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PhD Thesis - Cranfield University

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Chapter 7<br />

( 45)(<br />

12.<br />

5 ⋅10<br />

=<br />

2<br />

= 281.<br />

2 µ H<br />

−6<br />

)<br />

Similarly, the inductance required for the same ripple current limit at minimum Vuc dis is,<br />

( Vuc<br />

L =<br />

dis<br />

min)( ∆t<br />

∆I<br />

( 20)(<br />

33.<br />

5⋅10<br />

=<br />

2<br />

= 335 µ H<br />

−6<br />

mac<br />

)<br />

)<br />

189<br />

(7-46)<br />

The sizing methodology yields a minimum required inductance value of 335 µH. However,<br />

unlike the battery system, the duty cycle range of the ultracapacitor boost converter<br />

0 ≤ T 4 ≤<br />

( . 25 D 0.<br />

67 ) has a possible duty cycle condition of 0.5. In this event, the previously<br />

assumed inductance value is not the minimum required value.<br />

Rewriting (7-5) and (7-7) for the ultracapacitor parameters,<br />

∆i<br />

L f sw = Vout<br />

−V<br />

)<br />

uc<br />

uc<br />

( 1−<br />

DT<br />

4<br />

in<br />

(7-47)<br />

V = V 1−<br />

D )<br />

(7-48)<br />

in<br />

out ( T 4<br />

Solving for current ripple gives,<br />

−<br />

Vout<br />

DT<br />

4 ( 1 DT<br />

4 )<br />

∆ iuc<br />

=<br />

(7-49)<br />

Luc<br />

f sw<br />

From (7-49), the maximum current ripple will occur when the duty cycle assumes a value of<br />

0.5. The value of the inductance required to achieve the same ripple current limit of 2A is<br />

then calculated by setting D T4 = 0.5 in (7-49) and solving for L uc,

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