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Zero-Voltage–Zero-Current Switc

Zero-Voltage–Zero-Current Switc

Zero-V oltage–Zero-Current Switching in High-Output-V oltage Full-Bridge PWM Converters Using the Interwinding CapacitanceDjordje Garabandic,William G.Dunford,Senior Member,IEEE,and Mark EdmundsAbstract—A novel zero-voltage and zero-current-switching (ZVZCS)full-bridge(FB)pulsewidth-modulated(PWM) converter is proposed.The new converter uses the interwinding capacitance and a small primary-side inductor to achieve a zero-current–zero-voltage turn off and a zero-current turn on of the passive-to-active leg transistors.The turn off of the active-to-passive leg transistors is with zero voltage,and the turn on is with zero voltage and zero current across them.The ringing caused by the parasitic interwinding capacitance and by the reverse recovery of the rectifiers is reduced.The new converter is attractive for high-output-voltage applications(600–1000V), where the interwinding capacitance is sufficiently dominant. In addition,switches such as insulated gate bipolar transistors (IGBT’s)and MCT’s can be used at higher frequencies which is particularly desirable for high-power application(above2 kW).The experimental results obtained from an IGBT-based 62.5-kHz dc/dc converter with a rated output voltage of600V and a nominal power of1.2kW are presented.I.I NTRODUCTIONP ARASITIC components such as the leakage inductance of the transformer and the output capacitance of the switches are effectively used in the zero-voltage-switching(ZVS)full-bridge(FB)pulsewidth-modulated(PWM)converter to reduce the switching losses[1]–[4].This switching technique is particularly well suited for high-frequency MOSFET-based applications.Yet,ZVS alone does not address problems related to the reverse recovery of the output rectifiers,and this is critical in high-output-voltage(HOV)converters.In addition, the use of insulated gate bipolar transistors(IGBT’s)instead of MOSFET’s is not trivial.A common characteristic of HOV-FB converters is that the number of secondary turns of the power transformer is considerably larger than the number of primary turns. Unavoidably,this increases the interwinding capacitance of the secondary.The interwinding capacitance,together with the equivalent capacitance of the high-voltage rectifiers,causes the so-called reverse-recovery ringing and a high-reverse-recovery-voltage spike across the diodes.These phenomena are the major limiting factors for the maximum achievableManuscript received April8,1998;revised July14,1998.Recommended by Associate Editor,J.Thottuvelil.D.Garabandic and M.Edmunds are with Xantrex Technology,Inc., Burnaby,B.C.,V5A4V7,Canada(e-mail:gar@).W.G.Dunford is with the Department of Electrical Engineering,University of British Columbia,B.C.,V6T1Z4,Canada.Publisher Item Identifier S0885-8993(99)01835-9.output voltage,and at the same time they are the generators of much of the noise and losses.A possible dissipative clamp that limits the reverse-recovery voltage spike is presented in[2].The optimal use of that clamp is forfixed output-voltage converters,since the clamping level changes with the output voltage.A very efficient active clamp as in[3]is less cost effective since it requires an additional transistor andfloating drivers for each rectifier stage.The commutating aid circuit consisting of a small inductor and two clamping diodes improves the performance of a ZVS converter[4].It reduces the reverse-recovery ringing,extends the soft-switching region toward the light-load conditions,and enables an optimal transformer design.The main concern with the circuit proposed in[4],when used with IGBT’s,is that the ZVS is not the preferred oper-ating mode.The efficiency of an IGBT bridge is higher when operating in the zero-current-switching(ZCS)mode.A simple circuit proposed in[5]achieves this goal with a capacitor and a saturable reactor placed in series with the primary.There,the current in the primary is reset during the freewheeling period by the series capacitor and sustained at close to zero by the saturable reactor.However,the voltage that builds up across the series capacitor additionally increases the reverse voltage across the output diodes.In HOV applications,it is imperative to keep the reverse voltage of the diodes as low as possible and the circuit as in[5]is not suitable.The proposed HOV-FB-ZVZCS-PWM converter is shown in Fig.1.The basic topology is the same as that of a ZVS-FB-PWM converter.The output consists of two stacked rectifier bridges(if necessary,this number can be larger).The addi-tional small(balancing)transformers(and)balance the terminal currents of the two secondary windings,and their function will be explained later.Here,only an outline of the main concept is given.During the active-to-passive transition, the high interwinding capacity between the two secondaries resets the primary current to zero.By the time the freewheeling period begins(turn on of the active-to-passive leg transistor), the current in the primary is practically zero.Consequently, the passive-to-active leg transistor turns off with zero current. The primaryreactor delays the current buildup and ensures that the turn on of the passive-to-active leg transistor is with zero current.The proposed concept was verified on an experimental 1.2-kW62.5-kHz IGBT-based FB converter with a rated output voltage of600V and a nominal power of1.2kW.0885–8993/99$10.00©1999IEEEFig.1.The proposedHOV-ZVZCS-FB-PWM.Fig.2.The two secondaries formed by a bifilar winding.This paper gives design considerations as well as the obtained experimental results.II.P RINCIPLEOFO PERATIONThe proposed ZVZCS converter is controlled by phase shifting.Basically,the same control circuitry can be used which already exists for the FB-ZVS-PWM converter.In order to explain the operation of the proposed converter,certain general assumptions will be made.•is large enough and can be treatedas a constant current source.•The dominant interwinding capacitance–dischargesthrough,and themiddleFig.3.Idealized waveforms from the circuit in Fig.1.Fig.4.The sequence of events during an active-to-passive transition.GARABANDIC et al .:ZERO-VOLTAGE–ZERO-CURRENT SWITCHING IN PWM CONVERTERS 345pointvoltage starts toconductassumption:is the outputcurrent transferred to theprimary side.STRUCTURE 2—–is still not discharged,a negative voltageacrossforces the currentthrough to drop to zero.At ,the current through the primary has reached zero.Thetransistoris the voltageacrossand.STRUCTURE 3—–is stillcharged;the result is that thediodesis discharged by theoutputcurrentreaches zero.At ,all secondary-side diodes are forward biased and the freewheeling period beginsassumption:(3)whereis the primary-side equivalentof––(4)The slopeof ,thus reducing the effective dutycycleby ,the turn onof–for thediodesandis(5)and the pick reverse-recoverycurrentdenotes the carrierlifetime,.Fig.5.The sequence of events during a passive-to-active transition.STRUCTURE 7—–.Theand is ringing.The ringing is reduced with the balancing transformers becauseeffectivelyis charged through the (saturable)magnetizing inductance of the balancingtransformersand ,and this effect will be explained in the next section.By adding the clampingdiodes–and the reverse recovery can bereduced by:1)increasing the damping factor of theresonating.Fig.6(a)and (b)proposes snubbers that achieve these goals.The main idea in both cases is to use balancing transformers that equalizethe terminal currents of the twosecondariesand .The incremental models of Structure 7(Fig.5)are346IEEE TRANSACTIONS ON POWER ELECTRONICS,VOL.14,NO.2,MARCH1999(a)(b)Fig.6.Snubbing the C i w with balancing transformers T bal1and T bal2:(a)limiting the inrush current with R snb1and R snb2,(b)limiting the inrush current with the magnetizing inductance of T bal1and T bal2,(c)the incremental model of the circuit from Fig.6(a),and (d)the incremental model of the circuit from Fig.6(b).Fig.7.Experimental waveforms (a)without and (b)with balancing transformers.Traces:v d (200V/div),i prim (10A/div),and time =2 s/div.shown in Fig.6(c)and (d).In the case of the circuit in Fig6(a),the differenceand thatcharges and is limited (and the ringingis damped)by the saturable magnetizing inductance of thebalancingtransformersand .Fig.7shows the experimental waveforms with and without the proposed balancing transformers.A comparison of thesewaveforms shows a considerable improvement.Each balanc-ing transformer consists of214GARABANDIC et al .:ZERO-VOLTAGE–ZERO-CURRENT SWITCHING IN PWM CONVERTERS347Fig.8.The soft-switchingregion.Fig.9.Waveforms obtained from the experimental converter traces:V a (200V/div),V b (200V/div),i prim (10A/div),and time =2 s/div.2)ZVZC turn on of the active-to-passive leg transistor.3)ZVZC turn off of the passive-to-active leg transistor.4)ZC turn on of the passive-to-active leg transistor.5)The current thatchargesis limited,and the ringing is damped by the balancing transformers.In the active-to-passive leg,the turn-off losses can befurther minimized by the use of external capacitors(and )[5].In the passive-to-active leg,the turn-off losses are practically zero.The turn-on losses are low in both legs due to the ZCS.Because of that,the proposed converter is particularly welcome for IGBT-based bridges.From Fig.4it can be concluded that in order to achieve the ZVZCS by using the interwinding capacitance,the following conditions have to bemet:and to providethe ZVS.The second inequality reflects the condition under which the interwinding capacitance is capable of resetting the primary current for theZCS.Fig.10.The magnified active-to-passive transition traces:V a (200V/div),V b (200V/div),i prim (10A/div),V Ciw (200V/div),and time =1s/div.Fig.11.The magnified passive-to-active transition traces:V a (200V/div),V b (200V/div),i prim (10A/div),V Ciw (200V/div),and time =1 s/div.The soft-switching region,as a functionof ,is plotted in Fig.8.In this plot,three distinct sectors are identified.Depending in which of the sectors is the operating point,the following can be concluded.1)Sector 1:The active-to-passive leg is ZVS.The primary current is only partially reset and still flowing during the freewheeling period.Thus,a ZV transition in the passive-to-active leg is initiated.Basically,this operating mode is the same as that of a FB-ZVS-PWM [1]converter.2)Sector 2:The conditions (7)and (8)are satisfied,and the converter is in the ZVZC operating mode.3)Sector 3:In light-load conditions,the active-to-passive leg is no longer ZV switched.The effect of the primaryinductanceon the pick primary current (turn-on current spike)can be assessed from the incremental model of the Structure 7(Fig.5).The upperbound for the primary currentovershoot(worst case348IEEE TRANSACTIONS ON POWER ELECTRONICS,VOL.14,NO.2,MARCH 1999TABLE IT HE T HEORETICALANDM EASURED P ARAMETERSOF THECONVERTERFig.12.Efficiency measurements:IGBT versus MOSFET.no damping)is(9)Combining (6),(8),and (9),it followsthat(10)In other words,ahigherreduces the primary current over-shoot caused by both the reverse recovery and the interwindingcapacity.However,the lower limitforis .V.E XPERIMENTAL R ESULTSThe outlined concept was implemented and verified on a62.5-kHz converter and the basic circuit diagram is shown in Fig.1.The input-voltagerangenF,TrnF.Whendesigning a transformer for acertaincan be predicted by experimentally (empirically)derivedformulas,and in thiscaseand .The obtained production toleranceof25%.The combined primary series inductance,referred to as primary inductance,is14RHRP8120(Harris),,anddelays the buildup of theprimary current.A common feature of HOV applications is a turn-on spike in the primary current.The origin of that spike is the reverse-recovery characteristic of the high-voltage rectifiers and the interwinding capacitance.A transformer design that minimizes the interwinding capacity either decreases the magnetizing or increases the leakage inductance [8],[9],and the susceptibility of the circuit to ringing is not reduced.An alternative approach to avoid the switching losses associated with the capacitiveGARABANDIC et al.:ZERO-VOLTAGE–ZERO-CURRENT SWITCHING IN PWM CONVERTERS349load is by using the proposed ZVZCS principle.From Fig.11, it is evident that by the time the current turn-on spike builds up,the transistor is already well saturated.In order to correlate the theoretically predicted and experi-mentally obtained performance of the converter,Table I lists several measured and calculated parameters.The efficiency of the62.5-kHz IGBT-based converter versus MOSFET’s(IRFP460)is shown in Fig.12.This plot indicates that the traditional frequency limit for the IGBT’s can be extended to higher frequencies with the use of the proposed ZVZCS.VI.C ONCLUSIONThe interwinding capacitance,which is usually considered undesirable,is in this case constructively used for achiev-ing the ZVZCS.Thus,converters with a high interwinding capacitance(usually HOV converters)can benefit from that parasitic component.The novel ZVZCS method is presented and analyzed,including experimental results obtained from an IGBT-based62.5-kHz dc/dc converter with a rated output voltage of600V and a nominal power of1.2kW.The advantages of the new converter are:•lower switching losses:ZV turn off of the active-to-passive leg transistor,ZVZC turn on of the active-to-passive leg transistor,ZVZC turn off of the passive-to-active leg transistor,and ZC turn on of the passive-to-active leg transistor;•lower noise and reverse-recovery ringing by controlling the charge current of the interwinding capacitance with balancing transformers;•lower conduction losses in the primary since there is no currentflowing during the freewheeling period;•higher power density(IGBT’s can be used at higher switching frequencies).R EFERENCES[1]J.A.Sabate,V.Vlatkovic,R.B.Ridley,F.C.Lee,and B.H.Cho,“Design considerations for high-voltage high-power full-bridge zero-voltage-switching PWM converter,”in IEEE APEC Rec.,1990,pp.275–284.[2]L.H.Mweene,C.A.Wright,and M.F.Schlecht,“A500kHz front-endconverter for a distributed power supply system,”in IEEE APEC Rec., 1989,pp.423–432.[3]J. A.Sabate,V.Vlatkovic,R. B.Ridley,and F. C.Lee,“High-voltage,high-power,ZVS,full-bridge PWM converter employing an active snubber,”in IEEE APEC Rec.,1991,pp.158–163.[4]R.Redl,N.O.Sokal,and L.Balogh,“A novel soft-switching full-bridgedc/dc converter:Analysis,design considerations,and experimental re-sults at1.5kW,100kHz,”in IEEE PESC Rec.,1990,pp.162–172. [5]J.G.Cho,J.A.Sabate,G.Hua,and F.C.Lee,“Zero-voltage andzero-current-switching full bridge PWM converter for high power ap-plications,”in IEEE PESC Rec.,1994,pp.189–194.[6]N.Mohan,T.M.Underland,and W.P.Robbins,Power Electronics:Converters,Applications and Design.New York:Wiley,1989. [7] D.Garabandic,W.G.Dunford,and M.Edmunds,“Snubbers for theinterwinding capacitance in high-output-voltage converters,”in IEEEAPEC Rec.,1998,pp.846–849.[8]S.Ohitsu and T.Ogata,“Considerations on the relationship between dis-tributed capacitance and power loss in a push-pull current-fed converterin buck-mode,”in IEEE PESC Rec.,1988,pp.1007–1012.[9]S.Ohitsu,T.Yamashita,K.Yamamoto,and T.Sugiura,“Stabilityin high-output-voltage push-pull current-fed converters,”IEEE Trans.Power Electron.,vol.8,no.2,pp.135–139,1993.Djordje Garabandic was born in Novi Sad,Yu-goslavia,on December18,1965.He received theB.Sc.degree from the University of Novi Sad,NoviSad,and the Ph.D.degree from the University ofBelgrade,Belgrade,Yugoslavia,in1990and1995,respectively.From1996to1997,he was a Post-DoctoralFellow at the Department of Electrical Engineering,University of British Columbia,Canada.He is cur-rently with the power design team of Xantrex Tech-nology,Inc.,Burnaby,B.C.,Canada.His researchinterests include high-power dc/dc conversion,nondissipative snubbering,and application of the advanced control theory on power conversion systems.He is the author of several technical papers.Dr.Garabandic is the Chair of the IEEE Power Electronics Chapter in Vancouver,Canada.William G.Dunford(SM’92)received the B.Sc.and M.Sc.degrees from Imperial College,London,U.K.,and the Ph.D.degree from the University of Toronto,Toronto,P.Q.,Canada.He spent two years as a Field Engineer with Schlumberger Overseas and has been a Lecturer at Imperial College and the University of Toronto.He is an Associate Professor at the University of British Columbia,Vancouver,Canada. Currently,he is on a leave of absence at Alcatel Espace,Toulouse,France. His engineering interests include efficient and alternative power conversion, particularly at higher powers.He also has projects in battery management and modeling.Dr.Dunford currently chairs the Chapter Development for the IEEE Power Electronics Society and was the General Chairman of PESC in1986(and will be in2001).Mark Edmunds,photograph and biography not available at the time of publication.。

