电热膜热成像英文文献.docx
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电热膜热成像英文文献.docx
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电热膜热成像英文文献
英文文献翻译
Thetechnologyofgeneratinginfraredimagebasedonelectricheatingfilmtechnology
基于电热膜技术的红外图像生成技术
文献来源:
脉冲功率激光技术国家重点实验室
Thetechnologyofgeneratinginfraredimagebasedon
electricheatingfilmtechnology
ABSTRACT
Thetechnologyofgeneratinginfraredimagebasedonelectricheatingfilmtechnologybyitsresistanceperunitareawasstudied.ALifgt-off-roadvehiclewasusedasanobjecttobesimulated.Aninfraredthermographwasusedtophotographythelight-off-roadvehiclefromaspecificcorner.Asaresultseveralinfraredimagesofthelight-off-roadvehiclewereobtainedandthethermaldistributionofthevehiclewasalsoobtainedatthesametime.Amatlabprogramwasusedtoprocesstheimage.Theimagewasdividedintoseveralareasaccordingtoitsgreylevel.Eachareahasitsowntemperaturerange.Theaveragetemperatureofeachareawascalculated.Athermalbalanceequationwasestablishedaccordingtotheaveragetemperatureofeachareaandtheenvironmenttemperature.Bysolvingtheseequations,theradiantexistancesoftheseareasweregotten.Theheatingpowerperunitareaoftheseareaswascalculated.Theelectricheatingfilmwaspreparationaccordingly.Thepowerwasappliedonthefilmandtheinfraredthermographwasusedtoobserveit.Theinfraredimageofthefilmhasahighsimilaritywiththetruelight-off-roadvehicle’s.
Keywords:
electricheatingfilm,infraredimage,simulation
1.PRINCIPLESOFOPERATION
Allkindsobjectshaveinfraredradiation.Theinfraredradiantcharacteristicofanobjectisdependingonitssurfacetemperatureanditssurfaceemissivity.TheradiationcanbecalculatedbyPlanckequation.Theusualformoftheequationiswrittenintermsoftheradiantexitanceasafunctionofwavelength.Consideringtheemissivityofacertainobject,theradiantexitancecanbewritten[1]:
(1)
Where
isthespectralradiantexitance,
isthefirstradiationconstantand
isthesecondradiationconstant.Theyaregivenby:
Wherecisthespeedoflightinvacuum,hisPlanck’sconstant,kisBoltzmann’sconstant,andTisthetemperatureinkelvins.
Sincetheemissivityisfixedforcertainmaterial,thetemperatureisthemajorfactorthatinfluencesinfraredradiation.Itisusuallymoreusefultoknowthevalueofthetotalpoweremittedfromabody,ratherthanitsspectralextent.Thewell-knownStephan-Boltzmannlawgivesthetotalradiantexitanceas:
(2)
Whereistheemissivityofanobject.istheStephan-Boltzmannconstant.Ithasbeenevaluatedandisgivenby
Foranobject,thereasonofitshowingdifferentinfraredimageisthatithasdifferenttemperatureondifferentpartsofit.Thuswecansimulateatrueobject’sinfraredimagebyreappearingthetemperatureoftheobject.
Thetechnologyofgeneratinginfraredimagebasedonelectricheatingfilmtechnologywasbroughtforwardaccordingtotheinfraredradiationtheory.Themaincourseis:
theinfraredimageofanobjectwasobtainedfirstly,andthentheimagewasdividedintoseveralareasaccordingtoitstemperatureanditsgreylevel.Theradiationpowerofthesepartswascalculated.Theresistanceperunitareaofthesepartswerecalculatedwhenthevoltageofthefilmwascertain.Theheatingfilmwaspreparedaccordingtotheresistanceperunitarea.Whenthefilmwasheatedbyelectricitypower,therelevantinfraredimagewillappear.
2.INFRAREDIMAGEOBTAINOFANOBJECTANDRELATIVELYCALCULATION
2.1infraredimageanditstemperaturedistributing
ALight-off-roadvehiclewasusedasanobjecttobesimulated.Thevehiclewasfiredupinidlestate.Tenminuteslate,aninfraredthermographwasusedtophotographythelight-off-roadvehiclefromaspecificcorner.Fig.1wastheinfraredimageofthevehicle.
Fig.1infraredimageofaLight-off-roadvehicle
Theanalysisandprocesstotheimagewascarriedout.Theinfraredimagewasdividedintoseventemperatureareasbyitsgreylevel.Theseareasshowedinfig.2.Theaveragetemperatureoftheareaisthesameforthoseareaswhichhavethesamenumber.
Fig.2thegreylevelofthevehicle
Theaveragetemperatureoftheseareasshowedintable1andthetemperatureofbackgroundis24℃.
Table1Theaveragetemperatureofdifferentareas
AreaNo.
1
2
3
4
5
6
7
AverageTemperature(℃)
38.4
37.0
31.0
26.8
26.1
31.2
38.0
Fortheseareas,wehypothesizedthatthearea“i”hasatemperature
thetemperaturebackgroundis
.Theacreageofarea“i”is
.Theacreageoftheseareasiscalculated.
2.2Heatingpowercalculation
Whentheelectricheatingfilmwaspoweredon,mostoftheelectronpoweritgottenwasconvertedtoheatpower.Thetemperatureoftheseareasrose.Thetemperatureoftheseareaachievemaximumwhentheareawasinthermalequilibriumstatewiththeenvironment.Whenthefil
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