SMALL-ANGLE X-RAY-ANALYSIS OF THE EFFECT OF TEMPERATURE ON THE SELF-ASSEMBLING COLUMNAR STRUCTURES FORMED BY A POLYMETHACRYLATE WITH HIGHLYTAPERED SIDE-GROUPS AND BY ONE OF ITS LOW MOLAR-MASS PRECURSORS
Sn. Chvalun et al., SMALL-ANGLE X-RAY-ANALYSIS OF THE EFFECT OF TEMPERATURE ON THE SELF-ASSEMBLING COLUMNAR STRUCTURES FORMED BY A POLYMETHACRYLATE WITH HIGHLYTAPERED SIDE-GROUPS AND BY ONE OF ITS LOW MOLAR-MASS PRECURSORS, Macromolecular symposia, 118, 1997, pp. 663-675
Small angle X-ray methods have been used to investigate the self-assem
bling columnar structures formed by a polymethacrylate with large high
ly tapered side groups, and by one of its low molar mass precursors. T
he polymer is poly{2-{2-[2(2-methacryloyloxyethoxy)ethoxy] ethoxy}ethy
l-3,4,5-tris(p-dodecyloxybenzyloxy)- benzoate} (H12-ABG-4EO-PMA); the
precursor is 2-{2-[2-(2-hydroxpethoxy) ethoxy] }-ethyl-3,4,5-tris(p-do
decyl-oxybenzyloxy)benzoate (H12-ABG-4EO-OH). Both the polymer and the
precursor form three dimensionally ordered structures at room tempera
ture, consisting of hexagonally packed cylinders with diameters in the
region of 60 and 53 Angstrom, respectively, in which the interiors of
the columns probably have helical arrays of the stacked tapered group
s. At higher temperatures these are converted to columnar hexagonal (p
hi h) liquid crystalline phases. At temperatures close to this transit
ion for the precursor we detect two coexisting columnar structures, wi
th the phi h structure having a diameter approximately 1 Angstrom high
er than that in the solid state. For the polymer, the data are not so
well resolved, and coexisting phases cannot be resolved. However, the
changes in column dimensions are larger than for the precursor. Conver
sion of the room temperature phase to the phi h phase at 40 degrees C
results in an increase of 3 Angstrom in the diameter, which then decli
nes by approximately the same amount as the temperature rises to 90 de
grees C, close to the isotropization point. Cooling to room temperatur
e does not immediately restore the room temperature structure. Rather,
we obtain a quenched phi h structure, with a column diameter almost 1
0% higher. These dimensional changes correlate well with the changes i
n diameter with temperature seen for the bulk fiber, and suggest a con
tinuous rearrangement of the interiors of the columns in the phi h pha
se, such as a partial unwinding of a disordered helical structure.