Hayati_et_al-2013-Microwave_and_Optical_Technology_Letters

Hayati_et_al-2013-Microwave_and_Optical_Technology_Letters

2.88GHz.For the lower mode with C¼0.6pF and the higher mode with C¼5pF,the effects of varying/on CP perform-ance are given in Figures4and5,respectively.The simulation results suggest that an axial ratio of less than2dB can be found when/ranges between10and25 for the lower mode and between12and16 for the higher mode.3.RECONFIGURABLE DESIGN AND EXPERIMENTAL RESULTSAn antenna prototype with electrically switching was realized using a varactor diode(BB837,Siemens Semiconductor Group).For the dc bias(V0)used for controlling the varactor, its positive is connected to the feed line through a RF choke, which is composed of a high-impedance meandered microstrip line and a grounded capacitor of1nF,and the negative is directly linked to the RF ground plane,as shown in Figure1. Figure6exhibits the experimental results when V0is switched between two different values.From the measured results,it can be seen that the frequency with minimum axial ratio is1.83 GHz for the case of V0¼28V and it is2.96GHz for the case of V0¼6V.The CP bandwidths,determined by3dB axial ra-tio,are2.7and3.3%at the lower and higher CP operating fre-quencies,respectively.In addition,Figure6also demonstrates that a return loss of less than10dB is achieved within the two CP bandwidths.Therefore,the antenna can perform the dual-frequency operation with a frequency ratio of about1.6through switching.The radiation patterns at1.83and2.96GHz are measured and their results are plotted in Figure7.Broadside radiation with good CP performance is observed for each operating fre-quency,and the polarization in the plane of z>0is left-handed. The peak gain at1.83GHz is about3.3dBic and it is merely 0.2dB lower than that at2.96GHz.4.CONCLUSIONA design for circularly polarized annular slot antennas with switchable frequency has been presented.Only one diode is required in the reconfigurable design.With controlling the dc bias of the diode,the antenna can perform dual-frequency opera-tion with a high frequency ratio.Moreover,the antenna at the two operating frequencies has almost the same radiation pattern, polarization performance,and peak gain.REFERENCES1.Y.K.Jung and B.Lee,Dual-band circularly polarized microstripRFID reader antenna using metamaterial branch-line coupler,IEEE Trans Antennas Propag60(2012),786–791.2.Nasimuddin,Z.N.Chen,and X.Qing,Dual-band circularly-polar-ized S-shaped slotted patch antenna with a small frequency ratio, IEEE Trans Antennas Propag58(2010),2112–2115.3.J.Y.Sze,C.I.G.Hsu,and J.J.Jiao,CPW-fed circular slot antennawith slit back-patch for2.4/5GHz dual-band operation,Electron Lett42(2006),563–564.4.Y.L.Zhao,Y.C.Jiao,G.Zhao,Z.B.Weng,and F.S.Zhang,Anovel polarization reconfigurable ring-slot antenna with frequency agility,Microwave Opt Technol Lett51(2009),540–543.5.N.Jin,F.Yang,and Y.Rahmat-Samii,A novel patch antenna withswitchable slot(PASS):dual-frequency operation with reversed cir-cular polarizations,IEEE Trans Antennas Propag54(2006), 1031–1034.6.T.Y.Lee and J.S.Row,Frequency reconfigurable circularly polar-ized slot antennas with wide tuning range,Microwave Opt Technol Lett53(2011),1501–1505.V C2013Wiley Periodicals,Inc.DESIGN OF BROADBAND AND HIGH-EFFICIENCY CLASS-E AMPLIFIER WITH pHEMT USING A NOVEL LOW-PASS MICROSTRIP RESONATOR CELLMohsen Hayati1,2and Ali Lotfi11Electrical Engineering Department,Faculty of Engineering,Razi University,Tagh-E-Bostan,Kermanshah-67149,Iran; Corresponding author:mohsen_hayati@2Computational Intelligence Research Centre,Razi University,Tagh-E-Bostan,Kermanshah-67149,IranReceived31August2012ABSTRACT:In this article,a high-efficient class-E amplifier design with low voltage and broadband characteristics using a novel Front Coupled Tapered Compact Microstrip Resonant Cell is presented.The proposed micorstrip resonator is used as the harmonic control network in order to suppress higher order harmonics,which obtained the optimized impedance matching for the fundamental and harmonics.The class-E amplifier is realized from0.7to1.8GHz,and obtained the power added efficiency of72.5–77.5%.The maximum value of Power added efficiency(PAE)is79.7%with11-dBm input power at1.5GHz. The designed class-E amplifier using the proposed harmonic control network gained15.34%increment in PAE,and25.6%reduction in the circuit size in comparison with the conventional class-E amplifier.The simulation and measurement results show the validity of the proposed design procedure of the broadband class-E amplifier using a novel microstrip resonator cell.V C2013Wiley Periodicals,Inc.Microwave Opt Technol Lett55:1118–1118,2013;View this article online at .DOI10.1002/mop.27490Key words:switch mode;class-E amplifier;tapered cell;microstrip resonant cell;high efficiency;power added efficiency;zero voltage switching;zero voltage derivative switching1.INTRODUCTIONThe modern wireless communication systems need to consume the power supply.The main factor in reducing the consumption of the power supply is designing a low-voltage and high-effi-ciency power amplifier[1].The switch mode power amplifier is an efficient way for solving the efficiency problem.The class-E power amplifier is a kind of the switch mode power amplifier that the transistor acts as a switch.The class-E power amplifier is tuned by a shunt capacitance.This type of the power amplifier obtained100%drain efficiency theoretically[2].The class-E amplifier’s response conditions are zero voltage switching (ZVS)and zero voltage derivative switching(ZVDS),which lead to zero power loss in the transistor.Therefore,a high-effi-ciency power amplifier is obtained[3].The shunt capacitance in the class-E power amplifier has a main roll for achieving the class-E conditions[4].The power loss in the lower frequency can be neglected,but by increasing the operation frequency,the power dissipation is increased and the ideal operation of the class-E power amplifier will be missed.The antiphase of the voltage and current wave-forms throughout the signal period,obtain the class-E power amplifier with the maximum efficiency[5].This purpose can be achieved using a wave shaping network.The conventional class-E power amplifier load resistance is very much lower than the transistor ON-resistance.This effect leads to efficiency degrada-tion and a narrowband load matching network[6].Furthermore, the transistor parasitic resistance for both the switch on-state and parasitic inductance leads to efficiency degradation in the radio frequency(RF)and microwave applications[7,8].The optimum operation of the class-E power amplifier and the solution to the mentioned drawbacks can be obtained using two main methods:namely active device selection and circuit configuration[9].The class-E amplifier has various configura-tions such as the cascade[10]and push–pull[11].The cascade class-E configurations can double the maximum permissible drain voltage,and the push–pull class-E configuration increases the output power and decrease the harmonic distortion with high efficiency.A new topology for the class-E amplifier is proposed as an inverse class-E amplifier,which has inductive reactance [12].The inverse class-E amplifier has higher load resistance and lower peak switch voltage in comparison with the class-E amplifier.Also,because of the abruption of the device output inductances,the value of the inductance in the load network is decreased.However,the inverse class-E amplifier can be used only for the small to medium power applications.Therefore,to solve this drawback,the power combining methods have been used[13].Although,this method results in obtaining the inverse class-E amplifier for higher power application,but the circuit configuration and the design procedure are complicated with the circuit size increment because of using two power amplifier circuits.The class-E power amplifier is a high-efficiency power am-plifier for the microwave application,which is implemented using the transmission line as the harmonic control network at the output of the amplifier circuit[14].Furthermore,instead of the RF choke(RFC)a section of the transmission line is used.The transmission line has been used in the class-E power amplifier using LDMOS[15],GaN HEMT[16–19],SiC MES-FET[20],and LDMOSFET[21]as the harmonic control net-work increasingly,because of the simplicity of its structure and high rejection of harmonics.Therefore,the class-E amplifier configuration and operation are the best candidates for the design of the amplifier for the modern microwave communica-tion systems[22,23].Consequently,designing of the load network as the harmonic control network for suppression of harmonics in order to obtain a high-efficiency power amplifier is the main challenge of the switch mode power amplifiers.The designing of the class-E power amplifiers using various microstrip structures has been proposed such as a defected ground structure[24],an asymmet-rical spur-line[25],and composite right/left-handed transmission lines[26].The narrowband load network and low efficiency remain as the main challenge to the class-E power amplifier using the conventional microstrip transmission line[27].A compact microstrip resonant cell(CMRC)is a one-dimen-sional photonic band gap incorporating the microstrip transmis-sion line,which is,first,proposed in[28].The CMRC structure exhibits high rejection of the harmonics with the compact circuit size in comparison with the conventional micorstrip transmission lines.Therefore,it is used for the linearization and efficiency in-crement of the microwave power amplifiers[29,30].The appli-cation of the conventional CMRC is limited to obtain a high-ef-ficiency switch mode amplifier,as a result of the high insertion loss in the passband and restricted stopband.The front coupled tapered CMRC(FCTCMRC)is proposed in[31]for the implan-tation of a low-passfilter with high and wide rejection in the stopband with the compact circuit size in comparison with the conventional CMRC.Therefore,it can be widely used for designing the high-efficiency and broadband switch mode power amplifier because of high and wide suppression of harmonics.In this article,the harmonic suppression of the class-E ampli-fier using a novel FCTCMRC as the harmonic controller net-work is explored.A class-E amplifier with higher efficiency at a wider bandwidth in comparison with the conventional amplifiers is achieved.The proposed class-E power amplifier is designed and simulated for a frequency of1.5GHz using the micorstrip resonator structure.The measurement results of the proposed power amplifier validate our design procedure and simulation results.2.CLASS-E AMPLIFIER FUNDAMENTAL AND DESIGN THEORY2.1.Class-E Amplifier OperationThe basic circuit configuration of the class-E amplifier and switch waveforms are shown in Figures1(a)and1(b),respec-tively.The class-E amplifier consists of the switch device,shunt capacitance,series-tuned load network L-C,and an ideal RFC. The switch-on duty ratio is assumed to be50%in designing the class-E amplifier.This value of the duty ratio leads to optimum operation of the class-E amplifier for obtaining high efficiency [32].For an ideal class-E operation,three requirements for the drain voltage and current should be met[2]:1.The rise of the voltage across the transistor at turn-offshould be delayed until the transistor is off.2.The drain voltage should be brought back to zero at thetime of the transistor turn-on.3.The slope of the drain voltage should be zero at the timeof the transistor turn-on.Therefore,the class-E power amplifier is constructed based on two conditions as ZVS and ZVDS.These conditions are as follows:v s hðÞjh¼p¼0;(1)dv s hðÞd hh¼p¼0;(2)where v s(y)is the switch voltage,and y¼x t.The quality fac-tor of the output series resonant circuit is assumed infinite. Therefore,the output current is sinusoidal asi oðhÞ¼I m sinðhþuÞ:(3)In the time interval0y<p,the switch device is in the on-state,therefore,using Kirchhoff’s current law at the switch,we havei sðhÞ¼I dc1þa sin hþuðÞðÞ:(4)This is the currentflow through the shunt capacitance in the switch-off state.Therefore,the voltage across the switchisFigure1(a)The basic circuit of the class-E amplifier.(b)The class-E switch voltage and current waveformv sðtÞ¼1C sZ ti sðt0Þdt0¼I dcx C s1þa cos x tþuðÞÀcos uðÞðÞ:(5)Applying the class-E ZVS and ZVDS conditions to Eqs.(4)and (5),the value of a and u can be obtained asa¼ffiffiffiffiffiffiffiffiffiffiffiffiffi1þp24r;(6)u¼ÀtanÀ12p8>:9>;:(7)The drain voltage waveform is shaped by the harmonics so that the drain voltage and the slope of the drain voltage is zero when the transistor is in the on-state.The reactance for all harmonics is negative and comparable in magnitude to the fundamental fre-quency load resistance.The ideal class-E amplifier requirements are difficult to meet.So,we often only tuned the second and third harmonics to get the suboptimum class-E power amplifier solution.The analysis is performed considering just the output network behavior,thus neglecting input signal required to oper-ate the active device as an ideal switch.The optimal fundamental load by the Fourier-series expan-sion analysis in[7]used for achieving the perfect class-E opera-tion can be determined asZ E;f0¼0:28x C Pe49 :(8)This impedance is inductive.On the other hand,for the ideal operation of the class-E power amplifier the impedances at the higher order harmonics are infiniteZ E;fn¼1;for n!2:(9)From(8)the nominal class-E amplifier shunt capacitance C is defined byC¼0:1836x0R:(10)In order to achieve the maximum operation frequency of the class-E amplifier,the device output capacitance should be equal to Eq.(10).The matching network for the class-E power ampli-fier using a low-pass Chebyshev-form impedance transformer is proposed in[7].Therefore,the synthesis of the load network is done using a short circuit,and open circuit stubs instead of lumped capacitors in the load network for unwanted harmonics.2.2.Design of a Class-E Amplifier Using a pHEMTAchieving the optimum load is the main factor to obtain high efficiency when designing the class-E power amplifier.On the other hand,the optimum load is varied with the operating fre-quency as in Eq.(8).Therefore,designing of the load network, which can operate in the wide frequency range,is needed for designing the class-E power amplifier with the optimum condi-tions.The maximum operation frequency of the class-E power amplifier is restricted by the shunt capacitance.The shunt capac-itance consists of the transistor output capacitance and the exter-nal capacitance.Thus,the optimum operating frequency of the class-E power amplifier is achieved by selecting a transistor with lower output capacitance.On the other hand,the power loss is caused by ON-resistance of the transistor[33].Therefore, the active device with lower ON-resistance is preferred for designing the high-efficiency class-E power amplifier.We selected an ATF-34143pHEMT because of its lower ON-resist-ance and lower shunt parasitic capacitance,which provides lower power dissipation and optimum operation frequency using external capacitance,respectively.The circuit topology of the conventional class-E amplifier is shown in Figure2(a).It is designed using the design procedure,which is presented in[2, 3].The value of elements for an ideal class-E power amplifier is tabulated in Table1.In the design of the class-E power ampli-fier,it is assumed that the value of the DC-feed is infinitive,but in real implementation this value isfinite,and we used the half wavelength microstrip transmission line for the DC-feed.In the conventional class-E amplifier,using lumped elements, the second harmonic is located within the pass band.Therefore, the bandwidth is limited to one octave.In order to solve this drawback,one way is designing a multiple matching network for various bands and using switching element.This way leads to complexity of the amplifier circuit and degradation of the efficiency.The use of the micorstrip transmission line is a low-cost and simple way for designing the class-E amplifier with wide band and high-efficiency characteristics.We used the design proce-dure in Section2.1and designed the matching network for the amplifier as shown in Figure2(b).The values of the transmis-sion lines dimensions are given in Table2.The class-E ampli-fier is designed on RT/Duroid5880,a substrate with dielectric constant of2.2,height of15l l,and loss tangent of0.0009.Figure2Idealized class-E power amplifier:(a)lumped elements and(b)transmission lineTABLE1Element Design for the Nominal Class-E AmplifierC i1(pF)C i2(pF)C o1(pF)C o2(pF)C e(pF)C g1(pF)C g2(pF)C d1(pF)C d2(pF)L i1(nH)L o1(nH)L o2(nH) Theoretical10010010010 4.2221000.50.2312 4.7 3.33.FRONT COUPLED TAPERED CMRC CHARACTERISTICSA novel FCTCMRC is proposed in [31],for the first time,which is used to synthesize a low-pass filter with high and wide rejec-tion in the stopband.This microstrip structure exhibits bandstop characteristics and slow wave effects,which are used in the stopband extension and the circuit size reduction,respectively.The schematic and equivalent circuit of the resonator is shown in Figures 3(a)and 3(b),respectively.The proposed FCTCMRC has symmetrical topology.Therefore,the even–odd mode [34]can be used to simplify the analysis as shown in Figures 3(c)and 3(d).Consequently,theresonant condition for the odd-mode in Figure 3(c)is obtained by equating the input admittance Y o in of the proposed resonator to zero yields:Z 112x C 1ÀZ 1tan h 1 ÀZ 2tan h 2Z 1þtan h 12x C 1¼0:(11)Using the similar procedure,the even-mode resonant frequencies areobtained by equating the even admittance Y e in to zero as follows:Z 2tan h 1þZ 1tan h 2¼0:(12)The transmission zeros of the equivalent circuit for the proposed FCTCMRC,which is shown in Figure 3(a),is obtained whenY o in ¼Y ein asZ 2sin 2h 2þZ 1sin 2h 1¼cos 2h 1x C 1:(13)Therefore,the resonator characteristics for tuning transmission zeroes in the stopband can be achieved by the length and width of the tapered cells as shown in Figures 4(a)and 4(b).The pro-posed structure is optimized by an EM-simulator (ADS).The obtained dimensions are as follows:L t1¼2:58;L 2¼1:94;L 3¼2:7;W t1¼2:71;W t2¼5:6;W 1¼0:1;W 2¼0:56;L 3¼0:75;L f ¼2:36;W f ¼0:25all are in millimeter ðmm Þ:TABLE 2The Value of the Conventional Transmission Line for the class-E AmplifierTL 1TL 2TL b1TL 3TL 4TL 5TL b2Width (mm) 4.730.940.620.71 1.24 4.210.72Length (mm) 6.319.7262.3137.2318.4264.3Figure 3(a)Schematic of the proposed resonator.(b)Equivalent cir-cuit.(c)Odd-mode.(d)EvenmodeFigure 4(a)Changing of the transmission zeros with the width of tapered cell W t1.(b)Changing of the transmission zeros with the length of tapered cell L t .(c)Simulation and measurement results of the proposed harmonic control network.(d)Simulation input impedance of the FCTCMRCThe proposed FCTCMRC is fabricated,and the measurement is performed using an Agilent N5230A Network Analyzer.The simulation and measurement results of the proposed FCTCMRC are shown in Figure 4(c).As it is shown,it has an attenuation level À43and À33.1dB at 3.0and 4.5GHz,respectively.Therefore,the high suppression for the second and third har-monics is obtained.The insertion loss from DC to 2.39GHz is lower than À0.1dB.The simulation of the input impedance of the proposed CMRC for the fundamental and harmonics is shown in Figure 4(d).As it is observed,the harmonic impedan-ces are relatively open in comparison with the fundamental im-pedance.Consequently,it can be used as the matching network with high performance and low circuit complexity.4.CIRCUIT DESIGN AND IMPLEMENTATIONThe highly efficient and compact size class-E amplifier is designed and implemented for a 1.5-GHz band using an ATF-34143pHEMT.The proposed circuit is simulated using an Agi-lent’s Advanced Design System (ADS),and fabricated on an RT/Duroid 5880substrate.The active device is biased at V d ¼3V and V g ¼À0.7V.The FCTCMRC is used as the harmonic control network (HCN)at the output of the active device.The proposed HCN absorbed the parasitic reactance and capacitance of the active device.Therefore,it does not need to any lumped elements in series or parallel with the transistor to compensate the parasitic elements.The circuit schematic diagram of the designed class-E amplifier is shown in Figure 5(a).Moreover,the photograph of the fabricated circuit is shown in Figure 5(b).The RFC is realized using the microstrip transmission line (TLb2)with the quarter wavelength at a frequency of 1.5GHz.The input matching elements consist of two series and parallel open stubs.The dimensions of the tapered cells and transmission lines in the HCN are tuned in order to optimize harmonic termi-nation in the implemented amplifier circuit.The design and implementation of the output matching networks using the FCTCMRC as low-pass topology has been done from 0.7to 1.8GHz.The voltage and current waveforms of the designed class-E amplifier are shown in Figure 5(c).The switch is open for the time interval,0.2–0.4ns and the current through it is near zero.The switch is closed during the time interval 0.6–0.8ns,and the voltage across it is near to zero.The class-E ZVS and ZVDS conditions in the switch turn-off state are obtained.Therefore,the high-efficiency class-E amplifier is achieved.The input signal is generated using an Agilent E4433B signal generator,and the measurement is done by an E4440A PSA se-ries spectrum analyzer.The simulated and measured output power and gain for P in ¼11dBm (input power)are shown in Figure 6(a).The maximum output power at 1.5GHz with P in ¼11dBm is 25.3dBm,and the related gain is 14.3dB.The con-ventional class-E amplifier without CMRC has an output power of 18.5dBm and gain of 7.5dB.The class-E amplifier using CMRC has 36.7%output power improvement in comparison with the one without CMRC.The simulation and measurement results for the PAE at P in ¼11dBm (input power)is shown as a function of the operating frequency in Figure 6(b).The highest value of PAE at a fre-quency of 1.5GHz was 79.7%.The value of the PAE is 69.1%for the conventional class-E amplifier without CMRC.There-fore,the proposed class-E amplifier using the novel CMRC has 15.34%PAE improvement in comparison with the one without CMRC.The output power of the conventional class-E amplifier is decreased as the operating frequency is increased.As shown in Figure 6(a),this decrement is considerable when the operating frequency is more than 1.2GHz.Therefore,the conventional class-E amplifier has a drawback for the broadband applications.The designed class-E amplifier has 25.6%circuit size reduction in comparison with the conventional class-E amplifier.5.CONCLUSIONThe class-E amplifier with high efficiency and broadband char-acteristics has been designed and implemented.A novel and simple load-matching technique for the low-voltage microwave class-E amplifier using a front-coupled taperedcompactFigure 5The pHEMT class-E amplifier.(a)Circuit configuration.(b)A photograph of fabricated amplifier.(c)Simulated switch voltage and current waveforms.[Color figure can be viewed in the online issue,which is available at ]microcstrip resonant cell has been presented.The proposed am-plifier achieved an output power of 25.3dBm,a power added efficiency of 79.7%,and a gain of 7.5dB at input power of 11dBm.It has high-efficiency performance over a significant band-width form 0.7to 1.8GHz (88%).The proposed compact micro-strip resonant cell as the harmonic control network exhibited 15.34%improvement in PAE and 25.6%reduction in the circuit size in comparison with the conventional class-E amplifier.The extremely low insertion loss at the fundamental frequency and size reduction characteristics can be used in the design of the class-E amplifier with higher output power and smaller size,which are required in the broadband application.REFERENCES1.S.C.Cripps,Advanced techniques in RF power amplifiers design,Artech House,Norwood,MA,2002.2.N.O.Sokal and A.D.Sokal,Class E—A new class of high-effi-ciency tuned single-ended switching power amplifiers,IEEE J Sol-id-State Circuits 10(1975),168–176.3.F.H.Raab,Idealized operation of the class E tuned power ampli-fier,IEEE Trans Circuits Syst 25(1977),725–735.4.R.E.Zulinski and J.W.Steadman,Class E power amplifiers and frequency multipliers with finite DC-feed inductance,IEEE Trans Circuits Syst 34(1987),1074–1087.5.R.Negra,F.M.Ghannouchi,and W.Bachtold,Study and design optimization of multi-harmonic transmission-line load networks for class-E and class-F K-band MMIC power amplifiers,IEEE Trans Microwave Theory Tech 55(2007),1390–1397.6.K.L.R.Mertens and M.S.J.Steyaert,A 700-MHz 1-W fully differ-ential CMOS class-E power amplifier,IEEE J Solid-State Circuits 37(2002),137–141.7.T.B.Mader and Z.B.Popovic,The transmission line high-effi-ciency class-E amplifier,IEEE Microwave Guided Wave Lett 5(1995),290–292.8.T.Suetsugu and M.K.Kazimierczuk,Design procedure for lossless voltage-clamped class E amplifier with a transformer and a diode,IEEE Trans Power Electron 20(2005),56–64.9.H.J €a ger,A.V.Grebennikov,E.P.Heaney,and R.Weigel,Broad-band high-efficiency monolithic In-GaP/GaAs HBT power ampli-fiers for wireless applications,Int J RF Microwave Comput Aided Eng 13(2003),496–510.10.A.Mazzanti,rcher,R.Brama,and F.Svelto,Analysis of reli-ability and power efficiency in cascode class-E PAs,IEEE J Solid--State Circuits 41(2006),1222–1229.11.S.C.Wong and C.K.Tse,Design of symmetrical class-E poweramplifiers for very low harmonic-content applications,IEEE Trans Circuits Syst I,Reg Papers 52(2005),1684–1690.12.T.Mury and V.F.Fusco,Inverse class-E amplifier with transmis-sion line harmonic suppression,IEEE Trans Circuits Syst I,Reg.Papers 54(2007),1555–1561.13.T.Mury and V.F.Fusco,Power combining techniques into unbal-anced loads for class-e and inverse class-e amplifiers,IET Micro-wave Antennas Propag 2(2008),529–537.14.A.J.Wilkinson and J.K.A.Everard,Transmission-line load-networktopology for class-E power amplifiers,IEEE Trans Microwave Theory Tech 49(2001),1202–1210.15.J.Lee,S.Kim,J.Nam,J.Kim,I.Kim,and B.Kim,Highly effi-cient LDMOS power amplifier based on class-E topology,Micro-wave Optical Technol Lett 48(2006),789–791.16.Y.-S.Lee and Y.-H.Jeong,A high-efficiency class-E GaN HEMTpower amplifier for WCDMA applications,IEEE Microwave Wire-less Compon Lett 17(2007),622–624.17.H.G.Bae,R.Negra,S.Boumaiza,and F.M.Ghannouchi,High-ef-ficiency GaN class-E power amplifier with compact harmonic-sup-pression network,Proc 37th Europ Microwave Conf,2007,pp.1093–1096.18.Y.-S.Lee,M.-W.Lee,and Y.-H.Jeong,A 1-GHz GaN HEMTbased class-E power amplifier with 80%efficiency,Microwave Opt Technol Lett 50(2008),2989–2992.19.Y.-S.Lee,M.-W.Lee,and Y.-H.Jeong,A 40-W balanced GaNHEMT class-E power amplifier with 71%efficiency for WCDMA base station,Microwave Opt Technol Lett 51(2009),842–845.20.Y.S.Lee and Y.H.Jeong,A high-efficiency class-E power ampli-fier using SiC MESFET,Microwave Opt Technol Lett 49(2007),1447–1449.21.J.-H.Van,M.-S.Kim,S.-C.Jung,H.-C.Park,G.Ahn,C.-S.Park,B.-S.Kim,and Y.Yang,A high-frequency and high-power quasi-class-E amplifier design using a finite bias feed inductor,Micro-wave Opt Technol Lett 49(2007),1114–1118.22.R.Beltran,F.H.Raab,and A.Velazquez,High-efficiency out phas-ing transmitter using class-E power amplifiers and asymmetric combining,Microwave Opt Technol Lett 51(2009),2959–2963.23.C.Park,Y.Kim,H.Kim,and S.Hong,Fully integrated 1.9-GHzCMOS power amplifier for polar transmitter applications,Micro-wave Opt Technol Lett 48(2006),2053–2056.24.Y.C.Jeong,S.-G.Jeong,J.S.Lim,and S.W.Nam,A new methodto suppress harmonics using k /4bias line combined by defected ground structure in power amplifiers,IEEE Microwave Wireless Compon Lett 13(2003),538–540.25.L.Wang,W.Chen,P.Wang,X.Xue,J.Dong,and Z.Feng,Design of asymmetrical spur-line filter for a high power sic MES-FET class-E power amplifier,Microwave Opt Technol Lett 52(2010),1650–1652.26.M.Thian and V.Fusco,Design strategies for dual-band class-Epower amplifier using composite right/left-handed transmission lines,Microwave Opt Technol Lett 49(2007),2784–2788.27.Y.Qin,S.Gao,A.Sambell,and E.Korolkiewicz,Design of low-cost broadband class-e power amplifier using low-voltage supply,Microwave Opt Technol Lett 44(2005),103–106.28.Q.Xue,K.M.Shum,and C.H.Chan,Novel 1-D microstrip PBGcells,IEEE Microwave Wireless Comp Lett 10(2000),403–405.29.T.Yin,Q.Xue,and C.H.Chan,Amplifier linearization using com-pact microstrip resonant cell-theory and experiment,IEEE Trans Microwave Theory Tech 52(2004),927–934.Figure 6Comparison of the conventional amplifier simulation with the simulated and measured results of the proposed amplifier.(a)Output power and gain.(b)Power added efficiency (PAE %)。

