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陶瓷膜孔道內塵粒沉積及脫附的模擬

Numerical simulation of the fouling and cleaning of a ceramic membrane

  • 摘要: 陶瓷膜是過濾高溫含塵煙氣最有效的材料之一,其過濾性能和再生性能與塵粒在陶瓷膜孔道內的沉積和脫附機制相關。本文建立了不同孔隙率的陶瓷膜物理模型,然后結合連續性方程、動量方程和能量方程,設定邊界條件以及沉積條件,模擬了陶瓷膜過濾和脈沖反吹時,高溫煙氣的流動以及塵粒的沉積與脫附過程。結果表明,過濾速度較低和陶瓷膜孔隙率較高時,塵粒易于沉積在陶瓷膜孔道內;脈沖反吹時,增加反吹壓力,延長反吹時間,塵粒易于從陶瓷膜孔道脫附。采用厚度為20 mm,長度為1.5 m,孔隙率為40%的陶瓷膜管過濾溫度為1000 ℃,流速為1 m·min?1,壓力為0.1 MPa的含塵煙氣時,反吹氣壓力應不低于0.3 MPa,反吹時間不短于0.02 s,塵粒脫附時間在13 s,脈沖反吹時間間隔應高于452 s。

     

    Abstract: The main sources of fine particulate matter in the air are automobile exhaust and dust-containing hot flue gas emitted from combustion in the process of industrial manufacturing and municipal solid waste incineration, both of which are hard to clean at high temperatures. Ceramic membranes maintain high strength at high temperatures and an acid or alkaline atmosphere, and have a micron-scale and tortuous pores that block dust particles. The ceramic membrane is one of the most effective materials for successful hot flue gas cleaning as used in the integrated gasification combined cycle. Its filtration and regeneration performance are related to the deposition and desorption mechanism of dust particles in the channel of the membrane. In this study, a physical model of ceramic membranes of various porosities was established. Boundary and deposition conditions were then set up by combining continuity, momentum, and energy equations to simulate the flow of hot flue gas and the deposition and desorption process of dust particles during ceramic membrane filtration and pulse back-blowing. The results show that when the filtration velocity is low and porosity of the ceramic membrane is high, it is easy for dust particles to deposit in the membrane channel. Increasing back-blowing pressure prolongs back-blowing time during pulse back-blowing so that dust particles easily desorb from the channel of the ceramic membrane. When a ceramic membrane tube with a thickness of 20 mm, a length of 1.5 m, and a porosity of 40% is used to filtrate flue gas with a filtration temperature of 1000 °C, a flow rate of 1 m·min?1, and a pressure of 0.1 MPa, the blowback pressure should not be <0.3 MPa, blowback time should be longer than 0.02 s, and pulse blowback time interval should be more than 452 s.

     

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