Принцип на изобразяване на изпъкнала леща

Функции за изображения

Firstputtheobjectfarawayfromthelens,checkthepositionandsizeoftheimage,thenmovetheobjecttotheconvexlens,andthencheckthesizeandpositionoftheimageVariety.Itcanbeseenfromtheexperiment:

(1) Когато обектът е много далече, изображението не се ражда на фокус и изображението е много малко.

(2)Whentheobjectmovestothefrontoftheconvexlens,theimagemovesfromthefocalpointtotheoutsideoftheconvexlens,theimagebecomeslargerandupsidedown.

(3) Когато обектът не е далеч от фокуса, изображението е много далеч и изображението е много голямо.

(4) Обектът е на фокус и не се открива изображение, така че не е изобразен.

(5)Theobjectcannotbeimagedinthefocalpoint,buttheeyecanseeamagnifieduprightvirtualimagethroughthelens.

Принципът на изобразяване на увеличителното стъкло

Anopticallensmadeofglassorothertransparentmaterialswithacurvedsurfacecanmagnifyandimageanobject.TheopticalpathdiagramisshowninFigure1.TheobjectABlocatedwithinthefocusFoftheobjectsidehasasizeofy,anditismagnifiedintoavirtualimageA'B'ofsizey'.ThemagnificationofthemagnifyingglassΓ=250/f'where250--thedistanceoftheclearvision,inmmf'--thefocallengthofthemagnifyingglass,inmmThemagnificationreferstotheimageoftheobjectobservedbythemagnifyingglasswithinadistanceof250mmTheratiooftheviewingangletotheviewingangleofanobjectobservedwithoutamagnifyingglass.1.Drawastraightruler2.DrawapointOontheruler,whichistheopticalcenter,anddrawaconvexlensattheOpoint.Marktheone-timefocallengthpointfandthetwo-timefocallengthpoint2fonbothsidesoftheconvexlens.

3. Преградата е разделена на три области от лявата и дясната страна на изпъкналата леща. O──fisthefirst area,f──2fisthesecondarea, andoutside2fisthethretty area.

4. Закон:

Когато обектът е безкрайност, фокусирайте се върху точката.

Нещата три (област) са като две (област) малки, реално обърнати

Нещата две (област) като три (област) са обърнати големи

Area)Onthesamesideoftheimage,thepositiveandlargevirtualimage

The2Fpointisthedividingpointoftheenlargedandreducedimage

TheFpointisthedividingpointofthevirtualimageoftherealimage.

Използваме линийка, когато прилагаме и запомняме:

Принципът на изобразяване на микроскопа

Microscopeandmagnifyingglassplaythesamerole,thatis,toremovesmallobjectsnearbyIntoamagnifiedimageforhumaneyestoobserve.It'sjustthatamicroscopecanhaveahighermagnificationthanamagnifyingglass.Schematicdiagramofanobjectbeingimagedbyamicroscope.Fortheconvenienceofcalculation,boththeobjectivelensL1andtheeyepieceL2arerepresentedbyasinglelens.TheobjectABislocatedinfrontoftheobjectivelens,andthedistancefromtheobjectivelensisgreaterthanthefocallengthoftheobjectivelens,butlessthantwicethefocallengthoftheobjectivelens.Therefore,afteritpassesthroughtheobjectivelens,itwillinevitablyformaninvertedenlargedrealimageA'B'.A'B'islocatedontheobjectivefocalpointF2oftheeyepiece,orveryclosetoF2.ThenitismagnifiedbytheeyepieceintoavirtualimageA''B''foreyeobservation.ThepositionofthevirtualimageA''B''dependsonthedistancebetweenF2andA'B'.Itcanbeatinfinity(whenA'B'isonF2)orattheobserver'sphotopicdistance(WhenA'B'istotherightoffocusF2inthefigure).Theeyepiecehasthesamefunctionasamagnifyingglass.Thedifferenceisthatwhattheeyeseesthroughtheeyepieceisnottheobjectitself,buttheimageoftheobjectthathasbeenmagnifiedoncebytheobjectivelens.

