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CS5307GDWR24 データシート(PDF) 13 Page - ON Semiconductor |
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CS5307GDWR24 データシート(HTML) 13 Page - ON Semiconductor |
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13 / 24 page ![]() CS5307 http://onsemi.com 13 Figure 16. Enhanced V2 Control Employing Lossless Inductive Current Sensing and Internal Ramp + − SWNODE Lx RCSx RLx CSx CSA COx CSREF + VOUT (VCORE) “Fast−Feedback” Connection + − PWM COMP To F/F Reset Channel Start−Up Offset − + E.A. DAC Out VFB COMP Internal Ramp + x = 1, 2, 3, or 4 CCSx Inductive Current Sensing For lossless sensing, current can be sensed across the inductor as shown in Figure 16. In the diagram, L is the output inductance and RL is the inherent inductor resistance. To compensate the current sense signal, the values of RCSx and CCSx are chosen so that L/RL = RCSx ⋅ CCSx. If this criteria is met, the current sense signal will be the same shape as the inductor current and the voltage signal at CSx will represent the instantaneous value of inductor current. Also, the circuit can be analyzed as if a sense resistor of value RL was used. When choosing or designing inductors for use with inductive sensing, tolerances and temperature effects should be considered. Cores with a low permeability material or a large gap will usually have minimal inductance change with temperature and load. Copper magnet wire has a temperature coefficient of 0.39% per °C. The increase in winding resistance at higher temperatures should be considered when setting the OCSET threshold. If a more accurate current sense is required than inductive sensing can provide, current can be sensed through a resistor as shown in Figure 14. Current Sharing Accuracy Printed circuit board (PCB) traces that carry inductor current can be used as part of the current sense resistance depending on where the current sense signal is picked off. For accurate current sharing, the current sense inputs should sense the current at relatively the same point for each phase and the connection to the CSREF pin should be made so that no phase is favored. In some cases, especially with inductive sensing, resistance of the PCB can be useful for increasing the current sense resistance. The total current sense resistance used for calculations must include any PCB trace resistance between the CSx input and the CSREF input that carries inductor current. Current Sense Amplifier (CSA) input mismatch and the value of the current sense component will determine the accuracy of the current sharing between phases. The worst case CSA input mismatch is ±10 mV and will typically be within 4.0 mV. The difference in peak currents between phases will be the CSA input mismatch divided by the current sense resistance. If all current sense components are of equal resistance, a 3.0 mV mismatch with a 2.0 mΩ sense resistance will produce a 1.5 A difference in current between phases. External Ramp Size and Current Sensing The internal ramp allows flexibility in setting the current sense time constant. Typically, the current sense RCSx ⋅ CCSx time constant should be equal to or slightly slower than the inductor’s time constant. If RC is chosen to be smaller (faster) than L/RL, the AC or transient portion of the current sensing signal will be scaled larger than the DC portion. This will provide a larger steady−state ramp, but circuit performance will be affected and must be evaluated carefully. The current signal will overshoot during transients and settle at the rate determined by RCSx ⋅ CCSx. It will eventually settle to the correct DC level, but the error will decay with the time constant of RCSx ⋅ CCSx. If this error is excessive, it will affect transient response, adaptive positioning and current limit. During a positive current transient, the COMP pin will be required to undershoot in response to the current signal in order to maintain the output voltage. Similarly, the VDRP signal will overshoot which will produce too much transient droop in the output voltage. The single−phase pulse−by−pulse overcurrent protection will trip earlier than it would if compensated correctly and hiccup−mode current limit will have a lower threshold for fast rising step loads than for slowly rising output currents. The waveforms in Figure 17 show a simulation of the current sense signal and the actual inductor current during a positive step in load current with values of L = 500 nH, RL = 1.6 mΩ, RCSx = 20 kΩ and CCSx = .01 μF. In this case, ideal current signal compensation would require RCSx to be 31 kΩ. |
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