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L6717ATR 데이터시트(PDF) 51 Page - STMicroelectronics |
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L6717ATR 데이터시트(HTML) 51 Page - STMicroelectronics |
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51 / 57 page ![]() DocID024465 Rev 1 51/57 L6717A System control loop compensation Figure 18. Control loop bode diagram and fine tuning (not in scale) To obtain the desired shape an R F -C F series network is considered for the Z F (s) implementation. A zero at ω F =1/R F C F is then introduced together with an integrator. This integrator minimizes the static error while placing the zero ω F in correspondence with the L- C resonance assures a simple -20dB/Dec. shape of the gain. In fact, considering the usual value for the output filter, the LC resonance results to be at frequency lower than the above reported zero. Compensation network can be simply designed placing ω F = ω LC and imposing the cross- over frequency ω T as desired obtaining (always considering that ω T might be not higher than 1/10th of the switching frequency F SW ): 11.1 Compensation network guidelines The compensation network design assures to having system response according to the cross-over frequency selected and to the output filter considered: it is anyway possible to further fine-tune the compensation network modifying the bandwidth in order to get the best response of the system as follow (See Figure 18): – Increase R F to increase the system bandwidth accordingly; – Decrease R F to decrease the system bandwidth accordingly; – Increase C F to move ω F to low frequencies increasing as a consequence the system phase margin. Having the fastest compensation network gives not the confidence to satisfy the requirements of the load: the inductor still limits the maximum dI/dt that the system can afford. In fact, when a load transient is applied, the best that the controller can do is to “saturate” the duty cycle to its maximum (d MAX ) or minimum (0) value. The output voltage dV/dt is then limited by the inductor charge / discharge time and by the output capacitance. In particular, the most limiting transition corresponds to the load removal since the inductor results being discharged only by V OUT (while it is charged by d MAX V IN -V OUT during a load appliance). dB ω Z F (s) G LOOP (s) K ω LC = ω F ω ESR ω T R F [dB] dB ω Z F (s) G LOOP (s) K ω LC = ω F ω ESR ω T R F [dB] R F C F R F R FB ΔV OS C ⋅ V IN ---------------------------------- 3 5 --- ω T L NR LL ES R + () ⋅ ------------------------------------------- ⋅⋅ ⋅ = C F C O L ⋅ R F -------------------- = |
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