基于客户程序度量包内聚性

为了一致而高效地计算包内聚性,许多研究者提出了大量的包内聚性度量方法.然而,这些方法主要依赖于包内部的数据流关系,常导致度量结果与实际开发经验相悖.为了解决这一问题,首先以包的职责为基础将包划分为4类.然后,提出了共同重用内聚CRC,并根据包的分类框架讨论了CRC的适用性.CRC的核心思想是若多个类总被共同重用,则它们之间存在紧密耦合.最后,提出了度量CRC的海明内聚度HC.与现有方法相比,HC同时考虑了包内和包间的数据依赖.因而,该方法能够有效地反映包内部类间的语义关系.此外,HC利用包的使用模式提高了度量结果的可区分性.实验研究表明HC能够有效评估包的内聚程度.充分说明了作为HC基础的CRC具有较高的合理性.     

云南民族包设计中的点、线、面

点、线、面元素是艺术设计最基本的元素,在云南民族包设计中普遍运用。本论文主要从点、线、面的性质和作用来阐述了点线面元素是如何在云南民族包设计中得到运用的,从而使民族包的语言得到了充分的发挥。     

封装器件多应力叠加失效仿真分析与验证

针对某双列直插式(DIP)封装器件在整机温循试验中出现的失效现象,分析在器件与电路板焊接环节、电路板与整机装配环节和整机温循试验环节3个工况下可能的失效原因,对原因分别进行单工况和多工况的失效仿真分析。针对不同仿真模型在不同工况下的叠加仿真难题,提出基于ANSYS Workbench有限元软件的多应力叠加仿真方法,对比单一工况和多种工况下的仿真结果。结果表明,DIP封装器件失效是器件在焊接尺寸不匹配、过定位装配和温循试验三种工况下,机械应力和热应力的叠加使玻璃绝缘子产生裂纹导致的,有限元仿真结果与实验结果基本吻合,为DIP封装器件在多工况下应力叠加失效的故障机理研究提供一种可参考的仿真方法。     

微纳连接技术研究进展

近年来,集成电路不断向短小轻薄的高集成方向发展,推动着器件封装尺寸不断缩小,也使器件封装结构发生着改变.同时,作为信息革命的重要组成部分,集成电路技术往往涉及到多个领域的交叉和相互渗透,如微机电系统、精密仪表以及柔性器件等,而作为电子元器件封装中的关键技术,微纳连接技术的发展直接关系到电子工业中新型封装结构的研发与技术革新.因此,集成电路中微纳连接技术的发展也与多个技术领域密切相关.本文针对电子组装中微连接技术进行归纳和总结,并阐述纳米连接技术所取得的最新研究进展.通过总结微纳连接技术在不同互联尺度下的研究与应用现状,明确了微纳连接技术在电子工业领域中的重要作用,也为目前和未来的相关研究工作提供参考方向.     

面皮快餐食品工业化生产的调查及工艺研究

通过对面皮传统手工制作工艺的调查分析,提出了面皮工业化生产的工艺和方法,进而对面皮作为方便快餐食品的开发进行了论述。利用先前开发的面皮机和小麦淀粉厂的有关设备,进行了中试试验,在此基础上提出了有关工艺和经济技术指标。     

自动测试系统中的仪器设备驱动通用封装研究

在目前的自动测试系统软件开发中,虚拟仪器设备指令的非通用性会导致系统开发繁琐、无法集成等问题,针对这些问题提出了一种适合大部分仪器设备的封装方法;这种封装方法,通过动态链接库的形式将事件处理机制嵌入到仪器驱动封装里,拥有跨平台、适用面广、开发速度快和仪器可互换等特点;经过在实际雷达射频模块自动测试系统项目中的应用,结果表明该方法能够实现跨平台操作、具有仪器互换和封装简便等特点,并且表现出极强的通用性,具有一定的实用性和推广价值.     

一类积分不等式的机器判定

将一类积分不等式转化为Tarski模型外的齐次对称多项式不等式,该类齐次对称多项式的次数是给定的,变元个数可以是任意多个,并且多项式的系数是与变元个数相关的变系数.这些特点与杨路等人最近提出的几个公开问题密切相关,是比较有代表性的一类齐次对称多项式.然后利用Timofte关于对称多项式不等式判定的降维方法,结合不等式证明软件BOTTEMA及差分代换方法,给出对应的一类Tarski模型外的齐次对称多项式不等式的机器判定算法,从而实现原积分不等式的机器判定.当给定的积分不等式及齐次对称多项式不等式不成立时,可给出具体不成立的数值反例.应用例子表明问题的广泛性及算法的有效性.     

