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Mechanics and Fracture Toughness Theories

Chapter 6. Interface mechanics and fracture toughness theories... [Pg.241]

The mechanical and viscoelastic behaviours of natural rubber based blends and interpenetrating polymer networks (IPNs) are fimctions of their structures or morphologies. These properties of blended materials are generally not constant and depend on the chemical nature and type of the polymer blends, and also enviromnental faetors involved with any measurements. Preparations of natural rubber blends and IPNs are well known as effeetive modifieation methods used to improve the original meehanieal and viscoelastie properties of one or both of the eomponents, or to obtain new natural rubber blended materials that exhibit widely variable properties. The most common consideration for their mechanical properties include strength, duetility, hardness, impact resistance and fracture toughness, each of which can be deformed by tension, compression, shear, flexure, torsion and impaet methods, or a eombination of two or more methods. Moreover, the viseoelastieity theory is a way to predict the behaviours of deformation of natural rubber blends and IPNs. The time and... [Pg.501]

By metallurgists in terms of the mechanical properties, such as modulus, fracture toughness, ultimate tensile strength. And they came up with a theory that deals with dislocation, fracture mechanic and continuum mechanics. [Pg.208]

There are two principal theories, or models, that attempt to describe what happens during brittle fracture, the Griffith fracture theory and the Irwin model. Both assume that fracture takes place through the presence of preexisting cracks or flaws in the polymer and are concerned with what happens near such a crack when a load is applied. Each leads to the definition of a fracture-toughness parameter and the two parameters are closely related to each other. The Griffith theory is concerned with the elastically stored energy near the crack, whereas the Irwin model is concerned with the distribution of stresses near the crack. Both theories apply strictly only for materials that are perfectly elastic for small strains and are therefore said to describe linear fracture mechanics. [Pg.235]


See other pages where Mechanics and Fracture Toughness Theories is mentioned: [Pg.239]    [Pg.239]    [Pg.3]    [Pg.4]    [Pg.240]    [Pg.279]    [Pg.416]    [Pg.2289]    [Pg.2272]    [Pg.47]    [Pg.413]    [Pg.167]    [Pg.342]    [Pg.239]    [Pg.241]    [Pg.247]    [Pg.307]    [Pg.319]    [Pg.153]    [Pg.552]    [Pg.293]    [Pg.425]    [Pg.751]    [Pg.514]    [Pg.387]    [Pg.349]    [Pg.229]    [Pg.334]    [Pg.808]    [Pg.601]    [Pg.601]   


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