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ISOGRID DESIGN HANDBOOK - NASA

NASACONTRACTORREPORTNASACR-124075 REVISIONAISOGRIDDESIGNHANDBOOKMcDonnellD ouglasAstronauticsCompany5301 BotsaAvenueHuntingtonBeach,Ca92647 February1973[NASA-CR-12_075)150 GRIDDESIGNHANDBOOK(McDonnell-DouqlasAstr onauticsCo.)222pHC$ .) ,GRIDDESIGNHANDBOOKMDCG4295 APREPAREDBY,V1 CDONNELLDOUGLASASTRONAUFIL;SCO_.,1 PANYFOR:NASAMARSHALLSPACEFLIGItTCEN] FOREWORDT hisprogram,thedevelopmentoftheisogriddes ignhandbook,wasconductedbytheMcDonnellDo uglasAstronauticsCompanyatHuntingtonBeac h,Cal.;forniaund_, ,MarshallSpaceFlightCenter, ,Direct:or,ResearchandDevelopment, ,beingresponsibleforSections2and4, :(1)theresultsofanalysis,test,andadvance dmanufacturingstudiesofIndependentResear chandDevelopmentprogcams,(2)aphaseBspace shuttleboosterstudyfundedbytheNASAM arshallSpaceFlightCenter,(3)anisogridtan ktestprogramfundedbytheNASAM arshallSpaceFlightCenter,and(4)theDeltap rogramisogridstructuraltestsfundedbytheN ASAG oddardSpaceFlightCenter, ' :: ,BendingCylindersUnderTorsionalShearCyli nderUnderUniformExternalPressureln-Plane ConcentratedIx}adinInfiniteSheetIn-Plane ConcentratedLoadatEdgeofSheetCutoutReinf orcementOpenIsogri

many years of development, this stiffening concept is now being used as structure for Delta vehicle tanks and interstages (Reference 1o2), Delta shrouds, orbital shrouds, and Orbital Workshop interiors. The new structure is caUed "Isogrid" since it acts like an isotropic material. In a recent phase B design study funded by NASA for a ...

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Transcription of ISOGRID DESIGN HANDBOOK - NASA

1 NASACONTRACTORREPORTNASACR-124075 REVISIONAISOGRIDDESIGNHANDBOOKMcDonnellD ouglasAstronauticsCompany5301 BotsaAvenueHuntingtonBeach,Ca92647 February1973[NASA-CR-12_075)150 GRIDDESIGNHANDBOOK(McDonnell-DouqlasAstr onauticsCo.)222pHC$ .) ,GRIDDESIGNHANDBOOKMDCG4295 APREPAREDBY,V1 CDONNELLDOUGLASASTRONAUFIL;SCO_.,1 PANYFOR:NASAMARSHALLSPACEFLIGItTCEN] FOREWORDT hisprogram,thedevelopmentoftheisogriddes ignhandbook,wasconductedbytheMcDonnellDo uglasAstronauticsCompanyatHuntingtonBeac h,Cal.;forniaund_, ,MarshallSpaceFlightCenter, ,Direct:or,ResearchandDevelopment, ,beingresponsibleforSections2and4, :(1)theresultsofanalysis,test,andadvance dmanufacturingstudiesofIndependentResear chandDevelopmentprogcams,(2)aphaseBspace shuttleboosterstudyfundedbytheNASAM arshallSpaceFlightCenter,(3)anisogridtan ktestprogramfundedbytheNASAM arshallSpaceFlightCenter,and(4)theDeltap rogramisogridstructuraltestsfundedbytheN ASAG oddardSpaceFlightCenter, '.

