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Research Highlights on Soft Matter |
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There is an increasing need to understand the self-assembling properties of short amphiphilic chain molecules as they find ample uses in forming templates in nano-fabrication of various devices. For example, semiconductor nano-structures are synthesized by the use of diblock copolymers as nano-lithographic masks. Broadly speaking, this is an emergent theme where it is believed that the self-assembling properties of amphiphiles and block copolymers can be utilized in parallel production of devices in nano-meso scales which are otherwise difficult to produce using conventional lithographic techniques. We have used Monte Carlo and Molecular dynamics simulations to explore the following:
Quite naturally, we have extended the above calculations to find how packing constraints affect
the phase diagram of amphiphiles with different hydrophilic heads. This is a natural generalization of
applying Gibbs ensemble Monte Carlo method pioneered by Panagiotopolous and co-workers who applied this
technique to polymers and amphiphiles on lattice. The accompanying figure shows how the critical point
shifts in the temperature-density plane.
Apart from carrying out Molecular dynamics and Monte Carlo calculations for models in continuum,
we have also investigated amphiphiles on a lattice as shown in the figure. These calculations are
order of magnitude faster, solvents molecules, which are eliminated in continuum calculations, here
can be kept at no additional cost, and for certain properties lattice models are as good as their
off-lattice counterparts. The figure on the left and right shows depiction of lattice amphiphiles and
vesicle formation respectively.
Ionomers are polymers having a tiny fraction of charges
at the backbone and equal numbers of
counter-ions present in the vicinity for charge neutrality. Attractive Coulomb interaction
among opposite ions pairs gives rise to formation of multiplets and bridges, as shown in the
figure, responsible for
gel like properties even at very low concentration. Ionomers also exhibit unusual shear
thinning behavior and other anomalous viscoelastic properties. They are potential candidates
for artificial muscles, fuel cell membranes, and self-healing materials to design exterior
body of space-crafts. At a fundamental level, glass transition and formation of Coulomb gels
in these systems is a nearly unexplored field.
Unlike previous studies, we have developed
modes for ionomers with explicit incorporation of ions and counter-ions and plan to make
an in depth study of the structure-function relationship in these systems. The figure (right)
shows a snapshot of formation of multiples from our simulation.
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The polymer-induced depletion interaction between mesoscopic colloid particles in a solution
of non-adsorbing polymer chains is of fundamental interest in colloid physics. For
entropic reasons the chains avoid the space between two close particles, or between a particle
and a planar wall, and create an effective attraction among the colloid particles, or push the
particles toward the walls of the container. This depletion interaction has been used to explain
phase diagrams of colloid-polymer mixtures and is believed to be important for a
variety of interesting colloid systems such as casein micelles, hemoglubine,
and globular proteins.
We have used an off-lattice bead-spring model of a polymer solution in a container with impenetrable walls
to study the depletion interaction of a colloid particle with the planar wall by means
of a Monte Carlo simulation. As expected, this interaction is found to depend essentially on
the ratio R/Rg of the particle radius R to the mean radius of gyration Rg of the
polymer chains in the case of dilute and semi-dilute solutions.
The driven diffusion of an entangled polymer in disordered media is a theoretical problem that
has received much attention because of its close connection to Biology.
The enormous motivation stems from the prospect of high speed detection of sequences in a
single polynucleotide molecule. As a result,
the behavior of large flexible molecules e.g., DNA, RNA, proteins, and
synthetic polyelectrolytes in disordered porous media offers many challenges
and excitement to the scientific community.
Therefore, it is rather important to identify different mechanism of transportation
of polymers as it moves through a disordered medium
where the chain entanglement effect plays a crucial role.\par
We have examined the properties of an end-labeled
telechelic polymer chain where only the first monomer of the chain is
influenced by an external force using a stochastic molecular dynamics simulation method.
and calculated the dynamic properties of the chain directly from the
simulation as a function of bias and impurity density as well.
Conformations of a telechelic chain of length N=64 in
porous media with rho_imp= 0.1. In both cases the external field points
from left to the right. The top snapshot shows a situation where the rest
of the chain has overtaken the immobile head which has got stuck between obstacles.
The left snapshot displays a freely drifting chain among obstacles.
Most of the obstacles have been removed for better visibility.
A rather different picture emerges when the phase separating system
is confined in restricted geometries.
We have studied the phase ordering dynamics of a
binary liquid mixture
and nematic liquid crystals in restricted geometries
under different
surface anchoring conditions. We find that depending upon the symmetry and
the conservation laws of the order parameter,
geometric confinement and surface anchoring
have marked impact on the growth dynamics. We have extended these calculations from simple mixture to a phase separating polymer solution where the coarsening process gets more complicated by chain conformations and entanglement effects. Our simulations strongly indicate that the true late time growth kinetics of quenched polymer solutions belong to the same universality class of small molecular mixtures.Following the general theme, the above study has been extended to the case where polymers are confined in a long and narrow cylindrical pore subject to an attractive wall potential. We find that for deep quenches the uniform density state breaks up into alternate polymer rich phase in the form of plugs and the solvent rich phase. |