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Unit1CircuitComponents1.1Text1.2ReadingMaterials
1.1Text
Resistors:Aresistorisanelectricalcomponentthatresiststheflowofelectricalcurrent.Theamountofcurrent(I)flowinginacircuitisdirectlyproportionaltothevoltageacrossitandinverselyproportionaltotheresistanceofthecircuit.ThisisOhmlawandcanbeexpressedasaformula: .Theresistorisgenerallyalineardeviceanditscharacteristicsformastraightlinewhenplottedonagraph.
Resistorsareusedtolimitcurrentflowingtoadevice,therebypreventingitfromburningout,asvoltagedividerstoreducevoltageforothercircuits,astransistorbiasingcircuits,andtoserveascircuitloads.
Generally,resistors(Fig1.1)consistofcarboncomposition,wire-wound,andmetalfilm.Thesizeofresistorsdependsonpowerratings.Largersizesarereferredtoaspowerresistors.Variableresistorsareadjustable:rheostats,potentiometers,andtrimmerpots.Precisionresistorshaveatoleranceof1%orless.
Fig1.1VariousResistors
IfyouareabitseriousabouttheelectronicshobbyIrecommendlearningthe“ColorCode”.Itmakesaloteasier.Thesamecolorcodeisusedforeverythingelse,likecoils,capacitorsetc.Again,justthecolorcodeassociatedwithanumber,like:black=0brown=1red=2,etc.Fig1.2isanexample;itisa4-bandresistor.
Canyou“create”yourownresistors?Ofcauseandnotdifficult.Hereishowtodoit.Drawalineonapieceofpaperwithasoftpencil,HBor2HBwilldofine.Makethelinethickandabout2inches(5cm)long.Withyourmultimeter,measuretheohm’svalueofthislinebyputtingaprobeoneachsideoftheline;makesuretheprobesaretouchingthecarbonfromthepencil.Thevaluewouldprobablybearoundthe800kto1.5Mdependingline.Theresistancewilldropconsiderably,ifyouerasesomeofit(length-wiseobviously!).Youcanalsousecarbonwithsiliconglueandwhenitdriesmeasuretheresistance,etc.
Fig1.2Anexampleofresistorcolorcode
Capacitors:Acapacitorisanelectricaldevicethatcantemporarilystoreelectricalenergy.Basically,acapacitorconsistsoftwoconductors(metalplates)separatedbyadielectricinsulatingmaterial(Fig1.3(a)),whichincreasestheabilitytostoreacharge.
Fig1.3Capacitor
Thedielectriccanbepaper,plasticfilm,mica,ceramic,airoravacuum.Theplatescanbealuminumdiscs,aluminumfoilorathinfilmofmetalappliedtooppositesidesofasoliddielectric.Theconductor-dielectric-conductorsandwichcanberolledintoacylinderorleftflat,thesymbolsofcapacitorareshowninFig1.3(b).
AcapacitorwillblockDCcurrent,butappearstopassACcurrentbycharginganddischarging.ItdevelopsanACresistance,knownascapacitivereactance,whichisaffectedbythecapacitanceandACfrequency.TheformulaforcapacitivereactanceisXC?=?1/(2
fC),withunitsofohms.
Inductors:Aninductorisanelectricaldevice,whichcantemporarilystoreelectromagneticenergyinthefieldaboutitaslongascurrentisflowingthroughit.Theinductorisacoilofwirethatmayhaveanaircoreoranironcoretoincreaseitsinductance.Apoweredironcoreintheshapeofacylindermaybeadjustedinandoutofthecore.
Aninductortendstoopposeachangeinelectricalcurrent,ithasnoresistancetoDCcurrentbuthasanACresistancetoACcurrent,knownasinductivereactance,thisinductivereactanceisaffectedbyinductanceandtheACfrequencyandisgivenbytheformulaXL?=?2
fL,withunitsofohms.InductorsareusedforfilteringACcurrent,increasingtheoutputoftheRF(RadioFrequency)amplifier.
