XIX Sympozjum Srodowiskowe PTZE - materialy.pdf
XIX Sympozjum Srodowiskowe PTZE - materialy.pdf XIX Sympozjum Srodowiskowe PTZE - materialy.pdf
XIX Sympozjum PTZE, Worliny 2009 characteristics depend on the winding design, as well. In case of the design presented in Fig. 2b, more copper material can be placed in the active part of AFPMSM. The active part presents the part of the machine, where the influence of magnetic flux density on the AFPMSM characteristic is not negligible. On the other hand, it is not always necessary to place as much copper as possible in the coreless stator, especially when constructing AFPMSMs with larger diameters, where plenty of space is available. For this reason the winding design presented in Fig. 2a is often chosen. ro-ri ro-ri Fig. 2. Winding designs of AFPMSM. Influence of winding design on static characteristics of AFPMSM Right-hand side of Fig. 3 presents the electrical current, current density, copper wire crosssection and the number of turns in dependency on the coil and stator width. On the left-hand side of Fig. 3 the comparison of analytically calculated back EMF for both winding designs (Fig. 2) is presented. Fig. 4 presents the comparison of static torque and normal force according to displacement at 5A/mm 2 and 4,94A/mm. Back EMF (V) Fig. 3. Left: Back EMF according to displacement. Right: electrical and dimensional parameters in dependency on coil and stator width. I (A), J (A/mm 2 ), S (mm 2 ), N (turns) 170
M (Nm) XIX Sympozjum PTZE, Worliny 2009 Fig. 4. Left: Static torque according to displacement. Right: Normal force according to displacement. The comparisons between static characteristics on Fig. 3 and Fig. 4 show that the topology in Fig. 2a gives better resultant characteristics at the same copper wire cross-section and the same number of turns. This ascertainment is relevant only with declared geometrical winding parameters in this digest. Moreover, the tendencies of AFPMSM characteristics according to the parameters of winding design will be presented in full paper. 171 F (N)
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<strong>XIX</strong> <strong>Sympozjum</strong> <strong>PTZE</strong>, Worliny 2009<br />
characteristics depend on the winding design, as well. In case of the design presented in Fig.<br />
2b, more copper material can be placed in the active part of AFPMSM. The active part<br />
presents the part of the machine, where the influence of magnetic flux density on the<br />
AFPMSM characteristic is not negligible. On the other hand, it is not always necessary to<br />
place as much copper as possible in the coreless stator, especially when constructing<br />
AFPMSMs with larger diameters, where plenty of space is available. For this reason the<br />
winding design presented in Fig. 2a is often chosen.<br />
ro-ri<br />
ro-ri<br />
Fig. 2. Winding designs of AFPMSM.<br />
Influence of winding design on static characteristics of AFPMSM<br />
Right-hand side of Fig. 3 presents the electrical current, current density, copper wire crosssection<br />
and the number of turns in dependency on the coil and stator width. On the left-hand<br />
side of Fig. 3 the comparison of analytically calculated back EMF for both winding designs<br />
(Fig. 2) is presented. Fig. 4 presents the comparison of static torque and normal force<br />
according to displacement at 5A/mm 2 and 4,94A/mm.<br />
Back EMF (V)<br />
Fig. 3. Left: Back EMF according to displacement.<br />
Right: electrical and dimensional parameters in dependency on coil and stator width.<br />
I (A), J (A/mm 2 ), S (mm 2 ), N (turns)<br />
170