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 b
rick-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.





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