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1.
为了对低温液相甲醇合成反应的模试及进一步的工业应用提供一定的预测和参考,用搅拌釜中得出的低温液相甲醇合成反应的动力学方程,经过合理的反应器模型假设,对低温甲醇合成鼓泡浆态床反应器进行了数学模拟,其中的非线性常微分方程组,采用变步长四阶Runge-Kutta法进行数值计算,结果表明,模试操作条件下对CO转化率和H2转化率的模拟计算结果与实际的模模试值的误差分别为13%和4%,模拟结果与模试实验结果比较相符;对不同条件下的反应速率和转化率进行了模拟预测。  相似文献   

2.
浆态床气泡特性的研究   总被引:1,自引:0,他引:1  
用三种不同直径的浆态鼓泡塔研究气速、塔径、固相浓度、静止床层高度和气体分布器等对气含率的影响。平均气含率随气速变化分为稳定区、过渡区和湍流区,得到各区平均气含率的计算式,其平均误差小于5%。用气隙率仪测定了局部气含率和气泡频率的分布并研究了气泡直径、气泡上升速度和气、液相界面积等,并给出了计算式。  相似文献   

3.
研究了以粉体氧化铝水合物为固相的鼓泡浆液反应器的平均气含率和固体浓度分布特性。考察了表观气速、体系温度、静液高度、固相浓度及气体分布板的开孔率等对气含率的影响和不同性质氧化铝水合物在塔中的悬浮和轴向浓度分布情况。结果表明气速增大或开孔率较大时气含率增大,但固相浓度大小对气含率没有影响。水合氧化铝固体粉末在鼓泡塔中的浓度分布特性与固体的堆积密度和吸水性能有关,吸水率大堆积密度小的拟薄水铝石在低气速条件下就可完全均匀悬浮。以上结果为用气液固三相鼓泡反应器制备晶粒大小均匀的拟薄水铝石提供了可能性。  相似文献   

4.
建立了费托合成鼓泡浆态床反应器双泡模型,通过模型对比的方法模拟讨论了多个反应器模型,双泡模型、全混模型以及多级串联模型,对比模拟讨论了费托合成反应各模型的适用性。模拟结果说明,全混模型适用于费托合成动力学行为的考察模拟;多级串联模型在一定的级数下能够近似模拟鼓泡浆态床中费托合成反应结果,更适用于探讨返混对费托合成反应行为的影响;双泡模型能够描述鼓泡浆态床中流体力学对反应的影响。  相似文献   

5.
以空气 -甲醇 -石英砂体系为对象 ,研究了锥形鼓泡浆液反应器的气含率和颗粒浓度分布 ,考察了气速、颗粒浓度、液体性质对水力学性质的影响 ,并且得到平均气含率经验关联式和予测颗粒浓度分布用的Pe关联式εg(1 -εg) 4 =0 .0 82u1.3g (1 -Cs) 10 9Pe =0 0 81 4Fr0 .0 52 6Ar0 50 9(1 -Cs) 0 94 5Sb1.2 56  相似文献   

6.
浆态床反应器中生物质合成气合成二甲醚的研究   总被引:1,自引:0,他引:1  
进行了浆态床反应器中,甲醇合成催化剂与分子筛混合制复合催化剂上,生物质制取的合成气(简称生物质合成气)一步法合成二甲醚的研究,重点考察了不同脱水组分和工艺条件对催化剂反应性能的影响,同时,结合NH3-TPD等手段对催化剂进行了表征。结果表明,含有较弱酸性SAPO-11分子筛的复合催化剂更适合生物质合成气原料气杂质多、氢碳比低的特点,在合成二甲醚反应中具有更高的选择性和稳定性。250℃、5 MPa、500 h-1时,在甲醇催化剂与SAPO-11分子筛比例为3:1的复合催化剂上,合成气合成二甲醚反应35 h内,CO转化率稳定在40%以上,二甲醚在有机产品中的选择性保持在97%左右。  相似文献   

