共查询到18条相似文献,搜索用时 625 毫秒
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熔融聚合物中气泡的动力学实验研究 总被引:3,自引:0,他引:3
通过可视化通道,进行大量的实验,观察CO2气体与熔融聚合物在各种流场中(延伸流场、螺旋流场、几种不同流场的组合)的形态、大小、运动、变形等现象。从实验观察角度出发,分析了流场结构参数、加工条件与气泡在聚合物熔体中形态、分布、运动变化等的内在关系。 相似文献
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贺朝晖;信春玲;李庆春;何亚东 《中国塑料》2010,24(11):62-67
以聚苯乙烯/CO2发泡体系为研究对象,利用细胞模型推导出了基于牛顿流体本构方程、幂律流体本构方程、dewitt黏弹性本构方程3种本构方程的气泡生长数学模型,通过比较分析得出了最适合该发泡体系的气泡生长模型,并研究了熔体弹性和非牛顿性质等物性参数对气泡生长过程的影响。结果表明,dewitt模型能更加准确地反映实际的气泡生长的过程;聚合物熔体弹性在生长初期对气泡生长有明显的促进作用;聚合物熔体的非牛顿性质对于气泡生长全过程都有影响。 相似文献
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剪切流场中微孔发泡的气泡成核理论研究现状 总被引:1,自引:0,他引:1
分析了经典成核理论对于动态聚合物熔体中气泡成核的局限性;概括了剪切流场中气泡成核的研究进展,并对剪切流场中泡核拉伸模型、空穴成核模型进行了详细的分析和讨论,指出了其对气泡成核过程解释的不足;介绍了最新的气泡成核中的剪切能成核理论,该理论较完善地解释了剪切流场中气泡成核过程;最后指出了气泡成核研究的发展方向。 相似文献
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利用有限元软件包Polyflow模拟不同条件下发泡机头流道内PS/CO2熔体的流动,获得了压力,计算出压降速率,并分析熔体温度、CO2含量、机头模口流道直径和质量流率对流道内压力和压降速率的影响。结果表明,在加工条件允许的范围内,降低熔体温度,可以显著提高机头流道中的压力和机头模口流道中的压降速率;当熔体温度一定时,机头流道中的压力和机头模口流道中的压降速率随着CO2含量的增加而降低。尤其当熔体温度为150℃,CO2质量含量由1%增加到2%时,机头模口流道中的压降速率急剧降低;减小机头模口流道直径可有效地提高机头流道内的压力和压降速率。熔体温度175℃,CO2质量含量5%、质量流率1kg/h时,模口直径由1mm减小到0.5mm,机头入口段压力由5.9MPa增大到近30MPa。 相似文献
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基于壁面滑移条件,建立了微小流道内聚合物黏弹三维共挤出流动模型,并运用有限元方法对流动模型进行了模拟计算。为探究壁面滑移条件下聚合物熔体工艺条件和物性参数对成型的影响,分别设置芯、壳层熔体不同的流率比和黏度比,通过分析流道内外的熔体速度分布及层间界面形貌,探究了无滑移和完全滑移两种壁面条件下,熔体流率和黏度对聚合物微共挤成型层间界面的影响规律。结果表明,无滑移壁面条件下,熔体层间界面不稳定,口模内和口模外界面均发生偏移,且在口模出口处发生突变,熔体离开口后存在胀大和变形现象,其胀大和变形程度随着熔体入口流率比和黏度比的变化而变化;完全滑移壁面条件下,口模内熔体层间界面发生偏移,但口模外界面稳定,不存在挤出胀大和变形,且不受熔体入口流率比和黏度比的影响,这对实现聚合物微复合制品的精密成型具有重要意义。 相似文献
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采用高速摄像法测量了均匀鼓泡流状态下,水以及体积分数分别为20%和40%的甘油-水体系中气泡群的浮升运动,考察了气含率、雷诺数和分布器孔径对气泡尺寸、形状、浮升速率和曳力系数的影响。构建了立方体单元胞模型,并根据雷诺数的不同选取层流和湍流模型,模拟得到气泡的浮升速率和曳力系数与实验值吻合较好。结果表明:随着气含率及液体黏度的提高,气泡群浮升阻力增大,浮升速率减少;随着雷诺数和气泡直径的增加,曳力系数减小,气泡浮升速率增大。单元胞模型能较好地反映气泡群浮升过程中各因素的影响,是处理气泡群运动的有效工具。 相似文献
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对三种管口浸没方式下气泡生成行为过程进行可视化实验和三维数值模拟。对比分析了管口浸没方式、管口直径、气体流量等因素对气泡生成形态、气泡脱离直径、气泡膨胀脱离时间以及气液流场速度的影响。实验与数值模拟取得较为一致的结果。研究发现,气泡生成过程可分为单气泡生成和双气泡生成聚并两种模式,两者之间存在明显的气泡脱离形态转折点;三种管口浸没方式下,气泡脱离直径均随着管径和气体流量的增大而增大;气泡膨胀脱离时间随管径的增大而增加,而随气体流量的增加先急剧下降然后趋于平缓;在底吹和侧吹方式下,气泡长短轴比C值分别在0.75和1.1附近波动,其最终脱离形式均接近于球形;而顶吹方式下,C值在1.5附近波动,气泡脱离形态为椭球形。 相似文献
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The investigation on bubble behavior in electric field helps to analyze the mechanism of electric enhancement of boiling heat transfer. Experiments were performed to investigate the bubble deformation in direct current (DC) electric field with bubbles attached to the orifice. The air bubbles were slowly generated in the transformer oil pool at different orifices, so that the effect of flow on bubble shape was eliminated. The results showed that the bubbles were elongated and the departure volume decreased when the electric field was intensified. The major and minor axes, aspect ratio and departure volume increased with increasing the orifice diameter. Both the electric field and orifice size have great influence on bubble behavior. The bubble deformation was also simulated to compare with the experimental results. The numerical and experimental data qualitatively agree with each other. 相似文献
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采用实验和仿真方法,对一特定气泡雾化喷嘴泡状流时混合室内的气液两相混合形态以及喷孔出口喷雾脉动特征进行了研究。研究结果表明,泡状流时气泡尺寸呈近似正态分布,气泡尺寸随液相质量流量和气液质量比增大而减小;喷雾形态和喷孔出口气液流动参数存在较大脉动,喷雾锥角脉动超过20°;气泡数量密度小且气泡直径较大时,喷雾平均锥角相对较小,且喷雾脉动现象比较严重;随着气泡数量密度增加,喷雾平均锥角呈现先快速增大后缓慢增大趋势,而喷雾锥角变异系数先快速增大随后逐渐减小并趋于稳定;复杂的流场结构是喷孔内气泡表观形态发生较大变化以及喷孔出口气液流动参数产生较大脉动的主要原因。 相似文献