ZVS三电平DCDC变换器的研究

ZVS三电平DCDC变换器的研究

华中科技大学硕士学位论文ZVS三电平DC/DC变换器的研究姓名:李小兵申请学位级别:硕士专业:电力电子与电力传动指导教师:李晓帆20060428摘 要直流变换器是电力电子变换器的重要组成部分,软开关技术是电力电子装置向高频化、高功率密度化发展的关键技术,成为现代电力电子技术研究的热点之一。

由于对电源设备电磁兼容的要求的提高,一般在电源设备中都要加入功率因数校正环节,导致后继开关管电压应力的提高。

三电平直流变换器相应提出,主开关管的电压应力为输入直流电压的一半。

使得三电平直流变换器一提出就得到全世界电源专家和学者的重视,短短十几年内,相继提出许多种改进型三电平直流变换器,包括半桥式和全桥式。

根据主开关管实现软开关的不同,将三电平直流变换器分为零电压软开关和零电压零电流软开关。

本文首先给出了基本半桥式三电平DC/DC变换器,详细分析了其工作原理,讨论了主要参数的设计和由于次级整流二极管的反向恢复导致主开关管的电压尖峰。

接着给出一种带箝位二极管的改进型半桥式三电平DC/DC变换器。

文中给出了Saber软件的仿真结果,进一步证明改进方案的正确性和可行性。

针对前面讨论的两种半桥式三电平DC/DC变换器,设计了实验电路来验证理论分析的正确性,文中给出了实验结果。

接着研究了一种新型ZVS三电平LLC谐振型DC/DC变换器,文中详细讨论了该变换器的工作原理,讨论了主要参数的设计过程,给出了仿真结果。

最后,设计了一台实验装置来验证理论分析的正确性,给出了实验结果,说明了主开关管可以在全负载范围内实现零电压软开关,变换器的效率在输入电压高端较高,并且次级整流二极管实现了零电流开关,二极管电压应力为输出电压的2倍。

本文通过理论分析、仿真研究和实验验证,证实了半桥式三电平DC/DC变换器的优越性能,改进型的半桥式三电平DC/DC变换器比较好地消除了主开关管上的电压尖峰。

ZVS三电平LLC谐振型DC/DC变换器良好的性能,使得在有掉电维持时间限制的场合得到广泛应用。

Switching Power Supply Design ( phase shuft )

Switching Power Supply Design ( phase shuft )

• Q1-Q2 leg sets tmax limit for transition at light load • This leg has mostly resonant transition
t3~t4
t4~t5
t5~t6
ZVS design
Resonant frequency:
Dead Time:
Resonant Capacitance:
Energy in Cr: Resonant inductance: Energy in Lr: ZVS condition:
Lr
UCC3895 Block Diagram
Zero-voltage switching of each halfbridge section
Each half-bridge produces a square wave voltage. Phase-shifted control of converter output
A popular converter for server frontend power systems Efficiencies of 90% to 95% regularly attained
Full-Bridge Phase Shift
• Topology similar to conventional hardswitched design
– shim inductor usually needed to extend ZVS range – duty cycle modified by current transitions – circuit parasitics more critical yet more useful

Zero-Voltage and Zero-Current-Switching Full-Bridge PWM Converter Using

Zero-Voltage and Zero-Current-Switching Full-Bridge PWM Converter Using

Zero-V oltage and Zero-Current-Switching Full-Bridge PWM Converter UsingSecondary Active Clamp Jung-Goo Cho,Member,IEEE,Chang-Yong Jeong,and Fred C.Y.Lee,Fellow,IEEEAbstract—A new zero-voltage and zero-current-switching (ZVZCS)full-bridge(FB)pulsewidth modulation(PWM) converter is proposed to improve the performance of the previously presented ZVZCS FB PWM converters.By adding a secondary active clamp and controlling the clamp switch moderately,ZVS(for leading-leg switches)and ZCS(for lagging-leg switches)are achieved without adding any lossy components or the saturable reactor.Many advantages including simple circuit topology,high efficiency,and low cost make the new converter attractive for high-voltage and high-power(>10 kW)applications.The principle of operation is explained and analyzed.The features and design considerations of the new converter are also illustrated and verified on a1.8-kW100-kHz insulated gate bipolar transistor(IGBT)-based experimental circuit.Index Terms—DC–DC power conversion.I.I NTRODUCTIONI NSULATED gate bipolar transistors(IGBT’s)are widelyused in switching power conversion applications because of their distinctive advantages such as easiness in drive and high-frequency switching capability.The performance of IGBT’s has been continuously improved,and the latest IGBT’s can be operated at10–20kHz without including any snubber circuit. Moreover,IGBT’s are replacing MOSFET’s for the several or several tens of kilowatts power range applications since IGBT’s can handle higher voltage and power with higher power density and lower cost compared to MOSFET’s.The maximum operating frequency of IGBT’s,however,is limited to20–30kHz[1]because of their tail-current characteristic. To operate IGBT’s at high switching frequencies,it is required to reduce the turn-off switching loss.Zero-voltage switching (ZVS)with a substantial external snubber capacitor or zero-current switching(ZCS)can be a solution.The ZCS,however, is deemed more effective since the minority carrier is swept out before turning off[6].ZVS full-bridge(FB)pulsewidth modulation(PWM)con-verters have received considerable attention in recent years [2]–[5].This converter is controlled by a phase-shifted PWMManuscript received July18,1996;revised October14,1997.Recom-mended by Associate Editor,L.Xu.J.-G.Cho and C.-Y.Jeong are with the Power Electronics Research Division,Korea Electrotechnology Research Institute,Changwon641-120, Korea(e-mail:jgcho@keri.re.kr).F. C.Y.Lee is with the Virginia Power Electronics Center,Virginia Polytechnic Institute and State University,Blacksburg,V A24061USA. Publisher Item Identifier S0885-8993(98)04842-X.technique which enables the use of all parasitic elements in the bridge to provide ZVS conditions for the switches.Distinctive advantages including ZVS with no additional components, and low-device voltage/current stresses make it very attractive for high-frequency high-power applications,where MOSFET’s are predominantly used as the power switches.The IGBT’s, however,are not suited for the ZVS FB PWM converter because the ZVS range is quite limited unless the leakage inductance is very large.In addition,several demerits such as duty-cycle loss and parasitic ringing in the secondary limit the maximum power rating of the converter.To apply IGBT’s for a high-frequency converter,a ZVZCS FB PWM converter was presented[7].IGBT’s with no an-tiparallel diodes are used for all primary switches.During the freewheeling period,the primary current is reset by us-ing reverse avalanche-breakdown voltage of the leading-leg IGBT’s,which provides ZCS condition to lagging-leg IGBT’s. However,it has some drawbacks as follows.The stored energy in the leakage inductance is completely dissipated in the leading-leg IGBT’s.There is parasitic ringing in the primary during the freewheeling period.The maximum controllable duty cycle is limited since the reverse avalanche-breakdown voltage is low(15–30V)andfixed.Therefore,the overall efficiency will be deteriorated unless the leakage inductance is very low.Another approach for ZVZCS FB PWM converter was presented[8].By utilizing a dc blocking capacitor and adding a saturable inductor in the primary,the primary current during the freewheeling period is reset,which provides ZCS condi-tion to the lagging-leg switches.Meanwhile,the leading-leg switches are still operated with ZVS.The stored energy in the leakage inductance is recovered to the dc blocking capacitor andfinally transferred to the load.By increasing the blocking capacitor voltage(i.e.,by reducing the capacitance of the blocking capacitor),wide duty-cycle control range is attainable even when the leakage inductance is relatively large.This converter can be effectively applied to several kilowatts power range applications.Some demerits including loss in saturable inductor and its cooling problem hinder further increase of the power level above10kW.This paper proposes a novel ZVZCS FB PWM converter (see Fig.1)to improve the performance of the previously presented ZVZCS FB PWM converters[7],[8].The ZVS mechanism of leading-leg switches is the same as that of the converters[2]–[5],[8].The ZCS of lagging-leg switches,how-0885–8993/98$10.00©1998IEEEFig.1.Circuit topology of the proposed ZVZCS FB PWM converter.ever,is achieved by adding an active clamp in the secondaryrectifier and by controlling it moderately.No lossy componentsare added to achieve ZVZCS operation.The duty-cycle loss isalmost negligible although the leakage inductance is a little bitlarge since a high voltage(higher than input voltage)is appliedto the leakage inductance to reset the primary current duringfreewheeling period.So,the new converter overcomes mostof the limitations of the soft-switching FB PWM converters,which makes the new converter very attractive for high-voltage high-power((2)This mode ends when(3)CHO et al.:FULL-BRIDGE PWM CONVERTER USING SECONDARY ACTIVE CLAMP603Fig.3.Operation waveforms.C.Mode3According to the given dutycycle,,and.The rectifier voltage is still zero.This is the end ofan operating half cycle.III.F EATURES OF THE P ROPOSED C ONVERTERA.Effective Soft Switching(ZVZCS)Soft-switching mechanism(ZVS for leading-leg switchesand ZCS for lagging-leg switches)of the proposed converterhas exactly the same as those of the ZVZCS converterspresented in[7]and[8].The converters[7],[8]use lossycomponents to achieve ZCS of lagging-leg switches.Thestored energy in the leakage inductance is completely dissi-pated in the leading-leg IGBT’s during freewheeling mode[7]or there exists the core loss of saturable reactor[8].In addition,additional loss exists in the clamp resistor forboth converters if the passive clamp circuit is used to clampthe secondary rectifier voltage.Therefore,both convertershave limited power range(several kilowatts).In the proposedconverter,however,ZCS of lagging-leg switches is achievedmore efficiently by modifying control of the active clamp[3].No lossy components are involved in achieving ZCS,and noparasitic ringing is generated in the secondary rectifier.So,theproposed converter can handle a higher power level(duringfreewheeling period asfollows:604IEEE TRANSACTIONS ON POWER ELECTRONICS,VOL.13,NO.4,JULY1998(a)(b)(c)parison of the simplified waveforms of primary voltages and currents and secondary rectifier voltages.(a)ZVS PWM converter.(b)ZVZCS PWM converters [7],[8].(c)Proposed converter.is applied to the leakage inductance,which is a kind of duty-cycle loss.In the proposed ZVZCS converter,however,asmallis achieved since the high reversevoltage is applied to the leakage inductance.So,the overall efficiency of the proposed converter is improved due to low duty-cycleloss as well assmall .C.Duty-Cycle Boost EffectThe duty cycle of the secondary rectifier is usually lowerthan that of the primary because of the duty-cycle loss.In the proposed converter,however,the duty cycle of the rectifier can be higher than that of the primary as shown in Fig.5.This phenomenon is named as duty-cycle boost effect .The duty-cycle boost effect is caused by the operation of the active clamp from the beginning of freewheeling period to provide ZCS condition to the lagging-leg switches.This means that the stored energy in the leakage inductance is recovered to the clamp capacitor and finally transferred to the load by means of the duty-cycle boost effect.This feature is very important for the ZVZCS converters,which use IGBT’s for main switches.The duty cycle of the primary is more limited than MOSFET-based ZVS converters since the minimum dead time((6)whereis determined directly by the turn-on time of the clamp switch.The duty-cycle boost effect also helps to improve the overall efficiency.IV.D ESIGN C ONSIDERATIONSA.Decision of Dead TimesAn appropriate dead time is required for both leading-and lagging-leg switches to achieve maximum performance.1)Dead Time for Leading-Leg Switches:The dead time for leading-leg switches is determined by two factors—the ZVS range and maximum duty cycle of the primary side.The minimum dead time is determined by ZVS range asfollows:(8)wheretheCHO et al.:FULL-BRIDGE PWM CONVERTER USING SECONDARY ACTIVE CLAMP605Fig.6.Illustrative waveforms of the rectifier voltage and the clamp capacitorcurrent.Fig.7.Circuit diagram of the active clamp circuit for a center-tappedtransformer.required turn-on time ofs.The primary current isquickly reset right after the primary voltage is dropped to zeroand sustained during the freewheeling period.The primary cur-rent reset time is only0.15606IEEE TRANSACTIONS ON POWER ELECTRONICS,VOL.13,NO.4,JULY1998(a)(b)Fig.10.Extended waveforms at (a)leading-leg and (b)lagging-leg switchingtransitions.(a)(b)Fig.11.Extended ZVS switching waveforms of leading-leg switches:(a)turn on and (b)turnoff.Fig.12.Extended ZCS waveforms of lagging-leg switches.waveforms of leading-leg switches.It can be seen that the antiparallel diode current flows for a short time and stays zero,and,thus,a complete ZVS turn on is achieved.The tail current is seen,but the turn-off switching loss is remarkably reduced comparing to hard switching since the rising slope of the switch voltage is slow.The ZVS range for the leading-leg switches is about 20%of full load.Fig.12shows theextended Fig.13.Waveforms of secondary active clamp.switching waveforms of lagging-leg switches.It can be seen that a complete ZCS turn off is achieved since the primary current is zero during the whole freewheeling period and the turn-on process of the other switch is almost ZCS.Small pulse current during turn-on transition is the charging current of the switch output capacitor.Fig.13shows the waveforms of the secondary active clamp.The clamp switch is turned on for aCHO et al.:FULL-BRIDGE PWM CONVERTER USING SECONDARY ACTIVE CLAMP607Fig.14.Measured efficiencies.very short time compared to the operating period(7%).The rectifier voltage waveform is a little noisy since the clamp switch operates under hard switching.The clamp capacitor current waveform is the same as the expected.Fig.14shows the measured efficiencies of the proposed ZVZCS FB PWM converter.The maximum overall efficiency is about94%at full load.The efficiency improvement is not much comparing to the previous ZVZCS converter[8],but it will be considerable at higher power(10kW)applications with high-power density.R EFERENCES[1]IGBT Designer’s Manual,International Rectifier,El Segundo,CA,1994.[2]J.A.Sabate,V.Vlatkovic,R.B.Ridley,F.C.Lee,and B.H.Cho,“Design considerations for high-voltage high-power full-bridge zero-voltage-switched PWM converter,”in IEEE APEC Rec.,1990,pp.275–284.[3],“High voltage high power ZVS full bridge PWM converteremploying active snubber,”in IEEE APEC Rec.,1991,pp.158–163.[4]R.Redl,N.O.Sokal,and L.Balogh,“A novel soft switching fullbridge dc/dc converter:Analysis,design considerations,and experi-mental results at1.5kW,100kHz,”in IEEE PESC Rec.,1990,pp.162–172.[5] A.W.Lotfi,Q.Chen,and F.C.Lee,“A nonlinear optimization tool forthe full bridge zero-voltage-switched PWM dc/dc converter,”in IEEE APEC Rec.,1992,pp.1301–1309.[6]G.Hua,E.X.Yang,Y.Jiang,and F.C.Lee,“Novel zero-current-transition PWM converters,”in IEEE PESC Rec.,1993,pp.538–544.[7]K.Chen and T.A.Stuart,“1.6kW,110kHz dc/dc converter optimizedfor IGBT’s,”IEEE Trans.Power Electron.,vol.8,no.1,pp.18–25, 1993.[8]J.G.Cho,J.Sabate,G.Hua,and F. C.Lee,“Zero voltage andzero current switching full bridge PWM converter for high power applications,”in IEEE PESC Rec.,1994,pp.102–108.Jung-Goo Cho(S’89–M’91)received the M.S.andPh.D.degrees in electrical engineering from theKorea Advanced Institute of Science and Technol-ogy(KAIST),Daejon,Korea,in1988and1992,respectively.Since1992,he has been with KAIST for one anda half years as a Post-Doctoral Fellow,where heparticipated in the development of a1-MV A mul-tilevel GTO inverter for an induction motor drive.From1993to1994,he was with the Virginia PowerElectronics Center(VPEC),Virginia Polytechnic Institute and State University,as a Visiting Research Scientist,where he studied soft-switching PWM converters and power-factor-correction circuits. Since1995,he has been with the Power Electronics Research Division, Korea Electrotechnology Research Institute(KERI),Changwon,Korea,as a Senior Researcher.His primary areas of research interests include:soft-switching converters,power-factor-correction circuits,high-power multilevel GTO inverters,high-voltage pulse power supplies,activefilters,and FACTS. Dr.Cho is a Member of KIEE andKITE.Chang-Yong Jeong received the B.S.degree fromKyungpook National University,Taegu,Korea,in1993and the M.S.degree in electrical engineeringfrom the Korea Advanced Institute of Science andTechnology(KAIST),Daejon,Korea,in1995.Since1995,he has been with the Power Elec-tronics Research Division,Korea ElectrotechnologyResearch Institute(KERI),Changwon,Korea,as aResearcher.His primary areas of research interestsinclude:activefilters,FACTS and applications ofhigh-power inverters,power circuit modeling,and data-acquisitionsystems.Fred C.Y.Lee(S’72–M’74–SM’87–F’90)receivedthe B.S.degree in electrical engineering from theNational Cheng Kung University,Taiwan,in1968and the M.S.and Ph.D.degrees from Duke Univer-sity,Durham,NC,in1971and1974,respectively.He is the Lewis A.Hester Chair of Engineering atVirginia Polytechnic Institute and State University,Blacksburg,and was the James S.Tucker EndowedProfessor at the Bradley Department of ElectricalEngineering at Virginia Polytechnic Institute andState University.He is the Founder and Director of the Virginia Power Electronics Center(VPEC),a Technology Development Center of Virginia’s Center for Innovative Technology(CIT).Under his leadership,VPEC has become one of the largest university-based power electronics research centers in the country.The Center’s Industry Partnership Program has enrolled more than70companies from around the world.His research interests include:high-frequency power conversion,distributed power systems,space power systems,device characterization,and modeling and control of converters and design optimization.During his career,he has published over100refereed journal papers,more than200technical papers in national and international conferences,and over150industry and government reports.He currently holds19U.S.patents.Dr.Lee is a recipient of the1985Ralph R.Teeter Educational Award of the Society of Automotive Engineering,the1989William E.Newell Power Electronics Award of the IEEE Power Electronics Society,the1990PCIM Award for Leadership in Power Electronics Education,and the1990Virginia Tech Alumni Award for Research Excellence.He is a Past President of the Power Electronics Society.。

