Blanket Dynamics in Upflow Suspended Bed
碩士 === 國立臺灣大學 === 化學工程學研究所 === 91 === A one-dimensional model for the spatio-temporal variation of solids fraction in the blanket considering both the hydrodynamic dispersion and the convection effects was proposed in this study. The model equation was a wave equation whose solution presented shock-...
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ndltd-TW-091NTU000630762016-06-20T04:15:20Z http://ndltd.ncl.edu.tw/handle/74855700530712755782 Blanket Dynamics in Upflow Suspended Bed 向上流動懸浮流體床之泥毯動態研究 Shu Hsin Tuan 蘇信團 碩士 國立臺灣大學 化學工程學研究所 91 A one-dimensional model for the spatio-temporal variation of solids fraction in the blanket considering both the hydrodynamic dispersion and the convection effects was proposed in this study. The model equation was a wave equation whose solution presented shock-wave like characteristic. The model output predicted that the distribution of the solids fraction in the blanket would firstly evolve to a uniform distribution at a lower solids fraction. Afterward the blanket would compact itself to another uniform distribution at a higher solids fraction. Experimental works with synthetic raw water coagulated with PACl suspended in a lab-scale suspended bed confirmed the theoretical predictions. The solids flux plot was constructed with underdosed, optimal, and overdosed suspensions. Change in coagulant dose would affect the blanket height and the response time. The solids flux curve was shifted accordingly. The “optimal’ operational condition for the upflow suspended bed that produced the lowest effluent turbidity was discussed. D J Lee 李篤中 2003 學位論文 ; thesis 40 zh-TW |
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碩士 === 國立臺灣大學 === 化學工程學研究所 === 91 === A one-dimensional model for the spatio-temporal variation of solids fraction in the blanket considering both the hydrodynamic dispersion and the convection effects was proposed in this study. The model equation was a wave equation whose solution presented shock-wave like characteristic. The model output predicted that the distribution of the solids fraction in the blanket would firstly evolve to a uniform distribution at a lower solids fraction. Afterward the blanket would compact itself to another uniform distribution at a higher solids fraction. Experimental works with synthetic raw water coagulated with PACl suspended in a lab-scale suspended bed confirmed the theoretical predictions. The solids flux plot was constructed with underdosed, optimal, and overdosed suspensions. Change in coagulant dose would affect the blanket height and the response time. The solids flux curve was shifted accordingly. The “optimal’ operational condition for the upflow suspended bed that produced the lowest effluent turbidity was discussed.
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author2 |
D J Lee |
author_facet |
D J Lee Shu Hsin Tuan 蘇信團 |
author |
Shu Hsin Tuan 蘇信團 |
spellingShingle |
Shu Hsin Tuan 蘇信團 Blanket Dynamics in Upflow Suspended Bed |
author_sort |
Shu Hsin Tuan |
title |
Blanket Dynamics in Upflow Suspended Bed |
title_short |
Blanket Dynamics in Upflow Suspended Bed |
title_full |
Blanket Dynamics in Upflow Suspended Bed |
title_fullStr |
Blanket Dynamics in Upflow Suspended Bed |
title_full_unstemmed |
Blanket Dynamics in Upflow Suspended Bed |
title_sort |
blanket dynamics in upflow suspended bed |
publishDate |
2003 |
url |
http://ndltd.ncl.edu.tw/handle/74855700530712755782 |
work_keys_str_mv |
AT shuhsintuan blanketdynamicsinupflowsuspendedbed AT sūxìntuán blanketdynamicsinupflowsuspendedbed AT shuhsintuan xiàngshàngliúdòngxuánfúliútǐchuángzhīnítǎndòngtàiyánjiū AT sūxìntuán xiàngshàngliúdòngxuánfúliútǐchuángzhīnítǎndòngtàiyánjiū |
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