直线式箱体全自动无氟发泡线充注机械手的设计

介绍了直线式全自动箱体发泡线充注机械手的结构及其驱动系统,该系统可直接应用在新箱体发泡线的制造上,又可用在老箱体发泡线的改造上,因此具有极大的推广价值和显著的经济效益.     

铜线替代金线在晶体管封装中的压焊工艺研究

通过比较铜线与金线的性能,论述了铜线压焊的特点、设备的改造、铜线产品质量检验与常见不良产品等,在晶体管产量较大时,使用铜线压焊能有效地降低生产成本,因而在通用民品中有着非常广阔的应用前景.     

金亿机械有限公司:玉米收获机创造新纪录

11月18日,山东金亿机械制造有限公司在美丽的海滨城市日照举办了山东省玉米机械化发展与推广研讨会暨2008年商务年会.原计划600多人参加的会议却来了900多人,这在金亿公司是史无前例的,让公司领导及员工忙得不亦乐乎.金亿公司董事长马金英满面春风对记者说:"人气旺盛,一是得益于党的政策好,二是今年金亿公司拥有喜人的表现,小麦机产销1600台,市场占有率由去年的5%提升为15%,玉米机销售1200台,占行业内同类机型首位.同时,金亿产品也是获得政府补贴最多的产品."     

SIMATIC IT助力制造

西门子中国有限公司的业务结构涉及的行业和领域主要包括:信息通讯、自动化与控制、医疗、照明、能源、交通、金融和房地产等.西门子MES属于西门子自动化与驱动集团,这个业务集团是西门子最古老的集团之一,在中国的业务也发展非常好,产品覆盖各行业客户的自动化需求.自动化与驱动集团分为七个部门,MES隶属于其中的自动化与系统部.整个集团全球有近10万种产品,每个月约有18种新产品问世.自动化与驱动集团将其年销售额的约9%用于研发投资,尤其在工业软件方面很多人都认为自动化是一个硬件设备,但随着现在软件的发展,西门子也提供大量的软件开发.     

为推动国内实验室离心机行业升级而努力——专访上海安亭科学仪器厂董事长陆永泉先生

我国的实验室离心机产业近年来在研发生产方面取得了进步,但由于大部分企业的规模较小等原因,整体上与国外产品尚有一定差距。《中国仪器仪表》杂志记者专访了上海安亭科学仪器有限公司董事长陆永泉先生,陆先生评述了实验室离心机行业现状并提出了提高产品水平的措施,为推动国内实验室离心机行业升级提供了很好的建议。     

"数字化组织"迈出智能化敏捷制造第一步

PTC这支在船舶领域雄立多年的老牌劲旅,早在1992年就开始涉足船舶业,并取得了不错的成绩,1998年收购CV公司后更加强了其在船舶业的发展势头.目前在中国,军船市场一直占主导地位,民船虽然近几年才开始兴起,但市场表现也不俗.2007年我国的船舶业迎来了前所未有的井喷时期,也为PTC船舶业绩的提升带来了发展良机,而这一切早已洋溢在了PTC中国船舶业销售总监王慧杰的脸上.     

颅骨解剖机械设备的研制

本文针对目前法医解剖人体颅骨用设备存在的问题,探讨研究一种科学实用的颅骨解剖专用设备,用以提高解剖人员的工作效率,提高解剖质量,改善工作环境.     

防雨、防暴晒、夜晚能自动收缩的智能晾衣架设计

智能晾衣架的机械部分是在普通拉杆式晾衣架两支撑杆的端部各安装一个滑轮,再穿入钢丝绳.钢丝绳与最前外面的晾衣杆固定连接.钢丝绳的另一端连接到与直流电动机相连的转轴上,通过电动机的正反转达到晾衣架的伸缩效果.其控制部分的电路CPU采用89C2051单片机.利用温度、雨水、光敏等传感器,达到下雨时自动收回,雨后自动伸展;气温高于设定值时自动收回,低于设定值时自动伸展;夜晚自动收回,白天自动伸展的功能.     

基于WTK冷冻缸产品设计及加工虚拟现实软件的开发

在虚拟环境中利用数字化产品模型来代替实物模型进行仿真、分析,实现产品设计和制造过程的集成,已成为目前产品开发技术的重要发展方向.文中应用SolidWorks实现产品零配件和虚拟车床、夹具的实体造型,在VC 6.0开发平台上采用与World Tool Kit软件相结合的方法,同时利用与实体造型连接的技术实现虚拟设计和运动视景仿真并虚拟加工过程.     

AutoCAD下幻灯片文件的应用及其批量制作幻灯片文件的方法

AutoCAD环境下的幻灯片文件是一个屏幕显示的快照,目前主要应用在AutoCAD环境下进行二次开发所涉及的用户化界面设计方面.本文尝试了AutoCAD环境下幻灯片文件在零件资料库和用脚本文件播放幻灯片两方面的应用,研究了使用VisualLISP批量制作幻灯片的方法.     

Static friction at high contact temperatures and low contact pressure

The problem of measuring static friction at high temperatures and low contact pressures is theoretically analyzed, as well as the instruments for the accurate determination of the coefficient of static friction at high temperatures for contact pairs made of steel and bronze. The results of experimental investigation show that at low contact pressure and temperature above 120°C coefficient of static friction dramatically increases. This increase in the coefficient of friction can be of great practical value with regard to the load capacity of contacts where external forces are balanced with friction forces.     

