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AN441 数据表(PDF) 13 Page - STMicroelectronics |
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AN441 数据表(HTML) 13 Page - STMicroelectronics |
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13 / 16 page ![]() AN441 BMAX calculation for remanent induction Doc ID 3579 Rev 3 13/16 Appendix A BMAX calculation for remanent induction The winding is supplied by an alternating mains voltage “u(t)” given by Equation 5. Equation 5 According to the laws of Lenz and Faraday, we have Equation 6, Equation 7 and Equation 8. Equation 6 With: ● Φ = Flux ● B = Induction ● N = spires number (spires number of the primary for a transformer) ● S = section area for magnetic material Then, induction versus time is: Equation 7 Equation 8 We consider the case where the Triac is first triggered at mains zero voltage. We can distinguish two cases: Case 1 Winding is switched on whereas a remanent positive induction remains on magnetic core. According to Equation 8, for t = 0, we have: Equation 9 So Equation 10 So the maximum induction will be: BMAX = 2·Bn +Br ·t) ·sin( ù 2 U u(t) = dt dB N·S dt d Ö N u(t) = = )dt ·t sin( N.S 2 U B(t) ∫ ω = N·S· ù 2 U B with 0 B ) 2 ð t ·sin( ù n B B(t) n = + − = r n 0 r 0 n B B B B B B B(0) + = → = + − = r B n B ) 2 ð t ·sin( ù n B B(t) + + − = ⇒ |
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