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AN2450 Datasheet(PDF) 22 Page - STMicroelectronics |
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AN2450 Datasheet(HTML) 22 Page - STMicroelectronics |
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22 / 35 page ![]() Magnetic integration AN2450 22/35 DocID12784 Rev 6 Figure 10. Transformer's APR (all primary referred) model The problem is mathematically undetermined: there are 5 unknowns (LL1, Lµ, nt, and LL2a, LL2b) in the physical model and only three parameters in the APR model. The simplifying assumption that overcomes this issue is that of magnetic circuit symmetry: flux linkage is assumed to be exactly the same for both primary and secondary windings. This provides the two missing conditions: Equation 52 With this assumption it is now possible to find the relationship between n and nt: Equation 53 Figure 11. Transformer construction: E-cores and slotted bobbin It is not difficult to find real-world structures where the condition of magnetic symmetry is quite close to reality. Consider for example the ferrite E-core plus slotted bobbin assembly, using side-by-side winding arrangement, shown in Figure 11. L r L m Ideal Transformer n : 1 : 1 L r L m Ideal Transformer n : 1 : 1 LL2a LL2b LL1 nt 2 --------- = = nt n Lm Lr + Lm ------------------ n1 + = = Air gap symmetrically placed between the windings Separator Slotted bobbin Ferrite E half-cores Winding Winding Top view |
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