Inductorsareavailableinvarietyofshapes(Fig1.4):aircore,ironcore(whichmaylooklikeatransformer,buthasonlytwoleads),toroidal(doughnutshaped),smalltubularwithepoxy,RFchokewithseparatecoilsonacylinder,andtunableRFcoilwithascrewdriveradjustment.
Fig1.4Variousinductors
TechnicalWordsandPhrases
reactance n.電抗
resistance n.【電】電阻值,中文有時(shí)簡稱電阻
resistor
n.【電】電阻器,中文有時(shí)簡稱電阻
voltage
n.【電工】電壓,伏特?cái)?shù);電壓(電位差)
capacitance n.電容量
capacitor n.電容器
charge n.負(fù)荷,電荷,充電v.裝滿,充電
dielectric n.電介質(zhì),絕緣體adj.非傳導(dǎo)性的
electrical adj.電的,有關(guān)電的
formula n.公式,規(guī)則,客套話
inductance n.電感量,電感值
inductor n.誘導(dǎo)物,感應(yīng)器,電感器
insulating adj.絕緣的
multimeter n.萬用表vt.多點(diǎn)測(cè)量
probe n.探針,外太空探測(cè)器;探測(cè)飛船,探索
beinverselyproportionalto 與……成反比
beaffectedby… 受……影響
beavailable 是可利用的,可用的
bedirectlyproportionalto
與……成正比
beexpressedasaformula 用公式表示成……
beproportionalto 與……成比例
beusedto…
被用于……
invariousshapesandsizes 各種形狀和尺寸
toserveas… 用作……
1.1.1Exercises
1.PutthePhrasesintoEnglish
(1)運(yùn)算放大器; (2)傳遞函數(shù);
(3)電子器件; (4)集成電路;
(5)反饋電路; (6)性能參數(shù)。
2.PutthePhrasesintoChinese
(1)electricalcomponents; (2)Ohmlaw;
(3)limitcurrent; (4)voltagedivider;
(5)transistorbiasingcircuits.
3.Translation
(1)Resistorsareusedtolimitcurrentflowingtoadevice,therebypreventingitfromburningout,asvoltagedividerstoreducevoltageforothercircuits,astransistorbiasingcircuits,andtoserveascircuitloads.
(2)IfyouareabitseriousabouttheelectronicshobbyIrecommendlearningthe“ColorCode”.
(3)AcapacitorwillblockDCcurrent,butappearstopassACcurrentbycharginganddischarging.
(4)Capacitorsareavailableinvariousshapesandsizes.
(5)Capacitorsareusedforfiltering,bypassingsignals,fortimingcircuits,andforradio-frequency(RF)tuningcircuits.
(6)Aninductorisanelectricaldevice,whichcantemporarilystoreelectromagneticenergyinthefieldaboutitaslongascurrentisflowingthroughit.
(7)Theinductivereactanceisaffectedbyinductanceandtheacfrequency.
(8)Theinputvoltageistotheprimarywindingandtheinducedvoltageistakenoffthesecondarywinding.