ZVS零电压开关电路原理与设计

ZVS零电压开关电路原理与设计

ZVS零电压开关电路原理与设计一、初识ZVSZVS是什么,度娘查的为”零电压开关(Zero Voltage Switch)“。

即开关管关断时,开关管导通时,其两端的电压已经为0。

这样开关管的开关损耗可以降到最低。

我们平时使用的电磁炉和LLC电源都是这种谐振电源,普通的充电器等都是硬开关的,比这种谐振电源损耗要大些。

所以ZVS可以做到很高效率,但是有一个缺点,就是其调节范围一般都比较窄。

例如电磁炉,当我们把功率调到比较大时,为持续加热;当功率调的较小时,就开始断断续续加热,因为那个时候已经不能达到谐振状态了。

像我们普通充电器那种硬开关的电源,不管空载和满载都是持续震荡的。

初次看到ZVS电路,我惊呆了,两个MOS管加几个电阻电容就能组成谐振开关。

真是佩服人民的想象力啊。

该电路只需要少量元件即可达到零电压开关。

功率有人做到2KW以上,几百瓦的话两个开关管只需加小型散热器即可。

于是花了几天时间对ZVS电路进行了下深入研究,让大家明白其工作原理。

一、基本电路现在我们来进行分析其原理,首先使用proteus仿真电路进行仿真。

二、原理图分析1. 上电时L1通入的电流为零,电源通过R1、R2是Q1、Q 2导通,L1电流逐渐增加,由于两个开关管特性差异,将导致流入两个开关管的电流不同,假设Q1电流大于Q2电流,T1将产生b为正,a为负的感应电压,于是通过T1形成正反馈,使Q1导通,Q2截止。

完成启动过程。

2. (t0~t1时间)稳态Q1导通时,由于上个周期T1电流为a到c,并且C 1两端电压为零。

由于电流不能突变,T1电流将对C1充电,C1逐渐为a负c正的电压,并且正弦变大,T1电流正弦变小。

此时a电压被Q1下拉到0V,所以C点电压正弦变大,Q1栅极电压被D3稳压管钳位,Q1时钟保持导通。

3. (t1时间)当T1中电流下降为零,其能量全部释放到C1,此时C1电压达到最大值。

4. (t1~t2时间)C1开始通过T1由c到a放电,C1电压即c点电压正弦变小,T1电流由c到a正弦变大。

NORMA 4000 5000 Power Analyzer 用户说明手册说明书

NORMA 4000 5000 Power Analyzer 用户说明手册说明书

Since some countries or states do not allow limitation of the term of an implied warranty, or exclusion or limitation of incidental or consequential damages, the limitations and exclusions of this warranty may not apply to every buyer. If any provision of this Warranty is held invalid or unenforceable by a court or other decision-maker of competent jurisdiction, such holding will not affect the validity or enforceability of any other provision.
BEGRENZTE GEWÄHRLEISTUNG UND HAFTUNGSBESCHRÄNKUNG
Fluke gewährleistet, daß jedes Fluke-Produkt unter normalem Gebrauch und Service frei von Material- und Fertigungsdefekten ist. Die Garantiedauer beträgt 2 Jahre ab Versanddatum. Die Garantiedauer für Teile, Produktreparaturen und Service beträgt 90 Tage. Diese Garantie wird ausschließlich dem Erster

AHB 直流变换器的 ZVS 原理分析与控制

AHB 直流变换器的 ZVS 原理分析与控制

AHB 直流变换器的ZVS 原理分析与控制Z"#$%&’(&$)*+’,)-.&.,’/01’2%1)31%+456076001’8*%2*%张友军(苏州大学机电工程学院,苏州215021)摘要针对一种小功率的不对称半桥AHB 直流变换器。

利用其变压器励磁电流实现开关管零电压开关ZVS ,采用同步整流控制和突发模式控制技术,可以有效地提高变频器的效率和减少待机功耗。

关键词变换器零电压开关同步整流突发模式控制待机功率AbstractFor a kind of Asymmetrical Half Bridge(AHB )DC/DC converter ,the operation principle and its control method are analyzed and studied in this pa-per.By using the magnetizing current of the transformer ,Zero Voltage Switching(ZVS )is realized for the switches of the converter ,which suits low power situ-ation.A 150W prototype was manufactured.Its experiment and test results show that the efficiency can be improved and the standby power loss decreased by adopting synchronous rectifying and burst mode control.Keywords ConverterZero Voltage Switching (ZVS )Synchronous rectifyingBurst mode controlStandby power0引言各种电子电子变换器在对电能进行处理的时候,存在多种能量损耗。

