The control design for formation flight about multiple Unmanned Aerial VehiclesWord格式文档下载.docx

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The control design for formation flight about multiple Unmanned Aerial VehiclesWord格式文档下载.docx

ModelingandcontrolofformationflightofmultipleUAVsisangrowingtopicofresearchintheaerospacefield,andhasanumberofapplicationsinmilitarymissionssuchasreconnaissanceandsurveillance,taskallocationandtargetdataacquisition,radiojamming,andthesuppressionsofenemyairdefenseaswellasincivilianmissionssuchascropmonitoring,areasearchandrescue.ThemultipleUAVsformationflightproblemaimstoachievedesiredgeometriesbycontrollingtheoverallbehaviorofthegroup.AccuratemaintenanceoftheformationcanoftenaccomplishobjectivesimpossibleforasingleUAVandleadtocertainadvantagessuchasareductionintheformation’sinduceddragandenergysavingfromvortexforcecreatedbytheleadaircraft.DevelopmentofformationcontrolproblemsandnumerousapproachesforUAVsformationcontroldesignhavebeenwelldemonstrated.InRef,R.Sattigerietal.proposedadecentralizedadaptiveoutputfeedbackapproachwhichallowedthevehiclestomaintaintheformationwhileconsideringobstacles.InRef,W.Renetal.developedaleaderlessformationcontrolschemebasedonconsensusalgorithmswhichovercomeasinglepointoffailurefortheformation.InRef,D.Galzietal.proposedHighOrderSlidingMode(HOSM)controllerforaswarmofUAVstoachieveleader/followerscollision-freeformationinthepresenceofunknowndisturbances.InRef,MasayukiSuzukietal.designedathree-dimensionalformationcontrolschemeusingthenewapproachofbifurcatingartificialpotentialfields.InRef,YunfeiZouandPrabhakarR.PagillausedthetheoryofconstraintforcestodeterminethetotalforcerequiredoneveryaircrafttobuildaformationfromarbitraryinitialconditionsforUAVs.Butthesemethodsmaynotbeabletodealwiththeconstraintseasily,suchastheaccelerationofvelocityandangularturnrateconstraints,andcontrolinputsaturationconstraints.Optimization-basedapproachescansolvetheconstraintsofUAVformationcontrolsystemsappropriatelyandhavebeenprovedtoasuccessfulwaytothemultipleUAVsformationproblems.Amongthemostpopularoptimization-basedmethodsisRHCmethod.

II.ProblemFormulation

2.1ModelofUAVflightdynamicsandcontrolsystems

TheequationsofmotiondescribingUAVflightdynamicsaregivenasfollows[23,24]:

Forceequations:

(1)

Kinematicequations:

(2)

Momentequations:

(3)

Navigationequations:

(4)

Inthispaper,wereducedthecomplexmodeltoasimplermodelforthepurposeofguidancelawdesign.Accordingly,first-ordersystemsareadoptedtorepresenttwocontrolchannelsincludingtheUAVflightdynamicsasfollows:

(speedcontrolchannel)(5)

(headinganglecontrolchannel)(6)

Where

arethetimeconstantsand

arethecontrolcommandinputofeachcontrolloop.

2.2RecedingHorizonControl

Recedinghorizoncontrol(RHC),alsoknownasmodelpredictivecontrol(MPC),isafeedbackcontrolschemeinwhichafinitehorizonopen-loopoptimizationproblemissolvedateachsamplinginstant[25,26].

TheRHCprocedureworksasshowninFig.1.Attimet,weconsideratimeintervalextendingpstepsintothefuture,t,t+1,…,t+p.Wethencarryoutthefollowingsteps:

(1)Replacealltheuncertainquantitiesoverthepredictionhorizonpwiththeirestimatesusingtheinformationavailableattimettopredictthefuturedynamicbehaviorofthesystem.

(2)Optimizeapredeterminedperformanceobjectivefunctionsubjecttotheestimateddynamicsandconstraints.Theoptimizationresultisaplanofactionforthenextpsteps.

(3)Determinetheinputoveracontrolhorizonmusingtheplanofaction.Atthenexttimestep,theprocessisrepeated,withtheupdatedestimatesofthecurrentstateandfuturequantities.

