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2004, Physical Review E
AI
Velocity fluctuations of fast-moving cracks in stressed materials may result from interactions between macro cracks and micro cracks, whether these are pre-existing defects or formed during crack evolution. The study develops a theoretical framework analyzing this interaction in two-dimensional space, leading to the conclusion that these interactions cause significant and rapid fluctuations in crack velocity, which align with experimental observations. The authors propose a novel approximation method to simplify the complex dynamics into ordinary differential equations for crack tip positions, supported by simulation results.
Phys Rev E, 2004
We address the velocity fluctuations of fastly moving cracks in stressed materials. One possible mechanism for such fluctuations is the interaction of the main crack with micro cracks (irrespective whether these are existing material defects or they form during the crack evolution). We analyze carefully the dynamics (in 2 space dimensions) of one macro and one micro crack, and demonstrate that their interaction results in a {\em large} and {\em rapid} velocity fluctuation, in qualitative correspondence with typical velocity fluctuations observed in experiments. In developing the theory of the dynamical interaction we invoke an approximation that affords a reduction in mathematical complexity to a simple set of ordinary differential equations for the positions of the cracks tips; we propose that this kind of approximation has a range of usefulness that exceeds the present context.
Arxiv preprint arXiv:0911.0173, 2009
Cracks are the major vehicle for material failure and often exhibit rather complex dynamics. The laws that govern their motion have remained an object of constant study for nearly a century. The simplest kind of dynamic crack is a single crack that moves along a straight line. We first briefly review the current understanding of this "simple" object. We then critically examine the assumptions of the classic, scale-free theory of dynamic fracture and note when it works and how it may fail if certain assumptions are relaxed. Several examples are provided in which the introduction of physical scales into this scale-free theory profoundly affects both a crack's structure and the resulting dynamics.
Journal of The Mechanics and Physics of Solids, 1995
This paper demonstrates that rapid fracture of ideal brittle lattices naturally mvolves phenomena long seen m expenment, but which have been hard to understand from a contmuum point of view. These Idealized models do not mimic realistic microstructure, but can be solved exactly and understood completely. First It IS shown that constant velocity crack solutions do not exist at all for a range of velocltles startmg at zero and rangmg up to about one quarter of the shear wave speed. Next It is shown that above this speed cracks are by and large linearly stable, but that at sufficiently high velocity they become unstable with respect to a nonlinear microcracking instablhty The way this instabllity works Itself out IS related to the scenario known as mtermittency, and the basic time scale which governs It is the inverse of the amount of disslpatlon m the model. Finally, we compare the theoretical framework with some new experiments in Plexiglas, and show that all qualitative features of the theory are mlrrored in our experlmental results.
Elsevier eBooks, 1985
Modern engineering design against fracture in Isaftey-critica1" structures genera 11 y is based on the concept of defector damagetolerance, where projected life is estimated in terms of the time for an assumed initial defect to propagate to some critical size. Accordingly, from a materials standpoint, increased resistance to failure can be achieved by retarding the sub-critical growth of cracks prior to final failure. In the current paper, an overview is presented of severa 1 recent advances in the understanding of the salient mechanisms of such slow crack growth, involving fracture under both monotonic and cyclic loading at ambient and elevated temperatures. '. ' .
Engineering Fracture Mechanics
The experimental data presented in this paper reveals that even if the growth of long cracks in two materials, with different microstructures, have different ⁄ versus ∆ curves the corresponding small crack curves can be similar. We also see that long cracks in a large range of steels with different microstructures, chemical compositions, and yield stresses can have similar crack growth rates. The materials science community is challenged to explain these observations. The experimental data also suggests that the threshold term ∆ thr in the Hartman-Schijve variant of the NASGRO crack growth equation appears to have the potential to quantify the way in which small cracks interact with the local microstructure. In this context it is also noted that the variability in the life of operational aircraft is controlled by the probability distribution associated with the size and nature of the material discontinuities in the airframe rather than the probability distribution associated with the scatter in the growth of small cracks with a fixed initial size.
