Molecular mechanics simulations in Cerius(2) have been used for modelling v
ermiculite intercalated with tetramethylammonium and aniline cations. The p
ublished structure data obtained for these intercalated structures from X-r
ay single crystal diffraction have been used to test the force fields and m
odelling strategy for organo-clays. The strategy of modelling was based on
the nonbond host-guest interactions and on rigid silicate layers and rigid
guest species. The rigidity of silicate layers requires that the cell param
eters a, b and gamma are kept fixed during the energy minimisation. The ene
rgy term was set up using the nonbond interaction terms only and the Crysta
l Packer module in Cerius(2) has been used for the energy minimisation. In
Crystal Packer the rigid units, i.e. the silicate layers and guest species
can be translated and rotated during energy minimisation and the cell param
eters c, alpha, and beta have been varied. Three sets of Van derWaals (VDW)
parameters available in Crystal Packer: Tripos, Universal and Dreiding hav
e been used in present molecular simulations. Ab initio MP2 calculations we
re performed to justify the application of the force field. The best agreem
ent of molecular mechanics simulations with both: experimental and ab initi
o data was obtained with the Tripos VDW parameters for both intercalates. T
he results of modelling are in good agreement with the experimental data as
to the cell parameters and the interlayer packing. The cell parameters rep
orted by Vahedi-Faridi and Guggenheim (1997) for tetramethylammonium-vermic
ulite are: c = 13.616 Angstrom, alpha = 90 degrees, beta = 97.68 degrees; f
rom the present modelling we obtained: c = 13.609 Angstrom, alpha = 90.19 d
egrees, beta = 97.56 degrees. Tetramethylammonium-cations are arranged in o
ne layer in the interlayer space. One C-C edge of NC4 tetrahedra is perpend
icular to the silicate layers. The deep immersion of the methyl groups into
the ditrigonal cavities suggested by Vahedi-Faridi and Guggenheim was not
confirmed by modelling. Slade and Stone (1984) presented the measured cell
parameters for aniline vermiculite: c = 14.89 Angstrom, alpha = 90 degrees,
beta = 97 degrees; present result is: c = 14.81 Angstrom , alpha = 90.72 d
egrees, beta = 96.70 degrees for partially exchanged vermiculite and c = 14
.84 Angstrom, alpha = 90.53 degrees, beta = 97.17 degrees for fully exchang
ed vermiculite. The aniline cations are positioned over the ditrigonal cavi
ties alternating in their anchoring to lower and upper silicate layer. The
C-N bonds are perpendicular to layers.