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1.
本文对矩形通道内水的放热进行了试验研究,除了平板区外还测定了角区的局部放热系数;同时在气回路里测定了矩形通道角区及定位肋条附近的切应力分布;将局部放热系数分布与切应力分布进行了比较,二者是接近的.  相似文献   

2.
切应力协同下受热过冷层流液膜的破断特性   总被引:1,自引:0,他引:1  
针对界面切应力协同下受热过冷层流液膜流动的破断过程, 建立了不同气液流向下的临界液膜厚度和最小润湿量的理论模型, 分析了不同驱动力作用下, 接触角、流体温度、界面切应力和壁面热流密度对液膜破断特性的影响. 研究表明: 临界液膜厚度和最小润湿量均随壁面热流密度的增加而增大; 重力驱动下的接触角影响在不同热流密度下有所不同, 流体温度在不同驱动力下对最小润湿量的影响截然相反; 同向切应力驱动下临界液膜厚度和最小润湿量随切应力增加而减小; 在重力和切应力协同驱动下, 同向切应力对最小润湿量的影响与重力和切应力所起作用的相对大小有关, 反向切应力使得临界液膜厚度和最小润湿量有所增大.   相似文献   

3.
本文求解局部缓慢扩张动脉管中血液振荡流的基本方程,得到血管内血液的流速与压力梯度的关系。通过导出压力梯度沿局部扩张管轴向的变化特性。建立利用扩张段上游血管均匀段中心流速波形确定局部扩张管中血液流的速度和切应力分布的方法,文章以人体颈动脉余弦扩张为例进行分析。详细讨论了局部扩张对血管壁切应力及其梯度分布的影响。数值结果表明,在与刚性均匀管中管壁切应力沿轴向保持不变不同,在局部扩张段,管壁切应力将随着血管半径的增大而减小,因而管壁切应力梯度一般不为零,甚至在某些位置达到相当大的数值。另外,随着血管扩张程度的增加,管壁切应力还将进一步减小,而且管壁切应力梯度也将进一步增大,血管扩张导致管壁切应力的这些变化将直接影响血管壁的结构和功能,使其产生适应性的变化。  相似文献   

4.
复杂应力状态下岩石破坏特性的精确描述对于岩土工程结构设计具有重要的意义.基于多种岩石不同受力形式下的试验结果,将岩石的破坏形式分为拉断、局部剪切破坏和整体剪切破坏,使用应力三维度作为应力状态参数,分析岩石的破坏形式及不同破坏形式下强度参数随应力状态的变化规律.结果表明:对同种岩石,随应力三维度代数值减小,其破坏机理由拉断逐渐变化为局部剪切破坏和整体剪切破坏,三种破坏形式之间存在两个应力三维度分界值.对三种破坏形式,控制断裂发生的主要因素也不同.拉断主要受最大拉应力控制,局部剪切破坏由最大切应力主导,但同时受体变应力的影响,而整体剪切破坏仅由最大切应力控制.因此针对三种破坏形式,分别选择控制破坏的参量,提出破坏判据,并通过煤样和大理岩的单轴和三轴压缩试验结果验证了判据的正确性.  相似文献   

5.
微重力下薄燃料表面火焰传播的地面窄通道模拟   总被引:1,自引:0,他引:1  
张夏 《力学学报》2007,39(4):466-472
对微重力下薄燃料表面逆风火焰传播的地面窄通道模拟,进行了量纲分析,并通过火焰传播 图像记录进行了实验验证. 结果表明,减小实验段特征尺寸可以实现微重力燃烧的地面模拟. 在各种氧气浓度条件下,竖直和水平窄通道内的火焰传播速度随气流速度的变化趋势完全不 同,而且,水平窄通道可以有效限制自然对流,而竖直窄通道较难. 当通道高度增大时,竖 直和水平窄通道中,火焰传播速度和吹熄极限速度都不同程度地增大,这是热损失减小、火 焰面遇见的气流速度减小以及自然对流速度增大3个因素的综合结果. 对于水平窄通道, 1cm是一个可以定性模拟微重力下自然对流的尺寸. 对于竖直窄通道,则需要高度更小的窄通 道来限制自然对流.  相似文献   

