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HVLED007 数据表(PDF) 16 Page - STMicroelectronics |
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HVLED007 数据表(HTML) 16 Page - STMicroelectronics |
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16 / 33 page ![]() Application information HVLED007 16/33 DS12866 Rev 1 As to the dynamic properties of a HVLED007-based Hi-PF QR flyback converter, the ICS circuit is essentially transparent: it only affects the DC gain of the feedback loop. This is intuitive if one recalls that one of the basic assumptions was that the time constant associated to the ICS circuit were << 1/(2 fline) and that in Hi-PF converters the crossover frequency of the loop is typically much lower than fline. Assuming 100% efficiency and that the Hi-PF QR flyback converter powers one or more downstream switching regulators that drive the LED strings, the control-to-output transfer function is: Equation 8 4.4 Shaping capacitor (Ct) selection (pin CT) As previously mentioned, one fundamental assumption for proper operation of the novel control method implemented in the HVLED007 is that the time constant Rt Ct associated to the ICS meets the constraints: Equation 9 The left-hand side inequality ensures that the voltage across the shaping capacitor Ct is essentially a DC level in any given switching cycle; the right-hand inequality ensures that this DC level is able to change quickly enough to closely follow the ideal reference given by (Equation 6) and depicted in Figure 7. 7 Secondary rms current 8 Secondary DC current 9 Secondary AC current 10 Low-frequency secondary current 11 Low-frequency output voltage ripple Eq. # Parameter Expression Isrms = Iout 2 64 9 K v -------------- + Isdc = Iout Isac = Iout 1 64 9 K v ------------- + Io = 2 I out sin 2 = I out (1 - cos 2 V o pk – = Iout 1 22 f line C out --------------------------------------- = I out 4 f line Cout ------------------------------- G s = Iout V c -------- 1 sCout -------------= 1 2 ---- N pri N sec ------------- Kv 2 KM KP V out Rs ------------ 1 sCout ------------- T << R t Ct << 1/ 2 f line |
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