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141.
无限长空间板在轴对称荷载作用下的位移和应力分析   总被引:1,自引:0,他引:1  
运用汉克尔变换导出了无限长空间板在轴对称荷载作用下的位移和应力解答,并通过与完全位移约束下的有限深地基模型、半无限大弹性地基模型和文克尔地基模型进行比较,分析它们之间的异同.分析结果表明:当H→∞时,无论底部是光滑刚性支承约束还是完全位移约束,在法向集中力作用下得到的水平面位移结果与半空间体的布希涅斯克位移解答在水平面上的位移是一致的;当H→0时,底部是光滑刚性支承约束与底部是完全位移约束取极限得到的文克勒地基基床系数是不同的.  相似文献   
142.
In this study, nineteen unmodified lignins from various sources (hardwood, softwood, wheat straw, and corn stover) and isolation processes (kraft, soda, organosolv, sulfite, and enzymatic hydrolysis) were used to replace 30 wt.% of petroleum-based polyol in rigid polyurethane/polyisocyanurate (PUR/PIR) foam formulations. Lignin samples were characterized by measuring their ash content, hydroxyl content (Phosphorus Nuclear Magnetic Resonance Spectroscopy), impurities (Inductively Coupled Plasma), and pH. After foam formulation, properties of lignin-based foams were evaluated and compared with a control foam (with no lignin) via cell morphology, closed-cell content, compression strength, apparent density, thermal conductivity, and color analysis. Lignin-based foams passed all measured standard specifications required by ASTM International C1029-15 for type 1 rigid insulation foams, except for three foams. These three foams had poor compressive strengths, significantly larger cell sizes, darker color, lower closed-cell contents, and slower foaming times. The foam made with corn stover enzymatic hydrolysis lignin showed no significant difference from the control foam in terms of compressive strength and outperformed all other lignin-based foams due to its higher aliphatic and p-hydroxyphenyl hydroxyl contents. Lignin-based foams that passed all required performance testing were made with lignins having higher pH, potassium, sodium, calcium, magnesium, and aliphatic/p-hydroxyphenyl hydroxyl group contents than those that failed.  相似文献   
143.
以Winkler分布弹簧模拟垫层的作用,考虑垫层、桩和土之间的相互作用;并以Geddes解和Boussinesq解为依据,求出了在单位荷载下网格单元顶部的沉降,即单元的柔度系数;运用弹性理论叠加原理,建立了包括桩顶沉降、土顶沉降及其对应荷载的线性方程组.求解该方程可以进一步求出多元复合地基中主桩、次桩对土的桩土应力比和主桩、次桩及土的荷载分担比.通过工程实例进行分析,表明本文方法的计算结果和现场实测结果符合很好.  相似文献   
144.
从工程应用出发,阐述了强夯法在处理湿陷性黄土地基的加固机理以及强夯技术在处理黄土地基中的有效加固深度、夯击能等的确定,并对夯点的布置、夯击遍数和间歇时间和夯击加载机具的选择进行了介绍.  相似文献   
145.
以南京市绕城公路拓宽工程软基加固为例,探讨现浇薄壁管(PCC)桩的应用,并对地基加固效果进行初步分析与评价.选取桩号为K4 120,K6 920,K6 986的3个典型的观测断面进行沉降、沉降速率、水平位移观测成果分析.结果表明,PCC桩复合地基可有效地控制加宽路基自身的沉降、与老路基间的差异沉降和路基的稳定性,可以满足施工控制标准,具有沉降收敛快,工后沉降小的特点,荷载-沉降曲线呈缓变形特点,与文献得到的结论一致.  相似文献   
146.
