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Poly elongation-induced crystallization

It is interesting to note that junction fluctuations increase in the direction of stretching but decrease in the direction perpendicular to it. Therefore the modulus decreases in the direction of stretching, but increases in the normal direction since the state of the network probed in this direction tends to be more nearly affine. The curve of [/" ] versus 1/a is sigmoidal. The parameters k and f of poly(dimethylsiloxane) networks are determined in Figure 17 (155) the intercept of the sigmoidal curves is the phantom modulus. This Flory-Erman theory has been compared successfully with such experiments in elongation and compression (155,162,162-166). It has not yet been extended to take account of limited chain extensibility or strain-induced crystallization (167). [Pg.2339]


See other pages where Poly elongation-induced crystallization is mentioned: [Pg.410]    [Pg.362]    [Pg.693]    [Pg.169]    [Pg.13]    [Pg.191]    [Pg.13]    [Pg.408]    [Pg.800]    [Pg.458]    [Pg.370]    [Pg.305]    [Pg.1215]    [Pg.499]    [Pg.227]    [Pg.469]   
See also in sourсe #XX -- [ Pg.410 ]




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