惰性粒子流化床干燥钻井废泥浆实验研究

实验考察惰性粒子流化床干燥钻井废泥浆,关联了干燥器的体积传热系数表达式,可定量计算进风速度、进风温度、废泥浆体积流量和含水量等参数的影响。结果表明,惰性粒子流化床干燥热效率达55%,体积传热系数可达6kW/(m3.K),可用于钻井现场柴油机废气干燥钻井废泥浆。激光粒度分析仪测试干燥产物粒度平均值为12μm,且分布较为集中,其密度为3.2g/cm3,可以回用于钻井泥浆的加重材料。浸毒试验表明,干燥产物CODcr值大幅度下降。     

惰性粒子流化床干燥器干燥硫酸镁的实验研究

用惰性粒子流化床干燥器对硫酸镁溶液进行干燥。考察了分布板开孔率、惰性粒子直径与装填量、加料量、气体流量、进气温度等操作参数对干燥过程的影响 ,得出了实验条件下的干燥速率、体积传热系数和热效率 ,为工程设计和生产操作提供了参考     

惰性粒子流化床中的悬浮液干燥

用惰性粒子流化床干燥器对混凝土外加剂等5种物料进行了干燥实验研究，提出了计算体积传热系数的关联式．实验结果表明，由于惰性粒子的存在，强化了传热传质，体积传热系数可达3000W·m~(-3)·K~(-1)，但是，床层压力降较高．干燥强度（以蒸出水计）可达50～60kg·m~(-3)·h~(-1)，热效率30％～43％，若提高热风进口温度，后两项指标还可提高.     

液状物料在振动惰性粒子流化床中干燥的研究

以豆浆为物料 ,在振动惰性粒子流化床中研究了进风温度、进风速度、进料量、惰性载体种类对体积传热系数和滞留率的影响 ,分析了床层的热利用率情况 ,提出了计算体积传热系数的经验公式 ,并将振动惰性粒子流化床与普通惰性粒子流化床进行了比较。     

带浸没加热管的惰性粒子振动流化床干燥强度研究

采用带浸没加热管的惰性粒子振动流化床对（石灰）膏状物料干燥进行了实验研究。利用正交实验，考察了加料速率、振动条件、进气温度、进气速度、加热管功率等参数对干燥强度的影响，得出了计算干燥器干燥强度的关联式。结果表明，由于浸没加热管热量的引入，能显著增加干燥器的干燥能力，实验条件下干燥器干燥强度超过250kg·（m^3·h）^-1，干品湿含量可降至1．5％以下，质量能达到要求，相关数据可为膏状物料干燥器的设计和开发提供借鉴。     

膏状物烊惰性粒子流化床中的干燥试验研究

利用４种物烊惰性粒子流化床干燥器中进行性能试验，得出了在试验条件下的容积传热系数、干燥强度及热效率。     

洗衣粉悬浮液在惰性粒子流化床中干燥的研究

针对气体分布板开直孔的惰性粒子流化床,开展了洗衣粉悬浮液在床内的干燥性能研究。测定了流化床的床层压降曲线,考察了进料量、进风温度、进风速度及惰性粒子直径对于流化床传热性能的影响,且与气体分布板开斜孔的传热性能进行了初步比较。结果表明,流化床的床层压降主要是由惰性粒子的流化阻力所致;适当增加进料量和进风速度,或减小惰性粒子直径,以及将气体分布板的孔道由直孔改为斜孔,均可提高流化床的传热性能,但过高的进风温度则可能导致传热性能的下降。     

内热式惰性粒子流化床中膏状物料干燥模型

通过对惰性粒子流化床中膏状物料干燥机理的分析,得到了干燥时间及单位面积床层水分汽化量的数学计算式,可对干燥器的性能进行预测。采用带浸没加热管的惰性粒子流化床对膏状钛白物料进行干燥中试研究,采用气流式喷嘴将膏状物料分散成200～400μm的小液滴喷洒在惰性粒子表面进行干燥,探索了适宜的干燥条件,测定和确定了最佳的干燥工艺参数、操作参数和设备参数。结果表明:该干燥工艺能强化床内传热传质,促进高黏性膏糊状物料很好地分散,床层温度分布均匀,干燥器的操作弹性大,热量消耗低,干燥强度高,传热系数可达300W·m-2·K-1以上。     

惰性粒子振动流化床中膏状物料干燥

报道了采用带浸没加热管的惰性粒子振动流化床干燥膏状物料的实验研究结果。考察了加料速率、振动条件、进气温度、进气速度、加热管功率等参数对干燥过程的影响,提出采用体积传热系数来评价干燥器传热性能,并得出了计算体积传热系数的准数关联式。结果表明,在流化床中增设振动和浸没加热管装置,能大大强化传热、传质,干燥器热效率达60%,干燥强度超过300 kg·m^-3·h^-1,体积传热系数可达25 kW·m^-3·K^-1,激光粒度分析仪的测定结果表明产品的粒度分布范围较窄,该流化床干燥可以直接得到平均粒径为0.35 μm、比表面积为5.024 m²·g^-1的粉状产品。     

液状物料在惰性粒子流化床干燥器中的试验研究

利用两种物料在惰性粒子流化床干燥器中进行性能试验，得出了在试验条件下的容积传热系数，蒸发强度及热效率，并作了经济性评价。     

Measurement of constant drying rate of wet material placed in a fluidized bed of inert particles under reduced pressure

The objective of this study is to estimate the drying characteristics of a relatively large material immersed in a fluidized bed under reduced pressure by measuring the constant drying rate. The constant drying-rate period in a fluidized bed under reduced pressure is difficult to measure because it is extremely short. To maintain the constant drying-rate period, distilled water is directly supplied to the drying material. Through our experiment, the heat transfer coefficient of the material surface was also determined. The results were compared with data on hot air drying. The constant drying rate is higher for fluidized bed drying than for hot air drying. It suggests that the heat transfer coefficient on the surface of the drying material is much larger for fluidized bed drying than for hot air drying. For fluidized bed drying, the effect of pressure in the drying chamber on the heat transfer coefficient is slight at the same normalized mass velocity of dry air (G/G_mf). The temperature difference between the inside of the drying chamber and the drying material is much smaller for fluidized bed drying than for hot air drying. The constant drying rate increases as the pressure in the drying chamber decreases.     

