残余奥氏体含量对马氏体高强钢滑动磨损性能的影响

对3种不同残奥(RA)含量的马氏体高强钢进行干滑动摩擦磨损试验, 研究RA含量对其磨损性能的影响. 利用扫描电镜、透射电镜、X射线衍射仪等对试验后的磨损表面及横截面显微组织进行表征. 结果表明, RA含量越高, 磨损表面越光滑, 摩擦系数和磨损率越小, 也即马氏体高强钢的耐磨性越好. 磨损引起的大应变使RA发生应变诱导马氏体相变, 导致硬度和硬化层厚度显著增大. RA含量最高的HT3试样的硬度提高了18.3%, 硬化层厚度达70μm. 相比RA含量低的试样, HT3试样表现出很好的耐磨性. 这是因为马氏体相变使硬度逐步增加, 抗裂纹萌生能力提高; 同时由于亚表面良好的韧性, 可延缓和阻止裂纹扩展, 使得点蚀和剥落不易形成. 因此, 要提高马氏体高强钢的耐磨性, 除了硬度要求外, 还需要考虑其亚表面韧性.     

基于布拉格光栅的边坡监测实验研究

提出了一种基于分布式光纤光栅的边坡监测与报警系统.根据强度折减法,利用ANSYS软件分析出边坡的软弱面及滑体所在的具体位置,从而在该处安装经过特殊封装的拉线式光纤光栅位移传感器.滑体的位移通过拉线转换为作用在光栅上的应力,而光纤光栅反射波长与应变具有良好的线性关系,因此通过检测光栅反射光的中心波长的偏移量,就可以解调出...     

基于MATLAB的静电场模拟

在静电场中引入电位和电场强度后,通过等电位线图和场强分布图可以具体的描述静电场这种抽象的物质场。传统的静电场模拟实验直观地展现出了静电场的分布从而形象地描述了静电场,由于这种方法属于类比模拟,所以存在一定的缺陷(比如不直接,不能描述立体规律等等)。随着计算机技术的发展,利用计算机技术来模拟静电场等物质场逐渐成为趋势。通过借鉴大量资料简要地介绍了如何利用计算机模拟静电场,如何利用MATLAB软件模拟静电场的问题。     

38≤Z≤42类钴离子n =3、Δn=0跃迁的理论计算

用多组态自洽场方法,结合作者提出的半经验拟合公式,首先对38≤Z≤42类钴离子3p63d9,3p53d10,3p63d84p组态的能级进行计算,然后根据能级值算出相应的电偶极跃迁的谱线波长,并给出各谱线的HFR振子强度。     

固体材料脆性断裂的多尺度时空模型(英文)

通过实例分析了动态断裂过程所固有的典型动态作用,基于断裂孵化时间理论的时空结构方法提出了固体材料断裂的统一解释.此外,还提出了计及尺度效应的广义断裂模型,该模型可以用于预测准脆性非均质材料的多尺度断裂,并证明此模型基于实验室尺度的实验数据可以预测更高尺度(真实尺度)的宏观断裂.     

高强钢筋混凝土单向板在非接触爆炸下的抗爆性能研究

钢筋混凝土(RC)单向板是桥梁建设的重要组成部分. 对6块高强RC单向板进行非接触爆炸试验, 研究HRB400、HRB500和HTRB600高强RC单向板的抗爆性能, 分析爆炸后试件的破坏形态和参数. 结果表明 非接触爆炸下, 3种类型高强钢筋混凝土单向板的破坏形态相似, 单向板整体响应后出现弯曲破坏, 侧表面出现多条弯曲破坏裂缝; 在2.5kgTNT作用下的HTRB600高强RC单向板的裂缝数量和裂缝类型与2.1kgTNT作用下的HRB500高强RC单向板和1.7 kgTNT作用下的HRB400高强RC单向板差别不大, 相差范围在1条裂缝以内; HTRB600高强RC单向板在承受更大载荷时, 其平均加速度峰值比低载荷下HRB500、HRB400高强RC单向板分别增加45.1%和88.6%, 其抗弯承载力更好, 刚度更大.     

Electronic structure of C60 films

A complete set of fundamental optical functions of fullerite (C₆₀) films in energy ranges of 2.5–5.0 and 4.0–9.0 eV is calculated using the known spectra of the imaginary and real parts of the dielectric constant. An integrated spectrum of the dielectric constant is decomposed into elementary components. Three basic parameters of each component (the maximum and halfwidth energies and oscillator strength) are determined. Based on the known theoretical calculations of fullerite zones, a scheme of the nature of these components of the dielectric constant is suggested. Udmurt State University, 71, Krasnogeroiskaya Str., Izhevsk, 426034, Russia. Translated from Zhurnal Prikladnoi Spektroskopii, Vol. 66, No. 2, pp. 227–232, March–April, 1999.     

Determination of the Gamow–Teller strength function for the neutron-deficient isotopes In

The Gamow–Teller β decays of the neutron-deficient indium isotopes ^104–107In have been investigated by using total absorption γ-ray spectrometry on mass-separated sources. The experimental Gamow–Teller strength, deduced as a function of the excitation energy in the daughter nuclei ^104–107Cd, is compared to shell-model predictions.     

NMR imaging of white button mushroom (Agaricus bisporis) at various magnetic fields

Nuclear magnetic resonance (NMR) and magnetic resonance imaging (MRI) have been applied to visualize physiological phenomena in plants and agricultural crops. Imaging sequences that result in contrast of a combination of parameters (e.g., proton density, ) cannot be used for a correct and unique interpretation of the results. In this study multiecho imaging together with monoexponential T₂ decay fitting was applied to determine reliable proton density and T₂ distributions over a mushroom. This was done at three magnetic field strengths (9.4, 4.7, and 0.47 T) because susceptibility inhomogeneities were suspected to influence the T₂ relaxation times negatively, and because the inflences of susceptibility inhomogeneities increase with a rise in magnetic field strength. Electron microscopy was used to understand the different T₂'s for the various tissue types in mushrooms. Large influences of the tissue ultrastructure on the observed T₂ relaxation times were found and explained. Based on the results, it is concluded that imaging mushrooms at low fields (around or below 0.47T) and short echo times has strong advantages over its high-field counterpart, especially with respect to quantitative imaging of the water balance of mushrooms. These conclusions indicate general validity whenever NMR imaging contrast is influenced by susceptibility inhomogeneities.     

The randomly fluctuating impurity strength initiated excitation in doped quantum dots

We investigate the excitation behavior of a repulsive impurity doped quantum dot under the influence of randomly fluctuating dopant potential. We have considered Gaussian impurity centers doped at different locations. The investigation reveals the interplay between dopant location and dopant’s spatial stretch in modulating the excitation pattern. Maximization in the excitation rate has been observed as a function of fluctuating dopant strength owing to the conflict between opposing influences that promote and hinder excitation.