Важни оптични технически параметри

Duringmicroscopicexamination,peoplealwayshopetohaveaclearandbrightidealimage,whichrequirestheopticaltechnicalparametersofthemicroscopetoreachcertainstandardsAnditisrequiredthatwheninuse,therelationshipbetweenthevariousparametersmustbecoordinatedaccordingtothepurposeofthemicroscopyandtheactualsituation.Onlyinthiswaycanwegivefullplaytotheproperperformanceofthemicroscopeandobtainsatisfactorymicroscopicexaminationresults.Theopticaltechnicalparametersofthemicroscopeinclude:numericalaperture,resolution,magnification,depthoffocus,fieldofviewwidth,coveragedifference,workingdistance,andsoon.Theseparametersarenotallashighaspossible.Theyareinterrelatedandrestricteachother.Inuse,therelationshipbetweentheparametersshouldbecoordinatedaccordingtothepurposeofmicroscopyandtheactualsituation,buttheresolutionshouldbeguaranteed..

1.NumericalApertureNumericalapertureisabbreviatedNA.Numericalapertureisthemaintechnicalparameterofobjectivelensandcondenserlens,anditisanimportantindicatorofjudgingtheperformanceofboth(especiallyforobjectivelens).Thenumericalvalueismarkedontheshelloftheobjectivelensandcondenserlensrespectively.Thenumericalaperture(NA)istheproductoftherefractiveindex(n)ofthemediumbetweenthefrontlensoftheobjectivelensandtheinspectedobjectandthehalfsineoftheapertureangle(u).Theformulaisasfollows:NA=nsinu/2Theapertureangleisalsocalled"lensangle",whichistheangleformedbytheobjectpointontheopticalaxisoftheobjectivelensandtheeffectivediameterofthefrontlensoftheobjectivelens.Thelargertheapertureangle,thebrighterthelightenteringtheobjectivelens,whichisproportionaltotheeffectivediameteroftheobjectivelensandinverselyproportionaltothedistanceofthefocalpoint.Duringmicroscopeobservation,ifyouwanttoincreasetheNAvalue,theapertureanglecannotbeincreased.Theonlywayistoincreasetherefractiveindexnofthemedium.Basedonthisprinciple,awaterimmersionobjectivelensandanoilimmersionobjectivelensareproduced.Becausetherefractiveindexnofthemediumisgreaterthan1,theNAvaluecanbegreaterthan1.Themaximumnumericalapertureis1.4,whichhasreachedthelimittheoreticallyandtechnically.Therefractiveindexofbromonaphthaleneis1.66,sotheNAvaluecanbegreaterthan1.4.Itmustbepointedoutherethatinordertogivefullplaytotheroleoftheobjectivelensnumericalaperture,theNAvalueofthecondenserlensshouldbeequaltoorslightlygreaterthantheNAvalueoftheobjectivelensduringobservation.Numericalaperturehasacloserelationshipwithothertechnicalparameters,italmostdeterminesandaffectsothertechnicalparameters.Itisproportionaltotheresolution,proportionaltothemagnification,andinverselyproportionaltothedepthoffocus.AstheNAvalueincreases,thewidthofthefieldofviewandtheworkingdistancewilldecreaseaccordingly.

2.ResolutionTheresolutionofamicroscopereferstotheminimumdistancebetweentwoobjectpointsthatcanbeclearlydistinguishedbythemicroscope,alsoknownasthe"discriminationrate".Thecalculationformulaisσ=λ/NAwhereσistheminimumresolutiondistance;λisthewavelengthoflight;NAisthenumericalapertureoftheobjectivelens.Itcanbeseenthattheresolutionoftheobjectivelensisdeterminedbytwofactors,theNAvalueoftheobjectivelensandthewavelengthoftheilluminatinglightsource.ThelargertheNAvalue,theshorterthewavelengthoftheilluminatinglight,andthesmallertheσvalue,thehighertheresolution.Toimprovetheresolution,thatis,reducethevalueofσ,thefollowingmeasurescanbetaken(1)Reducethevalueofwavelengthλanduseashort-wavelengthlightsource.(2)IncreasethevalueofmediumntoincreasethevalueofNA(NA=nsinu/2).(3)IncreasetheapertureangleuvaluetoincreasetheNAvalue.(4)Increasethecontrastbetweenlightanddark.

