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**Unilab Coils 6 5 40**

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0. The area under the demagnetizing curve is C and the area under the effective field curve is A. The ratio of these areas, A/C, is a function of the number of turns in the winding, N, and the area of the magnetic core, E. The result is R=E/C. A/C increases when N increases, but for a given E, A/C decreases as N increases. The number of turns can be adjusted so as to achieve a desired value of R. The self-resonance frequency of the induction machine coil can be adjusted by adjusting the number of turns of the induction machine coil 5. By the same token, a low frequency self-resonance frequency can be tuned by adjusting the number of turns of the induction machine coil 5. FIG. 7 shows the result of changing the number of turns in the induction machine coil 5 from a value that produces a low frequency self-resonance frequency to a value that produces a high frequency self-resonance frequency. The induction machine coil 5 is wound at the number of turns indicated by a dot-dashed line at about 1.25. The result is an induction machine coil 5 that produces a self-resonance frequency of about 50 Hz. The peak value of the self-resonance curve (at 50 Hz) is about 49.5. However, there is a significant residual current flowing in the induction machine coil 5. The next step is to reduce the number of turns of the induction machine coil 5 to a value that produces a self-resonance frequency of approximately 1 kHz. The result is an induction machine coil 5 that produces a self-resonance frequency of about 100 Hz. The peak value of the self-resonance curve is about 102.6. Again, there is a significant residual current flowing in the induction machine coil 5. If the number of turns is decreased to a value that produces a self-resonance frequency of about 10 kHz, then the peak value of the self-resonance curve is about 103.5. The result is an induction machine coil 5 that produces a self-resonance frequency of about 10 kHz. The peak value of the self-resonance curve is about 103.5. Again, there is a significant residual current flowing in the induction machine coil 5. A significant disadvantage of this approach is that the value of R, which is a function of E, C,

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