Propagating crack

Crack Reflection. Crack deflection can result when particles transform ahead of a propagating crack. The crack can be deflected by the locali2ed residual stress field which develops as a result of phase transformation. The force is effectively reduced on the deflected portion of the propagating crack resulting in toughening of the part. 

Fracture mechanics (qv) affect adhesion. Fractures can result from imperfections in a coating film which act to concentrate stresses. In some cases, stress concentration results in the propagation of a crack through the film, leading to cohesive failure with less total stress appHcation. Propagating cracks can proceed to the coating/substrate interface, then the coating may peel off the interface, which may require much less force than a normal force pull would require. 

The implications of a significant role for strain rate are wider than the obvious one that stress corrosion should only occur over a restricted range of strain rates. Thus, in constant load tests, since cracks will continue to propagate only if their rate of advancement is sufficient to maintain the crack-tip strain rate above the minimum rate for cracking, it is to be expected that cracks will sometimes stop propagating, particularly below the threshold stress. Such non-propagating cracks are indeed observed below the thres-hold . Moreover, in constant-load or constant-strain tests, the strain rate diminishes with time after loading, by creep exhaustion if the stress remains sensibly constant, and it is found that the stress-corrosion results are sensitive to the relative times at which the stress and electrochemical... 

Fig. 9.12 Results of molecular mechanics simulations (a) A Stone-Wales defect (A mode) in a zigzag SWCNT, (b) a Stone-Wales defect (B mode) in a zigzag SWCNT, the bonds with highest potential energy are indicated by arrows. Propagating cracks in (c) A defect-fiee zigzag tube, and (d) defect-lfee armchair tube. Fracture mode of armchair tube with (e) Stone-Wales defect (A mode), and (f) Stone-Wales defect (B mode). Fracture mode of zigzag tube with (g) Stone-Wales defect (A mode), and (h) Stone-Wales defect (B mode) (Huynh et al., 2002. With permission from Wiley)...

As mentioned earlier, fatigue is the result of crack initiation and propagation. Crack growth under fatigue is estimated by the Paris equation ... 

Early explanations about the effect of mechanical energy on the reactivity of solids are the hot-spot-model [23] and the magma-plasma-model [8]. The generation of hot-spof may be used to explain the initiation of a self-sustained reaction such as explosion, deflagration, or decomposition. Temperatures of over 1000 K on surfaces of about 1 pm2 for KM to 10-3 s can be created. These temperatures can also be found near the tip of a propagating crack [24]. Typically nonequilibrium thermodynamics are used to describe these phenomena. The magma-plasma-model allows for local nonequilibrium states on the solid surface during impact however, due to the very short time scale of 1(H s of these states only statistical thermodynamics can describe the behavior. 

Wallner lines are formed when sonic waves generated during fracture interact with principal stress driving the propagating crack front. Wallner lines appear as a series of arc shaped steps as shown in Figure 2.33. 

Types of tests. Laboratory corrosion fatigue tests can be classified as either cycles-to-failure (complete fracture) or crack propagation (crack growth) test. In cycles-to-failure testing, specimens or parts are subjected to a sufficient number of stress cycles to initiate and propagate cracks until complete fracture occurs. Such data are usually obtained by... 

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