Shark -new motor design concept for energy saving- applied to - VBN
Shark -new motor design concept for energy saving- applied to - VBN
Shark -new motor design concept for energy saving- applied to - VBN
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24<br />
Chapter 2 Linear analysis of the <strong>Shark</strong> switched Reluctance Mo<strong>to</strong>r<br />
In order <strong>to</strong> highlight the dependence of the inductance gain on the number of <strong>Shark</strong> segments and<br />
on their height, expression (2.8) may be rewritten based on the saw-<strong>to</strong>othed geometry illustrated in<br />
Fig. 2.4 as follows:<br />
k saw<br />
Lsaw<br />
L0<br />
2<br />
lshk<br />
2<br />
lshk<br />
2<br />
2<br />
hshk<br />
1<br />
2 hshk<br />
lshk<br />
2<br />
(2.9)<br />
Now the influence of the length and height of the <strong>Shark</strong> profile can be studied separately. If, <strong>for</strong><br />
instance, the height of the <strong>Shark</strong> segment is held constant the inductance gain increases with<br />
reduction of the <strong>Shark</strong> segment pitch. The variation is shown in Fig.2.9. On the other hand, if the<br />
length of the <strong>Shark</strong> segment is held constant, then the inductance gain increases as the height of the<br />
<strong>Shark</strong> segment increases as shown in Fig.2.9.<br />
inductance gain = L saw /L 0<br />
8<br />
7<br />
6<br />
5<br />
4<br />
3<br />
2<br />
h shk /g=1<br />
h shk /g=5<br />
h shk /g=10<br />
h shk /g=15<br />
1<br />
0 10 20<br />
l /g<br />
shk<br />
30 40<br />
Fig.2.9 Inductance gain <strong>for</strong> the saw-<strong>to</strong>othed air gap showing<br />
the influence of the height and length of the <strong>Shark</strong> <strong>to</strong>oth<br />
The change in the <strong>energy</strong> of the saw <strong>to</strong>othed air gap may be determined as:<br />
<strong>energy</strong> gain = W saw / W 0<br />
9<br />
8<br />
7<br />
6<br />
5<br />
4<br />
3<br />
2<br />
h shk /g=1<br />
h shk /g=5<br />
h shk /g=10<br />
h shk /g=15<br />
1<br />
0 10 20<br />
l /g<br />
shk<br />
30 40<br />
Fig.2.10 Energy gain <strong>for</strong> the saw-<strong>to</strong>othed air gap showing<br />
the influence of the height and length of the <strong>Shark</strong> <strong>to</strong>oth<br />
a u<br />
W saw Wsaw<br />
Wsaw<br />
(2.10)<br />
a u<br />
where: W saw and W saw are the energies of the saw <strong>to</strong>othed SRM in the aligned and unaligned<br />
position respectively.<br />
As mentioned in the previous section, the inductance in the unaligned ro<strong>to</strong>r position, was assumed<br />
<strong>to</strong> be equal <strong>for</strong> the <strong>Shark</strong> SRM and CSRM. There<strong>for</strong>e, the <strong>energy</strong> in the unaligned position is also