流化床內(nèi)固液兩相流特性及底板布孔優(yōu)化的模擬研究
[Abstract]:With the development of economy and society, environmental problems have become one of the most important problems that restrict the development of our society. In many environmental problems, water pollution is the most prominent and serious problem. In particular, the rapid development of the city has produced a large number of domestic sewage, and most of these domestic sewage are not treated directly to the water in the natural world. In the body, it has caused serious pollution to the environment of rivers, lakes and oceans. It is very difficult to restore to the natural state. Water resources in our country are not rich, and the pollution of various water bodies will make the available water resources further reduced, affecting the people's normal life and the production of industry and agriculture. To realize the sustainable benefit of water resources. It is necessary to purify industrial and domestic sewage and develop a complete set of economical and practical sewage treatment equipment and methods. In many sewage treatment methods, the biofilm sewage treatment technology is one of the most important sewage treatment methods because of its convenient operation and low operating cost. This paper uses RNG k- e turbulence. The flow model is combined with the Euler Orla multiphase flow model to simulate a typical fluid flow dynamic fluidized bed. A variety of physical quantities are compared in the opening form of different distributed plates, thus the pore form of a reasonable fluidized bed inlet distribution plate is determined, and the solid volume in the fluidized bed is analyzed under the different carrier properties and operating conditions. The physical parameters such as fraction, flow flow, turbulent kinetic energy and turbulent energy dissipation rate have been determined, and the optimal operating parameters of the fluidized bed are determined. The advantages and disadvantages of different operating conditions are found, so that readers can choose the distribution pattern of distribution plates suitable for their own working conditions according to their needs, the carrier and the operating parameters. Through analysis and comparison, the following conclusions are drawn. (1) through the comparison and analysis of the model verification one, it is found that the Euler Euler multiphase flow model can be used to simulate the solid and liquid two phase flow in the fluidized bed with the RNGk- epsilon turbulence model. Through the model verification, two models of the selected multiphase flow, the turbulence model and its boundary conditions and numerical solution methods are verified, the simulation values and the experiments are carried out. The data are in good agreement, and the mathematical model, numerical solution and boundary condition can be used to simulate the flow characteristics of solid-liquid two-phase flow in the fluidized bed. (2) the carrier particles in the fluidized bed are completely fluidizing in the fluidized bed, forming a homogeneous flow layer, and there is no local flow layer. (2) compared with other forms of carrier distribution plate, the carrier particles are in the fluidized bed. In the high concentration region, the axial concentration fluctuates but is not obvious, the concentration distribution in the fluidized bed is the most uniform. The axial velocity distribution of the carrier is more uniform in the fluidized bed, and the velocity gradient along the axial and radial direction changes little. When the distribution plate A is set up, the distribution of the radial velocity of the carrier is obviously larger than that of the other distribution plates. The maximum radial velocity is 0.17m/s, and the collision and friction between the carrier particles in the radial direction is more intense. (3) in the case of the other initial conditions, the volume fraction and axial velocity of the carrier in the fluidized bed decrease with the increase of the carrier particle size, and the expansion height of the bed layer decreases obviously, the velocity uniformity and the flow state of the fluidized bed are all worse. With the increase of carrier density, the volume fraction of carrier in the fluidized bed becomes larger, the expansion rate and axial velocity of bed layer decrease, the velocity uniformity becomes worse and the flow state becomes unstable. With the increase of the initial filling height of the carrier, the volume fraction of carrier in the fluidized bed is correspondingly larger, the axial velocity decreases, the bed expansion rate has small amplitude fluctuation and the flow velocity is uniform. With the increase of the liquid velocity at the entrance of the fluidized bed, the volume fraction of the carrier in the fluidized bed decreases, the bed expansion rate and the axial velocity are obviously increased and the velocity uniformity becomes worse. (4) the analysis and comparison of the carrier volume fraction in the fluidized bed, the axial velocity distribution of the carrier and the non uniform velocity coefficient of the flow velocity are compared. The density of the body particles is 1500kg/m3, the carrier particle size is 1mm, the initial filling height is 0.3m, and the liquid velocity at the inlet of the fluidized bed is 0.15m/S, which is the best carrier property and operating parameter for the given biological fluidized bed. It is the most favorable for improving the efficiency of the sewage treatment in the fluidized bed.
【學(xué)位授予單位】:西安理工大學(xué)
【學(xué)位級別】:碩士
【學(xué)位授予年份】:2017
【分類號】:X703
【參考文獻】
相關(guān)期刊論文 前10條
1 李松;范曉旭;郭冬彥;初雷哲;王琪;;0.15MW單循環(huán)流化床的稻殼粉氣化實驗研究[J];中國農(nóng)機化學(xué)報;2016年08期
2 劉洪鵬;賈春霞;肖劍波;秦宏;王擎;;65t/h高低差速循環(huán)流化床鍋爐燃燒特性模擬[J];化工機械;2016年03期
3 王紹慶;李志合;李寧;王祥;;可視化鼓泡流化床內(nèi)顆粒流動特性的實驗研究[J];可再生能源;2016年02期
4 孫銘陽;韋魯濱;朱學(xué)帥;李大虎;李陽;;液固分選流化床三相流場模擬中各粘性流動模型的適用性[J];過程工程學(xué)報;2016年01期
5 湯亮;葉方平;龔發(fā)云;郭衛(wèi)林;徐顯金;姚元軍;;流化床中液固物性參數(shù)對流場影響的數(shù)值模擬[J];武漢大學(xué)學(xué)報(工學(xué)版);2016年01期
6 劉燕;陳赫宇;周千淅;張少峰;王智;;液固外循環(huán)流化床內(nèi)噴嘴對流場影響的數(shù)值模擬[J];河北工業(yè)大學(xué)學(xué)報;2016年01期
7 李希;應(yīng)磊;成有為;王麗軍;;甲醇制烯烴多級串聯(lián)流化床反應(yīng)器模擬[J];化工學(xué)報;2015年08期
8 金娟;;生物流化床處理有機廢水的研究現(xiàn)狀[J];輕工科技;2015年07期
9 賀長營;李延鋒;張文軍;趙明輝;李東澤;張遲強;;加重質(zhì)液固流化床流化特性研究[J];煤炭技術(shù);2015年03期
10 馮楊陽;廖延廣;陳英文;沈樹寶;;生物流化床處理廢水的研究進展[J];工業(yè)水處理;2014年10期
,本文編號:2166622
本文鏈接:http://sikaile.net/shengtaihuanjingbaohulunwen/2166622.html