Large Scale Fabrication of Quasi-Aligned ZnO Stacking Nanoplates

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复合材料英汉词汇

复合材料英汉词汇

复合材料英汉词汇Fabric composites||织物复合材料Fabric impregnation||织物浸渍Fabric preform||织物预成型Fabric prereg||织物预浸料Fabrication parameter||制造参数Fabrication procedure||制造工序Fabricating machinery||加工设备Face plate coupling||法兰式连接Factory primer||工厂底漆,工厂防锈漆Fairing||整流罩,整流装置Fairing panel||前裙板Fascia bracket||仪表板支架Fascia mask||仪表板罩板Fastening clamp||夹紧装置,紧固夹子Fatigue tension test||拉伸疲劳性试验FCM(Fibrous Composite material)||纤维复合材料FEA(Finite Element Anlysis)||有限元分析Feed system||供料系统Feeding pump||供给泵Feeding speed||进给速度Female groove||凹模Female mould(tooling)||阴模Fender||翼子板;护板Fender apron||挡泥板Fender inner panel||翼子板内衬护板Fiber composite laminate||纤维复合材料层板Fiber mat layer||纤维毡层Finisher(Finishing component)||装饰件Flange||法兰, 凸缘Flange fitting||法兰式管接头Flash||毛边Flash mold||毛边模具Front sheet metal||车前板制件Fuselage fairing||机身整流装置Gage kit||仪表组,仪表套件Gas cavity||气泡,砂眼Gauge panel||仪表板Gear assembly||齿轮传动装置, 减速器Gearbox cover||变速器壳盖Gear bracket support||齿轮托支架Gel coat||胶衣,凝胶涂层Gel coat drum||胶衣圆桶Gel coat flow monitor||胶衣流量监控器Gel time||凝胶时间Glass fiber winding machine||玻璃纤维缠绕机Glass wool||玻璃棉Glass yarn||玻璃丝Guiding device||导向装置Gunk||预混料Gusset||角撑件Gutter channel||流水槽Hand lay-up ||手工铺叠,手工铺贴Hardness testing machine||硬度测试仪Hauling truck||拖车Header board outside panel||前板外板Headrest||靠枕Heat barrier material||隔热材料Heat forming||热成型High molecular material||高分子材料High pressure bag molding||高压袋成型工艺High pressure injection moulding||高压注射成型,高压注射模塑High-strength structural adhesives||高强度结构粘合剂High temperature coating||高温涂层Hose support||软管支架Hub assembly||毂组件Hub bearing||车轮轮毂轴承Hydraulic device||液压装置Hydraulic engine||液压发动机Hydrostatic strength||流体静力强度IMC(In-Mold Coating)||模具内部涂层Immersion paint||浸漆Immersion test||浸渍试验,浸泡试验Immovable support||固定刀架Impact analysis||碰撞试验撞击分析Impact bending||冲击挠曲Impact specimen||冲击试样Impegnate||浸渍Impelling strength||冲击韧性Injection head||注射头Injection-moulded composites||注射模塑复合材料Injection moulded part||注塑制件Injection nozzle||注射喷口,压注喷口Intermittent entry||间歇供给,不连续供给Intermittent failure||间接性故障Izod test||悬臂冲击试验Jack||千斤顶,起重器;传动装置Jack engine||辅助发动机Jackbit insert||切刀,刀具,刃口Jacket||护套,套管,保护罩,蒙皮Jar-proof||防震的Jaw||钳口;定位销Jell||胶凝,凝固,固结Jet milling||喷射研磨Jig||夹具,定位模具Jig-adjusted||粗调的Job program||工作程序Joining nipple||接合螺管Joining on butt||对头接合Joint face of a pattern||分模面Joint gate||分型面内浇口Joint packing||填充垫圈,接合填密Joint sealing material||填缝料Joint-shaped support||铰接支架Joint strenght||连接强度Jump welded tube||对缝焊管,焊接管Junction bolt||接合螺栓Junction point||接点Keeping life||保存期,产品有效期Kenel||型芯Ketene||乙烯酮, 烯酮Ketene dimethyl||二甲酮Ketimide||酰基酮亚胺Ketimine||酮亚胺Ketoamine||酮胺,氨基酮Ketol||乙酮醇Ketone||甲酮Keying strength||咬合强度Knife holder||刀具,刀架Knockout||脱模Knockout pin||脱模销Knockout plate||脱模板Knoop scale||努氏硬度标度Knuckle joint||铰链连接Koplon||高湿模量粘胶纤维Koroseal||氯乙烯树脂Lacquer||挥发性漆;涂漆Lacquer finish||喷漆,上漆,罩光Lacquer formation||漆膜形成,成漆Lacquer putty||腻子,整面用油灰Lacquering ||上清漆Laminate construction thickness||结构层厚度Laminated panel||薄层状板Laminated plastics||层压塑料制品, 塑料层板Laminated thermosetting plastics||层压热固塑料Latex paints ||清漆Lay-up||(塑料,夹板的)铺叠成型Light-alloy body part||轻合金车身零件Lining ||衬里,衬垫Loaded haul cycle||载货行程Location bearing||定位轴承Location guide||固定导杆,定位导杆Location hole||定位孔Location tolerance||位置公差, 安装公差Locatin pin||定位销Lock bolt||锁紧螺钉Low pressure injection moulding||低压模塑成型Low shrink resin||低收缩树脂Luggage rack||行李架Machining accuracy||加工精度Machining center||加工中心Main shaft gear bushing||主轴齿轮衬套Mandrel ||卷芯,模芯;芯轴Manifold hood||歧管外罩Manual Lay-Up||人工手糊Manual spray-up||手工喷射Manual truck||手推车Manufacturing drawing||制造图纸Matched molds||合模Matrix ||基体,基质Mechanical properties||机械性能Metal bonding||金属粘结Metal-working machine||金属加工机床Methanol||甲醇Mismachining tolerance||加工误差Modular||组装式的Mofulus of elasticity||弹性模量Mould operation||模具操作Moulded plastics||模压塑料Moulding||嵌条;成型;装饰件Mount support||装配支架Multi-axial stress||多轴向应力Multi-tool machining||多刀切削加工Needled mat||针刺毡,针织毡Non-ductile fracture||无塑性破坏Nontwisting fiber||不加捻纤维Notched izod test||带缺口悬臂梁式冲击试验Nozzle||管嘴,喷嘴Numerically controlled engine lathe||数控普通车床Nylon resin||尼龙树脂OEM (Original Equipment Manufacturer) ||原始设备生产商Offset cab||侧置驾驶室On-site forming||现场发泡On-site winding||现场缠绕成型Open molding||敞开式模塑法Opening mould||开模Optimized design||优化设计Orifice||注孔Orthophenyl tolyl ketone||邻苯基甲苯基酮Orthophthalic resin ortho||邻苯二甲酸树脂Osmotic pressure||渗透压力Outboard wing||外翼Outer panel skin||蒙皮Oven heating||烘箱加热,加热固化Over-engineering||过份设计的Over flow||溢流Over-spray||过喷Overhead traveling crane||高空移动行车Overhead-valve engine||顶置气门发动机Overhung trailer||外伸式拖车Oxide paint||氧化物涂料Package power||动力装置总成Packed ||紧密的,密实的;有密封的,有填料的Packing||衬垫;填料,密封填料;包装PAD(Paint As Required)||按需涂漆Paint base coat||上底漆Paint blemish||涂漆缺陷Paint blower||喷漆用压力机,喷漆枪Paint brush||涂漆刷Paint dilution||油漆稀释PE(Polyethlene)||聚乙烯Pedestal mounted||落地安装的Phenolic plastic||酚醛塑料Phenyl ketone||苯基甲酮Pit mounted||嵌入式安装Pivotal arm||枢轴Platic structural component||塑料结构零部件Plastic upholstery||(座椅)塑料蒙面Play compensation||间隙补偿PLC(Programmable Logical Controller) ||可编程序逻辑控制器Polycarbonate plastics||聚碳酸脂塑料Polyester resin||聚脂树脂Polyimide||聚酰亚胺Polymer||聚合物,高分子,多聚体Polyurethane foam||聚氨酯泡沫塑料Polyvinyl||聚乙烯的, 聚乙烯Polyvinyl fluoride||聚氟乙烯Prefabricated parts||成品零部件,制造好的零部件Propylene resin||丙烯类树脂Protecting lacquer||防护漆PSF(Polystyrene Foam)||聚苯乙烯泡沫塑料PTFE(Polytetrafluoroethylene)||聚四氟乙烯Pultrusion||拉挤成型Putty knife||油灰(腻子)刮铲QC(Quality Control)||质量控制QCS(Quality Control Standard)||质量管理控制标准QR(Quality Requirements)||质量规格(要求)Quality certification||质量认证Quantity production||大量(成批)生产,大规模生产Quantity production||大量(成批)生产,大规模生产Quarter panel brace||后侧围板支撑件Quarter panel lower extension||后侧围板下延伸部Quarter trim cap||后侧围装饰板盖Quarte wheel house||后侧围轮滚罩,后侧围车轮室Quasi-isotropic laminate||准各向同性层板Quench||淬火Rack truck||架子车, 移动架Radial dispersion||径向位移Radial loading||径向力(载荷)Radial pump||径向离心泵Radiation protective paint||防辐射涂料Radiator||散热器Rag||毛刺RARTM(Rubber-assisted RTM)||橡胶辅助RTM(用橡胶取代芯材的热膨胀RTM) Reactive resin||活性树脂, 反应型树脂Rear skirt rail||后围裙边梁Reciprocating engine||活塞式发动机, 往复式发动机Reinforcement||车身加强件,增强材料;构架Repeat accuracy||重复精确度Repeatability||设备重复定位精度Resin formulation||树脂配方Retaining nest||定位槽Return trip||回程,返回行程Rib||筋,加强筋RIFT(Resin Infusion Under Flexible Tooling)||挠性上模具树脂浸渍工艺RIM(Reaction Injection Molding)||反应注射模塑Safety hood||安全罩Sample testing||样品试验Sand wet||(车身/涂装)湿砂打磨Sandwich body||夹层结构车身Sandwich construction||夹层结构Sandwich panel||多层板,复合板Shaft assembly||轴组件Skin coat||表层;罩面层Solvent reclaim||溶剂的回收Stiffener||加强件Storage modulus||储能模量Stress at definite elongation||定伸应力Stretched actylic plastic||拉伸丙烯酸塑料String milling||连续铣削Stroke||(悬架)减振器,冲程Structural instrument panel||结构仪表板Structural layer||结构层Styrene||苯乙烯Styrofoam||聚苯乙烯泡沫塑料Surface mat||表面薄毡Synthetic resin paint||合成树脂涂料Tack strength||粘着强度Tail gate||(卡车等的)后挡板Teflon||聚四氟乙烯(塑料, 绝缘材料)TERTM(Thermal-Expansion Resin Transfer Molding)||热膨胀树脂传递模塑Thermoplastic plastics||热塑性塑料Thermoset resin||热固性树脂Thickening agent||增粘剂Trim waste||内饰废料Trimming orientation||修边定位Turbulent heating||湍流加热Turndown ratio||衰减比率Twisting stress||扭胁强, 扭应力U bolt||U形螺栓U bolt plate||U 形螺栓垫板Ultimate mechanical strength||极限机械强度Ultraviolent sensitive coating||紫外线感光涂层Undercoat paint||头道漆Uniaxial drawing||单轴拉伸Unsaturated polyester resin||非饱和聚酯树脂Unyielding support||不可压缩支架, 刚性支架Upper yield stress||上屈服应力Urethane coating||氨基甲酸乙酯涂层UVRTM(Ultra-violet RTM)||紫外线固化RTM(利用紫外线进行固化)VA RTM (Vacuum Assisted Resin Transfer Molding) ||真空辅助RTM Vacuum bag molding||真空袋模制法VARI(Vacuum Assisted Resin njection)||真空辅助树脂注射Variable speed||无级变速Ventilation duct||通风管Ventilator(Ventilating equipment)||通风装置Vibratory stress||振动应力VIMP (Variable Infusion Molding Process)||可变浸渍模塑Vinyl chloride resin||聚氯乙烯树脂VOC(Volatile Organic Compound)||挥发性有机化合物Volume modulus||体积模数Vortex generator||(车身)扰流器,导流板VRV(Vacuum Reducer Valve)||真空减压阀Warping stress||翘曲应力Waste utilization||废物利用,废物处理Water shield||防水罩,挡泥板;密封条Water tolerance||耐水性Wedge gripping||楔形夹具Wheel fender||翼子板Wing trussgrid||翼子(挡泥)板加强件Winding||缠绕Wingtip assembly||翼尖整流罩Wire drawing||拉丝Wiring press||卷边压力机, 嵌线卷边机Workpiece grippe||工件夹子(持器),机械手Woven roving fabric||(玻璃纤维)无捻粗纱布织物Xylenol Carboxylic Acid||二甲苯酚酸Xlylene||亚二甲苯基Xyster||刮刀X alloy||铜铝合金Xenidium||胶合板Xenidium||胶合板Xylene ||二甲苯Xylene resin||二甲苯树脂Yard-crane||移动吊车,场内移动起重机Yarn count||纱线支数,丝线支数Yarn strength||纱线强度,长丝强度Yield limit||屈服极限,屈服点Yield point under bending stress||弯曲应力下的屈服点Yield stress||屈服应力, 屈服点Yield stress controlled bonding||屈服应力粘结Zedeflon||四氟乙烯均聚物Zero checker||定零位装置, 零位校验Zero clearance||零间隙Zero compensation||零位补偿Zero initial condition||零初始条件Zero setting||(仪表)零位调整, 置零Zero shrinkage resin||零收缩树脂Zone control||区域控制复合材料Acetyl 乙酰Acid-proof paint 耐酸涂料, 耐酸油漆Acrylic fiber 丙烯酸纤维Acrylic resin 丙烯酸树脂Active filler 活性填料Adapter assembly 接头组件Addition polyimide 加成型聚酰亚胺Addition polymer 加聚物Adjusting valve 调整阀,调节阀Adhersion assembly 粘合装配Adhersion bond 胶结Adjustable-bed press 工作台可调式压力机Adjuster shim 调整垫片Adjusting accuracy 调整精度,调校精度Admissible error 容许误差Admissible load 容许载荷Adsorbed layer 吸附层Advanced composite material 先进复合材料,高级复合材料Advanced development vehicle 试制车,预研样车AE(Automobile Engineering) 汽车工程技术Aeolotropic material 各向异性材料Aerated plastics 泡沫塑料, 多孔塑料Aerodynamic body 流线型车身Aft cross member 底盘/车架后横梁Air bleeder 排气孔Air clamp 气动夹具Air deflector 导流板;导风板,气流偏转板Air intake manifold 进气歧管Air servo 伺服气泵Air-tight joint 气密接头All-plastic molded 全塑模注的All polyster seat 全聚酯座椅Alligatoring 龟裂,涂膜皱皮,表面裂痕Amino resin 氨基树脂Angular test 挠曲试验Anti-chipping primer 抗破裂底漆(底层涂料)Apron 防护挡板Aramid fibre composites 芳胺纤维复合材料Assembly drawing 装配图Assembly jig 装配夹具Assembly part 装配件,组合件Autoclave forming 热压罐成型Autocorrection 自动校正Automatic compensation 自动补偿Automatic feed 自动进料Automobile instrument 汽车仪表板Automotive transmission 汽车传动装置,汽车变速器Auxiliary fasia console 副仪表板Axial strain 轴向应变Axle bushing 轴衬Axle fairing 底盘车桥整流罩A Stage A 阶段(某些热固性树脂聚合作用的初期阶段)AAC(Auxiliary Air Control) 辅助空气控制ABC(Active Body Control) 主动式车身控制装置Abherent 阻粘剂Ability meter 测力计,性能测试仪ABL (Ablative) 烧蚀剂Ablation 烧蚀Ablative composite material 烧蚀复合材料Ablative insulative material 烧蚀绝热材料Ablative polymer 烧蚀聚合物Ablative prepreg 烧蚀性预浸料Ablative resistance 耐烧蚀性ABR(Acrylate Butadience Rubber) 丙烯酸丁二烯橡胶Abradant material 研磨材料,磨料Abrade 研磨;用喷砂清理Abrasion 磨耗Abrasion coefficient 磨耗系数Abrasion loss 磨耗量,磨损量Abrasion performance 磨耗性Abrasion-proof material 耐磨材料Abrasion resistant paint 耐磨涂料Abrasion test 磨损试验Abrasive blast system 喷砂清理系统Abrasive cloth 砂布Abrasive disc 砂轮盘,砂轮片Abrasive finishing 抛光Abrasive paper 砂纸Abrasive resistance 耐磨性ABS(Acrylonitrile Butadiene Styrene)resin ABS树脂,丙烯腈-丁二烯-苯乙烯(热塑性)树脂ABSM(American Bureau of Standard Materials) 美国标准材料局Absolute dynamic modulus 绝对动态模量Absolute error 绝对误差Absorbent material 吸收性材料,吸收性物质,吸声材料,吸收剂Absorber 减振器,阻尼器,缓冲器ACA(Automotive Composite Alliance) 汽车复合材料协会ACC(Automatic Clutch Control) 自动离合器操纵控制Accelerant 促进剂,加速剂Accelerated aging test 加速老化试验,人工老化试验Accelerator pedal shaft 加速踏板轴Accelerator pump nozzle 加速泵喷嘴Acceptable life 有效使用寿命Acceptance test specification 验收测试规范Access panel 罩板,盖板Accessory 配件,附属品Accessory equipment 辅助设备Accessory kit 附件包,成套附件Accumulator can 储电池外壳Accumulator package 蓄压器组件,蓄压器单元Accuracy in calibration 校准精度Accuracy of finish 最终加工精度Accuracy of manufacture 制造精度Accuracy of positioning 定位精度Accuracy of repetition 重现精度,复制精度Acetal matrix composites 缩醛树脂基复合材料Acetal plastic 缩醛塑料,聚甲醛塑料Acetal resin 缩醛树脂Acetamide 乙酰胺Acetate fiber 醋酸纤维,乙酸纤维Acetone 丙酮Back corner