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  • 學位論文

非牛頓流體之液固磁流體化床中不同區域內軸向分散行為之分析

The study of axial dispersion behavior of non-Newtonian fluid at various flow regimes in a liquid-solid magnetofluidized bed

指導教授 : 呂理平

摘要


本論文在探討有外加磁場作用下,液、固流體化床之流動模式、分散行為與傳統液、固流體化床之差異。流體化床採用內徑0.05 m高約0.75 m壓克力管,固相以平均粒徑274 μm之鐵粒子為磁性粒子,液相為水及濃度分別為0.03 wt%、0.1 wt%與0.2 wt%之CMC(carboxymethyl cellulose)溶液。床體外部利用漆包線纏繞成的兩螺線管來產生穩定的軸向磁場,使其作用於床體內部之粒子。利用壓力轉換器測量所得之單點壓力降對流體速度之曲線圖,來界定各流態間轉變之速度。並且利用追蹤劑技術分析不同流態區域下的軸向分散情況。   單點壓降實驗中,藉由Leva法所得鐵砂粒子之最小流體化速度Umf(L)並不會受磁場強度影響;而以Davidson and Harrison法所得之最小流體化速度Umf(DH)則會隨磁場強度上升而增加。磁滯現象的形成即可決定移轉速度Ut(P),且隨著磁場強度上升而增加。 實驗結果顯示液、固磁流體化床共有四種不同流域,分別為固定床區、過渡區、磁穩定區和不穩定區;由低流速至高流速區分,其間之分隔分別是最小流體化速度Umf(L)、最小流體化速度Umf(DH)與移轉速度Ut(P)。當CMC溶液濃度上升,固定床區、過渡區與磁穩定區的範圍將隨之縮小,而不穩定區即相對擴大。 在軸向分散行為方面,軸向分散係數會隨流體速度上升而增加,而磁流體化床相較傳統流體化床有著較低之軸向分散係數。在使用水(Newtonian)或CMC(non-Newtonian)溶液的磁流體化床中,其軸向分散係數均隨磁場強度增加而下降。此外,磁場影響軸向分散係數的效果隨著CMC溶液濃度提升而逐漸減弱。

並列摘要


In this study, the difference of hydrodynamic and dispersion behavior between the liquid-solid magneto-fluidized (0.05 m i.d. × 0.075 m height) bed and the liquid-solid traditional fluidized bed was investigated. The sphere iron particles of 274 μm average diameter were used as the solid phase, water and CMC (carboxymethyl cellulose) (0.03 wt%, 0.1 wt% and 0.2 wt%) solution were used as the liquid phase. A magnetic solenoid coiled by the magnet wire was applied to generate axially magnetic field. The dependency of pressure drop on the velocity was used to establish transition velocities between various regimes. The axial dispersion of various regimes was analyzed by the tracer input-response technique. By Leva’s method, the minimum fluidization velocity Umf(L) was not affect by magnetic force. However, by Davidson and Harrison’s method, the minimum fluidization velocity Umf(DH) was increased with increasing magnetic field intensity. Further more, the transition velocity Ut(P) determined by the hysteresis phenomenon was increased with increasing magnetic field intensity. The experimental results show that there were four flow regimes in a magneto-fluidized bed: fixed bed, transition, magnetically stabilized and unstable regime. The boundaries were minimum fluidization velocity Umf(L), minimum fluidization velocity Umf(DH) and transition velocity Ut(P). When the concentration of the CMC solution increased, the range of fixed bed, transition and magnetically stabilized regime was narrowed down, the unstable regime was enlarged. Both in the magnetic and the traditional fluidized beds, the axial dispersion coefficient was increased with the enhancing fluid velocity. The axial dispersion coefficient of the magnetic fluidized bed was lower than the traditional fluidized bed. The dispersion coefficient of the water (Newtonian) and the CMC solutions (non-Newtonian) both were decreased with the enhancing magnetic field intensity. Besides, the effect of magnetic field on the dispersion coefficient was decreased with the increasing concentration of CMC solution.

參考文獻


Albert, R. V. and C. Tien, “Particle Collection in Magnetically Stabilized Fluidized Filters”, AIChEJ., 31, 288-295 (1985).
Arnaldos, J., J. Casal and L. Puigjaner, “Le Lit Fluidise Stabilise Magnetiquement: Characterisiques et Possibilities D’application”, Powder Technol., 36, 33-38 (1983).
Arnaldos, J., J. Casal, A. Lucas and L. Puigjaner, “Magnetically Stabilized Fluidization: Modelling and Application to Mixtures”, Powder Technol., 44, 57-62 (1985).
Brea, F. M., M. F. Edwards and W. L. Wilkinson, “The Flow of Non-Newtonian Slurries Through Fixed and Fluidised Beds”, Chem. Eng. Sci., 31, 329-336 (1976).
Burns, M. A. and D. J. Graves, “Continuous Affinity Chromatography Using a Magnetically Fluidized Stabilized Bed”, Biotechnol. Prog., 1, 95-103 (1985).

被引用紀錄


盧廷政(2008)。氣、液、固三相磁流體化床(生物流體化床)中質傳與流力行為之探討〔碩士論文,國立臺灣大學〕。華藝線上圖書館。https://doi.org/10.6342/NTU.2008.00840

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