Glenohumeral contact forces

Glenohumeral contact forces have only been calculated previously either for simple abduction or for athletic activities. The objective of this study was to determine the glenohumeral contact forces for tasks which are demanding of the shoulder but which would commonly be performed by older people. The functional tasks chosen were using the arms to stand up from and sit down into a chair, walking with a cane, lifting a 5 kg box to shoulder height with both hands, and lifting a 10 kg suitcase. The trunk angles, arm angles and hand loads of six healthy subjects, average age 55 years, were recorded. This information was input into a biomechanical computer model which optimized the muscle force distribution by minimizing the sum of squared muscle stresses subject to constraints on the maximum muscle forces and maintaining the direction of the resultant force within the glenoid fossa. Average contact forces ranged from 1.3 to 2.4 times body weight (930-1720 N), the highest force being for lifting a suitcase. This latter value would be even higher if lifting either a greater load or to a greater height. Thus, contact forces at the shoulder should not be underestimated. This study provides functionally relevant contact forces which can be used for mechanical testing or finite element modelling of shoulder prostheses.     

Edge contact effect on thermal elastohydrodynamic lubrication of finite contact lines

Minimum lubricant film thickness and maximum pressure every so often appear close to roller ends. This study combines the Boussinesq–Cerruti half-space equations with a free boundary correction procedure for precise modeling of edge contact conditions. The thermal EHL model developed associates this representation to a standard finite difference of the energy equation, and to a modified finite difference expansion of the Couette term of the Reynolds equation. To complete the model, the Carreau expression describes the shear-thinning response of the lubricant. The investigation includes different roller profile corrections. The results show that a large radius crowning modification combined with a rounding of the corners constitutes the most effective profile adjustment.     

Thermomechanical contact homogenization with random rough surfaces and microscopic contact resistance

We extend an earlier computational thermomechanical contact homogenization framework [Temizer ?, Wriggers P. International Journal for Numerical Methods in Engineering 2010; 83:27-58] to random rough surfaces generated through the random-field model based on the concepts of ensemble averaging and sample enlargement towards the effective limit. Additionally, the homogenization theory is revisited in order to incorporate thermal dissipation at the microscopic contact interface within a thermodynamically consistent approach that preserves dissipation across the scales. Large-scale three-dimensional computations were performed to demonstrate the effectiveness and feasibility of the computational framework for an accurate characterization of the macroscopic thermomechanical response of rough surfaces in contact.     

双列角接触球轴承的游隙与接触角

通过对双列角接触球轴承轴向游隙、径向游隙、接触角关系的推导换算,分析影响接触角的各因素,采取合理可行的方法保证接触角。     

Evaluation of the real contact areas, pressure distributions and contact temperatures during sliding contact between real metal surfaces

A three-dimensional elastic contact algorithm has been developed to analyse the normal contact problems of bodies having rough surfaces. The algorithm can evaluate the real contact areas and contact pressure distributions using measured surface roughness data.

Following an approximate elastic-plastic contact solution the analysis produces more realistic elastic and plastic contact areas; in addition results of contact pressure distributions can be predicted according to a given maximum plastic limit pressure.

The technique can simulate (in an approximate way) the elastic-plastic sliding contact behaviour in the vicinity of asperities or concentrated contact areas by ignoring the effect of the tangential forces on the vertical displacement.

Assuming a certain sliding speed and a particular coefficient of friction the local temperature distribution due to the heat generation over the real contact areas can also be calculated for 'slow sliding' problems.

The results show the moving real contact areas and the contact temperature fields for an electric spark mechanical steel surface moving over a planed bronze surface. Changes of the rigid body displacement, as well as the average and maximum pressures are also presented during sliding.

The micro-contact or asperity contact behaviour for bodies having large nominal contact area and the macro-contact behaviour for bodies being in 'concentrated contact' are also compared. In the latter case an ideal smooth steel ball was slid over the previously mentioned bronze surface.     

Modeling the edge contact effect of finite contact lines on subsurface stresses

Finite contact line conditions lead to subsurface stress distributions determined by the free boundaries. Combined with a correction procedure, Semi-Analytical Methods (SAMs) accurately include the free boundary effects, and represent a rapid alternative to the Finite Element Method (FEM) for contact pressure calculation. This paper extends the free boundary correction procedure to the evaluation of surface and subsurface stresses from SAMs. The investigation integrates a validation based on a two-level factorial comparison confronting the stress distributions established with the developed procedure to results obtained from FEM models. The comparison examines three dimensionless factors, and shows that the stress distributions are evaluated with a high level of precision. The model also offers evaluation more than 125 times faster than FEM simulations.     

A model of thermal contact conductance at high real contact area fractions

Thermal contact conductance (TCC) is studied in the whole range of real contact area fractions between zero and unity. For this purpose, a two-scale model is developed in which the effective (macroscopic) TCC coefficient is obtained from the solution of the heat conduction problem at the scale of asperities. Additional thermal resistance at the real contact spots is included in the model. The model is applied for several real 3D roughness topographies for which the effective TCC coefficient is determined as a function of the real contact area fraction and the local TCC coefficient at real contact spots. An analytical function is found which approximates this relationship in the whole range of parameters, and a characteristic length-scale parameter is introduced which characterizes the effective TCC properties of a rough surface.     

Self-levitating sliding air contact

A linear sliding contact with self-lifting capability due to squeeze film action was theoretically investigated. It was found that this type of contact can operate under a wide range of frequency and load conditions. Calculations for frequency of up to 4000 Hz and the mass of up to 800 g indicate that a air film with thickness of a few microns can be created.It is the unsymmetrical pressure distribution in a time period or positive mean film force that makes squeeze air film contact able of self-levitation. The mean film force is equal to the weight supported. A physical rationale for the load-carrying capacity of a squeeze air film is that because of the viscous resistance around contact boundary, the air is repeatedly compressed and expanded in the central part of the contact, which results in a positive mean film force.