Scripta Metallurgica et Materialia, 1994
Physical Review B, 1992
We report on experimental investigations of the propagation of cracks in the brittle plastic polymethyl methacrylate (PMMA). Velocity measurements with resolution an order of magnitude better than previous experiments reveal the existence of a critical velocity (330+30 m/s) at which the velocity of the crack tip begins to oscillate, the dynamics of the crack abruptly change, and a periodic pattern is formed on the crack surface. Beyond the critical point the amplitude of the oscillations depends linearly on the mean velocity of the crack. The existence of this instability may explain the failure of theoretical predictions of crack dynamics and provides a mechanism for the enhanced dissipation observed experimentally in the fracture of brittle materials.
Crack trajectories under different loading conditions and material microstructural features play an important role when the conditions of crack initiation and crack growth under fatigue loading have to be evaluated. Unavoidable inhomogeneities in the material microstructure tend to affect the crack propagation pattern, especially in the short crack regime. Several crack extension criteria have been proposed in the past decades to describe crack paths under mixed mode loading conditions. In the present paper, both the Sih criterion (maximum principal stress criterion) and the R-criterion (minimum extension of the core plastic zone) are adopted in order to predict the crack path at the microscopic scale level by taking into account microstress fluctuations due to material inhomogeneities. Even in the simple case of an elastic behaviour under uniaxial remote stress, microstress field is multiaxial and highly non-uniform. It is herein shown a strong dependence of the crack path on the material microstructure in the short crack regime, while the microstructure of the material does not influence the crack trajectory for relatively long cracks.
Philosophical Magazine B, 1998
The classical theory of fracture mechanics states that a crack propagating in an unbounded body should smoothly accelerate until it reaches the Rayleigh wave speed. We introduce here a general approach for solving the equation of motion of the crack tip. We show that the loading conditions and the geometry of the con® guration do not produce inertial e ects. The equation of motion of a propagating crack is always a ® rst-order di erential equation.
Physical Review E, 2013
We employ a recently developed model that allows the study of two-dimensional brittle crack propagation under fixed grip boundary conditions. The crack development highlights the importance of voids which appear ahead of the crack as observed in experiments on the nano-scale. The appearance of these voids is responsible for roughening the crack path on small scales, in agreement with theoretical expectations. With increasing speed of propagation one observes the branching instabilities that were reported in experiments. The simulations allow understanding the phenomena by analyzing the elastic stress field that accompanies the crack dynamics.
The European Physical Journal Special Topics, 2007
The properties of slow crack growth in brittle materials are analyzed both theoretically and experimentally. We propose a model based on a thermally activated rupture process. Considering a 2D spring network submitted to an external load and to thermal noise, we show that a preexisting crack in the network may slowly grow because of stress fluctuations. An analytical solution is found for the evolution of the crack length as a function of time, the time to rupture and the statistics of the crack jumps. These theoretical predictions are verified by studying experimentally the subcritical growth of a single crack in thin sheets of paper. A good agreement between the theoretical predictions and the experimental results is found. In particular, our model suggests that the statistical stress fluctuations trigger rupture events at a nanometric scale corresponding to the diameter of cellulose microfibrils.
Physical Review Letters, 2001
We address the role of material heterogeneities on the propagation of a slow rupture at laboratory scale. With a high speed camera, we follow an in-plane crack front during its propagation through a transparent heterogeneous Plexiglas block. We obtain two major results. First, the slip along the interface is strongly correlated over scales much larger than the asperity sizes. Second, the dynamics is scale dependent. Locally, mechanical instabilities are triggered during asperity depinning and propagate along the front. The intermittent behavior at the asperity scale is in contrast with the large scale smooth creeping evolution of the average crack position. The dynamics is described on the basis of a Family-Vicsek scaling.
