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Reaction cavity idealized model

This description is elaborated below with an idealized model shown in Figure 17. Imagine a molecule tightly enclosed within a cube (model 10). Under such conditions, its translational mobility is restricted in all three dimensions. The extent of restrictions experienced by the molecule will decrease as the walls of the enclosure are removed one at a time, eventually reaching a situation where there is no restriction to motion in any direction (i.e., the gas phase model 1). However, other cases can be conceived for a reaction cavity which do not enforce spatial restrictions upon the shape changes suffered by a guest molecule as it proceeds to products. These correspond to various situations in isotropic solutions with low viscosities. We term all models in Figure 17 except the first as reaction cavities even... [Pg.88]

As previously stated, this discussion is valid for homogeneous explosives, such as the ones used in the military, since their reactions are predominantly intramolecular. Such explosives are often referred to as ideal explosives, in particular when they can be described using the steady state model of Chapman and Jouguet. In heterogeneous explosives (non-ideal), which are currently used in civil applications, intermolecular (diffusion controlled) mechanisms are predominant for the air bubbles, cavities or cracks (etc.). As a general rule detonation velocities increase proportional to the diameter. [Pg.103]


See other pages where Reaction cavity idealized model is mentioned: [Pg.112]    [Pg.327]    [Pg.54]    [Pg.115]    [Pg.29]    [Pg.350]    [Pg.220]    [Pg.76]    [Pg.22]    [Pg.22]    [Pg.875]    [Pg.47]    [Pg.600]    [Pg.163]    [Pg.162]    [Pg.605]    [Pg.12]   
See also in sourсe #XX -- [ Pg.88 ]




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