• 検索結果がありません。

鹿児島大学リポジトリ

N/A
N/A
Protected

Academic year: 2021

シェア "鹿児島大学リポジトリ"

Copied!
2
0
0

読み込み中.... (全文を見る)

全文

(1)

Effects of gas properties on bubble behaviors

in fluidized catalyst beds

著者

ETO Keita, KAI Takami, NAKAZATO Tsutomu

journal or

publication title

The Research Reports of the Faculty of

Engineering, Kagoshima University

volume

58

page range

66-66

year

2017-03

(2)

2015 Taiwan/Korea/Japan Joint Meeting on Chemical Engineering, November 5-7, 2015, E-DA Royal Hotel, Kaohsiung, Taiwan

Effects of gas properties on bubble behaviors in fluidized catalyst beds

Keita ETO, Takami KAI, Tsutomu NAKAZATO

Department of Chemical Engineering, Kagoshima University, Kagoshima 890-0065, Japan

Abstract

Bubble size is an important parameter for the reactor model of fluidized beds. Therefore, many researchers have measured bubble size and proposed the equations to predict bubble size (Karimipour and Pugsley, 2011). However, almost all the measurements were carried out using air at ambient temperature, and so the proposed equations ignore the influence of the gas properties such as density and viscosity. As the results, these equations cannot correctly predict the bubble size in fluidized catalyst beds. It has been reported that bubble size is affected by the apparent viscosity of the emulsion phase (Kai et al., 1987b). In addition, the emulsion phase voidage is greater than that at minimum fluidization for the fluidized bed with fine particles, and the apparent viscosity decreased with an increase of the voidage (Kai et al., 1991). Furthermore, because the emulsion phase voidage is affected by the gas properties (Kai et al., 1987a), hence the gas properties affect the bubble size in the fluidized catalyst beds. In this study, the expansion ratio of the emulsion phase and bubble size were measured in a two-dimensional fluidized bed. Five types of gases were used as the fluidizing gas; argon, helium, carbon dioxide, nitrogen and hydrogen. The measurement was carried out using two optical probes, and the bubble size was calculated from the signals from these probes.

The emulsion phase voidage was strongly affected by gas viscosity. The voidage was high for high viscosity gas. The bubble size was small

for high viscosity gas, while was large for low viscosity gas such as hydrogen. The binarized images of the beds fluidized by argon gas and hydrogen gas are shown in Figure 1. This figure indicates that the bubble size were affected by the type of fluidizing gas. The relationship between the apparent viscosity of the emulsion phase and bubble size was obtained using the correlation of the apparent viscosity considering the emulsion phase voidage. The relationship agreed with the theoretical formula introduced by Kurooka et al. (2008).

References

Kai, T., A. Iwakiri, T. Takahashi, Emulsion phase expansion and sedimentation velocity in fluidized beds of fine particles, J. Chem. Eng. Japan 20 (1987a) 282–286.

Kai, T., Y. Shirakawa, T. Takahashi, S. Furusaki, Change in bubble behavior for different fluidizing gases in a fluidized bed, Powder Technol., 51, 267–271 (1987b).

Kai, T., M. Murakami, K. Yamasaki, T. Takahashi, Relationship between apparent viscosity and fluidization quality in a fluidized bed with fine particles, J. Chem. Eng. Japan, 24, 494–500 (1991).

Karimipour, S., T. Pugsley, A critical evaluation of literature correlations for predicting bubble size and velocity in gas–solid fluidized beds, Powder Techonl. 205, 1–14 (2011).

Kurooka, T., R. Yamazaki, G. Liu, Hydrodynamics of gas-solid fluidized bed of fine particles and two phase theory, Kagaku Kogaku Ronbunshu, 34, 571–579 (2008).

(a) Ar (UG=3.16, 6.95, 10.5 cm s−1) (b) H2 (UG=2.97, 6.67, 9.71 cm s−1) Fig. 1 Binarized images of 2D bed fluidized by (a) Ar and (b) H2.

参照

関連したドキュメント

Indeed, if we use the indicated decoration for this knot, it is straightforward if tedious to verify that there is a unique essential state in dimension 0, and it has filtration

In Section 3, we show that the clique- width is unbounded in any superfactorial class of graphs, and in Section 4, we prove that the clique-width is bounded in any hereditary

Theorem 4.8 shows that the addition of the nonlocal term to local diffusion pro- duces similar early pattern results when compared to the pure local case considered in [33].. Lemma

In this paper, under some conditions, we show that the so- lution of a semidiscrete form of a nonlocal parabolic problem quenches in a finite time and estimate its semidiscrete

Hong: Asymptotic behavior for minimizers of a Ginzburg-Landau type functional in higher dimensions associated with n-harmonic maps, Adv. Yuan: Radial minimizers of a

Kilbas; Conditions of the existence of a classical solution of a Cauchy type problem for the diffusion equation with the Riemann-Liouville partial derivative, Differential Equations,

Analogs of this theorem were proved by Roitberg for nonregular elliptic boundary- value problems and for general elliptic systems of differential equations, the mod- ified scale of

Then it follows immediately from a suitable version of “Hensel’s Lemma” [cf., e.g., the argument of [4], Lemma 2.1] that S may be obtained, as the notation suggests, as the m A