2012 Vol. 32, No. 3
                Display Method:
    			
	    		
	    		
	    		
   			
    	
		            2012, 32(3): 225-230. 
	            	doi: 10.11883/1001-1455(2012)03-0225-06 
   					
					
		        
					Abstract: 
Theaxialstressandtheaxialdeformationofthechargeexplosiveinaprojectilewastheoreticallyanalyzedduringthepenetrationprocess. Thecorrespondingdistributionfunctionsalongtheaxis ofthechargeexplosivewereattainedbyconsideringtheelasticandplasticdeformationofthecharge explosive.Basedonthefriction-inducedheataswellastheheatconduction,thetemperaturedistributionalongtheaxisofthechargeexplosivewasobtained. Calculatedresultsshowthatthemaximum temperatureriseanditslocationinthechargeexplosivearedependentonthechargelengthandtheoverloadpeakinadditiontothephysicalpropert parametersoftheexplosive.Thecalculatedcritical chargelengthcanbetakenasareferenceforthechargedesign.Thisinvestigationcanprovideatheoreticalbasisforthechargedesignandthesafetyanalysisintheengineeringpracticeoftheprojectile penetration.
		       
		        
		        
			  
			Theaxialstressandtheaxialdeformationofthechargeexplosiveinaprojectilewastheoreticallyanalyzedduringthepenetrationprocess. Thecorrespondingdistributionfunctionsalongtheaxis ofthechargeexplosivewereattainedbyconsideringtheelasticandplasticdeformationofthecharge explosive.Basedonthefriction-inducedheataswellastheheatconduction,thetemperaturedistributionalongtheaxisofthechargeexplosivewasobtained. Calculatedresultsshowthatthemaximum temperatureriseanditslocationinthechargeexplosivearedependentonthechargelengthandtheoverloadpeakinadditiontothephysicalpropert parametersoftheexplosive.Thecalculatedcritical chargelengthcanbetakenasareferenceforthechargedesign.Thisinvestigationcanprovideatheoreticalbasisforthechargedesignandthesafetyanalysisintheengineeringpracticeoftheprojectile penetration.
		            2012, 32(3): 231-236. 
	            	doi: 10.11883/1001-1455(2012)03-0231-06 
   					
					
		        
					Abstract: 
Dynamicuniaxialcompressionandindirecttensile(Brazilian)testswereconductedforcertaintypicalplastic- bondedexplosivesonasplitHopkinsonpressurebar(SHPB),respectively.The stressequilibriumandconstantstrainrateoflowimpedancematerialswereachievedbyusingthe pulseshapertechnique,andthestress-straincurvesoftheplastic-bondedexplosiveswereobtainedby combiningthesemi-conductorstraingaugesandpiezoelectricityquartzgauges.Basedontheexperimentaldataobtained, thephenomenologicalconstitutivemodelforacertainplastic-bondedexplosive wasproposedbymodifyingtheSarginmodel.Thefractureprocessesontheexplosivesamplesurfaces werecapturedbyusingahigh-speedcamerainthedynamicBraziliantestsandthestrainfieldwascalculatedbythedigitalspecklecorrelationmethod. AndthemodifiedJohnson-Cookmodelswereobtainedforthreekindsoftheplastic- bondedexplosives.Theobtainedmodelsareconsistentwiththe experimentaldata.
		       
		        
		        
			  
			Dynamicuniaxialcompressionandindirecttensile(Brazilian)testswereconductedforcertaintypicalplastic- bondedexplosivesonasplitHopkinsonpressurebar(SHPB),respectively.The stressequilibriumandconstantstrainrateoflowimpedancematerialswereachievedbyusingthe pulseshapertechnique,andthestress-straincurvesoftheplastic-bondedexplosiveswereobtainedby combiningthesemi-conductorstraingaugesandpiezoelectricityquartzgauges.Basedontheexperimentaldataobtained, thephenomenologicalconstitutivemodelforacertainplastic-bondedexplosive wasproposedbymodifyingtheSarginmodel.Thefractureprocessesontheexplosivesamplesurfaces werecapturedbyusingahigh-speedcamerainthedynamicBraziliantestsandthestrainfieldwascalculatedbythedigitalspecklecorrelationmethod. AndthemodifiedJohnson-Cookmodelswereobtainedforthreekindsoftheplastic- bondedexplosives.Theobtainedmodelsareconsistentwiththe experimentaldata.
					Characteristiccurvemethodforanalyzingmovementofflyerplate
basedonuniversalequationofstateofexplosive
						
				
		        
		            2012, 32(3): 237-242. 
	            	doi: 10.11883/1001-1455(2012)03-0237-06 
   					
					
		        
					Abstract: 
Fromthephysicaldefinitionofperturbationpropagation(Machwaves),thecharacteristic equationsofatwo-dimensionalsupersonicflowwerededucedintotheformswhichwereuncorrelated withtheformulaofEOS.Meanwhile,anewPrantl-Meyerfunctionwasexpressedintoasimplevariablefunctionoffluiddensityalso. Basedoncharacteristicdifference,asolutionmethodofthetwo-dimensionalsupersonicflowwasbuiltup. Therefore,asanapplicationexampleofthesolutionmethod, themovementoftheflyerplatedrivenbyglancingdetonationwasanalyzed.Forcomparison,DetonationdrivesoftheTNTandemulsionexplosiveswerecalculatedwithJWLandpolytropicEOSs. The numericalresultsshowthatcharacteristicdifferencesolutionscompletelyagreewiththeexpanding worksofexplosiveEOSs.
		       
