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NASA Technical Reports Server (NTRS) 20010064392: Creep-Fatigue Interaction Testing PDF

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Creep-fatigue Interaction Testing Fatigue livesinmetals arenominally time independent below 0.5 To.,,. A: higher temperatures, fatigue lives arealtered dueto rime-dependent, thermally activated creep. Conversely, creep rates arealtered by super. imposed fatigue loading. Creep and fatigue generally interact synergistically to reduce material lifetime. Their interaction, therefore, L_of £mpbrtanc_) to structural durability of high-temperature structures such asnuclear reactors, reusable rocket engines, gas turbine engines, terrestrial steam turbines, pressure vessel and piping components, castingdies, molds for plastics, and pollution control devices. Safety and life- cycle costs force designers to quantify these inter- actions. Analytical and experimental approaches to creep-fatigue began intheera following World War1I. In this article experimental and life prediction approaches ate reviewed for assessing creep-fatigue interactions of metallic materials. Mechanistic models are also discussed briefly. 1. I'estFacilities sx0015 Modern creep-fatigue testing facilities are sophisti- cated closed-loospe,rvo-con_olled, electro-hydraulic fatiguteestinmgachines('I-Ialfeotarld._ adapted to high-temperature operation (Fig.---l_. Typical machinesconsisotftwoorfourposts,arigidloading frame, andahydraulic cylinder mounted in the center ofthebase.Thecylindetrransmiths_'draulicpressure from a pump throughan electromcscrvovalveA. specimengripismounted on theupperend ofthe cylinderram,andanotherisattachedtoa loadcell mounted to the uppercross member to measure axial loadtransmittetdhroughthespecimenM.odern grips utilizheydraulictsoalignandsecurethespecimen. Alignmentof thespecimenand loadingaxesis importantto minimizebendingloadsand avoid bucklingS.pecimenshaveauniformlyreducedcross- sectionthatisasuniformlyheatedaspossiblaend experiencesthecyclicstresseasnd strainsC.yclic strains aremeasured and controlled withcommercially availableextensometers withresolutioonnsthe order of I0microstrain, A specimenheatingsystemisthecoreofhigh- sx0020 temperature testing.Test machine components such as the extensometer sensing element, specimen grips, load cell, and all hydraulic components must bekept cool.Themostversatile heating systemusesinduction coilssurroundingthespecimen.High-frequenccyur. rentpassingthroughthecoilisnduceseddycurrentast the surfacoef the specimen. Specimen heating results. The highthermalconductivity ofmost alloys results in a specimen with minimal thermal gradients in the radial direction. Coil spacing controls axial thermal gradientTsh.reeindependentlcyontrollecdoilcsanbe This report is apreprint of an article submitted to ajournal for publication. Because of changes that may be made before formal publication, this preprint is made available with the understanding that it will not be cited or reproduced without the permission of the author. / C:/jan/emr409037 Apr04-pro p lc- lm 3 _ 2) i i C I i/ Error Specimen_ Gain I f I [ .. ve ,o.v, I [ ,( Servovalve |$ Figure 1 Modern creep-fatiguetesting machine. employed to minimize the axial thermal gradient. Coil spacing will allow visual observation of the specimen and permits attachment of an extensonjgter sporting ceramic extension rods that transmiq_gage section displane.mmz_ to the more distant sensini[ element. A thermocouple held in direct contact with the specimen surface supplies feedback for temperature control. Commercial noncontacfing optical pyrometers are also available. Alternate heating techniques, such as a sxO025 combination of induction and radiation, are required for low conductivity materials such as ceramics. A small metallic susceptor surrounds the specimen and is heated by induction. The susceptor then radiates heat to the specimen. The low thermal mass of this system permits reasonably fast temperature changes. Radi- ation furnacesare quite common. They use coiled Nichrome wire or siliconcarbideelementsor even banks ofquartzlamps.Furnaces offerhighthermal stability because of the large thermal mass, but are slow to respond to intentional temperature changes during thermomechanical testing. Direct resistance heating also has been used successfully, but remains uncommon. High current (low voltage) passed / C:/jan/emr409037 Apr04-pro p Ic-lm 4 (X 31 "_'.roughthe specimen results inseE-heating due tothe specimen's electrical resistivity. This technique is the =ost di_cult toconuolt_causeoftbe _l"enfly high £_e:mal response. Heating of the test section does not reiy on the thermal conductivity of the specimen; cooling, however, does. Maintaining an accurate constanttemperaturiesdilr_-ult. Moderntestfacilities arctypicalilnyappropriatfoer _0030 long-term(_ 1month)testingL.essexpensivem,ore reliabl¢, screw-driven machines aresul:_rioforr purpose. If long-termcreep-fatigue resistanciesa designrequirementl,ong-tertmestresultasrenecess- ary to verifylifepredictiomnodels foraccurate extrapolation. 