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Models for Yield

The strain rate in the stress direction is proportional to the net jump rate v+ — v, leading to Eq. (62), where V = xA typically corresponds to a few repeat units and is interpreted as an activation volume. [Pg.744]

Among the better-known efforts to provide a more microscopic description of yield within the general Ree-Eyring framework is the approach of Argon, based on metallurgical models, in which the energy barrier is associated with the elastic displacements necessary to accommodate the elementary shear processes [24]. Another well known, but somewhat different, approach is that of Robertson, who [Pg.744]


The optimization variables values are SQ = 118.3 kg/m3, tr = lh,R = 0.2, and r = 0.2. The values for % yield and productivity calculated by the statistical models are 0.82 and 26.73 kg/(m3-h), respectively. Using the values calculated for S0, tr/ R, and r in the rigorous model, however, the % yield calculated was 0.69 and productivity was 26.39 kg/(m3-h). Note that although the statistical model for yield developed by Costa et al. (5) has a high correlation coefficient and passed the F-test with 99% confidence, at the calculated optimal conditions, it presents a great deviation from the rigorous model. [Pg.492]

A simple model for yield in disordered solids can be derived from the Eyring model, discussed in Section 1.5.1. If the enthalpy of a hop AH is very large, then flow is essentially impossible unless the applied shear stress is large, so that v a approaches AH in magnitude. Then the frcqueney of forward hops is much larger than that of reverse... [Pg.37]

Young, R. J. (1988) Screw dislocation model for yield of polyethylene, Mater. Forum, 11, 210-216. [Pg.324]

Haward and Thackray Model, in 1968 Haward and Thackray (37) developed a one-dimensional model for yield using a spring in series with a parallel arrangement of a spring and dashpot (Fig. 12). The dashpot, rather than being Newtonian as with the standard Maxwell/Kelvin models, was instead an Eyring... [Pg.7387]

Thus the term sq in the original Argon model for yield (eq. 36) is replaced by s to give... [Pg.7389]

P. B. Bowden and S. Raha, A Molecular Model for Yield and Flow in Amorphous Glassy Polymers Making Use of a Dislocation Analogue , Philos. Mag. 29, 149-166 (1974). [Pg.7419]

Young RJ (1974) Dislocation model for yield in polyethylene. Philos Mag 30 85 Zhou J-J, Liu J-G, Yan S-K, Dong J-Y, Li L, Oian C-M, Schultz JM (2005) Atomic force microscopy study of the lamellar growth of isotactic polypropylene. Polymer 46 4077-4087 Zia Q, Radusch HI, Androsch R (2009) Deformation behavior of isotactic polypropylene crystallized via a mesophase. Polym Bull 63 755... [Pg.328]

Bowden, P.B. and Raha, S. (1974) A molecular model for yield and flow in amorphous glassy polymers making use of a dislocation analogue. Phil. Mag., 29,149. [Pg.374]

Young, R.J. (1988) A dislocation model for yield in polyethylene. Materials Forum,... [Pg.376]

Young R J (1974) Dislocation model for yield in polyethylene, Philos Afa 30 85-94. [Pg.72]

Herschel-Bulkley model for yield stress fluids. [Pg.100]


See other pages where Models for Yield is mentioned: [Pg.465]    [Pg.96]    [Pg.96]    [Pg.373]    [Pg.7420]    [Pg.744]    [Pg.374]    [Pg.167]    [Pg.47]    [Pg.70]    [Pg.1503]    [Pg.1536]    [Pg.102]   


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