亚微米氮化钛膜的纳米压痕和划痕测定

采用等离子电弧沉积的方法，分别在GT35和40CrNiMo钢上沉积厚约为0．5μm的氮化钛(TiN)膜．为了筛选基材，采用纳米压痕和划痕技术，评价膜基界面结合和固体润滑效果．纳米压痕结果，GT35，40CrNiMo和TiN的纳米硬度／弹性模量的典型值分别约为11．5GPa／330GPa，6．0GPa／210GPa，30GPa／450GPa．纳米划痕结果，GT35有较理想的膜基结合能力；GT35，40CrNiMo，TiN及其有机膜的摩擦系数分别约为0．25，0．45，0．i5，0．i0．同40CrNiMo相比，GT35是较为理想的基体材料．纳米压痕和划痕技术能提供丰富的近表面的弹塑性变形、断裂和摩擦等的信息，是评价亚微米薄膜力学性能的有效手段．     

脉冲直流等离子体增强化学气相沉积Ti—Si—N纳米薄膜的摩擦磨损特性

采用工业型脉冲等离子体增强化学气相沉积设备，通过调节氯化物混合比例控制薄膜成分，在高速钢基材表面于550℃下沉积由纳米晶TiN和纳米非晶Si3N4组成的Ti—Si—N复合薄膜；采用扫描电子显微镜、透射电子显微镜、X射线衍射仪及X射线光电子能谱仪分析了薄膜的结构、组成和化学状态；采用球-盘高温摩擦磨损试验机考察了薄膜同GCrl5钢对摩时的摩擦磨损性能．结果表明：薄膜的Si含量在0％～35％范围内变化，随着Si含量增大，薄膜沉积速率增大，但薄膜由致密形态向大颗粒疏松态过渡；薄膜的晶粒尺寸为7～50nm；Ti—Si—N薄膜的显微硬度高于TiN的硬度，最高可达60GPa；引入少量Si可以显著改善TiN薄膜的抗磨性能，但薄膜的摩擦系数较高(室温下约0．8、400℃下约0．7)；随着Si含量的增加，Ti—Si—N薄膜的耐磨性能有所降低，其原因在于引入导电性较差的Si元素使得薄膜的组织变得疏松．     

磁过滤真空弧源沉积技术制备C/C多层类金刚石膜及其摩擦磨损性能研究

采用磁过滤直流阴极真空弧源沉积技术在Si基体和GCr15基体表面制备了C/C多层DLC膜,通过X射线光电子能谱仪分析薄膜结构特征;用原子力显微镜观察C/C多层DLC膜的表面形貌;采用台阶仪测试薄膜厚度;利用纳米硬度仪测试薄膜纳米硬度;在销盘式摩擦磨损试验机上进行C/C多层DLC膜在大气下的摩擦性能评价,同时比较了单层DLC膜、TiN膜和C/C多层DLC膜的耐磨性能.结果表明:C/C多层DLC膜表面光滑、致密,厚度达0.7 μm,硬度高达68 GPa,与SiC球对摩时的摩擦系数为0.10左右,耐磨性明显优于单层DLC膜和TiN膜.     

电化学沉积DLC薄膜的摩擦学性能研究

采用直流电源,以有机溶剂作为碳源,通过电化学沉积方法在单晶硅表面制备了类金刚石碳薄膜．用原子力显微镜、拉曼光谱仪和傅立叶红外光谱仪等表征了薄膜的结构,用DF-PM型动-静摩擦系数精密测定仪考察了薄膜的摩擦学性能．结果表明：电化学沉积含氢类金刚石碳薄膜的硬度较高(约14GPa),薄膜均匀、致密,表面粗糙度小;在室温干摩擦条件下,薄膜同GCrl5钢以及α-Al2O和Si3N4陶瓷对摩时的摩擦系数随载荷增加而略微减小;陶瓷材料／类金刚石碳膜的摩擦系数较低,钢／类金刚石碳膜的摩擦系数较高;类金刚石碳薄膜同Si3N4陶瓷对摩时呈现断裂剥落特征;同GCrl5钢对摩时发生转移并形成转移膜,耐磨寿命缩短．     

碳化硅薄膜的力学性能测试分析

对利用射频磁控溅射及真空退火方法在(100)硅晶片衬底上制备的纳米晶碳化硅(SiC)薄膜,用纳米压痕仪进行了力学性能测试分析。纳米压痕技术测试给出两块SiC薄膜样品I和II的弹性模量/硬度分别约为106GPa/9.5GPa和175GPa/15.6GPa。纳米划痕技术测试两块SiC薄膜的摩擦系数分别约为0.02~0.15和0.05~0.18,显示出良好的润滑性能;对薄膜的临界附着力等进行测量以评价膜基结合强度,分析了划痕过程中薄膜近表面弹塑性变形和断裂信息。在原子力显微镜下对SiC薄膜样品的初始表面及残余压痕和划痕形貌进行了观察分析,与测试结果相符。综合比较,样品II的整体性能优于样品I。本文中薄膜的弹性模量和硬度值较低可归因于制膜技术的不同和表层碳含量偏高。     

真空磁过滤电弧离子镀法制备DLC膜的机械性能

采用真空磁过滤电弧离子镀法分别在9Cr18和40CrNiMo钢上沉积厚约为0.2μm的类金刚石（DLC）膜。为了检测成膜质量，分别使用纳米压痕和纳米划痕技术表征钢基材和DLC/基材的机械性能，对这种亚微米厚的膜，纳米压痕技术和纳米划痕技术能提供丰富的近表面的弹塑性变形，断裂和摩擦等的信息。同DLC/40CrNiMo相比。DLC/9Cr18的硬度高和固体润滑效果显著，9Cr18是较为理想的基体材料。     

