METALLURGICAL AND MATERIALS TRANSACTIONS A
ABSTRACTS
Volume 27A, No. 1, January 1996

This Month Featuring: Alloy Phases; Transformations; Transport Phenomena; Mechanical Behavior; Surface Treatment; Solidification; Materials Processing; Composite Materials. View January 1996 Table of Contents.

ALLOY PHASES

Evolution of Microstructures in the Nickel Modified Titanium Trialuminides Near the Ll2 Phase Field
S. BISWAS and R.A. VARIN
This study focuses upon the evolution of microstructures during solidification processing of several intermetallic alloys around the Ll2 phase in the Al-rich corner of the Al-Ti-Ni ternary system. The alloys were produced by double induction melting and subsequent homogenization followed by furnace cooling. The microstructure was characterized by means of optical and scanning electron microscopy with energy-dispersive spectroscopy (EDS) analysis and X-ray diffraction. The microstructural evolution in homogenized alloys was dependent on both nickel and titanium content. Very fine precipitates of Al2Ti were observed within the Ll2 phase in alloys containing 62 to 65 at. pct Al and at least 25 at. pct Ti. The Al2Ti precipitates are stable at least up to 1000 °C and undergo complete dissolution at 1200 °C. In alloys containing around 66 at. pct Al and 25 to 31 at. pct Ti, phases such as Al3Ti, Al5Ti2, and Al11Ti5 were observed. A modified room temperature isotherm in the Al-Ti-Ni ternary system is proposed, taking into account the existence of Al2Ti, Al11Ti5, Al5Ti2, and Al3Ti in equilibrium with the Ll2 phase. It seems that at room temperature, the Ll2 phase field for homogenized alloys is extremely small. It will be practically impossible to obtain a single-phase microstructure at room temperature in the Al-Ti-Ni ternary alloys after homogenization at 1000 °C followed by furnace cooling.

The Effect of Iron and Manganese on the Recrystallization Behavior of Hot-Rolled and Solution-Heat-Treated Aluminum Alloy 6013
RICHARD A. JENISKI, JR., BUNCHA THANABOONSOMBUT, and T.H. SANDERS, JR.
The influence of manganese and iron additions on the recrystallization behavior of a hot-rolled Al-Mg-Si-Cu alloy has been investigated. In the as-cast ingot, some manganese remains in supersaturated solid solution and, during the preheating step, precipitates as fine (0.1 to 0.3 µm) dispersoids Al12Mn3Si and (AlFeMnSi), depending on the local iron content. The presence of the dispersoids increases the alloy's resistance to recrystallization. The remaining manganese along with iron forms coarse (30 to 100 µm) (AlFeMnSi) phases in the interdendritic channels upon solidification. During rolling, these coarse phases are broken up and the matrix surrounding the phases is highly strained. The highly strained regions around the precipitates are preferential sites for the nucleation and growth of new, strain-free, recrystallized grains. Decreasing the iron content decreases the amount of coarse (AlFeMnSi) constituent phase and increases the recrystallization resistance of the alloy for a given concentration of manganese. For iron-free alloys, coarse -Al12Mn3Si phase forms during solidification. The increased recrystallization resistance is attributed to the lower probability for particle-stimulated recrystallization. Increasing the manganese content beyond what is normally found in 6013 increases the volume fraction of both the dispersoids and the coarse constituent phases. However, the increased volume fraction of the dispersoids in the iron-containing alloys more than compensates for the increase in volume fraction of coarse constituent particles, resulting in an increase in the recrystallization resistance with increased manganese content. In this research, alloys containing varying amounts of manganese and iron with levels of magnesium, silicon, and copper consistent with the nominal composition of 6013 were hot deformed and solution heat treated to produce microstructures ranging from fully recrystallized to unrecrystallized.

