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The Discontinuous Conduction Mode Sepic and ´ Cuk Power

The Discontinuous Conduction Mode Sepic and ´ Cuk Power

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632 IEEE TRANSACTIONS ON INDUSTRIAL ELECTRONICS, VOL. 44, NO. 5, OCTOBER 1997<br />

Fig. 4. Diode current.<br />

C. Third Stage of Operation<br />

This is a freewheeling stage, shown in Fig. 3(c). This stage<br />

lasts until the start of a new switching period. <strong>The</strong> switch <strong>and</strong><br />

output diode OFF time is given by<br />

D. Average Output Current<br />

For both converters, the average output current is the<br />

average diode current, shown in Fig. 4. Its peak value is given<br />

by<br />

where<br />

Its average value in a switching period is given by<br />

<strong>and</strong> the average for half of a line period becomes<br />

E. Input Current<br />

Considering 100% of efficiency, ,<br />

Using (9) in (11), <strong>and</strong> noting that ,<br />

where<br />

(6)<br />

(7)<br />

(8)<br />

(9)<br />

(10)<br />

(11)<br />

(12)<br />

(13)<br />

Fig. 5. Input current ripple.<br />

From (12), it can be seen that <strong>Sepic</strong> <strong>and</strong> Ćuk converters<br />

as DCM–PFP are perfect PFP in theory ( is perfectly<br />

sinusoidal).<br />

F. <strong>Discontinuous</strong> <strong>Conduction</strong> <strong>Mode</strong> Operation<br />

<strong>and</strong> the Critical <strong>Conduction</strong> Parameter<br />

To operate at DCM, the following inequalities must hold<br />

[see Fig. 3(d)]:<br />

(14)<br />

(15)<br />

<strong>The</strong> worst situation occurs for . <strong>The</strong>refore, to<br />

operate at DCM,<br />

On the other h<strong>and</strong>, the average output current is given by<br />

Using (10) <strong>and</strong> (17) results in<br />

(16)<br />

(17)<br />

(18)<br />

where is the conduction parameter of the <strong>Sepic</strong> or Ćuk<br />

PFP:<br />

(19)<br />

From (16) <strong>and</strong> (18), the critical value of to<br />

operate at DCM [8] can be found as<br />

(20)<br />

G. <strong>and</strong> Design<br />

<strong>The</strong> equivalent inductance<br />

is given by<br />

is obtained using (19) <strong>and</strong><br />

(21)<br />

<strong>The</strong> design of <strong>and</strong> is made using the desired ripple<br />

value of the input current. Considering the input current shown<br />

in Fig. 5, its peak-to-peak value is given as<br />

Its maximum value occurs for <strong>and</strong> is given by<br />

Authorized licensed use limited to: ELETTRONICA E INFORMATICA PADOVA. Downloaded on April 12, 2009 at 16:08 from IEEE Xplore. Restrictions apply.<br />

(22)<br />

(23)

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