AETA 2013: Recent Advances in Electrical Engineering and by Ivan Zelinka, Vo Hoang Duy, Jaesang Cha

By Ivan Zelinka, Vo Hoang Duy, Jaesang Cha

Over the prior many years, fault analysis (FDI) and fault tolerant keep watch over concepts (FTC) were proposed in response to diverse strategies for linear and nonlinear platforms. certainly a substantial recognition is deployed with the intention to deal with different damages leading to faults occurrence.

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Example text

Typical example of evolutionary identification is in Equation (10), (11) and visualization in Figure 3. According to obtained results, it can be stated that evolutionary identification is an alternative and promising way as to how to identify chaotic systems. Extended case study is also reported in [16]. x A+ (A + A(x + Ax)) −1 − A + x − Ax + x2 − −A+x A 2 2A (1 − x)x2 (3A + x − 3Ax + Ax2) (10) (11) 22 I. Zelinka Fig. 2. and its scheme Fig. 3. Original (black fat points) and identified (red thin points) behavior 4 Conclusion Based on various applications of methods of symbolic regression, it can be stated that symbolic regression seems to be powerful algorithmic method to design and solve complex problems like electronic circuits etc.

And its scheme Fig. 3. Original (black fat points) and identified (red thin points) behavior 4 Conclusion Based on various applications of methods of symbolic regression, it can be stated that symbolic regression seems to be powerful algorithmic method to design and solve complex problems like electronic circuits etc. All mentioned methods of symbolic regression and especially AP has been carefully tested during the last years on various examples including selected examples for comparative studies with very good results.

In order to solve the Poisson system for the potential, the following boundary conditions are applied, φ r =0 = 0 , 4 ∂φ ∂r =0 (9) r=R Simulation Settings The input parameters for the flowmeter are the coil radius rm (both coils being assumed to be equal in size), the coil separation Δ and the currents J1 and J2 flowing through each coil. Both same-sign currents (J1=J2) and opposite-sign currents J1=J2 are considered, see Fig. 1. The primary magnetic field is computed through BiotSavart's law, see Eq.

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