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A new theoretical model for calculating bubble formation at an orifice submerged in an inviscid liquid is presented. Simplified equations of motion for the gas—liquid interface were developed, and together with thermodynamic equations for the gas in the bubble and the chamber below the orifice plate, the instantaneous shape of the bubble during its formation was calculated. In contrast with previous models, the present model is able to determine the instant of detachment as the moment at which the neck of the bubble closes. The present model gives also a more detailed treatment of the flow through the orifice, and is suitable for low as well as high chamber volumes. Calculated results are presented for a wide range of orifice radii (0.0175–0.48 cm), gas flow rates (0.4–100 cm3/sec) and chamber volume (1–5000 cm3), including examples of calculated bubble shapes. The present model is restricted to single bubble formation, but it is able to calculate the critical flow rates and critical chamber volumes which limit this region. 相似文献
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To investigate the mechanism of gas absorption from a bubble containing soluble and insoluble components, a gaseous mixture of ammonia and nitrogen was bubbled into water. The growth curve, volume, surface area and shape of the growing bubbles were measured with parameters such as inlet gas composition, gas flow rate and gas chamber volume. The bubble volume decreased with the increasing composition of ammonia in a bubble, decreasing gas chamber volume and decreasing gas flow rate.To reasonably express the mass transfer from the bulk of a gas in a bubble to the bulk of a liquid, the overall mass transfer resistance was evaluated by the mass transfers in the gas phase, interface and liquid phase.The non-spherical bubble formation model combined with the overall mass transfer resistance estimated well experimental bubble shape, bubble volume at its detachment from an orifice, growth rate and mass transfer rate.Moreover, the change of concentration with bubble growth time and the fractional absorption during bubble formation were simulated. 相似文献
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从实验和数值计算两方面研究了超声速气体射流在水中的喷射过程.用高速摄影机拍摄了三维水下超声速气体射流的流场.针对实验工况,基于VOF方法,建立水下超声速气体射流的二维轴对称数值计算模型,并开展了相关数值模拟.成功模拟了射流初期气泡运动演化的复杂过程;分析了水下超声速气体欠膨胀射流的流场结构,包括流场的压力和速度等参数分布以及变化规律.数值结果与实验结果对比得知数值计算结果不仅与实验数据吻合较好,而且给出了实验中没有发现的激波、膨胀波等流场结构. 相似文献
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M. K. Moraveji A. Amirimehr S. Nadery P. Rafiee 《Theoretical Foundations of Chemical Engineering》2013,47(6):779-787
Computational fluid dynamics (CFD) simulation of the hydrodynamics of slug flow which is generated by air sparging in a vertical tubular membrane has been investigated. The results of simulation have been reported in the form of parameters such as shape, velocity profile, surface shear stresses and gas slug (Taylor bubble) rising velocities, and evaluated with experimental data which were presented in previous articles. This study showed that CFD modeling is able to accurately simulate the shape and velocity field around the gas slugs. Also the shear stress induced by slug flow passage and rising velocity of gas slugs for high-velocity liquid and low-velocity gas fit appropriately to values in reference data. Simulation results for gas slug rising velocity showed about 0.35–9% error in the different conditions investigated in respect to experimental data. 相似文献