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Shark -new motor design concept for energy saving- applied to - VBN

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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

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