panel 后围角板Back panel 后围板Back side panel 后侧板Back wall pillar 后围立柱Backer 衬料Baffler 挡板,阻尼器;导流叶片Bag Molding 气囊施压成型(袋模法)Baggage holder 行李架Barrier coat 阻挡层;防渗涂层Batch mixing 分批混合,批混Batching unit 分批加料装置Bearing assembly 轴承组合件Biaxial winding 双角缠绕, 双轴缠绕Binder fiber 粘合纤维Bipolymer 二元共聚物Bismaleimide composites 双马来酰亚胺复合材料Blank placement 坯料的放置Blanket 玻璃纤维毡;坯料Blanking press 冲压机, 冲割压力机Blending resin 掺合树脂BMC(Bulk Moulding Compound) 团状膜塑料BMI (Bismaleimide) 双马来酰亚胺Body back panel 车身后板Body back wall 车身驾驶室后围Body bracket 车身支架Body control module 车身控制模块Body frame (Body skeleton) 车身骨架Body front panel 车身驾驶室前围板Body monocoque 单壳体车身,单壳式结构车身Body outer panel 驾驶室覆盖件;驾驶室覆盖件Body structural member 车身结构件Body trim 车身装饰件Bonded riveted structure 胶铆结构Bonnet 发动机罩Brake 制动器Brake arrangement 制动装置Brinell hardness test 布氏硬度试验Brittle coating 脆性涂层Bulk coat 整体涂层Bulk heat treatment 整体热处理Bulk moulding compound (增强塑料)预制整体模塑料Bumper bracket(holder) 保险杠托架Bus brake system 客车制动系Butt flange 对接法兰Butt joint 对接接头;对接Butterfly valve 节流阀,节气门BWI (Body In White) 白车身Cab deflector shield 驾驶室导流板Cab fairing 驾驶室整流罩Cab floor 驾驶室地板Cab mounting 驾驶室悬置CAD(Computer Aided Design) 计算机辅助设计CAE (Computer Aided Engineering) 计算机辅助工程设计Calibration tolerance 校准公差Calibrating instrument 校准仪表Camouflage paint 覆面漆, 盖面涂料, 伪假漆Cantilever beam impact test 悬臂梁冲击试验Carbon-felt reinforced carbon composites 碳毡增强碳复合材料Carbon fiber clutch 碳纤维离合器Carbon filament cloth 碳丝织物Case extension 外壳的伸出部分,延伸外壳Casing gasket 外壳密封垫Catalyst manifold 固化剂总成Catalyst pump 固化剂泵Catalyst ratio 固化剂比率Cavity 模槽,型腔;凹模Cavity block 阴模Cavity depth 模槽深度Cellular board 蜂窝状板,多孔板Cellular plastics 泡沫塑料,多孔塑料Centre boss 轮毂Centre pin 销轴,枢轴,主销Centrifugal casting moulding 离心浇铸成型Centrosymmetry 中心对称层板Ceramic matrix composites 陶瓷基复合材料Charge 填充气体,填充料Chasis 底盘;机壳,车架Chlorinated polyethlene 聚氯乙烯Chopped fiber 短切纤维Chopped random mat 短切无序毡Chopped strand 短切原丝CIRTM(Co-Injection RTM) 共注射RTM Clamping fixture 夹具,夹紧装置Clamping force 夹持力,合模力Class A surface A级表面Clear coat 透明涂层,透明罩漆,清漆层Clear coat finish 清漆涂层Clicker die 冲模Climb milling 同向铣削, 顺铣Clipping press 切边压力机Closure pressing speed 合模速度CMM(Closed Mould Moulding) 闭合模塑CMT(Compression Molding 挤压成型工艺CNC(Computerized Numerical Control)电脑数值控制Coarse grinding 粗磨,用砂轮初加工Coating defect 涂层缺陷Collision test 碰撞试验,撞车试验Combination property 综合性能Concept design 概念设计Convection modulus 对流模量Convergence test 收敛试验Cooling fixture 冷却夹具Cooling tower 冷却塔Crazing 龟裂,细裂纹Cresol resin 甲酚树脂Cutting felt 毡的剪切Cutting-off bushing 环形下料模; 下料环Damped structure 阻尼缓冲结构Damper bracket 件振器支架Dashboard illumination 仪表板照明Dash trimming 前围板衬板Deburring 去毛刺,倒角,除飞边Deepdrawing forming 深拉成型Deflection test 挠曲试验Dent resistance 耐冲击性Design freedom 设计自由度Detail drawing 祥图,零件图Die assembly 压模装置Die casting 压模铸件,压模铸法Dimethyl fomamide 二甲基甲酰胺Dimethyl ketone 二甲基甲酮; 丙酮Dip pretreatment 浸渍预处理Die prime coat 浸渍打底漆Dimensional stability 尺寸稳定性Dip coating 浸涂Dip forming 浸渍成型Durability testing 耐久性试验,寿命试验Dwell 保压,暂停加压;滞留时间Dynamometer 测力计Edge effect 边缘效应,边界效应Edge feed 边缘进料Edge gate 侧浇口Ejection force 脱模力Ejector 起模杆Ejector guide pillar 推板导套Ejector housing 支架Elasticizer 增塑剂Elastomeric composites 高弹体复合材料Elongation at break 断裂延伸率Energy absorbing foam 吸能泡沫塑料Epoxy resin 环氧树脂Ether ketone 酮醚Explosion proof 防爆Exterior body panelling 车身外板部蒙皮Exterior trim 外饰,外饰件Fabric composites 织物复合材料Fabric impregnation 织物浸渍Fabric preform 织物预成型Fabric prereg 织物预浸料Fabrication parameter 制造参数Fabrication procedure 制造工序Fabricating machinery 加工设备Face plate coupling 法兰式连接Factory primer 工厂底漆,工厂防锈漆Fairing 整流罩,整流装置Fairing panel 前裙板Fascia bracket 仪表板支架Fascia mask 仪表板罩板Fastening clamp 夹紧装置,紧固夹子Fatigue tension test 拉伸疲劳性试验FCM(Fibrous Composite material) 纤维复合材料FEA(Finite Element Anlysis) 有限元分析Feed system 供料系统Feeding pump 供给泵Feeding speed 进给速度Female groove 凹模Female mould(tooling) 阴模Fender 翼子板;护板Fender apron 挡泥板Fender inner panel 翼子板内衬护板Fiber composite laminate 纤维复合材料层板Fiber mat layer 纤维毡层Finisher(Finishing component) 装饰件Flange 法兰, 凸缘Flange fitting 法兰式管接头Flash 毛边Flash mold 毛边模具Front sheet metal 车前板制件Fuselage fairing 机身整流装置Gage kit 仪表组,仪表套件Gas cavity 气泡,砂眼Gauge panel 仪表板Gear assembly 齿轮传动装置, 减速器Gearbox cover 变速器壳盖Gear bracket support 齿轮托支架Gel coat 胶衣,凝胶涂层Gel coat drum 胶衣圆桶Gel coat flow monitor 胶衣流量监控器Gel time 凝胶时间Glass fiber winding machine 玻璃纤维缠绕机Glass wool 玻璃棉Glass yarn 玻璃丝Guiding device 导向装置Gunk 预混料Gusset 角撑件Gutter channel 流水槽Hand lay-up 手工铺叠,手工铺贴Hardness testing machine 硬度测试仪Hauling truck 拖车Header board outside panel 前板外板Headrest 靠枕Heat barrier material 隔热材料Heat forming 热成型High molecular material 高分子材料High pressure bag molding 高压袋成型工艺High pressure injection moulding 高压注射成型,高压注射模塑High-strength structural adhesives 高强度结构粘合剂High temperature coating 高温涂层Hose support 软管支架Hub assembly 毂组件Hub bearing 车轮轮毂轴承Hydraulic device 液压装置Hydraulic engine 液压发动机Hydrostatic strength 流体静力强度IMC(In-Mold Coating) 模具内部涂层Immersion paint 浸漆Immersion test 浸渍试验,浸泡试验Immovable support 固定刀架Impact analysis 碰撞试验撞击分析Impact bending 冲击挠曲Impact specimen 冲击试样Impegnate 浸渍Impelling strength 冲击韧性Injection head 注射头Injection-moulded composites 注射模塑复合材料Injection moulded part 注塑制件Injection nozzle 注射喷口,压注喷口Intermittent entry 间歇供给,不连续供给Intermittent failure 间接性故障Izod test 悬臂冲击试验Jack 千斤顶,起重器;传动装置Jack engine 辅助发动机Jackbit insert 切刀,刀具,刃口Jacket 护套,套管,保护罩,蒙皮Jar-proof 防震的Jaw 钳口;定位销Jell 胶凝,凝固,固结Jet milling 喷射研磨Jig 夹具,定位模具Jig-adjusted 粗调的Job program 工作程序Joining nipple 接合螺管Joining on butt 对头接合Joint face of a pattern 分模面Joint gate 分型面内浇口Joint packing 填充垫圈,接合填密Joint sealing material 填缝料Joint-shaped support 铰接支架Joint strenght 连接强度Jump welded tube 对缝焊管,焊接管Junction bolt 接合螺栓Junction point 接点Keeping life 保存期,产品有效期Kenel 型芯Ketene 乙烯酮, 烯酮Ketene dimethyl 二甲酮Ketimide 酰基酮亚胺Ketimine 酮亚胺Ketoamine 酮胺,氨基酮Ketol 乙酮醇Ketone 甲酮Keying strength 咬合强度Knife holder 刀具,刀架Knockout 脱模Knockout pin 脱模销Knockout plate 脱模板Knoop scale 努氏硬度标度Knuckle joint 铰链连接Koplon 高湿模量粘胶纤维Koroseal 氯乙烯树脂Lacquer 挥发性漆;涂漆Lacquer finish 喷漆,上漆,罩光Lacquer formation 漆膜形成,成漆Lacquer putty 腻子,整面用油灰Lacquering 上清漆Laminate construction thickness 结构层厚度Laminated panel 薄层状板Laminated plastics 层压塑料制品, 塑料层板Laminated thermosetting plastics 层压热固塑料Latex paints 清漆Lay-up (塑料,夹板的)铺叠成型Light-alloy body part 轻合金车身零件Lining 衬里,衬垫Loaded haul cycle 载货行程Location bearing 定位轴承Location guide 固定导杆,定位导杆Location hole 定位孔Location tolerance 位置公差, 安装公差Locatin pin 定位销Lock bolt 锁紧螺钉Low pressure injection moulding 低压模塑成型Low shrink resin 低收缩树脂Luggage rack 行李架Machining accuracy 加工精度Machining center 加工中心Main shaft gear bushing 主轴齿轮衬套Mandrel 卷芯,模芯;芯轴Manifold hood 歧管外罩Manual Lay-Up 人工手糊Manual spray-up 手工喷射Manual truck 手推车Manufacturing drawing 制造图纸Matched molds 合模Matrix 基体,基质Mechanical properties 机械性能Metal bonding 金属粘结Metal-working machine 金属加工机床Methanol 甲醇Mismachining tolerance 加工误差Modular 组装式的Mofulus of elasticity 弹性模量Mould operation 模具操作Moulded plastics 模压塑料Moulding 嵌条;成型;装饰件Mount support 装配支架Multi-axial stress 多轴向应力Multi-tool machining 多刀切削加工Needled mat 针刺毡,针织毡Non-ductile fracture 无塑性破坏Nontwisting fiber 不加捻纤维Notched izod test 带缺口悬臂梁式冲击试验Nozzle 管嘴,喷嘴Numerically controlled engine lathe 数控普通车床Nylon resin 尼龙树脂OEM (Original Equipment Manufacturer) 原始设备生产商Offset cab 侧置驾驶室On-site forming 现场发泡On-site winding 现场缠绕成型Open molding 敞开式模塑法Opening mould 开模Optimized design 优化设计Orifice 注孔Orthophenyl tolyl ketone 邻苯基甲苯基酮Orthophthalic resin ortho 邻苯二甲酸树脂Osmotic pressure 渗透压力Outboard wing 外翼Outer panel skin 蒙皮Oven heating 烘箱加热,加热固化Over-engineering 过份设计的Over flow 溢流Over-spray 过喷Overhead traveling crane 高空移动行车Overhead-valve engine 顶置气门发动机Overhung trailer 外伸式拖车Oxide paint 氧化物涂料Package power 动力装置总成Packed 紧密的,密实的;有密封的,有填料的Packing 衬垫;填料,密封填料;包装PAD(Paint As Required) 按需涂漆Paint base coat 上底漆Paint blemish 涂漆缺陷Paint blower 喷漆用压力机,喷漆枪Paint brush 涂漆刷Paint dilution 油漆稀释PE(Polyethlene) 聚乙烯Pedestal mounted 落地安装的Phenolic plastic 酚醛塑料Phenyl ketone 苯基甲酮Pit mounted 嵌入式安装Pivotal arm 枢轴Platic structural component 塑料结构零部件Plastic upholstery (座椅)塑料蒙面Play compensation 间隙补偿PLC(Programmable Logical Controller) 可编程序逻辑控制器Polycarbonate plastics 聚碳酸脂塑料Polyester resin 聚脂树脂Polyimide 聚酰亚胺Polymer 聚合物,高分子,多聚体Polyurethane foam 聚氨酯泡沫塑料Polyvinyl 聚乙烯的, 聚乙烯Polyvinyl fluoride 聚氟乙烯Prefabricated parts 成品零部件,制造好的零部件Propylene resin 丙烯类树脂Protecting lacquer 防护漆PSF(Polystyrene Foam) 聚苯乙烯泡沫塑料PTFE(Polytetrafluoroethylene) 聚四氟乙烯Pultrusion 拉挤成型Putty knife 油灰(腻子)刮铲QC(Quality Control) 质量控制QCS(Quality Control Standard) 质量管理控制标准QR(Quality Requirements) 质量规格(要求)Quality certification 质量认证Quantity production 大量(成批)生产,大规模生产Quantity production 大量(成批)生产,大规模生产Quarter panel brace 后侧围板支撑件Quarter panel lower extension 后侧围板下延伸部Quarter trim cap 后侧围装饰板盖Quarte wheel house 后侧围轮滚罩,后侧围车轮室Quasi-isotropic laminate 准各向同性层板Quench 淬火Rack truck 架子车, 移动架Radial dispersion 径向位移Radial loading 径向力(载荷)Radial pump 径向离心泵Radiation protective paint 防辐射涂料Radiator 散热器Rag 毛刺RARTM(Rubber-assisted RTM) 橡胶辅助RTM(用橡胶取代芯材的热膨胀RTM) Reactive resin 活性树脂, 反应型树脂Rear skirt rail 后围裙边梁Reciprocating engine 活塞式发动机, 往复式发动机Reinforcement 车身加强件,增强材料;构架Repeat accuracy 重复精确度Repeatability 设备重复定位精度Resin formulation 树脂配方Retaining nest 定位槽Return trip 回程,返回行程Rib 筋,加强筋RIFT(Resin Infusion Under Flexible Tooling) 挠性上模具树脂浸渍工艺RIM(Reaction Injection Molding) 反应注射模塑Safety hood 安全罩Sample testing 样品试验Sand wet (车身/涂装)湿砂打磨Sandwich body 夹层结构车身Sandwich construction 夹层结构Sandwich panel 多层板,复合板Shaft assembly 轴组件Skin coat 表层;罩面层Solvent reclaim 溶剂的回收Stiffener 加强件Storage modulus 储能模量Stress at definite elongation 定伸应力Stretched actylic plastic 拉伸丙烯酸塑料String milling 连续铣削Stroke (悬架)减振器,冲程Structural instrument panel 结构仪表板Structural layer 结构层Styrene 苯乙烯Styrofoam 聚苯乙烯泡沫塑料Surface mat 表面薄毡Synthetic resin paint 合成树脂涂料Tack strength 粘着强度Tail gate (卡车等的)后挡板Teflon 聚四氟乙烯(塑料, 绝缘材料)TERTM(Thermal-Expansion Resin Transfer Molding) 热膨胀树脂传递模塑Thermoplastic plastics 热塑性塑料Thermoset resin 热固性树脂Thickening agent 增粘剂Trim waste 内饰废料Trimming orientation 修边定位Turbulent heating 湍流加热Turndown ratio 衰减比率Twisting stress 扭胁强, 扭应力U bolt U形螺栓U bolt plate U 形螺栓垫板Ultimate mechanical strength 极限机械强度Ultraviolent sensitive coating 紫外线感光涂层Undercoat paint 头道漆Uniaxial drawing 单轴拉伸Unsaturated polyester resin 非饱和聚酯树脂Unyielding support 不可压缩支架, 刚性支架Upper yield stress 上屈服应力Urethane coating 氨基甲酸乙酯涂层UVRTM(Ultra-violet RTM) 紫外线固化RTM(利用紫外线进行固化)VA RTM (Vacuum Assisted Resin Transfer Molding) 真空辅助RTM Vacuum bag molding 真空袋模制法VARI(Vacuum Assisted Resin njection) 真空辅助树脂注射Variable speed 无级变速Ventilation duct 通风管Ventilator(Ventilating equipment) 通风装置Vibratory stress 振动应力VIMP (Variable Infusion Molding Process) 可变浸渍模塑Vinyl chloride resin 聚氯乙烯树脂VOC(Volatile Organic Compound) 挥发性有机化合物Volume modulus 体积模数Vortex generator (车身)扰流器,导流板VRV(Vacuum Reducer Valve) 真空减压阀Warping stress 翘曲应力Waste utilization 废物利用,废物处理Water shield 防水罩,挡泥板;密封条Water tolerance 耐水性Wedge gripping 楔形夹具Wheel fender 翼子板Wing trussgrid 翼子(挡泥)板加强件Winding 缠绕Wingtip assembly 翼尖整流罩Wire drawing 拉丝Wiring press 卷边压力机, 嵌线卷边机Workpiece grippe 工件夹子(持器),机械手Woven roving fabric (玻璃纤维)无捻粗纱布织物Xylenol Carboxylic Acid 二甲苯酚酸Xlylene 亚二甲苯基Xyster 刮刀X alloy 铜铝合金Xenidium 胶合板Xenidium 胶合板Xylene 二甲苯Xylene resin 二甲苯树脂Yard-crane 移动吊车,场内移动起重机Yarn count 纱线支数,丝线支数Yarn strength 纱线强度,长丝强度Yield limit 屈服极限,屈服点Yield point under bending stress 弯曲应力下的屈服点Yield stress 屈服应力, 屈服点Yield stress controlled bonding 屈服应力粘结Zedeflon 四氟乙烯均聚物Zero checker 定零位装置, 零位校验Zero clearance 零间隙Zero compensation 零位补偿Zero initial condition 零初始条件Zero setting (仪表)零位调整, 置零Zero shrinkage resin 零收缩树脂Zone control 区域控制。

