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Thermal stabilities, packing coefficients and molecular packings in a series of homologous liquid crystals
J. Shashidhara Prasad, P.K. Rajalakshmi
To cite this version:
J. Shashidhara Prasad, P.K. Rajalakshmi. Thermal stabilities, packing coefficients and molecular packings in a series of homologous liquid crystals. Journal de Physique, 1979, 40 (3), pp.309-313.
�10.1051/jphys:01979004003030900�. �jpa-00209110�
Thermal stabilities, packing coefficients and molecular
packings in a series of homologous liquid crystals
J. Shashidhara Prasad and P. K. Rajalakshmi
Department of Physics, University of Mysore, Mysore 570006, India
(Reçu le 2 août 1978, révisé le 13 octobre 1978, accepté le 23 novembre 1978)
Résumé.
2014L’étude systématique des structures cristallines et moléculaires des composés mésogènes est d’un grand intérêt pour l’interprétation d’un certain nombre de propriétés physiques de base des cristaux liquides.
Dans cette optique,
on adéterminé a priori la structure des arrangements moléculaires des matériaux liquides-
cristallins para-heptanoate de phénylazo-para’-éthoxyphényl (P1) et undécylénate correspondant (P1 et P21/c
pour les deux modifications)
enutilisant les données
connues surla structure moléculaire de molécules semblables, para-valérate de phénylazo-para’-éthoxyphényl (P1) et para-hexanoate correspondant (P21/c), suivant l’approche
du modèle de Kitaigorodsky. Les coefficients d’empilements estimés correspondent bien
auxstabilités thermiques
dans les séries homologues.
Abstract.
2014A systematic study of the molecular and crystalline structures of the mesogenic compounds is of
considerable interest in order to interpret
anumber of basic physical properties of liquid crystals. In view of this
an a
priori determination of the molecular packings have been made for the liquid crystalline materials p-p-ethoxy- phenylazo phenyl heptanoate (P1) and undecylenate (P1 and P21/c for the two modifications) based
onthe earlier results of detailed molecular structure data for the similar molecules, p-p-ethoxyphenylazo phenyl valerate (P1)
and hexanoate (P21/c) and the model approach of Kitaigorodsky. The estimated packing coefficients correlate well with thermal stabilities in the homologous series.
Classification Physics Abstracts
61.30
-64.70E
An investigation of single crystals of mesogenic
materials (that is compounds which exhibit smectic, nematic or cholesteric liquid crystalline phases
onheating) shows the nature of packing of molecules in the solid state and provides other molecular characte- ristics which could give insight into the nature of liquid crystals. A systematic study of the molecular and crystalline structure of the mesogenic materials
is of considerable interest for
anumber of basic pro- blems, for example, to help interpret the bulk pro-
perties of the liquid crystalline phase, such
asoptical anisotropy, diamagnetic anisotropy etc. It may also provide
an answerto the problem
asto why only
afew organic substances exhibit liquid crystallinity and why
some of these exhibit more than one phase. In view
of the very little work [1-23] that has been done since the first diffraction studies
onliquid crystalline mate-
rials by Bernal and Crowfoot [24],
aproject has been
started to study the state of molecular packing in
different homologous series in order to achieve
agreater insight regarding imbricated packing and
hence to increase knowledge of the variation in
melting points, thermal stabilities etc., within homo-
logous series and between groups of different homo-
logous series. As a part of this project detailed mole- cular structures of crystals of p-p-ethoxyphenylazo phenyl valerate and hexanoate have been obtained [ 19, 20].
Herein
wehave tried to obtain the molecular struc- ture of the higher homologs viz p-p-ethoxyphenylazo phenyl, heptanoate and undecylenate using the results
available for the lower members of the homologous
series and the model approach of Kitaigorodsky [25].
Also packing coefficients for all the members of the
homologous series of p-p-ethoxyphenylazo phenyl
alkanoate have been estimated, these well explain
the thermal stability variations within the homologous
series.
l. Molecular packing in heptanoate and undecy-
lenate.
