Microstructure-Properties: II Lecture 12: Martensitic Transformations
advertisement
1 Objective Basics Microstructure-Properties: II Martensitic Transformations T0 concept Microstructures Bain model Carbon in Fe SME 27-302 Lecture 6 Fall, 2002 Prof. A. D. Rollett 2 Materials Tetrahedron Processing Performance Objective Basics T0 concept Microstructures Bain model Carbon in Fe SME Microstructure Properties 3 Objective • The objective of this lecture is to explain the basic features of martensitic transformations. • Martensitic transformations are the most important type of military transformations, i.e. transformations that do not require Objective diffusion for the change in crystal structure to occur. Basics • Why study martensitic transformations?! They occur in many T0 concept different metal, ceramic & polymer systems, and are generally important to understand. Steels represent the classical Microexample (and a rate case of a mechanically hard martensite). structures Also, there are remarkable devices that exploit the shape Bain memory effect (a consequence of martensitic transformation) model such as stents that open up once at body temperature. The Carbon martensites in this case are generally soft, mechanically in Fe speaking. SME 4 References Objective Basics T0 concept Microstructures Bain model Carbon in Fe SME • Phase transformations in metals and alloys, D.A. Porter, & K.E. Easterling, Chapman & Hall. Porter & Easterling concentrate on the geometrical and crystallographic characteristics of Fe-based martensites. • Materials Principles & Practice, Butterworth Heinemann, Edited by C. Newey & G. Weaver. • Otsuka, K. and C. M. Wayman (1998). Shape Memory Materials. Cambridge, England, Cambridge University Press. This book provides a very thorough description of the scientific and technological basis for the shape memory effect. 5 Notation Objective Basics T0 concept Microstructures Bain model Carbon in Fe SME T0 := Eq. Temp. for 2 phases at same composition ∆T := undercooling ∆S := entropy of transformation ∆H := enthalpy of transformation ∆G := Gibbs free energy e := transformation strain g := Interface energy 6 Military Transformations Objective Basics T0 concept Microstructures Bain model Carbon in Fe SME • What is a martensitic transformation? • Most phase transformations studied in this course have been diffusional transformations where long range diffusion is required for the (nucleation and) growth of the new phase(s). • There is a whole other class of military transformations which are diffusionless transformations in which the atoms move only short distances in order to join the new phase (on the order of the interatomic spacing). • These transformations are also subject to the constraints of nucleation and growth. They are (almost invariably) associated with allotropic transformations. 7 Massive vs. Martensitic Transformations • There are two basic types of diffusionless transformations. • One is the massive transformation. In this type, a diffusionless transformation takes place without a definite orientation relationship. The interphase boundary (between parent and Objective product phases) migrates so as to allow the new phase to Basics grow. It is, however, a civilian transformation because the T0 concept atoms move individually. Micro• The other is the martensitic transformation. In this type, the structures change in phase involves a definite orientation relationship Bain because the atoms have to move in a coordinated manner. model There is always a change in shape which means that there is a strain associated with the transformation. The strain is a Carbon in Fe general one, meaning that all six (independent) coefficients can be different. SME 8 Classification of Transformations Civilian Military Precipitation, Spinodal Decomposition ? Massive Martensitic Transformations Transformations Objective Basics T0 concept Microstructures Diffusion Required Bain model Carbon in Fe SME Diffusionless 9 Driving Forces Objective Basics T0 concept Microstructures Bain model Carbon in Fe SME • These transformations require larger driving forces than for diffusional transformations. • Why? In order for a transformation to occur without long range diffusion, it must take place without a change in composition. • This leads to the so-called T0 concept, which is the temperature at which the new phase can appear with a net decrease in free energy at the same composition as the parent (matrix) phase. • As the following diagram demonstrates, the temperature, T0, at which segregation-less transformation becomes possible (i.e. a decrease in free energy would occur), is always less than the solvus (liquidus) temperature. 