A model to calculate the fatigue life (residual durability) of solids under rolling contact, which is based on the concepts of linear fracture mechanics, has been proposed. The construction of a crack growth path in one of the bodies of a contacting pair, using applicable criteria of local fracture,
The random walk theory of crack propagation
β Scribed by A.S. Krausz
- Publisher
- Elsevier Science
- Year
- 1979
- Tongue
- English
- Weight
- 397 KB
- Volume
- 12
- Category
- Article
- ISSN
- 0013-7944
No coin nor oath required. For personal study only.
β¦ Synopsis
Crack propagation is considered as a random walk process of consecutive atomic bond breaking and healing steps. The total number of steps is propo~ion~ to tfre propa~t~n time, and the difference of the number of breaking and healing steps is propo~ional to the location of the crack tip at that time. The analysis of the probability and of the number of distinct sequences led to a rigorous expression of a crack size probability distribution function in terms of time, mechanical work, bond free energy or surface energy, and temperature. It is shown that the shape of the probability distribution function is proportional to the sum of the breaking and healing rate constants, and the average crack size is determined by the difference of these two rate constants and by the propagation time.
π SIMILAR VOLUMES
## Most fatigue crack proration studies reported in the literature have been conducted from either a continuum or micro-mechanics point of view. Attempts to combine these points of view within a single experimental study or modeling effort have been relatively scarce. This is surprising considerin
An extension of the validity of a theory proposed at the Crack Propagation Symposium in Cranfield, September 1961, has been performed by introducing a new parameter, the endurance limit n,, i&o the basic formula, which thus takes the form dx/&? = k(o -a,)@. The relationship between crack length z a
The kinetics theory of thermally activated time dependent crack propagation is extended to describe the crack size dist~but~on in non-steady state. The dis~but~on is represented by a series of n differential equations, each expressing the rate of crack tip concentration change over the system of n c