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1.
Abstract:  This study proposes an alternate method for the analysis of beams with solid cross-section or built as a framed structure and subjected to transverse impact loads from an external striker. The procedure used in the analysis is a combination of two essential tools using pseudo-dynamic techniques. The method reported here involves only one degree of freedom for the structure modelling and assumes an elastic contact between an external striker and the beam structure, which in reality does not happen. As only one degree of freedom is considered in the analysis, some important limitations are inherent to the method proposed here. Essentially, there is the difficulty of modelling the displacement field associated with the transient structure behaviour accurately, as a consequence of fast-rate impact loads. Another difficulty faced by the method refers to a local structure behaviour associated with contact loads. The present method can deal with large displacements in transversely loaded beams associated to a collapse mechanism having a simple geometry and defined with precision from a single parameter. This ensures reasonable accuracy in the evaluation of the strain energy absorbing capacity of transversely impacted beam structures using a single degree of freedom model in a pseudo-dynamic procedure.  相似文献   
2.
PSD激光直线度测量仪   总被引:2,自引:0,他引:2  
介绍了采用PSD传感器设计的激光直线度测量的工作原理,以及激光器、光靶和计算机系统的设计。  相似文献   
3.
基于数字运算的PSD调理电路设计   总被引:2,自引:0,他引:2  
介绍了基于数字运算的PSD调理电路思想及具体线路构造,该电路避免了模拟运算的缺陷,提高了精度和可靠性.  相似文献   
4.
用PSD检测长直导轨准直度   总被引:4,自引:0,他引:4  
介绍了用光电位置传感器(PSD)检测长直导轨的原理和方法。利用PSD作为位置传感的检测系统能实时、连续地对被测件三维空间准直度进行检测,更好地解决了以往移动桥板分段测量、人工读数(数格)局部检测的方法存在的问题。  相似文献   
5.
马长林 《机床与液压》2006,(3):195-196,218
研究了单神经元PSD控制器的一般结构,探讨了自适应PSD算法和改进的神经元学习规则,在SIMULINK环境下,针对实际的电液位置伺服系统进行了动态仿真,结果表明单神经元PSD控制器能使系统得到较好的控制效果。  相似文献   
6.
The shrinking core model (SCM) is widely used to model fluid-solid reactions such as the leaching of metals from minerals. In most cases, however, the particle size distribution (PSD) of the solid material was disregarded. In this paper the erroneous shift in the control regime when neglecting PSD was quantified and the dependence of the shift on the coefficients of variation (CV) and the type of PSD was analysed. By coupling the SCM with a Gamma PSD, it was found that neglecting the PSD would shift the control regime from chemical reaction to inert/ash layer diffusion, when the CV was between 0.7 and 1.2. For a system controlled by liquid film diffusion, neglect of the PSD, would shift the control regime to chemical reaction when CV is between 0.3 and 0.7 or to inert/ash layer diffusion when CV is greater (0.9-1.5). It was therefore postulated that some researchers had unknowingly made invalid conclusions about the control regime due to the neglect of PSD. However, an inert/ash layer diffusion-controlled process was insensitive to the neglect of PSD. When CV<0.3, neglect of the PSD would not cause any erroneous shifts, irrespective of the control regime. Experimental data confirmed the observation. For a given CV, the deviation in the fraction reacted from the mono-PSD increases with CV and decreases with time. The maximum deviation, which occurs at the beginning, is about 10% with a gamma PSD of CV=0.3. The percent deviation is dependent of the type of PSDs. Gamma PSD gives the lowest deviation while Gaudin-Schuhmann results in the largest deviation (maxi. ∼19%, with CV=0.3) in the first half of dissolution process. Log-normal distribution gives a larger deviation than gamma but quickly approaches the latter with time. The deviation for Rosin-Rammler is between log-normal and Gaudin-Schuhmann. For systems with CV less than 0.3, the SCM can be fairly used without considering PSD. When CV is greater than 0.3, particularly in the early stage of a dissolution process with a PSD other than gamma, PSD should be included to avoid substantial errors.  相似文献   
7.
In this paper, the theory on the translation of a measured chord length distribution (CLD) into its particle size distribution (PSD), which was developed in the first part of this study [Li and Wilkinson, 2005. Determination of non-spherical particle size distribution from chord length measurements. Part 1: theoretical analysis. Chemical Engineering Science 60, 3251-3265], has been validated using experimental results. CLDs were measured using the Lasentec focused beam reflectance measurement (FBRM) with three different materials, spherical ceramic beads and non-spherical plasma aluminium and zinc dust particles. Meanwhile, the particle shape and PSD of each material were also investigated by image analysis (IA). Comparison of the retrieved PSDs with the measured PSDs by IA shows that the PSD can be retrieved from a measured CLD successfully using the proposed iterative nonnegative least squares (NNLS) method based on the PSD-CLD model.  相似文献   
8.
针对现有图像融合方法的规则不易根据融合图像的后续使用要求进行自适应调整,并且各种方法的优点不易综合的问题,提出一种数据同化框架下的基于粒子群优化(PSD)和差分进化(DE)算法的融合方法。该方法把比率低通金字塔变换作为数据同化系统的模型算子,把非下采样的Contourlet变换(NSCT,nonsubsampled contourlet transform)作为观测算子,根据后续处理对图像各个属性指标值的依赖程度构造目标函数,再利用PSD和DE的混合算法来优化目标函数从而获取合适的影像。两组实验从视觉效果和定量指标两方面验证了方法的有效性。  相似文献   
9.
为了给混联式混合动力汽车提供新型的动力耦合装置,同时突破Toyota汽车公司的THS动力耦合系统专利的限制、束缚,通过对传统锥齿轮差速器的结构及工作原理的研究与分析,并与日本Toyota公司Prius混合动力汽车的THS系统中的PSD(动力耦合装置)进行对比研究,得出传统的差速器可以作为混联混合动力汽车的动力耦合装置的可行性,同时,通过仿真对可行性的结论进行了验证。  相似文献   
10.
提出了一种基于滨松S3931型号PSD器件和飞思卡尔Kinetis K60系列微控制器的激光位移测距系统.该测距系统主要利用了光学三角测量法的工作原理,将被测位移量通过光路系统转换为相应的微弱电信号,再由微弱电信号处理电路,经过放大、滤波、信号处理、A/D采集等一系列处理后,转换为实际位移量,并在LCD液晶显示屏上显示.本系统能够实现±5 mm范围内位移的快速测量,测量精度为30 μm,可以用于精密仪器尺寸测量、物体表面平整度检测等.  相似文献   
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