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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

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