钢闸门支承滑道摩擦随时间变化的研究

研究了胶木、油尼龙和铜塑固体自润滑复合材料（ＴＳ－７０）３种平面滑动钢闸门支承滑道的摩擦时间效应,介绍了胶木和ＴＳ－７０滑道摩擦时间效应的原型试验结果,用粘着理论解释胶木与油尼龙滑道摩擦时间效应强、ＴＳ－７０滑道摩擦时间效应弱的原因在于粘弹性材料的蠕变大,引起实际接触面积增大,粘弹性材料的剪切模量的时间效应也大,使界面剪切强度增大。     

不同温度下半金属摩擦材料的摩擦磨损性能研究

利用Ｄ－ＭＳ型定速摩擦试验机,考察了２种润滑相对半金属摩擦材料摩擦系数和磨损率随温度变化的影响情况,并采用扫描电子显微镜（ＳＥＭ）和Ｘ射线能量色散谱等（ＥＤＡＸ）分析了２种复合摩擦材料中各组分对摩擦磨损性能的交互作用,揭示了半金属摩擦材料摩擦磨损的特性和机制。     

O‘—Sialon—ZrO2—SiC高温干摩擦下的摩擦磨损行为

研究了Ｏ’－Ｓｉａｌｏｎ－ＺｒＯ２－ＳｉＣ复合材料／１Ｃｒ１３钢摩擦副在６００℃不同工况条件下的摩擦磨损特性。结果表明：在６００℃干摩擦条件下,Ｏ’－Ｓｉａｌｏｎ－ＺｒＯ２－ＳｉＣ复合材料的磨损质量损失无穷氏于１Ｃｒ１我的磨损质量损失,Ｏ’－Ｓｉａｌｏｎ－ＺｒＯ２－ＳｉＣ复合材料／１Ｃｒ１３钢摩擦副的摩擦系数波动较大,磨损机制以粘着磨损和磨粒磨损为主。     

添加剂与铝合金的相互作用研究 Ⅰ.静态反应膜及油润滑下的摩擦学性能

静态下分别于２５℃，９０℃及１８０℃下进行硫化异丁烯（ＳＯ）、亚磷酸二正丁酯（ＤＢＰ）、ＳＯ＋ＤＢＰ的混合物（质量比２０∶１）、二烷基二硫代磷酸锌（ＺＤＤＰ）及十二酸（ＬＡ）５种添加剂均以质量分数为２％的比例添加到液体石蜡（ＬＰ）中与铝合金进行油浸试验．用动－静摩擦系数精密测定仪评价了在铝合金表面上所形成的静态反应膜的摩擦磨损行为，并考察了上述添加剂在ＬＰ中对铝合金－钢摩擦副的润滑作用．结果表明：静态反应膜的摩擦磨损行为与添加剂的化学活性密切相关，其中ＤＢＰ最易与铝合金发生反应，故其反应膜具有最低的摩擦系数和最长的耐磨寿命；ＺＤＤＰ在１８０℃下的静态反应膜具有较低的摩擦系数和较长的耐磨寿命；ＳＯ、ＳＯ与ＤＢＰ的混合物及ＬＡ的静态反应膜则不具有减摩抗磨性能，预示这些添加剂在ＬＰ中不与铝合金发生较强的化学作用．含上述添加剂的ＬＰ润滑下的摩擦磨损试验显示，ＤＢＰ与ＺＤＤＰ具有较好的摩擦学性能．这表明添加剂在铝合金表面静态反应膜的摩擦磨损试验结果与其在常规润滑下的具有较好的相关性．     

冷压盘式刹车片摩擦磨损性能的研究

采用ＭＭ－１０００型摩擦试验机、定速式摩擦试验机和台架试验机研究了冷压盘式刹车片的摩擦磨损性能。结果表明：采用冷压工艺制造的杀车片材料的摩擦磨损性能较好，摩擦系数在不同压力、速度和温度下较稳定，在汽车盘式刹车片中试用性能良好。根据刹车片的使用工况，利用ＭＭ－１０００型摩擦试验机进行小样模拟试验，所得测试结果与台架试验有较好的一致性。     

