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SECTION 4 SWITCHED CAPACITOR VOLTAGE CONVERTERS …

SWITCHED CAPACITOR VOLTAGE 4 SWITCHED CAPACITOR VOLTAGECONVERTERSWalt Kester, Brian Erisman, Gurjit ThandiINTRODUCTIONIn the previous SECTION , we saw how inductors can be used to transfer energy andperform VOLTAGE conversions. This SECTION examines SWITCHED CAPACITOR voltageconverters which accomplish energy transfer and VOLTAGE conversion two most common SWITCHED CAPACITOR VOLTAGE CONVERTERS are the VOLTAGE inverterand the VOLTAGE doubler circuit shown in Figure In the VOLTAGE inverter, thecharge pump CAPACITOR , C1, is charged to the input VOLTAGE during the first half ofthe switching cycle. During the second half of the switching cycle, its VOLTAGE isinverted and applied to CAPACITOR C2 and the load.

converters which accomplish energy transfer and voltage conversion using capacitors. The two most common switched capacitor voltage converters are the voltage inverter and the voltage doubler circuit shown in Figure 4.1. In the voltage inverter, the charge pump capacitor, C1, is charged to the input voltage during the first half of the ...

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Transcription of SECTION 4 SWITCHED CAPACITOR VOLTAGE CONVERTERS …

1 SWITCHED CAPACITOR VOLTAGE 4 SWITCHED CAPACITOR VOLTAGECONVERTERSWalt Kester, Brian Erisman, Gurjit ThandiINTRODUCTIONIn the previous SECTION , we saw how inductors can be used to transfer energy andperform VOLTAGE conversions. This SECTION examines SWITCHED CAPACITOR voltageconverters which accomplish energy transfer and VOLTAGE conversion two most common SWITCHED CAPACITOR VOLTAGE CONVERTERS are the VOLTAGE inverterand the VOLTAGE doubler circuit shown in Figure In the VOLTAGE inverter, thecharge pump CAPACITOR , C1, is charged to the input VOLTAGE during the first half ofthe switching cycle. During the second half of the switching cycle, its VOLTAGE isinverted and applied to CAPACITOR C2 and the load.

2 The output VOLTAGE is thenegative of the input VOLTAGE , and the average input current is approximately equalto the output current. The switching frequency impacts the size of the externalcapacitors required, and higher switching frequencies allow the use of smallercapacitors. The duty cycle - defined as the ratio of charging time for C1 to the entireswitching cycle time - is usually 50%, because that generally yields the optimalcharge transfer initial start-up transient conditions and when a steady-state condition isreached, the charge pump CAPACITOR only has to supply a small amount of charge tothe output CAPACITOR on each switching cycle. The amount of charge transferreddepends upon the load current and the switching frequency.

3 During the time thepump CAPACITOR is charged by the input VOLTAGE , the output CAPACITOR C2 must supplythe load current. The load current flowing out of C2 causes a droop in the outputvoltage which corresponds to a component of output VOLTAGE ripple. Higherswitching frequencies allow smaller capacitors for the same amount of droop. Thereare, however, practical limitations on the switching speeds and switching losses, andswitching frequencies are generally limited to a few hundred VOLTAGE doubler works similarly to the inverter; however, the pump CAPACITOR isplaced in series with the input VOLTAGE during its discharge cycle, therebyaccomplishing the VOLTAGE doubling function.

4 In the VOLTAGE doubler, the averageinput current is approximately twice the average output basic inverter and doubler circuits provide no output VOLTAGE regulation,however, techniques exist to add regulated capability and have been implemented inthe ADP3603/3604/3605 CAPACITOR VOLTAGE SWITCHED CAPACITOR VOLTAGEINVERTER AND VOLTAGE DOUBLERVOUT VINLOADVIN+C1C2 IOUTINVERTERVOUT 2 VINLOADVIN+C1C2 IOUTDOUBLERF igure are certain advantages and disadvantages of using SWITCHED capacitortechniques rather than inductor-based switching regulators. An obvious keyadvantage is the elimination of the inductor and the related magnetic design addition, these CONVERTERS typically have relatively low noise and minimalradiated EMI.