磁控溅射制备BCN薄膜纳米力学和摩擦磨损行为的研究

利用直流磁控溅射技术制备三元BCN薄膜，通过改变N2／Ar流量比（0．0～0．3）得到不同含氮量的薄膜．采用X射线光电子能谱仪和傅立叶红外光谱仪分析薄膜的成分和结构，采用纳米压入仪分析薄膜的纳米力学性能和纳米摩擦磨损特性，分别采用连续刚度测量法和横向力测量法测试薄膜的硬度和划痕行为．结果表明：薄膜中氮含量随N2／Ar流量比增加而增大并趋于稳定；反应气体中的氮优先与硼结合生成B—N键，当N2／Ar流量比超过一定值后，部分氮与碳结合生成C=N键；薄膜的纳米硬度和弹性模量随薄膜中氮含量的增加而下降；BCN薄膜的划痕深度与薄膜的结构密切相关，而摩擦系数受薄膜结构的影响不明显；在相同载荷下薄膜的划痕深度随薄膜中氮含量增加而增大；对于同一试样，薄膜在未破裂之前摩擦系数基本保持在0．10左右，薄膜破裂后摩擦系数迅速增至0．46．     

脉冲直流等离子体辅助化学气相沉积TiN和TiCN薄膜摩擦磨损特性研究

对比研究了脉冲直流等离子体辅助化学气相沉积TiN和TiCN薄膜的摩擦磨损特性，用扫描电子显微镜、X射线衍射仪及销-盘摩擦磨损试验机分析薄膜形貌和结合力，考察了不同沉积条件下2种薄膜的摩擦磨损过程及其影响因素．结果表明，TiCN薄膜具有较高硬度、良好的膜基结合力，相对于TiN薄膜而言表现出更低的摩擦系数和更好的耐磨性能．在实际使用中应注重成分和结构优化设计，以保证薄膜具有良优良的减摩性能．     

镁合金表面磁控溅射CNx/SiC/Ti多层膜的摩擦磨损性能

采用室温磁控溅射技术在镁合金(AZ91D)表面制备了CNx/SiC/Ti(氮化碳/碳化硅/钛)多层膜(SiC、Ti为中间层),研究了CNx薄膜的纳米压痕行为和摩擦磨损性能.结果表明:CNx薄膜具有低的纳米硬度(6.67GPa)、低的弹性模量(54.68GPa)和高的硬度与弹性模量比值(0.122);在以氮化硅球为对摩副的室温干摩擦条件下摩擦系数约为0.162,磨损率在10-6mm3/(m.N)级,薄膜经长时间(3.5h)磨损后未出现裂纹和剥落.分析表明,摩擦化学和硬度与弹性模量比值对摩擦系数和磨损率有重要影响.     

磁过滤多弧离子镀C/C多层膜在模拟体液中的微磨粒磨损行为

采用磁过滤直流阴极真空弧源沉积技术在Ti6Al4V表面制备C/C多层DLC膜,利用纳米压痕划痕仪测试薄膜的纳米硬度和膜-基结合强度,采用微磨粒磨损试验机对C/C多层DLC膜在模拟体液环境中的磨损性能进行评价,并与Ti6Al4V的耐磨性能进行对比.结果表明:C/C多层DLC膜硬度达54.82 GPa,弹性模量和划痕临界载荷分别为342.27 GPa和0.52 N;在模拟体液环境中DLC膜的耐磨性能显著优于Ti6Al4V合金,DLC膜的磨损机制主要包括二体磨损及混合磨损;随着料浆浓度的增加,DLC膜的磨损机制从二体磨损向混合磨损过渡.     

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.     

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.     

Impact non-pénétrant sur le thorax : influence de la courbure sur la propagation des ondesNonpenetrating impact on the thorax: influence of curvature on wave propagation

Theoretical studies of the propagation of impact waves through the thorax are needed to improve the design of bulletproof jackets and blast protections (Fung in ‘Biomechanics Motions, Flow, Stress, and Growth’, Springer-Verlag, 1990; Cooper et al., J. Trauma 40 (1996) S38–S41). The influence of the weak acoustic coupling at the interface between the thoracic wall and the lung were described in (Grimal et al., C. R. Acad. Sci. IIB 329 (2001) 655–662); in this work, we study, within the frame of elastodynamics and with an approximate analytical method, the effects of the curvature of this interface. Results are given in terms of strain energy for the pressure wave, transmitted or converted. Focalisation of energy in the medium representing the lung is important for curvatures measured in humans. To cite this article: Q. Grimal et al., C. R. Mecanique 330 (2002) 569–574.     

Vérification expérimentale de la relation de réciprocité d'Onsager pour l'électro-osmose et l'électro-filtration dans une argile naturelleExperimental verification of the Onsager's reciprocal relations for electro-osmosis and electro-filtration phenomena on a saturated clay

This Note is devoted to the experimental verification of the Onsager's reciprocal relations in the particular case of electro-osmosis and electro-filtration. A special set up has been designed to carry out the measurements of both the electro-osmotic permeability and the streaming potential. This has been performed by using a natural material i.e., saturated kaolinite. To cite this article: K. Beddiar et al., C. R. Mecanique 330 (2002) 893–898.