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IP1202PBF 数据表(PDF) 18 Page - International Rectifier |
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IP1202PBF 数据表(HTML) 18 Page - International Rectifier |
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18 / 29 page ![]() www.irf.com 18 iP1202PbF Control Loop Compensation The iP1202PbF feedback control is based on single loop voltage mode control principle if both outputs are configured in dual output independent mode. In this case, both outputs can have identical compen- sation. If iP1202PbF outputs are configured for par- allel operation, then compensation of the outputs will differ slightly. The goal in the design of the compensator is to achieve the highest unity gain (0 db) crossover fre- quency with sufficient phase margin for the closed loop transfer function. The LC filter of the power sup- ply introduces a double pole with 40db/dec slope and 1800 phase lag. The 180° phase contribution from the LC filter is the source of instabilty. The resonant frequency of the LC filter is expressed by equation (10): (10) The error amplifiers of the iP1202PbF PWM control- ler are transconductance amplifiers, and their out- puts are available for external compensation. Two type of compensators are studied in this sec- tion. The first one is called Type II and it is used to compensate systems the e.s.r. frequency f esr (equa- tion 8) of which is in the midfrequency range and Type III that can be used for any type of output capacitors and have a wide range of f esr. Fig. 18: Typical Type II compensation and its gain plot From Fig.18 the transfer function H(s) of the error amplifier is given by (11): (11) The term s represents the frequency dependence of the transfer function. The Type II controller introduces a gain and a zero expressed by equations (12) and (13): 5 9 7 7 ) ( R R R R g s H m × + × = (12) where, g m is the transconductance of the error am- plifier. (13) Follow the steps below to determine the feedback loop compensation component values: 1. Select a zero db crossover frequency f 0 in the range of 10% to 20% of the switching frequency f sw. 9 5 2 1 C R f z × × = π 5 9 9 5 9 7 7 1 ) ( R sC C sR R R R g s H m + × + × = ) (2 / 1 0 0 C L f LC × = π Magnitude(dB) Frequency FZ H(s) dB C10 R9 R7 E/A1 Vout1 FB1 VREF CC1 iP1202 C9 R5 (Optional) Type II The inductor L ois selected according to equation (9): L O = Vout x (1 - D) / (fsw x Iripple) (9) For output 1 of the above example, and for I ripple of 30% of I OUT1, LO1 is calculated to be 1.0µH. The core must be selected according to the peak of maximum output current. A similar calculation can be applied to find an induc- tor value for the second output. iP1202PbF |
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