TRANSFORMATIONS

Hydride Formation and Decomposition in Electrolytically Charged Metastable Austenitic Stainless Steels
SHUCHUN CHEN, MING GAO, and ROBERT P. WEI
An investigation of phase transformations in hydrogen-charged metastable austenitic stainless steels was carried out. Solution-annealed, high-purity, ultralow-carbon Fe18Cr12Ni (305) and laboratory-heat Fe18Cr9Ni (304) stainless steels were examined. The steels were cathodically charged with hydrogen at 1, 10, and 100 mA/cm2, at room temperature for 5 minutes to 32 hours, in an 1N H2SO4 solution with 0.25 g/L of NaAsO2 added as a hydrogen recombination poison. Changes in microstructure and hydrogen damage that resulted from charging and subsequent room-temperature aging were studied by X-ray diffraction (XRD) and transmission electron microscopy (TEM). Hydrides from hydrogen charging (hcp * in 305 SS and fcc * and hcp * in 304 SS) were observed. The evidence suggests the following mechanisms for hydride formation during charging: (1) * hydride and (2) * hydride. These hydrides were found to be unstable and decomposed during room-temperature aging in air by the following suggested mechanisms: (1) * hydride (hcp) expanded (hcp) phase ' (bcc) phase and (2) * hydride phase. The transformation from * to ', however, was incomplete, and a substantial fraction of was retained. A kinetics model for hydride decomposition and the accompanying phase transformation during aging is proposed.

Mechanical Alloying of Nb-Al Powders
ZHIXUE PENG, C. SURYANARAYANA, and F.H. (SAM) FROES
The effect of mechanical alloying (MA) on solid solubility extension, nanostructure formation, amorphization, intermetallic compound formation, and the occurrence of a face-centered cubic (fcc) phase in the Nb-Al system has been studied. Solid solubility extension was observed in both the terminal compositions and intermetallic compounds: 15 pct Nb in Al and 60 pct Al in Nb, well beyond the equilibrium and even rapid solidification levels (2.4 pct Nb and 25 pct Al, respectively) and increased homogeneity range for the NbAl3 phase. Nanostructured grains formed in all compositions. In the central part of the phase diagram, amorphization occurred predominantly. Only NbAl3, the most stable intermetallic, formed during MA; in most cases, a subsequent anneal was required. On long milling time, an fcc phase, probably a nitride, formed as a result of contamination from the ambient atmosphere.

Experimental Investigation of the Transformation Texture in Hot-Rolled Ferritic Stainless Steel Using Single Orientation Determination
D. RAABE and M. YLITALO
Two ferritic stainless steels (16.5 mass pct Cr) were hot-rolled using seven subsequent passes. The first sample was rolled within the range 1280 °C to 750 °C, i.e., the deformation started in the ferritic region. The second sample was rolled within the range 1080 °C to 770 °C, i.e., the deformation started in the ferritic-austenitic region. In both cases, up to 40 vol pct of the ferrite transformed into austenite during hot rolling. During the last passes, the austenite transformed into cubic martensite. After hot rolling, these former austenitic regions were identified using a selective etching technique and examined using single orientation determination in the scanning electron microscope. The regions which remained ferritic throughout the hot-rolling process were investigated as well. Whereas the texture of the martensite considerably depended on the hot-rolling conditions, especially on the temperature and on the intervals between the rollings, the texture of the ferrite was less affected. The textures of the martensite were interpreted in terms of the crystallographic transformation rules between austenite and martensite. The textures of the ferrite were discussed in terms of recovery and recrystallization.

TRANSPORT PHENOMENA

High-Temperature Nitridation of Ni-Cr Alloys
A.A. KODENTSOV, J.H. GULPEN, C. CSERHATI, J.K. KIVILAHTI, and F.J.J. VAN LOO
The nitriding behavior of nickel-chromium alloys was investigated at 1398 K over the range 1 to 6000 bar of external nitrogen pressure. The morphology of the nitrided zone depends on the concentration of chromium in the initial alloy and the N2 pressure (fugacity) applied upon the system. The transition from CrN to Cr2N precipitation was observed within the reaction zone after nitriding at 100 to 6000 bar of N2 when the chromium content in the initial alloys was 28.0 at. pct or higher. It is shown that the ternary phase ¼ (Cr10Ni7N3) is formed in this system at 1273 K through a peritectoid reaction between Cr2N and nickel solid solution and becomes unstable above 1373 K. The thermodynamic evaluation of the Ni-Cr-N system was performed and phase equilibria calculated. Evidence for "up hill" diffusion of nitrogen near the reaction front during the internal nitridation of Ni-Cr alloys at 1398 K was found. It was attributed to the relative instability of chromium nitrides and strong Cr-N interaction in the matrix of the Ni-based solid solution within the nitrided zone.