色彩与包装

包装是生活中不可或缺的一部分,色彩是包装设计中重要元素,人们通过长期的生活体验,有意无意之中形成了根据色彩来判断和感受商品包装的方式,包装色彩不仅增强消费者的审美愉悦,吸引消费者的注意力,更能激发消费者的购买欲望,它的运用是否合理直接影响到该包装设计是否成功。     

ISICS2011, an updated version of ISICS: A program for calculation K-, L-, and M-shell cross sections from PWBA and ECPSSR theories using a personal computer

In this new version of ISICS, called ISICS2011, a few omissions and incorrect entries in the built-in file of electron binding energies have been corrected; operational situations leading to un-physical behavior have been identified and flagged.

New version program summary

Program title: ISICS2011Catalogue identifier: ADDS_v5_0Program summary URL:http://cpc.cs.qub.ac.uk/summaries/ADDS_v5_0.htmlProgram obtainable from: CPC Program Library, Queen?s University, Belfast, N. IrelandLicensing provisions: Standard CPC licence, http://cpc.cs.qub.ac.uk/licence/licence.htmlNo. of lines in distributed program, including test data, etc.: 6011No. of bytes in distributed program, including test data, etc.: 130 587Distribution format: tar.gzProgramming language: CComputer: 80486 or higher-level PCsOperating system: WINDOWS XP and all earlier operating systemsClassification: 16.7Catalogue identifier of previous version: ADDS_v4_0Journal reference of previous version: Comput. Phys. Commun. 180 (2009) 1716.Does the new version supersede the previous version?: YesNature of problem: Ionization and X-ray production cross section calculations for ion–atom collisions.Solution method: Numerical integration of form factor using a logarithmic transform and Gaussian quadrature, plus exact integration limits.Reasons for new version: General need for higher precision in output format for projectile energies; some built-in binding energies needed correcting; some anomalous results occur due to faulty read-in data or calculated parameters becoming un-physical; erroneous calculations could result for the L and M shells when restricted K-shell options are inadvertently chosen; to achieve general compatibility with ISICSoo, a companion C++ version that is portable to Linux and MacOS platforms, has been submitted for publication in the CPC Program Library approximately at the same time as this present new standalone version of ISICS [1].Summary of revisions: The format field for projectile energies in the output has been expanded from two to four decimal places in order to distinguish between closely spaced energy values. There were a few entries in the executable binding energy file that needed correcting; K shell of Eu, M shells of Zn, M1 shell of Kr. The corrected values were also entered in the ENERGY.DAT file. In addition, an alternate data file of binding energies is included, called ENERGY_GW.DAT, which is more up-to-date [2]. Likewise, an alternate atomic parameters data file is now included, called FLOURE_JC.DAT, which is more up-to-date [3] fluorescence yields for the K and L shells and Coster–Kronig parameters for the L shell. Both data files can be read in using the -f usage option. To do this, the original energy file should be renamed and saved (e.g., ENERGY_BB.DAT) and the new file (ENERGY_GW.DAT ) should be duplicated as ENERGY.DAT to be read in using the -f option. Similarly for reading in an alternate FLOURE.DAT file. As with previous versions, the user can also simply input different values of any input quantity by invoking the “specify your own parameters” option from the main menu. You can also use this option to simply check the values of the built-in values of the parameters. If it still happens that a zero binding energy for a particular sub-shell is read in, the program will not completely abort, but will calculate results for the other sub-shells while setting the affected sub-shell output to zero. In calculating the Coulomb deflection factor, if the quantity inside the radical sign of the parameter zs becomes zero or negative, to prevent the program from aborting, the PWBA cross sections are still calculated while the ECPSSR cross sections are set to zero. This situation can happen for very low energy collisions, such as were noticed for helium ions on copper at energies of E?11.2 keV. It was observed during the engineering of ISICSoo [1] that erroneous calculations could result for the L- and M-shell cases when restricted K-shell R or HSR scaling options were inappropriately chosen. The program has now been fixed so that these inappropriate options are ignored for the L and M shells. In the previous versions, the usage for inputting a batch data file was incorrectly stated in the Users Manual as -Bxxx; the correct designation is -Fxxx, or alternatively, -Ixxx, as indicated on the usage screen in running the program.A revised Users Manual is also available.Restrictions: The consumed CPU time increases with the atomic shell (K, L, M), but execution is still very fast.Running time: This depends on which shell and the number of different energies to be used in the calculation. The running time is not significantly changed from the previous version.References:

• [1] 

  M. Batic, M.G. Pia, S. Cipolla, Comput. Phys. Commun. (2011), submitted for publication.

• [2] 

  http://www.jlab.org/~gwyn/ebindene.html.

• [3] 

  J. Campbell, At. Data Nucl. Data Tables 85 (2003) 291.

     

基于MATLAB的小波包信号消噪处理

信噪分离是小波包应用于信号分析的一个重要方面。本文在基于MATLAB的基础上,采用小波包对含高斯白噪声信号进行分解,通过不同的量化阈值对小波包系数进行处理、重构得出小波包消噪后的信号。计算机仿真结果表明,用不同量化阈值的小波包可对含高斯白声信号进行消噪重构。