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1、INTENSITYANGLEOFARRIVALEFFECTSONMICROWAVEPROPAGATIONCAUSEDBYATMOSPHERICTURBULENCER.W.McMillanU.S.ArmySpaceMissileDefenseCommPOBox1500HuntsvilleAlabama358073801USAAbstractAtmosphericturbulencehasbeenshowntocausemeasurable
2、effectsonthepropagationofmicrowavemillimeterwavesignals.Althoughtheseeffectsarenotasstrongasthoseencounteredatvisiblewavelengthsbecauseoftheirvariationasf76wherefisfrequencythecontributionofthehuitystructurefunctionCQ2ma
3、kestheseeffectssignificantfmanyapplications.Inthispaperwepresentresultsofcalculationsmeasurementsoftheeffectsofatmosphericturbulenceonmillimeterwavesignalsat117140173230GHzaswellascalculationsmeasurementsoftheseeffectsat
4、10GHz.Theagreementbetweentheeticalmeasuredvaluesisconsideredgoodfthistypeexperiment.BackgroundDuringaseriesofmeasurementsofmillimeterwavepropagationthroughdustsmokein1977J.J.GallagherR.W.McMillanthenwkingattheGegiaTechRe
5、searchInstituteobservedlargeintensityfluctuationsof94140GHzsignalspropagatingthroughclearair.Althoughthisobservationwasnotsurprisinginlightofatmosphericturbulencetheywhichpredictscontributionstotheindexofrefractionstruct
6、ureparameterCn2fromboththetemperaturestructureparameterCT2thehuitystructureparameterCQ2aswellastheircrosscrelationCTQatmillimeterwavefrequenciesitwassurprisingtothemicrowavemillimeterwavecommunitiesbecauseithadrarelyifev
7、erbeenobservedbefe.AreptonthesemeasurementsledtosupptfromtheU.S.ArmyResearchOfficefmedetailedmeasurementsofthesephenomenaincludingcarefulmicrometerologicalinstrumentationfacterizationofthestructureparametersmentionedabov
8、ecrelationoftheseobservationswithmillimeterwavemeasurements.ThisseriesofexperimentswascarriedoutwiththesupptcollabationoftheNationalOceanicAtmosphericAdministrationprimarilyresponsiblefmeteologicalinstrumentationbytheaut
9、hcolleaguesattheGegiaTechResearchInstitute.TheresultsofthesemeasurementswhichweremadeatasitenearChampagneUrbanaIllinoischosenfthehomogeneityofitsterrainaregiveninseveralpapersfexample[12].Theseresultswillbediscussedinmed
10、etailinsubsequentsections.Apotentiallyseriousproblemfmicrowavemillimeterwaveradarsystemsinparticularisthatofangleofarrivalofthesignalsscatteredbytargetscausedbyturbulenceinducedwavefrontdisttion.Theangleofarrivalθisgiven
11、byθ=λ?2πdwhere?isthephasedifferenceinthewavefrontmeasuredoverthepathd.FmostradarscenariostheAOAisnegligiblebutinthosecaseswherethewavefrontmusttravelthroughgreatdistancesintheatmosphericboundarylayerfexampleinlongrangelo
12、wangletrackingapplicationsAOAcanbesignificant.MeasurementsofAOAFigure1.Experimentalconfigurationftheturbulencemeasurements.Figure2.Intensityfluctuationsmeasuredat140GHzMicrowaveRadarAngleofArrivalTheeffectsofatmospherict
13、urbulenceonradarangleerrsaregenerallysmallbutinthosecaseswherearadarisrequiredtoguideamissilewithoutaseeker(commguide)afewmicradiansoferrmaybeenoughtocausethemissiletomissitstarget.Inthispaperwecomparetwomethodsofcalcula
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