6.
结合非局部弹性应力/应变梯度耦合本构关系和流体非局部应力关系式,基于Euler梁理论,建立了充流微通道流固耦合波传导模型;根据耦合固体非局部应力/应变梯度弹性效应以及流体非局部效应,分别模拟了微通道和管腔内流体的尺度效应,推导得出了充流微通道在微纳米尺度的波动控制方程和边界条件。通过对控制方程的求解,分析了不同类型尺度效应对微通道的波动和振动特性的影响。结果显示,各类尺度效应对系统的动力学特性影响不同。微通道非局部弹性效应对波动产生阻尼,特别是对波长较短的波传导;而应变梯度弹性效应对波传导有促进作用,且该效应对波动的影响与波长无关;非局部效应和应变梯度效应对微通道刚度产生不同影响,非局部效应降低刚度,应变梯度效应增加刚度。  相似文献   

7.
本文利用液晶高弹体的应力-应变本构方程和力-序耦合方程,研究了沿指向矢单轴拉伸下液晶高弹体力学行为的热力序耦合特性。由于力-序耦合,有序度在拉伸作用下变大,从而影响了液晶高弹体的应力-应变关系,使得应力在相同伸长下变小。不同温度下应力受到有序度变化影响的程度不同.由于有序度随温度升高而减小,当工程应力不变时,伸长随着温度升高而减小;当伸长不变时,应力随着温度升高而增大;伸长随温度的变化关系和应力随温度的变化关系都呈非线性。  相似文献   

8.
首先推导出不同剪切位移下试样截面惯性矩表达式,然后计算得到试样剪切面上归一化最大、最小法向应力随剪切位移变化的关系曲线,发现两法向应力及其差值随剪切位移的增大而增大,随试样剪切面直径或剪切边长的增大而减小。当试样剪切面直径和边长相同时,圆形试样剪切面上的法向应力要比方形上均匀些。当试样剪切面为矩形,沿矩形长边方向剪切时,其上法向应力的分布要比沿短边方向剪切时均匀些。建议尽量使用剪切面为圆形的大样进行直剪试验。  相似文献   

9.
金属轧制过程辊缝非稳态混合润滑特性研究   总被引:2,自引:1,他引:1  
根据Tsao和Sargent的混合润滑假设,建立了板带轧制时混合润滑状态下的非稳态润滑基本模型.系统分析了非稳态混合润滑状态下,基于正弦后张应力输入时,摩擦应力、压应力随时间和表面粗糙度变化的分布情况,以及基于某一压下率下在不同时刻表面粗糙度对摩擦应力、压应力分布的影响.结果表明:在较大的后张应力情形下,工作区中的压应力对表面粗糙度非常敏感,且随着表面粗糙度的增加相应增加;当后张应力减小时,压应力对表面粗糙度的敏感度下降.表面粗糙度对工作区中摩擦应力的分布有较大影响,当有较大后张应力输入时,辊缝间压应力相应较低,此时摩擦应力大小分布对表面粗糙度非常敏感,且随着表面粗糙度的增加而增加.与后张应力相比,表面粗糙度对摩擦应力的影响更为显著.  相似文献   

10.
基于率相关的晶体塑性滑移理论,论文考虑晶体内部塑性变形产生的热以及快速热冲击作用下温度急剧变化产生热应力的热-力双向耦合效应,建立起微观单晶的瞬态热-弹-塑性耦合模型,推导出与温度有关的剪应变率和弹塑性切模量公式.根据论文建立的模型,对ABAQUS软件进行二次开发[1],数值模拟出<001>/{100}单晶Cu在单轴拉伸状态下的应力、应变与温度的关系和弹性模量的变化,结果如下:轴向应力随温度升高先呈线性增加再呈非线性减小,轴向应变随温度增加而增加;弹性模量随塑性变形的增加而降低,与分子动力学模拟的趋势[2]是一致的.数值实验表明,论文建立的模型和算法是正确合理的,且计算量远远小于分子动力学模拟.  相似文献   

11.
Blood flow through a catheterized artery is analyzed, assuming the flow is steady and blood is treated as a two-fluid model with the suspension of all the erythrocytes in the core region as a Casson fluid and the plasma in the peripheral region as a Newtonian fluid. The expressions for velocity, flow rate, wall shear stress and frictional resistance are obtained. The variations of these flow quantities with yield stress, catheter radius ratio and peripheral layer thickness are discussed. It is noticed that the velocity and flow rate decrease while the wall shear stress and resistance to flow increase when the yield stress or the catheter radius ratio increases while all the other parameters were held fixed. It is found that the velocity and flow rate increase while the wall shear stress and frictional resistance decrease with the increase of the peripheral layer thickness. The estimates of the increase in the frictional resistance are significantly very small for the present two-fluid model than those of the single-fluid Casson model.  相似文献   