10 Free Energy - Composition: T0 a, product T1 ∆Gga g, Objective parent Basics T0 concept Microstructures Bain model Carbon in Fe SME G ∆Gga Common tangent T2 Diffusionless transformation impossible at T1, Diffusionless transformation possible at T2; “T0” is defined by no difference in free energy between the phases, ∆G=0. T1>T2 T2 corresponds to figure 6.3b in P&E. X 11 Driving Force Estimation Objective Basics T0 concept Microstructures Bain model Carbon in Fe SME • The driving force for a martensitic transformation can be estimated in exactly the same way as for other transformations such as solidification. • Provided that an enthalpy (latent heat of transformation) is known for the transformation, the driving force can be estimated as proportional to the latent heat and the undercooling below T0. ∆Gga = ∆Hga ∆T/T0. • Thus P&E estimate the driving force at the temperature at which martensite formation starts in Eq. 6.1 using this relationship. Phase relationships 12 equilibrium Objective Basics T0 concept Microstructures Bain model Carbon in Fe SME T near T0 Note that the Ms line is horizontal in the TTT diagram; also, the Mf line. diffusionless 13 Heterogeneous Nucleation Objective Basics T0 concept Microstructures Bain model Carbon in Fe SME • Why does martensite not form until well below the T0 temperature? The reason is that a finite driving force is required to supply the energy needed for (a) the interfacial energy of the nucleus and (b) the elastic energy associated with the transformation strain. The former is a small quantity (estimated at 0.02 J.m-2) but the elastic strain is large (estimated at 0.2 in the Fe-C system), see section 6.3.1 for details. Therefore the following (standard) equation applies. ∆G* = 16πg3 / 3(∆GV - ∆GS)2 • Why does martensite require heterogeneous nucleation? The reason is the large critical free energy for nucleation outlined above. 14 Microstructure of Martensite Objective Basics T0 concept Microstructures Bain model Carbon in Fe SME • The microstructural characteristics of martensite are: - the product (martensite) phase has a well defined crystallographic relationship with the parent (matrix). - martensite forms as platelets within grains. - each platelet is accompanied by a shape change - the shape change appears to be a simple shear parallel to a habit plane (the common, coherent plane between the phases) and a uniaxial expansion (dilatation) normal to the habit plane. The habit plane in plain-carbon steels is close to (225), for example (see P&E fig. 6.11). - successive sets of platelets form, each generation forming between pairs of the previous set. - the transformation rarely goes to completion. 15 Microstructures Objective Basics T0 concept Microstructures Bain model Carbon in Fe SME Martensite formation rarely goes to completion because of the strain associated with the product that leads to back stresses in the parent phase. 16 Self-accommodation by variants Objective Basics T0 concept Microstructures Bain model Carbon in Fe SME • A typical feature of martensitic transformations is that each colony of martensite laths/plates consists of a stack in which different variants alternate. This allows large shears to be accommodated with minimal macroscopic shear. 17 Mechanisms Objective Basics T0 concept Microstructures Bain model Carbon in Fe SME • The mechanisms of military transformations are not entirely clear. The small length scales mean that the reactions propagate at high rates - close to the speed of sound. The high rates are possible because of the absence of long range atomic movement (via diffusion). • Possible mechanisms for martensitic transformations include (a) dislocation based (b) shear based • Martensitic transformations strongly constrained by crystallography of the parent and product phases. • This is analogous to slip (dislocation glide) and twinning, especially the latter. 