1.1.2參考譯文
電阻器:電阻器是一種能阻礙電流流動(dòng)的電子器件。電阻器中流過的電流與加在電阻兩端的電壓成正比,與電阻的阻值成反比。這就是歐姆定律,可以用公式表示成I=UR/R。
電阻器通常是線性器件,它的(伏安)特性曲線是一條直線。
電阻器常用作限流器,以限制流過器件的電流,以防止器件因流過的電流過大而燒壞。電阻器也可以用作分壓器,以減小其他電路的電壓,如晶體管偏置電路。電阻器還可用作電路的負(fù)載。
一般來說,電阻有碳(膜)電阻、線繞電阻和金屬膜電阻(如圖1.1所示),電阻器尺寸的大小與電阻的(額定)功率有關(guān),尺寸比較大的電阻器通常是高功率電阻器。可變電阻器是電阻值可調(diào)節(jié)的電阻器,如變阻器、電位器和微調(diào)電位器。精密電阻器是指其誤差率在1%或更小的電阻器。
如果你對(duì)電子技術(shù)頗有興趣,建議學(xué)會(huì)電阻的“彩色條形碼”識(shí)別方法,這樣會(huì)帶來很多方便。而且這種彩色條形碼標(biāo)注方法在其他器件上也適用,如線圈(電感)、電容等。這種方法是用彩色表示數(shù)字,如黑色=0,棕色=1,紅色=2等,圖1.2是個(gè)彩色條形碼電阻的例子。
自己可以制作一個(gè)電阻(器)嗎?當(dāng)然可以,而且也不難。這里教你如何做一個(gè)電阻(器),用一支軟鉛筆(HB鉛筆或用2HB鉛筆更好),在紙上畫一段大約2英寸(5cm)長的粗線。用萬用表測(cè)量這段線的歐姆值,(方法是)把萬用表的兩個(gè)探筆分別與鉛筆線的兩端相接觸,一定要讓探筆與線端的碳接觸。根據(jù)線的粗細(xì),電阻值大約為800kΩ~1.5MΩ。如果你擦掉一些線,使線明顯變短,電阻值就會(huì)變小。你也可以用摻有硅膠的碳粉來制作電阻器,當(dāng)硅膠干了以后測(cè)量其電阻值等。
電容器:電容器是可以暫時(shí)存儲(chǔ)電能的電子器件。電容器一般由兩塊導(dǎo)體(金屬極板)組成(見圖1.3(a)),中間用一層不導(dǎo)電的絕緣材料隔開,這層絕緣材料可以增加電容存儲(chǔ)電荷的本領(lǐng)(即增大電容量)。
絕緣材料可以是紙、塑料片、云母、陶瓷材料、空氣或真空。極板可以是薄鋁板、鋁箔或在一片兩面各貼上一層金屬薄膜的絕緣板??梢灾苯影岩粋€(gè)這種導(dǎo)體-絕緣體-導(dǎo)體(三明治式)制成平板電容器,也可以把它卷起來成為圓柱形電容器。電容器的符號(hào)如圖1.3(b)所示。
電容器隔直流電,但能以充電和放電的方式通過交流電。它構(gòu)成的交流電阻抗稱為容抗。容抗與電容量和交流電的頻率有關(guān),容抗的公式為XC=1/(2πfC),其單位為歐姆。
電感器:當(dāng)電流流過電感器時(shí),電感器周圍就有電磁場,電感器是以電磁場的形式暫時(shí)存儲(chǔ)電磁能量的電子器件。電感器是一組線圈,有的電感器線圈中有可增加其電感量的鐵芯,可調(diào)電感有一個(gè)強(qiáng)磁的圓柱狀鐵芯,通過調(diào)節(jié)鐵芯可以增加或減少電感量。
電感量有阻礙電流變化的趨勢(shì),對(duì)直流電而言,電感器是沒有阻礙作用的,但對(duì)交流電來說,電感器有一個(gè)交流阻抗,稱為感抗。這個(gè)感抗與電感量和交流電的頻率有關(guān),可以用公式表示為XL=2πfL,其單位為歐姆。電感器可以用來濾波、增加RF(無線電頻率)放大器的輸出。電感器有各式各樣的形狀(如圖1.4所示),空芯的、鐵芯的(鐵芯的有時(shí)看起來像個(gè)變壓器,但只有兩個(gè)端口)、環(huán)狀的(圓環(huán)形的)、管狀的(以環(huán)氧樹脂為材料),RF扼流圈是由圓柱上分開的線圈構(gòu)成,而且可調(diào)的線圈帶有一把調(diào)整螺絲刀。
1.2ReadingMaterials
1.2.1HowSemiconductorsWork
Semiconductorshavehadamonumentalimpactonoursociety.Youfindsemiconductorsattheheartofmicroprocessorchipsaswellastransistors.Anythingthat’scomputerizedorusesradiowavesdependsonsemiconductors.
