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OPTIMIZATION AND MINIATURIZATION OF MICROPROCESSOR POWER SUPPLIES

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However, as the number of devices increased, so did the demands on processor power. Therefore, reducing the size of the power supply is inevitably accompanied by a decrease in its efficiency.

Table  2.1:  Pentium Pro power supply specifications
Table 2.1: Pentium Pro power supply specifications

Conventional Power Distribution Architecture

Effects of the Parasitic Resistance of the Supply Path on the

Instead, the inductance of the power supply determines how quickly power can be delivered to the load. In the previous discussion, the output of the silver box was modeled by an ideal voltage source to illustrate the effect of the power line inductance on the voltage on the processor pins.

Figure 2.3: a) Simplified model of the conventional power distribution  scheme;  b) Voltage drops observed in  the system
Figure 2.3: a) Simplified model of the conventional power distribution scheme; b) Voltage drops observed in the system

Distributed Power Architecture

The VRM

The total loss in the main switch of the regular buck topology can be expressed as: Thus, the loss in the main switch will not be affected by the reverse recovery of the body diode. A graph of the inductor current, phase junction and output voltage is given in Fig.

Figure 2.7:  Basic buck converter
Figure 2.7: Basic buck converter

Overview of the Buck Converter Load Transient Response

Equation (3.19) gives an expression for 6 V5 as a function of switching frequency and output capacitance. To do this, the buck topology losses are analyzed in detail in Chapter 4 as a function of load current and switching frequency. Therefore, it is not possible to offset the output voltage according to the value of the inductor current.

Figure  3.2:  Typical load transient response of a buck converter: a) load  current step,  and b)  output voltage
Figure 3.2: Typical load transient response of a buck converter: a) load current step, and b) output voltage

Interval 1 2

Interval 1 3

Thus, despite the second term in (3.14), it is possible to minimize ~V5 by increasing the output capacitance or reducing the size of the inductor. From (3.19), the amount of output capacitance required to achieve the prescribed maximum drop between () can be expressed as a function of the switching frequency with the inductor current ripple as a parameter.

Fig.  3.6  shows  that  at  500kHz  achieving  100mV  of  voltage  drop  during  h  requires  between  150l-lF  and  650/-lF  of  output  capacitance,  depending  on  the  size  of  the  buck  inductor
Fig. 3.6 shows that at 500kHz achieving 100mV of voltage drop during h requires between 150l-lF and 650/-lF of output capacitance, depending on the size of the buck inductor

Interval 1 4

Optimizing Voltage Budgeting

A plot of the output capacitance needed to achieve a combined voltage drop of 150 mV over the intervals lz and 13 is shown in Fig. Therefore, the size penalty resulting from the ESR and ESL of the selected capacitors is somewhat offset by the overall efficiency improvement.

Fig.  3.7  shows  that  with  better  voltage  budgeting  during  the  intervals  lz  and  h,  the  total  output  capacitance  can  be  significantly  reduced
Fig. 3.7 shows that with better voltage budgeting during the intervals lz and h, the total output capacitance can be significantly reduced

Approaching the VRM Design Problem

  • Merits of the High Switching Frequency

The obvious advantage of a higher switching frequency is the reduction of the physical size of the buck inductor. In short, a higher switching frequency allows the designer to reduce the size of both the buck inductor and the output capacitors and increase the bandwidth of the control loop.

VRM Design Philosophy

On the other hand, operation at a high switching frequency will reduce the efficiency of the converter and require advanced packaging techniques. The optimization of the transient response of the voltage-controlled step-down converter is carried out in Chapter 7.

Overview of Various Loss Mechanisms in the Regular Buck Topology

  • Loss Mechanisms in the Schottky Diode

Conductivity loss in the main switch, Pel, can be expressed as:. where RDSoll1 is the drain to source on main switch resistor, Nml is the number of MOSFETs used in parallel, hrms is the rms current of the inductor and D is the duty cycle. The loss due to the junction capacitance can be expressed as: 4.11) where Cj is the capacitance of the Schottky diode junction.

