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AN3180 Datasheet(PDF) 32 Page - STMicroelectronics |
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AN3180 Datasheet(HTML) 32 Page - STMicroelectronics |
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32 / 39 page ![]() Electrical equivalent circuit models of coupled inductors and transformers AN3180 32/39 Doc ID 17273 Rev 1 inductance Lb is associated to the secondary leakage flux, the flux generated by the secondary winding and not completely linked to itself nor to the primary winding: it is called secondary leakage inductance and is designated by Ll2. This choice of a is perhaps the most logical one, and is also very useful because it provides a clear physical meaning to each element of the equivalent circuit, shown in Figure 25, but it is not the only one that makes sense. Figure 25. Model of coupled inductors with a = n (a=n model) Another possible choice, which leads to always positive values for La and Lb, is a = . This quantity, usually indicated with ne, is termed “equivalent turn ratio” and is conceptually and numerically different from the physical turn ratio n: Equation 27 which coincides with n if and only if Ll2 = n 2 L l1, that is in case of symmetrical magnetic coupling (k1 = k2 = k). This choice is particularly useful when the physical turn ratio n is unknown, so that it is possible to complete the model computing ne from L1 and L2, which are easily measurable. In this case, Equation 26, considering Equation 23, takes the form: Equation 28 It is worth noting that Lb, reflected back to the primary side, equals La, as pointed out by the third Equation 28. Note that this property is often erroneously attributed to the primary and secondary leakage inductances Ll1 and Ll2. It is worth stating once more that k represents an average coupling between the windings and that the coupling k1 of the primary winding to the secondary one is generally different from the coupling k2 of the secondary winding to the primary one, and so Ll2 ≠ n2 Ll1. It is Ll2 = n2 Ll1 only in the special case of a winding geometry symmetrical in such a way that the reluctance of the leakage flux path is the same for both windings, resulting in symmetrical coupling between windings (k1 = k2 = k). L 2 L1 ⁄ M 1 M 2 2 1 2 L L L L L L + + = = l l n ne ( ) () ⎪ ⎩ ⎪ ⎨ ⎧ = − = = − = μ a 2 2 b 1 1 a L L k 1 L L k L L k 1 L e n |
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