翻译1环境化学实验教学的案例研究.docx
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翻译1环境化学实验教学的案例研究
CreativeEducation
2012.Vol.3,No.4,600-602
PublishedOnlineAugust2012inSciRes(http:
//www.SciRP.org/journal/ce)DOI:
10.4236/ce.2012.34088
TeachinganEnvironmentalChemistryExperiment—A
CaseStudy
——SimpleTestforMeasuringtheEmissionSpectraofLamps
LinZhang,LongChen,MeiXiao,FengWu*,NanshengDeng
DepartmentofEnvironmentalScience,SchoolofResourcesandEnvironmentalScience,
WuhanUniversity,Wuhan,China
Email:
*fengwu@
ReceivedMay24th2012;revisedJune30th,2012;acceptedJuly10th,2012
Herewepresentthesignificance,content,results,andteachingeffectofaselectiveself-designexperi-ment—asimpletestformeasuringtheemissionspectraofartificiallightsources,anddiscussitsfunctionandpotentialproblemsinanenvironmentalchemistryclassforundergraduatestudents.Also,weproposeseveralwaystoreformexperimentalteaching,andprovidereferencestootherexperimentalcourses.
Keywords:
Self-DesignExperiment;Spectrophotometer;Spectrum;HighPressureMercuryLamp;
DeuteriumLamp
Introduction
LaboratorycoursesareacrucialcomponentofaNationalQualityCourse(NQC)—EnvironmentalChemistry.Inthisre-searchgroup,webelievethattheconstructionandreformofthissubjectisimportant,andourcoretaskistodevelopteach-ingquality,improvestudents’experimentalabilities,promotemotivationandenthusiasm,inspireaspiritofscientificexplora-tionandcreativity,thusenablingstudentstoconductscientificresearchandsolvepracticalproblems.
TheaimoftheNQCistosettlevariousproblemsregardingtheconstructionofcoursecontent,andweasNQCinstructorsmanageanddesignthelaboratoryteachingourselves,andin-creasinglyself-designcomprehensiveexperiments.Weofferopportunitiesforstudentstogainknowledge,developtheirre-searchabilities,andenhancetheirindependence.Meanwhile,wereformthelaboratoryteachingmethods,andencouragedis-cussionandanactiveclassatmosphere,toinspirestudents’brainstormingabilities,andtoenhancetheteachingeffect.
Inthefollowingcase—asimpletestforalampemissionspectrum,webrieflyillustratehowstudents’researchabilitiesareclearlyimprovedthroughdesigninganexperiment.
ObjectiveofThisStudy
Ultravioletandvisible(UV-Vis)spectrophotometryisoneofthemostpracticalandfunctionaltoolsinquantitativeanalysis,andaUV-Visspectrophotometer(UVVS)isoneofthemostcommonlyusedinstrumentsinlaboratoryteachingforenvi-ronmentalmajorundergraduates.Therefore,mostinstructorswillregardthisascritical.Whileinlaboratoryclass,thepur-poseofsettingupthisexperimentisto:
makestudentslearnabouttheinnerstructureandworkingprincipleofaUVVSthroughdisassemblingit,e.g.thecharacteristicsofemissionspectraofahighpressuremercurylamp(HPML)anddeute-
*Correspondingauthor.
riumlamp(DL)usingremoldedUVVS;increasetheirtheoreti-calknowledgeaboutopticsviadeterminingemissionspectraofseveralartificiallightsources;promotetheircomprehensivescientificresearchabilityandtheabilitytodesignexperimentsbycomposinganexperimentalplan,accomplishingitandsub-mittingthefinalresultintheformofanessay.
ExperimentalPrinciple
TheUVVSconsistsoffourmajorparts:
alightsource,abeamsplittingsystem,anabsorptioncell,andadetectionsys-tem(Figure1).Inordertodeterminetheilluminationintensityofourtargetlamps(HPMLandDL),indifferentwavelengths,weneedtoutilizethebeamsplittingsystemtosplitthecon-tinuousspectra,thusfullytakingadvantageofregularUVVS.Therefore,weonlyhavetoalterthelightsourceforothersourcestobeexamined,andafteradjustingthewavelengthwecanobtainthetransmissivity(T)fordifferentwavelengths.
Inthisexperiment,weneedabaselinetoquantifytherelativeemissionintensity.Therefore,thevalueofTforaspecificwavelengthhastobefixedto0%,inwhichtheremightbelu-minance.Therelativeintensityinotherwavelengthscanbequantifiedbysubsequentcomparison.Similarly,wecanalsofixthevalueofTofaspecificwavelengthto100%,andthenperformthesameprocessdescribedabove.Giventhefactthatthereisaglasscoveronthemercurylampandthereisnotransmissioninwavelengthslessthan280nm,280nmwaschosenasthebaselineandfixedto0%,andwedeterminedthespectraupto800nm.However,fortheDL,thecoverismadeofquartz,thushavinglowerabsorptionlimit(160nm).There-foreweshouldset160nmasthebaseline,butbecausetheshortestwavelengthwecanuseintheUVVSis180nm,weset180nmasthebaseline,andalsocontinuedupto800nm.
Owingtothelimitsofthelaboratory,wecouldnotevacuatetheabsorptioncell.However,infact,theimpactofairisnegli-gible.
600Copyright©2012SciRes.
L.ZHANGETAL.
Figure1.