Today,mostsemiconductorchipsandtransistorsarecreatedwithsilicon.Youmayhaveheardexpressionslike“SiliconValley”andthe“siliconeconomy,”andthat’swhy—siliconistheheartofanyelectronicdevice.
Adiodeisthesimplestpossiblesemiconductordevice,andisthereforeanexcellentbeginningpointifyouwanttounderstandhowsemiconductorswork.Inthisarticle,you’lllearnwhatasemiconductoris,howdopingworksandhowadiodecanbecreatedusingsemiconductors.Butfirst,let’stakeacloselookatsilicon.
Siliconisaverycommonelement—forexample,itisthemainelementinsandandquartz.Ifyoulook“silicon”upintheperiodictable(Fig1.5),youwillfindthatitsitsnexttoaluminum,belowcarbonandabovegermanium.
Fig1.5Siliconsitsnexttoaluminumandbelowcarbonintheperiodictable
Carbon,siliconandgermanium(germanium,likesilicon,isalsoasemiconductor)haveauniquepropertyintheirelectronstructure—eachhasfourelectronsinitsouterorbital.Thisallowsthemtoformnicecrystals.Thefourelectronsformperfectcovalentbondswithfourneighboringatoms,creatingalattice.Incarbon,weknowthecrystallineformasdiamond.Insilicon,thecrystallineformisasilvery,metallic-lookingsubstance.
Inasiliconlattice(Fig1.6),allsiliconatomsbondperfectlytofourneighbors,leavingnofreeelectronstoconductelectriccurrent.Thismakesasiliconcrystalaninsulatorratherthanaconductor.
Fig1.6Siliconlattice
Metalstendtobegoodconductorsofelectricitybecausetheyusuallyhave“freeelectrons”thatcanmoveeasilybetweenatoms,andelectricityinvolvestheflowofelectrons.Whilesiliconcrystalslookmetallic,theyarenot,infact,metals.Alloftheouterelectronsinasiliconcrystalareinvolvedinperfectcovalentbonds,sotheycan’tmovearound.Apuresiliconcrystalisnearlyaninsulator—verylittleelectricitywillflowthroughit.
Butyoucanchangeallthisthroughaprocesscalleddoping.Youcanchangethebehaviorofsiliconandturnitintoaconductorbydopingit.Indoping,youmixasmallamountofanimpurityintothesiliconcrystal.
Therearetwotypesofimpurities:
N-type-InN-typedoping,phosphorusorarsenicisaddedtothesiliconinsmallquantities.Phosphorusandarseniceachhavefiveouterelectrons,sothey’reoutofplacewhentheygetintothesiliconlattice.Thefifthelectronhasnothingtobondto,soit’sfreetomovearound.Ittakesonlyaverysmallquantityoftheimpuritytocreateenoughfreeelectronstoallowanelectriccurrenttoflowthroughthesilicon.N-typesiliconisagoodconductor.Electronshaveanegativecharge,hencethenameN-type.
P-type-InP-typedoping,boronorgalliumisthedopant.Boronandgalliumeachhaveonlythreeouterelectrons.Whenmixedintothesiliconlattice,theyform“holes”inthelatticewhereasiliconelectronhasnothingtobondto.Theabsenceofanelectroncreatestheeffectofapositivecharge,hencethenameP-type.Holescanconductcurrent.Aholehappilyacceptsanelectronfromaneighbor,movingtheholeoveraspace.P-typesiliconisagoodconductor.
AminuteamountofeitherN-typeorP-typedopingturnsasiliconcrystalfromagoodinsulatorintoaviable(butnotgreat)conductor—hencethename“semiconductor”.
N-typeandP-typesiliconarenotthatamazingbythemselves;butwhenyouputthemtogether,yougetsomeveryinterestingbehavioratthejunction.That’swhathappensinadiode.