		        
		        
			  
			Fromthephysicaldefinitionofperturbationpropagation(Machwaves),thecharacteristic equationsofatwo-dimensionalsupersonicflowwerededucedintotheformswhichwereuncorrelated withtheformulaofEOS.Meanwhile,anewPrantl-Meyerfunctionwasexpressedintoasimplevariablefunctionoffluiddensityalso. Basedoncharacteristicdifference,asolutionmethodofthetwo-dimensionalsupersonicflowwasbuiltup. Therefore,asanapplicationexampleofthesolutionmethod, themovementoftheflyerplatedrivenbyglancingdetonationwasanalyzed.Forcomparison,DetonationdrivesoftheTNTandemulsionexplosiveswerecalculatedwithJWLandpolytropicEOSs. The numericalresultsshowthatcharacteristicdifferencesolutionscompletelyagreewiththeexpanding worksofexplosiveEOSs.
		            2012, 32(3): 243-250. 
	            	doi: 10.11883/1001-1455(2012)03-0243-08 
   					
					
		        
					Abstract: 
Theignition-growthreactivemodelandadesensitizingmodelwereintroducedintotheselfdevelopedtwo- dimensionalmulticomponentEulerianelastic-plastichydrodynamicscode(MEPH2Y), respectively.Numericalstudieswerecarriedoutonsomedetonativephenomenaincludingtheshock ignition,thediametereffectandtheformationofthedeadzone,withtheaidoftheadaptivemeshrefinementtechnique. Thenumericalresultsshowthatthecomputationcansimulatethemajorcharacteristicsoftheplanardetonationwaves, suchasthedetonationwavespeed,CJstate,vonNeumann spikestateandsoon.Andthediametereffectsoftheexplosivescanbesimulatedcorrectly.Under theconsiderationofthedesensitizingreactivemodel,thedeadzoneformationoftheinsensitivehigh explosivescanalsobereproduced.
		       
		        
		        
			  
			Theignition-growthreactivemodelandadesensitizingmodelwereintroducedintotheselfdevelopedtwo- dimensionalmulticomponentEulerianelastic-plastichydrodynamicscode(MEPH2Y), respectively.Numericalstudieswerecarriedoutonsomedetonativephenomenaincludingtheshock ignition,thediametereffectandtheformationofthedeadzone,withtheaidoftheadaptivemeshrefinementtechnique. Thenumericalresultsshowthatthecomputationcansimulatethemajorcharacteristicsoftheplanardetonationwaves, suchasthedetonationwavespeed,CJstate,vonNeumann spikestateandsoon.Andthediametereffectsoftheexplosivescanbesimulatedcorrectly.Under theconsiderationofthedesensitizingreactivemodel,thedeadzoneformationoftheinsensitivehigh explosivescanalsobereproduced.
		            2012, 32(3): 251-258. 
	            	doi: 10.11883/1001-1455(2012)03-0251-08 
   					
					
		        
					Abstract: 
Toidentifytheanti-explosionperformancesofreinforcedconcrete(RC)slabs,close-inexplosionexperimentswereconductedforsquareRCslabssupportedunidirectionally, inwhichtheRC slabswereloadedbyTNTcharges.BasedonthecommercialhydrocodeAUTODYN,athree-dimensionalsolidmodelincludingexplosive, airandRCslabwithconcreteandreinforcingbarsbeingseparatedwasdevelopedbyusingthegas- solidcoupledtechniquetosimulatethedynamicresponseofthe RCslabs.Inthenumericalsimulation,thestrainrateeffectsweretakenintoaccountonthedynamicalconstitutivebehaviorsofthesophisticatedconcreteandreinforcingbarmaterial .Sequentially,the correspondingdamagemechanismsandfailuremodesoftheRCslabswereanalyzedunderdifferent TNTchargeweights.ThedynamicalevolutionprocessofRCslabswasobservedrealisticallyfrom crackingandbreaking-upoftheconcrete,yieldingandrupturingofreinforcingbarstolocalperforation. ThedamageoftheRCslabsbythenumericalsimulationisingoodagreementwiththeexperimentalresults. AndwiththeincreaseoftheTNTchargeweights,thefailuremodeofRCslabsgraduallychangesfromoverallflexurefailuretolocalpunchingfailure
		       
		        
		        