高速运动条件下玄武岩摩擦系数的实验研究

在MM－1000型摩擦磨损试验机上采用不同试验条件对玄武岩试件进行了高速摩擦试验研究,结果表明：摩擦表面载荷、运动速度以及摩擦速度以及摩擦表面特性等因素均对摩擦系数产生影响;摩擦系数随载荷的增大呈现减小趋势;对于饱和吸水试件,摩擦系数随运动速度增大持续降低;在其它试验条件下,饱和吸水试件的动摩擦系数比干燥试件明显要低。     

特定密封环摩擦系数的测定及其在储存期时效对比试验研究

特定密封环摩擦性能的时效对比试验研究是为其定型设计提供科学依据的重要手段．以聚四氟乙烯与Ｌｙ１２Ｃｚ铝合金作为摩擦副，运用牵引法原理，在自行设计制造的由微机实时控制的ＮＰＵ８９－Ｉ型测定仪上测定摩擦系数．试件在温度（１８±２）℃和相对湿度（７０±５）％的环境中存放，而有大部分试件于测试之前分别在－２０℃，－２５℃，－３０℃，－３５℃和－４０℃的低温下冷冻３６ｈ，测得平均滑动摩擦系数μ＝０．２９９±０．０１９．在５年储存期内的时效对比试验结果表明，其摩擦系数没有发生明显的变化     

添加剂与铝合金的相互作用研究：Ⅰ.静态反应膜及油润滑下的摩擦 …

静态下分别于２５℃，９０℃及１８０℃下进行硫化异丁烯，亚磷酸二正丁酯，ＳＯ＋ＤＢＰ的混合物（质量比２０：１），二烷基二硫代磷酸锌（ＺＤＤＰ）及十二酸（ＬＡ）５种添加剂均以质量分数为２％的比例添加到液体石蜡（ＬＰ）中与铝合金进行油浸试验。用动－静摩擦系数精密测定仪评价了在铝合金表面上所形成的静态反应膜的摩擦磨损行为，并考察了上述添加剂在ＬＰ中对铝合金－钢摩擦副的润滑作用。结果表明：静态反膜的摩擦磨损     

相对湿度对几种摩擦副静摩擦系数的影响

在自制的试验台上考察了相对湿度对金属－金属摩擦副、金属－石墨摩擦副、金属－TiN涂层摩擦副及金属－WC涂层摩擦副的静摩擦系数的影响。结果发现,相对湿度对金属－石墨摩擦副和金属－WC涂层摩擦副的静摩擦系数没有影响,而对金属－金属摩擦副和金属－TiN涂层摩擦副的静摩擦系数有影响。利用分形接触模型推导并计算了由水膜的弯月面效应引起的附加静摩擦系数,计算结果与实际变化趋势相吻合,静摩擦系数的计算值比实际值稍偏大。     

W18Cr4V钢表面离子氮碳共渗—离子渗硫复合处理渗层的摩擦磨损性能 …

研究了Ｗ１８Ｃｒ４Ｖ钢离子氮碳共渗－离子渗硫复合处理渗层的摩擦磨损性能,在环－块摩擦磨损试验机上测定复合物渗层与ＧＣｒ１５钢对摩时的摩擦系数,在往复式滑动磨损试验机上进行磨损试验,采用扫描电镜（ＳＥＭ）对磨损表面进行形貌分析,试验结果表明,复合渗层与ＧＣｒ１５钢对摩时的摩擦系数比未处理的Ｗ１８Ｃｒ４Ｖ钢与ＧＣｒ１５钢低,由于复合渗层中的氮碳化合物和硫化物降低了摩擦系数和粘关倾向,复合渗层的耐磨性高     

The 7th International Conference on Fluid Mechanics May 24-27,2015,Qingdao,China

正http://www.icfm7.org First Announcement and Call for PapersThe objective of International Conference on Fluid Mechanics(ICFM)is to provide a forum for researchers to exchange new ideas and recent advances in the fields of theoretical,experimental,computational Fluid Mechanics as well as interdisciplinary subjects.It was successfully convened by the Chinese Society of Theoretical and Applied Mechanics(CSTAM)in Beijing(1987,     

INFORMATION FOR CONTRIBUTORS

Contributions： The Journal, Acta Mechanica Solida Sinica, is pleased to receive papers from engineers and scientists working in various aspects of solid mechanics. All contributions are subject to critical review prior to acceptance and publication.     