Fig.1ProcedureofRecedingHorizonControl

 

2.3Leader-followerformationflightmodel

Inthispaper,wemainlyfocusonmultipleUAVsformationproblemonahorizontalplane.Thehorizontalformationgeometricparametersaretheforwardclearance

andthelateralclearance

asdefinedinFig.2.ThereferencepositionforthefollowerUAVcanbecalculatedusingthefollowingrelationship:

(7)

where

representthefollower’sdesiredposition,

and

representthepositionandtheheadingangleoftheleaderUAV.

areexpressedas:

(8)

(9)

Fig.2HorizontalFormationGeometry

Weformulatearecedinghorizoncontrolschemebasedonthecostfunction.Attimek,thecontrollerpredictsacontrolsequencefromtimektotime(k+p),whichcanberepresentedby

…,

.Usingthiscontrolsequenceandthecurrentstateofthesystem

thestateattimek+1,…,k+p,whicharerepresentedby

canbeobtained.Thefitnessfunctionattimekcanbedefinedas:

(10)

subjectto

(11)

whereQandRarepositive-definiteweightedmatrices.

isreferencestateoffollowerUAVsattimek.

isthestateoffollowerUAVsattimek+joverthepredictionhorizon.

isthesamplingtime.

Fig.3RecedingHorizonControlScheme

Minimizingthisfitnessfunctionyieldsanoptimalcontrolsequence,thenthefirstmcontrolactionsinthissequenceisappliedtotheformationflightsystem.Attimek+m,repeatsampling,predicting,optimizationandimplementing.ThisprocedurecanbedescribedasFig.3.

III.PrinciplesofthebasicCROalgorithm

ChemicalReactionOptimization(CRO)isarecentlyestablishedmetaheuristicsforoptimization,inspiredbythenatureofchemicalreactions.Inmicroscopicview,achemicalreactionstartswithsomeunstablemoleculeswithexcessiveenergy.Themoleculesinteractwitheachotherthro-ughasequenceofelementaryreactions.Attheend,theyareconvertedtothosewithminimumenergytosupporttheirexistence.ThispropertyisembeddedinCROtosolveoptimizationproblems.

Ingeneral,theprinciplesofchemicalreactionsaregovernedbythefirsttwolawsofthermodynamics.Thefirstlaw(conservationofenergy)saysthatenergycannotbecreatedordestroyed;

energycantransformfromoneformtoanotherandtransferfromoneentitytoanother.Thesecondlawsaysthattheentropyofasystemtendstoincrease,whereentropyisthemeasureofthedegreeofdisorder.Potentialenergyistheenergystoredinamoleculewithrespecttoitsmolecularconfiguration.Whenitisconvertedtootherforms,thesystembecomesmoredisordered.Allreactingsystemstendtoreachthestateofequilibrium,whosepotentialenergydropstoaminimum.InCRO,wecapturethephenomenonbyconvertingpotentialenergytokineticenergyandbygraduallylosingtheenergyofthechemicalmoleculestothesurroundings.

3.1Themanipulatedagent

CROisamulti-agentalgorithmandthemanipulatedagentsaremolecules.Eachmoleculehasseveralattributes,someofwhichareessentialtothebasicoperationsofCRO.Theessentialattributesinclude:

themolecularstructure(ω);

thepotentialenergy(PE);

thekineticenergy(KE);

thenumberofhits(NumHit);

theminimumstructure(Min-Struct);

theminimumPE(MinPE);

andtheminimumhitnumber(MinHit).

3.2Elementaryreactions

Achemicalchangeofamoleculeistriggeredbyacollision.Therearetwotypesofcollisions:

uni-molecularandinter-molecularcollisions.Weconsiderfourkindsofelementaryreactions:

on-wallineffectivecollision,decomposition,inter-molecularineffectivecollision,andsynthesis.Thetwoineffectivecollisionsimplementlocalsearch(intensification)whiledecompositionandsynthesisgivetheeffectofdiversification.Anappropriatemixtureofintensificationanddiversificationmakesaneffectivesearchoftheglobalminimuminthesolutionspace.

3.2.1On-wallIneffectiveCollision

Anon-wallineffectivecollisionoccurswhenamoleculehitsthewallandthenbouncesback.Somemolecularattributeschangeinthiscollision,andthus,themolecularstructurevariesaccordingly.Asthecollisionisnotsovigorous,theresultantmolecularstructureshouldnotbetoodifferentfromtheoriginalone.Supposethecurrentmolecularstructureisω.Themoleculeintendstoobtainanewstructureω`=Neighbor(ω)initsneighborhoodonthePESinthiscollision.Thechangeisallowedonlyif

PEω+KEω≥PEω`

Weget

KEω`=(PEω+KEω–PEω`)×

q

whereq∈[KELossRate,1],and(1−q)representsthefractionofKElosttotheenvironmentwhenithitsthewall.KELossRateisasystemparameterwhichlimitsthemaximumpercentageofKElostatatime.Thelostenergyisstoredinthecentralenergybuffer.Thestoredenergycanbeusedtosupportdecomposition.Ifitdoesnothold,thechangeisprohibitedandthemoleculeretainsitsoriginalω,PEandKE.

3.2.2Decomposition

Decompositionr

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