18 Atomic model - the Bain Model Objective Basics T0 concept Microstructures Bain model Carbon in Fe SME • For the case of fcc Fe transforming to bct ferrite (Fe-C martensite), there is a basic model known as the Bain model. • The essential point of the Bain model is that it accounts for the structural transformation with a minimum of atomic motion. • Start with two fcc unit cells: contract by 20% in the z direction, and expand by 12% along the x and y directions. 19 Bain model Objective Basics T0 concept Microstructures Bain model Carbon in Fe SME • Orientation relationships in the Bain model are: (111)g <=> (011)a’ [101]g <=> [111]a’ [110]g <=> [100]a’ [112]g <=> [011]a’ 20 Crystallography, contd. Objective Basics T0 concept Microstructures Bain model Carbon in Fe SME • Although the Bain model explains several basic aspects of martensite formation, additional features must be added for complete explanations (not discussed here). • The missing component of the transformation strain is an additional shear that changes the character of the strain so that an invariant plane exists. This is explained in fig. 6.8. 21 Role of Dislocations Objective Basics T0 concept Microstructures Bain model Carbon in Fe SME • Dislocations play an important, albeit hard to define role in martensitic transformations. • Dislocations in the parent phase (austenite) clearly provide sites for heterogeneous nucleation. • Dislocation mechanisms are thought to be important for propagation/growth of martensite platelets or laths. Unfortunately, the transformation strain (and invariant plane) does not correspond to simple lattice dislocations in the fcc phase. Instead, more complex models of interfacial dislocations are required. 22 Why tetragonal Fe-C martensite? • At this point, it is worth stopping to ask why a tetragonal martensite forms in iron. The answer has to do with the preferred site for carbon as an interstitial impurity in bcc Fe. • Remember: Fe-C martensites are unusual for being so strong Objective (& brittle). Most martensites are not significantly stronger than Basics their parent phases. T0 concept • Interstitial sites: fcc: octahedral sites radius= 0.052 nm Microtetrahedral sites radius= 0.028 nm structures bcc: octahedral sites radius= 0.019 nm Bain tetrahedral sites radius= 0.036 nm model • Carbon atom radius = 0.08 nm. Carbon • Surprisingly, it occupies the octahedral site in the bcc Fe in Fe structure, despite the smaller size of this site (compared to the tetrahedral sites) presumably because of the low modulus in SME the <100> directions. 23 Interstitial sites for C in Fe Objective Basics T0 concept Microstructures Bain model Carbon in Fe fcc: carbon occupies the octahedral sites bcc: carbon occupies the octahedral sites SME [Leslie] 24 Carbon in ferrite • One consequence of the occupation of the octahedral site in ferrite is that the carbon atom has only two nearest neighbors. Objective • Each carbon atom therefore distorts the iron lattice in its vicinity. Basics • The distortion is a tetragonal T0 concept distortion. Micro• If all the carbon atoms occupy the structures same type of site then the entire lattice becomes tetragonal, as in the Bain martensitic structure. model • Switching of the carbon atom Carbon between adjacent sites leads to in Fe strong internal friction peaks at SME characteristic temperatures and frequencies. [P&E] 25 Shape Memory Effect (SME) Objective Basics T0 concept Microstructures Bain model Carbon in Fe SME • General phenomenon associated with martensitic transformations. • Characteristic feature = strain induced martensite (SIM), capable of thermal reversion. • Ferroelasticity and Superelasticity also possible. • Md,Af,As,Ad,Ms,Mf temperatures. [Shape Memory Materials] 26 Temperatures Ms Objective Af T0 Basics T0 concept Ad As Microstructures Bain model Md Mf Carbon in Fe SME The Md and Ad temperatures bracket T0 because they define the oncooling and on-heating temperatures at which the transformation is possible with allowance for the effect of strain energy. 27 SME Definitions Objective Basics T0 concept Microstructures Bain model Carbon in Fe SME • Md: SIM possible below Md. • Af: reversion of SIM complete above Af (heating). • As: reversion of SIM starts above As (heating). • Ad: formation of parent phase possible above Ad. • Ms: martensite start temperature (cooling). • Mf: martensite finish temperature (cooling). 