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CS5166 数据表(PDF) 21 Page - ON Semiconductor |
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CS5166 数据表(HTML) 21 Page - ON Semiconductor |
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21 / 25 page ![]() CS5166 http://onsemi.com 21 Implementing Current Sharing Using the “Droop Resistor” In addition to improving load transient performance, the CS5166 V2 control method allows the droop resistor to provide the additional capability to easily implement current sharing. Figure 31 shows a simplified schematic of two current sharing synchronous buck regulators. Each buck regulator’s droop resistor is terminated at the load. The PWM control signal from each Error Amp is connected together, causing the inner PWM loop to regulate to a common voltage. Since the voltage at each resistor terminal is the same, this configuration results in equal voltage being applied across each matched droop resistor. The result is equal current flowing through each buck regulator. An additional benefit is that synchronization to a common switching frequency tends to be achieved because each regulator shares a common PWM ramp signal. In practice, each buck regulator will regulate to a slightly different output voltage due to mismatching of the PWM comparators, slope of the PWM ramp (output voltage ripple), and propagation delays. At light loads, the results can be very poor current sharing. With zero output current, some regulators may be sourcing current while others may be sinking current. This results in additional power dissipation and lower efficiency than would be obtained by a single regulator. This is usually not an issue since efficiency is most important when a supply is fully loaded. This effect is similar to the difference in efficiency between synchronous and non−synchronous buck regulators. Synchronous buck regulators have lower efficiency at light loads because inductor current is always continuous, flowing from the load to ground during switch off−time through the synchronous rectifier. Under full load conditions, the synchronous design is more efficient due to the lower voltage drop across the synchronous rectifier. Likewise, the efficiency of droop sharing regulators will be lower at light loads due to the continuous current flow in the droop resistors. Efficiency at heavy loads tends to be higher due to reduced I2R losses. The output current of each regulator can be calculated from: IN + (VOUT(N) * VOUT) RDROOP(N) where: VOUT(N) and RDROOP(N) are the output voltage and droop resistance of a particular regulator and VOUT is the system output voltage. Output current is the sum of each regulator’s current: IOUT + I1 ) I2 ) AAA ) IN Current sharing improves with increasing load current. The increasing voltage drop across the droop resistor due to increasing load current eventually swamps out the differences in regulator output voltages. If a large enough voltage can be developed across the droop resistors, current sharing accuracy will be determined solely by their matching. To realize the benefits of current sharing, it is not necessary to obtain perfect matching. Keeping output currents within ± 10% is usually acceptable. For microprocessor applications, the value of the droop resistor must be selected to optimize adaptive voltage positioning, current sharing, current limit and efficiency. Current sharing is realized by simply connecting the COMP pins of the respective buck regulators, as shown in Figure 31. Figure 32 shows operation with no load. In this case, there is insufficient output voltage ripple across the droop resistor to produce complete synchronization. Duty Cycle is close to the theoretical 56% (VOUT/VIN) resulting in a switching frequency of approximately 275 kHz. Figure 34 shows operation with a 30 Amp load. Synchronization between the two regulators is now obtained due to increased ripple voltage. Increases losses cause the V2 control loop to increase on−time to compensate. This results in a larger duty cycle and a corresponding decrease in switching frequency to 233 kHz. Figure 32. No Load Waveforms Trace 1 = Output voltage ripple. Trace 2 = Buck regulator #1 inductor switching node. Trace 3 = Buck regulator #2 inductor switching node. |
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