海尔电子洗衣机产品说明书

海尔电子洗衣机产品说明书

Section 6: Parts DataDC50X264310131211216547Cabinet GroupKey Part Number Description Quantity * 9960-285-008Door Assy., Loading Complete-Wht (2)* 9960-285-011Door Assy., Loading Complete-SS (2)* 9960-285-007Door Assy., Loading Complete-Chrome/BLK/SS (2)1 9960-284-002Door Assy., Loading-SS(ring only) (2)1 9960-284-004Door Assy., Loading-Chrome(ring only) (2)2 9982-353-002Plate Assy., Hinge (Wht) No Pin (2)2 9982-353-001Plate Assy., Hinge (SS) No Pin (2)* 9545-012-015Screw, Hinge to Door (8)* 8640-413-002Nut, Hinge to Door (8)3 9212-002-004Glass, Door (2)4 9206-413-002Gasket, Glass Black (2)* 9548-117-000Support, Door Glass (2)5 9206-420-005Gasket, Outer Rim Black (2)6 9244-082-001Handle, Loading Door (2)* 9545-018-017Screw, Handle 1/4-20 x 3/8 (4)* 9531-033-003Stud, Door Catch (2)* 8640-413-001Nut, Hex (2)* 8640-413-003Nut, Acorn (2)* 9086-015-002Catch, Loading Door (2)* 8638-190-009Pop Rivet for mtg. catch (4)* 8641-582-006Lockwasher (4)* 8640-399-001Spring Nut (6)7 9989-521-003Panel Assy., Front- Lower (Wht) (1)7 9989-521-001Panel Assy., Front- Lower (SS) (1)8 9989-517-003Panel Assy., Front- Upper (Wht) (1)8 9989-517-001Panel Assy., Front- Upper (SS) (1)* 9277-054-001Insulation Front Panel, half moon (top) (2)* 9277-054-002Insulation Front Panel, half moon (bottom) (2)9 9545-008-014Screw, FLHDCR, 10B x 1 (14) (6)* 8641-585-001 Lockwasher* 8640-399-001Nut, Spring (12)10 9544-069-002Strap, Hinge (Wht) (2)10 9544-069-005Strap, Hinge (SS/Black) (2)* 9545-012-028Screw, Hinge to Panel (8)11 9545-052-001Screw, Door to Hinge Strap (Special Black Type) (2)12 8641-436-003Washer, Fiber (2)13 9021-041-001Acceptor, Coin (1)* 9486-149-001Retainer, Coin Acceptor (2)14 9545-053-002Screw (4)* 9801-099-001Switch, Optical (1)Cabinet Group ContinuedKey Part Number Description Quantity15 9994-032-001Escutcheon, Upper (1)16 9435-039-002Trim, Overlay-Upper Blue (1)16 9435-039-001 Trim, Overlay-Upper Black (1)17 9994-033-001Escutcheon, Lower (1)18 9435-023-001Trim, Overlay-Lower Blue (1)18 9435-031-001Trim, Overlay-Lower Black (1)* 9545-020-009Screw (20)19 9412-167-002Nameplate Stack Dryer Express Blue (1)19 9412-167-001Nameplate Stack Dryer Express Black (1)20 9866-005-001Lint Drawer Assembly Blue (2)20 9866-005-004Lint Drawer Assembly Black (2)21 9435-024-001Overlay Trim, Lint Drwr-Blue (1)21 9435-032-001Overlay Trim, Lint Drwr-Black (1)* 9532-074-003Felt Seal ( back of lint screen assembly ) (2)* 9805-033-002Lint Screen Assembly ONLY (no front) (2)* 9555-057-008Replaceable Lint Screen Only (2)22 8650-012-004Lock and Key, Lint Drawer (2)* 6292-006-010Key 6101 only (2)* 9095-043-001Cam, Lock (2)* 9545-008-001Lint Screen Strap Hold Down Screws 10Bx 1/4 (32)23 9857-198-001Controls Assy, Blue (1)23 9857-198-003Controls Assy, Black (1)* 9627-869-001Harness, Electronic Control (1)24 8650-012-003Lock and Key, Control (1)* 9095-041-001Cam, Lock (1)* 6292-006-007Key only 6324 (1)* 9627-855-003Harness, Heat Sensor (1)* 8640-276-002Wire Nut Connector Grey (4)25 9501-004-003Sensor Temp Control (2)26 9501-008-001Bracket for Heat Sensor Mounting (Under Basket) w/ sensor..2* 9545-045-005Screw, Round Head (Mounts sensor; phillips head) (2)* 9209-037-002Gromm.et, 3/16 ID (2)* 8544-006-001Leg, Leveling 1/2” (4)* 9074-320-001 Cover, Cabinet (Top) (1)* 9277-041-017 Insulation Cabinet Cover (1)* 9732-276-001Kit for Dryers without Neutral and using 208-240 volt (1)* 9732-102-013LP Kit for 50Lb Stk Dryers (1)* 9732-243-001Stack Dryer Trunion Puller (1)* 9544-041-002 Strap - Bead Tie (1)27 9942-038-005 Vault, Coin Box (1)* 9545-008-024 Screws, Mounting-Coin Vault (2)28 9897-099-002 Coin Box Assy, Large Blue (1)28 9807-099-004 Coin Box Assy, Large Black (1)191526252792531089Control Parts GroupKey Part Number Description Quantity * 9857-198-001Controls Assy, Electronic Mounted With Membrane Switch, BLU (1)* 9857-198-003Controls Assy, Electronic Mounted With Membrane Switch, BLK (1)1 9826-008-001 Trough Assembly (1)2 9032-062-002 Button-Push, Control, Blue (2)2 9032-062-001 Button-Push, Control, Black (2)3 9538-166-011Spacer-Metal, 4mm (4)4 9486-158-001 Retainer-Push Button (2)5 8640-424-002Nut-Hex, Elastic stop, #4-40 (4)6 8652-130-038Terminal-Grounding clip (1)7 9534-365-001Spring-Flat, Control (1)8 9545-008-001Screw-Hex, #10B x 1/4 (2)9 9545-044-010 Screw-Hex, #10B x 1/4 (10)9 8641-582-005Washer-External tooth, #6 (10)10 9435-038-001Overlay-Control, Coin, Black (1)10 9435-038-002Overlay-Control, Coin, Blue (1)11 9021-041-001Acceptor-Coin, Optical (1)* 9486-149-001Retainer, Coin Acceptor (1)12 9545-053-002Screw (4)* 9801-099-001 Optical Sensor, Replacement (1)Note: Jumpers required if using 1.5 Control on Older Machines (P9 Connection)* 8220-155-001 Wire Assy, Jumper, 30Lb Stack Coin (1)* 8220-155-002 Wire Assy, Jumper, 50Lb Stack Coin (1)Door Switch GroupPart NumberDescription Quantity9539-487-001Door Switches (2)Hinge Plate Cover1 9074-340-002 Cover-Hinge, Black .....................................................................22 8636-008-010 Screw-TRHDCR, 10B x 3/8, Black.. (4)12Bearing Housing GroupKey Part Number Description Quantity J1 9241-189-002 Housing, Bearing (2)J2 9036-159-003Bearing, Ball Rear..................................................................... .2 * 9538-183-001 Spacer, Bearing (2)* 9036-159-001Bearing, Ball Front .................................................................... .2 J5 9545-017-017Bolt, 1/2 x 3/4 . (8)J7 8640-417-002Nut, 1/2 (8)* 9803-201-001Bearing Housing Complete Ass’y (includes bearings,spacer) (2)J4 9545-017-018Screw 1/2 x 1 1/2 (4)Burner Housing GroupKey Part Number Description Quantity * 9803-207-001 Housing Assembly, Burner (2)1a 9452-730-001Service Burner Plate Front... (2)1 9452-729-001 Service Plate baffl e Recirculation Chamber Clean Out (2)* 9545-008-006Screws (8)2 9545-008-001Screw (16)18 9003-220-001Angle, Burner Support (2)* 9545-008-006Screw (4)17 9048-020-002Burner, Main (4)* 9545-008-006Screw 10AB x 3/8” (4)* 9454-824-001 Panel, Back Burner Housing (2)4 9545-008-001Screw 10B x1/4” (8)5 9875-002-003Electrode Assy, Ignition (2)19 9545-045-001Screw, Electrode Mtg 8B x 1/4” (4)7 9379-186-001Valve, Gas Shut Off (1)8 9857-134-001Control Assy, Gas (2)9 9381-012-001Manifold, Assy (2)* 9425-069-021Orifi ce, Burner-Natural #27 (4)* 9425-069-022Orifi ce, Burner-LP #44 (4)10 9029-175-001Bracket, Manifold (2)22 8615-104-038Pipe Plug in end of Burner Manifold (2)* 9545-008-006Screw (4)12 9576-203-002Thermostat, Hi-Limit (2)* 9538-142-001Spacer, Hi-Limit (4)* 9545-045-007 Screw 8B x 3/4” (4)13 9074-329-001Cover, Hi-Limit Stat Ignitor (2)* 9545-008-006Screw (6)* 9576-207-008Thermostat, Safety Shutoff (2)* 9545-008-006Screw (4)15 9825-062-001Cover, Safety Stat (2)* 9545-008-024Screw (6)16 9857-116-003Control, Ignition Fenwall (3 trybox) (2)* 9732-102-013Kit, LP Conversion 50Lb Stack Kit (2)* 9838-018-003Welded One Piece Gas Pipe Assembly (1)Part # 8533-085-001 9/14Burner Housing Group Photos10221092221851A141594851613Rear ViewKey Part Number Description Quantity * 9627-861-001Wire Harness Overtemperature Switch/Air Switch (2)* 9801-098-001Switch Assy, Air Flow (2)1 9539-461-009Switch, Air Flow (2)2 9029-200-001 Bracket, Switch- Air Flow (2)3 9008-007-001Actuator, Switch (2)4 9451-169-002Pin, Cotter (2)5 9545-020-001Screw 4-40 x 5/8” (4)* 8640-401-001Nut, Special Twin .#4-40 (2)* 9550-169-003Shield, Switch (2)6 9376-322-001Motor, Drive (2)7 9452-770-001Plate, Motor Mounting (1)* 9545-029-008Bolt 3/8” - 16 x 3/4” (8)* 8641-582-003Lockwash Spring 3/8 (8)8 9545-018-019Screw, Motor Plate to Back Assy. 1/4-20x 2 1/2 (8)* 8641-582-007Lockwasher 1/4 (8)9 9538-163-006Spacr (8)* 8641-581-017Flat Washer 1/4 x 7/8 (24)* 9209-086-002Rubber Grommet (8)* 9538-166-006Grommet Spacers (8)* 9545-028-013Screw, Set (4)10 9962-018-002Back Assy, Blower Hsg (2)11 9991-053-001Support Assy, Intermed. Pulley (2)12 9545-029-010Bolt, Rd Hd 3/8-16 x 1 1/4 (6)12 8640-415-004Nut Flange Wizlock 3/8” - 16 (6)12 8641-581-035Washer, Flat (6)13 9545-029-003Bolt, 3/8-16 x 1 1/2 (2)14 9861-022-001Arm Assy-Tension, Complete (2)* 9487-200-003Ring-Retaining (6)15 9908-048-003Pulley Assy, Intermediate with bronze fl ange bearing (2)* 9036-145-002Bronze Flange Bearing (4)16 9908-047-002Pulley Driven Tumbler (2)17 9040-076-009Belt, Drive Motor (2)18 9040-073-011Belt, Driven Intermediate to Tumbler (2)19 9534-151-000Spring, Tension (2)20 9099-012-005Chain, Tension (2)21 9248-022-002Hook, Tension (2)* 9451-146-001Pin, Damper Hinge (2)* 9074-334-001 Cover Duct Upper (1)22 9973-032-001 Heat Recirculation Assembly Duct (2)* 9453-169-013Motor Pulley - Driver (1)* 9545-028-013Set Screws (2) (2)* 9278-043-001Impeller23 8641-581-026Washer, Flat 1/2” for Tumbler Pulley (2)24 9545-017-009Bolt, 1/2”-13 x 1 1/4 (2)25 8641-582-016Washer, Star 1/2” for Tumbler Pulley (2)* 9545-008-001Screw 10 Bx 1/4” (6)* 9545-014-004Bolt, 5/16-18 x 5/8” (8) (8)5/16-18* 8640-400-003Nut,* 9538-184-001Spacer, Shaft (2)* 9487-234-005Ring Tolerance (2)* 9125-007-001Damper Inside Duct Exhaust (2)* 9125-007-002Damper Inside Duct Exhaust (1)* 8520-141-000Nut, Spring (4)* 9074-335-001Cover Duct Lower (1)* 9545-008-024Screw 10ABx 3/8” (72)* 9029-173-001Bracket for Wire Harness Under Burner Housing (2)Part # 8533-085-001 9/14Part # 8533-085-001 9/14Rear View Photos1264722Rear Panel & Cover GroupKey Part Number Description Quantity19208-090-001Rear Guard Side Panel 1 (2)4 9545-008-024Screws 10 AB x 3/8 (30)5 8502-649-001Label - Connection Electrical (1)8 9208-089-001Rear Guard Back Panel (2)10 8502-600-001Label Warning & Notice (1)11 8502-645-001Label - Instructions (1)12 9109-113-001Transition Assembly Outlet (1)13 9074-320-001 Top Cover Dryer Panel (1)14 9550-188-001 Top Burner Housing Heat Shield Inlet (1)15 9074-321-001 Top Panel Burner Housing Cover (1)Part # 8533-085-001 9/141851113121514Tumbler GroupKey Part Number Description Quantity 9848-131-001Tumbler Assembly Galvanized w/spider (2)G2 9568-013-001Spider Assembly (2)G3 9497-226-002Rod, Tumbler (6)G4 8640-417-005Nut, 1/2 - 13 (6)G6 8641-590-002Washer, Special (6).............................................................................AR G7 9552-013-000Shim* 9848-130-002Tumbler Assembly Stainless Steel (2)G1 9848-130-001Tumber Assembly Galvanized (2)Part # 8533-085-001 9/14Control Assembly GroupKey Part Number DescriptionQuantity* 9857-189-001 Control Assmbly Complete (all below included) .............................1* 9108-117-001 Control Box Cover ..................................................................... 1* 8220-001-478 Wire Assembly Green 7” ............................................................ 1* 8639-621-007 Screw #10-32 x 12 Green ............................................................1* 8641-582-006 Lockwasher Ext Tooth #10 ..........................................................13 9897-026-002 Terminal Block Main Power Middle ...............................................14 9897-026-001 Terminal Block ............................................................................2* 9545-045-012 Screw #8 ABx 1/2 for terminal block ............................................6 5 8711-011-001 Transformer Ignition ...................................................................2* 9545-008-024 Screws 10AB x 3/8” ...................................................................46 9982-348-001 Plate Assembly MTG Ignition Control............................................2* 9545-008-024 Screws 10B x 1/4” MTG Above Plate and Others ...........................47 9857-116-003 Ignition Control ..........................................................................2* 8640-411-003 #6-32 Nuts ................................................................................48 9631-403-009 Wire Assembly High Voltage Upper ..............................................19 9627-860-001 Wire Harness Ignition Control Upper ............................................110 9627-860-002 Wire Harness Ignition Control Lower ............................................1* 9053-067-002 Bushing Wire 7/8” .......................................................................413 9200-001-002 Fuseholder Assembly ..................................................................314 8636-018-001 Fuse 1.5 Amp .............................................................................315 5192-299-001 Relay Power ...............................................................................216 9897-035-001 Terminal Block Assembly Main Power Inlet ...................................1* 9545-008-024 Screw #8 AB x 1/2” ....................................................................2* 8220-062-036 Wire Assembly Red/Black 14” ......................................................1* 8220-062-037 Wire Assembly Red/White 14” .....................................................1* 8220-062-038 Wire Assembly White 14” ............................................................221 9627-864-004 Wire Harness Motor Extension .....................................................2* 9527-007-001 Stand Off - Wire Saddle / Arrowhead ..........................................13* 9545-031-005 Screw 6 B x 3/8” ........................................................................422 9558-029-003 Strip Terminal Marker (Behind Input Power) ..................................124 9627-863-001 Wire Harness Main Extension Access Under Burner Housing .........123 9631-403-008 Wire Ass’y - High Voltage Lower ..................................................125 9627-859-001 Wire Harness - Main Power (1)Part # 8533-085-001 9/14Control Assembly GroupPart # 8533-085-001 9/1416252223245Coin AccecptorKey Part Number Description Quantity1 9021-041-001Coin Accecptor, Optical (1)Replacement (1)2 9801-099-001Sensor-Optical,3 9545-039-002Screw, Heighth Bar, 3mm (2)* 9486-136-001 Retainer, Coin Acceptor (1)* 9545-053-002 Screw (4)Part # 8533-085-001 9/14NotesPart # 8533-085-001 9/14NotesPart # 8533-085-001 9/14Section 7: VoltageConversionPart # 8533-085-001 9/14Part # 8533-085-001 9/14Instructions - Convert a Dual Voltage Stack Dryer from 120V to 208-240V with Neutral Wire Only1. Remove incoming power from the dryer. Use a known working voltmeter to check power.2. Remove the cover of both the upper and lower control box assemblies from the dryer using a 5/16” wrench.3. Move the black/blue wire from the N position of the main power terminal block to the L2 position of the mainpower terminal block in the upper control box assembly. See Figure 6 below.4. Move the white wire of the upper motor harness to an upper inner left terminal in the middle terminal block in thelower control box assembly. See Figure 6 below.5. Move the orange wire of the upper motor harness to an upper inner left terminal in the middle terminal block inthe lower control box assembly. See Figure 6 below.6. Move the white wire of the lower motor harness to a lower inner left terminal in the middle terminal block in thelower control box assembly. See Figure 6 below.7. Move the orange wire of the lower motor harness to a lower inner left terminal in the middle terminal block in thelower control box assembly. See Figure 6 below.8. Reconnect power to the dryer and test to ensure proper operation; one line voltage to L1, one line voltage to L2,the neutral to N, and the earth ground to E.9. Reinstall the cover of both the upper and lower control box assemblies from the dryer using a 5/16” wrench.Part # 8533-085-001 9/14NotesPart # 8533-085-001 9/14Section 9: MaintenancePart # 8533-085-001 9/14MaintenanceDaily1. Clean lint screen by unlocking and sliding out in their tracks for access. Use soft brush ifnecessary. Failure to do so will slow drying and increase gas usage and temperatures through out the dryer.2. Check lint screen for tears. Replace if necessary.Monthly1. Remove lint accumulation from end bells of motor.2. Clean lint from lint screen compartment.3. Remove lint and dirt accumulation from top of the dryer and all areas above, and around theburners and burner housing. Failure to keep this portion of the dryer clean can lead to a buildup of lint creating a fi re hazard.4. Inspect Recirculation burner housing for excessive buildup.5. Place a few drops of light oil on top and bottom pivots of the clothes door hinge.6. Grease bearings and shaft of intermediate drive pulley.Quarterly1. Check belts for looseness, wear or fraying.2. Inspect gasket of door glass for excessive wear.3. Check tightness of all fasteners holding parts to support channel.4. Check tightness of tumbler shaft retaining nut. MUST MAINTAIN 150 FOOT LBS.5. Remove lint accumulation from primary air ports in burners.6. Grease pivot pins and tension arms where in contact with each other.Semiannually1. Remove and clean main burners.2. Remove all orifi ces and examine for dirt and hole obstruction.3. Remove all lint accumulation. Remove front panel, lint screen housing and remove lintaccumulation.Annually1. Check intermediate pulley bearings for wear.2. Check and remove any lint accumulation from exhaust system.NOTE: DRYER MUST NOT BE OPERATED WITHOUT LINT SCREEN IN PLACE。

外文翻译:智能开关电源

外文翻译:智能开关电源

Intelligent switch power supply英文:With the rapid development of electronic technology, application field of electronic system is more and more extensive, electronic equipment, there are more and more people work with electronic equipment, life is increasingly close relationship. Any electronic equipment are inseparable from reliable power supply for power requirements, they more and more is also high. Electronic equipment miniaturized and low cost in the power of light and thin, small and efficient for development direction. The traditional transistors series adjustment manostat is continuous control linear manostat. This traditional manostat technology more mature, and there has been a large number of integrated linear manostat module, has the stable performance is good, output ripple voltage small, reliable operation, etc. But usually need are bulky and heavy industrial frequency transformer and bulk and weight are big filter.In the 1950s, NASA to miniaturization, light weight as the goal, for a rocket carrying the switch power development. In almost half a century of development process, switch power because of its small volume, light weight, high efficiency, wide range, voltage advantages in electric, control, computer, and many other areas of electronic equipment has been widely used. In the 1980s, a computer is made up of all of switch power supply, the first complete computer power generation. Throughout the 1990s, switching power supply in electronics, electrical equipment, home appliances areas to be widely, switch power technology into the rapid development. In addition, large scale integrated circuit technology, and the rapid development of switch power supply with a qualitative leap, raised high frequency power products of, miniaturization, modular tide.Power switch tube, PWM controller and high-frequency transformer is an indispensable part of the switch power supply. The traditional switch power supply is normally made by using high frequency power switch tube division and the pins, such as using PWM integrated controller UC3842 + MOSFET is domestic small powerswitch power supply, the design method of a more popularity.Since the 1970s, emerged in many function complete integrated control circuit, switch power supply circuit increasingly simplified, working frequency enhances unceasingly, improving efficiency, and for power miniaturization provides the broad prospect. Three end off-line pulse width modulation monolithic integrated circuit TOP (Three switch Line) will Terminal Off with power switch MOSFET PWM controller one package together, has become the mainstream of switch power IC development. Adopt TOP switch IC design switch power, can make the circuit simplified, volume further narrowing, cost also is decreased obviouslyMonolithic switching power supply has the monolithic integrated, the minimalist peripheral circuit, best performance index, no work frequency transformer can constitute a significant advantage switching power supply, etc. American PI (with) company in Power in the mid 1990s first launched the new high frequency switching Power supply chip, known as the "top switch Power", with low cost, simple circuit, higher efficiency. The first generation of products launched in 1994 represented TOP100/200 series, the second generation product is the TOP Switch - debuted in 1997 Ⅱ. The above products once appeared showed strong vitality and he greatly simplifies thedesign of 150W following switching power supply and the development of new products for the new job, also, high efficiency and low cost switch power supply promotion and popularization created good condition, which can be widely used in instrumentation, notebook computers, mobile phones, TV, VCD and DVD, perturbation VCR, mobile phone battery chargers, power amplifier and other fields, and form various miniaturization, density, on price can compete with the linear manostat AC/DC power transformation module.Switching power supply to integrated direction of future development will be the main trend, power density will more and more big, to process requirements will increasingly high. In semiconductor devices and magnetic materials, no new breakthrough technology progress before major might find it hard to achieve, technology innovation will focus on how to improve the efficiency and focus onreducing weight. Therefore, craft level will be in the position of power supply manufacturing higher in. In addition, the application of digital control IC is the future direction of the development of a switch power. This trust in DSP for speed and anti-interference technology unceasing enhancement. As for advanced control method, now the individual feels haven't seen practicability of the method appears particularly strong,perhaps with the popularity of digital control, and there are some new control theory into switching power supply.(1)The technology: with high frequency switching frequencies increase, switch converter volume also decrease, power density has also been boosted, dynamic response improved. Small power DC - DC converter switch frequency will rise to MHz. But as the switch frequency unceasing enhancement, switch components and passive components loss increases, high-frequency parasitic parameters and high-frequency EMI and so on the new issues will also be caused.(2)Soft switching technologies: in order to improve the efficiency of non-linearity of various soft switch, commutation technical application and hygiene, representative of soft switch technology is passive and active soft switch technology, mainly including zero voltage switch/zero current switch (ZVS/ZCS) resonance, quasi resonant, zero voltage/zero current pulse width modulation technology (ZVS/ZCS - PWM) and zero voltage transition/zero current transition pulse width modulation (PWM) ZVT/ZCT - technical, etc. By means of soft switch technology can effectively reduce switch loss and switch stress, help converter transformation efficiency (3)Power factor correction technology (IC simplifies PFC). At present mainly divided into IC simplifies PFC technology passive and active IC simplifies PFC technology using IC simplifies PFC technology two kinds big, IC simplifies PFC technology can improve AC - DC change device input power factor, reduce the harmonic pollution of power grid.(4)Modular technology. Modular technology can meet the needs of the distributed power system, enhance the system reliability.(5)Low output voltage technology. With the continuous development of semiconductor manufacturing technology, microprocessor and portable electronic devices work more and more low, this requires future DC - DC converter can provide low output voltage to adapt microprocessor and power supply requirement of portable electronic devicesPeople in switching power supply technical fields are edge developing related power electronics device, the side of frequency conversion technology, development of switch between mutual promotion push switch power supply with more than two year growth toward light, digital small, thin, low noise and high reliability, anti-interference direction. Switching powersupply can be divided into the AC/DC and DC/DC two kinds big, also have AC/AC DC/AC as inverter DC/DC converter is now realize modular, and design technology and production process at home and abroad, are mature and standardization, and has approved by users, but the AC/DC modular, because of its own characteristics in the process of making modular, meet more complex technology and craft manufacture problems. The following two types of switch power supply respectively on the structure and properties of this.Switching power supply is the development direction of high frequency, high reliability, low consumption, low noise, anti-jamming and modular. Because light switch power, small, thin key techniques are changed, so high overseas each big switch power supply manufacturer are devoted to the development of new high intelligent synchronous rectifier, especially the improvement of secondary devices of the device, and power loss of Zn ferrite (Mn) material? By increasing scientific and technological innovation, to enhance in high frequency and larger magnetic flux density (Bs) can get high magnetic under the miniaturization of, and capacitor is a key technology. SMT technology application makes switching power supply has made considerable progress, both sides in the circuitboard to ensure that decorate components of switch power supply light, small, thin. The high frequency switching power supply of the traditional PWM must innovate switch technology, to realize the ZCS ZVS, soft switch technology hasbecome the mainstream of switch power supply technical, and greatly improve the efficiency of switch power. For high reliability index, America's switch power producers, reduce by lowering operating current measures such as junction temperature of the device, in order to reduce stress the reliability of products made greatly increased.Modularity is of the general development of switch power supply trend can be modular power component distributed power system, can be designed to N + 1 redundant system, and realize the capacity expansion parallel. According to switch power running large noise this one defect, if separate the pursuit of high frequency noise will increase its with the partial resonance, and transform circuit technology, high frequency can be realized in theory and can reduce the noise, but part of the practical application of resonant conversion technology still have a technical problem, so in this area still need to carry out a lot of work, in order to make the technology to practional utilization.Power electronic technology unceasing innovation, switch power supply industry has broad prospects for development. To speed up the development of switch power industry in China, we must walk speed of technological innovation road, combination with Chinese characteristics in the joint development path, for I the high-speed development of national economy to make the contribution. The basic principle and component functionAccording to the control principle of switch power to classification, we have the following 3 kinds of work mode:1) pulse width adjustment type, abbreviation Modulation Pulse Width pulse width Modulation (PWM) type, abbreviation for. Its main characteristic is fixed switching frequency, pulse width to adjust by changing voltage 390v, realize the purpose. Its core is the pulse width modulator. Switch cycle for designing filter circuit fixed provided convenience. However, its shortcomings is influenced by the power switch conduction time limit minimum of output voltage cannot be wide range regulation; In addition, the output will take dummy loads commonly (also called pre load), in order to prevent the drag elevated when output voltage. At present, most ofthe integrated switch power adopt PWM way.2) pulse frequency Modulation mode pulse frequency Modulation (, referred to Pulse Frequency Modulation, abbreviation for PFM) type. Its characteristic is will pulse width fixed by changing switch frequency to adjust voltage 390v, realize the purpose. Its core is the pulse frequency modulator. Circuit design to use fixed pulse-width generator to replace the pulse width omdulatros and use sawtooth wave generator voltage?Frequency converter (for example VCO changes frequency VCO). It on voltage stability principle is: when the output voltage Uo rises, the output signal controller pulse width unchanged and cycle longer, make Uo 390v decreases, and reduction. PFM type of switch power supply output voltage range is very wide, output terminal don't meet dummy loads. PWM way and way of PFM respectively modulating waveform is shown in figure 1 (a), (b) shows, tp says pulse width (namely power switch tube conduction time tON), T represent cycle. It can be easy to see the difference between the two. But they have something in common: (1) all use time ratio control (TRC) on voltage stability principle, whether change tp, finally adjustment or T is pulse 390v. Although adopted in different ways, but control goals, is all rivers run into the sea. (2) when load by light weight, or input voltage respectively, from high changed by increasing the pulse width, higher frequency method to make the output voltage remained stable.3) mix modulation mode, it is to point to the pulse width and switching frequency is not fixed, each other can change, it belongs to the way the PWM and PFM blend mode. It contains a pulsewidthomdulatros and pulse frequency modulator. Because and T all can adjust alone, so occupies emptiescompared to adjust the most wide range, suitable for making the output voltage for laboratories that use a wide range of can adjust switching power supply. Above 3 work collectively referred to as "Time Ratio Control" (as a Control, from TRC) way. As noted, pulse width omdulatros either as a independent IC use (for example UC3842 type pulse width omdulatros), can also be integrated in DC/DC converter (for example LM2576 type switching voltage regulators integrated circuit), still can integration in AC/DC converter (for exampleTOP250 type monolithic integrated circuit switching power supply. Among them, the switching voltage regulators belong to DC/DC power converter, switching power supply general for AC/DC power converter.The typical structure of switch power as figure1shows, its working principle is: the first utility into power rectifier and filtering into high voltage dc and then through the switch circuit and high-frequency switch to high frequency low pressure pulse transformer, and then after rectification and filter circuits, finally output low voltage dc power. Meanwhile in the output parts have a circuit feedback to control circuit, through the control PWM occupies emptiescompared to achieve output voltage stability.Figure 1 typical structure of switch power supplySwitching power supply by these four components:1) the main circuit: exchange network input, from the main circuit to dc output. Mainly includes input filter, rectifier and filtering, inverter, and output rectifier and filtering.(1) input filter: its effect is the power grid existing clutter filtering, also hinder the machine produces clutter feedback to public power grid.(2) rectifier and filter: the power grid ac power directly for a smooth dc rectifier, for the next level transformation.(3) inverter: will the dc after rectifying a high-frequency ac, this is the core of high frequency switching power supply, the higher the frequency, the volume, weight and the ratio of power output and smaller.(4) Out put rectifier and filter: according to load needs, providing stable and reliable dc power supply. 2) control circuit: on the one hand, from the output bysampling with set standards to compare, and then to control inverter, changing its frequency or pulse width, achieve output stability, on the other hand, according to data provided by the test circuit, the protection circuit differential, provide control circuit to the machine to various protection measures. Including the output feedback circuit and sampling circuit, pulse width modulator. 3) the detection and protection circuit: detection circuit had current detection, over-voltage detection, owe voltage detection, overheat detection, etc.; Protection circuit can be divided over current protection, over-voltage protection, owe voltage protection, the ground-clamp protection, overheating protection, automatic restart, soft start, slow startup, etc. Various types. 4) Other circuit: if the sawtooth wave generator, offset circuit, optical coupler, etc.智能开关电源中文:随着电子技术的高速发展,电子系统的应用领域越来越广泛,电子设备的种类也越来越多,电子设备与人们的工作、生活的关系日益密切。