Adiode(Fig1.7)isthesimplestpossiblesemiconductordevice.Adiodeallowscurrenttoflowinonedirectionbutnottheother.Youmayhaveseenturnstilesatastadiumorasubwaystationthatletpeoplegothroughinonlyonedirection.Adiodeisaone-wayturnstileforelectrons.
Fig1.7Diode
WhenyouputN-TYPEandP-TYPEsilicontogetherasshowninthisdiagram,yougetaveryinterestingphenomenonthatgivesadiodeitsuniqueproperties.
EventhoughN-TYPEsiliconbyitselfisaconductor,andP-TYPEsiliconbyitselfisalsoaconductor,thecombinationshowninthediagramdoesnotconductanyelectricity.ThenegativeelectronsintheN-typesilicongetattractedtothepositiveterminalofthebattery.
ThepositiveholesintheP-TYPEsilicongetattractedtothenegativeterminalofthebattery.Nocurrentflowsacrossthejunctionbecausetheholesandtheelectronsareeachmovinginthewrongdirection.Ifyouflipthebatteryaround,thediodeconductselectricityjustfine.ThefreeelectronsintheN-TYPEsiliconarerepelledbythenegativeterminalofthebattery.TheholesintheP-TYPEsiliconarerepelledbythepositiveterminal.AtthejunctionbetweentheN-TYPEandP-TYPEsilicon,holesandfreeelectronsmeet.Theelectronsfilltheholes.Thoseholesandfreeelectronsceasetoexist,andnewholesandelectronsspringuptotaketheirplace.Theeffectisthatcurrentflowsthroughthejunction.
1.2.2ThePowerSupply
Apowersupplyisadevicethattakesanincomingelectricalcurrentandamplifiesittolevelsrequiredbyvariousdevices.Inmanyinstances,apowersupplyisalsoimplementedtotaketheincomingelectricityanddeliveritacrossmanyotherelectronicdevices,oftenatdifferentpresetlevels.Thisdeviceallowsmanufacturerstocreateelectronicsandmachinerythatcanhandlemanydifferenttasksfromasinglesourceofpower,withouttheneedforvariousadaptersandadditionalhardware.Withinotherdevices,apowersupplyisusedtotransformvarioustypesofpowerintoacompatibleformattobestored,likesolarenergytoelectricalenergy.
Perhapsthemostcommonuseofapowersupplyiswithincomputersystems.Aselectricityentersthepowersupply,itismomentarilystoredandthendistributedtonumerousfunctionsthroughoutthesystem,allowingthemotherboard,harddrive,andothervariousdevicestoreceiveelectricityinordertofunction.Eachoneoftheseitemsrequiresaseparatevoltage(amperes),anditisdeliveredthroughspecializedconnectorsthatattachinacertainmanner.Forexample,motherboardsrequireeithera20-pinpowersupplyora24-pinpowersupply,andtheyarenotinterchangeablewithoutthepurchaseofanadditionaladapter.
Modernvehiclesalsorequireatypeofpowersupplyinordertofunction,anditisreferredtoasanalternator(Fig1.8).Althoughthewiringanddesignmaybedifferent,itessentiallyworksintheexactsamemannerbytakingincomingpoweranddeliveringitthroughoutthevehicleatthenecessarylevels.Alternatorscanbefoundoneverythingfromlawnmowerstoseacraftandindustrialequipment,andwithoutthem,thedeviceswouldberendereduseless.
Fig1.8Alternatorformodernvehicles
Anothercommontypeofpowersupplycanbefoundonwindmillsandsolarpanels(Fig1.9),anditsprimaryfunctionistoconvertvarioustypesofenergyintoelectricitysothatitcanbestoredanddistributedacrossagrid.Thistypeofpowersupplyisreferredtoasagenerator,anditisoftenafree-standingobjectthatisinstalledbetweenthepowersourceandthestorageunit.Homeandcommercialgenerators,usedduringpoweroutages,alsoworkoffofthissamepremisebytransformingpetroleumproductsintoelectricalenergybymeansofanengine.Manytypesofindustrialtoolsalsoimplementatypeofgenerator.Othercommontypesofpowersuppliesareusedwithincircuitbreakers,battery-powereditemsandtransformers.
