Datenblatt-Suchmaschine für elektronische Bauteile |
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1N4005 Datenblatt(PDF) 10 Page - STMicroelectronics |
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1N4005 Datenblatt(HTML) 10 Page - STMicroelectronics |
10 / 42 page AN1262 APPLICATION NOTE 10/42 (that is a larger input capacitor) is of help. Some iterations, involving a recheck of the points mentioned in "Pre- liminary Calculations - step 2", may be necessary. If no solution can be found, either some specification should be relaxed or the power handled by the converter should be derated. 9 FLYBACK TRANSFORMER DESIGN To complete the set of data needed to design the flyback transformer, the primary inductance value (Lp) and the primary-to-secondary turns ratio (n) are still to be defined. The primary inductance will be chosen so that the converter is operated on the boundary between DCM and CCM at Vin = Vinmin: (4) while the primary-to-secondary turns ratio is defined so as to get the desired reflected voltage VR: (5) With the complete set of specification, the transformer design can start with the selection of the magnetic core material and geometry. Table 9. Ferrite Materials selection As to the magnetic material, a standard soft ferrite for power applications (gapped core-set with bobbin) is the usual choice: the switching frequency is not so high thus special grades for high frequency operation are not required. Table 9 shows some suitable materials. The geometry will be usually a popular E or E-derived type. Other configurations, such as RM or PQ cores, are not recommended because they are inherently high leakage geometries, since they result in narrower and thicker wind- ings. Consider that minimizing leakage inductance is one of the major tasks in the design of a flyback transformer. Among the various shapes and styles offered by manufacturers the most suitable one will be selected with technical and economic considerations. Table 10 shows some possible choices with the relevant data useful for the design. The next quantity to be defined is the peak flux density Bmax which the transformer will be operated at. Being this a DCM design, Bmax will also equal the maximum flux density swing ∆Bmax. Grade Saturation flux density [T] Specific Power Losses @100 °C [W/cm3] Manufacturer B2 0.36 THOMSON 3C85 0.33 PHILIPS N67 0.38 EPCOS (ex S+M) PC30 0.39 TDK F44 0.4 MMG Lp V inm i n V DS on )x () – () D X ⋅ [] 2 2f sw P inT ⋅⋅ ------------------------------------------------------------------------- = n V R V out V F + ------------------------- = PFe 1.15 10 5 – B 2.26 ∆ f sw 1.11 ⋅⋅ ⋅ = PFe 1.54 10 7 – B 2.62 ∆ f sw 1.54 ⋅⋅ ⋅ = PFe 8.53 10 7 – B 2.54 ∆ f sw 1.36 ⋅⋅ ⋅ = PFe 1.59 10 6 – B 2.58 ∆ f sw 1.32 ⋅⋅ ⋅ = PFe 2.39 10 6 – B 2.23 ∆ f sw 1.26 ⋅⋅ ⋅ = |
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Ähnliche Beschreibung - 1N4005 |
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