			  
			Toidentifytheanti-explosionperformancesofreinforcedconcrete(RC)slabs,close-inexplosionexperimentswereconductedforsquareRCslabssupportedunidirectionally, inwhichtheRC slabswereloadedbyTNTcharges.BasedonthecommercialhydrocodeAUTODYN,athree-dimensionalsolidmodelincludingexplosive, airandRCslabwithconcreteandreinforcingbarsbeingseparatedwasdevelopedbyusingthegas- solidcoupledtechniquetosimulatethedynamicresponseofthe RCslabs.Inthenumericalsimulation,thestrainrateeffectsweretakenintoaccountonthedynamicalconstitutivebehaviorsofthesophisticatedconcreteandreinforcingbarmaterial .Sequentially,the correspondingdamagemechanismsandfailuremodesoftheRCslabswereanalyzedunderdifferent TNTchargeweights.ThedynamicalevolutionprocessofRCslabswasobservedrealisticallyfrom crackingandbreaking-upoftheconcrete,yieldingandrupturingofreinforcingbarstolocalperforation. ThedamageoftheRCslabsbythenumericalsimulationisingoodagreementwiththeexperimentalresults. AndwiththeincreaseoftheTNTchargeweights,thefailuremodeofRCslabsgraduallychangesfromoverallflexurefailuretolocalpunchingfailure
		            2012, 32(3): 259-266. 
	            	doi: 10.11883/1001-1455(2012)03-0259-08 
   					
					
		        
					Abstract: 
AdamageimagingmethodusingLambwaveandmatchingpursuitmethodforcontinuous on-linemonitoringofcompositewasproposed.First,asignalprocessingmethodisdevelopedusing matchingpursuits.ItcandecomposeLambsignalsintoalinearexpansionofseveralchirpletatoms withafastoperationspeed.Second,therelationshipbetweenLambwavesdispersionandchirplets chirprateisdeveloped.Itshowsthatthechirpletatomcanmatchthedispersionpulseaccurately,and itcanbeusedtoidentifythemodesofLambwaves.Third,accordingtothesignaldifferencebefore andafterdamage,adamageindexcanbegetfromthedifferencesintheenergycharacteristicsoflamb wave.TheimagethatindicatesthedamagecanbeobtainedbytheRAPIDalgorithm.Theexperimentalresultsdemonstratetheapplicabilityandeffectivenessoftheproposedmethod.
		       
		        
		        
			  
			AdamageimagingmethodusingLambwaveandmatchingpursuitmethodforcontinuous on-linemonitoringofcompositewasproposed.First,asignalprocessingmethodisdevelopedusing matchingpursuits.ItcandecomposeLambsignalsintoalinearexpansionofseveralchirpletatoms withafastoperationspeed.Second,therelationshipbetweenLambwavesdispersionandchirplets chirprateisdeveloped.Itshowsthatthechirpletatomcanmatchthedispersionpulseaccurately,and itcanbeusedtoidentifythemodesofLambwaves.Third,accordingtothesignaldifferencebefore andafterdamage,adamageindexcanbegetfromthedifferencesintheenergycharacteristicsoflamb wave.TheimagethatindicatesthedamagecanbeobtainedbytheRAPIDalgorithm.Theexperimentalresultsdemonstratetheapplicabilityandeffectivenessoftheproposedmethod.
		            2012, 32(3): 267-272. 
	            	doi: 10.11883/1001-1455(2012)03-0267-06 
   					
					
		        
					Abstract: 
Abstract:Undergroundexplosionexperimentswiththeexplosionequivalentof100kgTNTwereperformedindifferentgeologicalmediums, suchasloess,sand-gravelcompositeandgranite.Andthe correspondingsurfacegroundmotionsinducedbyundergroundexplosionswereobservedbyaseriesof seismometers.Byusingtheseobserveddata,thesourceparameterswereobtained,aswellasthe seismiccouplingefficiencyrepresentedbythesteadyvalueofreducedvelocitypotentialatlowfrequencies. Experimentalresultsdisplaythatfortheundergroundexplosionswiththesamescaleddepth ofburialandsameexplosionequivalent,theseismiccouplingefficiencywasstronglydependantonthe sourcemediumpropertyinsuchawaythatthemediumstrengthplaysthemostsignificantrolesindeterminingtheseismiccouplingeffectandthenthe orosityandthewatersaturation.Andbasedonthe experimentaldata,thefeasibilityoftheempiricalformulaproposedbyM.D.Denny,etalwasanalyzedinestimatingtheseismiccouplingeffectofundergroundexplosionswiththeexplosionequivalent of100kgTNT.
		       