弹性力学专业英语词汇-elasticity

弹性力学专业英语词汇-elasticity

弹性力学专业英语词汇-elasticity环板Annular plate波纹板Corrugated plate加劲板Stiffened plate,reinforced Plate中厚板Plate of moderate thickness弯[曲]应力函数Stress function of bending 壳Shell扁壳Shallow shell旋转壳Revolutionary shell球壳Spherical shell[圆]柱壳Cylindrical shell锥壳Conical shell环壳Toroidal shell封闭壳Closed shell波纹壳Corrugated shell扭[转]应力函数Stress function of torsion 翘曲函数Warping function半逆解法semi-inverse method瑞利——里茨法Rayleigh-Ritz method松弛法Relaxation method莱维法Levy method松弛Relaxation量纲分析Dimensional analysis自相似[性] self-similarity影响面Influence surface接触应力Contact stress赫兹理论Hertz theory协调接触Conforming contact滑动接触Sliding contact滚动接触Rolling contact压入Indentation各向异性弹性Anisotropic elasticity颗粒材料Granular material散体力学Mechanics of granular media 热弹性Thermoelasticity超弹性Hyperelasticity粘弹性Viscoelasticity对应原理Correspondence principle褶皱Wrinkle塑性全量理论Total theory of plasticity 滑动Sliding微滑Microslip粗糙度Roughness非线性弹性Nonlinear elasticity大挠度Large deflection突弹跳变snap-through有限变形Finite deformation格林应变Green strain阿尔曼西应变Almansi strain弹性动力学Dynamic elasticity运动方程Equation of motion准静态的Quasi-static气动弹性Aeroelasticity水弹性Hydroelasticity颤振Flutter弹性波Elastic wave简单波Simple wave柱面波Cylindrical wave水平剪切波Horizontal shear wave 竖直剪切波Vertical shear wave体波body wave无旋波Irrotational wave畸变波Distortion wave膨胀波Dilatation wave瑞利波Rayleigh wave等容波Equivoluminal wave勒夫波Love wave界面波Interfacial wave边缘效应edge effect塑性力学Plasticity可成形性Formability金属成形Metal forming耐撞性Crashworthiness结构抗撞毁性Structural crashworthiness拉拔Drawing破坏机构Collapse mechanism回弹Springback挤压Extrusion冲压Stamping穿透Perforation层裂Spalling塑性理论Theory of plasticity安定[性]理论Shake-down theory运动安定定理kinematic shake-down theorem静力安定定理Static shake-down theorem率相关理论rate dependent theorem载荷因子load factor加载准则Loading criterion加载函数Loading function加载面Loading surface塑性加载Plastic loading塑性加载波Plastic loading wave 简单加载Simple loading比例加载Proportional loading 卸载Unloading卸载波Unloading wave冲击载荷Impulsive load阶跃载荷step load脉冲载荷pulse load极限载荷limit load中性变载nentral loading拉抻失稳instability in tension 加速度波acceleration wave本构方程constitutive equation 完全解complete solution名义应力nominal stress过应力over-stress真应力true stress等效应力equivalent stress流动应力flow stress应力间断stress discontinuity应力空间stress space主应力空间principal stress space静水应力状态hydrostatic state of stress对数应变logarithmic strain工程应变engineering strain等效应变equivalent strain应变局部化strain localization应变率strain rate应变率敏感性strain rate sensitivity应变空间strain space有限应变finite strain塑性应变增量plastic strain increment累积塑性应变accumulated plastic strain永久变形permanent deformation内变量internal variable应变软化strain-softening理想刚塑性材料rigid-perfectly plastic Material刚塑性材料rigid-plastic material理想塑性材料perfectl plastic material材料稳定性stability of material应变偏张量deviatoric tensor of strain应力偏张量deviatori tensor of stress应变球张量spherical tensor of strain应力球张量spherical tensor of stress路径相关性path-dependency线性强化linear strain-hardening应变强化strain-hardening随动强化kinematic hardening各向同性强化isotropic hardening强化模量strain-hardening modulus幂强化power hardening塑性极限弯矩plastic limit bending Moment塑性极限扭矩plastic limit torque弹塑性弯曲elastic-plastic bending弹塑性交界面elastic-plastic interface弹塑性扭转elastic-plastic torsion粘塑性Viscoplasticity非弹性Inelasticity理想弹塑性材料elastic-perfectly plastic Material极限分析limit analysis极限设计limit design极限面limit surface上限定理upper bound theorem上屈服点upper yield point下限定理lower bound theorem下屈服点lower yield point界限定理bound theorem初始屈服面initial yield surface后继屈服面subsequent yield surface屈服面[的]外凸性convexity of yield surface截面形状因子shape factor of cross-section沙堆比拟sand heap analogy屈服Yield屈服条件yield condition屈服准则yield criterion屈服函数yield function屈服面yield surface塑性势plastic potential能量吸收装置energy absorbing device能量耗散率energy absorbing device塑性动力学dynamic plasticity塑性动力屈曲dynamic plastic buckling塑性动力响应dynamic plastic response塑性波plastic wave运动容许场kinematically admissible Field静力容许场statically admissible Field流动法则flow rule速度间断velocity discontinuity滑移线slip-lines滑移线场slip-lines field移行塑性铰travelling plastic hinge塑性增量理论incremental theory of Plasticity米泽斯屈服准则Mises yield criterion普朗特——罗伊斯关系prandtl- Reuss relation特雷斯卡屈服准则Tresca yield criterion洛德应力参数Lode stress parameter莱维——米泽斯关系Levy-Mises relation亨基应力方程Hencky stress equation赫艾——韦斯特加德应力空间Haigh-Westergaard stress space洛德应变参数Lode strain parameter德鲁克公设Drucker postulate盖林格速度方程Geiringer velocity Equation结构力学structural mechanics结构分析structural analysis结构动力学structural dynamics拱Arch三铰拱three-hinged arch抛物线拱parabolic arch圆拱circular arch穹顶Dome空间结构space structure空间桁架space truss雪载[荷] snow load风载[荷] wind load土压力earth pressure地震载荷earthquake loading弹簧支座spring support支座位移support displacement支座沉降support settlement超静定次数degree of indeterminacy机动分析kinematic analysis结点法method of joints截面法method of sections结点力joint forces共轭位移conjugate displacement影响线influence line三弯矩方程three-moment equation单位虚力unit virtual force刚度系数stiffness coefficient柔度系数flexibility coefficient力矩分配moment distribution力矩分配法moment distribution method力矩再分配moment redistribution分配系数distribution factor矩阵位移法matri displacement method单元刚度矩阵element stiffness matrix单元应变矩阵element strain matrix总体坐标global coordinates贝蒂定理Betti theorem高斯——若尔当消去法Gauss-Jordan elimination Method屈曲模态buckling mode复合材料力学mechanics of composites复合材料composite material纤维复合材料fibrous composite单向复合材料unidirectional composite 泡沫复合材料foamed composite颗粒复合材料particulate composite层板Laminate夹层板sandwich panel正交层板cross-ply laminate斜交层板angle-ply laminate层片Ply多胞固体cellular solid膨胀Expansion压实Debulk劣化Degradation脱层Delamination脱粘Debond纤维应力fiber stress层应力ply stress层应变ply strain层间应力interlaminar stress比强度specific strength强度折减系数strength reduction factor强度应力比strength -stress ratio横向剪切模量transverse shear modulus横观各向同性transverse isotropy正交各向异Orthotropy剪滞分析shear lag analysis短纤维chopped fiber长纤维continuous fiber纤维方向fiber direction纤维断裂fiber break纤维拔脱fiber pull-out纤维增强fiber reinforcement致密化Densification最小重量设计optimum weight design网格分析法netting analysis混合律rule of mixture失效准则failure criterion蔡——吴失效准则Tsai-W u failure criterion达格代尔模型Dugdale model断裂力学fracture mechanics概率断裂力学probabilistic fracture Mechanics格里菲思理论Griffith theory线弹性断裂力学linear elastic fracture mechanics, LEFM弹塑性断裂力学elastic-plastic fracture mecha-nics, EPFM断裂Fracture脆性断裂brittle fracture解理断裂cleavage fracture蠕变断裂creep fracture延性断裂ductile fracture晶间断裂inter-granular fracture准解理断裂quasi-cleavage fracture穿晶断裂trans-granular fracture裂纹Crack裂缝Flaw缺陷Defect割缝Slit微裂纹Microcrack折裂Kink椭圆裂纹elliptical crack深埋裂纹embedded crack[钱]币状裂纹penny-shape crack预制裂纹Precrack短裂纹short crack表面裂纹surface crack裂纹钝化crack blunting裂纹分叉crack branching裂纹闭合crack closure裂纹前缘crack front裂纹嘴crack mouth裂纹张开角crack opening angle,COA裂纹张开位移crack opening displacement, COD裂纹阻力crack resistance裂纹面crack surface裂纹尖端crack tip裂尖张角crack tip opening angle, CTOA裂尖张开位移crack tip opening displacement, CTOD裂尖奇异场crack tip singularity Field裂纹扩展速率crack growth rate稳定裂纹扩展stable crack growth定常裂纹扩展steady crack growth亚临界裂纹扩展subcritical crack growth裂纹[扩展]减速crack retardation止裂crack arrest止裂韧度arrest toughness断裂类型fracture mode滑开型sliding mode张开型opening mode撕开型tearing mode复合型mixed mode撕裂Tearing撕裂模量tearing modulus断裂准则fracture criterionJ积分J-integralJ阻力曲线J-resistance curve断裂韧度fracture toughness应力强度因子stress intensity factorHRR场Hutchinson-Rice-Rosengren Field 守恒积分conservation integral有效应力张量effective stress tensor应变能密度strain energy density能量释放率energy release rate内聚区cohesive zone塑性区plastic zone张拉区stretched zone热影响区heat affected zone, HAZ延脆转变温度brittle-ductile transition temperature剪切带shear band剪切唇shear lip无损检测non-destructive inspection双边缺口试件double edge notched specimen, DEN specimen单边缺口试件single edge notched specimen, SEN specimen三点弯曲试件three point bending specimen, TPB specimen中心裂纹拉伸试件center cracked tension specimen, CCT specimen中心裂纹板试件center cracked panel specimen, CCP specimen紧凑拉伸试件compact tension specimen, CT specimen大范围屈服large scale yielding小范围攻屈服small scale yielding韦布尔分布Weibull distribution帕里斯公式paris formula空穴化Cavitation应力腐蚀stress corrosion概率风险判定probabilistic risk assessment, PRA损伤力学damage mechanics损伤Damage连续介质损伤力学continuum damage mechanics细观损伤力学microscopic damage mechanics累积损伤accumulated damage脆性损伤brittle damage延性损伤ductile damage宏观损伤macroscopic damage细观损伤microscopic damage微观损伤microscopic damage损伤准则damage criterion损伤演化方程damage evolution equation损伤软化damage softening损伤强化damage strengthening损伤张量damage tensor损伤阈值damage threshold 损伤变量damage variable 损伤矢量damage vector损伤区damage zone疲劳Fatigue低周疲劳low cycle fatigue 应力疲劳stress fatigue随机疲劳random fatigue 蠕变疲劳creep fatigue腐蚀疲劳corrosion fatigue 疲劳损伤fatigue damage 疲劳失效fatigue failure疲劳断裂fatigue fracture 疲劳裂纹fatigue crack疲劳寿命fatigue life疲劳破坏fatigue rupture 疲劳强度fatigue strength 疲劳辉纹fatigue striations 疲劳阈值fatigue threshold 交变载荷alternating load 交变应力alternating stress 应力幅值stress amplitude应变疲劳strain fatigue应力循环stress cycle应力比stress ratio安全寿命safe life过载效应overloading effect循环硬化cyclic hardening循环软化cyclic softening环境效应environmental effect裂纹片crack gage裂纹扩展crack growth, crack Propagation 裂纹萌生crack initiation循环比cycle ratio实验应力分析experimental stress Analysis 工作[应变]片active[strain] gage基底材料backing material应力计stress gage零[点]飘移zero shift, zero drift应变测量strain measurement应变计strain gage应变指示器strain indicator应变花strain rosette应变灵敏度strain sensitivity机械式应变仪mechanical strain gage直角应变花rectangular rosette引伸仪Extensometer应变遥测telemetering of strain横向灵敏系数transverse gage factor横向灵敏度transverse sensitivity焊接式应变计weldable strain gage平衡电桥balanced bridge粘贴式应变计bonded strain gage粘贴箔式应变计bonded foiled gage粘贴丝式应变计bonded wire gage桥路平衡bridge balancing电容应变计capacitance strain gage补偿片compensation technique补偿技术compensation technique基准电桥reference bridge电阻应变计resistance strain gage温度自补偿应变计self-temperature compensating gage半导体应变计semiconductor strain Gage集流器slip ring应变放大镜strain amplifier疲劳寿命计fatigue life gage电感应变计inductance [strain] gage光[测]力学Photomechanics光弹性Photoelasticity光塑性Photoplasticity杨氏条纹Young fringe双折射效应birefrigent effect等位移线contour of equal Displacement暗条纹dark fringe条纹倍增fringe multiplication干涉条纹interference fringe等差线Isochromatic等倾线Isoclinic等和线isopachic应力光学定律stress- optic law主应力迹线Isostatic亮条纹light fringe光程差optical path difference热光弹性photo-thermo -elasticity光弹性贴片法photoelastic coating Method光弹性夹片法photoelastic sandwich Method动态光弹性dynamic photo-elasticity空间滤波spatial filtering空间频率spatial frequency起偏镜Polarizer反射式光弹性仪reflection polariscope残余双折射效应residual birefringent Effect应变条纹值strain fringe value应变光学灵敏度strain-optic sensitivity应力冻结效应stress freezing effect应力条纹值stress fringe value应力光图stress-optic pattern暂时双折射效应temporary birefringent Effect脉冲全息法pulsed holography透射式光弹性仪transmission polariscope实时全息干涉法real-time holographic interferometry网格法grid method全息光弹性法holo-photoelasticity全息图Hologram全息照相Holograph全息干涉法holographic interferometry全息云纹法holographic moire technique全息术Holography全场分析法whole-field analysis散斑干涉法speckle interferometry散斑Speckle错位散斑干涉法speckle-shearing interferometry, shearography散斑图Specklegram白光散斑法white-light speckle method云纹干涉法moire interferometry[叠栅]云纹moire fringe[叠栅]云纹法moire method云纹图moire pattern离面云纹法off-plane moire method参考栅reference grating试件栅specimen grating分析栅analyzer grating面内云纹法in-plane moire method脆性涂层法brittle-coating method条带法strip coating method坐标变换transformation of Coordinates计算结构力学computational structural mechanics加权残量法weighted residual method有限差分法finite difference method有限[单]元法finite element method配点法point collocation里茨法Ritz method广义变分原理generalized variational Principle最小二乘法least square method胡[海昌]一鹫津原理Hu-Washizu principle赫林格-赖斯纳原理Hellinger-Reissner Principle修正变分原理modified variational Principle约束变分原理constrained variational Principle混合法mixed method杂交法hybrid method边界解法boundary solution method有限条法finite strip method半解析法semi-analytical method协调元conforming element非协调元non-conforming element混合元mixed element杂交元hybrid element边界元boundary element强迫边界条件forced boundary condition 自然边界条件natural boundary condition 离散化Discretization离散系统discrete system连续问题continuous problem广义位移generalized displacement广义载荷generalized load广义应变generalized strain广义应力generalized stress界面变量interface variable节点node, nodal point[单]元Element角节点corner node边节点mid-side node内节点internal node无节点变量nodeless variable杆元bar element桁架杆元truss element梁元beam element二维元two-dimensional element一维元one-dimensional element三维元three-dimensional element轴对称元axisymmetric element板元plate element壳元shell element厚板元thick plate element三角形元triangular element四边形元quadrilateral element四面体元tetrahedral element曲线元curved element二次元quadratic element线性元linear element三次元cubic element四次元quartic element等参[数]元isoparametric element超参数元super-parametric element亚参数元sub-parametric element节点数可变元variable-number-node element拉格朗日元Lagrange element拉格朗日族Lagrange family巧凑边点元serendipity element巧凑边点族serendipity family无限元infinite element单元分析element analysis单元特性element characteristics刚度矩阵stiffness matrix几何矩阵geometric matrix等效节点力equivalent nodal force节点位移nodal displacement节点载荷nodal load位移矢量displacement vector载荷矢量load vector质量矩阵mass matrix集总质量矩阵lumped mass matrix相容质量矩阵consistent mass matrix阻尼矩阵damping matrix瑞利阻尼Rayleigh damping刚度矩阵的组集assembly of stiffness Matrices载荷矢量的组集consistent mass matrix质量矩阵的组集assembly of mass matrices单元的组集assembly of elements局部坐标系local coordinate system局部坐标local coordinate面积坐标area coordinates体积坐标volume coordinates曲线坐标curvilinear coordinates静凝聚static condensation合同变换contragradient transformation形状函数shape function试探函数trial function检验函数test function权函数weight function样条函数spline function代用函数substitute function降阶积分reduced integration零能模式zero-energy modeP收敛p-convergenceH收敛h-convergence掺混插值blended interpolation等参数映射isoparametric mapping双线性插值bilinear interpolation小块检验patch test非协调模式incompatible mode节点号node number单元号element number带宽band width带状矩阵banded matrix变带状矩阵profile matrix带宽最小化minimization of band width 波前法frontal method子空间迭代法subspace iteration method 行列式搜索法determinant search method 逐步法step-by-step method纽马克法Newmark威尔逊法Wilson拟牛顿法quasi-Newton method牛顿-拉弗森法Newton-Raphson method 增量法incremental method初应变initial strain初应力initial stress切线刚度矩阵tangent stiffness matrix割线刚度矩阵secant stiffness matrix模态叠加法mode superposition method平衡迭代equilibrium iteration子结构Substructure子结构法substructure technique超单元super-element网格生成mesh generation结构分析程序structural analysis program前处理pre-processing后处理post-processing网格细化mesh refinement应力光顺stress smoothing组合结构composite structure流体动力学fluid dynamics连续介质力学mechanics of continuous media介质medium流体质点fluid particle无粘性流体nonviscous fluid, inviscid fluid 连续介质假设continuous medium hypothesis流体运动学fluid kinematics水静力学hydrostatics液体静力学hydrostatics支配方程governing equation伯努利方程Bernoulli equation伯努利定理Bernonlli theorem毕奥-萨伐尔定律Biot-Savart law欧拉方程Euler equation亥姆霍兹定理Helmholtz theorem开尔文定理Kelvin theorem涡片vortex sheet库塔-茹可夫斯基条件Kutta-Zhoukowski condition布拉休斯解Blasius solution达朗贝尔佯廖d&;am #39;Alembert paradox 雷诺数Reynolds number施特鲁哈尔数Strouhal number随体导数material derivative不可压缩流体incompre ible fluid质量守恒co ervation of ma动量守恒co ervation of momentum能量守恒co ervation of energy动量方程momentum equation能量方程energy equation控制体积control volume液体静压hydrostatic pre ure 涡量拟能 e trophy压差differential pre ure流[动] flow流线stream line流面stream surface流管stream tube迹线path, path line流场flow field流态flow regime流动参量flow parameter流量flow rate, flow discharge 涡旋vortex涡量vorticity涡丝vortex filament涡线vortex line涡面vortex surface涡层vortex layer涡环vortex ring涡对vortex pair涡管vortex tube涡街vortex street卡门涡街Karman vortex street 马蹄涡horseshoe vortex对流涡胞convective cell卷筒涡胞roll cell涡eddy涡粘性eddy viscosity环流circulation环量circulation速度环量velocity circulation偶极子doublet, dipole驻点stagnation point总压[力] total pre ure总压头total head静压头static head总焓total enthalpy能量输运energy tra ort速度剖面velocity profile库埃特流Couette flow单相流single phase flow单组份流single-component flow 均匀流uniform flow非均匀流nonuniform flow二维流two-dime ional flow三维流three-dime ional flow准定常流quasi-steady flow非定常流u teady flow, non-steady flow 暂态流tra ient flow周期流periodic flow振荡流oscillatory flow分层流stratified flow无旋流irrotational flow有旋流rotational flow轴对称流axisymmetric flow不可压缩性incompre ibility不可压缩流[动] incompre ible flow浮体floating body定倾中心metacenter阻力drag, resistance减阻drag reduction表面力surface force表面张力surface te ion毛细[管]作用capillarity来流incoming flow自由流free stream自由流线free stream line外流external flow进口entrance, inlet出口exit, outlet扰动disturbance, perturbation分布distribution传播propagation色散di ersion弥散di ersion附加质量added ma ,a ociated ma 收缩contraction镜象法image method无量纲参数dime ionle parameter 几何相似geometric similarity运动相似kinematic similarity动力相似[性] dynamic similarity平面流plane flow势potential势流potential flow速度势velocity potential复势complex potential复速度complex velocity流函数stream function源source汇sink速度[水]头velocity head拐角流corner flow空泡流cavity flow超空泡supercavity超空泡流supercavity flow空气动力学aerodynamics低速空气动力学low- eed aerodynamics 高速空气动力学high- eed aerodynamics 气动热力学aerothermodynamics亚声速流[动] su onic flow跨声速流[动] tra onic flow超声速流[动] supersonic flow锥形流conical flow楔流wedge flow叶栅流cascade flow非平衡流[动] non-equilibrium flow细长体slender body细长度slenderne钝头体bluff body钝体blunt body翼型airfoil翼弦chord薄翼理论thin-airfoil theory构型configuration后缘trailing edge迎角angle of attack失速stall脱体激波detached shock wave波阻wave drag诱导阻力induced drag诱导速度induced velocity临界雷诺数critical Reynolds number 前缘涡leading edge vortex附着涡bound vortex约束涡confined vortex气动中心aerodynamic center气动力aerodynamic force气动噪声aerodynamic noise气动加热aerodynamic heating离解di ociation地面效应ground effect气体动力学gas dynamics稀疏波rarefaction wave热状态方程thermal equation of state喷管Nozzle普朗特-迈耶流Prandtl-Meyer flow瑞利流Rayleigh flow可压缩流[动] compre ible flow可压缩流体compre ible fluid绝热流adiabatic flow非绝热流diabatic flow未扰动流undisturbed flow等熵流isentropic flow匀熵流homoentropic flow兰金-于戈尼奥条件Rankine-Hugoniot condition状态方程equation of state量热状态方程caloric equation of state完全气体perfect gas拉瓦尔喷管Laval nozzle马赫角Mach angle马赫锥Mach cone马赫线Mach line马赫数Mach number马赫波Mach wave当地马赫数local Mach number 冲击波shock wave激波shock wave正激波normal shock wave斜激波oblique shock wave头波bow wave附体激波attached shock wave 激波阵面shock front激波层shock layer压缩波compre ion wave反射reflection折射refraction散射scattering衍射diffraction绕射diffraction出口压力exit pre ure超压[强] over pre ure反压back pre ure爆炸explosion爆轰detonation缓燃deflagration水动力学hydrodynamics液体动力学hydrodynamics泰勒不稳定性Taylor i tability 盖斯特纳波Gerstner wave斯托克斯波Stokes wave瑞利数Rayleigh number自由面free surface波速wave eed, wave velocity 波高wave height波列wave train波群wave group波能wave energy表面波surface wave表面张力波capillary wave规则波regular wave不规则波irregular wave浅水波shallow water wave深水波deep water wave重力波gravity wave椭圆余弦波cnoidal wave潮波tidal wave涌波surge wave破碎波breaking wave船波ship wave非线性波nonlinear wave孤立子soliton水动[力]噪声hydrodynamic noise水击water hammer空化cavitation空化数cavitation number空蚀cavitation damage超空化流supercavitating flow水翼hydrofoil水力学hydraulics洪水波flood wave涟漪ri le消能energy di ipation海洋水动力学marine hydrodynamics 谢齐公式Chezy formula欧拉数Euler number弗劳德数Froude number水力半径hydraulic radius水力坡度hvdraulic slope高度水头elevating head水头损失head lo水位water level水跃hydraulic jump含水层aquifer排水drainage排放量discharge壅水曲线back water curve压[强水]头pre ure head过水断面flow cro -section明槽流open cha el flow孔流orifice flow无压流free surface flow有压流pre ure flow缓流subcritical flow急流supercritical flow渐变流gradually varied flow急变流rapidly varied flow临界流critical flow异重流de ity current, gravity flow 堰流weir flow掺气流aerated flow含沙流sediment-laden stream降水曲线dropdown curve沉积物sediment, deposit沉[降堆]积sedimentation, deposition沉降速度settling velocity流动稳定性flow stability不稳定性i tability奥尔-索末菲方程Orr-Sommerfeld equation 涡量方程vorticity equation泊肃叶流Poiseuille flow奥辛流Oseen flow剪切流shear flow粘性流[动] viscous flow层流laminar flow分离流separated flow二次流secondary flow近场流near field flow远场流far field flow滞止流stagnation flow尾流wake [flow]回流back flow反流reverse flow射流jet自由射流free jet管流pipe flow, tube flow内流internal flow拟序结构coherent structure 猝发过程bursting proce表观粘度 a arent viscosity运动粘性kinematic viscosity 动力粘性dynamic viscosity 泊poise厘泊centipoise厘沱centistoke剪切层shear layer次层sublayer流动分离flow separation层流分离laminar separation 湍流分离turbulent separation 分离点separation point附着点attachment point再附reattachment再层流化relaminarization起动涡starting vortex驻涡standing vortex涡旋破碎vortex breakdown涡旋脱落vortex shedding压[力]降pre ure drop压差阻力pre ure drag压力能pre ure energy型阻profile drag滑移速度slip velocity无滑移条件non-slip condition壁剪应力skin friction, frictional drag壁剪切速度friction velocity磨擦损失friction lo磨擦因子friction factor耗散di ipation滞后lag相似性解similar solution局域相似local similarity气体润滑gas lubrication液体动力润滑hydrodynamic lubrication 浆体slurry泰勒数Taylor number纳维-斯托克斯方程Navier-Stokes equation 牛顿流体Newtonian fluid边界层理论boundary later theory边界层方程boundary layer equation边界层boundary layer附面层boundary layer层流边界层laminar boundary layer湍流边界层turbulent boundary layer温度边界层thermal boundary layer边界层转捩boundary layer tra ition边界层分离boundary layer separation边界层厚度boundary layer thickne位移厚度di lacement thickne动量厚度momentum thickne能量厚度energy thickne焓厚度enthalpy thickne注入injection吸出suction泰勒涡Taylor vortex速度亏损律velocity defect law形状因子shape factor测速法anemometry。

