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LTC3703 датащи(PDF) 18 Page - Linear Technology |
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LTC3703 датащи(HTML) 18 Page - Linear Technology |
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18 / 32 page ![]() LTC3703 18 3703f Bottom MOSFET Source Supply (BGRTN) The bottom gate driver, BG, switches from DRVCCtoBGRTN where BGRTN can be a voltage between ground and –5V. Why not just keep it simple and always connect BGRTN to ground? In high voltage switching converters, the switch node dV/dt can be many volts/ns, which will pull up on the gate of the bottom MOSFET through its Miller capacitance. If this Miller current, times the internal gate resistance of the MOSFET plus the driver resistance, exceeds the thresh- old of the FET, shoot-through will occur. By using a nega- tive supply on BGRTN, the BG can be pulled below ground when turning the bottom MOSFET off. This provides a few extra volts of margin before the gate reaches the turn-on threshold of the MOSFET. Be aware that the maximum voltage difference between DRVCC and BGRTN is 15V. If, for example, VBGRTN = –2V, the maximum voltage on DRVCC pin is now 13V instead of 15V. Current Limit Programming Programming current limit on the LTC3703 is straight forward. The IMAX pin sets the current limit by setting the maximum allowable voltage drop across the bottom MOSFET. The voltage across the MOSFET is set by its on- resistance and the current flowing in the inductor, which is the same as the output current. The LTC3703 current limit circuit inverts the negative voltage across the MOSFET before comparing it to the voltage at IMAX, allowing the current limit to be set with a positive voltage. To set the current limit, calculate the expected voltage drop across the bottom MOSFET at the maximum desired current and maximum junction temperature: VPROG = (ILIMIT)(RDS(ON))(1 + δ) where δ is explained in the MOSFET Selection section. VPROG is then programmed at the IMAX pin using the internal 12 µA pull-up and an external resistor: RIMAX = VPROG/12µA The current limit value should be checked to ensure that ILIMIT(MIN) > IOUT(MAX). The minimum value of current limit generally occurs with the largest VIN at the highest ambi- ent temperature, conditions that cause the largest power loss in the converter. Note that it is important to check for self-consistency between the assumed MOSFET junction temperature and the resulting value of ILIMIT which heats the MOSFET switches. Caution should be used when setting the current limit based upon the RDS(ON) of the MOSFETs. The maximum current limit is determined by the minimum MOSFET on- resistance. Data sheets typically specify nominal and maximum values for RDS(ON), but not a minimum. A reasonable assumption is that the minimum RDS(ON) lies the same amount below the typical value as the maximum lies above it. Consult the MOSFET manufacturer for further guidelines. For best results, use a VPROG voltage between 100mV and 500mV. Values outside of this range may give less accu- rate current limit. The current limit can also be disabled by floating the IMAX pin. FEEDBACK LOOP/COMPENSATION Feedback Loop Types In a typical LTC3703 circuit, the feedback loop consists of the modulator, the external inductor, the output capacitor and the feedback amplifier with its compensation network. All of these components affect loop behavior and must be accounted for in the loop compensation. The modulator consists of the internal PWM generator, the output MOSFET drivers and the external MOSFETs themselves. From a feedback loop point of view, it looks like a linear voltage transfer function from COMP to SW and has a gain roughly equal to the input voltage. It has fairly benign AC behavior at typical loop compensation frequencies with significant phase shift appearing at half the switching frequency. The external inductor/output capacitor combination makes a more significant contribution to loop behavior. These components cause a second order LC roll off at the output, with the attendant 180 ° phase shift. This rolloff is what filters the PWM waveform, resulting in the desired DC output voltage, but the phase shift complicates the loop compensation if the gain is still higher than unity at the pole frequency. Eventually (usually well above the LC pole frequency), the reactance of the output capacitor will approach its ESR and the rolloff due to the capacitor will stop, leaving 6dB/octave and 90 ° of phase shift (Figure 11). APPLICATIO S I FOR ATIO |
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