		        
		        
			  
			Abstract:Undergroundexplosionexperimentswiththeexplosionequivalentof100kgTNTwereperformedindifferentgeologicalmediums, suchasloess,sand-gravelcompositeandgranite.Andthe correspondingsurfacegroundmotionsinducedbyundergroundexplosionswereobservedbyaseriesof seismometers.Byusingtheseobserveddata,thesourceparameterswereobtained,aswellasthe seismiccouplingefficiencyrepresentedbythesteadyvalueofreducedvelocitypotentialatlowfrequencies. Experimentalresultsdisplaythatfortheundergroundexplosionswiththesamescaleddepth ofburialandsameexplosionequivalent,theseismiccouplingefficiencywasstronglydependantonthe sourcemediumpropertyinsuchawaythatthemediumstrengthplaysthemostsignificantrolesindeterminingtheseismiccouplingeffectandthenthe orosityandthewatersaturation.Andbasedonthe experimentaldata,thefeasibilityoftheempiricalformulaproposedbyM.D.Denny,etalwasanalyzedinestimatingtheseismiccouplingeffectofundergroundexplosionswiththeexplosionequivalent of100kgTNT.
		            2012, 32(3): 273-277. 
	            	doi: 10.11883/1001-1455(2012)03-0273-05 
   					
					
		        
					Abstract: 
LiquidparaffinandRDXexplosiveweremixedintocopperacetateusedasaprecursor.The well-proportionedmixturewasinitiatedinadetonationreactioncontainerthatwasvacuumedtoprepareperfectsphericalnano- coppercrystalparticles.Themorphologyandcompositionofthedetonationsootwereanalyzedbytransmissionelectronmicroscopy (TEM)andX-raydiffraction (XRD). AndthecarbonstructuresinthedetonationsootwerecharacterizedbyRamanspectroscopy.Theresultsindicatethatthestructureofthecoppernano- particlespreparedbythedetonationtechniqueis sphericalwithasmoothsurface.Moreover,thediametersofthecoppernano-particlesaredistributed between150~200nm.Sothedetonationtechniquecanprovideasimpleandrapidwaytopreparecoppernano- particleswithagoodroundness.
		       
		        
		        
			  
			LiquidparaffinandRDXexplosiveweremixedintocopperacetateusedasaprecursor.The well-proportionedmixturewasinitiatedinadetonationreactioncontainerthatwasvacuumedtoprepareperfectsphericalnano- coppercrystalparticles.Themorphologyandcompositionofthedetonationsootwereanalyzedbytransmissionelectronmicroscopy (TEM)andX-raydiffraction (XRD). AndthecarbonstructuresinthedetonationsootwerecharacterizedbyRamanspectroscopy.Theresultsindicatethatthestructureofthecoppernano- particlespreparedbythedetonationtechniqueis sphericalwithasmoothsurface.Moreover,thediametersofthecoppernano-particlesaredistributed between150~200nm.Sothedetonationtechniquecanprovideasimpleandrapidwaytopreparecoppernano- particleswithagoodroundness.
		            2012, 32(3): 278-282. 
	            	doi: 10.11883/1001-1455(2012)03-0278-05 
   					
					
		        
					Abstract: 
Basedonthetwo-dimensionalaxisymmetricEulerequationscouplingwithchemicalreactions, thephenomenaofobliquedetonationinducedbyahypervelocityballinhydrogen-oxygen-nitrogen mixturewerenumericallystudiedbyusingwavepropagationalgorithm withSuperbeelimiter. Theresultsshowthatthestandingdetonationinducedbyaballshowthecompositestructureat Damkohlernumberconditionslightlylargerthanthethreshold,whosestructureiscomposedofa strongoverdrivenobliquedetonation,aweakoverdrivenobliquedetonation,areactingshockwave andainertshockwave.Thereweretwosubsoniczoneandasupersoniczoneintheflowpastasphere afterwave.Thesecondobliqueshockwavewasformedintheleewardsurfaceoftheball.
		       
		        
		        
			  
			Basedonthetwo-dimensionalaxisymmetricEulerequationscouplingwithchemicalreactions, thephenomenaofobliquedetonationinducedbyahypervelocityballinhydrogen-oxygen-nitrogen mixturewerenumericallystudiedbyusingwavepropagationalgorithm withSuperbeelimiter. Theresultsshowthatthestandingdetonationinducedbyaballshowthecompositestructureat Damkohlernumberconditionslightlylargerthanthethreshold,whosestructureiscomposedofa strongoverdrivenobliquedetonation,aweakoverdrivenobliquedetonation,areactingshockwave andainertshockwave.Thereweretwosubsoniczoneandasupersoniczoneintheflowpastasphere afterwave.Thesecondobliqueshockwavewasformedintheleewardsurfaceoftheball.
		            2012, 32(3): 283-290. 
	            	doi: 10.11883/1001-1455(2012)03-0283-08 
   					
					
		        
