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Chains entropic tightness

Let us consider two limiting cases of the adduced in Fig. 4.15 dependence at = 0 and 1.0, both at d = 3. In the first case (d = 2) the value dU = 0 or, as it follows from dU definition (the Eq. (4.31)), dW = dQ and polymer possesses an ideal elastic-plastic deformation. Within the frameworks of the fractal analysis d =2 means, that (p, = 1.0, that is, amorphous glassy polymer structure represents itself one gigantic cluster. However, as it has been shown above, the condition d =2 achievement for polymers is impossible in virtue of entropic tightness of chains, joining clusters, and therefore, d > 2 for real amorphous glassy polymers. This explains the experimental observation for the indicated polymers dU 0 or dW dQ [57], At Vg, =... [Pg.72]


See other pages where Chains entropic tightness is mentioned: [Pg.226]    [Pg.226]    [Pg.398]    [Pg.285]    [Pg.221]    [Pg.97]    [Pg.381]    [Pg.330]    [Pg.152]    [Pg.285]    [Pg.87]    [Pg.740]    [Pg.912]    [Pg.166]    [Pg.303]    [Pg.5]    [Pg.120]    [Pg.20]    [Pg.1057]    [Pg.14]    [Pg.203]   
See also in sourсe #XX -- [ Pg.226 ]




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