By Harkins W. D.
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28. , and S. Hahn (1997). Optimal Design of Induction Heating Devices Using Physical and Geometrical Sensitivity. Proceedings of the Fourth JapanKorea Symposium on Electrical Engineering, Seoul, Korea: 55-58. 29. al. (1994). An inverse analysis for crack identification in eddy current NDT of tubes. IEEE Transactions on Magnetics, vol 30, no5: 3403-3406. 30. , et al. (1997). The application of artificial neural network to defect characterization in eddy current NDT. NDT and E International, vol 30,no5:328.
16. K. Daugavet (1993). Approximation of Nonlinear Operators by Volterra Polynomials. Amer Math Soc Transl (2), vol 155: 47-57. 17. Volterra, V. (1959). Theory of Functional and of Integral and Integro-diffential Equations. NY: Dover Publ. 18. Wiener, N. (1966). Nonlinear problems in random theory. Cambridge: Ma MIT. 19. Eykhoff, P. ed. (1981). Trends and progress in system identification. England: Pergamon, Oxford. 20. Eykhoff, P. (1974). System Identification. London:John Wiley and Sons. 21. V.
03 A are calculated from Eq. 14) and they are essentially closer to the true val- Inverse Problems in Electrical Circuits and Electromagnetic Field Theory 33 ues than originally measured currents. Using thus found /i, /i values, resistances R\ and R2 can be calculated: ^ ^ 1 \ - \ h -\(h : — ^ + ^2) 5 D _ ^0 - W i -\ih ^ - z, + ^2) : 5 ^2 where r. ,r. ,r. are the resistances of ammeters. Use of a priori information allows us to remove ambiguous interpretations of experimental results and to obtain more accurate solutions.
An Electromagnetic Hypothesis of the Kinetics of Heterogeneous Equilibrium, and of the Structure of by Harkins W. D.