Preface

This special issue of PARTICUOLOGY is devoted to the first UK-China Particle Technology Forum taking place in Leeds, UK, on 1-3 April 2007. The forum was initiated by a number of UK and Chinese leading academics and organised by the University of Leeds in collaboration with Chinese Society of Particuology, Particle Technology Subject Group （PTSG） of the Institution of Chemical Engineers （IChemE）, Particle Characterisation Interest Group （PCIG） of the Royal Society of Chemistry （RSC） and International Fine Particle Research Institute （IFPRI）. The forum was supported financially by the Engineering and Physics Sciences Research Council （EPSRC） of United Kingdom,     

基于鲁棒滤波的捷联导引头视线角速度估计方法

针对捷联导引头无法直接获取视线角速度等信息的问题,研究了鲁棒滤波在大气层外飞行器捷联导引头视线角速度估计中的应用。为了建立非线性滤波估计模型,考虑目标视线角速度的慢变特性,采用一阶马尔科夫模型建立了状态方程;推导了视线角速度的解耦模型,并建立了量测方程;考虑到实际应用中存在系统噪声统计特性失准的问题,基于Huber-Based鲁棒滤波方法,设计了视线角速度滤波器,并完成了基于Huber-Based滤波方法和扩展卡尔曼滤波方法的数学仿真。仿真结果表明Huber-Based滤波方法的视线角、视线角速度及视线角加速度估计精度分别达到0.1140'、0.1423'/s、0.0203'/s2,而扩展卡尔曼滤波方法的视线角、视线角速度及视线角加速度估计精度仅分别为0.6577'、0.6415'/s、0.0979'/s~2。仿真结果证明了该方法可以有效地估计出相对视线角速度等信息,并且在非高斯噪声的条件下,依然可获得较高的估计精度,具有一定的鲁棒性。     

Guide for authors

正Each of the sections below provides essential information for authors.We recommend that you take the time to read them before submitting a contribution to Acta Mechanica Sinica.We hope our guide to authors may help you navigate to the appropriate section.How to prepare a submission This document provides an outline of the editorial process involved in publishing a scientific paper in Acta Mechanica     

Use specification of multiscale materials for life spanned over macro-, micro-, nano-, and pico-scale

Multiscale material intends to enhance the strength and life of mechanical systems by matching the transmitted spatiotemporal energy distribution to the constituents at the different scale, say—macro, micro, nano, and pico,—, depending on the needs. Lower scale entities are, particularly, critical to small size systems. Large structures are less sensitive to microscopic effects. Scale shifting laws will be developed for relating test data from nano-, micro-, and macro-specimens. The benefit of reinforcement at the lower scale constituents needs to be justified at the macroscopic scale. Filling the void and space in regions of high energy density is considered.Material inhomogeneity interacts with specimen size. Their combined effect is non-equilibrium. Energy exchange between the environment and specimen becomes increasingly more significant as the specimen size is reduced. Perturbation of the operational conditions can further aggravate the situation. Scale transitional functions and/or f_j/j+1 are introduced to quantify these characteristics. They are represented, respectively, by , and (f_mi/ma,f_na/mi,f_pi/na). The abbreviations pi, na, mi, and ma refer to pico, nano, micro and macro.Local damage is assumed to initiate at a small scale, grows to a larger scale, and terminate at an even larger scale. The mechanism of energy absorption and dissipation will be introduced to develop a consistent book keeping system. Compaction of mass density for constituents of size 10⁻¹², 10⁻⁹, 10⁻⁶, 10⁻³ m, will be considered. Energy dissipation at all scales must be accounted for. Dissipations at the smaller scale must not only be included but they must abide by the same physical and mathematical interpretation, in order to avoid inconsistencies when making connections with those at the larger scale where dissipations are eminent.Three fundamental Problems I, II, and III are stated. They correspond to the commonly used service conditions. Reference is made to a Representative Tip (RT), the location where energy absorption and dissipation takes place. The RT can be a crack tip or a particle. At the larger size scales, RT can refer to a region. Scale shifting of results from the very small to the very large is needed to identify the benefit of using multiscale materials.