Journal of Applied Physics, 2003
Evaluation of the relationship between the effective strain and the springback behavior during the deformation of metallic glass ribbons Appl. Phys. Lett. 105, 061906 (2014); 10.1063/1.4893159
Fracture analysis is one important role in a material characterization. Many theory and observation on the subject especially after the matter was broken or post cracked, but on the other hand, as far as author knowledge, only a few research are did in in situ observation on micro crack propagation, because of the propagation is in a micrometer scale and can't be observed using a naked eye and has difficulties to observed using standard optical microscope. In this study, different material are observed, the micro cracks propagation in Aluminum foil is observed in an in situ mode using an optical microscope during loaded in an axial tensile mode, the other is a Si thin plate was observed using TEM after compressed in axial compressed.
Journal of Engineering Materials and Technology, 2020
The dynamic fracture behavior of brittle materials that contain micro-level cracks should be examined when material subjected to impact loading. We investigated the effect of micro-cracks on the propagation of macro-cracks that initiate from notch tips in the Kalthoff–Winkler experiment, a classical impact problem. To define predefined micro-cracks in three-dimensional space, we proposed a two-dimensional micro-crack plane definition in the bond-based peridynamics (PD) that is a non-local form of classical continuum theory. Randomly distributed micro-cracks with different number densities in a constant area and number in expending area models were examined to monitor the toughening of the material. The velocities of macro-crack propagation and the time required for completing fractures were considered in several predefined micro-cracks cases. It has been observed that toughening mechanism is only initiated by exceeding a certain number of micro-cracks; therefore, there is a positive...
Physical review. E, Statistical physics, plasmas, fluids, and related interdisciplinary topics, 1996
This paper describes a formalism designed to answer questions about Hamiltonian systems in contact with a heat bath. The formalism is applied to a simple model of fracture to find, first, the rate at which a crack creeps through a brittle body as a result of thermal fluctuations and, second, the rate at which the crack jumps from creeping to rapid motion. The dominant exponential behavior of these processes is calculated exactly, but the prefactors are only estimated. Some of the solutions cannot be viewed in the traditional manner as corresponding to passage over a saddle point. Viewed as an isolated Hamiltonian system, the crack shows that irreversible behavior can arise because, although the probability of traveling from past to present equals the probability of traveling backwards from present to past, the probabilty of traveling still further into the future is exponentially greater. ͓S1063-651X͑96͒06410-0͔
Physical Review Letters, 1999
Mendeleev Communications, 2003
The terminal velocity of a crack determines the reasonability of the application of classical or quantum approaches to the description of phenomena at the crack tip; an expression for the fractoemission intensity of crystals accounting the quantum character of energy transfer at the tip of a fast-moving crack was obtained.
2020
The main objective of this research is to determine the influence of micro-crack on the propagation of a semi-infinite crack. This study is mainly based on the determination of the strain energy during the interaction between the semi-infinite crack and the neighboring microcrack. The problem is formulated by a plane element, having a micro-crack varies around itself and around a semi-infinite crack. The cracked element is subjected to a uniform load according to mode I. The theoretical analysis of the strain energy is based on the stress found during the propagation of the semi-infinite crack. During the positioning of the micro-crack with respect to the semi-infinite crack, according to the strain energy results, the presence of the micro-crack can amplify, reduce and sometimes arrest the propagation of the semi-infinite crack.
2013
Nonlinear dynamics of crack propagation is investigated experimentally and theoretically with a goal to clarify the nature of limiting crack velocity, the transition from steady-state to branching regimes of crack dynamics, the dynamics of crack arrest. Theoretical explanation of limiting steady-state crack velocity and the transition to branching regime was proposed due to the study of collective behavior of microcrack ensemble at the crack tip area. Experimental study of crack dynamics was carried out in the preloaded plate PMMA specimen using the high speed camera coupled with the photo-elasticity method, the point stress recording with a laser system, the failure surface roughness measurement.
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