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LTC1430AIGN 数据表(PDF) 15 Page - Linear Technology |
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LTC1430AIGN 数据表(HTML) 15 Page - Linear Technology |
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15 / 24 page ![]() 15 LTC1430A S APPLICATI I FOR ATIO Longer overload conditions will allow the SS pin to reach a steady level, and the output will remain at a reduced voltage until the overload is removed. Serious overloads will generate a larger overdrive at ILIM, allowing it to pull SS down more quickly and preventing damage to the output components. The ILIM amplifier output is disabled when Q1 is OFF to prevent the low IFB voltage in this condition from activating the current limit. It is re-enabled a fixed 170ns after Q1 turns on; this allows for the IFB node to slew back high and the ILIM amplifier to settle to the correct value. As the LTC1430A goes deeper into current limit, it will reach a point where the Q1 on-time needs to be cut to below 170ns to control the output current. This conflicts with the minimum settling time needed for proper operation of the ILIM amplifier. At this point, a secondary current limit circuit begins to reduce the internal oscillator frequency, lengthening the off-time of Q1 while the on-time remains constant at 170ns. This further reduces the duty cycle, allowing the LTC1430A to maintain control over the output current. Under extreme output overloads or short circuits, the ILIM amplifier will pull the SS pin more than 2V below VCC in a single switching cycle, cutting the duty cycle to zero. At this point all switching stops, the output current decays through Q2 and the LTC1430A runs a partial soft start cycle and restarts. If the short is still present the cycle will repeat. Peak currents can be quite high in this condition, but the average current is controlled and a properly designed circuit can withstand short circuits indefinitely with only moderate heat rise in the output FETs. In addi- tion, the soft start cycle repeat frequency can drop into the low kHz range, causing vibrations in the inductor which provide an audible alarm that something is wrong. Oscillator Frequency The LTC1430A includes an onboard current controlled oscillator which will typically free-run at 200kHz. An internal 20 µA current is summed with any current in or out of the FREQSET pin (Pin 11), setting the oscillator fre- quency to approximately 10kHz/ µA. FREQSET is internally servoed to the LTC1430A reference voltage (1.265V). With FREQSET floating, the oscillator is biased from the LTC1430A will be in full operation. An internal switch shorts the SS pin to GND during shutdown. The LTC1430A detects the output current by watching the voltage at IFB while Q1 is ON. The ILIM amplifier compares this voltage to the voltage at IMAX (Figure 13). In the ON state, Q1 has a known resistance; by calculating back- wards, the voltage generated at IFB by the maximum output current in Q1 can be determined. As IFB falls below IMAX, ILIM will begin to sink current from the soft start pin, causing the voltage at SS to fall. As SS falls, it will limit the output duty cycle, limiting the current at the output. Eventually the system will reach equilibrium, where the pull-up current at the SS pin matches the pull-down current in the ILIM amplifier; the LTC1430A will stay in this state until the overcurrent condition disappears. At this time IFB will rise, ILIM will stop sinking current and the internal pull-up will recharge the soft start capacitor, restoring normal operation. Note that the IFB pin requires an external 1k series resistor to prevent voltage transients at the drain of Q2 from damaging internal structures. – + ILIM LTC1430A 1430 F13 RIMAX PVCC IMAX IFB SS CSS 12 µA Q1 Q2 12 µA VCC 1k 0.1 µF Figure 13. Current Limit Operation The ILIM amplifier pulls current out of SS in proportion to the difference between IFB and IMAX. Under mild overload conditions, the SS pin will fall gradually, creating a time delay before current limit takes effect. Very short, mild overloads may not trip the current limit circuit at all. |
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