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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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