Large-area synthesis of high-quality and uniform graphene films on copper foils

Large-area synthesis of high-quality and uniform graphene films on copper foils

DOI: 10.1126/science.1171245, 1312 (2009);324Scienceet al.Xuesong Li,Graphene Films on Copper Foils Large-Area Synthesis of High-Quality and Uniform (this information is current as of June 8, 2009 ):The following resources related to this article are available online at/cgi/content/full/324/5932/1312version of this article at:including high-resolution figures, can be found in the online Updated information and services,/cgi/content/full/1171245/DC1 can be found at:Supporting Online Material /cgi/content/full/324/5932/1312#otherarticles , 2 of which can be accessed for free:cites 25 articles This article/cgi/collection/mat_sci Materials Science: subject collections This article appears in the following/about/permissions.dtl in whole or in part can be found at: this article permission to reproduce of this article or about obtaining reprints Information about obtaining registered trademark of AAAS.is a Science 2009 by the American Association for the Advancement of Science; all rights reserved. The title Copyright American Association for the Advancement of Science, 1200 New York Avenue NW, Washington, DC 20005. (print ISSN 0036-8075; online ISSN 1095-9203) is published weekly, except the last week in December, by the Science o n J u n e 8, 2009w w w .s c i e n c e m a g .o r g D o w n l o a d e d f r o m3.B.L.Cushing,V.L.Kolesnichenko,C.J.O ’Connor,Chem.Rev.104,3893(2004).4.Y.Yin,A.P.Alivisatos,Nature 437,664(2005).5.D.J.Norris,A.L.Efros,S.C.Erwin,Science 319,1776(2008).6.X.G.Peng et al .,Nature 404,59(2000).7.L.Manna,E.C.Scher,A.P.Alivisatos,J.Am.Chem.Soc.122,12700(2000).8.V.F.Puntes,K.M.Krishnan,A.P.Alivisatos,Science 291,2115(2001).9.V.F.Puntes,D.Zanchet,C.K.Erdonmez,A.P.Alivisatos,J.Am.Chem.Soc.124,12874(2002).liron et al .,Nature 430,190(2004).11.Y.D.Yin et al .,Science 304,711(2004).Mer,R.H.Dinergar,J.Am.Chem.Soc.72,4847(1950).13.H.Reiss,J.Chem.Phys.19,482(1951).14.T.Sugimoto,Adv.Colloid Interface Sci.28,65(1987).15.D.V.Leff,P.C.Ohara,J.R.Heath,W.M.Gelbart,J.Phys.Chem.B 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for their help with the initial tests on the liquid cells.This project is supported by the Director,Office of Science,Office of Basic Energy Sciences,Materials Sciences and Engineering Division of the U.S.Department of Energy under contract DE-AC02-05CH11231.Supporting Online Material/cgi/content/full/324/5932/1309/DC1Materials and Methods Figs.S1to S3Movies S1and S2References10February 2009;accepted 8April 200910.1126/science.1172104Large-Area Synthesis of High-Quality and Uniform Graphene Films on Copper FoilsXuesong Li,1Weiwei Cai,1Jinho An,1Seyoung Kim,2Junghyo Nah,2Dongxing Yang,1Richard Piner,1Aruna Velamakanni,1Inhwa Jung,1Emanuel Tutuc,2Sanjay K.Banerjee,2Luigi Colombo,3*Rodney S.Ruoff 1*Graphene has been attracting great interest because of its distinctive band structure and physical properties.Today,graphene is limited to small sizes because it is produced mostly by exfoliating graphite.We grew large-area graphene films of the order of centimeters on copper substrates by chemical vapor deposition using methane.The films are predominantly single-layer graphene,with a small percentage (less than 5%)of the area having few layers,and are continuous across copper surface steps and grain boundaries.The low solubility of carbon in copper appears to help make this growth process self-limiting.We also developed graphene film transfer processes to arbitrary substrates,and dual-gated field-effect transistors fabricated on silicon/silicon dioxide substrates showed electron mobilities as high as 4050square centimeters per volt per second at room temperature.Graphene,a monolayer of sp 2-bonded car-bon atoms,is a quasi –two-dimensional (2D)material.Graphene has been attract-ing great interest because of its distinctive band structure and physical properties (1).Today,the size of graphene films produced is limited to small sizes (usually <1000m m 2)because the films are produced mostly by exfoliating graphite,which is not a scalable technique.Graphene has also been synthesized by the desorption of Si from SiC single-crystal surfaces,which yields a multilayered graphene structure that behaves like graphene (2,3),and by a surface precipitation process of carbon in some transition metals (4–8).Electronic application will require high-quality large-area graphene that can be manipu-lated to make complex devices and integrated in silicon device flows.Field-effect transistors (FETs)fabricated with exfoliated graphite have shown promising electrical properties (9,10),but these devices will not meet the silicon device scaling requirements,especially those for power reduction and performance.One device that could meet the silicon roadmap requirements beyond the 15-nm node was proposed by S.K.Banerjee et al .(11).The device is a “BisFET ”(bilayer pseudospin FET)that is made up of two graphene layers separated by a thin dielectric.The ability to create this device can be facilitated by the availability of large-area graphene.Making a transparent electrode,another prom-ising application of graphene,also requires large films (6,12–14).At this time,there is no pathway for the formation of a graphene layer that can be ex-foliated from or transferred from the graphene synthesized on SiC,but there is a way to growand transfer graphene grown on metal substrates (5–7).Although graphene has been grown on a number of metals,we still have the challenge of growing large-area graphene.For example,graphene grown on Ni seems to be limited by its small grain size,presence of multilayers at the grain boundaries,and the high solubility of car-bon (6,7).We have developed a graphene chem-ical vapor deposition (CVD)growth process on copper foils (25m m thick in our experiment).The films grow directly on the surface by a surface-catalyzed process,and the film is predominantly graphene with <5%of the area having two-and three-layer graphene flakes.Under our process-ing conditions,the two-and three-layer flakes do not grow larger with time.One of the major benefits of our process is that it can be used to grow graphene on 300-mm copper films on Si substrates (a standard process in Si technology).It is also well known that annealing of Cu can lead to very large grains.As described in (15),we grew graphene on copper foils at temperatures up to 1000°C by CVD of carbon using a mixture of methane and hydrogen.Figure 1A shows a scanning electron microscopy (SEM)image of graphene on a copper substrate where the Cu grains are clearly visible.A higher-resolution image of graphene on Cu (Fig.1B)shows the presence of Cu surface steps,graphene “wrinkles,”and the presence of non-uniform dark flakes.The wrinkles associated with the thermal expansion coefficient difference between Cu and graphene are also found to cross Cu grain boundaries,indicating that the graphene film is continuous.The inset in Fig.1B shows transmission electron microscopy (TEM)images of graphene and bilayer graphene.With the use of a process similar to that described in (16),the as-grown graphene can be easily transferred to alternative substrates,such as SiO 2/Si or glass (Fig.1,C and D),for further evaluation and for various applications;a detailed transfer process is described (15).The process and method used to transfer graphene from Cu was the same for the SiO 2/Si substrate and the glass substrate.Al-1Department of Mechanical Engineering and the Texas Materials Institute,1University Station C2200,The University of Texas at Austin,Austin,TX 78712–0292,USA.2Department of Electrical and Computer Engineering,Microelectronics Research Center,The University of Texas at Austin,Austin,TX 78758,USA.3Texas Instruments,Dallas,TX 75243,USA.*To whom correspondence should be addressed.E-mail:colombo@ (L.C.);r.ruoff@ (R.S.R.)5JUNE 2009VOL 324SCIENCE1312REPORTSo n J u n e 8, 2009w w w .s c i e n c e m a g .o r g D o w n l o a d e d f r o mthough it is difficult to see the graphene on the SiO 2/Si substrate,a similar graphene film from another Cu substrate transferred on glass clearly shows that it is optically uniform.We used Raman spectroscopy to evaluate the quality and uniformity of graphene on a SiO 2/Si substrate.Figure 2shows SEM and optical im-ages with the corresponding Raman spectra and maps of the D,G,and 2D bands providing in-formation on the defect density and film thick-ness.The Raman spectra are from the spots marked with the corresponding colored circles shown in the other panels (in Fig.2,A and B,green arrows are used instead of circles so as to show the trilayer region more clearly).The thickness and uniformity of the graphene films were evaluated via color contrast under optical microscope (17)and Raman spectra (7,18,19).The Raman spectrum from the lightest pink background in Fig.2B shows typical features of monolayer graphene:(i)a ~0.5G –to –2D inten-sity ratio and (ii)a symmetric 2D band centered at ~2680cm –1with a full width at half maxi-mum of ~33cm –1.The second lightest pink flakes (blue circle)correspond to bilayer graphene,and the darkest one (green arrow)represents trilayer graphene.This thickness variation is more clearly shown in the SEM image in Fig.2A.The D map in Fig.2D,which has been associated with defects in graphene,is rather uniform and near the background level,except for regions where wrinkles are present and close to few-layer regions.The G and the 2D maps clearly show the presence of more than one layer in the flakes.In the wrinkled regions,there are peak height variations in both the G and 2D bands,and there is a broadening of the 2D band.An analysis of the intensity of the optical image over the whole sample (1cm by 1cm)showed that the area with the lightest pink color is more than 95%,and all 40Raman spectra randomly collected from this area show monolayer graphene.There is only a small fraction of trilayer or few-layer (<10)graphene (<1%),and the rest is bilayer graphene (~3to 4%).We grew films on Cu as a function of time and Cu foil thickness under isothermal and iso-baric ing the process flow de-scribed in (15),we found that graphene growth on Cu is self-limited;growth that proceeded for more than 60min yielded a similar structure to growth runs performed for ~10min.For timesFig.2.(A )SEM image of graphene transferred on SiO 2/Si (285-nm-thick oxide layer)showing wrin-kles,as well as two-and three-layerregions.(B )Op-tical microscope image of the same regions as in (A).(C )Raman spectra from the marked spots with cor-responding colored circles or arrows showing the pres-enceofone,two,andthree layers of graphene.a.u.,ar-bitrary units.(D to F )Ra-man maps of the D (1300to 1400cm –1),G (1560to 1620cm –1),and 2D (2660to 2700cm –1)bands,re-spectively (WITec alpha300,l laser =532nm,~500-nm spot size,100×objector).CCD cts.,charge-coupled device counts.Scale bars,5mm.Fig.1.(A )SEM image of graphene on a copper foil with a growth time of 30min.(B )High-resolution SEM image showing a Cu grain boundary and steps,two-and three-layer graphene flakes,and graphene wrinkles.Inset in (B)shows TEM images of folded graphene edges.1L,one layer;2L,two layers.(C and D )Graphene films transferred onto a SiO 2/Si substrate and a glass plate,respectively. SCIENCE VOL 3245JUNE 20091313REPORTSo n J u n e 8, 2009w w w .s c i e n c e m a g .o r g D o w n l o a d e d f r o mmuch less than 10min,the Cu surface is usually not fully covered [SEM images of graphene on Cu with different growth time are shown in fig.S3(15)].The growth of graphene on Cu foils of varying thickness (12.5,25,and 50m m)also yielded similar graphene structure with re-gions of double and triple flakes,but neither discontinuous monolayer graphene for thinner Cu foils nor continuous multilayer graphene for thicker Cu foils,as we would have expected based on the precipitation mechanism.Accord-ing to these observations,we concluded that graphene is growing by a surface-catalyzed pro-cess rather than a precipitation process,as has been reported by others for Ni (5–7).Monolayer graphene formation caused by surface segrega-tion or surface adsorption of carbon has also been observed on transition metals such as Ni and Co at elevated temperatures by Blakely and coauthors (20–22).However,when the metal substrates were cooled down to room temper-ature,thick graphite films were obtained because of precipitation of excess C from these metals,in which the solubility of C is relatively high.In recent work,thin Ni films and a fast-cooling process have been used to suppress the amount of precipitated C.However,this process still yields films with a wide range of graphene layer thicknesses,from one to a few tens of lay-ers and with defects associated with fast cooling (5–7).Our results suggest that the graphene growth process is not one of C precipitation but rather a CVD process.The precise mechanism will require additional experiments to understand in full,but very low C solubility in Cu (23–25)and poor C saturation as a result of graphene sur-face coverage may be playing a role in limiting or preventing the precipitation process altogether at high temperature,similar to the case of im-peding of carburization of Ni (26).This provides a pathway for growing self-limited graphene films.To evaluate the electrical quality of the syn-thesized graphene,we fabricated dual-gated FETs with Al 2O 3as the gate dielectric and measured them at room temperature.Along with a device model that incorporates a finite density at the Dirac point,the dielectric,and the quantum ca-pacitances (9),the data are shown in Fig.3.The extracted carrier mobility for this device is ~4050cm 2V –1s –1,with the residual carrier concentra-tion at the Dirac point of n 0=3.2×1011cm –2.These data suggest that the films are of rea-sonable quality,at least sufficient to continue improving the growth process to achieve a ma-terial quality equivalent to the exfoliated natural graphite.References and Notes1.A.K.Geim,K.S.Novoselov,Nat.Mater.6,183(2007).2.C.Berger et al .,Science 312,1191(2006);published online 12April 2006(10.1126/science.1125925).3.K.V.Emtsev et al .,Nat.Mater.8,203(2009).4.P.W.Sutter,J.-I.Flege,E.A.Sutter,Nat.Mater.7,406(2008).5.Q.Yu et al 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.,Nat.Nanotechnol.3,210(2008).20.M.Eizenberg,J.M.Blakely,Surf.Sci.82,228(1979).21.M.Eizenberg,J.M.Blakely,J.Chem.Phys.71,3467(1979).22.J.C.Hamilton,J.M.Blakely,Surf.Sci.91,199(1980).23.R.B.McLellan,Scr.Metal.3,389(1969).24.G.Mathieu,S.Guiot,J.Carbané,Scr.Metal.7,421(1973).25.G.A.López,E.J.Mittemeijer,Scr.Mater.51,1(2004).26.R.Kikowatz,K.Flad,G.Horz,J.Vac.Sci.Technol.A 5,1009(1987).27.We thank the Nanoelectronic Research Initiative(NRI –Southwest Area Nanoelectronics Center,grant no.2006-NE-1464),the Defense Advanced Research Projects Agency Carbon Electronics for RF Applications Center,and the University of Texas at Austin for support.Supporting Online Material/cgi/content/full/1171245/DC1Materials and Methods Figs.S1to S322January 2009;accepted 9April 2009Published online 7May 2009;10.1126/science.1171245Include this information when citing this paper.Superconductivity at the Two-Dimensional LimitShengyong Qin,Jungdae Kim,Qian Niu,Chih-Kang Shih *Superconductivity in the extreme two-dimensional limit is studied on ultrathin lead films down to two atomic layers,where only a single channel of quantum well states exists.Scanning tunneling spectroscopy reveals that local superconducting order remains robust until two atomic layers,where the transition temperature abruptly plunges to a lower value,depending sensitively on the exact atomic structure of the film.Our result shows that Cooper pairs can still form in the last two-dimensional channel of electron states,although their binding is strongly affected by the substrate.Studies of two-dimensional (2D)super-conductivities have been generally limited to the regime where the superconducting order parameter behaves as a 2D wave func-tion but the underline electrons are still three-dimensional (1–11).Recent advancements in materials synthesis have enabled the growth of epitaxial superconductor thin films with unprec-Fig.3.(A )Optical micro-scope imageofa graphene FET.(B )Device resistance versus top-gate voltage (V TG ),with different back-gate (V BG )biases,and ver-sus V TG -V Dirac,TG (V TG at the Dirac point),with a model fit (solidline).5JUNE 2009VOL 324SCIENCE1314REPORTSo n J u n e 8, 2009w w w .s c i e n c e m a g .o r g D o w n l o a d e d f r o m。