28 SME, contd. • Classic alloy = Nitinol = NiTi – alloying for control of Ms. Objective Basics T0 concept Microstructures Bain model Carbon in Fe SME • Stress for SIM must be less than yield stress for plastic deformation. • SME depends on incomplete transformation and elastic back stresses to provide memory (>MS). – SME more effective in single xtals. • Alloying permits variations in the equilibrium transformation temperature, for example (critical for bio applications, for example). Also variations in the maximum strain that can be recovered are possible. 29 Super-elasticity Objective Basics • Super-elasticity is simply reversible (therefore “elastic”) deformation over very large strain ranges (many %). • Example: Ti-50.2%Ni. T0 concept Microstructures Bain model Carbon in Fe SME [Shape Memory Materials] 30 Role of Ordering Objective Basics T0 concept Microstructures Bain model Carbon in Fe SME • A key feature of the Ni-Ti alloys for shape memory applications is that their compositions are all in the vicinity of 50Ni-50Ti and that the high temperature phase is an ordered B2 structure. The low temperature B19’ monoclinic structure is therefore also ordered (as is the other, intermediate R phase which is trigonal). • The ordered structure (recall the discussion of ordered particle strengthening) means that there is an appreciable resistance to dislocation motion. This is critical for favoring strain accommodation via transformation and twinning as opposed to dislocation glide. 31 Self-accommodation Objective Basics T0 concept Microstructures Bain model Carbon in Fe SME • Micrograph with diagram shows how different variants of a given martensitic phase form so as to minimize macroscopic shear strains in a given region. 32 Shape Memory Effect • Demonstration of shape memory effect Objective (SME) in a spring Basics • Mechanism of SME: 1) transformation; T0 concept 2) martensite, selfMicroaccommodated; structures 3) deformation by Bain variant growth; model 4) heating causes Carbon re-growth of parent in Fe phase in original SME orientation 33 Surface Relief Objective Basics T0 concept Microstructures Bain model Carbon in Fe SME Micrographs show a sequence of temperatures with surface relief from the martensite plates. 34 Stress versus Temperature • The stress applied to the material must be less than the critical resolved shear stress for dislocation motion, because the latter is not recoverable; SME= Shape Memory Effect; SE = Superelasticity Objective Basics d/dT = ∆S/e = ∆H/(Tee T0 concept Microstructures Bain model Mf Stress SME Critical Stress for Martensite Formation As SE Carbon in Fe SME Ms Af Temperature Critical Stress for Slip 35 Ni-Ti Alloys [Wasilewski, SME in Alloys, p245] X Ms Mf As Af V > 25 < -140 < -64 > 25 Cr -100 < -180 < -58 > 25 Mn -116 < -180 < -63 > 10 Fe No information < -180 -30 > 25 Bain model Co No information No information 0 > 25 Carbon in Fe Cu > 25 < -100 ? > 25 TiNi0.95 70 60 108 113 TiNi 60 52 71 77 Ti0.95Ni -50 < -180 ? 20 (?) Objective Basics T0 concept Microstructures SME 36 SME Requirements Objective Basics T0 concept Microstructures Bain model Carbon in Fe SME • For achieving a strong or technologically useful SME, the following characteristics are required. • High resistance to dislocation slip (to avoid irreversible deformation). • Easy twin motion in the martensitic state so that variants can exchange volume at low stresses. • Crystallographically reversible transformation from product phase back to parent phase. Ordered structures have this property (whereas for a disordered parent phase, e.g. most Fe-alloys, multiple routes back to the parent structure exist.) 37 Photostimulated SME! Objective Basics T0 concept Microstructures Bain model Carbon in Fe SME 38 Summary Objective Basics T0 concept Microstructures Bain model Carbon in Fe SME • Martensitic transformations are characterized by a diffusionless change in crystal structure. • The lack of change in composition means that larger driving forces and undercoolings are required in order for this type of transformation to occur. • The temperature below which a diffusionless transformation is possible is known as “T0”. • Martensitic transformations invariably result in significant strains with well defined (if irrational, in terms of Miller indices) crystallography. • Technological applications abound - quenched and tempered steels, Nitinol shape memory alloys etc.
