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376                             Handbook of Properties of Textile and Technical Fibres


                              Antiparallel chains
                             Crystallographic unit
                             Chemical
                               unit
                                                   N–C
                    α form
                                                   C–N

                                                              PA 6


                                                   N–C           O
                    γ form                                       C
                                                                 H
                                                   N–C
                                                                 N
                                Parallel chains
         Figure 12.9 Molecular arrangement in the a and the g crystal lattices of PA 6 (according to
         Millot, 2015).

         phase, they have noncrystalline portions containing some chain-based structural
         arrangements (entanglements, loops, chain ends, tie molecules). The crystal structures
         of polyamides are of two main types (Dasgupta et al., 1996):

         1. The a and b forms appears in even AB polyamides PA 4, PA 6; odd AB polyamides PA 7,
            PA 11; and even AABB polyamides PA 46, PA 66, PA 610.
         2. The g form appears in even AB polyamides from PA 8 and in the even-odd, odd-even, and
            odd-odd AABB polyamides.
            The stable a form consists of planar sheets of hydrogen-bonded fully extended
         planar zigzag chains with sheets stacked upon one another (Fig. 12.9).
            The sheets are easy to define since the eCH 2 e groups are nearly coplanar with
         the amides, which are hydrogen-bonded to amides from the adjacent chains. In even
         AB or even-even AABB polyamides, two successive amide groups along a chain
         are rotated 180 degrees and a forms appear. This form is obtained in PA 6 and PA
         66 by crystallization from the melt by slow cooling. The distances between both the
         hydrogen-bonded chain segments (0.44 nm) and the sheets linked by van der Waal’s
         forces (0.37 nm) are about the same for PA 6 and PA 66.
            The crystals of a form of PA 6 are characterized by an antiparallel alignment of the
         chain segments in a monoclinic cell (Fig. 12.10).
            The calculated optimum cell dimension along the chain axis of PA 6 is 1.7602 nm
         (0 K) (Dasgupta et al., 1996), the interchain distance is 0.44 nm, and the intersheet
         distance is 0.37 nm (Mather and Wardman, 2015). In PA 66 the chain segments run par-
         allel to one another in a triclinic cell (Fig. 12.9). The distance between neighboring chains
         is 0.42 nm, and between adjacent sheets is 0.36 nm (Mather and Wardman, 2015).
            The g form has pleated sheets of the methylene units with hydrogen bonding
         between sheets rather than within sheets (Fig. 12.11). This form results from the
         quenching of PA 6 and PA 66 from the melt. The higher spinning speed leads to
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