电气词语

电气词语

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卷积神经网络机器学习外文文献翻译中英文2020

卷积神经网络机器学习外文文献翻译中英文2020

卷积神经网络机器学习相关外文翻译中英文2020英文Prediction of composite microstructure stress-strain curves usingconvolutional neural networksCharles Yang,Youngsoo Kim,Seunghwa Ryu,Grace GuAbstractStress-strain curves are an important representation of a material's mechanical properties, from which important properties such as elastic modulus, strength, and toughness, are defined. However, generating stress-strain curves from numerical methods such as finite element method (FEM) is computationally intensive, especially when considering the entire failure path for a material. As a result, it is difficult to perform high throughput computational design of materials with large design spaces, especially when considering mechanical responses beyond the elastic limit. In this work, a combination of principal component analysis (PCA) and convolutional neural networks (CNN) are used to predict the entire stress-strain behavior of binary composites evaluated over the entire failure path, motivated by the significantly faster inference speed of empirical models. We show that PCA transforms the stress-strain curves into an effective latent space by visualizing the eigenbasis of PCA. Despite having a dataset of only 10-27% of possible microstructure configurations, the mean absolute error of the prediction is <10% of therange of values in the dataset, when measuring model performance based on derived material descriptors, such as modulus, strength, and toughness. Our study demonstrates the potential to use machine learning to accelerate material design, characterization, and optimization.Keywords:Machine learning,Convolutional neural networks,Mechanical properties,Microstructure,Computational mechanics IntroductionUnderstanding the relationship between structure and property for materials is a seminal problem in material science, with significant applications for designing next-generation materials. A primary motivating example is designing composite microstructures for load-bearing applications, as composites offer advantageously high specific strength and specific toughness. Recent advancements in additive manufacturing have facilitated the fabrication of complex composite structures, and as a result, a variety of complex designs have been fabricated and tested via 3D-printing methods. While more advanced manufacturing techniques are opening up unprecedented opportunities for advanced materials and novel functionalities, identifying microstructures with desirable properties is a difficult optimization problem.One method of identifying optimal composite designs is by constructing analytical theories. For conventional particulate/fiber-reinforced composites, a variety of homogenizationtheories have been developed to predict the mechanical properties of composites as a function of volume fraction, aspect ratio, and orientation distribution of reinforcements. Because many natural composites, synthesized via self-assembly processes, have relatively periodic and regular structures, their mechanical properties can be predicted if the load transfer mechanism of a representative unit cell and the role of the self-similar hierarchical structure are understood. However, the applicability of analytical theories is limited in quantitatively predicting composite properties beyond the elastic limit in the presence of defects, because such theories rely on the concept of representative volume element (RVE), a statistical representation of material properties, whereas the strength and failure is determined by the weakest defect in the entire sample domain. Numerical modeling based on finite element methods (FEM) can complement analytical methods for predicting inelastic properties such as strength and toughness modulus (referred to as toughness, hereafter) which can only be obtained from full stress-strain curves.However, numerical schemes capable of modeling the initiation and propagation of the curvilinear cracks, such as the crack phase field model, are computationally expensive and time-consuming because a very fine mesh is required to accommodate highly concentrated stress field near crack tip and the rapid variation of damage parameter near diffusive cracksurface. Meanwhile, analytical models require significant human effort and domain expertise and fail to generalize to similar domain problems.In order to identify high-performing composites in the midst of large design spaces within realistic time-frames, we need models that can rapidly describe the mechanical properties of complex systems and be generalized easily to analogous systems. Machine learning offers the benefit of extremely fast inference times and requires only training data to learn relationships between inputs and outputs e.g., composite microstructures and their mechanical properties. Machine learning has already been applied to speed up the optimization of several different physical systems, including graphene kirigami cuts, fine-tuning spin qubit parameters, and probe microscopy tuning. Such models do not require significant human intervention or knowledge, learn relationships efficiently relative to the input design space, and can be generalized to different systems.In this paper, we utilize a combination of principal component analysis (PCA) and convolutional neural networks (CNN) to predict the entire stress-strain c urve of composite failures beyond the elastic limit. Stress-strain curves are chosen as the model's target because t hey are difficult to predict given their high dimensionality. In addition, stress-strain curves are used to derive important material descriptors such as modulus, strength, and toughness. In this sense, predicting stress-straincurves is a more general description of composites properties than any combination of scaler material descriptors. A dataset of 100,000 different composite microstructures and their corresponding stress-strain curves are used to train and evaluate model performance. Due to the high dimensionality of the stress-strain dataset, several dimensionality reduction methods are used, including PCA, featuring a blend of domain understanding and traditional machine learning, to simplify the problem without loss of generality for the model.We will first describe our modeling methodology and the parameters of our finite-element method (FEM) used to generate data. Visualizations of the learned PCA latent space are then presented, a long with model performance results.CNN implementation and trainingA convolutional neural network was trained to predict this lower dimensional representation of the stress vector. The input to the CNN was a binary matrix representing the composite design, with 0's corresponding to soft blocks and 1's corresponding to stiff blocks. PCA was implemented with the open-source Python package scikit-learn, using the default hyperparameters. CNN was implemented using Keras with a TensorFlow backend. The batch size for all experiments was set to 16 and the number of epochs to 30; the Adam optimizer was used to update the CNN weights during backpropagation.A train/test split ratio of 95:5 is used –we justify using a smaller ratio than the standard 80:20 because of a relatively large dataset. With a ratio of 95:5 and a dataset with 100,000 instances, the test set size still has enough data points, roughly several thousands, for its results to generalize. Each column of the target PCA-representation was normalized to have a mean of 0 and a standard deviation of 1 to prevent instable training.Finite element method data generationFEM was used to generate training data for the CNN model. Although initially obtained training data is compute-intensive, it takes much less time to train the CNN model and even less time to make high-throughput inferences over thousands of new, randomly generated composites. The crack phase field solver was based on the hybrid formulation for the quasi-static fracture of elastic solids and implementedin the commercial FEM software ABAQUS with a user-element subroutine (UEL).Visualizing PCAIn order to better understand the role PCA plays in effectively capturing the information contained in stress-strain curves, the principal component representation of stress-strain curves is plotted in 3 dimensions. Specifically, we take the first three principal components, which have a cumulative explained variance ~85%, and plot stress-strain curves in that basis and provide several different angles from which toview the 3D plot. Each point represents a stress-strain curve in the PCA latent space and is colored based on the associated modulus value. it seems that the PCA is able to spread out the curves in the latent space based on modulus values, which suggests that this is a useful latent space for CNN to make predictions in.CNN model design and performanceOur CNN was a fully convolutional neural network i.e. the only dense layer was the output layer. All convolution layers used 16 filters with a stride of 1, with a LeakyReLU activation followed by BatchNormalization. The first 3 Conv blocks did not have 2D MaxPooling, followed by 9 conv blocks which did have a 2D MaxPooling layer, placed after the BatchNormalization layer. A GlobalAveragePooling was used to reduce the dimensionality of the output tensor from the sequential convolution blocks and the final output layer was a Dense layer with 15 nodes, where each node corresponded to a principal component. In total, our model had 26,319 trainable weights.Our architecture was motivated by the recent development and convergence onto fully-convolutional architectures for traditional computer vision applications, where convolutions are empirically observed to be more efficient and stable for learning as opposed to dense layers. In addition, in our previous work, we had shown that CNN's werea capable architecture for learning to predict mechanical properties of 2Dcomposites [30]. The convolution operation is an intuitively good fit forpredicting crack propagation because it is a local operation, allowing it toimplicitly featurize and learn the local spatial effects of crack propagation.After applying PCA transformation to reduce the dimensionality ofthe target variable, CNN is used to predict the PCA representation of thestress-strain curve of a given binary composite design. After training theCNN on a training set, its ability to generalize to composite designs it hasnot seen is evaluated by comparing its predictions on an unseen test set.However, a natural question that emerges i s how to evaluate a model's performance at predicting stress-strain curves in a real-world engineeringcontext. While simple scaler metrics such as mean squared error (MSE)and mean absolute error (MAE) generalize easily to vector targets, it isnot clear how to interpret these aggregate summaries of performance. It isdifficult to use such metrics to ask questions such as “Is this modeand “On average, how poorly will aenough to use in the real world” given prediction be incorrect relative to some given specification”. Although being able to predict stress-strain curves is an importantapplication of FEM and a highly desirable property for any machinelearning model to learn, it does not easily lend itself to interpretation. Specifically, there is no simple quantitative way to define whether two-world units.stress-s train curves are “close” or “similar” with real Given that stress-strain curves are oftentimes intermediary representations of a composite property that are used to derive more meaningful descriptors such as modulus, strength, and toughness, we decided to evaluate the model in an analogous fashion. The CNN prediction in the PCA latent space representation is transformed back to a stress-strain curve using PCA, and used to derive the predicted modulus, strength, and toughness of the composite. The predicted material descriptors are then compared with the actual material descriptors. In this way, MSE and MAE now have clearly interpretable units and meanings. The average performance of the model with respect to the error between the actual and predicted material descriptor values derived from stress-strain curves are presented in Table. The MAE for material descriptors provides an easily interpretable metric of model performance and can easily be used in any design specification to provide confidence estimates of a model prediction. When comparing the mean absolute error (MAE) to the range of values taken on by the distribution of material descriptors, we can see that the MAE is relatively small compared to the range. The MAE compared to the range is <10% for all material descriptors. Relatively tight confidence intervals on the error indicate that this model architecture is stable, the model performance is not heavily dependent on initialization, and that our results are robust to differenttrain-test splits of the data.Future workFuture work includes combining empirical models with optimization algorithms, such as gradient-based methods, to identify composite designs that yield complementary mechanical properties. The ability of a trained empirical model to make high-throughput predictions over designs it has never seen before allows for large parameter space optimization that would be computationally infeasible for FEM. In addition, we plan to explore different visualizations of empirical models-box” of such models. Applying machine in an effort to “open up the blacklearning to finite-element methods is a rapidly growing field with the potential to discover novel next-generation materials tailored for a variety of applications. We also note that the proposed method can be readily applied to predict other physical properties represented in a similar vectorized format, such as electron/phonon density of states, and sound/light absorption spectrum.ConclusionIn conclusion, we applied PCA and CNN to rapidly and accurately predict the stress-strain curves of composites beyond the elastic limit. In doing so, several novel methodological approaches were developed, including using the derived material descriptors from the stress-strain curves as interpretable metrics for model performance and dimensionalityreduction techniques to stress-strain curves. This method has the potential to enable composite design with respect to mechanical response beyond the elastic limit, which was previously computationally infeasible, and can generalize easily to related problems outside of microstructural design for enhancing mechanical properties.中文基于卷积神经网络的复合材料微结构应力-应变曲线预测查尔斯,吉姆,瑞恩,格瑞斯摘要应力-应变曲线是材料机械性能的重要代表,从中可以定义重要的性能,例如弹性模量,强度和韧性。

船舶专业英语词汇(按英文字母排序)

船舶专业英语词汇(按英文字母排序)

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box girder bracket floor brake brake band brake crank arm brake drum brake hydraulic cylinder brake hydraulic pipe breadth extreme breadth moulded breakbulk breasthook bridge bridge console stand BSRA buckle buffer spring built-up plate section bulb plate bulbous bow bulk carrier bulk oil carrier bulkhead bulwark bulwark plate bulwark stay buoy tender buoyant buoyant box Bureau Veritas butt weld butterfly screw cap buttock

