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LTC3900 データシート(PDF) 10 Page - Linear Technology |
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LTC3900 データシート(HTML) 10 Page - Linear Technology |
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10 / 12 page ![]() LTC3900 10 3900i APPLICATIO S I FOR ATIO Figure 9. VCC Regulator If the LTC3900 still operates in discontinuous mode with the calculated resistance value, increase the value of RCS1 to raise the threshold. The resistors RCS1 and RCS2 and the CS+ pins input capacitance plus the PCB trace capacitance forms an R-C delay; this slows down the response time of the comparator. The resistors and CS+ input leakage currents also create an input offset error. To minimize this delay and error, do not use resistance value higher than required and make the PCB trace from the resistors to the LTC3900 CS+/CS– pins as short as possible. Add a series resistor, RCS3 with value equal to parallel sum of RCS1 and RCS2 to the CS– pin and connect the other end of RCS3 directly to the source of Q4. SYNC Input Figure 7 shows the external circuit for the LTC3900 SYNC input. With a selected type of pulse transformers, the values of the CSG and RSYNC should be adjusted to obtain a optimum SYNC pulse amplitude and width. A bigger capacitor, CSG, generates a higher and wider SYNC pulse. The peak of this pulse should be much higher than the typical LTC3900 SYNC threshold of ±1.4V. Amplitudes greater than ±5V will help to speed up the SYNC compara- tor and reduce the SYNC to drivers propagation delay. The pulse width should be wider than 75ns. Overshoot during the pulse transformer reset interval must be minimized and kept below the minimum SYNC threshold of ±1V. The amount of overshoot can be reduced by having a smaller RSYNC. VCC Regulator The VCC supply for the LTC3900 can be generated by peak rectifying the transformer secondary winding as shown in Figure 9. The Zener diode DZ sets the output voltage to (VZ – 0.7V). A resistor, RB (on the order of a few hundred ohms), in series with the base of QREG may be required to surpress high frequency oscillations depending on QREG’s selection. The LTC3900 has an UVLO detector that pulls the drivers output low if VCC < 4.1V. The UVLO detector has 0.5V of hysteresis to prevent chattering. In a typical forward converter, the secondary-side circuits have no power until the primary-side controller starts operating. Since the power for biasing the LTC3900 is derived from the power transformer T1, the LTC3900 will initially remain off. During that period (VCC < 4.1V), the output rectifier MOSFETs Q3 and Q4 will remain off and the MOSFETs body diodes will conduct. The MOSFETs may experience very high power dissipation due to a high voltage drop in the body diodes. To prevent MOSFET damage, VCC voltage greater than 4.1V should be provided Figure 7. SYNC Input Circuit Figure 8. Symmetrical SYNC Drive RSYNC 470 Ω T2 T2: COILCRAFT Q4470B OR PULSE P0926 CSG 220pF PRIMARY CONTROLLER SG LTC3900 SYNC 3900 F06 RSYNC 470 Ω T2 LTC3900 SYNC 3900 F07 74HC14 74HC14 74HC132 R1 470 Ω C1 220pF SYNC SG PRIMARY CONTROLLER SG 3900 F08 D3 MBR0540 T1 SECONDARY WINDING 0.1 µF RZ 2k RB 10 Ω QREG BCX55 CVCC 4.7 µF VCC DZ 7.5V An alternative method of generating the SYNC pulse is shown in Figure 8. This circuit produces square SYNC pulses with amplitude dependent on the logic supply voltage. The SYNC pulse width can be adjusted with R1 and C1 without affecting the pulse amplitude. For nonisolated applications, the SYNC input can be driven directly by a bipolar square pulse. To reduce the propaga- tion delay, make the positive and negative magnitude of the square wave much greater than the ±1.4V SYNC threshold. |
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