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The interaction phenomenon can be analysed with the help of complex torque coefficients k;(jλ) and k;(jλ) for the electrical and the mechanical systems respectively, as explained in Part I of the paper. k;(λj) is dependent on the network configuration and represents also electrical damping during rotor oscillations. It will now be shown how k;(jλ) can be precisely calculated for any network configuration. For this purpose a frequency scan of the network up to twice the nominal frequency (2fn) must be available.
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I. M. Canay (1982) studied this question.
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