使用硝酸镍分别与2个含取代基的苯基二羧酸3-硝基邻苯二甲酸(3-NPAH2)和5-溴间苯二甲酸(H2BIPA)以及2个刚性含氮配体4,4’-联吡啶(4,4’-bipy)、1,4’-二咪唑基二苯(L=1,4’-bis(imidazol-yl)benzene)在水热条件下合成了2个镍配位聚合物,即,[Ni(3-NPA)(4,4’-bipy)(H2O)]n1)和[Ni(BIPA)(L)]n2)。表征了2个化合物的红外光谱、元素分析、热重、X-射线单晶衍射以及X-射线粉末衍射。化合物1是三斜晶系,P1空间群,含有[Ni(OCO)4Ni]双核单元,该双核单元再通过4,4’-联吡啶连接而成一个二维单层结构。层与层之间通过羧酸氧原子与配位水分子之间产生氢键作用。化合物2是单斜晶系,P21/c空间群,含有[Ni2(COO)2]双核单元,该双核单元进一步通过BIPA2-构成了一个双链结构,该双链再通过1,4’-二咪唑基二苯桥联配体连接形成了一个三维框架结构。此外,热重分析结果显示化合物2具有较高的热稳定性。  相似文献   
147.
本文研究了弹性地基上梁主共振响应的时滞效应.基于Hamilton原理,建立了时滞影响下弹性地基上梁的非线性运动微分方程,采用多尺度法,求得了时滞效应下主共振响应调制方程以及稳定性条件.通过数值算例,分析了时滞和调谐参数影响下主共振响应的峰值及幅频响应特性.结果表明,地基反力中的时滞效应对主共振响应影响较大,会导致共振域偏移,在一定区间内,响应幅值随时滞变化先减小再增大,呈现出周期性,并导致幅频曲线弯曲程度增大.  相似文献   
148.
刘又文  杨班权 《力学季刊》2003,24(1):142-145
研究含双周期分布的圆形刚性夹杂在无穷远受纵向剪切的弹性平面问题,遵循复合材料中各夹杂相互影响的重要条件。采用复变函数方法。构造相应模型的复应力函数。通过坐标变换,同时满足夹杂边界位移条件,再利用围线积分将求争方程组化为线性代数方程组。导出了圆形刚性夹杂双周期分布的界面应力解析表达式。算例给出了界面应力最大值与夹杂间距的变化规律。求出了刚性夹杂的合理间距问题,本文发展的分析方法为研究夹杂材料的细观机理探索了一条有效的分析途径。  相似文献   
149.
Chaotic motions of a rigid rotor in short journal bearings   总被引:65,自引:0,他引:65  
In the present paper the conditions that give rise to chaotic motions in a rigid rotor on short journal bearings are investigated and determined. A suitable symmetry was given to the rotor, to the supporting system, to the acting system of forces and to the system of initial conditions, in order to restrict the motions of the rotor to translatory whirl. For an assigned distance between the supports, the ratio between the transverse and the polar mass moments of the rotor was selected conveniently small, with the aim of avoiding conical instability. Since the theoretical analysis of a system's chaotic motions can only be carried out by means of numerical investigation, the procedure here adopted by the authors consists of numerical integration of the rotor's equations of motion, with trial and error regarding the three parameters that characterise the theoretical model of the system: m, the half non-dimensional mass of the rotor, , the modified Sommerfeld number relating to the lubricated bearings, and , the dimensionless value of rotor unbalance. In the rotor's equations of motion, the forces due to the lubricating film are written under the assumption of isothermal and laminar flow in short bearings. The number of numerical trials needed to find the system's chaotic responses has been greatly reduced by recognition of the fact that chaotic motions become possible when the value of the dimensionless static eccentricity % MathType!MTEF!2!1!+-% feaafiart1ev1aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbnL2yY9% 2CVzgDGmvyUnhitvMCPzgarmWu51MyVXgaruWqVvNCPvMCG4uz3bqe% fqvATv2CG4uz3bIuV1wyUbqee0evGueE0jxyaibaieYlf9irVeeu0d% Xdh9vqqj-hEeeu0xXdbba9frFf0-OqFfea0dXdd9vqaq-JfrVkFHe9% pgea0dXdar-Jb9hs0dXdbPYxe9vr0-vr0-vqpWqaaeaabiGaciaaca% qabeaadaabauaaaOqaaiabew7aLnaaBaaaleaacaWGZbaabeaaaaa!4046!