X-ray Photographic Studies of Liquid Crystals: III. Structure Determination of the Smectic Phase of 4-Butyloxybenzal- 4′-Ethylaniline
Adriaan de Vries, Derry L. Fishel
Abstract
Adriaan de Vries, Derry L. Fishel
Abstract
A new type of smectic phase (smectic H) is described, using microscopic and X-ray data. The structure of this phase can be assigned a three dimensional monoclinic lattice, with a = 10.32 Å, b = 4.986 Å, c = 20.73 Å, and β = 123.8°, probably space group P21, or Pa. The ab plane is parallel to the smectic layers; the thickness of the layers is 17.27 Å. The molecules are most probably approximately parallel to the c axis, thus making an angle of 56.2° with the smectic layers and forming continuous columns of molecules parallel to the c axis. In planes perpendicular to the c axis the arrangement of the molecular axes is approximately hexagonal, with a spacing of 4.97 Å. Successive layers of molecules parallel to the bc plane are shifted 2.87 Å with respect to each other in the direction of the c axis. The most probable arrangement of the molecular planes is a herringbone-type packing. It appears that within the regular three-dimensional structure there are a considerable number of columns of molecules displaced parallel to the c-axis, thus giving rise to continuous diffuse planes in the reciprocal lattice.
OpenAlex reports 91 citations for this work. Citation counts describe recorded attention and do not establish research quality.
A contribution statement is not available in the OpenAlex record.
Method details are not available in the OpenAlex metadata.
Findings are not separately available in the OpenAlex metadata.
Limitations are not available in the OpenAlex metadata.
Application details are not available in the OpenAlex metadata.
A new type of smectic phase (smectic H) is described, using microscopic and X-ray data. The structure of this phase can be assigned a three dimensional monoclinic lattice, with a = 10.32 Å, b = 4.986 Å, c = 20.73 Å, and β = 123.8°, probably space group P21, or Pa. The ab plane is parallel to the smectic layers; the thickness of the layers is 17.27 Å. The molecules are most probably approximately parallel to the c axis, thus making an angle of 56.2° with the smectic layers and forming continuous columns of molecules parallel to the c axis. In planes perpendicular to the c axis the arrangement of the molecular axes is approximately hexagonal, with a spacing of 4.97 Å. Successive layers of molecules parallel to the bc plane are shifted 2.87 Å with respect to each other in the direction of the c axis. The most probable arrangement of the molecular planes is a herringbone-type packing. It appears that within the regular three-dimensional structure there are a considerable number of columns of molecules displaced parallel to the c-axis, thus giving rise to continuous diffuse planes in the reciprocal lattice.
Key concepts: Perpendicular, Monoclinic crystal system, Reciprocal lattice, Liquid crystal, Screw axis, Crystallography, Molecule, Lattice (music)