-The geometrical analysis technique or
model approach of Kitaigorodsky has been used for
the a priori determination of the molecular packing
for undecylenate and heptanoate without detailed X-ray diffraction studies. Cell dimensions, which
are essential for this approach,
weredetermined by Weissenberg and Precession methods (Table I). Unde- cylenate crystallizes in two space groups viz Pl and
Article published online by EDP Sciences and available at http://dx.doi.org/10.1051/jphys:01979004003030900
310
Table I.
-Crystallographic data for the homologous series p-(p-ethoxyphenylazo) phenyl alkanoates
P21/c. The molecular models
wereconstructed using
the intermolecular radii Rcarbon
=1.80 À,
and Rnitrogen
=1.58 A, and were arranged
sothat the
distances between their centres corresponded to unit
cell dimensions while taking care that the projection
of one molecule falls into the hollows of adjacent
molecules with the closest possible packing. By means
of the symmetry elements of the particular space group, the initial orientation of the molecules were fixed by the angles ({Jl’ ({J2 and p3
asdefined in figure 1.
Subsequently geometrical calculations were made with the contacts of molecules related by different symmetry conditions using the bond lengths of
various bonds that were obtained for the crystals of
hexanoate and valerate by X-ray diffraction methods and refined values of (pl, (P2 and (P3
wereestimated.
With these refined values of (Pl, (P2 and (P3 for the molecular orientation, the molecular packing dia-
grams have been obtained and
areshown in figures 2
to 7 for the two compounds. Several reflections observ- ed on X-ray diffraction photographs of heptanoate
and undecylenate are in very good agreement with the intensities of several major reflections which determine the arrangement of molecules in the case of valerate and hexanoate in their respective space groups, justifying the molecular geometry and arran- gement.
Fig. l.
-The designation of the angles for molecular orientation.
Fig. 2.
-Projection of the molecular packing of heptanoate along
the z-axis.
Fig. 3.
-Projection of the molecular packing of heptanoate along
the y-axis.
2. Packing coefficients and thennal stabilities. - The molecular packing coefficient defined as the ratio of the geometrical volume of the molecule to that of the volume of the molécule as determined by X-ray diffraction experiments, has been estimated for all the members of the series by using the bond length
valence angles and intermolecular contacts obtained
Fig. 5.
-Projection of the molecular packing of undecylenate (Pl) along the y-axis.
Fig. 5.
-Projection of the molecular packing of undecylenate (Pl) along the y-axis.
for crystals of valerate and hexanoate from detailed
crystal structure analysis and the formula for volume increments
where R is the intermolecular radius of the atom
concerned, Ri is the intermolecular radii of atoms that are valence bonded with this atom and
areat
positions distance di from this atom; the height of
the cut off segment is
Fig. 6.
-Projection of the molecular packing of undecylenate (P21/c) along the x-axis.
Fig. 7.
-Projection of the molecular packing of undecylenate (P2,/c) along the y-axis.
The intermolecular radii used for hydrogen, carbon,
oxygen and nitrogen
arerespectively 1.17, 1.80, 1.52 and 1.58 Á. The volumes of the unit cells of different members, the number of molecules per unit cell, the densities, the melting points, the geometrical mole-
cular volumes and the packing coefficients are given
in table II.
312
Table II.
-The volumes of the unit cells of different members, the number of molecules per unit cell.Zl the den-
sities, the melting points, the geometrical molecular volumes and the packing coefficients
3. Discussion.
-It was shown earlier by molecular
structure studies that the change in stability within
the homologs valerate and hexanoate could be accôunted for by the varying difference in the angles
between the benzene planes. As the angle between
the benzene planes increases thermal stability
decreases. The angle between the benzene planes goes up from 4.84 to 10.16 to 23 .2°
aswe pass from valerate to heptanoate. This trend should have been exhibited for undecylenate, but the thermal stability
has increased again, due to an additional dipole at
the end of the chain. These results could be explained
more
elegantly and easily from the knowledge of the packing coefficients which have been estimated. As
wego up the homologous series the packing coefficient of successive members gradually decreases and the
packing coefficient itself shows odd-even phenome-
non