\[\varepsilon _s \] is greater than 0.4. In these conditions, non-periodic motions can be obtained even when rotor unbalance values are not particularly high (=0.05), whereas higher values (>0.4) make the rotor motion periodic and synchronous with the driving rotation. The present investigation has also identified the route that leads an assigned rotor to chaos when its angular speed is varied with prefixed values of the dimensionless unbalance . The theoretical results obtained have then been compared with experimental data. Both the theoretical and the experimental data have pointed out that in the circumstances investigated chaotic motions deserve more attention, from a technical point of view, than is normally ascribed to behaviours of this sort. This is mainly because such behaviours are usually considered of scarce practical significance owing to the typically bounded nature of chaotic evolution. The present analysis has shown that when the rotor exhibits chaotic motions, the centres of the journals describe orbits that alternate between small and large in an unpredictable and disordered manner. In these conditions the thickness of the lubricating film can assume values that are extremely low and such as to compromise the efficiency of the bearings, whereas the rotor is affected by inertia forces that are so high as to determine severe vibrations of the supports.Nomenclature C radial clearance of bearing (m) - D diameter of bearing (m) - e dimensional eccentricity of journal (m) - e s value of e corresponding to the static position of the journal - E dimensional static unbalance of rotor (m) - f x, f y =F x/(P), F y/(P): non-dimensional components of fluid film force - F x, F y dimensional components of fluid film force (N) - g acceleration of gravity (m/s2) - L axial length of bearing (m) - m % MathType!MTEF!2!1!+-% feaafiart1ev1aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbnL2yY9% 2CVzgDGmvyUnhitvMCPzgarmWu51MyVXgaruWqVvNCPvMCG4uz3bqe% fqvATv2CG4uz3bIuV1wyUbqee0evGueE0jxyaibaieYlf9irVeeu0d% Xdh9vqqj-hEeeu0xXdbba9frFf0-OqFfea0dXdd9vqaq-JfrVkFHe9% pgea0dXdar-Jb9hs0dXdbPYxe9vr0-vr0-vqpWqaaeaabiGaciaaca% qabeaadaabauaaaOqaaiabg2da9maalaaabaGaeqyYdC3aaWbaaSqa% beaacaaIYaaaaaGcbaGaeqyYdC3aa0baaSqaaGabciaa-bdaaeaaca% WFYaaaaaaakiabg2da9maalaaabaGaeqyYdC3aaWbaaSqabeaacaaI% YaaaaOGaam4qaaqaaiabeo8aZjaadEgaaaaaaa!4C14!\[ = \frac{{\omega ^2 }}{{\omega _0^2 }} = \frac{{\omega ^2 C}}{{\sigma g}}\]: half non-dimensional mass of rotor - M half mass of rotor (kg) - n angular speed of rotor (in r.p.m.=60/2) - t time  相似文献   
150.
方棋洪  刘又文 《力学季刊》2004,25(2):279-285
位错和夹杂的干涉效应对于理解材料的强化和韧化机理具有十分重要的意义。文中研究了晶体材料中刃型位错和多条共圆弧刚性线夹杂的干涉作用。利用Riemann—Schwarz反照原理和复势函数的奇性主部分析技术,得到了问题的一般解答;对于只含一条刚性线夹杂的情况,给出了复势函数的封闭形式解。由Peach-Koehler公式求出了作用在刃型位错上的位错力,并讨论了圆弧形刚性线夹杂对位错力的影响规律,发现弧形刚性线对刃型位错有很强的排斥作用。本文解答不但可作为格林函数获得任意分布位错的相应解答,而且可以用于研究刚性线夹杂和任意形状裂纹的干涉效应问题。  相似文献   
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