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Fracture energy experimental determination

The theoretically estimated and experimentally determined CGRs agree well over a considerable temperature range after calibration at one temperature and specification of an appropriate activation energy for the crack-tip strain rate (Fig. 10). The numerical solution employed in the version of the CEFM described here yields very reasonable results for the environmentally assisted and creep fracture of sensitized... [Pg.683]

Once Klc was detennined, the fracture energy, GIc, was calculated with Youngs modulus and the Poisson coefficient, which were determined experimentally for every formulation following usual procedures. [Pg.190]

Figure 7. Experimentally determined time-temperature shift of the cohesive fracture energy for model solid propellent... Figure 7. Experimentally determined time-temperature shift of the cohesive fracture energy for model solid propellent...
As expected, the energy release rate J and lump-sum cohesive law can be experimentally determined if the crack tip separation 8, the loadhne rotation Op of the adherends, and the global peel load P are simultaneously recorded during the fracture test. It is noted that this interface constitutive relationship is the equivalent interface cohesive law, not necessarily the intrinsic cohesive law. This is because, in addition to the intrinsic cohesive separation, possible plastic deformation in the adhesive layer contributes to the entire normal separation between the two adherends during the fracture test. Of course, with the decrease of the adhesive thickness, it is expected that this equivalent interface cohesive law will finally approach the intrinsic cohesive law [66]. [Pg.337]

Similar to the Mode I fracture test, the energy release rate /jj can be experimentally determined as a function of the crack tip slip Sq and the global shear force gj. Once the experimental /n o curves are obtained according to Equation (8.13), the Mode 11 interfacial traction-separation law t = t(Sq) can be experimentally determined as foUows ... [Pg.344]

A completely different set of tests are referred to as Fracture mechanics test methods. In these tests, attempts are made to measure true material properties of the adhesive joint independent of the geometry test. Such test methodologies require careful preparation of samples so that all experimental variables are controlled. A typical parameter measured for such joints would be the adhesive fracture energy, and normally, this would be determined as a function of some parameter such as the rate or temperature of testing. [Pg.534]

This latest trend in load-bearing materials for arthroplastic applications involves the development of highly fracture-resistant alumina/zirconia composites, as an alternative choice to alumina and zirconia monolithic ceramics. Composite materials are designed from both chemical and microstructural viewpoints in order to prevent environmental degradation and fracture events in vivo. Based on the experimental determination of an activation energy value for an environmentally driven tetragonal to monoclinic transformation, the long-term in vivo environmental resistance of prostheses made from these composite materials can be predicted (Chevalier et al., 2009). [Pg.359]

Elastic fracture mechanics can be applied to rubbers provided that allowance is made for their non-linear stress-strain behaviour. The steps are (a) replacing experimentally determined strain energy density remote from the crack and (b) replacing uq, the crack length in the unstrained state, by u = >n... [Pg.203]

Fig. 4.18. Experimentally determined interface fracture energy F as a function of the local stress state phase angle for the epoxy—glass bilayer system. The measurements were made using an edge-cracked bimaterial strip specimen on which prescribed values of normal and shear displacements were imposed. The different symbols represent four different sets of experiments conducted for this material system. Adapted from Liechti and Ghai (1992). Fig. 4.18. Experimentally determined interface fracture energy F as a function of the local stress state phase angle for the epoxy—glass bilayer system. The measurements were made using an edge-cracked bimaterial strip specimen on which prescribed values of normal and shear displacements were imposed. The different symbols represent four different sets of experiments conducted for this material system. Adapted from Liechti and Ghai (1992).
Modem finite element analysis or other numerical methods have no problem in treating non-linear behavior. Our physical understanding of material behavior at such levels is lacking, however, and effective numerical analysis depends to a large extent on the experimental determination of these properties. Despite these limitations, many researchers have shown that elastic analyses of many adhesive systems can be very Informative and useful. A number of adhesive systems are sufficiently linear, such that it is adequate to lump the plastic deformation and other dissipative mechanisms at the crack tip into the adhesive fracture energy (critical energy release rate) term. [Pg.224]

The surface energy of a material is of fundamental interest, for example in the prediction of crystal morphologies and in understanding fracture. Accurate experimental measurements of the surface energy are difficult to perform. In fact, such measurements are mostly constrained to the determination of surface energies at high temperatures and are subject to numerous errors due to surface-active contaminants. For... [Pg.1569]


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See also in sourсe #XX -- [ Pg.534 ]




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