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One-component systems subject to a tensile force

Consider a cross-linked fibrous system, composed of highly axially oriented crystalline regions co-existing with amorphous zones the latter being devoid of any vestiges of crystalline order. The fiber is subject to a uniform tensile force,/, acting [Pg.360]

According to the first law of thermodynamics, the change in internal energy E of any system can be written with complete generality as [Pg.361]

For a one-component system the intensive-extensive pairs p, V and /, L are those of interest. Here, p and V are the pressure and volume, respectively, and Lis the length of the fiber. For a process that is conducted reversibly, dQ = T dS, where S is the entropy. Thus [Pg.361]

For present purposes, it is convenient to choose p, T and / as the independent variables. It is advantageous to utilize the equivalent relation [Pg.361]

For the system to be in equilibrium at constant p, T and/, the function G — fL must be a minimum with respect to all permissible displacements. In particular. [Pg.361]


One-component system subject to a tensile force highly ordered chains, where B is given by Eq. (8.21),... [Pg.365]


See other pages where One-component systems subject to a tensile force is mentioned: [Pg.360]    [Pg.361]    [Pg.363]    [Pg.367]    [Pg.369]    [Pg.371]    [Pg.373]    [Pg.375]    [Pg.377]    [Pg.379]    [Pg.360]    [Pg.361]    [Pg.363]    [Pg.367]    [Pg.369]    [Pg.371]    [Pg.373]    [Pg.375]    [Pg.377]    [Pg.379]    [Pg.94]   


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