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1.1 Block Copolymers as Useful Nanomaterials 7
1.1.4
Rod – Coil Block Copolymers
There are essentially two types of BCP, both of which highlight interesting
avenues for BCP self - assembly. “ Coil – coil ” BCPs, which are the most commonly
studied, contain A and B blocks that can both be theoretically modeled as fl ex-
ible chains. “ Rod – coil ” BCPs, on the other hand, have one polymer chain that
is best represented as a rigid rod due to its stiff nature and anisotropic molecular
shape. Rod - type molecules, also known as mesogens , can be incorporated into
the main chain of a polymer backbone or appended from the polymer backbone
as a side - chain substituent. Both types of rod – coil BCP have been shown to
exhibit liquid crystalline ( LC ) behavior when placed in solution [21, 22] . These
solutions are known as lyotropic solutions, which means that their phase behavior
changes at different polymer concentrations. Initially, the polymers exhibit a
disordered state called the isotropic phase; however, when the solution reaches
a critical concentration, the molecular chains become locally packed and are
forced to orient in a particular direction ( nematic phase) due to the anisotropy
of their shape. They can also arrange into several types of well - defi ned layers
( smectic phases). By creating a BCP with a combination of a rod - like polymer
block and a fl exible polymer block, molecular level ordering characteristic of
liquid crystals can be combined with the microphase - separated behavior typical
of BCPs to produce hierarchical levels of self - assembly [23] .
In a groundbreaking study on poly(hexylisocyanate - block - styrene) ( PHIC - b -
PS ) – where the PHIC block represents the “ rod ” and the PS represents the
“ coil ” block – it was found that, with increasing concentration of the polymer,
isotropic, nematic and smectic LC phases each developed before the polymer
adopted its fi nal microphase - separated state [24] . As the PHIC chain was
much longer than the PS chain in this case, the PHIC chain axis tilted with
respect to the layer normal and interdigitated with the PS in order to accom-
modate the strain, resulting in wavy lamellae and never - before - seen zigzag
and arrowhead morphologies. Electron diffraction experiments revealed ∼ 1 nm
spacings between the PHIC chains and a smectic layer repeat distance of
approximately 200 nm. Furthermore, shearing a nematic solution of the polymer
on a glass substrate induced over 10 μ m of perfect long - range ordering of the
layers, thus powerfully illustrating the multiple levels of ordering possible
with LC - BCPs.
In further studies conducted by Mao and coworkers [25] , a LC side group was
attached as a pendent unit to a modifi ed poly(styrene - block - isoprene) BCP. In this
material, the phase transitions occurred in the opposite direction. The microphase
separation of the classical lamellae and cylinders developed fi rst, after which
smectic layering of the LC blocks developed within the BCP microdomains due to
constraint by the intermaterial dividing surface ( IMDS ) (Figure 1.5 ). Again, by
incorporating a rigid block into a BCP framework, a hierarchy of ordering is
observed. Unique chemical properties such as LC behavior may turn out to be
crucial for future self - assembled synthetic materials.