2. MeehanDma and Life Prediction Modela sx0035 Fatigue crackinitiation and earlygrowth mechanisms differ substantially from those for creep cracking. Fatigue damage is time-lndependent to-and-fro crys- tallographic slip, most evident atfree surfaces. Creep damage occurs throughout the volume of stressed material and requires the thermally activated diffusion of atomic vacancies. Creep damage due to grain boundary sliding, however, intersects free surfaces in much thesameway as fatiguselip. Theadditioonfcreeptoanotherwispeuretension/sx0040 compressionfatiguecyclecan be accomplishedin threedistinctdliyfferenwtays asshown below.A baselinceonditionofpurefatiguecyclingwillhave negligiblcereeppresentifa highenough cyclic frequency(_>IHz)isimposed. - Constantstraininrgatelowenoughtointroduce creepinadditiotnocrystallograpshliicp. -Constantstresasscreepoccurswithtime. - Constanttotalstrainwhilestressrelaxesc,on- vertingelastitcocreepstrain(lefptanelsofFig.2). Sinceanyoneofthesethreewaysofintroducingsx0045 creepintoacyclecouldbeappliedtotensiononly, compressiononly,orbothtenslonandcompression, thereemerge,intheextreme,onlyfourbasiccom- binationosfcompletelryeversecdreep-fatigsuteress- straicnycles: -Tensileplastisctrai(np)reversebdycompressive plastisctrai(np),i.e.(,pp) -Tensileplastisctrai(np)reversebdycompressive creepstrai(nc)i,.e.(,pc) - Tensilecreepstrai(ne)reversedbycompressive creepstrai(nc)i,.e.(,cp) -Tensilecreepstrai(nc)reversedby compressive plastisctrai(np),i.e.(,cc) The rightpanelsofFig.2 illustrattyepicasltress-sx0050 strainhysteresilsoopsforstrainholdtypecycles. Invariablcyreep-fatigcuyeclesinvolve(p.vs)training inadditionto(cp),(pc),or (cc)components.Such cyclesdemand useofservo-controllseydstemswith extensometerasnd state-of-the-faurntctiongener- / C:/jan/emr409037 Apr04-pro p It- lm 5(X 4) ,',Slnm c,$1_u ,, .' _.,\ / ", / ', , _ ,:%/ :Y___.a' /'qtarc2 Creep.fatigue testcycles. ators. The cycles are simplifications of actual complex service cycles. Experimental replication of service histories would requirecomplex programming achiev- able through a computer-controlled servo system. Usually, life prediction models are reliedupon to link single lah_,to_ ¢_e.s _th mlggi¢ se_,d¢.¢t'_,_.s. The deformation, crack initiation, and earlygrowth sx0055 mechanisms, in general, will be different for each of these discrete cycles. Schematic models developed to illustrate these differences have been compared to experimental observations for a variety of alloys (Manson and Halford [I]_. Of the more than 100 creep-fatigue lifepredicuon models proposed since the 1950s,onlyabout10% havebeenapplieedxtensively enoughtowarranttheirreview(Mille[r_ Halford 84 B2 et al._. The three most widely used-aTffthe time- 81 and cyc--'ffd-fractionrule (ASME _), strai_ange partitioning (SLIP), and damage--_-echanics. Few specitically address inevitable oxidation interactions. The ASME Code Case is extremeIy conservative and doesnotdirectlayddresswhenhilurewouldoccur. Thatconditionisacceptablbeecausepowerplantsdo nothavethesamestringenwteightandperformance requirementass,forexample,aerospacepropulsion ..-_:.?.:_;.;_.:,.. , -" 7, . v I C:[_an/emr409037 Apr04-pro p lc- lm 6 (X 5) systems. The Inner require mtr.h g_mm:r life .1_ accuracy to conserve weight while m2,_._, z a combination of durability and performance. 3. Co_ Re_ks Ix0060 Creep-fa6gue interactionisreasonablywelluader- stood at thephenomeuological level.A sisni_:ant short-termexperimentaldatabaseexistsand several satisfactory analytic models are in use for estir_fing cyclic lives. Modeling of oxldatioo interactlom with creep-fatigue, lack oflong-term databases, and verified long-term extrapolation procedures remain as im- portant areas of research. See also: Creep-Fatigue: Oxidation Interactions Creep-Fatigue: Oxidation Interactions Biblioftaph¥ _'_ricaa SocietoyfMechaaical Engineers1986CodeCase/¢- 47-2$.ASME, NewYork l:I'_ord GR, Lerch BA, McC_w MA 2000 Fatigue, ¢_-eep- fatigue,andthermomechanicalfatiguelifetestingofalloys In: (ed.}ASM Han_ook. Vol.8,MechanlcalTeJgln$and Evaluation. ASMInternational, MaterialsPark, OH,Sect. 8B a_l'_'nson SS, Halford GR 1984 Relation of cyclic loading pattern to mlcrostmctural fracture in creep-fatigue In: CJ Beevets (ed.) Proc. 2nd Int. Conf. Fatlfw and FaHfue ' Threzho!d_(Fatigue84). EngineeringMaterials AdvServLtd, !QA: What is_,dv Serv! short for? Wartey,UK, Vol. 3,pp.1237-55 l_[il]'erDA,PriestRH,EUisonEG 1984Areview of material response and lifeprediction techniques under fatigue-creep loadingconditions. HighTemp.Mater. Process. 6,155-94 G. R. Halford

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