反激有源钳位(Active-Clamp Flyback)

反激有源钳位(Active-Clamp Flyback)

3. ACTIVE-CLAMP FLYBACK AS AN ISOLATED PFC FRONT-END CONVERTER
46
peak current stress and RMS currents than CCM operation. However, ZVS can still be realized with unidirectional magnetizing current by utilizing the energy stored in the resonant inductor [44]. The presence of the resonant inductor also helps to softly commute the turn-off of the output rectifier, resulting in reduced output noise and rectifier switching losses. This would also be a particular advantage in high output voltage applications where slower rectifiers are more likely to be used. This chapter presents evaluation of a constant-frequency, soft switching, active-clamp flyback converter suitable for both PFC and DC/DC conversion applications. The basic principle of operation is analyzed and a design procedure is developed. Experimental results are then presented which illustrate converter function and verify the analysis presented. These results are then extended to active-clamp flyback single-stage and interleaved PFC applications where the system power levels are limited to about 500 600 W.

电工英语单词

电工英语单词

电工英语单词(1) 元件设备三绕组变压器:three-column transformer ThrClnTrans双绕组变压器:double-column transformer DblClmnTrans电容器:Capacitor 并联电容器:shunt capacitor 电抗器:Reactor 母线:Busbar输电线:TransmissionLine 发电厂:power plant 断路器:Breaker 刀闸(隔离开关):Isolator 分接头:tap 电动机:motor(2) 状态参数有功:active power 无功:reactive power 电流:current 容量:capacity 电压:voltage 档位:tap position 有功损耗:reactive loss 无功损耗:active loss 功率因数:power-factor 功率:power功角:power-angle 电压等级:voltage grade 空载损耗:no-load loss 铁损:iron loss铜损:copper loss 空载电流:no-load current阻抗:impedance正序阻抗:positive sequence impedance 负序阻抗:negative sequence impedance 零序阻抗:zero sequence impedance 电阻:resistor 电抗:reactance 电导:conductance 电纳:susceptance无功负载:reactive load 或者QLoad有功负载: active load PLoad遥测:YC(telemetering)遥信:YX励磁电流(转子电流):magnetizing current 定子:stator功角:power-angle上限:upper limit 下限:lower limit并列的:apposable 高压: high voltage 低压:low voltage 中压:middle voltage 电力系统 power system 发电机 generator 励磁 excitation 励磁器excitor 电压 voltage 电流 current 母线 bus 变压器 transformer 升压变压器 step-up transformer高压侧 high side 输电系统 power transmission system输电线 transmission line固定串联电容补偿fixed series capacitor compensation 稳定 stability 电压稳定 voltage stability功角稳定 angle stability 暂态稳定 transient stability 电厂 power plant 能量输送 power transfer交流 AC 装机容量 installed capacity电网 power system 落点 drop point开关站 switch station 双回同杆并架 double-circuit lines on the same tower变电站 transformer substation 补偿度 degree of compensation 高抗high voltage shunt reactor 无功补偿 reactive power compensation 故障fault 调节 regulation 裕度 magin 三相故障 three phase fault 故障切除时间fault clearing time极限切除时间 critical clearing time切机 generator triping 高顶值 high limited value 强行励磁 reinforced excitation 线路补偿器 LDC(line drop compensation) 机端 generator terminal静态 static (state) 动态 dynamic (state)单机无穷大系统 one machine - infinity bus system 机端电压控制 AVR 电抗 reactance 电阻 resistance 功角 power angle有功(功率) active power 无功(功率) reactive power 功率因数 power factor 无功电流 reactive current 下降特性 droop characteristics 斜率 slope 额定 rating 变比 ratio参考值 reference value 电压互感器 PT分接头 tap 下降率 droop rate仿真分析 simulation analysis 传递函数 transfer function 框图 block diagram 受端 receive-side 裕度 margin同步 synchronization 失去同步 loss of synchronization 阻尼 damping 摇摆 swing保护断路器 circuit breaker电阻:resistance 电抗:reactance 阻抗:impedance电导:conductance 电纳:susceptance导纳:admittance 电感:inductance电容: capacitancemagnetizing reacance 磁化电抗line-to-neutral 线与中性点间的 staor winding 定子绕组 leakage reactance 漏磁电抗no-load 空载 full load 满载 Polyphase 多相(的) iron-loss 铁损complex impedance 复数阻抗 rotor resistance 转子电阻 leakage flux 漏磁通 locked-rotor 锁定转子 chopper circuit 斩波电路 separately excited 他励的 compounded 复励 dc motor 直流电动机 de machine 直流电机 speed regulation 速度调节 shunt 并励 series 串励 armature circuit 电枢电路optical fiber 光纤 interoffice 局间的 waveguide 波导波导管 bandwidth 带宽 light emitting diode 发光二极管 silica 硅石二氧化硅 regeneration 再生, 后反馈放大 coaxial 共轴的,同轴的high-performance 高性能的 carrier 载波 mature 成熟的 Single Side Band(SSB) 单边带 coupling capacitor 结合电容 propagate 传导传播modulator 调制器 demodulator 解调器 line trap 限波器 shunt 分路器Amplitude Modulation(AM)调幅Frequency Shift Keying(FSK)移频键控tuner 调谐器 attenuate 衰减 incident 入射的 two-way configuration 二线制 generator voltage 发电机电压 dc generator 直流发电机 polyphase rectifier 多相整流器boost 增压 time constant 时间常数 forward transfer function 正向传递函数 error signal 误差信号 regulator 调节器 stabilizing transformer 稳定变压器 time delay 延时direct axis transient time constant 直轴瞬变时间常数transient response 瞬态响应 solid state 固体 buck 补偿 operational calculus 算符演算 gain 增益 pole 极点 feedback signal 反馈信号 dynamic response 动态响应 voltage control system 电压控制系统 mismatch 失配error detector 误差检测器 excitation system 励磁系统 field current励磁电流 transistor 晶体管 high-gain 高增益 boost-buck 升压去磁 feedback system 反馈系统reactive power 无功功率 feedback loop 反馈回路 automatic Voltage regulator(AVR)自动电压调整器reference Voltage 基准电压 magnetic amplifier 磁放大器amplidyne 微场扩流发电机self-exciting 自励的 limiter 限幅器manual control 手动控制block diagram 方框图 linear zone 线性区 potential transformer 电压互感器 stabilization network 稳定网络 stabilizer 稳定器 air-gap flux 气隙磁通 saturation effect 饱和效应 saturation curve 饱和曲线 flux linkage 磁链 per unit value 标么值 shunt field 并励磁场 magnetic circuit 磁路load-saturation curve 负载饱和曲线air-gap line 气隙磁化线 polyphase rectifier 多相整流器 induction machine 感应式电机 horseshoe magnet 马蹄形磁铁 magnetic field 磁场 eddy current 涡流 right-hand rule 右手定则 left-hand rule 左手定则 slip 转差率 induction motor 感应电动机 rotating magnetic field 旋转磁场 winding 绕组 stator 定子 rotor 转子 induced current 感生电流 time-phase 时间相位exciting voltage 励磁电压 solt 槽 lamination 叠片 laminated core 叠片铁芯 short-circuiting ring 短路环 squirrel cage 鼠笼 rotor core 转子铁芯cast-aluminum rotor 铸铝转子 bronze 青铜 horsepower 马力 random-wound 散绕 insulation 绝缘 ac motor 交流环电动机end ring 端环 alloy 合金 coil winding 线圈绕组form-wound 模绕 performance characteristic 工作特性 frequency 频率revolutions per minute 转/分 motoring 电动机驱动generating 发电 per-unit value 标么值 breakdown torque 极限转矩breakaway force 起步阻力 overhauling 检修 wind-driven generator 风动发电机revolutions per second 转/秒 number of poles 极数 speed-torque curve 转速力矩特性曲线plugging 反向制动synchronous speed 同步转速 percentage 百分数 locked-rotor torque 锁定转子转矩 full-load torque 满载转矩 prime mover 原动机 inrush current 涌流。

电气自动化专业英文词汇及缩写

电气自动化专业英文词汇及缩写

电力系统 power system 发电机generator 励磁 excitation 励磁器 excitor 电压 voltage 电流 current升压变压器 step-up transformer 母线 bus 变压器transformer空载损耗 no-load loss 铁损iron loss 铜损 copper loss 空载电流 no-load current 有功损耗 active loss 无功损耗reactive loss输电系统 power transmission system 高压侧 high side 输电线 transmission line高压 high voltage 低压 low voltage 中压 middle voltage 功角稳定 angle stability 稳定 stability 电压稳定voltage stability暂态稳定 transient stability 电厂 power plant 能量输送power transfer交流 AC 直流 DC 电网 power system落点 drop point 开关站switch station 调节regulation 高抗 high voltage shuntreactor 并列的 apposable 裕度 margin故障 fault 三相故障 threephase fault 分接头 tap切机 generator triping 高顶值 high limited value 静态static state动态 dynamic state 机端电压控制 AVR 电抗 reactance电阻 resistance 功角 powerangle 有功功率 active power电容器 Capacitor 电抗器Reactor 断路器 Breaker电动机 motor 功率因数power-factor 定子 stator阻抗 impedance 功角power-angle 电压等级voltage grade有功负载: active load PLoad无功负载 reactive load 档位tap position电阻 resistor 电抗reactance 电导 conductance电纳 susceptance 上限 upperlimit 下限 lower limit正序阻抗 positive sequenceimpedance 负序阻抗 negativesequence impedance 零序阻抗zero sequence impedance无功功率 reactive power 功率因数 power factor 无功电流reactive current斜率 slope 额定 rating 变比ratio参考值 reference value 电压互感器 PT 分接头 tap仿真分析 simulation analysis下降率 droop rate 传递函数transfer function框图 block diagram 受端receive-side 同步synchronization保护断路器 circuit breaker摇摆 swing 阻尼 damping无刷直流电机 Brusless DCmotor 刀闸隔离开关 Isolator机端 generator terminal变电站 transformersubstation永磁同步电机Permanent-magnet SynchronismMotor异步电机 Asynchronous Motor三绕组变压器 three-columntransformer ThrClnTrans双绕组变压器 double-columntransformer DblClmnTrans固定串联电容补偿 fixed series capacitor compensation双回同杆并架 double-circuit lines on the same tower单机无穷大系统 one machine - infinity bus system励磁电流 Magnetizing current 补偿度 degree of compensation电磁场:Electromagneticfields 失去同步 loss of synchronization装机容量 installed capacity 无功补偿 reactive power compensation故障切除时间 fault clearing time 极限切除时间 critical clearing time强行励磁 reinforced excitation 并联电容器 shunt capacitor<下降特性 droop characteristics 线路补偿器LDCline drop compensation电机学 Electrical Machinery 自动控制理论 Automatic Control Theory 电磁场 Electromagnetic Field微机原理 Principle ofMicrocomputer电工学 Electrotechnics 电路原理 Principle of circuits电机学 Electrical Machinery电力系统稳态分析Steady-State Analysis ofPower System电力系统暂态分析Transient-State Analysis ofPower System电力系统继电保护原理Principle of ElectricalSystem's Relay Protection电力系统元件保护原理Protection Principle of PowerSystem 's Element电力系统内部过电压 PastVoltage within Power system模拟电子技术基础 Basis ofAnalogue ElectronicTechnique数字电子技术DigitalElectrical Technique电路原理实验 Lab. ofprinciple of circuits电气工程讲座Lectures onelectrical power production电力电子基础 Basicfundamentals of powerelectronics高电压工程High voltageengineering电子专题实践Topics onexperimental project ofelectronics电气工程概论Introductionto electrical engineering电子电机集成系统Electronic machine system电力传动与控制ElectricalDrive and Control电力系统继电保护PowerSystem Relaying Protection主变压器 main transformer升压变压器 step-uptransformer降压变压器 step-downtransformer工作变压器 operatingtransformer备用变压器 standbytransformer公用变压器 commontransformer三相变压器 three-phasetransformer单相变压器 single-phase transformer带负荷调压变压器 on-load regulating transformer变压器铁芯 transformer core变压器线圈 transformercoil变压器绕组 transformer winding变压器油箱 transformer oil tank变压器外壳 transformer casing变压器风扇 transformer fan 变压器油枕transformer oil conservator ∽ drum变压器额定电压transformer reted voltage变压器额定电流transformer reted current变压器调压范围transformer voltage regulation rage配电设备 powerdistribution equipmentSF6断路器 SF6 circuit breaker开关 switch按钮 button隔离开关isolator,disconnector真空开关 vacuum switch刀闸开关 knife-switch接地刀闸 earthingknife-switch电气设备 electricalequipment变流器 current converter电流互感器 currenttransformer电压互感器 voltagetransformer电源 power source交流电源 AC power source直流电源 DC power source工作电源 operating source备用电源 Standby source强电 strong current弱电 weak current继电器 relay信号继电器 signal relay电流继电器 current relay电压继电器 voltage relay跳闸继电器 tripping relay合闸继电器 closing relay中间继电器 intermediaterelay时间继电器 time relay零序电压继电器zero-sequence voltage relay差动继电器 differentialrelay闭锁装置 locking device遥控 telecontrol遥信 telesignalisation遥测 telemetering遥调 teleregulation断路器 breaker,circuitbreaker少油断路器 mini-oilbreaker,oil-mini-mum breaker高频滤波器 high-frequencyfilter组合滤波器 combined filter常开触点 normally openedcontaact常闭触点 normally closedcontaact并联电容 parallelcapacitance保护接地 protectiveearthing熔断器 cutout,fusiblecutout电缆 cable跳闸脉冲 tripping pulse合闸脉冲 closing pulse一次电压 primary voltage二次电压 secondary voltage 并联电容器 parallel capacitor无功补偿器 reactive power compensation device消弧线圈 arc-suppressing coil母线 Bus,busbar三角接法 delta connection 星形接法 Wye connection原理图 schematic diagram 一次系统图 primary system diagram二次系统图 secondary system diagram两相短路 two-phase short circuit三相短路 three-phase short circuit单相接地短路 single-phase ground short circuit短路电流计算 calculation of short circuit current自动重合闸 automatic reclosing高频保护 high-freqency protection距离保护 distance protection横差保护 transversedifferential protection纵差保护 longitudinaldifferential protection线路保护 line protection过电压保护 over-voltageprotection母差保护 bus differentialprotection瓦斯保护 Buchholtzprotection变压器保护 transformerprotection电动机保护 motorprotection远方控制 remote control用电量 power consumption载波 carrier故障 fault选择性 selectivity速动性 speed灵敏性 sensitivity可靠性 reliability电磁型继电器electromagnetic无时限电流速断保护instantaneously over-currentprotection跳闸线圈 trip coil工作线圈 operating coil制动线圈 retraint coil主保护 main protection后备保护 back-upprotection定时限过电流保护 definitetime over-current protection三段式电流保护 the currentprotection with three stages反时限过电流保护 inversetime over-current protection方向性电流保护 thedirectional currentprotection零序电流保护zero-sequence currentprotection阻抗 impedance微机保护 MicroprocessorProtectionAGC Automatic GenerationControl 自动发电控制AMRAutomatic MessageRecording 自动抄表ASSAutomatic SynchronizedSystem 自动准同期装置ATSAutomatic TransformSystem 厂用电源快速切换装置AVR Automatic VoltageRegulator 自动电压调节器BCS Burner Control System燃烧器控制系统BMS BurnerManagement System 燃烧器管理系统CCS Coordinated Control System 协调控制系统CIS Consumer Information System 用户信息系统CRMS Control Room Management System 控制室管理系统CRT Cathode Ray Tube 阴极射线管DA Distribution Automation 配电自动化DAS Data Acquisition System 数据采集与处理系统DCS Distributed Control System 分散控制系统DDC Direct Digital Control 直接数字控制系统DEH Digital Electronic Hydraulic Control 数字电液调节系统DMS Distribution Management System 配电管理系统DPU Distributed Processing Unit 分布式处理单元DSM Demand Side Management 需求侧管理EMS Energy Management System 能量管理系统ETS Emergency Trip System 汽轮机紧急跳闸系统EWS Engineering Working Station 工程师工作站FA Feeder Automation 馈线自动化FCS Fieldbus Control System 现场总线控制系统FSS Fuel Safety System 燃料安全系统FSSS Furnace Safeguard Supervisory System 炉膛安全监控系统FTU Feeder Terminal Unit 馈线远方终端GIS Gas InsulatedSwitchgear 气体绝缘开关设备GPS Global PositionSystem 全球定位系统HCSHierarchical ControlSystem 分级控制系统LCDLiquid Crystal Display 液晶显示屏LCP Local ControlPanel 就地控制柜MCC MotorControl Center 电动机马达控制中心MCS ModulatingControl System 模拟量控制系统MEH Micro ElectroHydraulic Control System给水泵汽轮机电波控制系统MIS ManagementInformation System 管理信息系统NCS Net ControlSystem 网络监控系统OISOperator InterfaceStation 操作员接口站OMSOutage Management System停电管理系统PAS PowerApplication Software 电力应用软件PID ProportionIntegrationDifferentiation 比例积分微分PIO Process InputOutput 过程输入输出通道PLC Programmable LogicalController 可编程逻辑控制器PSS Power SystemStabilizator 电力系统稳定器RTU Remote TerminalUnit 站内远方终端SASubstation Automation 变电站自动化SCADASupervisory Control AndData Acquisition 数据采集与监控系统SCC SupervisoryComputer Control 监督控制系统SCS Sequence ControlSystem 顺序程序控制系统SIS SupervisoryInformation System 监控信息系统TDCSTDC TotalDirect Digital Control 集散控制系统TSI TurbineSupervisoryInstrumentation 汽轮机监测仪表UPS UninterruptedPower Supply 不间断供电WMS Work Management System工作管理系统。

