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From the graph comparing three methods the resonator method is workable in spite of the fact that in Fig. 4 it does not show markable difference. The presented sensitivity was given by the quality factor of the used resonator, and can be improved by using a resonator with high sensitivity (approximately of 15000–20000) and this is not its only feature because also the detuning of the resonator can be very sensitive representation of the crack depth. Acknowledgement The author would like to thank MSc.

Comparison of the anisotropy measurements of stator laminations of the series A and B. tensively in the literature ([3]). Therefore, this work will concentrate in two other parasitic effects: torque ripple and radial forces on the stator teeth. These effects are going to be studied here analytically and through FE Simulation. Thanks to the fact that the studied machine has two pole pairs, it is possible to model the anisotropy only in the stator teeth. Moreover, it is assumed that there is a magnetic difference between teeth but not inside one of them, so that the magnetic anisotropy is modeled through a different magnetization curve for each tooth.

Dependence of reflected signal amplitude from the defect. calibration data [mm] 4 3,5 3 2,5 2 1,5 1 0 5 10 15 20 defect depth [mm] Figure 5. Calibration curve for magic T. For this purpose we have carried out an experiment with the resonator connected on standard microwave line. The resonator was connected on standard microwave line in the transmission way and one resonator aperture was terminated with an open waveguide probe. Resonator was tuned in resonance. In front of the probe was shifted a metal sample with the defect (width 0,5 mm, depth 8,5 mm).

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