Fig1.9Solarpanels
1.2.3MOSFETSwitches
TheN-channel,Enhancement-modeMOSFEToperatesusingapositiveinputvoltageandhasanextremelyhighinputresistance(almostinfinite)makingitpossibletointerfacewithnearlyanylogicgateordrivercapableofproducingapositiveoutput.Also,duetothisveryhighinput(Gate)resistancewecanparalleltogethermanydifferentMOSFET’suntilweachievethecurrenthandlinglimitrequired.WhileconnectingtogethervariousMOSFET’smayenableustoswitchhighcurrentorhighvoltageloads,doingsobecomesexpensiveandimpracticalinbothcomponentsandcircuitboardspace.ToovercomethisproblemPowerFieldEffectTransistorsorPowerFET’swheredeveloped.
WenowknowthattherearetwomaindifferencesbetweenFET’s,Depletion-modeforJFET’sandEnhancement-modeforMOSFET’sandonthispagewewilllookatusingtheEnhancement-modeMOSFETasaSwitch.
ByapplyingasuitabledrivevoltagetotheGateofanFETtheresistanceoftheDrain-Sourcechannelcanbevariedfroman“OFF-resistance”ofmanyhundredsofk?’s,effectivelyanopencircuit,toan“ON-resistance”oflessthan1?,effectivelyashortcircuit.WecanalsodrivetheMOSFETtoturn“ON”fastorslow,ortopasshighcurrentsorlowcurrents.ThisabilitytoturnthepowerMOSFET“ON”and“OFF”allowsthedevicetobeusedasaveryefficientswitchwithswitchingspeedsmuchfasterthanstandardbipolarjunctiontransistors.
AnexampleofusingtheMOSFETasaswitch:
Inthiscircuit(Fig1.10)arrangementanEnhancement-modeN-channelMOSFETisbeingusedtoswitchasimplelamp“ON”and“OFF”(couldalsobeanLED).ThegateinputvoltageVGSistakentoanappropriatepositivevoltageleveltoturnthedeviceandthelampeitherfully“ON”,(VGS=+ve)orazerovoltageleveltoturnthedevicefully“OFF”(VGS=0).Iftheresistiveloadofthelampwastobereplacedbyaninductiveloadsuchasacoilorsolenoid,a“Flywheel”diodewouldberequiredinparallelwiththeloadtoprotecttheMOSFETfromanyback-emf.
Fig1.10CircuitwithanEnhancement-modeN-channelMOSFET
AboveshowsaverysimplecircuitforswitchingaresistiveloadsuchasalamporLED.ButwhenusingpowerMOSFET’stoswitcheitherinductiveorcapacitiveloadssomeformofprotectionisrequiredtopreventtheMOSFETdevicefrombecomingdamaged.Drivinganinductiveloadhastheoppositeeffectfromdrivingacapacitiveload.Forexample,acapacitorwithoutanelectricalchargeisashortcircuit,resultinginahigh“inrush”ofcurrentandwhenweremovethevoltagefromaninductiveloadwehavealargereversevoltagebuildupasthemagneticfieldcollapses,resultinginaninducedback-emfinthewindingsoftheinductor.
ForthepowerMOSFETtooperateasananalogueswitchingdevice,itneedstobeswitchedbetweenits“Cut-offRegion”whereVGS=0andits“SaturationRegion”whereVGS(on).
ThepowerdissipatedintheMOSFET(PD)dependsuponthecurrentflowingthroughthechannelIDatsaturationandalsothe“ON-resistance”ofthechannelgivenasRDS(on).
Forexample:
Letsassumethatthelampisratedat6V,24Wandisfully“ON”andthestandardMOSFEThasachannel“ON-resistance”(RDS(on))valueof0.1ohms.CalculatethepowerdissipatedintheMOSFETswitch.
