Thermodynamics and Kinetics of Defect Motion and Annihilation in the Self-Assembly of Lamellar Diblock Copolymers

2016 ◽  
Vol 49 (16) ◽  
pp. 6126-6138 ◽  
Author(s):  
Weihua Li ◽  
Marcus Müller
Soft Matter ◽  
2020 ◽  
Vol 16 (26) ◽  
pp. 6056-6062 ◽  
Author(s):  
Xianggui Ye ◽  
Bamin Khomami

Large-scale dissipative particle dynamics (DPD) simulations have been performed to investigate the self-assembly of over 20 000 linear diblock copolymer chains in a selective solvent.


2012 ◽  
Vol 136 (23) ◽  
pp. 234905 ◽  
Author(s):  
Poornima Padmanabhan ◽  
Francisco J. Martinez-Veracoechea ◽  
Juan C. Araque ◽  
Fernando A. Escobedo

Soft Matter ◽  
2015 ◽  
Vol 11 (22) ◽  
pp. 4366-4374 ◽  
Author(s):  
Dan Mu ◽  
Jian-Quan Li ◽  
Sheng-Yu Feng

We designed twelve types of weak polyelectrolytes (i.e., PEO-b-PMMA copolymers (BCP) in multi-arm structures, where six include EO blocks as joint points and the other six have MMA blocks as joint points). Of these, six are displayed; structures with EO blocks as joint points on the left, and those with MMA blocks as joint points on the right.


Nanoscale ◽  
2012 ◽  
Vol 4 (20) ◽  
pp. 6574 ◽  
Author(s):  
Kun Liu ◽  
Cristina Resetco ◽  
Eugenia Kumacheva

1981 ◽  
Vol 197 (2) ◽  
pp. 309-314 ◽  
Author(s):  
J S Davis

The self-assembly of myosin monomer into thick filament occurs via a two-step mechanism. At first a pair of myosin monomers reacts to form a parallel dimer; the dimer in turn adds to the filament ends at a rate that is independent of filament length. The rate of the dissociation reaction on the other hand is length-dependent. The ‘off’ rate constant has been shown to increase exponentially by a factor of 500 as the filament grows from the bare-zone out to its full length. The length of the filament is thus kinetically controlled; myosin is added to the filament at a fixed rate, whereas the dissociation rate increases to a point where equilibrium is established and the filament ceases to grow. The structural implications implicit in the mechanism are discussed.


2012 ◽  
Vol 79 (5) ◽  
Author(s):  
Asha Nurse ◽  
L. B. Freund ◽  
Jacquelyn Youssef

Observation of the self-assembly of clusters of cells in three dimensions has raised questions about the forces that drive changes in the shape of the cell clusters. Cells that self-assemble into a toroidal cluster about the base of a conical pillar have been observed in the laboratory to spontaneously climb the conical pillar. Assuming that cell cluster reorganization is due solely to surface diffusion, a mathematical model based on the thermodynamics of an isothermal dissipative system is presented. The model shows that the cluster can reduce its surface area by climbing the conical pillar, however, this is at the expense of increasing its gravitational potential energy. As a result, the kinetics of the climb are affected by parameters that influence this energy competition, such as the slope of the conical pillar and a parameter of the model κ that represents the influence of the surface energy of the cluster relative to its gravitational potential energy.


2021 ◽  
Author(s):  
Zsombor Miskolczy ◽  
Mónika Megyesi ◽  
Stephan Sinn ◽  
Frank Biedermann ◽  
Laszlo Biczok

Very few information is available for the kinetics of the self-assembly and dissociation of optically silent building blocks despite the importance of such data in the rational design of tailor-made...


2015 ◽  
Vol 6 (39) ◽  
pp. 7015-7026 ◽  
Author(s):  
Anton H. Hofman ◽  
Gert O. R. Alberda van Ekenstein ◽  
Albert J. J. Woortman ◽  
Gerrit ten Brinke ◽  
Katja Loos

Evaluation of the Flory-Huggins interaction parameter confirmed the self-assembly of a series of RAFT-synthesized poly(4-vinylpyridine)-block-poly(N-acryloylpiperidine) diblock copolymers.


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