Figure 4.1:  Regular buck converter including parasitics
Figure 4.1: Regular buck converter including parasitics

Overview of the Losses in the Synchronous Buck Topology

  • Loss Mechanisms in the Main Switch
  • Loss Mechanisms in a Synchronous Switch

The main loss mechanisms in Schottky are conduction loss, loss due to reverse bias leakage current and loss due to charge and discharge of junction capacitance. 4.17) where VGS2 is the drive voltage and QG2 is the total gate charge that must be supplied in order to enable the synchronous PET.

Figure 4.3:  Synchronous buck topology including parasitics
Figure 4.3: Synchronous buck topology including parasitics

Efficiency Considerations

  • Overview of Previously Published Work
  • C Loss Distribution

During tdl, the dominant loss component is reverse recovery of the body of the SR diode. However, the overall efficiency degradation due to SR body diode conduction is not independent of the inductor current ripple. A current sense resistor of 7mQ will reduce the efficiency of the module by 2-3% depending on the output voltage.

Figure 5.1: a) Regular buck; b) Synchronous buck
Figure 5.1: a) Regular buck; b) Synchronous buck

Experimental Verfification

On the Accuracy of the Component Level Distribution

5.5-5.8 show that the overall circuit efficiency of both topologies was accurate, no experimental evidence has yet been presented to verify that the actual component level loss distribution can be trusted. Thus, since the accuracy of the overall circuit efficiency was not affected by the change in the operating point, Fig.

Conclusion

In the future, improved synchronous rectifiers could extend their competitiveness to higher frequencies and loads. As the switching frequency rises, the MOSFET's low on-resistance advantage (RDsoll) decreases due to increasing switching loss, gate drive loss, and diode body loss.

Figure 5.11: Efficiency comparison between a  regular and a synchronous  buck for Vn=5.0V,  Vo=2.0V for  f~=440kHz  and 850kHz
Figure 5.11: Efficiency comparison between a regular and a synchronous buck for Vn=5.0V, Vo=2.0V for f~=440kHz and 850kHz

Overview of Previously Published Work

Since in some applications the VRM must operate at a relatively high input voltage (12V) and produce a relatively low output voltage (1.8V to 3.3V), the VRM synchronous converter deserves careful analysis and optimization. Therefore, a compromise must be found between size, load transient response and efficiency.

Overview of the Proposed Approach

Existing Controllers

In both cases, the loss in the body diode contributes significantly to the total loss. Results from Sections 6.5, 6.6 and 6.7 are combined in Section 6.S to show the full effect of the SR body diode conduction on the efficiency of a synchronous buck converter.

Table  6.1:  Loss distribution  in  Q2  of the synchronous bllckfor  V in =5.0V,  V o =2.5V
Table 6.1: Loss distribution in Q2 of the synchronous bllckfor V in =5.0V, V o =2.5V

Overview of the Synchronous Rectifier Loss

Although a synchronous buck converter always operates in the continuous conduction mode (CCM), since the waveforms in Fig. the SR body mode will produce losses during the two dead time intervals, tdl and td2.

Figure  6.7:  Synchronous buck converter waveforms:  a) gate drive signals  for QJ  and Q2,  b) inductor current in  mode  1,  c)  SR body diode current in
Figure 6.7: Synchronous buck converter waveforms: a) gate drive signals for QJ and Q2, b) inductor current in mode 1, c) SR body diode current in

Effect of tdl on the Synchronous Buck Efficiency in Mode 1

  • Overall Efficiency Degradation Due to the Body Diode Conduction
  • Overall Efficiency Degradation Due to the Body Diode Reverse
  • Overall Efficiency Degradation Due to the Body Diode Conduction

On the other hand, during td2, the SR body diode carries the load current plus half of the inductor current ripple. The conduction loss of the SR body diode during both intervals depends on the size of the inductor current ripple.