InnerstructureofaUVVS.
Instruments
InstrumentsincludedtheUV-9100UVVS,anHPML,anironsupport,ascrewdriver,nipperpliersandawrench.TheDLusedwasintheUVVSitself.
ExperimentalMethod
StudyoftheDLEmissionSpectrum
Beforedetermination,theUVVSwasswitchedonandtheDLwaspreheatedfor15min.Thenweputthelidon,adjustedthewavelengthto180nm,andmadeT=0%.Thewavelengthintervalwaspreliminarilysetat10nm,butwhenitapproachedthepeak,2nmwasmoreappropriate.BecausetheUV-9100UVVScannotachievemoreaccurateperformance,andlargerintervalscannotpreciselyportraythespectrum.ThewavelengthwasalteredandTwasrecordeduntil800nmwasreached.Af-tertheexperimentwascompleted,boththeDLandUVVSwereswitchedoff,andthepowercablewasunplugged.
StudyoftheHPMLEmissionSpectrum
Forthesakeofsafety,thepowercablewasunplugged.ToeliminatetheeffectofDLandthetungstenlamp,theyhadtoberemovedbeforetheexperiment.Theoutercoverwaslifted,andthetoplidonthelamphousewasremoved.ThenthethreewiresconnectedtotheDLwerescrewedoff,clampedbythenipperpliers,thenthetightenedscrewswereunscrewedusingascrewdriver.ThentheDLcouldbeextractedfromUVVS.Thetungstenlampwasremovedusingthesamemethod.Thentheoutercoverwasreplaced,andthedam-boardinfrontofthelightsourceswasremoved.Withtheironsupport,theHPMLwasfixedoppositetheopticalchannel.ThenthepositionofHPMLwasadjustedtofocusitsradiationontheopticalcol-lector.After15minpreheatingtheHPML,theUVVSwasswitchedon.Forthisexperiment,250nmwasselectedasthebaseline,and2nmwaschosenasthewavelengthintervaluntil800nmwasreached.AftertheexperimenttheUVVSwasre-stored,andtheHPMLwasremoved.
Results
ThedataarepresentedrespectivelyfortheemissionspectraoftheHPMLandDL.Toanalyzetheiraccuracy,theywerecomparedwithstandardemissionspectra(EmissionSpectraof
Copyright©2012SciRes.
mercurylight,deuteriumlightandtungstenlamp.Availableonline)indetail.AllthespectraarepresentedinFigures2and3.
Discussion
CoincidenceAnalysisbetweenStandardandExperimentalSpectra
Bycomparisonwithstandardspectra,wefoundtheexperi-mentalspectraofbothHPMLandDLcoincidedwiththemsignificantly.Inparticular,theemissionpeaksofHPMLat404nm,436nm,546nmand577-579nmwerealldelineated.Moreover,themainpeakat365nmwasaccuratelydepicted.However,thestandardspectrumoftheDLisfarmorecomplexthanthatoftheHPML,sincethespectralbandwidthofitsslitiscomparativelytiny,andcanscanadjacentwavelengths.There-fore,toclearlydemonstratethedistinction,thisstandardspec-trumwasfittedtoamodifiedandsmoothcurve,inwhichthepeakswereingoodagreementwiththeexperimentalspectrum,asshown.
DifferenceAnalysisbetweenHPMLandDLEmissionSpectra
Obviousdifferencesinemissionspectracanbeobserved
ExperimentalSpectrum
16
StandardSpectrum
14
12
10
8
T
6
4
2
0
200300400500600700800wavelengthλ(nm)
Figure2.
EmissionspectraofDL.
ExperimentalSpectrum
StandardSpectrum
15
10
T
5
0
300400500600700800wavelengthλ(nm)
Figure3.
EmissionspectraofHPML.
601
L.ZHANGETAL.
betweentheHPMLandDL—thespectrumoftheformerisscattered,whilethespectrumofthelatterismorecontinuous.Thisisbecausetheirradiationofthemercurylampdependsonatoms.Aftertheyabsorbenergyfromthehighvoltage,theelectronscanmovetohigherenergylevels,andthisprocessiscalledtransition.Becausehigherenergylevelsresultinunsta-blestates,someelectronswillreturntolowerenergylevels,releasingelectromagneticradiation.Moreover,withincreasingmercuryvaporpressure,theatomiccollisionbecomesmorefrequentandintense,sotheemissionspectrawillbemoreandmorecontinuous.Infact,theemissionspectrumofanultrahighpressuremercurylampisalmostbandspectrum.However,aDLcanradiateacontinuousspectrumintheultravioletband.ThatiswhytheDLcanbetheultravioletlightsourceforaUVVS.
EffectAnalysisofThisExperimentalMethod
Withthewidespreaduseofvariouslampsanddevelopmentsinlamptechnology,nowadaysthelifespan,energysavingperformance,lightcoloretc.aregreatlyimproved.Sometimes,theabsolutecalibrationofthespectralirradiance,especiallyinmodernresearch,isnecessary.Tangetal.(Tang&Li,1996)hasstudiedtheabsolutecalibrationinshortwaveareasoftheDL.Huangetal.(Huang,Wang,Zhang,Lin,&Li,2007)onceusedaDLtostandardizetheirradianceinwavelengthsbetween200and300nm,whileWangetal.(Wang&Zhu,1992)dis-cussedmethodstoautomaticallycollectmercurylampspectra.