7.
锥形鼓泡浆液反应器内气含率和固含率轴向分布研究   总被引:1,自引:2,他引:1  
在不同表观气体速度、淤浆浓度、静止液体高度和不同颗粒直径下考察了锥形鼓泡浆液反应器内气含率及固率轴向分布。由气泡聚并和破碎机理解释了气含率轴向分布规律;结合固体颗粒悬浮机理,利用沉降-扩散模型分析了操作条件影响固含率轴向分布的原因,回归出表征固含率轴向分布的特征参数——Peclet准数的数学关联式,并在相似操作条件下与园柱床内实验结果作了比较。  相似文献   

8.
在内径98mm的鼓泡浆态反应器内,考察了工艺参数对浸没表面与浆液间的传热系数的影响。浆态反应器轴向装有一个外径20mm,长120mm的测量传热膜系数用的铜制元件。为了模拟浆态FT合成反应系统,三相系统由N2、液体石蜡和石英砂(平均粒径53μm、110μm、180μm)或63μm以下的Fe2O3组成。工艺参数变化范围如下:表观气速0.005m/s~0.08m/s, 温度353K~453K, 压力0.1MPa~0.8MPa,固体的质量分数0~20%,初始液位高度625mm~1240mm。本研究使用单孔板、多孔板、烧结金属板三种气体分布器类型。结合实验数据,应用最小二乘法求得各个参数值,得到的无因次传热系数关联式为St=0.179(ReFr)-0.25Pr-0.66,相关指数0.98,最大偏差18%。该关联式可应用于气-液和粒径小于100μm的气-液-固体系。  相似文献   

9.
工业固定床Fe-Cu-K催化剂浆态床F-T合成适应性研究   总被引:2,自引:3,他引:2  
采用连续搅拌釜式反应器,在接近F-T合成实际工况下考察了工业固定床Fe-Cu-K催化剂浆态床F-T合成反应性能,研究反应温度、压力、原料气空速和氢碳摩尔比等操作参数对催化剂反应活性、产物选择性和稳定性的影响,实验总运转时间达2 500 h;同时采用扫描电镜技术(SEM)对催化剂的抗磨损性能进行了研究,结果表明,操作参数对催化剂的活性、选择性和目标产物产率有较大的影响,工业固定床Fe-Cu-K催化剂具有一定的抗磨损性能,F-T合成烃产物分布合理;催化剂具有较高的稳定性,在589 h的稳定条件运行内,催化剂的失活速率为0.23%/d(以CO转化率的降低计);在整个运行期间CH4选择性维持在较低的水平。  相似文献   

10.
以FeCuK/Si O2为母体催化剂,通过乙酸钠浸渍得到一组不同Na含量的费托合成铁基催化剂.采用原子发射光谱、低温N2吸附、程序升温还原和M ssbauer谱等技术对催化剂进行了表征.在H2/CO摩尔比为0.67,空速为2 000 h-1,压力为1.5 MPa和温度为250℃的条件下进行了浆态床F-T合成反应性能评价实验.结果表明,浸渍少量Na能提高催化剂的比表面积,促进铁物相的分散,而浸渍大量Na却大大降低了催化剂的比表面积,使催化剂中的铁物相聚集形成较大的颗粒;浸渍Na抑制了催化剂在H2中的第一步还原,但促进了催化剂在CO中的碳化;在原位合成气还原过程中,浸渍Na有利于催化剂的碳化.在500 h的运行实验中,浸渍Na的催化剂均表现出不同程度的失活现象.反应结果表明,浸渍Na对水煤气变换反应活性影响不大,对费托合成反应活性和烃产物选择性有较大的影响.在铁基催化剂上浸渍Na有利于C12 重质烃和低碳烯烃的生成.  相似文献   

11.
分析研究了不同粒径分布的石油焦成浆性及制备水焦浆的流变性和稳定性。结果表明,石油焦的成浆性较好,成浆浓度近70%,浆体的表观黏度均随浓度的增大而增大。粒径分布越宽,越有利于堆积,堆积效率越高,可制浆浓度越高,制备水焦浆的最佳药剂量越低,采用萘系分散剂制备的水焦浆呈胀塑性流型,粒径分布越宽,胀塑性越弱,利用静置观察法与Turbiscan Lab稳定性分析仪测定相结合评价水焦浆的稳定性,水焦浆的稳定性差,且粒径越大,析水率越低,沉降区的焦粉颗粒越易发生聚结,底部越易产生硬沉淀,稳定性越差。颗粒聚结是水焦浆稳定性的主要影响因素。  相似文献   