12.
The rheology of concentrated planar fiber suspensions is investigated. A new experimental technique for fiber suspensions based on a sliding plate rheometer incorporating a shear stress transducer is developed. It is shown that this instrument works well for the tested material systems. The rheological behavior in steady shear is subsequently investigated. The results can be largely explained by a combination of frictional and hydrodynamic interaction. Despite this evidence of friction no yield stress could be detected for the investigated shear rates. It was also found that the fiber aspect ratio did not influence the steady shear viscosity.  相似文献   

13.
Shear viscosity, shear stress and first normal-stress difference have been investigated for glass- and vinylon-fiber filled polyethylene melts over a wide range of shear rate by means of three kinds of instruments. The influence of fiber content and fiber properties on the rheological properties is discussed. The viscosity increases with increasing aspect ratio and fiber content, and the influence of these parameters on the flow properties is evident at low shear rates. The first normalstress difference increases more rapidly with increasing glass fiber content, especially at low shear stresses. The influence of vinylon fibers on the first normal stress-difference vs. shear-stress relationship is different from that of glass fibers.  相似文献   

14.
The dynamic effective shear strength of saturated sand under cyclic loading is discussed in this paper. The discussion includes the transient time dependency behaviors based on the analysis of the results obtained in conventional cyclic triaxial tests and cyclic torsional shear triaxial tests. It has been found that the dynamic effective shear strength is composed of effective frictional resistance and viscous resistance, which are characterized by the strain rate dependent feature of strength magnitude, the coupling of consolidation stress with cyclic stress and the dependency of time needed to make the soil strength sufficiently mobilized, and can also be expressed by the extended Mohr-Coulomb's law. The two strength parameters of the dynamic effective internal frictional angle φd and the dynamic viscosity coefficient η are determined. The former is unvaried for different number of cyclic loading, dynamic stress form and consolidation stress ratio. And the later is unvaried for the different dynamic shear strain rate developed during the sand liquefaction, but increases with the increase of initial density of sand. The generalization of dynamic effective stress strength criterion in the 3-dimensional effective stress space is studied in detail for the purpose of its practical use. The project supported by the National Natural Science Foundation of China (10172070)  相似文献   

15.
王勃  张阳博  左宏  王厚锦 《力学学报》2019,51(3):845-851
本文针对压剪裂纹的启裂及扩展问题,研究了脆性材料中裂纹面压应力变化对其扩展的影响规律.借助双轴加载试验机可自由调节两个轴位移和力的优势,设计了一种单边对称双裂纹压剪试样.试验中,施加裂纹面压应力至不同的预设值后,使剪应力单调增大直至裂纹启裂及扩展,得到不同预设压应力下压剪裂纹启裂及扩展规律. 随着预设压应力增大,启裂角增大,裂纹扩展路径与初始裂纹的偏角也增大.但随着压应力增大,启裂角增大至一定值后趋于稳定,实验发现,依据裂纹是否闭合,压应力对压剪裂纹扩展的作用大致可分为两个阶段:闭合前,压应力对裂纹启裂载荷及启裂角、扩展路径均有影响,预设压应力增大,裂纹启裂载荷增大、启裂角增大,扩展路径愈来愈偏离初始裂纹方向;闭合后,压应力虽然增大,启裂角和临界压剪应力比始终恒定,压应力对临界剪力和扩展路径存在一定影响.研究表明,裂纹启裂角与启裂时的压剪应力比存在一定的对应关系.启裂时的压剪应力比增大,启裂角增大,启裂时的压剪应力比恒定,启裂角不变.   相似文献   

16.
张显涛  刘伟 《应用力学学报》2020,(2):509-516,I0003
提出了一种大展弦比机翼管路的抗大变形设计与优化方法。首先建立了大展弦比机翼平板-不同布局管路的装配简化模型;然后分析了在机翼大变形下,管道的弯曲位置、弯曲半径、横向距离、弯曲角度等几种不同布局参数,对管路根部应力、最大应力和卡箍处变形的影响关系。结果表明:弯曲位置与横向距离对应力有较大影响,弯曲位置靠近机翼根部可以降低管道根部应力,但是最大应力显著增加,横向距离的增加可以降低管路根部应力以及最大应力;弯曲位置和弯曲半径对卡箍处变形有较大影响,随着弯曲位置从机翼板根部向变形处移动,卡箍处变形量均先减小后增加,弯曲半径的增加会降低卡箍处变形量。采用遗传算法得到在机翼大变形下最优的管形布局,结果表明,卡箍附近最大应力比直管降低了51%。  相似文献   

