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Block copolymers, self-assembling effective composition

Nonionic block copolypeptides made of PEGylated L-lysine and L-leucine residues, PELLys- -PLLeu (Fig. lOh) have also been described [52], The copolymers adopted a rod-like conformation, due to the strong tendency of both segments to form a-helices (CD spectroscopy), and produced a variety of self-assembled structures in aqueous solution. Micrometer vesicles and sheet-like membranes could be obtained for copolymers with fractions of the hydrophobic leucine ranging from 10 to 30mol%. Conventional uncharged block copolymers of this composition would be expected to form spherical or cylindrical micelles. The assembly into bilayers was related to a secondary structure effect, as illustrated in Fig. 12. Accordingly, samples with the same composition but nonhelical chain conformation (CD),... [Pg.182]

A remarkable property of polymer melts is their ability to self-assemble, driven by thermodynamic incompatibilities of the different monomers. A brief introduction to the thermodynamic theory of macrophase separation in homopolymer blends and microphase separation in diblock copolymer melts is given. In particular, the effect of controllable parameters, including the monomer interactions, the block composition. [Pg.49]

Next we consider the effect of the block copolymer composition /= NfJN on the ordered morphology. In the limit of very strong segregation, that is, zero interface width, the natural idea is to let the stable ordered phase correspond to the phase with the minimal interface surface. To illustrate this principle and to obtain a semiquantitative estimate of the values of/for which the transitions between the three classical stmctures occur, we consider an LxLxL volume of the self-assembled diblock copolymer system. The ordered states that will be compared are the lamellar phase, a square lattice of cylinders, and spheres on a simple cubic (SC) lattice. L is the periodicity length scale of the layers, the square, and the cubic lattice (Figure 19). The LxLxL volirme element contains one cylinder resp. one sphere. Volirme conservation (Figure 20), therefore, requires fL = 7tRcL = 4n/SRs, where Rc and Rs are the radii of the cylinder and the sphere, respectively. [Pg.299]

Ko, M.J., Kim, S.H., and Jo, W.H. (2001) A molecular dynamics simulation on the self-assembly of ABC triblock copolymers, 1. Effects of block composition in symmetric triblock copolymers. Macromolecular Theory and Simulations, 10,381-388. [Pg.590]

The temperature-driven self-assembly of nonionie amphiphilie tailor-made triblock copolymers was studied by DLS, NMR, ITC, and SAXS. The composition of these triblock copolymers is more complex than that of the vast majority of poly(2-allqrl-2-oxazoline)s a statistical thermo-responsive (iPrOx) and hydrophobic (BuOx) central block with terminal hydrophilic blocks (MeOx). Researchers made a first attempt to resolve the effects of each block on nanoparticle formation. The iPrOx/MeOx ratio dets. the value of the cloud point temperature, whereas the different BuOx-iPrOx blocks determine the character of the process. Finally, a study on the thermodynamic and structural profiles of the complexation between these triblock poly(2-allqrl-2-oxazoline)s and two ionic surfactants was presented. [Pg.508]

Ramakrishnan et al. [19] discussed the effect of block copolymer nano-reinforcements on the low-velocity impact response of sandwich structures. They employed an instrumented drop tower setup for the low-velocity impact tests of the sandwich plates with neat and nano-reinforced epoxy matrix, at different energies. They identified the macroscopic response of the sandwich structure and the microscopic phenomena involved in dissipating the impact energy and compared it for the sandwich plates with (and without) nanoparticles. They evaluated the dynamic response of sandwich composites based on Kevlar fiber reinforced epoxy and Rohacell foam and reported an improvement in impact performance with these sandwich structures that was achieved by the addition of nanoparticles to the resin matrix. In their work an acrylate triblock copolymer that self-assembles in the nanometer scale, called Nanostrength, was added to the epoxy matrix. The effect of the nano-reinforcements on flat sandwich plates undergoing low-velocity impact was investigated at different scales. [Pg.376]

In a related work, a design of enzyme-inspired star block-copolymers with branched topologies and protein-Hke tertiary or quaternary structures was performed. These polymers incorporate hydrophihc, superhydrophobic, and polydentate metal-binding sites and self-assemble in water, their mode of assembly being controlled by the composition of the polymer. An important feature of the star block-copolymers is that they incorporate perfluorocarbons and, due to that, their emulsions in water can attract and preconcentrate O2 in the vicinity of the active metal site. Addition of Cu(II) and TEMPO leads to an effective catalytic system for oxidation of alcohols to aldehydes in water. " ... [Pg.96]

Monte Carlo simulations. Wescott et also applied DPD approaches to investigate the self-assembly of CNT percolating networks in thin films of block copolymer melts. Similarly, Tozzi et al. used particle-level simulations to investigate the stmctural evolution and electrical conductivity of CNT suspensions in shear flow. These approaches can be extended in future work to study the effects of complex interparticle and matrix-induced interactions, as well as the effects of external fields on the network stmcture and electrical properties of composite materials. The synthesis of chemically heterogeneous or Janus particles further motivate these developing techniques. [Pg.331]


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