2003
DOI: 10.1016/s1383-7303(03)80029-7
|View full text |Cite
|
Sign up to set email alerts
|

What Kinds of Molecular-Microsimulation Methods are Useful for Colloidal Dispersions ?

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
1
1

Citation Types

0
78
0
4

Year Published

2009
2009
2023
2023

Publication Types

Select...
8

Relationship

0
8

Authors

Journals

citations
Cited by 37 publications
(87 citation statements)
references
References 2 publications
0
78
0
4
Order By: Relevance
“…From figure 3(a), it is found that the magnetic force, namely, the gradient of potential U (H ) , is very small at the central area used in this simulation. The chainlike alignments obtained in this simulation are very long just as ferromagnetic particles in a ferrofluid form chainlike clusters, as determined by numerical simulation with a uniform magnetic field [16]. As discussed in section 4.1.1, we expected to control the cluster speed by selecting media with various viscosities.…”
Section: Simulation For Smaller Particlesmentioning
confidence: 81%
“…From figure 3(a), it is found that the magnetic force, namely, the gradient of potential U (H ) , is very small at the central area used in this simulation. The chainlike alignments obtained in this simulation are very long just as ferromagnetic particles in a ferrofluid form chainlike clusters, as determined by numerical simulation with a uniform magnetic field [16]. As discussed in section 4.1.1, we expected to control the cluster speed by selecting media with various viscosities.…”
Section: Simulation For Smaller Particlesmentioning
confidence: 81%
“…If a single colloidal particle is moving in a quiescent flow field, the translational motion of the particle can be described by the following Langevin equation (Allen and Tildesley, 1987;Satoh, 2003):…”
Section: Methods For Activating the Particle Brownian Motion Based On mentioning
confidence: 99%
“…F is the force acting on the particle which is the sum of the magnetic force described below and F (B) is the random force inducing the particle Brownian motion. For the case of a single-moving particle, this force is required to satisfy the following stochastic characteristic (Satoh, 2003): (8) in which I is the unit tensor, δ is Dirac's delta function, k is Boltzmann's constant, and T is the system temperature. The quantity ξ (t) is the translational friction coefficient expressed as expressed as ξ (t) =3πηD 0 (Brenner, 1974), in which η is the viscosity of a base liquid and D 0 is the particle diameter.…”
Section: Methods For Activating the Particle Brownian Motion Based On mentioning
confidence: 99%
See 1 more Smart Citation
“…(2), the quantities with superscript * are dimensionless, and ξ and Pe are the non-dimensional parameters representing the strengths of the magnetic particle-field interaction and the viscous shear force relative to random force (or thermal energy), respectively; Pe is called the Peclet number. X C , Y C and Y H are resistance functions specifying the resistance coefficients (Satoh, 2003b). The above-mentioned non-dimensional parameters are expressed as…”
Section: Basic Equation Of the Orientational Distribution Function Ofmentioning
confidence: 99%