written by Prof. 
Akira SATOH 
on 1st of January, 
2012
Results between 2006 and 2010
1. 
Self-Organization of Rod-like Hematite Particles ( Cluster-moving 
Monte 
Carlo Simulations) 

We have treated a suspension composed of ferromagnetic rod‑like 
particles with a magnetic
moment normal to the particle axis in order 
to 
investigate the self-organization of these 
particles.
Rod‑like particles tend to aggregate to form raft‑like clusters 
along the magnetic moment direction more significantly as magnetic 
particle‑particle interactions increase.
(a) For the case of no applied 
magnetic field  
(b) For the case where the magnetic 
interaction
between particles is more dominant than the 
applied magnetic 
field (the left-hand-side figure)   
(c) For the case where the applied magnetic field is more 
dominant than the magnetic interaction between particles (the 
right-hand-side figure)   
2.  
Application of the Dissipative Particle Dynamics Method to Magnetic 
Suspensions

Dissipative particles are regarded as fluid particles 
that are 
clusters of real solvent molecules. This modeling enables us 
to 
simulate the dispersed magnetic particles and the dissipative
particles 
simultaneously.  
The chain-like aggregate structures are in 
good agreement with those 
of Monte Carlo and Brownian dynamics 
simulations.  
The dissipative 
particle dynamics method is clearly seen to be a
useful technique as a 
simulation method for magnetic suspensions. 
It is clearly seen from the figure that the results can be 
expressed as a 
universal line by employing the quantity as abscissa, 
proposed in the 
present study.
3. Improvement of the Visibility of Water in Rivers and 
Lakes by Means 
of Applying the Suspension Physics Engineering 

Brownian dynamics simulations have been conducted 
to 
investigate the behavior of two types of spherical
particles, i.e. 
adsorption agent particles (large particles 
in the figure) and suspended 
substance particles (small
particles). 
The present study considers 
the influences of the
diameter ratio of such particles, the random forces 
of
particles due to the Brownian motion, and the thickness
of the initial 
layer of large particles. 
The snapshots at lower positions are obtained 
for
advancing time.  
The performance of removing suspended substance particles 
has a strong relationship with the particle
Brownian motion. 
4. 
Development of the Boundary Model in Lattice Boltzmann Method
for Applying 
It to Magnetic Suspensions (An Equilibrium Linear YMLS
Boundary 
Model) 
 

We 
have conducted the basic study on the lattice Boltzmann method from the 
viewpoint of applying it to magnetic suspensions, by considering a uniform 
flow past a two-dimensional circular particle (i.e., 
cylinder). 
The 
equilibrium linear YMLS boundary model is seen to be available for simulating 
particle suspensions.
The employment of the equilibrium linear YMLS 
boundary model gives rise to 
good agreement with the Navier-Stokes 
results concerning the formation of a
pair of vortices behind 
the cylinder.  
(1) For the case of Reynolds number Re=5 (upper 
figure)
(2) For the case of 
Reynolds number Re=20 (lower 
figure)

The employment of the equilibrium linear YMLS boundary 
model provides the result that the drag coefficient is in 
good
aggreeement with that of the Navier-Stokes equations
even if a coarse 
lattice system is 
used. 
 The length of a pair of 
vortices agrees well with the exact
solution of the Navier-Stokes 
equation. 
5. Behavior of Oblate Hematite Particles on the Material 
Surface for
Application to Surface-Quality-Changing Technology (2D Monte 
Carlo
Simulation of the Phase Transition) 

The 
figure shows the model of a disk-like particle, that is magnetized
in a 
direction normal to the particle direction: we employ 
the disk-like
particle model which is composed of a short cylinder surrounded 
by a
torus part.  
A magnetic field is applied in a direction normal to the 
material surface. 

As the magnetic field increases, 
a phase change 
appears from
column-like (left-hand-side figure)
to brick-wall-like 
(right-hand-
side figure)  
aggregates. 
 
6. Experimental Study on the Characteristics of a Microjet 
in an Electro-
Conjugate Fluid by 2D PIV Analysis 
If a high voltage is applied to a pair of 
electrodes immersed in a certain dielectric fluid, a strong
microjet occurs 
between the electrodes. This is called the electro-conjugate fluid (ECF) effect. 

     By means of a laser-visualization system, a flow 
field
      can be visualized and the digital data 
of the flow field
      is obtained by the PIV 
analysis.  
    
       
In present study, we use a dibutyl decanedioate (DBD) with 98 % 
       purity which is the most typical 
electro-conjugate fluid. This fluid 
       has 
a high boiling point and can be treated straightforwardly 
in
       the experiment. 

    By visualizing, using a laser light, 
the flow 
      field both on the horizontal 
and vertical
      planes, 3D information concerning 
the flow
      field is obtained. 

A microjet appears 
from the right positive electrode toward 
the left negative 
electrode. 
  
(1) For the case of a narrow separation of the 
electrodes
(2) For the case of a wide separation of the 
electrodes

The figure shows the flow 
field on a vertical plane.
The flow is induced from the right 
positive electrode in
an oblique direction (i.e., in the left-down 
direction).  
7. Negative Magneto-Rheological Effect of a Dispersion 
Composed of Spindle-like Hematite 
Particles

    The 
spindle-like hematite particles were synthesized by aging a solution of 
FeCl3 
        and 
KH2PO4 for 72 hours at 
373K.

The measurement of the viscosity was carried out using 
the rotational-type rheometer in an external magnetic 
field generated by 
the Helmholtz 
coils.

The present experiment has 
first verified that the negative
viscosity DOES APPEAR with increasing 
applied magnetic 
field strength. 
(1) For the case of a weak 
shear flow
(2) For the case of a 
strong shear flow
The Negative viscosity 
has been predicted by our theoretical observation and 
the present experiment 
has first verified the appearance of the negative viscosity. 
END.