MECHANICAL BEHAVIOR

Mechanical Behavior of the In Situ Composite Alloys in the Al-Ni-Ti System Near the L12 Phase Field
S. BISWAS and R.A. VARIN
The Vickers microhardness (VHN) test at room temperature and compressive tests at temperatures up to 1000 °C were carried out on the three-phase composite alloy, consisting of the L12, face-centered cubic (fcc) Al2TiNi, and Al2Ti intermetallic phases, in the Al-Ti-Ni system. The microhardness tests indicated that the fcc Al2TiNi phase was very hard and brittle. Comparatively, the L12 phase was softer and more crack resistant. A considerable hardening was noticed due to the precipitation of Al2Ti within L12. In addition, the VHN of the L12 phase was found to increase with the combined content of nickel and titanium without the presence of any observable precipitates. Under compressive loading at room temperature, microcracks nucleated in the fcc Al2TiNi phase. These cracks propagated catastrophically at a stress barely approaching yield stress, resulting in nil ductility. This behavior was observed up to 800 °C. Between 900 °C and 950 °C, brittle-to-ductile transition in compressive behavior was observed for the three-phase alloy. Compressive ductility of the order of 80 pct was observed at 1000 °C. The mechanism of dynamic recrystallization was found to be operative at 1000 °C. Metallographic investigation revealed new recrystallized grains in the primary L12 matrix. However, the oscillatory nature of the true stress-true strain curve could not be explained with the help of the existing model of dynamic recrystallization.

Non-Schmid Effects on the Behavior of Polycrystals-m with Applications to Ni3Al
MING DAO, BING JEAN LEE, and ROBERT J. ASARO
The elastoviscoplastic single crystal constitutive model incorporating non-Schmid effects developed by Dao and Asaro (Mater. Sci. Eng. A, 1993, vol. 170, pp. 143-60) is introduced into Asaro and Needleman's (Acta Metall., 1985, vol. 33, pp. 923-53) Taylor-like polycrystal model as well as Harren and Asaro's (J. Mech. Phys. Solids, 1989, vol. 37, pp. 191-232) finite element polycrystal model. The single crystal non-Schmid effects, strain hardening, latent hardening, and rate sensitivity, are all described on the individual slip system level, while polycrystal mechanical properties on macroscale are predicted. In general, it is found that non-Schmid effects can have important influences on the "constant offset plastic strain yield surfaces," stress-strain behavior, texture development, and shear band formation. Finite element calculations show that with moderate non-Schmid effects, localized deformation within a polycrystal aggregate tends to initiate earlier and form sharper and more intense shear bands. Heavy shear banding is found to produce less pronounced textures, which is consistent with existing experimental evidence on Ni3Al. Examples with Ni3Al demonstrate that the kind of non-Schmid effects existing in Ni3Al can increase the generalized Taylor factor to values much higher than 3.06, raise the polycrystal strain hardening rate much higher than that which would be obtained using Schmid's rule, and influence the deformation texture.

The Effect of Hydrogen on the Fracture of Alloy X-750
DOUGLAS M. SYMONS and ANTHONY W. THOMPSON
The effect of hydrogen on the fracture of a nickel-base superalloy, alloy X-750, was investigated in the HTH condition. The effect of hydrogen was examined through tensile testing incorporating observations from scanning electron microscopy and light microscopy. The ductility at 25 °C, as measured by elongation to failure for tensile specimens, was reduced from 21 pct for noncharged specimens to 7.3 pct for 5.7 ppm hydrogen and to 3.5 pct for 65 ppm hydrogen. The elongation to failure was a function of the strain rate and test temperature. For hydrogen-charged specimens, the elongation decreased as the strain rate decreased at a constant temperature, while for a constant strain rate and varying temperature, there was a maximum in embrittlement near 25 °C and no embrittlement at -196 °C. For the noncharged specimens, the elongation monotonically increased as temperature increased, while there was no noticeable effect of strain rate. Prestraining prior to charging dramatically decreased elongation after hydrogen charging. When the strain rate was increased on the prestrained specimens, more plastic deformation was observed prior to failure. Failure did not occur until the flow stress was reached, supporting the proposition that plasticity is required for failure. The intergranular failure mechanism in alloy X-750 was a microvoid initiation process at grain boundary carbides followed by void growth and coalescence. The void initiation strain, as determined from tensile data and from sectioning unfractured specimens, was observed to be much lower in the hydrogen-charged specimens as compared to noncharged specimens. The reduced ductility may be explained by either a reduction of the interfacial strength of the carbide-matrix interface or a local hydrogen pressure at the carbide-matrix interface.