Thecurrentflowingthroughthelampiscalculatedas:
ThenthepowerdissipatedintheMOSFETwillbegivenas:
Youmaythink,wellsowhat!butwhenusingtheMOSFETasaswitchtocontrolDCmotorsorhighinrushcurrentdevicesthe“ON”channelresistance(RDS(on))isveryimportant.Forexample,MOSFET’sthatcontrolDCmotors,aresubjectedtoahighin-rushcurrentasthemotorfirstbeginstorotate.ThenahighRDS(on)channelresistancevaluewouldsimplyresultinlargeamountsofpowerbeingdissipatedwithintheMOSFETitselfresultinginanexcessivetemperaturerise,andwhichinturncouldresultintheMOSFETbecomingveryhotanddamagedduetoathermaloverload.
ButalowRDS(on)valueontheotherhandisalsodesirabletohelpreducetheeffectivesaturationvoltage(VDS(sat)=ID×RDS(on))acrosstheMOSFET.WhenusingMOSFET’soranytypeofFieldEffectTransistorforthatmatterasaswitchingdevice,itisalwaysadvisabletoselectonesthathaveaverylowRDS(on)valueoratleastmountthemontoasuitableheatsinktohelpreduceanythermalrunawayanddamage.
PowerMOSFETMotorControl
BecauseoftheextremelyhighinputorGateresistancethattheMOSFEThas,itsveryfastswitchingspeedsandtheeaseatwhichtheycanbedrivenmakesthemidealtointerfacewithop-ampsorstandardlogicgates.However,caremustbetakentoensurethatthegate-sourceinputvoltageiscorrectlychosenbecausewhenusingtheMOSFETasaswitchthedevicemustobtainalowRDS(on)channelresistanceinproportiontothisinputgatevoltage.
Forexample,donotapplya12Vsignalifa5Vsignalvoltageisrequired.PowerMOSFET’scanbeusedtocontrolthemovementofDCmotorsorbrushlesssteppermotorsdirectlyfromcomputerlogicorPulse-widthModulation(PWM)typecontrollers.AsaDCmotoroffershighstartingtorqueandwhichisalsoproportionaltothearmaturecurrent,MOSFETswitchesalongwithaPWMcanbeusedasaverygoodspeedcontrollerthatwouldprovidesmoothandquietmotoroperation.
SimplePowerMOSFETMotorController
AsimplepowerMOSFETmotorcontrollerisshowninFig1.11.Asthemotorloadisinductive,asimple“Freewheeling”diodeisconnectedacrosstheloadtodissipateanybackemfgeneratedbythemotorwhentheMOSFETturnsit“OFF”.
TheZenerdiodeisusedtopreventexcessivegate-sourceinputvoltages.
Fig1.11SimplePowerMOSFETMotorController
1.2.4FrequencyDividers
Ifweapplyafixed-frequencypulsetraintoacounter,ratherthanindividualpulsescomingatrandomintervals,webegintonoticesomeinterestingcharacteristics,andsomeusefulrelationshipsbetweentheinputclocksignalandtheoutputsignals.
Considerasingleflip-flopwithacontinuoussuccessionofclockpulsesatafixedfrequency,suchastheoneshowninFig1.12.WenotethreeusefulfactsabouttheoutputsignalsseenatQand:
1.Theyareexactlyinvertedfromeachother.
2.Theyareperfectsquarewaves(50%dutycycle).
3.Theyhaveafrequencyjusthalfthatoftheclockpulsetrain.
Fig1.12Clockpulsesatafixedfrequencyofasingleflip-flop
Thedutycycleofanyrectangularwaveformreferstothepercentageofthefullcyclethatthesignalremainsatlogic1.Ifthesignalspendshalfitstimeatlogic1andtheotherhalfatlogic0,wehaveawaveformwitha50%dutycycle.Thisdescribesaperfect,symmetricalsquarewave.
Frequencydivisionbyanoddnumberisalsopossible.ThecircuitshowedinFig1.13isademonstrationofadivide-by-3counter.NogatesarerequiredtocontrolthesequenceifJKflip-flopsareused;feedingtheoutputsignalsbacktotheappropriateinputsissufficient.
