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ÇUKUROVA UNIVERSITY INSTITUTE OF NATURAL AND APPLIED ...

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4. MODELING <strong>OF</strong> PROPOSED DVR Mustafa İNCİ<br />

The voltage across L1 is Vo, resulting in a linearly decreasing current in L1.<br />

The change in current while both switches are open is<br />

∆I<br />

∆t<br />

L1<br />

∆I<br />

L1<br />

V<br />

= = −<br />

T / 2 − DT L<br />

O<br />

1<br />

(4.17)<br />

State 3, Second on-period, T3: A second on-period similar to the first is initiated<br />

when switches, S3 and S4, are turned on. Reflected inductor current flows from input<br />

capacitor, C1, through switch, S3, transformer, T1, (in opposite direction compared<br />

to first on-period) diode, D3, and inductor, L1, to the output. Current returns to input<br />

through diode, D4, and switch, S4. The period ends when switches, S3 and S4, are<br />

turned off again. Period time is equal to the first on-period, (Nymand et al.,<br />

2010).<br />

State 4, Second off-period, T4: Finally, a second off-period starts when switches,<br />

S3 and S4, are turned off. All primary switches are off. Inductor current, iL1, is freewheeling<br />

through the two parallel branches, D1-D4 and D3-D2, to output. Inductor<br />

current is discharging. Transformer magnetizing current circulates in the transformer<br />

secondary winding (in opposite direction to first off-period) and the diodes, D1-D3<br />

and/or D2-D4. The period ends when switches, S1 and S2, are turned on. Period time<br />

is equal to the first off-period time, T<br />

4<br />

= T 2<br />

. Duration of the off-period is (Nymand et<br />

al., 2010):<br />

Since the net change in inductor current over one period must be zero for<br />

steady-state operation,<br />

( ∆ ) + ( ∆I<br />

) 0<br />

I (4.18)<br />

L, closed L,<br />

open<br />

=<br />

1<br />

L<br />

1<br />

⎛ N<br />

S<br />

⎞ VO<br />

⎜ Vin<br />

−VO<br />

⎟DT<br />

+ ( T / 2 − DT ) = 0<br />

(4.19)<br />

⎝ N<br />

P ⎠ L1<br />

58

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