Pearlite in Ultrahigh Carbon Steels: Heat Treatments and Mechanical Properties
ERIC M. TALEFF, CHOL K. SYN, DONALD R. LESUER, and OLEG D. SHERBY
Two ultrahigh carbon steel (UHCS) alloys containing 1.5 and 1.8 wt pct carbon, respectively, were studied. These materials were processed into fully spheroidized microstructures and were then given heat treatments to form pearlite. The mechanical properties of the heat-treated materials were evaluated by tension tests at room temperature. Use of the hypereutectoid austenite-cementite to pearlite transformation enabled achievement of pearlitic microstructures with various interlamellar spacings. The yield strengths of the pearlitic steels are found to correlate with a predictive relation based on interlamellar spacing and pearlite colony size. Decreasing the pearlite interlamellar spacing increases the yield strength and the ultimate strength and decreases the tensile ductility. It is shown that solid solution alloying strongly influences the strength of pearlitic steels.

Optimization of Cold and Warm Workability in 304 Stainless Steel Using Instability Maps
S. VENUGOPAL, S.L. MANNAN, and Y.V.R.K. PRASAD
The deformation characteristics of stainless steel type AISI 304 under compression in the temperature range 20 °C to 600 °C and strain-rate range 0.001 to 100 s-1 have been studied with a view to characterizing the flow instabilities occurring in the microstructure. At strain rates less than 5 s-1, 304 stainless steel exhibits flow localization, whereas dynamic strain aging occurs at intermediate temperatures and below 0.5 s-1. At room temperatures and strain rates less than 10 s-1, martensite formation is observed. To avoid the preceding microstructural instabilities, cold and warm working should be carried out at strain rates greater than 5 s-1. The continuum criterion, developed on the basis of the principles of maximum rate of entropy production and separability of the dissipation function, predicts accurately all the preceding instability features.

Effect of Creep Strain on Microstructural Stability and Creep Resistance of a TiAl/Ti3Al Lamellar Alloy
J.A. WERT and M.F. BARTHOLOMEUSZ
Creep of a TiAl/Ti3Al alloy with a lamellar microstructure causes progressive spheroidization of the lamellar microstructure. Microstructural observations reveal that deformation-induced spheroidization (DIS) occurs by deformation and fragmentation of lamellae in localized shear zones at interpacket boundaries and within lamellar packets. Deformation-induced spheroidization substantially increases the interphase interfacial area per unit volume, demonstrating that DIS is not a coarsening process driven by reduction of interfacial energy per unit volume. Creep experiments reveal that DIS increases the minimum creep rate (min) during creep at constant stress and temperature; the activation energy (Qc) and stress exponent (n) for creep are both reduced as a result of DIS. Values of n and Qc for the lamellar microstructure are typical of a dislocation creep mechanism, while estimated values of n and Qc for the completely spheroidized microstructure are characteristic of a diffusional creep mechanism. The increase in min associated with DIS is thus attributed primarily to a change of creep mechanism resulting from microstructural refinement.

SURFACE TREATMENT

Surface Morphology and Compound Layer Pores of Plasma Nitrocarburized Low Carbon Steel
SHI LI and RAFAEL R. MANORY
This article deals with various aspects of nitrocarburizing of AISI 1010 steel by DC plasma at 600 °C. The initial stages of nitride formation and the effects of surface bombardment by hydrogen plasma species, as well as the effect of treatment current density on the surface morphology, were investigated in detail. The results show that in the pearlitic region carbides are removed during treatment in hydrogen plasma and that the current density influences the surface morphology significantly. A porous surface formed in a 1-minute treatment under high current density (8 mA/cm2), whereas a lower current density (2.4 mA/cm2) resulted in a highly stressed surface attributed to uneven thermal gradients. Iron nitrides were identified on the surface in either set of conditions. A pure epsilon compound layer was obtained by plasma nitrocarburizing for 6 hours and quenching. The pores in this layer are discussed in view of the 1-minute treatment results and are also compared to those observed in a nitriding treatment. The lack of carbon species in the nitriding plasma results in different mechanisms for pore formation and growth during the treatment. These results are discussed in view of current models for plasma nitriding and gas nitrocarburizing.

SOLIDIFICATION

Communication: Mechanical Deformation of Dendrites by Fluid Flow
J. PILLING and A. HELLAWELL

MATERIALS PROCESSING

The Effect of Thermal Cycle on the Microstructural Development of a Powder Metallurgy Superalloy Braze Material
R.G. IACOCCA
This investigation examines the effect of thermal cycle on the microstructural development in a powder metallurgy (P/M) superalloy braze material. Using a vertical quench furnace, samples were quenched at various stages within the heat treatment. Microstructures were analyzed using optical microscopy and an electron microprobe. The results show that borides having a blocky morphology are stable at all temperatures, both compositionally and morphologically. Script phase undergoes a drastic change in chemistry; however, it remains morphologically stable throughout. The chemical analysis of the microstructure supports the conclusion that the extended heat treatment, which is employed in industry to homogenize the microstructure and dissolve detrimental phases, does not have a significant effect in preventing these phases from forming. By using shorter times at elevated temperatures, similar microstructures can be produced.

