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
You also want an ePaper? Increase the reach of your titles
YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.
28<br />
Chapter 2 Linear analysis of the <strong>Shark</strong> switched Reluctance Mo<strong>to</strong>r<br />
where: A ellipse is the area of the elliptical air gap and<br />
'<br />
l stk is the equivalent length of the <strong>Shark</strong><br />
'<br />
SRM air gap. l stk may be determined from the semi perimeter of the ellipse multiplied by the<br />
number of <strong>Shark</strong> segments n t :<br />
( ) ( ) t n<br />
' π<br />
lstk = ⋅ a + b ⋅ − 43<br />
he<br />
⋅−<br />
2<br />
where<br />
(2.21)<br />
2<br />
2<br />
a − b 1 − tan β<br />
h e = =<br />
(2.22)<br />
a + b 1 + tan β<br />
From (2.20), (2.21) and (2.22) the inductance in the aligned position becomes:<br />
L<br />
L<br />
L<br />
ellipse<br />
ellipse<br />
ellipse<br />
µ 0 ⋅ N<br />
=<br />
µ 0 ⋅ N<br />
=<br />
2<br />
ph<br />
2<br />
ph<br />
2<br />
ph<br />
µ 0 ⋅ N<br />
=<br />
g<br />
⋅<br />
⋅<br />
⋅ l<br />
n<br />
n<br />
t<br />
t<br />
stk<br />
π<br />
⋅ ⋅<br />
2<br />
π l<br />
⋅ ⋅<br />
2 2<br />
⋅<br />
π<br />
⋅<br />
4<br />
( a + b)<br />
⋅ ( 3 − 4 − h )<br />
shk<br />
g<br />
⋅<br />
( 1 + tan β ) ⋅ ( 3 − 4 − h )<br />
g<br />
( 1 + tan β )<br />
⋅<br />
3 −<br />
e<br />
⋅ l<br />
4 −<br />
pol<br />
e<br />
⋅ l<br />
pol<br />
1 − tan β<br />
1 + tan β<br />
From (2.23) and (2.3) the inductance gain, k ellipse , of the elliptical <strong>Shark</strong> profile is given by:<br />
2<br />
(2.23)<br />
Lellipse<br />
π<br />
1−<br />
tan β<br />
kellipse<br />
= = ⋅ ( 1+<br />
tan β ) ⋅ 3 − 4 −<br />
(2.24)<br />
L 4 1+<br />
tan β<br />
0<br />
The inductance gain of the elliptical profile depends on the angle β only. The elliptical profile<br />
produces a higher aligned inductance compared with the saw-<strong>to</strong>othed profile <strong>for</strong> the whole range of<br />
angle β .<br />
To express the inductance gain as a function of the length and the height of the <strong>Shark</strong> segment,<br />
tan β is replaced by an expression in terms of h shk and l shk . Using this expression the variation of<br />
inductance gain with the length, l shk , is presented in Fig.2.13, <strong>for</strong> different heights, h shk , of the<br />
<strong>Shark</strong> profile. The variation is quite similar in shape <strong>to</strong> that in the case of the saw-<strong>to</strong>othed profile.<br />
The change of the co-<strong>energy</strong> of the elliptical <strong>to</strong>othed air gap may be determined as:<br />
2