华意低压电气品牌 0.4kV低压智能补偿电容器(HY-RZC)综合手册说明书

华意低压电气品牌 0.4kV低压智能补偿电容器(HY-RZC)综合手册说明书

Intelligent Capacitor Series (HY-RZC)intelligent capacitor series (HY-RZC)Intelligent Capacitor SeriesHY-RZC low voltage intelligent power capacitor takes two groups (△ type) orone group (Y type) of low voltage power capacitor as the main body, adoptsmicro-electronics software and hardware, micro sensor and other latest technologies, changed the backward controller technology and switching technology of traditional reactive power compensation device, and the bulky and heavy structure pattern, has the advantages of simple structure, convenient production, reduce cost, improveperformance, convenient maintenance and so on, meets the higher demand of modern electric power customer for reactive power compensation, is a new generation of intelligent reactive power compensation device applied to 0.4 kV low-voltage power grid.Huayi LV electric brand nameVoltage grade:0.4kV Primary compensation capacity (unit: kVar)Intelligent capacitorCompensation mode: S three-phase compensation F split-phase compensationSecondary compensation capacity (unit: kVar)MODELPRODUCT FEATURENote: split-phase compensation is without secondary compensation capacitySwitching switch device has strong withstand voltage impact ability and withstand strike current abilityWithstand voltage of impact ability >AC3500V (DC5000V )Zero-crossing switching performance of switching switch is excellentThe deviation degree of switching <2.5°Current shock resistance ability ≥ 100 times rated currentRated time of switching ≥1 million timesSwitching flow <2.5 times rated currentMan-machine coordinationProtection functionUse liquid crystal display, real-time display condition dataUse three-color LED lights (yellow, green, red) to indicate the operation of stateIntelligent network functionsUse intelligent network technology to build RS485 communication methods to realize data exchange between devicesWith overvoltage, undervoltage, electric loss protection, short circuit protection, over-current and over-temperature protection and other functionsIntelligent capacitor is mainly composed of intelligent control unit, zero-crossing switching switch device, low voltage power capacitor, and the internal temperature of the capacitor and acquisition of the current signal, etc, divides into total compensation and separate compensation, specific principle diagram is as follows.Working principle of total compensation intelligent capacitor Working principle of separate compensation intelligent capacitorTECHNICAL PARAMETERSSERVICE COMMITMENTPre-sale services: project consultancy, demand analysis, field test, schematic design and evaluationOn-purchase service: plan implementation, debugging, trainingAfter-sale service: operation maintenance, regular review, emergency treatmentReply to customer in 2 hours; arrived on the scene in 12 hours; solve the problem in 24 hoursCUSTOMER PERFORMANCEState Grid Corporation of ChinaHangzhou MetroTianqiPharmaceutical GroupGreenland GroupWanda Group。

电气专业英语词汇

电气专业英语词汇

电气常用英语词汇电力系统power system 发电机generator 励磁excitation 励磁器excitor电压voltage 电流current 升压变压器step-up transform er母线bus 变压器transformer 空载损耗no-load loss铁损iron loss铜损copper loss 空载电流no-load current 有功损耗act ive loss无功损耗reactive loss 输电系统power transmission syste m高压侧high side 输电线transmission line 高压high v oltage低压low voltage 中压middle voltage 功角稳定angle s tability稳定stability 电压稳定voltage stability 暂态稳定transi ent stability电厂power plant 能量输送power transfer 交流AC直流DC电网power system 落点drop point 开关站switch statio n调节regulation 高抗high voltage shunt reactor 并列的apposable裕度margin 故障fault 三相故障three phase fault分接头tap切机generator triping 高顶值high limited value 静态static (state)动态dynamic (state) 机端电压控制AVR 电抗reactance 电阻resistance功角power angle 有功〔功率〕active power 电容器Cap acitor 电抗器Reactor断路器Breaker 电动机motor 功率因数power-factor 定子stator 阻抗impedance功角power-angle 电压等级voltage grade 有功负载: active load PLoad无功负载reactive load 档位tap position 电阻resistor 电抗reactance电导conductance 电纳susceptance 上限upper limit下限lower limit正序阻抗positive sequence impedance 负序阻抗negative sequence impedance零序阻抗zero sequence impedance 无功〔功率〕reactive p ower功率因数power factor 无功电流reactive current 斜率slop e 额定rating变比ratio 参考值reference value 电压互感器PT 分接头tap仿真分析simulation analysis 下降率droop rate 传递函数transfer function框图block diagram 受端receive-side 同步synchronizat ion保护断路器circuit breaker 摇摆swing 阻尼damping无刷直流电机Brusless DC motor 刀闸(隔离开关) Isolator机端generator terminal变电站transformer substation 永磁同步电机Permanent-m agnet Synchronism Motor异步电机Asynchronous Motor 三绕组变压器three-column transformer ThrClnTrans双绕组变压器double-column transformer DblClmnTrans固定串联电容补偿fixed series capacitor compensation双回同杆并架double-circuit lines on the same tower单机无穷大系统one machine - infinity bus system励磁电流Magnetizing current 补偿度degree of compensati on电磁场:Electromagnetic fields 失去同步loss of synchronization装机容量installed capacity 无功补偿reactive power comp ensation故障切除时间fault clearing time 极限切除时间critical clear ing time强行励磁reinforced excitation 并联电容器shunt capacitor <下降特性droop characteristics 线路补偿器LDC(line drop c ompensation)电机学Electrical Machinery 自动控制理论Automatic Cont rol Theory电磁场Electromagnetic Field 微机原理Principle of Micro computer电工学Electrotechnics 电路原理Principle of circuits 电机学Electrical Machinery电力系统稳态分析Steady-State Analysis of Power System电力系统暂态分析Transient-State Analys is of Power System电力系统继电保护原理Principle of Electrical S ystem's Relay Protection电力系统元件保护原理Protection Principle ofPower System 's Element电力系统内部过电压Past Voltage within P ower system模拟电子技术根底Basis of Analogue Ele ctronic Technique数字电子技术Digital Electrical Techni que电路原理实验Lab. of principle of circ uits电气工程讲座Lectures on electrical p owerproduction电力电子根底Basic fundamentals of power electronics高电压工程High voltage engineering 电子专题实践Topics on experimental project of electronics电气工程概论Introduction to electric al engineering电子电机集成系统Electronic machine sy stem电力传动与控制Electrical Drive and C ontrol电力系统继电保护Power System Relayin g Protection主变压器main transformer升压变压器step-up transformer降压变压器step-down transformer 工作变压器operating transformer备用变压器standby transformer公用变压器common transformer 三相变压器three-phase transformer 单相变压器single-phase transforme r带负荷调压变压器on-load regulating transf ormer变压器铁芯transformer core变压器线圈transformer coil变压器绕组transformer winding变压器油箱transformer oil tank变压器外壳transformer casing变压器风扇transformer fan变压器油枕transformer oil conserva tor(∽drum变压器额定电压transformer reted voltage变压器额定电流transformer reted current 变压器调压范围transformer voltage reg ulation rage配电设备power distribution equip mentSF6断路器SF6 circuit breaker开关switch 按钮button 隔离开关isolator,disconne ctor真空开关vacuum switch 刀闸开关knife-switch接地刀闸earthing knife-switch 电气设备electrical equip ment变流器current converter 电流互感器current transf ormer电压互感器voltage transformer 电源power source交流电源AC power source 直流电源DC power sourc e工作电源operating source 备用电源 Standby source 强电strong current 弱电weak current继电器relay 信号继电器signal relay 电流继电器cur rent relay电压继电器voltage relay 跳闸继电器tripping relay合闸继电器closing relay中间继电器intermediate relay 时间继电器time relay零序电压继电器zero-sequence voltage relay 差动继电器differential relay闭锁装置locking device 遥控telecontrol 遥信tel esignalisation遥测telemetering 遥调teleregulation 断路器breaker,circuit breaker少油断路器mini-oil breaker,oil-mini-mum breaker高频滤波器high-frequency filter 组合滤波器combi ned filter常开触点normally opened contaact 常闭触点norma lly closed contaact并联电容parallel capacitance 保护接地protective earthing熔断器cutout,fusible cutout 电缆cable 跳闸脉冲tripping pulse合闸脉冲closing pulse 一次电压primary voltage 二次电压secondary voltage 并联电容器parallel ca pacitor无功补偿器reactive power compensation device消弧线圈arc-suppressing coil 母线Bus,busbar 三角接法delta connection星形接法Wye connection 原理图schematic diagra m一次系统图primary system diagram二次系统图secondary system diagram两相短路two-phase short circuit三相短路three-phase short circuit单相接地短路single-phase ground short circuit短路电流计算calculation of short circuit current自动重合闸automatic reclosing高频保护high-freqency protection距离保护distance protection横差保护transverse differential protection纵差保护longitudinal differential protection线路保护line protection 过电压保护over-voltage prot ection母差保护bus differential protection瓦斯保护Buchholtz protection 变压器保护transformer protection电动机保护motor protection 远方控制remote control 用电量power consumption载波carrier 故障fault 选择性selectivity 速动性s peed灵敏性sensitivity 可靠性reliability 电磁型继电器elect romagnetic无时限电流速断保护i nstantaneously over-current protect ion跳闸线圈trip coil 工作线圈operating coil制动线圈retraint coil 主保护main protection 后备保护back-up protection定时限过电流保护definite time over-current protection三段式电流保护the current protection with three stages 反时限过电流保护inverse time over-current protection方向性电流保护the directional current protection零序电流保护zero-sequence current protection阻抗impedance 微机保护Microprocessor Protection。

Resonant power converter

Resonant power converter

专利名称:Resonant power converter 发明人:Mark Adams申请号:US09/005950申请日:19980112公开号:US05909362A公开日:19990601专利内容由知识产权出版社提供摘要:A resonant power converter holds energy within the circuit for a variable period to provide fixed-frequency, zero-voltage switching power conversion. A first switch alternately connects and disconnects a DC voltage source to one side of the primary winding of the transformer of a power converter. A second switch is connected between the other side of the primary winding and ground. A switch controller is responsive to the difference between a reference voltage and the voltage level present at the output of the circuit associated with the secondary winding of the transformer. Energy is added to the circuit while the first and second switches are closed. The first switch is then opened and energy is held in the circuit for a variable period of time to delay the beginning of resonance. Finally, both switches are opened and the energy within the circuit resonates. The energy holding period is adjusted as necessary to maintain a fixed frequency with varying loads. Accordingly, the switch controller is configured to open and close the first and second switches to maintain fixed-frequency operation of the power converter and switching of the second switch under zero-voltage conditions and in the presence of varying loads.申请人:ELDEC CORPORATION代理机构:Christensen O'Connor Johnson & Kindness PLLC更多信息请下载全文后查看。

zvs限制功率方法

zvs限制功率方法

ZVS(Zero V oltage Switch)是一种软开关技术,可以应用于各种电源转换器和电机驱动器中,以提高效率和降低开关损耗。

限制ZVS的功率可以通过多种方法实现,下面列举几种常用的方法:
1. 限流电阻:在ZVS的输出端串联一个限流电阻,以限制电流的幅值。

通过调整限流电阻的阻值,可以控制ZVS的输出功率。

这种方法简单、可靠,但在大电流情况下,限流电阻的损耗会增加。

2. 磁性元件:利用磁性元件(如电感器或变压器)来实现ZVS的功率限制。

通过合理设计磁性元件的匝数比和磁芯材料,可以控制ZVS的输出功率。

这种方法适用于大功率应用,但需要精心设计和制造。

3. 自动功率限制:通过监测ZVS的输出电流或电压,使用自动控制系统来调整ZVS的工作状态,以实现功率的自动限制。

这种方法需要一定的控制电路和软件支持,但可以实现高精度的功率控制。

4. 分段控制:将ZVS的工作周期分成多个阶段,在不同的阶段设置不同的工作参数,以实现功率的限制。

这种方法可以通过简单的硬件和软件实现,但可能会影响ZVS的工作效率。

在实际应用中,需要根据具体的应用场景和要求选择适合的功率限制方法。

AOS万代MOS管选型与替换

AOS万代MOS管选型与替换

AO3160New SOT23-3Single High Voltage N No No AO3162NewSOT23-3Single High Voltage N No No AO3400Not for new designs AO3400A SOT23-3Single General Purpose N No No AO3400A Full ProductionSOT23-3Single General Purpose N No No AO3401Not for new designs AO3401ASOT23-3Single General Purpose P No No AO3401A Full Production SOT23-3Single General Purpose P No No AO3402Full Production SOT23-3Single General Purpose N No No AO3403Full ProductionSOT23-3Single General Purpose P No No AO3404Not for new designs AO3404ASOT23-3Single General Purpose N No No AO3404A Full Production SOT23-3Single General Purpose N No No AO3406Full ProductionSOT23-3Single General Purpose N No No AO3407Not for new designs AO3407ASOT23-3Single General Purpose P No No AO3407A Full Production SOT23-3Single General Purpose P No No AO3409Full Production SOT23-3Single General Purpose P No No AO3413Full Production SOT23-3Single General Purpose P No No AO3414Full ProductionSOT23-3Single General Purpose N No No AO3415Not for new designs AO3415ASOT23-3Single General Purpose P Yes No AO3415A Full Production SOT23-3Single General Purpose P Yes No AO3416Full Production SOT23-3Single Load Switch N Yes No AO3418Full Production SOT23-3Single SMPSN No No AO3419Full Production SOT23-3Single General Purpose P Yes No AO3420Full Production SOT23-3Single Load Switch N No No AO3421Full Production SOT23-3Single General Purpose P No No AO3421E NewSOT23-3Single General Purpose P No No AO3422Full Production SOT23-3Single General Purpose N No No AO3423Full Production SOT23-3Single General Purpose P Yes No AO3424Full Production SOT23-3Single General Purpose N No No AO3434Full Production SOT23-3Single Battery Protection N Yes No AO3434A NewSOT23-3Single Battery ProtectionN Yes No AO3435Full Production SOT23-3Single SMPS P No No AO3438Full Production SOT23-3Single Load Switch N No No AO3460Full Production SOT23-3Single Load Switch N Yes No AO3701Obsolete SOT23-5Single General Purpose P Yes No AO4202New SO-8Single SMPS Low Side N No No AO4240NewSO-8SingleGeneral PurposeNNoNoConfigurationPopular Application Type Part Number StatusReplacementPartPackage ESD Diode Schottky DiodeSchottky Type专业销售进口MOS管,销售工程 王工有SOT-23 SOP-8 SOT-89 TO-252 TO-220等封装全系列进口MOS管产品广泛应用于移动电源、LED电源,电池保护,充电保护,电脑周边、MP3、MP4、DVB、DVD、应用领域、LCD显示器、LCD TV、便携式车载DVD、笔记本电脑、PDA、电源、稳压器、逆变器、高压条、适配器、数码相机、电子游戏机、电子玩具等多重数码产品尚晶是鼎日MOS管 中国总代代理,进口原装品质,超低的价格和稳定的供货,可免费提供样品测试。