Modeling Texture Change during the Static Recrystallization of Interstitial Free Steels
L. KESTENS and J.J. JONAS
A recrystallization model was developed based on the principal features of oriented nucleation and selective growth. The nucleation mechanism that is adopted assumes that nucleation takes place in deformed grains with relatively high Taylor factors. The selective growth law is based on the assumed high mobility of {110} plane matching (PM) boundaries and also includes a variant selection rule. The two submodels enable the full recrystallization process to be simulated. The theory is applied to the annealing of a Ti-Nb alloyed interstitial free (IF) steel. It is demonstrated that the nucleation and growth algorithms can successfully account for the annealing textures observed, including the presence of a strong {111}<211> component. An important feature of the model is that it permits the role of variant selection to be assessed; it also shows the effect on the texture of the low mobility of low-angle grain boundaries (LAGBs).

Communication: Modeling of Dynamic Material Behavior: A Critical Evaluation of the Dissipator Power Co-content Approach
F. MONTHEILLET, J.J. JONAS, and K.W. NEALE

Communication: Author's Reply
Y.V.R.K. PRASAD

COMPOSITE MATERIALS

Effective Elastic Moduli of Fiber-Matrix Interphases in High-Temperature Composites
Y.C. CHU and S.I. ROKHLIN
This article describes a theoretical model and an experimental method for determination of interphasial elastic moduli in high-temperature composites. The interphasial moduli are calculated from the ultrasonically measured composite moduli via inversion of multiphase micromechanical models. Explicit equations are obtained for determination of interphasial stiffnesses for an interphase model with spring boundary conditions and multiphase fiber. The results are compared with the exact multiphase representation. The method was applied to ceramic and intermetallic matrix composites reinforced with SiC SCS-6 fibers. In both composites, the fiber-matrix interphases include approximately 3-µm-thick carbon-rich coatings on the outer surface of the SiC shell. Although the same fiber is used in both composite systems, experimental results indicate that the effective interphasial moduli in these two composite systems are very different. The interphasial moduli in intermetallic matrix composites are much greater than those in ceramic matrix composites. After taking the interphase microstructure into account, we found that the interphasial moduli measured for the intermetallic matrix composites are very close to the estimated bulk moduli of the pyrolytic carbon with SiC particle inclusions. Our analysis shows that the lower effective interphasial moduli in the reaction-bonded Si3N4 (RBSN) ceramic matrix composites are due to imperfect contact between the interphasial carbon and the porous matrix and to thermal tension forces which slightly unclamp the interphase. Thus, measured interphase effective moduli give information on the quality of mechanical contact between fiber and matrix. Possible errors in the interphasial moduli determined are analyzed and the results show that these errors are below 10 pct. In addition, the use of the measured interphasial moduli for assessment of interphasial damage and interphase reactions is discussed.

NiTi and NiTi-TiC Composites: Part II. Compressive Mechanical Properties
K.L. FUKAMI-USHIRO, D. MARI, and D.C. DUNAND
The deformation behavior under uniaxial compression of NiTi containing 0, 10, and 20 vol pct TiC particulates is investigated both below and above the matrix martensitic transformation temperature: (1) at room temperature, where the martensitic matrix deforms plastically by slip and/or twinning; and (2) at elevated temperature, where plastic deformation of the austenitic matrix takes place by slip and/or formation of stress-induced martensite. The effect of TiC particles on the stress-strain curves of the composites depends upon which of these deformation mechanisms is dominant. First, in the low-strain elastic region, the mismatch between the stiff, elastic particles and the elastic-plastic matrix is relaxed in the composites: (1) by twinning of the martensitic matrix, resulting in a macroscopic twinning yield stress and apparent elastic modulus lower than those predicted by the Eshelby elastic load-transfer theory; and (2) by dislocation slip of the austenitic matrix, thus increasing the transformation yield stress, as compared to a simple load-transfer prediction, because the austenite phase is stabilized by dislocations. Second, in the moderate-strain plastic region where nonslip deformation mechanisms are dominant, mismatch dislocations stabilize the matrix for all samples, thus (1) reducing the extent of twinning in the martensitic samples or (2) reducing the formation of stress-induced martensite in the austenitic samples. This leads to a strengthening of the composites, similar to the strain-hardening effect observed in metal matrix composites deforming solely by slip. Third, in the high-strain region controlled by dislocation slip, weakening of the NiTi composites results, because the matrix contains (1) untwinned martensite or (2) retained austenite, which exhibit lower slip yield stress than twinned or stress-induced martensite, respectively.