2 ,BendingCylindersUnderTorsionalShearCyli nderUnderUniformExternalPressureln-Plane ConcentratedIx}adinInfiniteSheetIn-Plane ConcentratedLoadatEdgeofSheetCutoutReinf orcementOpenIsogridShearWebs()penIsogrid CylindersinCompression,BendingOpenandSki nnedIsogridtqatesMinimumOverallWeightfor CylinderSubjectedtoAxialCompressionandBe ndingNoteonUseofx,y;o,,(. ' ' '.001ill,? ] [m----_? (a,6)CurvesIsogridisSimpletoAnalyzeDistr ibutingConcentratedLoadEquipmentAttached toNodesSkylabFloorandWallGridReinforcedH oleforConcentratedLoadFail-SafeConceptAc cessDoorDesignsSpeedBrakesManufacturingS amplesofIsogridFormingIsogridSampleOptim umCurvesforSphericalCapwithReversePressu reDesignofIsogridSphericalBulkheadsLengt hDependenceofTheoreticalAxialCompression andBendingBucklingSolutionsInteractionCu rveShowingtheEffectofLengthWeightofOptim izedCompression-CriticalIsogridCylinders DesignofIsogridCylindersX,Y,a, ,Y,a,5 CurvesforCylindersUnderUniformExternalPr essureMasterCurvesforUniformExternalPres sureMasterCurvesforUniformExternalPressu reConcentratedLoadShearPanelk1,a,6 Curvesk2,a,5.)

3 ,-esX,Y,a,6 CurvesIsogridNodeMachiningIsogridwithUnf langedRibsMachiningIsogridwithFlangedRib sATankWallConfigurationElectricalDischar ge(EDM)orElectrochemical(ECM) , , , ! :a=[32 ISOGRIDDEFINITIONS thicknessofskinwidthofribwebdepthofwebde pthofflangewidthofflanget+d=platethickne ssofunflangedisogridheightoftrianglelego ftriangle, ,d:=mt'KDteffdistancecentertocenterofnod esTcbdwc =_'_-W'_:t-ffnon-dimensionalparameters(l +_+_I[3(I+6_z+-3_I* )z+I+_62*_ z]3[(1+6)-b_(l+k)]2bendingstiffnessparam eter.(Forunflangedisogrid, ,_z:[3_(1+6)z+(1+_)(1+_62)].)Et2(1+a+_)1 -visogrid):extensionalstiffness(Iz=0foru nflanged=(Et312)(( )1+a+ ISOGRID ):t(I+a+_)bendingstiffness(g :0forunflanged:equivalentthicknessformem branestresses(1_=0forunflangedisogrid)t( 1+3a 3t_)=equivalentweightthickness(_:0forunf langedisogrid)vlll_LtE_=01t1+_+_Equivale ntthicknessandYoung'smodulus=toobtaincor rectKandD(_=0forunflangedE(1+a+_)Zisogri d)UseofE*andt*inmonocoqueequationsgivesc orrectstressresultants,couples,strains, ,lightweight,economical, ,compression-load-carryingstructuresform partofallair-craft,booster, ,frame,anctskinconstruction,whichareofco urse9' ,however,weredesignedasint(:graliystiffe nec} ,theS-IIsecondstageduplicatedaircraft0-t o90-degreepat=ernswithanintegral, ,aswellastheThor.)))]

4 Reeand45-degreestiffeningpatternsu_edint hestagesoftheSaturnvehi, ,theyareinherentlyfourbarlin,< , ,Reference1-1, , , ,,' ,thisstiffeningconceptisnowbeingusedasst ructureforDeltavehicletanksandinterstage s(Reference1o2),Deltashrouds,orbitalshro uds, " ISOGRID " , ISOGRID (triangularintegralstiffening) (1)thecapabilityofcarryinghightorquesfro mthewings,(2)supplyingmultipleattachpoin tsforanexternalthermalprotectionsystem,a nd(3) (1)hightorsional_'esistance,(2)manynodal points,whichcouldbeusedasattachpointsfor thethermalprotectionsystem3tandoffstruct ures,and(3)thecapabilityofresistingtheor biterattachloadswithlocalstiffeningofthe isog_' ,Figure1-1, , ,bothbuiltinthesamestructuralstyle,mustb eattributedmainlytotheinstallationofequi pmentinnon-standardfashionintheformercom partment(seeFig ure1-2).

