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AN628 数据表(PDF) 19 Page - STMicroelectronics |
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AN628 数据表(HTML) 19 Page - STMicroelectronics |
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19 / 35 page ![]() 19/35 AN628 APPLICATION NOTE The power transferred by the inductor in each cycle where: ton = δ / fsw and δ = (VO - VIt) / VO For a given L, the twice ripple current ∆IL is the quantity associated to the transferred energy and can be calcu- lated as a certain percentage of the ILpk inductor current. If the maximum Vlpk value is higher than the VO/2, the maximum ∆IL occours when VIt = and its value is If the Vlpk maximum value does not reach VO/2 voltage value, the maximum ∆IL is reduced and its value is : . In continuous mode operation, an acceptable curent ripple level (Kr) can be considered between 10% to 35%. Smaller current ripple on the inductor involves smaller noise on the rectified main bus reducing the input filter size; but the ripple reduction will impose an increase of the boost inductor. The high voltage, the flux density and the frequency range make the standard high frequency ferrite the most useful material in P.F.C. applications. To avoid the core saturation, related to the high permeability materials, it is necessary built an air-gap in order to allow an adequate magnetic force range (H+Hgap). An easy approach, is to have an approximated minimum value of core size that could be used to perform the conversion: Volume ≥ where : K = specific energy constant. L = Boost inductor value in H. The specific energy constant (K), mainly depends on the ratio between the gap length (lgap) and the effective length (leff) of the magnetic core set and on the maximum ∆B swing. Practically can be used to get the minimum volume of the core set in cm3. After the minimum core-set size is estimated, the suitable type will be selected with technical and economic evaluations. Next step will be the design of the coil parameters. The above mentioned formula P t LI Lt I L ∆ ⋅⋅ t on -------------------------- = I L ∆ V lt V O V lt – () ⋅ V O f sw L ⋅⋅ ------------------------------------- = V O 2 -------- I Lmax () ∆ V O 4f sw L ⋅⋅ ----------------------- = I Lmax () ∆ V lpk VO V lpk – () V O f sw L ⋅⋅ ----------------------------------------- = K r I L ∆ 2I Lpk ⋅ ------------------ = KLI Lpk I Lpk I L ∆ 2 -------- + ⋅⋅ ⋅ K14 I eff I gap ---------- ⋅ ≈ P Ot LI Lt I L ∆ ⋅⋅ t on -------------------------- = |
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