旋流振动流化床干燥性能的研究

文章以聚四氟乙烯粒子和蔗糖为物料研究了旋流振动流化床的流体力学及干燥特性,并与振动流化床的各种特性进行了对比。实验在一个干燥室直径为240 mm的小型圆筒振动流化床中进行,采用斜孔分布板使床内产生旋流。实验结果表明:在空气分布板开孔率相差不多的情况下,物料流化以前,旋流振动流化床的床层压降要大于普通振动流化床,一旦物料达到正常流化状态以后,2种振动流化床的床层压降相差不多;旋流振动流化床可以降低物料的临界含湿质量分数。     

Residence time distribution in spouted bed drying of maltodextrin solutions on a bed of inert particles

Residence time distributions (RTD) for aqueous maltodextrin solutions were determined in two kinds of spouted bed dryers: (1) conventional spouted bed (CSB) 0.305 m diameter with a bed of polypropylene beads and (2) spout‐fluid bed 0.143 m diameter with draft tube submerged in a bed of FEP® pellets (S‐FBDT). RTD, mean residence time t_m, and spread of the distribution σ², were determined at different drying temperatures, spouting velocities, bed depths, spraying pressures, and feed concentrations. Average values of t_m and σ² were 6.5 min and 26.6 min² for the CSB and 6.9 min and 36 min² for the S‐FBDT, respectively, for all operating conditions except spraying pressure. RTD curves were well represented by the response of an ideal stirred tank with a superimposed bypass of 15% on average for the CSB and 7% on average for the S‐FBDT dryer for all operating conditions. Increase in spraying pressure produced a reduction of t_m and an increase in the bypass fraction of the product in both dryers. © 2011 Canadian Society for Chemical Engineering     

带浸没管的惰性粒子振动流化床传热特性

采用带浸没加热管的惰性粒子振动流化床对膏状物料干燥进行了实验研究。考察了加料速率、进气温度、进气速度、加热管功率、振动强度等参数对床温和体积传热系数的影响,得出了计算体积传热系数的关联式。结果表明,在流化床中增设振动和浸没加热管装置,能大大强化传热传质,体积传热系数随加料量、振动强度、加热管功率、进风速度的增加而增大,随进气温度的增加而减小。其结果对惰性粒子流化床干燥器的设计和改进具有重要的指导意义。     

卧式沸腾干燥床在PVC生产中的应用

简单介绍了卧式沸腾干燥床干燥工艺的工艺流程及特点,比较了目前PVC生产中的几种干燥工艺,分析了卧式沸腾干燥床在实际生产中存在的问题及改进措施。     

From hygroscopic single particle to batch fluidized bed drying kinetics

A new normalization concept for convective drying of hygroscopic particulates is introduced. Both, intraparticle drying kinetics and sorption equilibrium are considered separately, and integrated into a new heterogeneous fluid bed model for coupled heat and mass transfer. Experiments were carried out using spherical γ-Al₂O₃ particles. Sorption isotherms, as well as drying curves, for single particles and fluidized beds have been measured. Batch fluid bed drying curves appear to be predictable on the basis of single particle and material equilibrium data and with the help of the model. All model parameters are directly taken, or estimated from fluidization literature, without any fitting.     

Attrition of Victorian brown coal during drying in a fluidized bed

Analyzing the attrition of Victorian brown coal during air and steam fluidized bed drying, the change in particle size distribution over a range of initial moisture contents (60% to 0%) and residence times (0 to 60 minutes) was determined. Dried at a temperature of 130°C with a fluidization velocity 0.55 m/s and an initial particle size of 0.5–1.2 mm, both fluidization mediums show a shift in the particle size distribution between three and four minutes of fluidization, with a decrease in mean particle size from 665 µm to around 560 µm. Using differential scanning calorimetry (DSC), the change in particle size has been attributed to the transition between bulk and non-freezable water (approximately 55% moisture loss) and can be linked to the removal of adhesion water, but not to fluidization effects. This is proved through the comparison of air fluidized bed drying, steam fluidized bed drying, and fixed bed drying—the fixed bed drying is being used to determine the particle size distribution as a function of drying. The results show the three drying methods produce similar particle size distributions, indicating that both fluidization and fluidization medium have no impact upon the particle size distribution at short residence times around ten minutes. The cumulative particle size distribution for air and steam fluidized bed dried coal has been modeled using the equation P_d = A₂ + (A₁ ? A₂)/(1 + (d/x₀)^p), with the resultant equations predicting the effects of moisture content on the particle size distribution. Analyzing the effect of longer residence times of 30 and 60 minutes, the particle size distribution for steam fluidized bed dried coal remains the same, while air fluidized bed dried coal has a greater proportion of smaller particles.