弹性力学专业英语词汇-elasticity

弹性力学专业英语词汇-elasticity

弹性力学专业英语词汇-elasticity弹性力学elasticity弹性理论theory of elasticity均匀应力状态homogeneous state of stress应力不变量stress invariant应变不变量strain invariant应变椭球strain ellipsoid均匀应变状态homogeneous state of strain应变协调方程equation of strain compatibility拉梅常量Lame constants各向同性弹性isotropic elasticity旋转圆盘rotating circular disk楔wedge开尔文问题Kelvin problem布西内斯克问题Boussinesq problem 艾里应力函数Airy stress function克罗索夫■穆斯赫利什维利法Kolosoff-Muskhelishvili method基尔霍夫假设Kirchhoff hypothesis 板Plate矩形板Rectangular plate板Circular plate环板Annular plate波纹板Corrugated plate 加劲板Stiffened plate,reinforced Plate 中厚板Plate of moderate thickness 弯[曲]应力函数Stress fun ctio n of ben di ng 壳Shell 扁壳Shallow shell 旋转壳Revolutionary shell 球壳Spherical shell[圆]柱壳Cylindrical shell 锥壳Coni cal shell 环壳Toroidal shell 封闭壳Closed shell 波纹壳Corrugated shell 扭[转]应力函数Stress function of torsion 翘曲函数Warping function 半逆解法semi-in verse method 瑞利里茨法Rayleigh-Ritz method 松弛法Relaxation method 莱维法Levy method 松弛Relaxation 量纲分析Dimensional analysis自相似[性]self-similarity 影响面In flue nee surface 接触应力Con tact stress 赫兹理论Hertz theory 协调接触Con formi ng con tact 滑动接触Slidi ng con tact 滚动接触Rolli ng con tact 压入Indentation 各向异性弹性An isotropic elasticity 颗粒材料Granular material 散体力学Mechanics of granular media 热弹性Thermoelasticity 超弹性Hyperelasticity 粘弹性Viscoelasticity 对应原理Correspondence principle 褶皱Wrinkle塑性全量理论Total theory of plasticity 滑动Sliding 微滑Microslip粗糙度Roughness 非线性弹性Nonlinear elasticity 大挠度Large deflection突弹跳变snap-through 有限变形Finite deformation 格林应变Green strain 阿尔曼西应变Almansi strain 弹性动力学Dynamic elasticity 运动方程Equation of motion 准静态的Quasi-static 气动弹性Aeroelasticity 水弹性Hydroelasticity 颤振Flutter 弹性波Elastic wave 简单波Simple wave 柱面波Cylindrical wave 水平剪切波Horizontal shear wave 竖直剪切波Vertical shear wave 体波body wave 无旋波Irrotational wave 畸变波Distortion wave 膨胀波Dilatation wave 壬瑞利波Rayleigh wave 等容波Equivoluminal wave 勒夫波Love wave界面波In terfacial wave 边缘效应edge effect 塑性力学Plasticity 可成形性Formability 金属成形Metal forming 耐撞性Crashworth in ess 结构抗撞毁性Structural crashworthi ness 拉拔Drawing破坏机构Collapse mechanism回弹Springback挤压Extrusion冲压Stamping穿透Perforation层裂Spalling塑性理论Theory of plasticity 安定[性]理论Shake-down theory 运动安定定理kinematic shake-down theorem静力安定定理Static shake-dow n theorem 率相关理论rate dependent theorem 载荷因子load factor加载准贝V Loading criterion加载函数Loading function 力口载面Loadingsurface 塑性加载Plastic loading 塑性加载波Plastic loading wave 简单加载Simple loading 比例加载Proportional loading 卸载Unloading 卸载波Unloading wave 冲击载荷Impulsive load 阶跃载荷step load 脉冲载荷pulse load 极限载荷limit load 中性变载nentral loading 拉抻失稳in stability in tension 力口速度波acceleration wave 本构方程constitutive equation 完全解completesolution 名义应力nominal stress 过应力over-stress 真应力true stress 等效应力equivale nt stress 流动应力flow stress应力间断stress disc on ti nuity 应力空间stress space 主应力空间principal stressspace 静水应力状态hydrostatic state ofstress 对数应变logarithmic strain 工程应变engineering strain 等效应变equivale nt strain 应变局部化strain localization 应变率strainrate 应变率敏感性strain rate sen sitivity 应变空间strain space 有限应变finite strain 塑性应变增量plastic strain in creme nt 累积塑性应变accumulated plastic strain 永久变形permanent deformation 内变量internalvariable 应变软化strain-softening理想刚塑性材料rigid-perfectly plastic Material刚塑性材料rigid-plastic material 理想塑性材料perfectl plastic material 材料稳定性stability of material应变偏张量deviatoric tensor of strain 应力偏张量deviatori tensor of stress 应变球张量spherical tensor of strain 应力球张量spherical tensor of stress 路径相关性path-dependency 线性强化linear strain-hardening 应变强化strain-hardening 随动强化kinematic hardening 各向同性强化isotropic harde ning 强化模量strain-hardening modulus 幂强化power hardening 塑性极限弯矩plastic limit bending Mome nt 塑性极限扭矩plastic limit torque 弹塑性弯曲elastic-plastic bending 弹塑性交界面elastic-plastic in terface 弹塑性扭转elastic-plastictorsion 粘塑性Viscoplasticity 非弹性Inelasticity理想弹塑性材料elastic-perfectly plastic Material极限分析limit analysis极限设计limit design 极限面limit surface上限定理upper bound theorem上屈服点upper yield point下限定理lower bound theorem 下屈服点lower yield point 界限定理bound theorem 初始屈服面initial yield surface 后继屈服面subsequent yield surface 屈服面[的]外凸性convexity of yield surface截面形状因子shape factor of cross-secti on沙堆比拟sand heap analogy屈服Yield屈服条件yield condition 屈服准则yieldcriterion 屈服函数yield function 屈服面yield surface 塑性势plastic potential 能量吸收装置energy absorb ing device 能量耗散率energy absorbing device 塑性动力学dynamicplasticity塑性动力屈曲dyn amic plastic buckli ng塑性动力响应dyn amic plastic resp onse 塑性波plastic wave运动容许场kinematically admissible Field 静力容许场statically admissible Field 流动法则flow rule速度间断velocity disc on ti nu ity滑移线slip-lines滑移线场slip-lines field移行塑性铰travelling plastic hinge塑性增量理论in creme ntal theory of Plasticity米泽斯屈服准则Mises yield criterio n 普朗特---------- 罗伊斯关系prandtl- Reussrelati on特雷斯卡屈服准则Tresca yield criteri on 洛德应力参数Lode stress parameter 莱维米泽斯关系Levy-Mises relation亨基应力方程Hencky stress equati on 赫艾一一韦斯特加德应力空间Haigh-Westergaard stress space洛德应变参数Lode strain parameter 德鲁克公设Drucker postulate_____ 盖林格速度方程Geiringer velocity Equati on 结构力学structural mechanics 结构分析structural analysis 结构动力学structuraldynamics 拱Arch三铰拱three-hinged arch 抛物线拱parabolicarch 圆拱circular arch 穹顶Dome 空间结构space structure 空间桁架space truss 雪载[荷]snow load 风载[荷]wind load 土压力earth pressure 地震载荷earthquake loading弹簧支座spring support 支座位移supportdisplacement 支座沉降support settlement 超静定次数degree of in determ inacy 机动分析kinematic analysis结点法method of joints 截面法method of sections 结点力joint forces 共轭位移conjugate displacement 影响线in flue nee line 三弯矩方程three-moment equation 单位虚力unit virtual force 刚度系数stiffness coefficient 柔度系数flexibility coefficient 力矩分配moment distribution 力矩分配法moment distribution method 力矩再分配moment redistribution 分配系数distribution factor 矩阵位移法matri displacement method 单元刚度矩阵eleme nt stiff ness matrix 单元应变矩阵eleme nt strain matrix 总体坐标global coord inates 贝蒂定理Betti theorem高斯---- 若尔当消去法Gauss-Jordan elim in ati on Method屈曲模态buckling mode 复合材料力学mecha nics of composites 复合材料composite material 纤维复合材料fibrouscomposite 单向复合材料uni directio nalcomposite 泡沫复合材料foamed composite颗粒复合材料particulate composite 层板Lam in ate 夹层板sandwich panel 正交层板cross-ply laminate 斜交层板an gle-ply lam inate 层片Ply多胞固体cellular solid膨胀Expansion 压实Debulk 劣化Degradation 脱层Delam in ati on 脱粘Debond 纤维应力fiber stress 层应力plystress 层应变ply strain 层间应力interlaminar stress 比强度specific strength 强度折减系数stre ngth reductio n factor强度应力比strength -stress ratio 横向剪切模量tran sverse shear modulus 横观各向同性tran sverse isotropy 正交各向异Orthotropy 剪滞分析shear lag analysis 短纤维chopped fiber 长纤维continuous fiber 纤维方向fiber directi on 纤维断裂fiber break 纤维拔脱fiber pull-out 纤维增强fiber reinforcement 致密化Densification 最小重量设计optimum weight desig n 网格分析法netting analysis 混合律rule of mixture 失效准贝V failure criterion蔡 --- 吴失效准则Tsai-W u failurecriteri on达格代尔模型Dugdale model 断裂力学fracture mechanics概率断裂力学probabilistic fracture Mecha nics格里菲思理论Griffith theory线弹性断裂力学linear elastic fracturemecha ni cs, LEFM弹塑性断裂力学 elastic-plastic fracture mecha-nics, EPFM断裂 Fracture脆性断裂 解理断裂 蠕变断裂 延性断裂 晶间断裂 微裂纹 Microcrack 折裂Kink 椭圆裂纹 elliptical crack 深埋裂纹 embedded crack [钱]币状裂纹 penny-shape crack预制裂纹 Precrack 短裂纹 short crackbrittle fracturecleavage fracturecreep fractureductile fracturein ter-gra nu lar fracture准解理断裂 quasi-cleavage fracture穿晶断裂 trans-granular fracture 裂纹 裂缝 缺陷 割缝 CrackFlawDefectSlit表面裂纹surface crack裂纹钝化crack blunting裂纹分叉crack branching裂纹闭合crack closure裂纹前缘crack front裂纹嘴crack mouth裂纹张开角crack ope ning an gle,COA 裂纹张开位移crack ope ning displaceme nt, COD 裂纹阻力crack resista nee裂纹面crack surface裂纹尖端crack tip裂尖张角crack tip opening angle, CTOA 裂尖张开位移crack tip opening displaceme nt, CTOD裂尖奇异场crack tip singularity Field 裂纹扩展速率crack growth rate 稳定裂纹扩展stable crack growth 定常裂纹扩展steadycrack growth 亚临界裂纹扩展subcriticalcrack growth裂纹[扩展]减速crack retardation止裂crack arrest止裂韧度arrest toughness 断裂类型fracturemode 滑开型sliding mode 张开型openingmode 撕开型tearing mode 复合型mixedmode 撕裂Tearing 撕裂模量tearingmodulus 断裂准贝V fracture criterion J 积分J-integralJ 阻力曲线J-resistanee curve 断裂韧度fracture toughness 应力强度因子stress inten sity factor HRR 场Hutchinson-Rice-Rosengren Field 守恒积分conservationintegral 有效应力张量effective stress ten sor应变能密度strain energy density 能量释放率energy release rate 内聚区cohesive zone 塑性区plastic zone张拉区stretched zone热影响区heat affected zone, HAZ延脆转变温度brittle-ductile tran siti on temperature剪切带shear band剪切唇shear lip无损检测non-destructive inspection双边缺口试件double edge no tched specime n, DEN specimen单边缺口试件sin gle edge no tched specime n, SEN specimen二点弯曲试件three poi nt bending specime n, TPB specime n中心裂纹拉伸试件center cracked tension specime n, CCT specime n中心裂纹板试件center cracked pane specime n, CCP specime n紧凑拉伸试件compact tension specimen, CT specime n大范围屈服large scale yielding 小范围攻屈服small scale yielding 韦布尔分布Weibulldistribution帕里斯公式paris formula 空穴化Cavitation 应力腐蚀stress corrosion 概率风险判定probabilistic risk assessme nt, PRA损伤力学damage mechanics损伤Damage连续介质损伤力学continuum damage mecha nics细观损伤力学microscopic damagemecha nics累积损伤accumulated damage脆性损伤brittle damage延性损伤ductile damage宏观损伤macroscopic damage细观损伤microscopic damage 微观损伤microscopic damage 损伤准贝V damagecriterion 损伤演化方程damage evoluti onequati on 损伤软化damage softening 损伤强化damage strengthening 损伤张量damagetensor损伤阈值damage threshold 损伤变量damage variable 损伤矢量damage vector 损伤区damage zone 疲劳Fatigue 低周疲劳low cycle fatigue 应力疲劳stress fatigue 随机疲劳random fatigue 蠕变疲劳creep fatigue腐蚀疲劳corrosion fatigue 疲劳损伤fatiguedamage 疲劳失效fatigue failure 疲劳断裂fatigue fracture 疲劳裂纹fatigue crack 疲劳寿命fatigue life 疲劳破坏fatigue rupture 疲劳强度fatigue strength 疲劳辉纹fatiguestriations 疲劳阈值fatigue threshold 交变载荷alternating load 交变应力alternatingstress 应力幅值stress amplitude 应变疲劳strain fatigue 应力循环stress cycle 应力比stress ratio 安全寿命safe life 过载效应overloading effect 循环硬化cyclic hardening循环软化cyclic softening 环境效应environmental effect 裂纹片crack gage 裂纹扩展crack growth, crack Propagation 裂纹萌生crack initiation 循环比cycle ratio 实验应力分析experime ntal stress An alysis 工作[应变]片active[strain] gage 基底材料backing material 应力计stress gage零[点]飘移zero shift, zero drift 应变测量strain measurement 应变计strain gage 应变指示器strain indicator 应变花strain rosette应变灵敏度strain sensitivity机械式应变仪mecha ni cal strain gage 直角应变花rectangular rosette弓丨伸仪Extensometer 应变遥测telemetering of strain 横向灵敏系数transverse gage factor 横向灵敏度transverse sensitivity 焊接式应变计weldable strain gage 平衡电桥balaneedbridge 粘贴式应变计bon ded stra in gage 粘贴箔式应变计bonded foiled gage 粘贴丝式应变计bon ded wire gage 桥路平衡bridge balancing 电容应变计capacitanee strain gage 补偿片compensation technique 补偿技术compensation technique 基准电桥referenee bridge 电阻应变计resista nee strain gage 温度自补偿应变计self-temperature compe nsati ng gage半导体应变计semic on ductor strain Gage 集流器slip ring应变放大镜strain amplifier疲劳寿命计fatigue life gage 电感应变计inductanee [strain] gage 光[测]力学Photomechanics 光弹性Photoelasticity 光塑性Photoplasticity 杨氏条纹Young fringe 双折射效应birefrigent effect 等位移线con tourof equal Displaceme nt 暗条纹dark fringe 条纹倍增fringe multiplication 干涉条纹interferenee fringe 等差线Isochromatic 等倾线Isoclinic 等和线isopachic 应力光学定律stress- optic law 主应力迹线Isostatic 亮条纹light fringe 光程差optical path differenee 热光弹性photo-thermo -elasticity 光弹性贴片法photoelastic coat ing Method 光弹性夹片法photoelastic sandwichMethod动态光弹性dynamic photo-elasticity 空间滤波spatial filtering空间频率spatial frequency起偏镜Polarizer反射式光弹性仪reflection polariscope残余双折射效应residual birefringent Effect应变条纹值strain fringe value应变光学灵敏度stra in-optic sen sitivity 应力冻结效应stress freez ing effect 应力条纹值stress fringe value 应力光图stress-opticpattern暂时双折射效应temporary birefri ngent Effect脉冲全息法pulsed holography透射式光弹性仪tran smissi on polariscope 实时全息干涉法real-time holographic in terferometry网格法grid method全息光弹性法holo-photoelasticity全息图Hologram全息照相Holograph全息干涉法holographic interferometry 全息云纹法holographic moire technique 全息术Holography全场分析法whole-field analysis 散斑干涉法speckle interferometry 散斑Speckle错位散斑干涉法speckle-shearing in terferometry, shearography散斑图Specklegram白光散斑法white-light speckle method 云纹干涉法moire interferometry[叠栅]云纹moire fringe[叠栅]云纹法moire method云纹图moire pattern离面云纹法off-plane moire method参考栅referenee grating 试件栅specimengrating 分析栅analyzer grating 面内云纹法in-plane moire method 脆性涂层法brittle-coating method 条带法strip coating method坐标变换transformation of Coordinates计算结构力学computational structural mecha nics力口权残量法weighted residual method 有限差分法finite differenee method 有限[单]元法finite element method 配点法pointcollocation 里茨法Ritz method广义变分原理generalized variational Prin ciple最小二乘法least square method胡[海昌]一鹫津原理Hu-Washizu prin ciple 赫林格-赖斯纳原理Helli nger-Reiss ner Prin ciple 修正变分原理modified variationalPrin ciple约束变分原理constrained variational Prin ciple混合法mixed method杂交法hybrid method边界解法boundary solution method有限条法finite strip method半解析法semi-analytical method协调元conforming element 非协调元non-conforming element 混合元mixed element 杂交元hybrid element 边界元boundary element 强迫边界条件forced boundary con diti on 自然边界条件n atural boundary con diti on 离散化Discretization 离散系统discrete system 连续问题continuous problem 广义位移generalized displacement 广义载荷generalized load 广义应变generalized strain 广义应力generalized stress 界面变量in terface variable 节点no de, no dal point [单]元Element 角节点corner node 边节点mid-side node 内节点in ter nal node 无节点变量nodeless variable 杆元bar element桁架杆元truss element 梁元beam element 二维元two-dimensional element 一维元one-dimensional element 三维元three-dimensional element 车由对称元axisymmetric element 板元plate element 壳元shell element 厚板元thick plate element 三角形元triangular element 四边形元quadrilateral element 四面体元tetrahedralelement 曲线元curved element 二次元quadratic element 线性元linear element 三次元cubic element 四次元quartic element 等参[数]元isoparametric element 超参数元super-parametric element 亚参数元sub-parametric element 节点数可变元variable-number-nodeeleme nt拉格朗日元Lagra nge eleme nt 拉格朗日族Lagrange family巧凑边点元serendipity element 巧凑边点族serendipity family 无限元infinite element 单元分析element analysis 单元特性elementcharacteristics 刚度矩阵stiffness matrix 几何矩阵geometric matrix 等效节点力equivalent no dal force 节点位移no dal displaceme nt 节点载荷no dal load 位移矢量displacementvector 载荷矢量load vector 质量矩阵massmatrix 集总质量矩阵lumped mass matrix 相容质量矩阵con siste nt mass matrix 阻尼矩阵damping matrix 壬瑞利阻尼Rayleighdamping刚度矩阵的组集assembly of stiffness Matrices载荷矢量的组集con siste nt mass matrix质量矩阵的组集assembly of mass matrices单元的组集assembly of elements 局部坐标系local coord in ate system 局部坐标localcoordinate 面积坐标area coordinates 体积坐标volume coordinates 曲线坐标curvilinearcoord inates 静凝聚static condensation 合同变换contragradient transformation 形状函数shape function 试探函数trial function 检验函数test function 权函数weight function 样条函数spline function 代用函数substitutefunction 降阶积分reduced integration 零能模式zero-energy mode P 收敛p-c on vergenee H 收敛h-c on verge nee 掺混插值blended interpolation 等参数映射isoparametric mapping双线性插值bilinear interpolation 小块检验patch test非协调模式in compatible mode 节点号node number 单元号element number 带宽band width 带状矩阵banded matrix 变带状矩阵profile matrix 带宽最小化mini mizatio n of band width 波前法frontal method 子空间迭代法subspace iterati on method 行列式搜索法determ inant search method 逐步法step-by-step method 纽马克法Newmark 威尔逊法Wilson 拟牛顿法quasi-Newton method 牛顿-拉弗森法Newton-Raphson method 增量法in creme ntal method 初应变initial strain 初应力initial stress 切线刚度矩阵tangent stiffness matrix 割线刚度矩阵seca nt stiffness matrix 模态叠加法mode superposition method 平衡迭代equilibrium iteration 子结构Substructure子结构法substructure technique 超单元super-element 网格生成mesh generation 结构分析程序structural an alysis program 前处理pre-processing 后处理post-processing 网格细化mesh refinement 应力光顺stress smoothing组合结构composite structure 流体动力学fluid dynamics 连续介质力学mechanics of continuousmedia 介质medium 流体质点fluid particle 无粘性流体non viscous fluid, i nviscid fluid 连续介质假设continuous medium hypothesis 流体运动学fluid kinematics 水静力学hydrostatics液体静力学hydrostatics 支配方程governing equation 伯努利方程Bernoulli equation 伯努利定理Bernonlli theorem 毕奥-萨伐尔定律Biot-Savart law 欧拉方程Euler equation 亥姆霍兹定理Helmholtz theorem 开尔文定理Kelvin theorem 涡片vortex sheet 库塔-茹可夫斯基条件Kutta-Zhoukowski con diti on布拉休斯解Blasius solution 达朗贝尔佯廖d&;am #39;Alembert paradox 雷诺数Reyno Ids n umber 施特鲁哈尔数Strouhal number 随体导数material derivative 不可压缩流体in compre ible fluid 质量守恒co ervation of ma 动量守恒co ervation of momentum 能量守恒co ervation of energy 动量方程momentum equation 能量方程energy equation控制体积control volume 液体静压hydrostatic pre ure 涡量拟能e trophy 压差differential pre ure 流[动]flow 流线stream line 流面stream surface 流管stream tube 迹线path, path line 流场flow field 流态flow regime 流动参量flow parameter 流量flow rate, flow discharge 涡旋vortex 涡量vorticity 涡丝vortex filament 涡线vortex line 涡面vortex surface 涡层vortex layer 涡环vortex ring 涡对vortex pair 涡管vortex tube涡街vortex street卡门涡街Karman vortex street 马蹄涡horseshoe vortex 对流涡胞convective cell 卷筒涡胞roll cell 涡eddy 涡粘性eddy viscosity 环流circulation 环量circulation速度环量velocity circulation 偶极子doublet, dipole 驻点stagnation point 总压[力]total pre ure 总压头total head 静压头static head 总焓total enthalpy 能量输运energy tra ort 速度剖面velocity profile 库埃特流Couette flow 单相流single phase flow 单组份流single-component flow 均匀流uniform flow非均匀流nonuniform flow 二维流two-dime ionalflow 三维流three-dime ional flow 准定常流quasi-steady flow 非定常流u teady flow, non-steady flow 暂态流tra ient flow 周期流periodic flow 振荡流oscillatory flow 分层流stratified flow 无旋流irrotational flow 有旋流rotational flow 车由对称流axisymmetric flow 不可压缩性incompre ibility 不可压缩流[动]incompre ible flow 浮体floating body 定倾中心metacenter 阻力drag, resista nee 减阻drag reduction 表面力surface force 表面张力surface te ion 毛细[管]作用capillarity 来流in com ing flow自由流free stream 自由流线free stream line 夕卜流external flow 进口entrance, inlet 出口exit, outlet 扰动disturbanee, perturbation 分布distribution 传播propagation 色散di ersion 弥散di ersion 附加质量added ma ,a oeiated ma 收缩eontraetion 镜象法image method 无量纲参数dime ionle parameter 几何相似geometric similarity 运动相似kinematic similarity 动力相似[性]dynamic similarity 平面流plane flow 势potential 势流potential flow 速度势velocity potential 复势complex potential复速度complex velocity 流函数stream function 源source 汇sink 速度[水]头velocity head 拐角流corner flow 空泡流cavity flow 超空泡supercavity 超空泡流supercavity flow 空气动力学aerodynamics 低速空气动力学low- eed aerod yn amics 高速空气动力学high- eed aerod yn amics 气动热力学aerothermodynamics 亚声速流[动]su onic flow 跨声速流[动]tra onic flow 超声速流[动]supersonic flow 锥形流coni cal flow 楔流wedge flow 叶栅流cascade flow非平衡流[动]non-equilibrium flow 细长体slender body 细长度slenderne钝头体bluff body 钝体blunt body 翼型airfoil 翼弦chord 薄翼理论thin-airfoil theory 构型configuration 后缘trailing edge 迎角angle of attack 失速stall 脱体激波detached shock wave 波阻wave drag 诱导阻力induced drag 诱导速度induced velocity 临界雷诺数critical Reyno Ids nu mber 前缘涡leading edge vortex 附着涡bound vortex 约束涡confined vortex 气动中心aerodynamic center 气动力aerodynamic force 气动噪声aerodynamic noise 气动加热aerodynamicheating 离解di ociation地面效应ground effect 气体动力学gas dynamics 稀疏波rarefaction wave 热状态方程thermal equation of state 喷管Nozzle普朗特-迈耶流Prandtl-Meyer flow 瑞利流Rayleigh flow 可压缩流[动]compre ible flow 可压缩流体compre ible fluid 绝热流adiabatic flow 非绝热流diabatic flow 未扰动流undisturbed flow 等熵流isentropic flow 匀熵流homoentropic flow 兰金-于戈尼奥条件Ran ki ne-Hugo niot con diti on 状态方程equation of state量热状态方程caloric equati on of state 完全气体perfect gas 拉瓦尔喷管Laval nozzle 马赫角Mach angle 马赫锥Mach cone马赫线Mach line 马赫数Mach number 马赫波Mach wave 当地马赫数local Mach number 冲击波shock wave 激波shock wave正激波normal shock wave 斜激波oblique shock wave 头波bow wave附体激波attached shock wave 激波阵面shock front 激波层shock layer 压缩波compre ion wave 反射reflection 折射refraction 散射scattering 衍射diffraction 绕射diffraction 出口压力exit pre ure 超压[强]over pre ure 反压back pre ure 爆炸explosion爆轰det on ati on 缓燃deflagration 水动力学hydrodynamics 液体动力学hydrodynamics 泰勒不稳定性Taylor i tability 盖斯特纳波Gerstner wave 斯托克斯波Stokes wave 壬瑞利数Rayleigh number 自由面free surface 波速wave eed, wave velocity 波高wave height 波列wave train 波群wave group 波能wave energy 表面波surface wave 表面张力波capillary wave 规则波regular wave 不规则波irregular wave 浅水波shallow water wave 深水波deep water wave 重力波gravity wave 椭圆余弦波enoidal wave 潮波tidal wave 涌波surge wave 破碎波breaking wave 船波ship wave 非线性波nonlinear wave 孤立子soliton 水动[力]噪声hydrodynamic noise 水击water hammer 空化cavitation 空化数cavitation number 空蚀cavitation damage 超空化流supercavitating flow 水翼hydrofoil 水力学hydraulics 洪水波flood wave 涟漪ri le 消能energy di ipation 海洋水动力学marine hydrod ynamics 谢齐公式Chezy formula 欧拉数Euler number 弗劳德数Froude number 水力半径hydraulic radius水力坡度hvdraulic slope 高度水头elevating head 水头损失head lo 水位water level 水跃hydraulic jump 含水层aquifer 排水drain age 排放量discharge 壅水曲线back water curve 压[强水]头pre ure head 过水断面flow cro -section 明槽流open cha el flow 孑L流orifice flow 无压流free surface flow 有压流pre ure flow 缓流subcritical flow 急流supercritical flow 渐变流gradually varied flow 急变流rapidly varied flow 临界流critical flow 异重流de ity current, gravity flow 堰流weir flow掺气流aerated flow含沙流sediment-laden stream 降水曲线dropdown curve 沉积物sediment, deposit 沉[降堆]积sedimentation, deposition 沉降速度settling velocity 流动稳定性flow stability 不稳定性i tability 奥尔-索末菲方程Orr-Sommerfeld equation 涡量方程vorticity equation 泊肃叶流Poiseuille flow 奥辛流Oseen flow 剪切流shear flow 粘性流[动]viscous flow 层流laminar flow分离流separated flow 二次流sec on dary flow 近场流near field flow 远场流far field flow 滞止流stagnation flow 尾流wake [flow]回流back flow反流reverse flow 射流jet 自由射流free jet 管流pipe flow, tube flow 内流internal flow 拟序结构cohere nt structure 猝发过程bursting proce 表观粘度 a arent viscosity 运动粘性kinematic viscosity 动力粘性dynamic viscosity 泊poise 厘泊centipoise 厘沱centistoke 剪切层shear layer 次层sublayer 流动分离flow separation 层流分离laminar separation 湍流分离turbulent separation 分离点separation point 附着点attachment point 再附reattachment 再层流化relam in arizati on 起动涡starting vortex 驻涡standing vortex 涡旋破碎vortex breakdown 涡旋脱落vortex shedding 压[力]降pre ure drop 压差阻力pre ure drag 压力能pre ure energy 型阻profile drag 滑移速度slip velocity 无滑移条件non-slip condition 壁剪应力skin friction, frictional drag 壁剪切速度friction velocity 磨擦损失friction lo 磨擦因子friction factor耗散di ipation 滞后lag 相似性解similar solution 局域相似local similarity 气体润滑gas lubrication 液体动力润滑hydrod yn amic lubricati on 浆体slurry泰勒数Taylor number纳维-斯托克斯方程Navier-Stokes equation 牛顿流体Newtonian fluid边界层理论boundary later theory 边界层方程boundary layer equation 边界层boundary layer 附面层boundary layer层流边界层laminar boundary layer 湍流边界层turbulent boundary layer 温度边界层thermal boundary layer 边界层转捩boundary layer tra ition 边界层分离boundary layer separation 边界层厚度boundary layer thickne 位移厚度di lacement thickne 动量厚度momentum thickne 能量厚度energy thickne 焓厚度enthalpy thickne 注入injection 吸出suction 泰勒涡Taylor vortex 速度亏损律velocity defect law 形状因子shape factor 测速法anemometry粘度测定法visco[si] metry 流动显示flow visualization 油烟显示oil smoke visualization 孑L板流量计orifice meter 频率响应frequency re o e 油膜显示oil film visualization 阴影法shadow method 纹影法schlieren method 烟丝法smoke wire method 丝线法tuft method 氢泡法nydrogen bu le method 相似理论similarity theory 相似律similarity law 咅B分相似partial similarity 定理pi theorem, Buck in gham theorem 静[态]校准static calibration 动态校准dynamic calibration 风洞wind tu el 激波管shock tube激波管风洞shock tube wind tu el 水洞water tu el 拖曳水池towing tank旋臂水池rotating arm basin 扩散段diffuser 测压孑L pre ure tap 皮托管pitot tube 普雷斯顿管preston tube 斯坦顿管Stanton tube 文丘里管Venturi tube U 形管U-tube 压强计manometer 微压计microma nometer 多管压强计multiple manometer 静压管static [pre ure]tube 流速计an emometer 风速管Pitot- static tube 激光多普勒测速计laser Do ler an emometer, laser Do ler velocimeter 热线流速计hot-wire an emometer 热膜流速计hot- film an emometer 流量计flow meter 粘度计visco[si] meter 涡量计vorticitymeter 传感器tra ducer, se or压强传感器pre ure tra ducer 热敏电阻thermistor 示踪物tracer 时间线time line 脉线streak line 尺度效应scale effect 壁效应wall effect 堵塞blockage 堵寒效应blockage effect 动态响应dynamic re o e 响应频率re o e frequency 底压base pre ure 菲克定律Fick law 巴塞特力Ba et force 埃克特数Eckert number 格拉斯霍夫数Grashof number 努塞特数Nu elt number 普朗特数prandtl number 雷诺比拟Reyno Ids an alogy 施密特数schmidt number 斯坦顿数Stanton number 对流convection自由对流n atural con vecti on,free con vec-ti on 强迫对流forced convection 热对流heat convection 质量传递ma tra fer 传质系数ma tra fer coefficient 热量传递heat tra fer 传热系数heat tra fer coefficient 对流传热convective heat tra fer 辐射传热radiative heat tra fer 动量交换momentum tra fer 能量传递energy tra fer 传导conduction 热传导conductive heat tra fer 热交换heat exchange 临界热通量critical heat flux 浓度concentration 扩散diffusion 扩散性diffusivity 扩散率diffusivity 扩散速度diffusion velocity 分子扩散molecular diffusion沸腾boiling蒸发evaporation 气化gasification 凝结conde ation 成核nucleation 计算流体力学computational fluid mecha nics多重尺度问题multiple scale problem 伯格斯方程Burgers equation对流扩散方程con vecti on diffusi on equati on KDU 方程KDV equation 修正微分方程modified differe ntial equati on 拉克斯等价定理Lax equivale nee theorem 数值模拟numerical simulation 大涡模拟large eddy simulation 数值粘性numerical viscosity 非线性不稳定性nonlinear i tability 希尔特稳定性分析Hirt stability an alysis 相容条件co istency conditionCFL 条件Courant- Friedrichs- Lewycon diti on ,CFL con diti on 狄里克雷边界条件Dirichlet bou ndarycon diti on熵条件entropy condition远场边界条件far field boundary con diti on 流入边界条件inflow boundary con diti on 无反射边界条件non reflect ing boundary con diti on数值边界条件numerical boundary con diti on流出边界条件outflow boundary con diti on 冯■诺伊曼条件von Neuma condition 近似因子分解法a roximate factorization method人工压缩artificial compre ion人工粘性artificial viscosity边界元法boundary element method 配置方法collocation method 能量法energy method 有限体积法finite volume method 流体网格法fluid in cell method, FLIC method通量校正传输法flux-corrected tra ort method通量矢量分解法flux vector litt ing method 伽辽金法Galerkin method 积分方法integral method标记网格法marker and cell method, MAC method 特征线法method of characteristics 直线法method of lines 矩量法moment method 多重网格法multi- grid method 板块法panel method 质点网格法particle in cell method, PIC method质点法particle method 预估校正法predictor-corrector method 投影法projection method 准谱法eudo- ectral method 随机选取法random choice method 激波捕捉法shock-capturing method 激波拟合法shock-fitting method 谱方法ectral method 稀疏矩阵分解法lit coefficient matrix method不定常法time-dependent method 时间分步法time litting method 变分法variational method 涡方法vortex method 隐格式implicit scheme 显格式explicit scheme交替方向隐格式alter nati ng directi on implicit scheme, ADI scheme反扩散差分格式anti-diffusion differenee scheme紧差分格式compact differenee scheme 守恒差分格式co ervation differenee scheme克兰克-尼科尔森格式Cran k-Nicolson scheme杜福特-弗兰克尔格式Dufort-Fra nkel scheme 指数格式exponential scheme 戈本诺夫格式Godu nov scheme 高分辨率格式high resoluti on scheme 拉克斯-温德罗夫格式Lax-We ndroff scheme 蛙跳格式leap-frog scheme单调差分格式monotone differe nee scheme保单调差分格式monotonicity preserving differe nee scheme穆曼-科尔格式Murman-Cole scheme 半隐格式semi-implicit scheme 斜迎风格式skew-u tream scheme 全变差下降格式total variation decreasing scheme TVD scheme迎风格式u tream scheme , upwind scheme计算区域computational domain物理区域physical domain 影响域domai n of in flue nee 依赖域domain of dependence 区域分解domain decomposition 维数分解dime ion al lit 物理解physical solution 弱解weak solution 黎曼解算子Riema solver 守恒型co ervation form 弱守恒型weak co ervation form 强守恒型strong coervation form 散度型diverge nee form 贴体曲线坐标body- fitted curvilinear coordi-nates[自]适应网格[self-] adaptive mesh 适应网格生成adaptive grid gen erati on 自动网格生成automatic grid gen erati on 数值网格生成n umerical grid gen erati on 交错网格staggered mesh 网格雷诺数cell Reynolds number 数植扩散numerical diffusion 数值耗散numerical di ipation 数值色散numerical di ersion 数值通量numerical flux 放大因子amplification factor 放大矩阵amplification matrix 阻尼误差damping error 离散涡discrete vortex 熵通量entropy flux 熵函数entropy function 分步法fractional step method 广义连续统力学generalized continuum mecha nics 简单物质simple material 纯力学物质purely mechanical material微分型物质material of differential type 积分型物质material of integral type 混合物组份co tituents of a mixture 非协调理论in compatibility theory 微极理论micropolar theory 决定性原理principle of determinism 等存在原理principle of equipresenee 局部作用原理prin ciple of objectivity 客观性原理。

