Fictitious particle method: A numerical model for flows including dense solids with large size difference

AIChE Journal ◽  
2014 ◽  
Vol 60 (5) ◽  
pp. 1606-1620 ◽  
Author(s):  
Takuya Tsuji ◽  
Kyohei Higashida ◽  
Yoshitomo Okuyama ◽  
Toshitsugu Tanaka
Author(s):  
Kyohei Higashida ◽  
Teppei Yamada ◽  
Takuya Tsuji ◽  
Toshitsugu Tanaka

In practical application of fluidized beds, large solids coexist with small solids. Tsuji et al. (AIChE J., 60(5), pp. 1606–1620, 2014) proposed a numerical model which expresses the behavior of flows including dense solid objects with large size difference based on the DEM-CFD coupling method. In the present study, the model is extended to represent the non-sphericity of large objects by adding a multi-sphere model. Firstly, we perform validation study in a mm-size bubbling fluidized bed and confirm qualitative agreements between the numerical model and the experiment. After that, sinking and floating motion of a large non-spherical object in a fluidized bed are numerically investigated in detail.


1977 ◽  
Vol 55 (8) ◽  
pp. 1360-1366 ◽  
Author(s):  
Claude Jambon ◽  
Geneviève Delmas

Solution viscosities have been measured at 25 °C on seven I systems of SnR4 compounds: SnBut4 with SnMe4, SnEt4, SnPr4, SnOct4, SnLaur4 and SnLaur4 with SnEt4 and SnPr4. The effect of shape difference on excess solution viscosities was investigated. The experimental value Δ ln ηexp = ln ηs − x1 ln η1 − x2 ln η2 was compared to Δ ln ηth.Δ ln ηth was obtained using ΔGM(mixing) in place of GM≠(activation) and free volume theories. Experimental heats of mixing have been measured and are used inΔ ln ηth. It was found that with the Van der Waals model for the energy, the difference Δ ln ηexp − Δ ln ηth, indicative of the agreement between the predicted and experimental value, is relatively small for mixtures of molecules not having a large size difference. However, for systems different in size, Δ ln ηexp − Δ ln ηth is positive and large and is shown to be an increasing function of the size difference. Δ ln ηth could be adjusted to Δ ln ηexp by adding a term ln ηΔV* = c(V1*1/2 − V2*1/2)2 where V* is the core volume. To confirm the validity of ln ηΔV*, the seven II systems chosen in order to present a large range (V1*1/2 − V2*1/2) were measured: SnBut4 + squalane, Si(OEt)4 + Si(OOct)4, n-C10 + Si(OOct)4, Si(OEt)4 + squalane, n-C12 + SnOct4, Si(OMe)4 + Si(OOct)4, n-C16 + benzene. A c value of 5.3 × 10−3 cm3 appears to be adequate for all the systems studied in this work. The 'condensation effect' of SnEt4 and SnPr4 observed by calorimetry is possibly seen here in the series SnLaur4 with SnEt4, SnPr4, SnBut4.


Author(s):  
Koji Nakaya ◽  
Shuhei Nishimaki ◽  
Osamu Mori ◽  
Jun’Ichiro Kawaguchi

This paper discusses dynamics of large membrane for achieving spinning solar sail-craft proposed by the Institute of Space and Astronautical Science (ISAS), Japan Aerospace Exploration Agency (JAXA). For comprehending the dynamics, firstly, two types of grand-scale experiments were conducted. One was an ice rink experiment. The other was a balloon experiment. In the both experiments, we succeeded in deploying 10m and 20m diameter membrane and observing the motion. Secondly, we constructed a numerical model using a multi-particle method, and numerical simulations were conducted. We drew a comparison between results of experiments and numerical simulations. The effectively of the multi-particle model was then indicated in this paper.


2019 ◽  
Vol 2 (1) ◽  
pp. 524-531
Author(s):  
Władysław Hamiga ◽  
Wojciech Ciesielka

Abstract This paper presents simulation studies on the aerodynamics of vehicles moving in an organized column. The object of research is a column that consist of three vehicles of the same type (homogeneous column). In this research geometry of Ford Transit was used. As a part of the studies, the air drag forces acting on individual vehicles were calculated. The results are presented in dimensionless drag coefficient. The influence of the distance between cars on the generated force was also determined. In the first stage of the work, a numerical model was developed based on the Ahmed body reference structure. The calculations were carried out for 9 different velocities. The obtained results of the drag coefficient were compared with the work of other authors. The applied turbulence model and parameters of the boundary layer were used to create a numerical model of a moving column of vehicles. Mesh independence for numerical model of van was verified. The Finite Volume Method was implemented in the ANSYS Fluent program and used for the calculations. The use of supercomputers was necessary due to the large size of the grid.


2021 ◽  
Vol 2083 (2) ◽  
pp. 022097
Author(s):  
Minghui Chen ◽  
Qiaorui Wu ◽  
Zhen Zhang ◽  
Huimin Yu ◽  
Ruichang Huang

Abstract This study adopts the numerical simulations of Moving Particle Semi-Implicit Methods (MPS), which are meshless methods based on Lagrange particles. Using Lagrange particle has an advantage that it can avoid numerical dissipation problems without directly discretizing the convection term in the governing equation. First of all, a numerical model of a liquid sloshing tank without baffles is used to confirm the effectiveness of the MPS by comparing the numerical results with the experimental data of Kang and Li. And the pressure curves obtained with MPS method were in good agreement with the experimental findings, which confirmed its effectiveness. On that basis, simulations of liquid sloshing movements with one baffle, two symmetrical baffles, and three baffles are performed, respectively. The results indicate that the addition of vertical baffles in the tanks effectively enhanced the ability to reduce liquid sloshing.


Author(s):  
R. A. Ricks ◽  
Angus J. Porter

During a recent investigation concerning the growth of γ' precipitates in nickel-base superalloys it was observed that the sign of the lattice mismatch between the coherent particles and the matrix (γ) was important in determining the ease with which matrix dislocations could be incorporated into the interface to relieve coherency strains. Thus alloys with a negative misfit (ie. the γ' lattice parameter was smaller than the matrix) could lose coherency easily and γ/γ' interfaces would exhibit regularly spaced networks of dislocations, as shown in figure 1 for the case of Nimonic 115 (misfit = -0.15%). In contrast, γ' particles in alloys with a positive misfit could grow to a large size and not show any such dislocation arrangements in the interface, thus indicating that coherency had not been lost. Figure 2 depicts a large γ' precipitate in Nimonic 80A (misfit = +0.32%) showing few interfacial dislocations.


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