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AN1889 датащи(PDF) 19 Page - STMicroelectronics |
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AN1889 датащи(HTML) 19 Page - STMicroelectronics |
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19 / 33 page ![]() AN1889 Current transformer core selection 19/33 6 Current transformer core selection The main challenge now is to choose the core material, its shape and dimension. A correct design of this current transformer has to take into consideration some constraints that, being in contrast each other, lead to a few iterative design steps. The needs to have magnetic permeability as high as possible to minimize the effect of magnetization inductance, is in contrast with the need of a negligible inductance with respect to that of primary transformer. In fact, being the primary winding of the fly-back transformer in series with the primary winding of the current transformer, the relevant inductance would be seen as an increase of the leakage inductance in the converter. Moreover a higher magnetic permeability implies a bigger core size (to avoid the core saturation) while the dimension of the current transformer has to be as small as possible for both space and cost reasons. Among all possible choices a ferrite ring with 12.5 mm diameter has been selected. Starting from the preliminarily fixed turn ratio (N=0.2), we must determine the minimum primary turns needed to avoid the core saturation. With reference to figure 7b, by applying the Faraday's law and imposing the maximum flux Bmax equals to Bsat/2, we have: Equation 26 Where Bsat is the saturation flux of the core. Both primary turn number and primary inductance for some common toroidal core have been calculated and summarized in the table below. For the consideration previously made, the relatively high primary inductance of T38 does not make its selection as a suitable choice, furthermore between N67 and N30, this last one, giving the best trade off, has been selected. To deeply explain this choice, we must observe that the magnetization inductance cannot be neglected and it also strongly contribute in determining the real transformer transfer rate. This can be explained looking at the figure below where the proportional driving schematic and its equivalent circuit is reported. Table 3. Primary Turn number and primary inductance for some common toroidal core Material Al value [nH] Bsat @ 25 OC [mT] Bsat @ 100 OC [mT] NP LTP [µH] N67 1070 480 370 1.85 ◊2 4.28 N30 2200 350 225 2.53 ◊3 19.8 T38 5100 350 220 2.53 ◊3 49.5 V 1 N TP d ϕ dt ------ • N TP A e ∆B ∆t -------- N TP ⇒ • • 2 V 1 T onmax • A e B sat • -------------------------------- • = ≅ = |
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