土木工程专业英语生词(个人整理版)

土木工程专业英语生词(个人整理版)

土木工程专业英语生词整理声明:本文档是笔者结合清华大学俞家欢老师《土木工程专业英语》与同济大学苏小卒老师《土木工程专业英语》上下册整理的一些土木工程领域常用的生词,仅供有需要的朋友学习交流使用。

可能有少量打错的字,请谅解。

barrages 水库canals 运河distributary 引流工程highway 公路expressway 高速公路(美式)levee 码头mitigate floods 减轻洪水construction 建造→施工survey 调查→工程勘察helipad 停机坪truck terminal 铁路站台sewage treatment 污水处理demolish 拆毁central government or local administration中央或地方政府reinvestment 再投资petroleum revenue 石油财政(指迪拜)resort island 度假岛desert country 沙漠地区国家waterfront 滨海区residential apartment 公寓住宅gulf 海湾buttressed design 扶壁设计tripod foundation 三脚架式基础tide and current 潮起潮落traffic congestion 交通拥挤regulate 限制financial crisis 金融危机escalate rent cost 租金持续上涨mega-project 大项目revale 媲美microcosm 缩影tropical cyclone 热带气旋(台风)downstream 产业链下游desalination 海水淡化distillation 蒸馏ubiquitous 无处不在的marine species 海洋生物density 重度(类似密度)gravity 重力→比重toughness 韧性ductility 延性brittleness 脆性creep 徐变,蠕变stiffness 刚度impact strength 冲击强度thermal 热力学特性corrosion resistance 耐腐蚀性acidity 酸性,酸度alkalinity 碱性,碱度sound 声absorption 吸收transmission 传导reflection 反射acoustical 声学特性optical 光学特性physiochemical 生化特性abrasion 磨损indentation 缺口,凹痕machining 蚀刻scratch 切削oxidize 氧化cement-mortar 水泥砂浆quarry 采掘lintel 过梁ballast 压载材料(铁轨下的垫材)brick 砖refractory brick 耐火砖ventilator 通风设备railway coaches 铁路车厢wagon 马车sleeper 枕木masonry construction 砌体结构gravel 砂石,砾石property 性能plastic stage 塑性workability 和易性mix 混合→拌和place 放置→浇筑compacte 压实finish 竣工homogeneity 同质性segregation 离析性coarse aggregate 粗骨料water tightness 水密性bleeding 裂隙pore 孔隙porous 多孔的harshness 粗糙的poorly graded aggregate 骨料级配不良withstand 抵抗moisture variation 潮湿变化freeze and thaw 冻融impermeability 密闭性resistance to wear and tear 耐磨性reinforced cement concrete 钢筋混凝土prestressed cement concrete 预应力混凝土silo 筒仓bunker 煤仓,地堡,掩体ornamental structure 装饰性结构tensile load 抗拉强度slab 板tall chimney 高烟囱aqueduct 高架渠ferro-cement 钢纤维混凝土skeletal steel 钢骨架pre-cast unit 预制单元(构件)vault 拱顶shell 壳结构grid surface 网格表面folded plate 褶皱板partition 隔断ductile 延展性好的susceptible to damage 易损坏harmony express 和谐号动车asbestos cement sheet 石棉水泥板shape memory alloy 形状记忆合金magnetostrictioe material 磁致伸缩材料piezoelectric material 压电材料electrorheological fluid 电流变材料viscosity 黏性deflection 挠度vibration 振动noise mitigation 噪声抑制bridge deck 桥面bridge pier 桥墩slab 板beam 梁grider 大梁、桁架restrained structure 超静定结构differential settlement 不均匀沉降hydrostatic load 静水荷载earth load 土压力earthquake load 地震荷载tile 瓦felt and gravel 毡及卵石层gypsum block 石膏wood stud 木栓texture of the building surface建筑表面形状纹理stiffness of the structure 建筑结构刚度stagnation pressure 风压wind suction 风吸力leeward 背风面的coefficient 系数gust factor 阵风系数essential factor 重要性系数hazardous facility 危险设备seismic load 地震荷载vibration 振型whiplash effect 鞭梢效应a portion of the base shear force底部剪力法storey 楼层hydraulic 水运elevator shaft 电梯井筒folded plate 折板屋顶bearing wall 承重墙shear wall 剪力墙unobstructed surface 无障碍表面erect 建造,建立residential 民用建筑institutional 公共结构serviceability 实用性failure 极限状态rehabilitation 加固verification 验证load transfer mechanism 荷载传递机理flexure 弯曲,屈曲torsion 扭转shear 剪切membrane 拱grid 柱reinforcement bars(rebars)钢筋patent 专利precast concrete 预制混凝土cast concrete 现浇混凝土brick chip 碎砖块cement hydrates 水泥水化物microscopic opaque crystal 微小透明晶体microscopic rigid lattice 微观晶格corrugated 有螺纹的cohesion 黏结力passivate 钝化(钢筋)chloride 氯离子provision 规定,要求moisture 潮湿,水分humidity 湿度,湿热curvature 弯曲,曲度,曲率singly-reinforced beam 单筋梁under-reinforced beam 少筋梁over-reinforced beam 超筋梁balanced-reinforced beam 适筋梁instantaneous 立即,突然material-safety factor 安全系数allowable stress design 许用应力设计flake 剥落mix design 配合比设计penetrate 侵入serviceability failure in limit state design正常使用极限状态破坏bond failure 黏结失效carbonation 碳化作用neutralisation 中和作用(即碳化作用)optimal 最佳选择phenolphthalein indicator 酚酞指示剂admixtures 外加剂rapid set-up 快速初凝mitigate 减轻,缓和capillary 毛细管sound attenuating layer 隔音层slump 坍落度concrete vibrating 振捣steel sire 箍筋iron chain suspension bridge 铁链吊桥rivets connection 铆钉连接wrought iron technology 锻铁技术cast iron 铸铁high-strength bolt 高强度螺栓fabrication 制作technical code 技术规程cold-formed thin-wall steel 冷弯薄壁型钢masonry 砌体材料plasticity 塑性tenacity 韧性isotropic 各项异性ideal elastic-plastic 理想弹塑体proportional limit 比例极限(σp)yield strength 屈服强度tensile strength 抗拉强度fabrication 制作weldability 焊接性能air tightness 气密性press vessel 压力容器heat resistance 耐热性non-refractory 防火性能差fire proof protection 防火保护brittle fracture 脆性断裂large span structure 大跨度结构crane 吊车profiled steel sheet 异型钢板mega-frame structure 组合结构demountable structure 可拆卸结构steel scaffolding 钢脚桁架rupture 破裂buckling 搭扣,屈曲formation of mechanism 形成机构(塑性铰)wind induced oscillation 风致振动provision 规定load-carrying structure 承重结构percentage of elongation 伸长率cold-bending test 冷弯实验single story frame 单层结构bridge crane 桥式起重机residual stress 残余应力sun-dried mud 晒干的泥土shale 页岩lateral load 水平荷载seismic 地震raw material 原材料mortar 砂浆mica 云母filthy 有机杂质odor 气体iron compound 铁化合物mold 模具stirrup 箍筋gravel 砾石compact sand 紧密的砂土trench 沟槽over footing 地梁adherence 黏结性confining column 构造柱minimum covering for concrete最小保护层厚度water cement ratio 水灰比mid-rise segment 中高层建筑glulam beam 胶合木梁dwelling 住宅sport arene 运动场better seismic performance更好的抗震性能interior 内部gypsum 石膏板external cladding 外覆盖层fire-rated assembly 防火组件hybrid construction 混合结构practical 实用的exterior infill wall 外部填充墙energy performance 节能性能renovation 装修flat roof 平屋面extra accommodation 阁楼solid wood panel 实木板freight 运送到up-front invesrment 前期投资mortise 榫眼,榫接tenon 榫erected 直立的flammable 易燃物purlin 檩条spatial construction 空间结构high load-bearing capacity很高的荷载承担能力compaction 密实erection 建造hollow steel tube 中空钢管unfilled tube 中空钢管confinement 约束作用schematic view 示意图favorable stress distribution有利的荷载分布terrain 地形cantilever bridge 悬臂桥arch bridge 拱桥suspension bridge 悬索桥cable-stayed bridge 斜拉桥truss bridge 桁架桥pier 桥墩dissipation 消散(荷载)box girder 箱梁meticulous analysis 精细分析foot bridge 人行桥false work 脚手架counter balance 平衡抵消anchor arm 锚固臂outermost 最外侧pinned joint 铰接节点segment construction 分布施工canyon 峡谷abutment 桥墩(基台)viaduct 高架桥thrust 推力spandrel 拱尖catenary 锁链aforementioned 如前所述的bluff 悬崖pillar 塔架slender 细的parabola 抛物线lattice girder 格构梁drought 干旱flood 洪水cyclone 飓风environmental degradation 环境恶化meteological disaster 气象灾害casualty 伤亡invariably 始终如一的secondary disaster 次生灾害earthquake portent 地震预警landslide 滑坡collapse 崩塌debris flow 泥石流river erosion 河流侵蚀turbid 浑浊fissure 裂缝resilient 弹回,有弹力的sewerage 污水,排水设备snowmelt 融雪水escalation of cast 超过预算time overrun 工期延长pharmaceutical 制药mitigate potential risk 化解潜在风险tenet 宗旨aqueduct 高架渠,渡槽ballistic 弹道学causeway 长堤,堤道channel 沟渠,海峡,槽钢equilibrium 平衡(状态)excavation 挖掘hydraulic 水力的mason 砖瓦石匠obelisk 方尖石塔quarry 采石场sewage 污水reimbursable 可报销的,可补偿的aerated concrete 加气混凝土aggregate 骨料binding agent 粘合剂bitumen 沥青blunt 钝的bolt 螺栓cast 浇筑clamp 夹子corrode 腐蚀course (砖)层,行form 模板grout 薄砂浆,灰浆multistory building 多层建筑rate of contraction 收缩率rate of expansion 膨胀率rivet 铆钉,铆接screw 螺丝钉slab 平板spray 喷射tarlike 沥青thread 螺纹tile 瓦片versatile 多用途的weld 焊接blastfurnace 高炉矿渣asbestos 石棉瓦modulus of rupture 断裂模量hydration 水化作用cohesive 粘性的rapid-hardening 速凝grading 级配dampness 湿度,含水量accelerator 速凝剂inhibitor 抑制剂plasticizer 塑化剂grouting agent 灌浆剂consistency 稠度mobility 流动性compactability 可密实性biaxial 二轴的distortion 扭曲,变形elongate 拉长,延长moment 力矩prismatic 棱柱形的superposition 迭加作用transverse 横向的triaxial 三轴的,空间的vessel 容器bracing 拉条,撑杆conservation of energy 能量守恒conveyor 输送机deviation 偏差flexibility coefficient 柔度系数method of section 截面法pin connection 铰接principle of virtual work 虚功原理redundant force 冗余力sever 断开,分开support reaction 支反力truss 桁架unit-load method 单位荷载法corridor 走廊counteration 退化ductile failure 延性破坏erection 直立建筑物impact factor 冲击系数iterative 重复的,反复的layout 规划,设计图案maintainability 可维护性monorail 单轨铁路quasi-permanent 准永久的sustained 持续不变的tenant 承租人torque 扭矩torsional 扭力,扭转的buggy 手推运料车commentary 注释,条文规范contractor 承包商couple 力偶entrain 加气(给混凝土)fire rating 耐火等级oscillate 摆动,震动rigidity 刚度shoring 支撑anchorage 锚固centroid 形心concrete cover 混凝土保护层eccentricity 偏心距helix 螺旋线的incipient 刚出现的lap splice 搭接longitudinal 纵向的pitch 坡度spall 剥落symmetrical 对称的tie 绑扎(钢筋)curvature 曲率detrimental 有害的flange 翼缘web 腹板render 粉刷,抹灰foundry 铸造厂incombustible 防火的residual 残余的stocky 短粗的vitreous 玻璃的withstand 抵抗,承受gusset 节点板,角板imperfection 缺陷purlin 檩条rafter 椽子slenderness 长细比spandrel 拱肩,托梁stringer 桁条,纵梁sway 晃动,侧接移forge 锻造inspection 检查,弹伤shank 末梢wrench 扳手nut 螺母slag 钢渣coordinate 坐标cruise 勘察datum 基准面elevation 高程,海拔remote sensing 遥感conductivity 传导性gradient 梯度ballast 石渣boulder 漂石cobble 卵石cohesive 有粘聚力的consolidation 固结depression 降低fine 细粒grit 粗砂silt 淤泥immediate settlement 瞬时沉降consolidation settlement 固结沉降pore water 孔隙水back-acting shovel 反铲(挖掘机的)bearing capacity 承载力bore hole 钻孔boring 钻探coefficient of permeability 渗透系数proposed structure 拟建结构shear vane test 十字板剪切试验consistency 稠度attorney 代理人currency 流通货币dispatch 派遣elicit 引出procure 获得remuneration 报酬stipulate 规定surety 担保tendering 招标,投标withhold 保留bidder 投标人contemplate 注视letting 公开开标recourse 追索stock holder 股东performance bond 履约profit margin 利润率stem from 基于a letter of intent 意向书rule of thumb 经验方法radius of gyration 回转半径transverse load 横向荷载shop-fabricated 工厂预制的capping beam 压顶梁channel element 槽型构件cladding brickwork 维护砌体cornice 檐口,飞檐finish 饰面,粉刷flat slab 无梁板footing 基础,垫层head room 净空高度joist 托梁,肋maritime 靠海的,港口的two-way slab 双向板waffle slab 密肋板yield line 塑性铰线inflate 充气,使膨胀perturbation 摄动,扰动cavity wall 空心墙chicken-wire 铁丝织网cut-and-try 试验性的emulsion 乳胶head(end) joint 端灰缝high-lift 高扬程的mortar bed 砂浆平缝partition 分隔墙mortar joint 灰缝retarder 缓凝剂rubble 毛石,块石veneer 饰面,镶板retaining wall 挡土墙custom-designed 定制cut-and-fill 挖方和填方placement 浇捣concrete batching plant 混凝土搅拌站bentonite slurry 泥浆asphalt 沥青,柏油gutter 排水沟auger boring 螺纹钻探group pile-efficiency 群桩效应in-situ 现场的,原位的fracture 断裂hysteresis 滞回inter-storey drift 层间位移longitudinal reinforcement 纵筋monotonic loading 单调加载partial safety factor 分项系数secondary-order effects 二阶效应shear span 剪跨sidesway 侧倾,侧移。