Figure  6.8:  The  overall efficiency degradation due  to the conduction of  D2  as afunction of the load current for tdJ=10ns-60ns (V in =12V,
Figure 6.8: The overall efficiency degradation due to the conduction of D2 as afunction of the load current for tdJ=10ns-60ns (V in =12V,

Effect of tdl on the Synchronous Buck Efficiency in mode 2

Effect of td2 on the Synchronous Buck Efficiency

A typical open-loop output impedance of a synchronous buck converter is shown in Fig. 7.7a shown. o) is a zero due to the ESR of the output capacitors. The location of this pin determines the rate of output voltage recovery after a weld transition.

Figure  6.11:  The  overall efficiency degradation due to the  conduction of  D2  as a function  of the load current for td2=10ns-60ns (Vin=12V,
Figure 6.11: The overall efficiency degradation due to the conduction of D2 as a function of the load current for td2=10ns-60ns (Vin=12V,

Effect of tdl and td2 on the Synchronous Buck Efficiency

New High Performance Gate Drive Circuit

Therefore, with this circuit we have achieved independent dead time control to less than ions. The prototype achieves a minimum dead time of lOns and an adequate switching speed for lMHz operation.

Experimental Verification

Independent control of the delay before each switch turns on allows us to optimize each delay separately for maximum efficiency. When the dead time becomes too long (tdl=60ns), the advantage is offset by the soft switching of the conduction loss of the diode DI.

Figure  6.16:  Measured and calculated overall synchronous buck  efficiency for tdl=td2=10ns (V ill =12V,  V out =3.3V, fs=1MHz)
Figure 6.16: Measured and calculated overall synchronous buck efficiency for tdl=td2=10ns (V ill =12V, V out =3.3V, fs=1MHz)

Conclusion

Namely, the loss due to body diode reverse recovery, dominant below tdl, will depend on the size of the ripple current. Therefore, the efficiency degradation due to SR body diode conduction decreases as the inductor current ripple increases.

Introduction

This article will focus on the design and optimization of the voltage mode control loop. An optimized control loop can save microfarads of output capacitance, thus reducing the size and cost of the point-of-load module.

Table  7.1:  Voltage and current specifications for 2.0V Pentium III (k)  processors
Table 7.1: Voltage and current specifications for 2.0V Pentium III (k) processors

Buck Converter Load Transient Response Revisited

  • Interval II
  • Interval 1 2
  • Interval 1 3
  • Interval 1 4

Finally, the integral action of the control circuit eliminates any steady-state error in the output voltage and returns it to its nominal value, as shown in Fig. 7.3, by inspection it can be determined that Zo is the impedance of the output capacitors.

Figure  7.2:  Typical transient response of a synchronous buck converter to  a  load current step  occurring at t=to
Figure 7.2: Typical transient response of a synchronous buck converter to a load current step occurring at t=to

Conventional Loop Compensation

Closing the loop in this way ensures tight control of the output voltage due to high DC gain, and reasonably good transient response, depending on the bandwidth achieved. Consequently, the peak-to-peak voltage deviation due to a charge transient followed by a discharge transient is approximately equal to twice the peak output voltage deviation due to a charge transient.

Figure  7.4:  The  Thevenin  equivalent model of a buck regulator output during  hand 14
Figure 7.4: The Thevenin equivalent model of a buck regulator output during hand 14

Optimum Load Transient Response

If, on the other hand, the output voltage remained at or near the lowest level it had reached after the load switch, there would be additional headroom for the discharge switch; the peak-to-peak deviation of the output voltage can be roughly halved.

Achieving Optimum Transient Response With Voltage Mode Control

A typical open-loop output impedance of a buck converter, b) Target loop gain, c) Optimal closed-loop output impedance. Setting %1 above zero frequency results in a finite DC closed-loop output impedance, and thus, a finite output voltage drift (steady-state error).