					Abstract: 
Accordingtothecharacteristicsoftransientplasmaejectorscreatedbyhypervelocityimpact, thesweepLangmuirprobe,thetripleLangmuirprobeandthecoilmeasurementsystemswere establishedtomeasuretheplasmacharacteristicparametersaswellasthemagneticinductionintensity inexpandingplasmacloud.Basedonthegivenlayoutandazimuthangleofthesensors,theelectromagneticcharacteristicmeasurementsofexpandingplasmacloudgeneratedbytheimpactof2024- T4 aluminumprojectilesagainstthe2024-T4aluminumtargetsinthelaboratorywerecarriedoutatthe twoimpactvelocities.Experimentalresultsshowthattheaverageelectrontemperature,electrondensity, andmagneticinductionintensityamplitudevalueare0.4~0.9eV,ontheorderof1012cm-3and 10~20nT,respectively.Byprocessingtheexperimentaldata,therelationshipsbetweenelectron temperature,electrondensityand magneticinductionintensitywereobtained,respectively,atthe givenpositionsoftheprobesandcoilsduringthewholephysicalprocessforthetwoexperiments.And theresultsmeasuredbythesweepLangmuirprobeandthetripleLangmuirprobewerecompared.
		       
		        
		        
			  
			Accordingtothecharacteristicsoftransientplasmaejectorscreatedbyhypervelocityimpact, thesweepLangmuirprobe,thetripleLangmuirprobeandthecoilmeasurementsystemswere establishedtomeasuretheplasmacharacteristicparametersaswellasthemagneticinductionintensity inexpandingplasmacloud.Basedonthegivenlayoutandazimuthangleofthesensors,theelectromagneticcharacteristicmeasurementsofexpandingplasmacloudgeneratedbytheimpactof2024- T4 aluminumprojectilesagainstthe2024-T4aluminumtargetsinthelaboratorywerecarriedoutatthe twoimpactvelocities.Experimentalresultsshowthattheaverageelectrontemperature,electrondensity, andmagneticinductionintensityamplitudevalueare0.4~0.9eV,ontheorderof1012cm-3and 10~20nT,respectively.Byprocessingtheexperimentaldata,therelationshipsbetweenelectron temperature,electrondensityand magneticinductionintensitywereobtained,respectively,atthe givenpositionsoftheprobesandcoilsduringthewholephysicalprocessforthetwoexperiments.And theresultsmeasuredbythesweepLangmuirprobeandthetripleLangmuirprobewerecompared.
		            2012, 32(3): 291-296. 
	            	doi: 10.11883/1001-1455(2012)03-0291-06 
   					
					
		        
					Abstract: 
Aimedathightemperatureandhighpressurecharacteristicsgeneratedfromtoroidalshock wavefocusing,adiscontinuousfiniteelementmethodwasusedtonumericallysimulatetoroidalshock wavefocusinginaco-axiscylindricaltube.Thesimulatedresultsindicatethatthediscontinuousfinite elementmethodcancaptureefficientlythecomplicatedflow-fieldwavestructureswhichincludesecondaryshock wave,vortexring,triplepointandsphericaldouble Machreflectionformedduring shockwavespropagatingintheco-axialcylindricalshocktube.Andfromthesimulatedresults,itcan befoundthattheinnerradiusofthetoroidalpipelinecanaffectmarkedlythevalueandlocationofthe peakpressurealongtheaxisline,andtheouterradiusofthetoroidalpipelineplaysaweakrole.The investigatedresultscanprovideatheoreticalguideforengineeringapplication.
		       
		        
		        
			  
			Aimedathightemperatureandhighpressurecharacteristicsgeneratedfromtoroidalshock wavefocusing,adiscontinuousfiniteelementmethodwasusedtonumericallysimulatetoroidalshock wavefocusinginaco-axiscylindricaltube.Thesimulatedresultsindicatethatthediscontinuousfinite elementmethodcancaptureefficientlythecomplicatedflow-fieldwavestructureswhichincludesecondaryshock wave,vortexring,triplepointandsphericaldouble Machreflectionformedduring shockwavespropagatingintheco-axialcylindricalshocktube.Andfromthesimulatedresults,itcan befoundthattheinnerradiusofthetoroidalpipelinecanaffectmarkedlythevalueandlocationofthe peakpressurealongtheaxisline,andtheouterradiusofthetoroidalpipelineplaysaweakrole.The investigatedresultscanprovideatheoreticalguideforengineeringapplication.
		            2012, 32(3): 297-302. 
	            	doi: 10.11883/1001-1455(2012)03-0297-06 
   					
					
		        
					Abstract: 
ByusinganelectronicuniversaltestingmachineandasplitHopkinsonpressurebardevice, aseriesofuniaxialcompressionexperimentswerecarriedouttoexplorethemechanicalbehaviorsofa 2DwovenC/SiCcompositeinthetemperaturerangefrom293to1273Kandthestrainraterange from10-4to103s-1.Theexperimentalresultsshowasfollows.Thecompositehasexcellenthigh temperaturemechanicalpropertiesinthetestedtemperaturerange.Thecompressivestrengthofthe compositedecreasesnomorethanthirtypercentat1273Kunderquasi-staticcompressionifcompared withthatatroomtemperature.Catastrophicbrittlefailureisnotobservedforthespecimenstestedat differentstrainrates.Withtheincreaseoftheexperimentaltemperature,thecompressivestrengthof the2DC/SiCcompositedecreases,butthedependenceofcompressivestrengthonstrainrateincreases. Atthetemperaturesabove1073K,thesensitivityfactorofcompressivestrengthonstrainrate increasesremarkably.Itisproposedthatthesharpincreaseinthedependenceofcompressivestrength onstrainrateisduetotheoxidationofthecomposites.
		       