5 Evidently, ,muchasisogrid, "-'-----C) (CONICAL)AFTSKIRTSKINAND"; ,-USEOFTIIEtL,kNI)t_()C)t,,.Thishandhoot<pr,,suntsinforr;_,;t:o:llu't'e!_,dtodesignis,)firid,triangularintegralstiffenedstructur4, ,,'>-pointsal)()utis(,uri({ar,,.,,t_)\ ('(},.' ,.:,_.(',_tndflaF=_vrlis()_t'idwiththvin l(_rzll,,tioz'ionflangediso_ri(lh_,in,,: soct,. ,, \11()th,,riIlt'(_rzl,nli_,nnpt)li,,sl(,u nflanRediso, ,,rth,, ,s()_'.'idispr,'_,_' ,,rtin,":,_'cti(>n2,"]h 'usershouldacquaintIzill_s,,ltxxllhthi_a nalysisnnditsa, ()llSl)('i'Ol'("usinRthehandl)n()l<.B()t htlllIl;tllt2_,(']all(ll'lnn_ediso, ) (-basicth(,oryi-su,'_11_ilrix_,datth{,cn ([()tth,,._,cti(_i1t_)s(,r\_,asareadyr,' f(,renc(, ,dkli(Itii_'I,_N,_iii,l,ll,,lllllllt,,I, i!l,i!,l,i_,,I|iIt_,l,ill,'lll1,0,004 Tablei-1 ISOGRID00 Alatticeofintersectingribsforminganarray ofequilateraltriangh,sCharacteristics:-I sotropic(nodirectionsofinst,,bilitvt)rwe akness)-Poisson'sratio1/-Efficientinconl p,,-cssi_nandbcndint,Advantages:-Easilya nalyzed-Canbeoptimizedforwiderang_, ,_a:'commodateequipm,,nt_nountine,witlmu tchan_t.))))))))))}

6 -Readilyreinforcedforconccntratt,dloadsa nticutouts-Redundantloadpaths-Lessstruct uraldt, ,,,_ccproorams,'lilot'-l)cltaandSkylal_, andcxtunsix'clyinvcsti_aludandtestedonsp aceshuttlestudyeffortSection3describt,st hechl,raclt'risticsandadvantal2,'sofisog rid,includingsomecurrentandlttlurt,appli cation:,!orvt,hiclt, ,,Ihodsfo,"typicalstruclurufoundiraat,to -spacevehicles,l'ypicaltit,signsiluatit, nsat,,describedfor"eachtypeofstructure,a ntinwthods_foptiTr:i.<in,.:thestruclttr' t,fornainimutalw,'ightart,Rivenwheresuch mvthedsexist."lh,,nwthodofanalx'sisisfol lowedbyworkedexamples,whichart,gix',,nto ,e,,,fi(l_,tht,trs,,rinllu,applicationof theequationsandofthegraphs,"Ih,,tzraphs, ,nal)luthe,u,-,,rtoquicklyandaccuratelys izeisogridslruclur,,."l'h,,structuralIx, pusprest,nt,,darc: Sphericalcat)withr,,','(,rs(,prt,ssuru Cylindersincotlq) )_, Cylindersund_,rtorsion,_!

7 ' , ,tethesections.,informationisgivenon:(1) theminimumoverallweightforcylinderssubje ctedtoaxialcompres,_ionandbending,and(2) , , ,.. ,amodel,sub-scale, , : Machining Powerbrakeforming Creepandageforming CompoundcurvaturesReferenctsusedintht, ' "Section2 BASICTHEORYT heisogridrib-gridsareanalyzedby"smearing out",averaging, ,thesmeared-outelasticconstantsareidenti cal' ,theco,npositeconstructionistreatedasani sotropiclayeredmaterial,withappropriatee lasticconstantsforeachlayer,viz., ,thestressesinth." , , 'SLAWFORISOGRIDRIB-GRIDT heisogridribpatternconsistsofanetworkofe quilateral(60degree) 'slawrelationsaredevelopedbyisolatingane len_entofthegridworkandassumingthatthein dividualbarsareir, /\ElementofIsogridRibCridXBymeansofthest raintransformationlaw, +YsinOcosO.