5 Application circuits are simple, and usually only two or three externalcapacitors are required. Because there is no need for an inductor, the final PCBcomponent height can generally be made smaller than a comparable switchingregulator. This is important in many applications such as display CAPACITOR inverters are low cost and compact and are capable of achievingefficiencies greater than 90%. Obviously, the current output is limited by the size ofthe capacitors and the current carrying capacity of the switches. Typical IC switchedcapacitor inverters have maximum output currents of about 150mA CAPACITOR VOLTAGE CONVERTERS do not maintain high efficiency for a widerange of ratios of input to output voltages, unlike their switching regulatorcounterparts.

6 Because the input to output current ratio is scaled according to thebasic VOLTAGE conversion ( , doubled for a doubler, inverted for an inverter)regardless of whether or not regulation is used to reduce the doubled or invertedvoltage, any output VOLTAGE magnitude less than 2 VIN for a doubler or less than|VIN| for an inverter will result in additional power dissipation within theconverter, and efficiency will be degraded CAPACITOR VOLTAGE CAPACITOR VOLTAGE CONVERTERSnNo Inductors!nMinimal Radiated EMInSimple Implementation: Only 2 External Capacitors(Plus an Input CAPACITOR if Required)nEfficiency > 90% AchievablenOptimized for Doubling or Inverting Supply VOLTAGE -Efficiency Degrades for Other Output VoltagesnLow Cost, Compact, Low Profile (Height)nParts with VOLTAGE Regulation are Available:ADP3603/ADP3604/ADP3605/ADP360 7 Figure VOLTAGE inverter is useful where a relatively low current negative VOLTAGE isrequired in addition to the primary positive VOLTAGE .

7 This may occur in a singlesupply system where only a few high performance parts require the negativevoltage. Similarly, VOLTAGE doublers are useful in low current applications where avoltage greater than the primary supply VOLTAGE is TRANSFER USING CAPACITORSA fundamental understanding of capacitors (theoretical and real) is required inorder to master the subtleties of SWITCHED CAPACITOR VOLTAGE CONVERTERS . Figure the theoretical CAPACITOR and its real-world counterpart. If the CAPACITOR ischarged to a VOLTAGE V, then the total charge stored in the CAPACITOR , q, is given by q= CV. Real capacitors have equivalent series resistance (ESR) and inductance (ESL)as shown in the diagram, but these parasitics do not affect the ability of thecapacitor to store charge.

8 They can, however, have a large effect on the overallefficiency of the SWITCHED CAPACITOR VOLTAGE CAPACITOR VOLTAGE CHARGE IN A CAPACITORESRESLCC+V-STORED CHARGEq = CV+V-IDEALACTUALF igure an ideal CAPACITOR is charged with an ideal VOLTAGE source as shown in (A), the CAPACITOR charge buildup occurs instantaneously, corresponding to a unitimpulse of current. A practical circuit (Figure (B)) will have resistance in theswitch (RSW) as well as the equivalent series resistance (ESR) of the CAPACITOR . Inaddition, the CAPACITOR has an equivalent series inductance (ESL). The chargingcurrent path also has an effective series inductance which can be minimized withproper component layout techniques.

9 These parasitics serve to limit the peakcurrent, and also increase the charge transfer time as shown in the diagram. Typicalswitch resistances can range from 1 to 50 , and ESRs between 50m and 200m .Typical CAPACITOR values may range from about F to 10 F, and typical ESLvalues 1 to 5nH. Although the equivalent RLC circuit of the CAPACITOR can beunderdamped or overdamped, the relatively large switch resistance generally makesthe final output VOLTAGE response CAPACITOR VOLTAGE A CAPACITOR FROM A VOLTAGE SOURCEVIN +CVIN +CiRSWiESRvOUTvOUT0 VINIPEAK t 0 VIN000 IDEAL (A)ACTUAL (B)vOUTvOUTiiESLF igure law of conservation of charge states that if two capacitors are connectedtogether, the total charge on the parallel combination is equal to the sum of theoriginal charges on the capacitors.

10 Figure shows two capacitors, C1 and C2, eachcharged to voltages V1 and V2, respectively. When the switch is closed, an impulseof current flows, and the charge is redistributed. The total charge on the parallelcombination of the two capacitors is qT = C1 V1 + C2 V2. This charge is distributedbetween the two capacitors, so the new VOLTAGE , VT, across the parallel combinationis equal to qT/(C1 + C2), orVTqTCCCVCVCCCCCVCCCV=+= + +=+ ++ principle may be used in the simple charge pump circuit shown in Figure that this circuit is neither a doubler nor inverter, but only a VOLTAGE pump CAPACITOR is C1, and the initial charge on C2 is zero. The pump capacitoris initially charged to VIN.


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