3.MagnificationandeffectivemagnificationDuetothetwomagnificationsoftheobjectivelensandtheeyepiece,theoverallmicroscopeThemagnificationΓshouldbetheproductoftheobjectivelensmagnificationβandtheeyepiecemagnificationΓ1:Γ=βΓ1Obviously,comparedwithamagnifyingglass,amicroscopecanhaveamuchhighermagnification,anditcanbeconvenienttoexchangeobjectivesandeyepieceswithdifferentmagnificationsChangethemagnificationofthemicroscope.Themagnificationisalsoanimportantparameterofthemicroscope,butyoushouldnotblindlybelievethatthehigherthemagnification,thebetter.Thelimitofmicroscopemagnificationistheeffectivemagnification.Resolutionandmagnificationaretwodifferentbutrelatedconcepts.Thereisarelationship:500NAnumericalapertureisnotlargeenough,thatis,whentheresolutionisnothighenough,themicroscopecannotdistinguishthefinestructureoftheobject.Atthistime,evenifthemagnificationisincreasedexcessively,theresultcanonlybealargeoutlinebutuncleardetailsTheimageiscalledinvalidmagnification.Conversely,iftheresolutionhasmettherequirementsandthemagnificationisinsufficient,themicroscopehastheabilitytodistinguish,buttheimageistoosmalltobeclearlyseenbythehumaneye.Therefore,inordertogivefullplaytotheresolvingpowerofthemicroscope,thenumericalapertureshouldbereasonablymatchedwiththetotalmagnificationofthemicroscope.

4.DepthoffocusDepthoffocusistheabbreviationofdepthoffocus,thatis,whenusingamicroscope,whenthefocusisonacertainobject,notonlyisitlocatedontheplaneofthepointEverypointcanbeseenclearly,andwithinacertainthicknessaboveandbelowtheplane,itcanalsobeseenclearly.Thethicknessofthisclearpartisthedepthoffocus.Ifthefocaldepthislarge,youcanseethewholelayeroftheobjecttobeinspected,whileifthefocaldepthissmall,youcanonlyseeathinlayeroftheobjecttobeinspected.Thefocaldepthhasthefollowingrelationshipwithothertechnicalparameters:

(1)Thedepthoffocusisinverselyproportionaltothetotalmagnificationandthenumericalapertureoftheobjectivelens.

(2)Thedepthoffocusislargeandtheresolutionisreduced.Duetothelargedepthoffieldofthelow-magnificationobjectivelens,itcausesdifficultieswhentakingpictureswiththelow-magnificationobjectivelens.Itwillbeintroducedindetailinthephotomicrograph.

5.FieldofView(FieldOfView)Whenobservingamicroscope,thebrightcircularareaseeniscalledthefieldofview.Itssizeisdeterminedbytheviewintheeyepiece.Determinedbythefielddiaphragm.Thefieldofviewdiameterisalsocalledthefieldofviewwidth,whichreferstotheactualrangeoftheobjecttobeinspectedinthecircularfieldofviewseenunderthemicroscope.Thelargerthediameterofthefieldofview,theeasieritistoobserve.ThereisaformulaF=FN/βwhereF:fieldofviewdiameter,FN:fieldnumber(FieldNumber,abbreviatedasFN,markedontheoutsideoftheeyepiecelensbarrel),β:objectivelensmagnification.Itcanbeseenfromtheformula:

(1)Thediameterofthefieldofviewisdirectlyproportionaltothenumberoffieldsofview.

(2)Increasethemultipleoftheobjectivelens,thediameterofthefieldofviewwilldecrease.Therefore,ifyoucanseethewholepictureoftheobjectunderinspectionwithalowmagnificationlens,youcanonlyseeasmallpartoftheobjectunderinspectionwithahighmagnificationobjectivelens.

6.PoorcoverageTheopticalsystemofthemicroscopealsoincludesthecoverglass.Becausethethicknessofthecoverglassisnotstandard,thelightpathafterthelightenterstheairfromthecoverglassischanged,resultinginaphasedifference,whichisthecoveragedifference.Poorcoverageaffectsthesoundqualityofthemicroscope.Internationally,thestandardthicknessofthecoverglassis0.17mm,andthepermittedrangeis0.16-0.18mm.Thedifferenceinthisthicknessrangehasbeencalculatedinthemanufactureoftheobjectivelens.The0.17ontheobjectivelensshellindicatesthethicknessofthecoverglassrequiredbytheobjectivelens.

7.WorkingdistanceWDworkingdistanceisalsocalledobjectdistance

Itreferstothedistancebetweenthesurfaceofthefrontlensoftheobjectivelensandtheobjecttobeinspected.

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