8 +eeixxxyixYx( )oneobtainatherela:ionbetweentheuniaxial barstrains,ei,andthex,yand_ gridcoordinatestrains,ex,eyxyele2'3!40I- q_( ) ,known(forexamplefromstraingagereadings} then(ex,Infact,eyt'Oi'''102q'_-2 2-1Ze3sothatif(el,e2,e3)areYxy'ey)maybe( ,_) ,2,3{ }Resolutesofthebarloadsinthexandydirecti onsdividedbytheperiodiclengths,aand_tTag ivethe"smeared-out" +(P2+P3}cos60 4Pl+P2+P3( )Ha2_a(P_+P_)sin60 _(P2+P3}ya2a( )(P2-P3)sin60 P2-P3( )--T----TXyyX'_a2aUsingeq.( ),thrsebecome,{x}yih33]{} ( )whert_h-_-a, ( )and( }withtheHooke'slawrelationforisotropicma terialsinplanestress,(ry1-v2vyxyEryx-2(l +v}Xxyitisevidentthateq.( ),( }areaspecialcaseof( ),whe"e13b( )( )( )( )andthebarredquantitiesindicatetheequiva lentPoisson'sratioandYoung' , , (loadingonthcsurfaceisconsidLredtoberesi stedbystressresultantsantistres_couph'so btainodbyintegratingthestressesand,laome ntsinthethicknessdirection,OvNyMyiy_Y_i' iyxZNxZMxxMxv$ *lThesearecomputedperunitlengthoftherefe rencesurfacecoordinates, ,thesestressresultantsandcour) "xTxy_yTZX"rzy:f'le:YJZdz( )ZdZ( )whereN=NandM=MxyyxxyyxByuseoftheKirchho ff-Loveassumptionoflinearstrain,(z)x^(z) {YfIEXI_xyEYL-Z_x2 xyXy( )\vhere(_x,_xy'Ey)arereferencesurfacestr ainsand( x'2 Xxy'X_)arereferencesurfacechangesofcurva ture,togetherwiththeappropriateHooke' :/[i0o0:=ltx]0vDYXy/.)))))))

9 V[:ol,,_xyj=_MyxJ_Kistheextension_isti'f ness,K"--L-ll-v2fE(z)dzzDisthebendingsti ffness( )( )( )D-1----_vlJE(z)z2dz!zandthereferencesur facehasbeenchosensothat( )JE(z)zdz:0Z( )E(z)ofcourseistheappropriateYoung'amodu lusofribsorskinasafunctionofthethickness coordinate, ( )-( )maybeevaluatedgeometricallybyadevicekno wnasthemethodofthe"transformedsection." ( ) ( )0--/_z2dz,Eo( ,11)ThequantityE(z)/E maynowbethoughtofasa"transformedwidth" "-I_Li ]_i d12bib_d/2 TRANSFORMEDSECTIONOFhSOGRIDWITHFLANGELet t:skinthicknessb,d=:ribwebthicknessandde pthw,c: ,g, ,z,willbechosentosatisfythecondition,_EE -_zdz= {X--thUsingtheparallelaxistheorem, !Ai_iZPart1-t2t3 Qtt(1+5)(1+5)--(1+5)2T4 Qta000tt23t__(l+x)--f_(l+_l__(l+ (tz)t3_-_[l+ab2 vk2] ".. "!Then_iAi_iAS2_ioi= (1*a_u/[(1+ (l+kl]__t__21+,_+t_tZIZ,)3(1+812+_,p.))) ))}

10 ( +1+o,_2+pk"_[_l_-,(!_>,I]2[I+c*4bttOFt3_ zI-12(l+_.+..'_'where(1+a+-g)_( )"_3t*(1+kl+1+c,t,v} (1+6} :a,b,k, { (=( )and( )oneobtains_8 EoIEoA( )sincev:1 'sratiooftheskinmaterialisalso1 ,itwillnotbepossibletoexpresseq.( )and( )inthesimpleformshown, ( )and( ).Forthinrib,thesetermsarenegligible, ,3 NON-DIMENSIONALSTIFFNESSESFORUNFLANGEDIS OGRIDF orunflangedisogrid,k=_t= :_(_,a):[3_(1+6)2+(1+_,)(l+,_a2)]( )Forconstructionconsistingofskinalone(mo nocoque),a=:b:o,13=1( ) [3,EtoK:_(l+a)1-v( )Et3oLD=12( )l+a( )ItwillbenotedthatEt/1-v2andEt3/12(1-v2) aretheextensionalandoobendingstiffnesses oftheskinalone,whilethenon-dimensionalfa ctors(l+a)and[52/(1+a) (a,b) [ ,forexample, ,[52=C1+ [3,Ifthisrelationisplottedontransparentp apertothesame[3,ascaleasthe[3(a,6)grapha ndsuperimposedonthe[5(a,6)graph, [5(a,6) , (a,dl) ,Reference2= ,Nxy, ( )reducesto,Ny[.))))))]]]]]]]]]]]


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