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EE462L, Power Electronics, DC-DC Boost Converter Version ... - ECS

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<strong>EE462L</strong>, <strong>Power</strong> <strong>Electronics</strong>, <strong>DC</strong>-<strong>DC</strong> <strong>Boost</strong> <strong>Converter</strong><br />

<strong>Version</strong> Oct. 3, 2011<br />

Current Ratings in Continuous Conduction<br />

Conservative current ratings for the inductor in continuous conduction correspond to the<br />

situation where<br />

Δ Imax = 2I in , (11)<br />

which, as explained in the Buck <strong>Converter</strong> experiment, yields<br />

1 2<br />

2<br />

⎛ ⎞<br />

=<br />

2 +<br />

2 1<br />

I Lrms, max Iin<br />

( 2Iin<br />

) = Iin<br />

⎜1<br />

+ ⎟ , (12)<br />

12<br />

⎝ 3 ⎠<br />

so that<br />

2<br />

I Lrms , max = I in . (13)<br />

3<br />

Conservative current ratings for the MOSFET and diode are when D is large, so that (13) applies<br />

for them also.<br />

To determine the rms current through C, consider the capacitor current in Figure 8, and the<br />

worst-case scenario in Figure 9.<br />

2 I<br />

−<br />

in I out<br />

0<br />

Iin − I out<br />

DT<br />

(1–D)T<br />

Figure 9. Maximum Ripple Current Case for Capacitor Current<br />

When the switch is closed, the capacitor current is − Iout<br />

. When the switch is open, the<br />

capacitor current is iL<br />

− Iout<br />

. If the “switch closed” interval lasted for the entire T, the squared<br />

2<br />

rms value would be I out . If the “switch open” interval lasted for the entire T, the rms value<br />

would be, for the maximum ripple case, 2 1<br />

( I in − Iout<br />

) + ( 2Iin<br />

) 2 . The time-weighted average<br />

12<br />

of the two gives the squared rms current<br />

−<br />

I out<br />

Page 6 of 11

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