Linear Viscoelastic Predictions Using a Single-Chain Mean-field Discrete Slip-link Model

2010 ◽  
Author(s):  
Tanya L. Chantawansri ◽  
Yelena R. Sliozberg ◽  
Jan W. Andzelm
2008 ◽  
Author(s):  
Jay D. Schieber ◽  
Renat Khaliullin ◽  
Albert Co ◽  
Gary L. Leal ◽  
Ralph H. Colby ◽  
...  

2009 ◽  
Vol 42 (19) ◽  
pp. 7504-7517 ◽  
Author(s):  
Renat N. Khaliullin ◽  
Jay D. Schieber

Materials ◽  
2021 ◽  
Vol 14 (4) ◽  
pp. 778
Author(s):  
Yingli Niu ◽  
Xiangyu Bu ◽  
Xinghua Zhang

The application of single chain mean-field theory (SCMFT) on semiflexible chain brushes is reviewed. The worm-like chain (WLC) model is the best mode of semiflexible chain that can continuously recover to the rigid rod model and Gaussian chain (GC) model in rigid and flexible limits, respectively. Compared with the commonly used GC model, SCMFT is more applicable to the WLC model because the algorithmic complexity of the WLC model is much higher than that of the GC model in self-consistent field theory (SCFT). On the contrary, the algorithmic complexity of both models in SCMFT are comparable. In SCMFT, the ensemble average of quantities is obtained by sampling the conformations of a single chain or multi-chains in the external auxiliary field instead of solving the modified diffuse equation (MDE) in SCFT. The precision of this calculation is controlled by the number of bonds Nm used to discretize the chain contour length L and the number of conformations M used in the ensemble average. The latter factor can be well controlled by metropolis Monte Carlo simulation. This approach can be easily generalized to solve problems with complex boundary conditions or in high-dimensional systems, which were once nightmares when solving MDEs in SCFT. Moreover, the calculations in SCMFT mainly relate to the assemble averages of chain conformations, for which a portion of conformations can be performed parallel on different computing cores using a message-passing interface (MPI).


2016 ◽  
Vol 145 (22) ◽  
pp. 224902 ◽  
Author(s):  
F. Léonforte ◽  
U. Welling ◽  
M. Müller

2014 ◽  
Vol 16 (1) ◽  
pp. 015027 ◽  
Author(s):  
Rudi J A Steenbakkers ◽  
Christos Tzoumanekas ◽  
Ying Li ◽  
Wing Kam Liu ◽  
Martin Kröger ◽  
...  

2004 ◽  
Vol 37 (3) ◽  
pp. 1124-1133 ◽  
Author(s):  
Josep Bonet Avalos ◽  
Allan D. Mackie ◽  
Silvia Díez-Orrite

2014 ◽  
Vol 11 (92) ◽  
pp. 20130884 ◽  
Author(s):  
Raghunath Chelakkot ◽  
Arvind Gopinath ◽  
L. Mahadevan ◽  
Michael F. Hagan

We show that active, self-propelled particles that are connected together to form a single chain that is anchored at one end can produce the graceful beating motions of flagella. Changing the boundary condition from a clamp to a pivot at the anchor leads to steadily rotating tight coils. Strong noise in the system disrupts the regularity of the oscillations. We use a combination of detailed numerical simulations, mean-field scaling analysis and first passage time theory to characterize the phase diagram as a function of the filament length, passive elasticity, propulsion force and noise. Our study suggests minimal experimental tests for the onset of oscillations in an active polar chain.


Soft Matter ◽  
2006 ◽  
Vol 2 (7) ◽  
pp. 573-583 ◽  
Author(s):  
Kostas Ch. Daoulas ◽  
Marcus Müller ◽  
Juan J. de Pablo ◽  
Paul F. Nealey ◽  
Grant D. Smith

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