		        
		        
			  
			ByusinganelectronicuniversaltestingmachineandasplitHopkinsonpressurebardevice, aseriesofuniaxialcompressionexperimentswerecarriedouttoexplorethemechanicalbehaviorsofa 2DwovenC/SiCcompositeinthetemperaturerangefrom293to1273Kandthestrainraterange from10-4to103s-1.Theexperimentalresultsshowasfollows.Thecompositehasexcellenthigh temperaturemechanicalpropertiesinthetestedtemperaturerange.Thecompressivestrengthofthe compositedecreasesnomorethanthirtypercentat1273Kunderquasi-staticcompressionifcompared withthatatroomtemperature.Catastrophicbrittlefailureisnotobservedforthespecimenstestedat differentstrainrates.Withtheincreaseoftheexperimentaltemperature,thecompressivestrengthof the2DC/SiCcompositedecreases,butthedependenceofcompressivestrengthonstrainrateincreases. Atthetemperaturesabove1073K,thesensitivityfactorofcompressivestrengthonstrainrate increasesremarkably.Itisproposedthatthesharpincreaseinthedependenceofcompressivestrength onstrainrateisduetotheoxidationofthecomposites.
		            2012, 32(3): 303-308. 
	            	doi: 10.11883/1001-1455(2012)03-0303-06 
   					
					
		        
					Abstract: 
Thegenerationcauseofimpactforceduringthemicro-detonationmachiningprocesswasintroduced. Themainprocessingparameterswereconfirmedby meansofsingle-factorexperiments. Basedonaboveparameters,anexponential-typeempiricalmodelforimpactforcewasbuiltbyemployingtheorthogonalexperimentsandtheregressionanalysis. Andtheinfluencesoftheprocessingparametersonimpactforcewereanalyzed. Investigatedresultsdisplaythat:theworkingcurrentandthe workingpressureaswellasthenozzlediameterofthemicro-detonationgeneratorarethemainprocessingparameterstodeterminetheimpactforcemagnitude. Theimpactforcedecreaseswithanincreaseintheworkingcurrentanditincreaseswithincreasesintheworkingpressureandthenozzlediameter. Ontheotherhand,theworkingpulsewidthandtheworkingdistancehaveinsignificantinfluencesontheimpactforcemagnitude. Andtheimpactforcemodelisconsistentwiththeexperimental results.Sotheresearchcanofferanimportantreferencefortheprocesscontrolofmicro-detonation machiningwithstrikingarc.
		       
		        
		        
			  
			Thegenerationcauseofimpactforceduringthemicro-detonationmachiningprocesswasintroduced. Themainprocessingparameterswereconfirmedby meansofsingle-factorexperiments. Basedonaboveparameters,anexponential-typeempiricalmodelforimpactforcewasbuiltbyemployingtheorthogonalexperimentsandtheregressionanalysis. Andtheinfluencesoftheprocessingparametersonimpactforcewereanalyzed. Investigatedresultsdisplaythat:theworkingcurrentandthe workingpressureaswellasthenozzlediameterofthemicro-detonationgeneratorarethemainprocessingparameterstodeterminetheimpactforcemagnitude. Theimpactforcedecreaseswithanincreaseintheworkingcurrentanditincreaseswithincreasesintheworkingpressureandthenozzlediameter. Ontheotherhand,theworkingpulsewidthandtheworkingdistancehaveinsignificantinfluencesontheimpactforcemagnitude. Andtheimpactforcemodelisconsistentwiththeexperimental results.Sotheresearchcanofferanimportantreferencefortheprocesscontrolofmicro-detonation machiningwithstrikingarc.
		            2012, 32(3): 309-315. 
	            	doi: 10.11883/1001-1455(2012)03-0309-07 
   					
					
		        
					Abstract: 
Basedontheexperimentaldataofanunderwatertargetsubjectedtounderwaterexplosion, thetime-frequencycharacteristicsofthemonitoredinterioraccelerationsignalswerestudiedbymeans ofwaveletanalysiswithhighresolvabilityandlocalization.Byusingthesesignals,theaccelerationtimecurvesandtheenergydistributionsindifferentblastingfrequencybandswereobtained. Theanalyzedresultsshowthatthewaveletenergyinagivenfrequencybandcancoinstantaneouslyreflectthe influencesofvibrationstrength,frequency,anddurationonthedamageeffectoftheunderwatertarget. Andthedistributionandattenuationdetailinformationoftheshockwaveandsecondarypressure waveindifferentfrequencybandswasobtainedbycombiningtheacceleration-timecurvesindifferent blastingfrequencybands.Thereby,theinfluencesoftheshockwaveandthesecondarypressurewave onthedamageeffectoftheunderwatertargetcanbeassessed,respectively.
		       