Vermason 200200台式零电压离子器安装和操作说明书

Vermason 200200台式零电压离子器安装和操作说明书

Bench Top Zero Volt IoniserInstallation and Operating InstructionsTECHNICALMade in AmericaFigure 1. Vermason 200200 Bench Top Zero Volt IoniserDescriptionThe 200200 is a compact and lightweight dual steady state DC auto-balancing benchtop ioniser. The unit is normally placed at one end of the workbench or area to be neutralised. It may also be wall mounted or mounted on a shelf. The ionizer's neutralisation time will be best approximately 30.48cm to 91.44cm directly in front of the unit and will increase as the distance from the unit increases.Figure 2. Area of Optimum Charge Neutralisation“Ionizers should be considered as amethod for charge neutralisation in cases where grounding cannot be achieved.” “Air ionization can neutralise the static charge on insulated and isolated objects by producing separate charges in the molecules of the gases of thesurrounding air. When a static charge is present on objects in the workenvironment, it will be neutralised by attracting opposite polarity charges from the ionized air.” “Note thationization systems should not be used as a primary means of charge control on conductors or people.” (EN 61340-5-2 paragraph 5.2.9)“As with all ionizers, periodic mainten-ance will be needed to provideoptimum performance.” “The following list contains important points for the selection process:- charge neutralisa-tion; - discharge time; - ion balance; -product sensitivity; - solution to static problem; - environmental considera-tions, - airflow; - physical dimensions.”(EN 61340-5-2 paragraph 5.2.9.2)InstallationRemove the ionizer from the carton and inspect for damage. Included with the unit should be:1 Stand assembly with hardware 4 Rubber feet1 Emitter point cleaner 1 NIST CertificateThe input voltage should be set to your specification prior to shipping. It can be verified or reset by referring to the Maintenance section of these instructions.Attach the stand to the unit by placing the plastic spacers between the unit and the stand and securing in place using the knurled knobs. If desired, attach rubber feet to each corner of the bottom of the stand. Press feet firmly in place.Before installing the unit, verify that the AC outlet is properly connected to earth ground. The unit must have a good earth ground to maintain proper balance.Install the unit in the desired location,making sure that the airflow will not be restricted. Be sure the ON/OFF switch,located on the rear of the unit, is in the "OFF" position. Plug the power cord into the unit and then into the appropriate AC power source. This equipment has a grounding type plug that has a third(grounding) pin. This plug will only fit into a grounding type power outlet. If the plug does not fit into the outlet, contact qualified personnel to install the proper outlet. Do not alter the plug in any way.Figure 3. 220 Volt Jumper SettingIf the supply voltage drops from 200 Volts to below 170 Volts, the unit will shut down the audible alarm will beep and the LED will blink RED. The unit will automatically reset when the minimum voltage is restored.Under normal conditions, the ioniser will attract dirt and dust (especially on the emitter electrodes). To maintain optimum neutralisation efficiency and operation,cleaning should be performed on a regular basis.In the event of circuit failure, the unit will enter shutdown mode.When the unit enters shutdown mode,ionisation will be stopped, the LED on the front of the unit will change to a steady of RED, and the audible alarm will sound continuously. If the ioniser entersshutdown mode, it must be turned OFF and then back ON to reset the unit.NOTE:The AC power cord MUST be disconnected before the unit isdisassembled for maintenance. The emitter electrodes should be cleaned using the alcohol cleaners included or a swab wet with Isopropyl alcohol. First,turn the unit OFF and unplug the power cord. Then remove the rear screen by disengaging the 4 screws on back. After cleaning the emitter electrodes, reattach the rear screen using the 4 screws. Plug in the power cord and turn the unit back ON.The emitter electrodes should not requirereplacement during the life of the unit with normal handling. Replacement emitter electrodes can be ordered if necessary.The best practice would be to verify the balance of the unit with a charge plate monitor after cleaning.Neutralisation (Decay) TimesThe comparative efficiency of benchtop ionisers is determined by a standard test published by the ESD Association:Standard S3.1. Typical positive andnegative decay times (from 1000 volts to 100 volts) measured using this standard are shown in Figure 4. The performance of the ionizer was measured with the unit positioned as shown, with the fan speed on high, and without a filter.SpecificationsAir FlowThree speed fan (125fpm -250fpm; 50-100cfm).Balance±3 volt, typical; ±5 volts maximum.(Temperature range: 18.33°C to 26.67°C,R.H.: 15% to 65%)ChassisStainless steelDimensions ( with stand )24.13cm high x 15.24cm wide x 7.874cm deep.Emitter Points.050" diameter pure tungsten for improved mechanical strength and ionization stability. Fuse250 mA slow blow.High Voltage Power Supply 5.5 kV DC nominal.Input PowerAC line power, internally selectable for 220/230 VAC-50/60Hz.Ion EmissionSteady state DC with sense feedback.MountingBench top tilt adjust frame.OzoneLess than 0.05ppm Weight 2.04 kgFigure 4. Decay time in seconds from 1000 volts to 100 volts on a 15.24cm x 15.24mm charged plate per ANSI EOS/ESD S3.1.NOTE: Unauthorized servicing ormodifications to your monitor will void the product warranty and may createdangerous conditions. Servicing should be performed only at the factory, or by a Vermason approved technician.。

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Power-Efficient Pulse Width Modulation DC/DC Converters with Zero Voltage Switching ControlChangbo Long,Sasank Reddy,Sudhakar Pamarti,Lei HeEE Dept.,UCLAlongchb@,{sasank,spamarti,lhe}@T anay KarnikInteltanay.karnik@ABSTRACTThis paper proposes a power-efficient PWM DC/DC con-verter design with a novel zero voltage switching(ZVS)con-trol technique.The ZVS control is realized by an inner feed-back loop which is implemented by simple digital circuitry between the input and output of the power transistors and achieves real-time zero voltage switching(ZVS)for various loading and device parameters with power efficiencies over 90.0%.In addition,an outer feedback loop is used to ensure that the output precisely tracks a reference voltage level.We have also built the relationship between the output voltage ripple and the speed of the voltage comparators which has shown to introduce new low-frequency signals to the loops and cause significant output voltage ripples.Experiment re-sults show that the output ripple could be reduced by4x by carefully handling the generation and propagation of these low frequency signals.Categories and Subject DescriptorsB.7.1[Integrated Circuits]:Types and Design StylesGeneral TermsDesign.KeywordsDC/DC conversion,zero voltage switching.1.INTRODUCTIONPower consumption has become one of the most important issues in modern electronics due to increased complexity and speed of the system.In order to curb the effect of power on a system as a whole,multiple power domains have been pro-posed as an architecture scheme for low power design.To support multi-Vdd,an array of supply voltages need to be generated.DC/DC converters can be integrated on chip and convert the input voltage to different voltage levels in-ternally.Recently,a great deal of research[1–5]has been devoted to improving the power efficiency and reducing the area cost of on-chip DC/DC converters.However,there arePermission to make digital or hard copies of all or part of this work for personal or classroom use is granted without fee provided that copies are not made or distributed for profit or commercial advantage and that copies bear this notice and the full citation on thefirst page.To copy otherwise,to republish,to post on servers or to redistribute to lists,requires prior specific permission and/or a fee.ISLPED’06,October4–6,2006,Tegernsee,Germany.Copyright2006ACM1-59593-462-6/06/0010...$5.00.still many unsolved problems.For instance,the basic lin-ear regulator and the charge-recycling voltage regulator are designs that have been looked at as candidates for on-chip integration because there are nofilter elements.However, the relative low power efficiency,typically less than80%[1],of these designs has limited their application.In this paper,we propose design techniques and analy-sis to address the above problems for high frequency PWM buck converters.Wefirst introduce a real-time ZVS tech-nique which relies on a feedback loop as opposed to tun-ing device parameters to achieve ZVS during design time as in traditional methods[4].Our experiment results show that the feedback mechanism guarantees ZVS under differ-ent loading and device parameters.Furthermore,using the real-time ZVS technique we are able to achieve power effi-ciencies over90.0%.We then study close loop design and analysis of PWM buck converters.Our experiment results show that output voltage ripple in a closed loop PWM buck converter can be reduced up to4x by correctly analyzing and optimizing the sources that generate and propagate low frequency signals.2.BACKGROUND AND DESIGN OVERVIEW 2.1Principles of PWM Buck ConvertersFigure1:Schematic of a PWM buck converter.Compared to other designs,such as linear regulators,PWM buck converters consume more area but have higher powerefficiency.The schematic of a PWM buck converter is shownin Fig.1.It consists of two power transistors,M1and M2, with their drivers,a low-pass LCfilter consisting of L f andC f,a snubber capacitor C snub,and a pulse width modula-tor.The output voltage level V out is the DC component of the pulse signal generated by the PWM,and it isV out=V dd in·D,(1) where D is the duty cycle of the pulse signal,which is con-trolled by V ref as an input of the PWM.In fact,D=V ref8L f C f f2,(4)where L f and C f are the inductance and capacitance of the LCfilter and f is the frequency of the pulse signal.f is also called the operation frequency of the buck converter. Equation(4)shows that to keep∆V out at a low level,L f and/or C f has to be large if the operation frequency f is low.In other words,an effective way to reduce the area of the LCfilter in the buck converter is to use a high operation frequency[2].However,a high operation frequency leads to a high switching power loss.To reduce the switching power loss,a technique called zero voltage switch(ZVS)has been widely adopted.As shown in[4],ZVS ensures that both power transistors switch under a zero voltage drop between source and drain.2.2Overview of the Proposed TopologyVctrlFigure2:Overview of the proposed circuit topology.Our study in this paper is based on the circuit topology shown in Figure2.This circuit contains two feedback loops. The outer loop consists of two power transistors M1and M2, LCfilter L f and C f,voltage comparator V C1,RC integra-tor R i and C i,pulse modulation element V C2,and real-time ZVS circuitry.The inner loop starts from the output of the two power transistors,passes through the ZVS circuitry and ends at the input of the two power transistors.The outer loop ensures that the output voltage level V out tracks the reference voltage level V ref.It is considered a negative feedback loop since there are only one set of nega-tive components,the power transistors,in the entire looop. For example,if V out is higher than V ref,the output of volt-age comparator V C1is high,C i is charged,and the voltage level at the positive input of V C2is increased,which in-creases the duty cycle of the switching signal and therefore decreases V out.The design of voltage comparator is adopted from[7], which has shown high resolution and low power consump-tion.The topology of the voltage comparator is shown in Figure3,which is composed by an input amplification stage, twoflipflops and a RS latch.Two clock signals are used to clear up previous results and evaluations.More details are described in[7].The real-time ZVS technique is achieved by the inner feed-back loop.To avoid the influence of startup strike,a detec-tion sub-circuit is included as shown in Figure2.The idea is not to startupthe ZVS circuitry until V out has been sta-bilized.More details will be described in Section4.Figure3:Topology of the voltage comparator.3.CLOSE LOOP DESIGN AND ANALYSIS 3.1Analysis on output voltage rippleFigure4:Illustration of changes in duty cycle in the switching signal.Our study is based on the design shown in Figure2.The voltage comparator V C2in thefigure modulates the duty cycle of the switching signal feeding the two power transis-tors and this modulation introduces a signal that containsa wide range of frequencies.Low frequency components ofthis signal may pass the LCfilter and cause a voltage ripplewith a frequency approximately equal to the frequency of the LCfilter,1/(2πpL f C f.(5)By Fourier transformation,the residual signals can be ex-pressed as follows,f(t)=2V dd2n+1)cos(2n+1)ωt +∞Xn=0(cos(2n+1)ωt1−cos(2n+1)ωt2π∞Xn=0p2n+1cos((2n+1)ωt+φ)≈2V ddwhereω=1L f C f.(6)Notice that t2−t1=T·∆Dπp V x,(9)andV m2=V ctrl·V xas shown in Figure2.To drive M1,V x is compared withV high=V DD−∆v and only when V x is is higher thanV high M1can open.Similarly,to drive M2,V x is comparedwith a low voltage level V low=∆v and only when V x is lowerthan V low,M2can open.In order to reduce the overshoot onV x,we use a∆v slightly larger than zero(0.3v).However,as shown in our experiment results,it is impossible to fullyeliminate overshoot.Overall,the real-time ZVS scheme presented as part ofthis design is very unique in the fact that it does not rely onmanually calculating the duty cycle delays for a particulardesign.Although there are designs that do automatic ZVScontrol,they do not meet the power and area requirementsfor on-chip high frequency applications[8,9].4.3ZVS startup detectionInitially,when the circuit is cold started,there is a periodof time where the output signals have abnormally large vari-ation.During this startup period there is no need to turnon the automatic ZVS calibration control for the system.Inorder to avoid tuning ZVS during the startup period,a se-ries of Dflip-flops are used as delay elements to prevent thestartup of the ZVS calibration scheme until after the initialtransient spikes,as shown in Fig.2.5.EXPERIMENT RESULTS5.1Close loop design and analysisTo verify the idea that the output voltage ripple is pro-portional to the smallest duty cycle change∆D,we haveimplemented the voltage comparator,as in Figure3,at twodifferent clock rates.One voltage comparator operates at400MHz and the other at1.6GHz frequencies.We comparethe output voltage ripple of the PWM buck converters im-plemented with these two comparators in Figure5.Notethat130nm technology is used,the V dd voltage is1.3Volt,and the reference voltage level is0.85Volt.As shown inthefigure,the voltage ripple of the400MHz comparator isabout11.7%as compared to the reference voltage,while thevoltage ripple of the1.6GHz comparator is2.9%.By in-creasing the frequency of the comparator by4X,we notice areduction in ripple by around4X.These experiment resultsshow that when designing the closed loop PWM buck con-verter,the elements of the closed loop need to be carefullyconsidered so that the output voltage ripple is minimized.Figure 5:Comparison of voltage ripple between buck converters implemented by a 0.4GHZ voltage compara-tor and 1.6GHz voltagecomparator.(a)(b)(c)(d)(e)(f)Figure 7:Design-time ZVS under loading of 5ohms (a),10ohms (b),and 50ohms (c)and real-time ZVS with feedback loop under loading of 5ohms (d),10ohms (e),and 50ohms (f).(A)and (c)fails ZVS.5.2ZVS controlOne of the strong points of the design presented in this paper is the fact that the power of the transistors is con-sistent over a multitude of loads.This is mainly due to the fact that there is a real-time ZVS control system established in the circuit.Figure 7contains a comparison between design-time ZVS without feedback and real-time ZVS with feedback.In the case of the load of 5and 50ohms with design-time ZVS,one can see that the circuit is out of the ZVS mode of operation.With a load of 5ohms,the C snub capacitor is charged too slow and the voltage of V x does not transition from the lower state to the higher state before the M 1transistor switches on.On the other hand with a load of 50ohms,the design-time ZVS circuit discharges the C snub too slowly and the circuit is in a non optimal energy efficiency state once again.The real-time circuit always stays in the ZVS mode of opera-tion with the various loads.Although,there is an overshoot (refer to Section 4.2)for the real-time ZVS circuit,this does not affect the energy usage of the power transistors.Overall,not having a proper ZVS control system will cause problems in terms of power usage of the switch tran-sistors.In terms of overall power efficiency of the circuit,both ZVS operation and the actual magnitude of the current through the load play significant roles.But our experiments show that if the proper load current is used with real-time ZVS,power efficiencies are greater than 90%consistently for various loads.6.CONCLUSIONIn this paper,we have designed a novel PWM circuit that can be used to provide a range of Vdd levels for a variety of loads by two feedback loops.With the use of an inner feed-back loop between the output and input of the power tran-sistors,we are able to ensure real-time zero voltage switch-ing.This enables the reduction of power consumed by these transistors and achieves power efficiencies over 90%for a va-riety of loads.Also,an outer feedback loop is employed in the PWM circuit to track the reference voltage level.We show that this closed loop should be propriately modeled and designed to ensure a low output voltage ripple.7.REFERENCES[1]S.Rajapandian,Z.Xu,and K.Shepard,“Charge-recyclingvoltage domains for energy-efficient low-voltage operation of digital cmos circuits,”in Computer Design,2003.Proceedings.21st International Conference on ,pp.98–102,2003.[2]V.Kursan,S.G.Narendra,V.K.De,and E.G.Friedman,“Analysis of buck converters for on-chip integration with a dual supply voltage microprocessor,”IEEE Trans.VLSI Syst.,vol.11,pp.514–522,June 2003.[3]G.Schrom,P.Hazucha,J.-H.Hahn,V.Kursun,D.Gardner,S.Narendra,T.Karnik,and V.De,“Feasibility of monolithic and 3d-stacked dc-dc converters formicroprocessors in 90nm technology generation,”in Proc.Intl.Symp.Low Power Electronics and Design ,pp.263–268,2004.[4] A.J.Stratakos,S.R.Sanders,and R.W.Brodersen,“Alow-voltage cmos dc-dc converter for a portablebattery-operated system,”in Power Electronics Specialists Conference,PESC ’94Record.,25th Annual IEEE ,pp.619–626,June 1994.[5] A.J.Stratakos,“High-efficiency low-voltage dc-dcconversion for portable applications,”PhD dissertation,University of California,Berkeley ,1998.[6] D.W.Hart,ed.,Introduction to Power Electronics .PrenticeHall,Upper Saddle River,N.J.,1997.[7]G.Yin,F.Eynde,and W.Sansen,“A high-speed CMOScomparator with 8-b resolution,”IEEE Journal of Solid-state Circuits ,vol.27,pp.208–211,Feb.1992.[8]Y.Jang and M.Jovanovic,“A new zvs-pwm full-bridgeconverter,”in IEEE International Telecommunications Energy Conference ,pp.232–239,Septemeber 2002.[9]J.Cho,J.Sabate,G.Hua,and F.Lee,“Zero-voltage andzero-current-switching full bridge pwm converter for high 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