2014
DOI: 10.1016/j.ijnonlinmec.2014.09.017
|View full text |Cite
|
Sign up to set email alerts
|

Mechanical modeling of rheometer experiments: Applications to rubber and actin networks

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1

Citation Types

0
3
0

Year Published

2014
2014
2016
2016

Publication Types

Select...
3
1

Relationship

0
4

Authors

Journals

citations
Cited by 4 publications
(3 citation statements)
references
References 36 publications
(86 reference statements)
0
3
0
Order By: Relevance
“…Owing to the existent barriers to link the phenomena between different length and time scales, reviews on cross-linked networks were performed. 153,157,158 Regarding the molecular level, the mathematical formulations 159 usually cannot be directly visualised by the current experimental techniques and, while Mikado models are capable to capture protein unfolding and cross-linker kinetics on the network requiring high computational costs, the continuum models loose microstructural information because they involve an homogenisation of the actin filaments properties.…”
Section: Passive Behaviourmentioning
confidence: 99%
“…Owing to the existent barriers to link the phenomena between different length and time scales, reviews on cross-linked networks were performed. 153,157,158 Regarding the molecular level, the mathematical formulations 159 usually cannot be directly visualised by the current experimental techniques and, while Mikado models are capable to capture protein unfolding and cross-linker kinetics on the network requiring high computational costs, the continuum models loose microstructural information because they involve an homogenisation of the actin filaments properties.…”
Section: Passive Behaviourmentioning
confidence: 99%
“…Away from equilibrium, we have found that this simple one-dimensional model has an elaborate steady-state phase diagram with transitions between different flowing phases. By choosing to represent the (x, y)-plane perpendicular to the direction of the 1D lattice, we can compare the model's local angular velocity with the rotation flow profile of a fluid in a parallel-plate rheometer [17,18]. Of course, our model is not truly three-dimensional like the fluid in a rheometric experiment, but it has many of the same features, including microscopic internal interactions, a macroscopic steady-state flow profile and shear rate, energy exchange, conserved angular momentum and torque propagation.…”
Section: Introductionmentioning
confidence: 99%
“…Hamilton's equations are recovered in the conservative case T = µ = 0. Although the model is insensitive to absolute rotational velocities, we can drive it into a non-equilibrium steady state by rotating one of its boundaries relative to the other (as in a parallel-plate rheometer shearing a sample of fluid [20][21][22]). To impose periodic boundary conditions whilst also applying a relative torque across the system, rotors at opposite ends of the chain are designated as neighbours, but see each other through an angular offset that increases at a constant angular velocity.…”
mentioning
confidence: 99%