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LTC1703 Datasheet(PDF) 14 Page - Linear Technology |
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LTC1703 Datasheet(HTML) 14 Page - Linear Technology |
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14 / 36 page ![]() 14 LTC1703 1703fa LTC1703 remains in continuous mode. See the Inductor Selection section for a detailed description of ripple current. As the output load current decreases in continuous mode, the average current in the inductor will reach a point where it drops below half the ripple current. At this point, the current in the inductor will reverse during a portion of the switching cycle, or begin to flow from the output back to the input. This does not adversely affect regulation, but does cause additional losses as a portion of the inductor current flows back and forth through the resistive power switches, giving away a little more power each time and lowering the efficiency. There are some benefits to allow- ing this reverse current flow: the circuit will maintain regulation even if the load current drops below zero (the load supplies current to the LTC1703) and the output ripple voltage and frequency remain constant at all loads, easing filtering requirements. Circuits that take advantage of this behavior can force the LTC1703 to operate in continuous mode at all loads by tying the FCB (Force Continuous Bar) pin to ground. Discontinuous Mode To minimize the efficiency loss due to reverse current flow at light loads, the LTC1703 switches to a second mode of operation: discontinuous mode (Figure 5b). In discontinu- ous mode, the LTC1703 detects when the inductor current approaches zero and turns off QB for the remainder of the switch cycle. During this time, the voltage at the SW pin will float about VOUT, the voltage across the inductor will be zero, and the inductor current remains zero until the next switching cycle begins and QT turns on again. This prevents current from flowing backwards in QB, eliminat- ing that power loss term. It also reduces the ripple current in the inductor as the output current approaches zero. The LTC1703 detects that the inductor current has reached zero by monitoring the voltage at the SW pin while QB is on. Since QB acts like a resistor, SW should ideally be right at 0V when the inductor current reaches zero. In reality, the SW node will ring to some degree immediately after it is switched to ground by QB, causing some uncertainty as to the actual moment the average current in QB goes to zero. The LTC1703 minimizes this effect by ignoring the SW node for a fixed 50ns after QB turns on when the ringing Figure 5a. Continuous Mode Figure 5b. Discontinuous Mode is most severe, and by including a few millivolts offset in the comparator that monitors the SW node. Despite these precautions, some combinations of inductor and layout parasitics can cause the LTC1703 to enter discontinuous mode erratically. In many cases, the time that QB turns off will correspond to a peak in the ringing waveform at the SW pin (Figure 6). This erratic operation isn’t pretty, but retains much of the efficiency benefit of discontinuous mode and maintains regulation at all times. TIME IRIPPLE IAVERAGE 1703 F05a TIME IRIPPLE IAVERAGE 1703 F05b Figure 6. Ringing at SW Causes Discontinuous Comparator to Trip Early TIME 50ns BLANK TIME 0V 0V 5V DISCONTINUOUS COMPARATOR TURNS OFF BG VSW VBG 1703 F06 TIME APPLICATIO S I FOR ATIO |
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