12.
The separation efficiency and kinetics of several commercial HPLC particle types (both fully porous and superficially porous) have been investigated using a pharmaceutical weakly basic N-containing compound as a test molecule. A strong trend between the particle size distribution (PSD) of the particles and the typically employed “goodness of packing”-parameters was observed. The relative standard deviation of the PSD of the tested particles ranged between 0.05 and 0.2, and in this range, a near linear relationship between the A-term constant, the hmin-value and the minimal separation impedance was found. The experimental findings hence confirm the recent observations regarding the relationship between the narrow PSD of the recently commercialized porous-shell particles and their superior efficiency and kinetic performance. The outcome also suggests that the performance of the current generation of fully porous particle columns could be significantly improved if the PSD of these particles could be reduced.  相似文献   

13.
采用神华煤制备煤浆,分析了颗粒粒径比λ和小颗粒体积分数ξ对双峰分布浆体黏度的影响,根据浆体黏度的关联式预测了煤浆的黏度并且与实验结果进行了比较。结果表明,采用双峰分布的颗粒制浆可以有效地降低浆体的黏度,同时可以获得较大的浆体体积分数 。在相同体积分数下,随着颗粒粒径比λ的增加,浆体的黏度迅速下降。当小颗粒体积分数ξdp1为35%时,浆体的黏度最小。采用Ouchiyama模型计算浆体的最大体积分数Φm与实验值较为吻合,而浆体的本质黏度[μ]基本保持不变。考虑λ和小颗粒体积分数ξ对双峰分布浆体的最大体积分数Φm的影响,可以采用单峰分布浆体的黏度关联式预测双峰分布浆体的黏度。  相似文献   

14.
In this study, sub-200?nm, crosslinked latex particles with a narrow particle size distribution were prepared by one-step emulsion polymerization in the presence of particle coagulation. The relationship between the particle shape and particle coagulation was investigated by varying the time of crosslinking network structure formation and particle coagulation. Particles with irregular shapes such as doublet, triplet, and ellipsoid were obtained using divinylbenzene (DVB) and ethylene glycol dimethacrylate (EGDMA) as the crosslinking agents, because the crosslinking network structure of particles was formed before the particle coagulation. In contrast, latex particles with a uniform spherical shape were also prepared using triallyl isocyanurate (TAIC) or dihydrodicyclopentadienyl acrylate (DCPA) as the crosslinking agents by delaying the time of crosslinking network structure formation. Alternatively, uniform spherical latex particles were prepared by bringing forward the particle coagulation time using cationic initiator, 2, 2′-azobis (2-methylpropionamidine) dihydrochloride (AAPH). This study presents a new idea that would further broaden the application of particle coagulation in emulsion polymerization.  相似文献   

15.
Summary A particle size distribution analysis has been completed on three different HPLC column packing materials including silica gel (Si60) and two bonded phases (RP8 and RP18). The stationary phases were subjected to 18 hours stress with 1 N or 3 N KOH and found to have quantitatively different distribution patterns initially, at 13 hours and finally at 18 hours although the average particle diameters for the Si60 and RP8 were the same or higher at 18 hours as initially. Thirteen hoursstress with sodium octanesulfonate, tetrabutylammonium phosphate and ammonium acetate at exaggerated conditions also resulted in distributional changes with the Si60 and RP8 decreasing in average particle diameter when exposed to ammonium acetate and tetrabutylammonium stressing respectively.  相似文献   

16.
Polybutadiene latexes made in emulsifier-free emulsion polymerization with diameters ranging from 50 to 300 nm of both unimodal and bimodal particles size distributions were analyzed by the line-start (LIST) method in a Brookhaven Disk Centrifuge Photosedimentometer (DCP). A special spin fluid was designed to be able to sediment polybutadiene since the density of the polymer is 0.89 gcm–3 and is thus less dense than its suspending medium. Density and viscosity gradients were created simply by adding five different mixtures of ethanol, water, and emulsifier in density sequence to the spinning disk. Coagulation problems caused by diluting polybutadiene latices with ethanol were overcome by using nonionic Triton X-100 surfactant. Good agreement in the average particle size and distribution as well as polydispersity between transmission electron microscope and disk centrifuge data was accomplished. The analysis time for polybutadiene latex particle sizing thus was reduced from several days to approximately 1 h.  相似文献   

