor after i time steps M is the number of reconstructed points. Our results:  = 0,0005

14 Slope is the largest Ljapunovuv exponent 0,00022.

15 The 0-1 test for chaos developed by Gottwald & Melbourne
scalar time series of observations φ1, ... , φN construct the Fourier transformed series

16 Logistic equation r=3, r=3,97

17

18 The 0-1 test for chaos the output is 0 or 1 Our result: 1
compute the smoothed mean square displacement estimate correlation coefficient to evaluate the strength of the linear growth

19 Test 0-1

20 Test 0-1

21 Long memory in time series
Hurst exponent (H) Is between 0 and 1 Random walk 0,5 Higher values  trend without volatility self-similarity process

22 Long memory in time series
is usually characterized in time or frequency domain Rescaled Range Analysis (R/S Analysis) Detrended Fluctuation Analysis (DFA) Geweke et Porter‐Hudak Analysis (GPH) Awerage Wavelet Coefficients (AWC)

23 Rescaled Range analysis
Hurst exponent [R(n)/S(n)] is the rescaled range E[y] is expected value n is number of data points in a time series C is a constant

24 Results Method Hurst koeficient R/S analýza 0,853 DFA 0,909 GPH 0,917
AWC 0,976 mean 0,914 Std dev 0,044

25 Fractal dimensions ε – side of hypercube N(ε) – minimum number

26 Correlation dimension
Correlation integral where Θ is the Heaviside step function Correlation dimension Our results: DC=1,3

27 Recurrence analysis based on topological approach, was used to show recurring patterns and non-stationarity in time series Recurrence is a fundamental property of dynamical systems

28

29 the electricity price series is chaotic and
Conclusions time delay  = 15 embedding dimension m = 6 the largest Lyapunov exponent  = 0,00022 chaos is present according to 0-1 test Hurst exponent: H=0,914 the electricity price series is chaotic and contains long memory

30 THANK YOU FOR YOUR ATTENTION
Any questions or comments?


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