Thermal Deformation Measurement and Stress Analysis of PQFP Assembly during Power Cycling

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复合采动影响下地表变形预测与危险区划分方法

矿山岩体工程开挖将改变原岩应力状态,由此引起岩体本身及周围一定区域的移动和变形,地下与露天复合开采的矿山更是如此,其变形速率之大、范围之广、时间之长已严重地影响周边环境的安全。通过对地下与露天复合采动影响下地表变形规律进行研究,建立了相应的移动模型。在此基础上,对移动参数的计算方法及地面变形区的划分方法等问题进行了研究。然后,依据当前形量和后续变形量大小,对矿山继续开采可能产生的破坏范围进行了划分     

粘弹基上受压粘弹杆的稳定性

由纤维复合等材料研制的各种结构的广泛应用,使得其力学性能的研究日趋重要。由于这类材料具有明显的时间效应,因而,必须采用粘弹性理论研究其与时间相关的各种性质。利用动力学的观点和方法,研究了粘弹性基础上两端受压粘弹性直杆的动力稳定性。考虑杆的线性变形,将问题化为等价的四阶常微分方程,分析了方程不动点的稳定性,由此得到杆的蠕变及瞬时临界载荷,讨论了杆失稳的临界时间,并数值计算了杆的动力响应,得到了相应的     

水库二维水流泥沙数学模型及应用

建立水库坝区平面二维水流泥沙数学模型,考虑了悬移质非均匀,非饱和输沙特性,采用正交曲线坐标拟合复杂边界、ＳＩＭＰＬＥＣ程式离散求解及动边界技术。用该模型对白沙水库流场和河床变形进行了数值验证,计算了典型年条件下,水库取水口附近流场和河床局部形态。结果表明,坝前取水口漏斗基本保持稳定状态。     

膨胀土的浸水规律

根据土体浸水速率（导水库）与土体结构的理论关系和膨胀土结构的分形模型,导出了膨胀土的浸水速率与含水量,吸力、时间和上覆荷载的相关关系。理论和试验结果表明：膨胀土的浸水速率与含水量、吸力和时间在双对数坐标上呈直线相关,随着含水量增加、吸力减小,浸水速率增大、浸水速率随时间延长而减小;浸水速率的对数与上覆荷载呈直线相关,上覆荷载越大,浸水速率越小。     

冲击波作用下粉末颗粒效应及其形成过程

采用两种颗粒尺寸相差悬珠的高速钢粉末进行爆炸烧结机制的研究,发现了明显的“颗粒效应”,烧结过程首先在小颗粒变形量最大的尖角处发生熔化,在冲击波作用下使液体流激烈运动,加速了颗粒的熔化,最后使颗粒相互粘结在一起,达到烧结的目的。     

STUDY ON THE DUCTILE DEFORMATION DOMAIN OF THE SIMPLE SHEAR IN ROCKS——TAKING BRITTLE FAULTS OF THE COVERING STRATA IN THE SOUTHERN JIANGSU AREA AS AN EXAMPLE

A study on the ductile deformation domain of the brittle fault in the shallow level ofthe crust is a new probe field for the modern structural geology. Taking the southern Jiang-su Province area as an example the orientation measurement of quartz crystals, the com-positional texture observation of three pressure sensitive minerals and the rheological param-eter determination of dislocation densities, etc. have been demonstrated and analysed basedon typical samples in the present paper. In addition, their generation mechanisms arealso discussed from the cataclastic rheology, the dynamic differentiation and the simpleshearing, specially, from the Ode strength theory. Finally, a generative relationship betweenthe ductile deformation domain of the brittle fault system, in the regional layer--slip andthe formation of the stratabound ore deposit is shown as well.     

Molecular structure of ethynylbenzene from electron diffraction and ab initio molecular orbital calculations

The molecular structure and benzene ring distortions of ethynylbenzene have been investigated by gas-phase electron diffraction and ab initio MO calculations at the HF/6-31G^* and 6-3G^** levels. Least-squares refinement of a model withC _2v, symmetry, with constraints from the MO calculations, yielded the following important bond distances and angles:r _g(C _i -C _o )=1.407±0.003 Å,r _g(C _o -C _m )=1.397±0.003 Å,r _g(C _m -C _p )=1.400±0.003 Å,r _g(Cr _i -CCH)=1.436 ±0.004 Å,r _g(C=C)=1.205±0.005 Å, C _o -C _i -C _o =119.8±0.4°. The deformation of the benzene ring of ethynylbenzene given by the MO calculations, including o-C_i-C_o=119.4°, is insensitive to the basis set used and agrees with that obtained by low-temperature X-ray crystallography for the phenylethynyl fragment, C₆H₅-CC-, in two different crystal environments. The partial substitution structure of ethynylbenzene from microwave spectroscopy is shown to be inaccurate in the ipso region of the benzene ring.     

Plastic deformation kinetics for glassy polymers and blends

Measurements of the plastic deformation kinetics for several glassy (PS, PC, PI-polyimide, PET, epoxy-amine network), semi crystalline polymers (PBT, PET) and blends (ABS, PC:ABS, PC: PBT) were performed for the unidirectional compression loading conditions by using constant temperature deformation calorimetry. The experiments have permitted us to follow the changes of the mechanical work (A), the heat of deformation (Q) and differences between these quantities, i.e., internal energy (U) stored in samples during their loading and unloading. Experiments have shown that the large portion (45–85%) of the mechanical work of deformation (A) is converted to heat (Q). The rest ofA is converted to internal energy (U) stored in deformed samples. U is quite high as compared with metals [1,2]. After complete unloading of plastically deformed samples, i.e., samples carrying irreversible atT _def plastic deformation ( _irr ), some amount (U) of stored energy disappeared. The amount of (U and (U) are different for different polymers. All data are analyzed in the framework of the model proposed in [3,4]. The experiments support the deformation model where the plasticity of glassy polymers is the process of nucleation and development of so-called PDs-plastic local shear defects of nonconformational and nondilatational nature.Dedicated to Prof. Dr. W. Pechhold on the occasion of his 60th birthday     

On the deformation mechanisms of oriented PET and PP films under load

Uniaxially orienred semicrystalline poly(ethylene terephthalate) (PET) and poly(propylene) (PP) films were loaded parallel to draw direction at various temperatures. Changes in the submicroscopical structure of the films under load were examined by small and wide-angle x-ray scattering (SAXS; WAXS) and birefringence measurements. WAXS measurements reveal a decrease of the initial high orientation of the chains in the crystallites during deformation. Simultaneously, an increase of the birefringence was detected, indicating an orientation of chains in the amorphous regions. The alteration of the long period reflections in the SAXS patterns give strong evidence that lamellar stacks with different orientation angles according to load direction are present. Depending on the orientation of stacks, the contribution of lamellar separation to sample deformation alters, giving rise to different amounts of density changes in the stacks. Absolute intensity measurements of SAXS using a Kratky apparatus reveal that lamellar separation occurs preferentially below or in the range of the glass-transition temperature at small strain. With increasing strain and temperatures above the glass-transition slip deformation mechanisms become more important. The formation of microvoids was observed at strain near to elongation at break below or in the range of glass-transition temperature.