Ofcourse,itisnotpossibletogetasymmetrical(50%dutycycle)squarewavewiththiscircuit.TheAoutputisatlogic1fortwoclockpulsesoutofthree;theBoutputisatlogic1foroneclockpulseoutofthree.Thus,dutycyclesof1/3(33.333%)and2/3(66.667%)areavailable.
Fig1.13Adivide-by-3counter
Thisrenditionofadivide-by-5counter(Fig1.14)actuallyfollowsthenormaldecimal(orbinary)countfromzerothroughfour.TheprimarycontrolfeatureisthefeedbackfromtheC’outputtoflip-flopA’sJinput.Thisfeedbackpreventsflip-flopAfromswitchingfromlogic0tologic1inanefforttogofromacountoffourtoacountoffive.Atthesametime,theCoutputisappliedtoflip-flopC’sKinputtoforceflip-flopCtoresetonthenextclockpulse.
Thisparticulararrangementisoftencombinedwithasingleflip-flopinanICpackage.Thecombinationcanthenbeusedeitherasanormaldecimalcounterorasadivide-by-10counterwithatruesquare-waveoutput.
Fig1.14Adivide-by-5counter
Ifitisnotnecessarytomaintainastandardbinarycountingsequence,wecanofteninterconnecttheflip-flopssoastoeliminatetheneedforanyextragates,asshowntotheleft.NotethattheKinputstobothflip-flopsAandBareconnectedtologic1.Asaresult,outputsAandBwillremainatlogic1foronlyoneclockpulseatatime,andwillthenresettologic0.OutputCwilltoggleafterBgoestologic1.
OutputChasa40%dutycycle.OutputsAandBproducetwooutputpulsesforeachpulsefromC,butnotatequalintervals.Thecountingsequenceis0,1,2,5,6,0,etc.
Thiscountercircuitactuallyhasaflawasshown:ifitpowersupinstate4(A=0,B=0,
C=1),itwillremaininthatstateandbeunabletochangeatall.Tocorrectthis,wecandisconnectC’sKinputfromoutputB,andconnectittooutputA’instead.Nowthefirstclockpulsewillforcethecircuittostate0(000),fromwhichthecountwillproceednormally.Thischangewillnotaffectthenormalcountingsequence,becausealogic1attheKinputcannotpreventtheflip-flopfromchangingtoalogic1,andwouldforceCbacktoalogic0atthesametimeitwouldchangeanyway.
Othercountingsequencesarealsopossible,ofcourse.Ifaneedexiststohavetwoormoresignalsinaparticularfrequencyrelationshipwitheachother,someextensionorvariationonthecircuitsshownherecanbedesignedtosupplytheneed.
Unit2TheBasicsofComputerSystem2.1Text2.2ReadingMaterials
2.1Text
TheVonNeumannArchitectureofComputerSystemAllcomputerssharethesamebasicarchitecture,whetheritisamainframeoraPalmPilot.Allhavememory,anI/Osystem,andarithmetic/logicunit,andacontrolunit.ThistypeofarchitectureisnamedVonNeumann’sArchitectureafterthemathematician,JohnVonNeumannwhoconceivedofthedesign.
JohnVonNeumannbeginshis“PreliminaryDiscussion”withabroaddescriptionofthegeneral-purposecomputingmachinecontainingfourbasiccomponents.Theseareknownasrelatingtoarithmetic,memory,control,andconnectionwiththehumanoperator.Inotherwords,thearithmetic/logicalunit(ALU),thememory,thecontrolunit(CU),andtheinput-output(I/O)devicesthatweseeintheclassicalmodelofwhatacomputer“l(fā)ookslike”.VonNeumannArchitectureofComputerSystemisshowninFig2.1.Fig2.1VonNeumannArchitectureofComputerSystem
Memory
ComputerMemoryisthesubsystem
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