17.
Determination of yield stress fluid behaviour from inclined plane test   总被引:1,自引:0,他引:1  
The aim of this paper is to determine precisely under which conditions an inclined plane can be used as a rheometer, which could represent a practical and rapid technique for various types of industrial or natural viscoplastic coarse suspensions. We first examine its efficiency and relevancy for determining fluid yield stress in a straight way by measuring the deepest fluid layer able to stay on the inclined plane. We have made experiments with different materials (clay-water suspensions) whose yield stress ranged from 35 to 90 Pa, using 1 m long open rectangular channels with a slope ranging from 10 to 30° and a width ranging from 5 to 25 cm. Our procedure involved measuring the final fluid depth far from edges a long time after the end of the slow gravity-induced emptying of a dam placed upstream. The fluid yield stress was also estimated independently by fitting a Herschel-Bulkley model to simple shear rheometry data obtained within a relatively wide shear rate range. A good agreement between inclined rectangular channel tests and independent usual rheometrical tests is obtained even for aspect ratios (flow depth to channel width ratio) as large as 1 when one assumes that, when the fluid has stopped, the side and bottom wall shear stresses are equal to the fluid yield stress. These results prove the efficiency of the inclined plane test for determining yield stress when appropriate experimental precautions are taken for both tests. In addition we examine the possibility of determining the simple shear flow curve of a mud suspension from fluid depth, velocity and discharge measurements of different steady flows in a wide open channel (8 m long; 60 cm wide) equipped with a recirculating system. The results obtained from inclined plane tests are in good agreement with independent rheometrical data (with torsional geometries). However it is technically difficult to cover a wide shear rate range from the inclined plane technique since this requires a rather wide channel flow rate range.  相似文献   

18.
The flow of an incompressible couple stress fluid in an annulus with local constriction at the outer wall is considered. This configuration is intended as a simple model for studying blood flow in a stenosed artery when a catheter is inserted into it. The effects couple stress fluid parameters α and σ, height of the constriction (ε), and ratio of radii (k) on the impedance and wall shear stresses are studied graphically. Graphical results show that the resistance to the flow as well as the wall shear stress increases as the ratio of the radii increases and decreases as the couple stress fluid parameters increases.  相似文献   

19.
对四川地区江河上数座水电站坝基砂层的26组动力三轴试验资料进行了统计分析,基于动剪应力比法的液化判别方法推导了的地震液化的极限状态方程,使用蒙特卡洛随机抽样的方法计算了砂层液化的失效概率,并对某水电站的厂房地基砂层的液化可靠度进行了计算分析。研究表明,统计按粉砂样总体和中细砂样总体划分较为合理;砂层的动剪应力比可采用正态分布;电站砂层地基地震液化的最危险工况为,闸坝盖重加稳定的向上渗流及遭遇Ⅶ度地震荷载,为高液化风险,其液化概率随埋深加大而增大,最危险部位为砂层底板,对坝基砂层应进行抗液化处理。  相似文献   

20.
赵玉萍  袁鸿  韩军 《力学学报》2015,47(1):127-134
用解析法分析了单纤维从聚合物基体中的拔出过程,采用弹性—塑性内聚力模型模拟裂纹的扩展和界面失效,确定了临界纤维埋入长度,该值区分两种不同长度的纤维拔出过程. 在纤维拔出过程,界面经历不同的阶段. 纤维埋长小于临界长度时,界面的脱粘载荷与纤维的埋长成正比;超过临界长度后,界面的脱粘载荷近似为常数. 分析了界面参数对脱粘载荷的影响:增加界面的剪切强度和界面的断裂韧性,或减小界面裂纹萌生位移,均能提高界面的脱粘载荷;界面脱粘后无界面摩擦应力时,拔出载荷—位移曲线的峰值载荷等于界面的脱粘载荷;界面摩擦应力存在时,使峰值载荷大于脱粘载荷,需要较长的纤维埋入长度和较大的界面摩擦应力.   相似文献   

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