17.
The dispersion of methyl methacrylate (MMA) and its suspension polymerization were used as models to elaborate the evolution of particle size average and size distribution in the course of suspension polymerization. The underlying mechanisms for the occurrence of the dynamic and static steady states in the population of drops were defined and their effects on the evolution of drop/particle size average and size distributions were examined. The characteristic intervals of suspension polymerizations (transition, steady-state, growth, and identification) were elaborated. The formation of satellite droplets and their evolution in the course of polymerization were also discussed.  相似文献   

18.
Summary Particle size distribution analysis and scanning electron microscopy (SEM) were carried out on eight used HPLC columns containing either irregular silica based, spherical silica based or spherical polymer based packing material. Particle size distributions of the used irregular silica based columns were at least bimodat at the outlet ends and either biomodal or log-normal at the inlet ends with regular progressions between the two extremes through the column. A new ODS-3 column showed log-normal size distributions from the inlet to the outlet ends. Spherical silica based column particle size distributions showed distinct shoulders on large central distribution peaks in most column sections with various degrees of shoulder erosion. The spherical resin based column showed a broader inlet particle size distribution progressing to a very narrow outlet distribution. SEMs of both irregular and spherical silica based columns revealed a larger number of undersized particles and debris at the outlet than inlet ends which could have resulted from stationary phase degradation, since this was not seen in the new ODS-3 column. While several SEMs of the spherical silica based columns revealed hollow spheres and twins, the spherical resin based column packing showed stress fractures or wrinkle lines resulting from use or dehydration.Presented in part as a poster at the HPLC '92, 16th Symposium on CLC, Baltimore, MD, USA.  相似文献   

19.
Latex emulsions depend strongly on the polymer composition, and particle size distribution, which in turn, is a function of the preparation of the latex and on the formulation and composition variables. This study reports measurements of particle size and particle size distribution of latex emulsions as function of the reaction time and the type and concentration of emulsifier by using the multiwavelength spectroscopy technique. Results show changes in the particle size of latex emulsions with the reaction time, obtaining larger particles and broader distributions with increasing of Tween 80 ratio. The steric stabilization provides the sole nonionic emulsifier is not enough to protect the polymer particle, causing the flocculation among the interactive particles, resulting in unstable latex. However, latex emulsions prepared with Tween 80 ratio <70 wt.% can stabilize efficiently the nucleated particles, probably due to the effects provided by both, the electrostatic and steric stabilization mechanisms. The same effect is shown in the curves of conversion (%) as a function of reaction time, resulting in slower polymerization rate for Tween 80 ratio >70 wt.%. On the other hand, smaller polymer particles, in all range of emulsifier mixture, have been obtained to higher emulsifier concentration.  相似文献   

20.
The mechanism of the miniemulsion polymerization of styrene was investiaged through a combination of calorimetry to monitor the polymerization rate and transmission electron microscopy (TEM) to follow the evolution of the particle size distribution. These techniques proved to be a powerful combination for gaining detailed mechanistic information regarding these polymerizations. Particle size analysis of the latexes withdrawn during the course of the reaction revealed that most of the polymer particles were formed by a relatively low conversion (i.e., 10% conversion). However, nucleation continued well past this point (to 40-60% conversion). In fact, it was observed that nucleation in miniemulsion polymerizations using cetyl alcohol continued past the maximum in the rate of polymerization. As a result of these long nucleation periods, the latex particle size distributions produced from these miniemulsion polymerizations were broader than their conventional emulsion polymerization counterparts, and were negatively skewed with a tail of small particles. The amount of negative skewing of the particle size distributions was found to decrease with increasing initiator (potassium persulfate) concentration. Finally, a correlation was observed between the length of time to the maximum polymerization rate and the breadth of the particle size distribution as reflected in the standard deviation. © 1995 John Wiley & Sons, Inc.  相似文献   

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