		        
		        
			  
			Basedontheexperimentaldataofanunderwatertargetsubjectedtounderwaterexplosion, thetime-frequencycharacteristicsofthemonitoredinterioraccelerationsignalswerestudiedbymeans ofwaveletanalysiswithhighresolvabilityandlocalization.Byusingthesesignals,theaccelerationtimecurvesandtheenergydistributionsindifferentblastingfrequencybandswereobtained. Theanalyzedresultsshowthatthewaveletenergyinagivenfrequencybandcancoinstantaneouslyreflectthe influencesofvibrationstrength,frequency,anddurationonthedamageeffectoftheunderwatertarget. Andthedistributionandattenuationdetailinformationoftheshockwaveandsecondarypressure waveindifferentfrequencybandswasobtainedbycombiningtheacceleration-timecurvesindifferent blastingfrequencybands.Thereby,theinfluencesoftheshockwaveandthesecondarypressurewave onthedamageeffectoftheunderwatertargetcanbeassessed,respectively.
		            2012, 32(3): 316-322. 
	            	doi: 10.11883/1001-1455(2012)03-0316-07 
   					
					
		        
					Abstract: 
Basedonthesmoothedparticlehydrodynamics(SPH)methodinLS-DYNAsoftware,the shapedchargejetprocesswassimulated.Andthemechanismoftheshapedchargejetwasdiscussed accordingtothenumericalsimulationresults.Toanalyzetheaccuracy,effectivenessandsuperiority aboutthismethod,aswellastheerrorbroughtbydifferentinitialnumbersN oftouchingneighbors perparticle,thenumericalsimulationresultswerecomparedwithtwo-dimensional(2D)finiteelementresultsandtheoreticalcalculations. Theinvestigatedresultsshowthatsomeproblems,suchas griddistortion,windingandcontactpenetrationwhichoftenhappeninthefiniteelementmethod,can beavoidedintheSPH method,sothecalculationprocessbytheSPH methodisstable,andthecalculationprecisionishigherthanthatbythe2Dfiniteelementmethod. Therelativeerrorofthejettip velocityandthejetlengthcalculatedbytheSPH methodcomparedwiththefiniteelementresultsand theoreticalcalculationsarebothlowerthanfivepercent,thereforetheSPH methodisadaptablein multi-material,largedeformationproblemssuchasshapedcharges.ThemostidealNisfrom600to 1800,inwhichtherelativeerrorislowerthan3%andthecomputationalefficiencyishigh.
		       
		        
		        
			  
			Basedonthesmoothedparticlehydrodynamics(SPH)methodinLS-DYNAsoftware,the shapedchargejetprocesswassimulated.Andthemechanismoftheshapedchargejetwasdiscussed accordingtothenumericalsimulationresults.Toanalyzetheaccuracy,effectivenessandsuperiority aboutthismethod,aswellastheerrorbroughtbydifferentinitialnumbersN oftouchingneighbors perparticle,thenumericalsimulationresultswerecomparedwithtwo-dimensional(2D)finiteelementresultsandtheoreticalcalculations. Theinvestigatedresultsshowthatsomeproblems,suchas griddistortion,windingandcontactpenetrationwhichoftenhappeninthefiniteelementmethod,can beavoidedintheSPH method,sothecalculationprocessbytheSPH methodisstable,andthecalculationprecisionishigherthanthatbythe2Dfiniteelementmethod. Therelativeerrorofthejettip velocityandthejetlengthcalculatedbytheSPH methodcomparedwiththefiniteelementresultsand theoreticalcalculationsarebothlowerthanfivepercent,thereforetheSPH methodisadaptablein multi-material,largedeformationproblemssuchasshapedcharges.ThemostidealNisfrom600to 1800,inwhichtherelativeerrorislowerthan3%andthecomputationalefficiencyishigh.
		            2012, 32(3): 323-327. 
	            	doi: 10.11883/1001-1455(2012)03-0323-05 
   					
					
		        
					Abstract: 
Inordertoobtaintheimpactparametersdominatingtheaccuracyandvalidityofgunrecoil simulationexperiments,thevirtualsimulationtestmodelforacertaingunwasdevelopedbasedon MSC.ADAMSsoftware.Andthedevelopedmodelwasappliedtonumericallysimulatethedynamic recoilandcounterrecoilofthegunandtoconducttheuniformdesignexperimentsfortheimpactparameters. Thenumericallysimulatedresultswerecomparedwiththeexperimentalones.Itisshown thattheimpactparametersobtainedbythedevelopedmodelarereasonableandthesimulationtestis valid.
		       