Figure  7.6:  Optirnum  transient response of a synchronous buck converter to  a load current step occurring at t=to
Figure 7.6: Optirnum transient response of a synchronous buck converter to a load current step occurring at t=to

Analysis and Simulation

Taking the inverse Laplace transform of (7.11) and (7.12) yields time domain equations for the converter output voltage, given by (7.13) and (7.14), respectively. The added value of (7.13) and (7.14) lies in the ability to investigate the contribution of each exponential term to the overall transient response and to derive closed formula expressions for peak voltage deviations.

Figure  7.8: Simulated converter transient response during hand 14
Figure 7.8: Simulated converter transient response during hand 14

Calculating the Peak Voltage Deviation

In other words, if lUe, lUzl, and W-.:2 are properly chosen, the transient response can be made to resemble the waveforms in Fig.

Experimental Verification

The transient response was measured for a load current step from 0.1 to 15A with a slew rate of 60All-ls and a frequency of 100Hz. The experimental results also confirmed the validity of (7.16): peak measured deviation under b was 56mV versus 60mV predicted by (7.16) and demonstrated in Fig.

Conclusion

Tight static voltage regulation and the desired shape of the converter's transient response were achieved by proper feedback loop design. Therefore, the overall efficiency of the module was improved by 2-3% by eliminating the current-sensing resistor without degrading the transient response.

Board Specifications

Introductory Remarks

Furthermore, due to the height restrictions, the value of the inductor may need to be limited. As a result, a higher than usual switching frequency may have to be chosen to keep the inductor current ripple reasonable.

Power Stage Design

  • Choosing the Inductor
  • Switch Implementation
  • A Choosing the Switches
  • B
  • Overall Circuit Efficiency

Similarly, using (3.19), we can plot the capacitance required to achieve ~V5=80mV as a function of the switching frequency. In contrast to the main switch (SJ), the synchronizing rectifier (SR) is switched on for approx. 70% of the switching period.

Figure  8.1:  Output capacitance required to achieve LlV 4 =80mV as a function  of the switching frequency
Figure 8.1: Output capacitance required to achieve LlV 4 =80mV as a function of the switching frequency

Control Loop Design

  • Placing Compensation Poles and Zeros
  • Circuit Implementation
  • Circuit Simulation
  • A Loopgain Calculation
  • B Load Transient Response Simulation

This small improvement in efficiency does not warrant the increase in board size and cost. Due to the limitations described, the gain in compensation must be limited to one in fa.

Figure  8.6:  Closing the  voltage loop:  a) duty ratio  to  output transfer  function,  b) compensation possibilities,  and c) resulting loopgain
Figure 8.6: Closing the voltage loop: a) duty ratio to output transfer function, b) compensation possibilities, and c) resulting loopgain

Experimental Results

  • Circuit Waveforms
  • Loopgain Measurement
  • Load Transient Response
  • Efficiency Measurements
  • Physical Dimensions

The effectiveness of the module was measured with the board mounted on the evaluation board. From Table 8.3 we note that the length of the board is 1.2 times less than specified.

Figure 8.10:  Circuit waveforms (Io=10A):  inductor current (top),  output  voltage (middle),  phase node (bottom)
Figure 8.10: Circuit waveforms (Io=10A): inductor current (top), output voltage (middle), phase node (bottom)

Concluding Remarks

A high switching frequency makes it possible to reduce both the physical size and value of the magnetic components. The only disadvantage of operating at a high switching frequency is the reduced efficiency of the power supply and more difficult thermal management.

Figure 8.20:  Optimized VRM module
Figure 8.20: Optimized VRM module

Gambar

Figure 2.4:  Conventional desktop computer power distribution scheme with  remote sensing in the supply path
Figure  3.2:  Typical load transient response of a buck converter: a) load  current step,  and b)  output voltage
Figure 4.2:  Switch voltage and current waveforms at a)  turn-on,  b) turn-off
Figure 5.4:  Overall efficiency of the circuit as a function  of the  load current  for  J\=1.5MHz,  O.9MHz,  and  O.5MHz  at  V ill =5V,  VOllt=3.0V
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