The structure of poly (epsilon-caprolactam) (nylon 6) in the beta meso
morphic form is here examined. The comparison of the diffraction inten
sity, calculated on modeled structures, with the experimental profiles
, collected by us through an automatic diffractometer, is presented. T
his analysis has put into evidence the following limiting structural f
eatures. (a) The beta form of nylon 6 is made of small mesomorphic agg
regates of chains (where the matter scatters coherently) with axes arr
anged in a hexagonal lattice (a = b = 0.48 nm; gamma = 120 degrees). (
b) The chains have disordered conformations (and do not have a definit
e chirality, as it is the case for the 2(1) helices in the alpha and g
amma forms) with the -CH2- chains close to nearly all-trans (antiperip
lanar) and the two dihedral angles adjacent to the amide bond, +/-120
degrees) to antiperiplanar (180 degrees). This notwithstanding, the ch
ains are straight and extended. As a result, the mean chain periodicit
y is close to 0.835 nm. (c) The H-bonds are formed along lines in the
[100], [010], and [1(1) over bar0$] directions; they force neighboring
chains within the small mesomorphic aggregates to adjust their confor
mation in such a way that nearly 100% of hydrogen bonds are always for
med, in agreement with the IR data. In the case of the alpha and gamma
more ordered forms of nylon 6, such lines are all in a unique directi
on, leading to hydrogen-bonded sheets (parallel to the chain axis) of
enantiomorphous anticlined, alternately up and down chains (in the alp
ha form) or of isomorphous isoclined chains, (in the gamma form), (d)
As a consequence, since the amide groups lie all at nearly the same he
ight along z, in the beta form of nylon 6 the lines of hydrogen bonds
lie in layers perpendicular to the chain asis and have the same direct
ion within each layer. However, consecutive layers along z may have th
e lines of H-bonds which are not parallel (e.g., occasionally rotated
by +120 or -120 degrees instead of the ''normal'' 180 degrees). (e) In
the beta form of nylon 6, disorder arises also from the random substi
tution of up and down chains in the lattice positions.