NiTi and NiTi-TiC Composites: Part III. Shape-Memory Recovery
K.L. FUKAMI-USHIRO and D.C. DUNAND
The transformation behavior of near-equiatomic NiTi containing 0, 10, and 20 vol pct TiC particulates is investigated by dilatometry. Undeformed composites exhibit a macroscopic transformation strain larger than predicted when assuming that the elastic transformation mismatch between the matrix and the particulates is unrelaxed, indicating that the mismatch is partially accommodated by matrix twinning during transformation. The thermal recovery behavior of unreinforced NiTi which was deformed primarily by twinning in the martensite phase shows that plastic deformation by slip increases with increasing prestrain, leading to (1) a decrease of the shape-memory strain on heating, (2) an increase of the two-way shape-memory strain on cooling, (3) a widening of the temperature interval over which the strain recovery occurs on heating, and (4) an increase of the transformation temperature hysteresis. For NiTi composites, the recovery behavior indicates that most of the mismatch during mechanical deformation between the TiC particulates and the NiTi matrix is relaxed by matrix twinning. However, some relaxation takes place by matrix slip, resulting in the following trends with increasing TiC content at constant prestrain: (1) decrease of the shape-memory strain on heating, (2) enhancement of the two-way shape-memory strain on cooling, and (3) broadening of the transformation interval on heating.

Subcritical Crack Growth at Bimaterial Interfaces: Part I. Flexural Peel Technique
ZHEHUA ZHANG and J.K. SHANG
A flexural peel (FP) technique was developed to study the crack growth behavior along a bimaterial interface. The technique was based on a sandwich specimen where one arm of the specimen was peeled away from the interface under a combined tensile and shear mode. An approximate linear elastic fracture mechanics solution was derived analytically from the J integral formulation. The solution was compared to finite element calculations based on the crack closure method and experimental measurements. From the finite element analysis, ratios of the mode-I and mode-II components of the crack tip field were determined for a wide range of modulus and thickness ratios.

Subcritical Crack Growth at Bimaterial Interfaces: Part II. Microstructural Effects on Fracture Resistance of Metal/Ceramic Interfaces
GANG LIU and J.K. SHANG
The flexural peel technique was used to study the fracture resistance of two model Al2O3/Al interfaces. The bimaterial interface was formed by bonding high-purity Al2O3 with molten Al-5 pct Cu alloy under pressure. The specimens were then heat treated so that the Al-Cu alloy reached peak-aged and extended-overaged conditions. The fracture resistance curve was established for two interfaces with either the peak-aged or overaged Al alloy. The fracture resistance of the interface with the peak-aged Al-Cu alloy was higher in terms of both the initiation and peak toughness. While the peak toughness of the interface scaled with the yield strength of the metal, the initiation toughness differed by a factor of 8. The difference in the initiation toughness is discussed in terms of the disparity in the interfacial microstructure.

Subcritical Crack Growth at Bimaterial Interfaces: Part III. Shear-Enhanced Fatigue Crack Growth Resistance at Polymer/Metal Interface
ZHEHUA ZHANG and J.K. SHANG
Fatigue crack growth along an Al/epoxy interface was examined under different combinations of mode-I and mode-II loadings using the flexural peel technique. Fatigue crack growth rates were obtained as a function of the total strain energy rate for GII/GI ratios of 0.3 to 1.4, achieved by varying the relative thickness of the outerlayers for the flexural peel specimen. Fatigue crack growth resistance of the interface was found to increase with increasing GII/GI ratio. Such a shear-enhanced crack growth resistance of the interface resulted in a gradual transition of crack growth mechanism from interfacial at the low GII/GI ratio to cohesive at the high GII/GI ratio. Under predominantly mode-I loading, the damage in the polymer took the form of crazing and cavitation. In contrast, laminar shear occurred under highly shear loading, resulting in a larger amount of plastic dissipation at the crack tip and improved fatigue crack growth resistance.

Communication: On the In Situ Formation of TiC and Ti2C Reinforcements in Combustion-Assisted Synthesis of Titanium Matrix Composites
S. RANGANATH and J. SUBRAHMANYAM


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