		        
		        
			  
			Inordertoobtaintheimpactparametersdominatingtheaccuracyandvalidityofgunrecoil simulationexperiments,thevirtualsimulationtestmodelforacertaingunwasdevelopedbasedon MSC.ADAMSsoftware.Andthedevelopedmodelwasappliedtonumericallysimulatethedynamic recoilandcounterrecoilofthegunandtoconducttheuniformdesignexperimentsfortheimpactparameters. Thenumericallysimulatedresultswerecomparedwiththeexperimentalones.Itisshown thattheimpactparametersobtainedbythedevelopedmodelarereasonableandthesimulationtestis valid.
		            2012, 32(3): 328-332. 
	            	doi: 10.11883/1001-1455(2012)03-0328-05 
   					
					
		        
					Abstract: 
TodevelopanignitionandgrowthreactionflowmodelforHNS-Ⅳexplosive,cylindertests wereconductedonHNS-ⅣexplosiveandtheexpansionprocessesofthecoppercylinderwallswererecordedbyaGSJhighspeedrotatingmirrorcamera, andparticlevelocitiesattheinterfacebetween HNS-ⅣexplosiveandLiFwindowweremeasuredwithlaservelocityinterferometry(VISAR).The correspondingnumericalsimulationswerecarriedoutbyANSYS/LS-DYNA,respectively.TheJWL equation-of-stateparametersforunreactedexplosivewerefittedtotheavailableshockHugoniotdata. Andbycombiningtheexperimentalresultsandnumericalsimulations,theJWLequation-of-stateparametersfordetonationproductweredetermined, aswellasreactiverateparametersforreactionignitionandgrowthin HNS-Ⅳ explosive.Investigatedresultsshowthatthedevelopedignitionand growthreactionflow modelcanbeusedtopicturethereactionprocessofHNS-Ⅳexplosive,andthe numericallysimulatedresultscanagreewiththeexperimentalones.
		       
		        
		        
			  
			TodevelopanignitionandgrowthreactionflowmodelforHNS-Ⅳexplosive,cylindertests wereconductedonHNS-ⅣexplosiveandtheexpansionprocessesofthecoppercylinderwallswererecordedbyaGSJhighspeedrotatingmirrorcamera, andparticlevelocitiesattheinterfacebetween HNS-ⅣexplosiveandLiFwindowweremeasuredwithlaservelocityinterferometry(VISAR).The correspondingnumericalsimulationswerecarriedoutbyANSYS/LS-DYNA,respectively.TheJWL equation-of-stateparametersforunreactedexplosivewerefittedtotheavailableshockHugoniotdata. Andbycombiningtheexperimentalresultsandnumericalsimulations,theJWLequation-of-stateparametersfordetonationproductweredetermined, aswellasreactiverateparametersforreactionignitionandgrowthin HNS-Ⅳ explosive.Investigatedresultsshowthatthedevelopedignitionand growthreactionflow modelcanbeusedtopicturethereactionprocessofHNS-Ⅳexplosive,andthe numericallysimulatedresultscanagreewiththeexperimentalones.
		            2012, 32(3): 333-336. 
	            	doi: 10.11883/1001-1455(2012)03-0333-04 
   					
					
		        
					Abstract: 
Drop-hammerloadexperimentswereperformedondifferentrocksamples.Bychangingthe drophammerweight,dropheightandpistonrodspacermaterial,transientshockpressurepulsesin therocksampleswererecordedbythepressuregauges.Experimentalresultsindicatethatthepropertiesoftherocksundergothefollowingchangesinducedbydilatancy:( 1)thepermeabilityoftherocks increasesinvaryingdegrees,andthedensertherockis,thegreatertheincreasemultipleofthepermeabilityis;( 2)theelasticmodulusandelasticlimitdecreasewiththeincreaseofrockvolume;(3) thepropagationvelocitiesoflongitudinalandtransversewavesdecreaseintherocks;(4)theporosities intherocksincreaseduetotheextensionofthenew-producedorinherentmicro-cracksintherocks.
		       
		        
		        
			  
			Drop-hammerloadexperimentswereperformedondifferentrocksamples.Bychangingthe drophammerweight,dropheightandpistonrodspacermaterial,transientshockpressurepulsesin therocksampleswererecordedbythepressuregauges.Experimentalresultsindicatethatthepropertiesoftherocksundergothefollowingchangesinducedbydilatancy:( 1)thepermeabilityoftherocks increasesinvaryingdegrees,andthedensertherockis,thegreatertheincreasemultipleofthepermeabilityis;( 2)theelasticmodulusandelasticlimitdecreasewiththeincreaseofrockvolume;(3) thepropagationvelocitiesoflongitudinalandtransversewavesdecreaseintherocks;(4)theporosities intherocksincreaseduetotheextensionofthenew-producedorinherentmicro-cracksintherocks.

    						
	   			
PDF 
Cited by