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Mechanical properties in the semi-solid state andhot tearing of aluminium alloysD.G.Eskin a ,Suyitno b ,L.Katgermana,b,*a Netherlands Institute for Metals Research,Rotterdamseweg 137,2628AL Delft,The Netherlandsb Delft University of Technology,Rotterdamseweg 137,2628AL Delft,The NetherlandsAbstractThis review represents a comprehensive coverage of results reported in the literature over last 50years on the methods of studying hot tearing and mechanical properties of semi-solid aluminium alloys;the mechanical properties of these alloys in the semi-solid state;and hot tearing criteria.While compiling this review,the authors attempted to include in it all available sources including quite a few works never published in English before.The review consists of three parts.The first part introduces the reader to the phenomenon of hot tearing.The second part describes different techniques for testing metallic alloys in the semi-solid state and sum-marizes reported results on strength and ductility of semi-solid model and commercial alu-minium alloys.The third part describes the methods for assessing hot tearing susceptibility of aluminium alloys,gives the results on hot cracking of various aluminium alloys and discusses different hot tearing criteria.Ó2003Elsevier Ltd.All rights reserved.Contents1.Introduction:theories of hot tearing...........................................................................................6302.Mechanical properties of aluminium alloys in the semi-solid state .................................6352.1.Techniques of testing metallic alloys in the semi-solid state .................................6352.1.1.Tensile tests...............................................................................................................6352.1.2.Shear tests..................................................................................................................pression tests...................................................................................................6452.2.Strength properties of aluminium alloys in the semi-solid state ..........................6452.2.1.Strength properties of semi-solid aluminium and model alloys ...........6452.2.2.Strength properties of semi-solid commercial alloys.................................653*Corresponding author.Tel.:+31-15-278-2249;fax:+31-15-278-6730.E-mail address:l.katgerman@tnw.tudelft.nl (L.Katgerman).0079-6425/$-see front matter Ó2003Elsevier Ltd.All rights reserved.doi:10.1016/S0079-6425(03)00037-9/locate/pmatsciProgress in Materials Science 49(2004)629–711630 D.G.Eskin et al./Progress in Materials Science49(2004)629–7112.3.Ductility of semi-solid aluminium alloys (663)2.3.1.Effect of some parameters on the ductility of semi-solid aluminiumalloys (665)2.3.2.Ductility of semi-solid binary aluminium alloys (670)2.3.3.Ductility of semi-solid ternary alloys (671)2.3.4.Ductility of semi-solid commercial aluminium alloys (673)3.Hot tearing (676)3.1.Methods for assessing hot tearing susceptibility (676)3.1.1.Ring mould testing (676)3.1.2.‘‘Coldfinger’’testing (679)3.1.3.Backbone mould testing (681)3.1.4.Tensile testing (683)3.2.Hot cracking susceptibility of aluminium alloys (684)3.2.1.Binary alloys (684)3.2.2.Ternary alloys (684)mercial alloys (688)3.3.Hot tearing criteria (692)3.3.1.Stress-based criteria (692)3.3.2.Strain-based criteria (700)3.3.3.Strain rate-based criteria (701)3.3.4.Criteria based on other principles (704)parison of hot tearing criteria (708)4.Concluding remarks (708)Acknowledgements (709)References (709)1.Introduction:theories of hot tearingThe solidification of alloys always occurs in some temperature range called the solidification or freezing range.On decreasing temperature,the solid phase nucle-ates,grows in a form of grains(usually dendritic in shape)and,starting from a certain point in the solidification range,grains start to interact with each other,first by feeling the presence of neighbours,then by contacting and bridging with them, andfinally by forming a continuous skeleton of the solid phase.The temperature at which the grains start to interact is called the coherence point,and the temperature when the continuous solid network is formed,the rigidity point.Below this rigidity point,the semi-solid body acquires the main characteristics of the solid phase––retention of the shape and mechanical properties,such as strength and ductility.Obviously,the thermomechanical behaviour of the semi-solid body depends very much on its mechanical properties.On one hand,there are intrinsic properties of this body(strength and ductility)and,on the other hand––stresses and strains induced in it during the process of solidification and resulted from solidification shrinkage, metallostatic pressure,hindered thermal contraction,thermal gradients etc.D.G.Eskin et al./Progress in Materials Science49(2004)629–711631Unlike pure metals,which solidify at one temperature,alloys transform gradually from liquid to solid over a(wide)temperature interval.During casting there is a considerable time during which the alloy consists of both solid and liquid.The material in this semi-solid state is divided into two classes:slurries and mush.A slurry is denned as a liquid with suspended solid particles.At some temperature solid grains start to interact with each other and the material develops a certain strength. Below this temperature,the material is called a mush,i.e.a solid network with liquid in between.The solid fraction at which this transition occurs varies between0.25and 0.6,depending on the morphology of the solid particles.Because of the strongly different mechanical behaviour of these different morphologies,slurries are usually described by viscosity-based models,and mush is usually described by deformation-based models[1].The viscosity-based models start from the liquid side and are modified to take into account the effect of the increasing amount of solid particles. The deformation-based models are based on models for hot working,which are modified to take into account the presence of liquid.The transition from a slurry to a mush remains a complicated problem to model,and a satisfactory model, which describes the behaviour for the complete solidification range,is yet to be developed.The casting practice of alloys is only too familiar with various defects occurring in thefinal product.One of the main defects is hot tearing or hot cracking,or hot shortness.Irrespective of the name,this phenomenon represents the formation of an irreversible crack(failure)in the still semi-solid casting.Industrial and fundamental studies of this phenomenon show that hot tearing occurs in the late stages of solidification when the volume fraction of solid is above 85–95%and the solid phase is organized in a continuous network of grains.It is also known that afine grain structure and controlled casting(without large temperature and stress gradients)help to avoid hot cracking.The correlation between the hot cracking susceptibility and the composition of an alloy is well established.The link between the appearance of hot tears and the mechanical properties in the semi-solid state is obvious.And this connection was explored for decades.Never-theless,the development of new theories,models and criteria for hot tearing is underway in the current metals science.During DC casting of aluminium alloys,the primary and secondary cooling causes strong thermal gradients in the ingot which may lead to distortion of the ingot shape(e.g.butt curl,butt swell,rolling face pull-in)and/or to hot tearing and cold cracking.In DC casting,the name‘‘mushy zone’’is misleading,as its top part is actually a slurry,because the newly formed grains are still suspended in the liquid. Only after the temperature has dropped below the coherency temperature,a real mush is formed.The deformation behaviour of the mush is very critical for the formation of pores or hot tears.From many studies[2–10]starting in the1950s,and reviewed by Novikov[11]and Sigworth[12],it appears that hot tears initiate above the solidus temperature and propagate in the interdendritic liquidfilm.This results in a bumpy fracture surface covered with a smooth layer and sometimes with solid bridges that connect or connected both sides of the crack[9,10,13–19].During solidification,the liquidflow632 D.G.Eskin et al./Progress in Materials Science49(2004)629–711through the mushy zone decreases until it becomes insufficient tofill initiated cavities so that they can grow further.The solidification process can be divided into four stages,based on the perme-ability of the solid network[4,7,10,20]:1.Mass feeding,in which both liquid and solid are free to move.2.Interdendritic feeding,in which the remaining liquid has toflow through the den-dritic network.After the dendrites have formed a solid skeleton,the remaining liquid has toflow through the dendritic network.A pressure gradient may devel-op across the mushy zone by solidification shrinkage occurring deeper in the mushy zone.However at this stage the permeability of the network is still large enough to prevent pore formation.3.Interdendritic separation,in which the liquid network becomes fragmented andpore formation or hot tearing may occur.With increasing solid fraction,liquid is isolated in pockets or immobilised by surface tension.When the permeability of the solid network becomes too small for the liquid toflow,further thermal con-traction of the solid will cause pore formation or hot tearing.4.Interdendritic bridging or solid feeding,in which the ingot has developed a consid-erable strength and solid-state creep compensates further contraction.At thefinal stage of solidificationðf S>0:9Þ,only isolated liquid pockets remain and the ingot has a considerable strength.Solid-state creep can now only compensate solidifica-tion shrinkage and thermal stresses.In this review we will mainly consider the last two stages,since in a slurry and during the interdendritic feeding stage in the mush feeding is usually sufficient to avoid any casting defects.It is mainly the‘‘interdendritic separation’’stage in which the ingot is vulnerable to pore formation and hot tearing.A large freezing range alloy promotes hot tearing since such an alloy spends a longer time in the vulnerable state in which thin liquidfilms exist between the den-drites.The liquidfilm distribution is determined by the dihedral angle h.With a low dihedral angle,the liquid will tend to spread out over the grain boundary surface, which strongly reduces the dendrite coherence.With a high dihedral angle the liquid will remain as droplets at the triple points so that the solid network holds its strength.Apart from these intrinsic factors,the solidification shrinkage and thermal con-traction impose strains and stresses on the solid network,which are required for hot tearing.It is argued that it is mainly the strain and the strain rate,which are critical for hot tearing[3,10].Stresses do not seem critical as the forces available during solidi-fication are very high compared to the stresses a semi-solid network can resist[10].A lot of efforts have been devoted to understand the hot tearing phenomenon. The compilation of research in thisfield has been done by Novikov[11]and Sig-worth[12].Zheng et al.[21]reviewed the possible causes of hot tearing.A few mechanisms of hot tearing are already suggested in literature.Some of those are briefly described below.Novikov and Novik[22]have reported that at low strain rates the grain boundary sliding is the main mechanism of deformation of a semi-solid body.The load appliedD.G.Eskin et al./Progress in Materials Science49(2004)629–711633 to the semi-solid body will be accommodated by a grain boundary displacement that is lubricated by liquidfilm surrounding the grain.Prokhorov[23]proposed a model for deformation of the semi-solid body.If two tangential forces s1and s2are applied to the equilibrium semi-solid body,the response of the body manifests itself as the grain movement and at some point the grains will touch each other.The liquid covering the grain will circulate to the lowest pressure point.Further deformation will be possible if the surface tension and resistance to liquidflow are sufficient to accommodate the stress imposed.If not,a brittle intergranular fracture or hot tearing will occur.In relation to this theory,Prokhorov postulated that:(1)an in-crease infilm thickness increases the fracture strain,(2)a decrease in grain size in-creases the fracture strain,(3)any non-uniformity of grain size decreases the fracture strain.Based on this theory,the main measure for hot tearing is the ductility of the semi-solid body.A hot tear will occur if the strain of the body exceeds its ductility.A theory of shrinkage-related brittleness divides the solidification range into two parts.In the upper part the coherent solid-phase network does not exist.Cracks or defects occurring in this stage can be healed by liquidflow.As the solidification progresses and the solid fraction further increases,at a certain stage or a certain solid fraction a coherent network is formed.This stage is considered as the start of linear shrinkage.Since the coherence point,the shrinkage stress is imposed onto the semi-solid body.Fracture or hot tearing occurs if the shrinkage stress exceeds the rupture stress[24,25].Pellini[3]suggested a hot tearing theory based on the strain accumulation with the following main features:(1)cracking occurs in a hot spot region,(2)hot tearing is a strain-controlled phenomenon which occurs if the accumulated strain of the hot spot reaches a certain critical value,and(3)the strain accumulated at the hot spot depends on the strain rate and time required for a sample to pass through afilm stage.The most important factor of hot tearing based on this theory is the total strain on the hot spot region.The total strain is the additive of strain over a period within which the hot spot exists.Taking into account that the highest strain accu-mulates in the liquidfilm,Dodd[26]and Metz and Flemings[27]explain the increase of hot tearing caused by the segregation of a low-melting component from the viewpoint that this addition increases the time of the liquidfilm existence.Although Pellini mentions a critical value of the accumulated strain,it is not clear whether it is ductility or another entity.Pellini’s theory is a basis for a hot tearing criterion proposed by Clyne and Davies[28].Some authors suggest that it is not the strain but the strain rate which is the critical parameter for hot cracking.The physical explanation of this approach at that the strain rate during solidification is limited by the minimum strain rate at which the material will fracture.Prokhorov[23]is thefirst who suggested a criterion based on this approach.More recently,a strain-rate based hot tearing criterion is proposed by Rappaz et al.[29].Yet another approach to the hot tearing phenomenon is the assumption that failure happens at a critical stress.The liquid surrounding the grain is considered as a stress riser of the semi-solid body[30,31].In this theory,a liquid-filled crack is considered as a crack initiation.The propagation of the crack initiator is determined634 D.G.Eskin et al./Progress in Materials Science49(2004)629–711by the critical stress[31].The critical stress is mostly determined using the modified Griffith energy balance approach.The modification of the Griffith approach is particularly in accounting for the effect of plasticity as proposed by Gilman[32]and Orowan[33].Another approach within the fracture mechanics theory is proposed by Sigworth[12]who considers a possibility of applying a liquid-metal-embrittlement concept to the hot tearing case.There is also a group of hot tearing theories that consider the hindered feeding of the solid phase by the liquid as the main cause of hot tearing.Niyama[34]and Feurer[35]use this approach to derive the hot tearing criterion.Based on this theory,the hot tear will not occur as long as there is no lack of feeding during solidification.Clyne and Davies[7,28,36]give more attention to the time spent in the mushy state.The last stage of solidification is considered as most susceptible to hot tearing.However,on further decreasing of the liquid fraction the bridging between adjacent dendrites is established so that the interdendritic separation is prevented.Several hot tearing criteria have been developed in the past decades.Feurer[6] used thefluidflow through a porous network to calculate the afterfeeding by liquid metal.Hot tears will initiate when this afterfeeding cannot compensate the solidifi-cation shrinkage.Clyne and Davies[7]defined a cracking susceptibility coefficient (CSC)as the ratio between the time t V during which the alloy is prone to hot tearing and the time t R during which stress relaxation and afterfeeding can take place.These times are defined as the periods during which the fraction liquid is between0.1and 0.01and between0.1and0.6respectively.These criteria were combined with a heat flow model describing the DC casting process by Katgerman[37].This enabled the determination of the cracking susceptibility coefficient as a function of the casting parameters.Unfortunately,the above criteria are restricted in their use because they give only a qualitative indication for the hot tearing susceptibility.Thefirst two-phase model,which takes into account bothfluidflow and defor-mation of the solid network,is the Rappaz–Drezet–Gremaud(RDG)hot tearing criterion[29].The RDG criterion is formulated on the basis of afterfeeding,which is limited by the permeability of the mushy zone.At the solidification front the per-meability is high but deeper in the mushy zone the permeability is restricted.A pressure drop along the mushy zone exists which is a function of this permeability and the strain rate.If the local pressure becomes lower than a critical pressure,a cavity is initiated.The model is implemented in a thermomechanical model for DC casting by Drezet et al.[38]to predict hot tearing during billet casting.The hot tearing susceptibility is found higher during start-up of the casting and in the centre of the billet,which agrees with general casting practice.A further development of the RDG criterion is carried out by Braccini et al.[39], They included plastic deformation of the solid phase and a criterion for the growth of a cavity.They base their model on two simplified geometric models,one for a columnar dendritic and one for an equiaxed dendritic structure.Explicit relations are developed for critical strain rates and they indicate that the critical strain rate de-creases with increasing solid fraction.Many studies have used tensile testing at semi-solid temperatures to study hot tearing either by in situ solidification experiments[13–15,20,40–42]or by reheatingD.G.Eskin et al./Progress in Materials Science49(2004)629–711635 specimens from room temperature[17,18,31,41,43,44].Both techniques led to the following general results.In several aluminium alloys it is observed that both strength and ductility strongly decrease from just below the solidus temperature to the semi-solid state,while the fracture surface changes from rough,related to the ductile behaviour,to smooth,related to the presence of a liquidfilm.Further,cracks initiate at micropores or molten inclusions and continue along grain boundaries.This review has the aim to summarize numerous results reported in the literature over the last50years on the methods of studying hot tearing and mechanical properties of semi-solid aluminium alloys;the mechanical properties in the semi-solid state;and hot tearing criteria that use these properties.Quite a few results in this review are from Russian works performed between1950and1970and largely unknown to Western scientists.2.Mechanical properties of aluminium alloys in the semi-solid stateOver the last60years there were a lot of attempts to determine the properties of metallic alloys in the semi-solid state.Some of these attempts were highly successful, others not,but nevertheless they suggested interesting approaches.In this chapter we will describe and discuss various designs and approaches toward the same goal––to estimate the mechanical behaviour of semi-solid metallic alloys.Most of the con-sidered works were staged to examine and study the phenomenon known as hot tearing,hot cracking or hot shortness,in other words the failure of the semi-solid mush under external or internally-induced stresses.The necessary condition for an alloy to be tested for mechanical properties is the ability to retain the shape and to transfer stress.In a lower part of the solidification range,so-called solid-liquid or semi-solid part,alloys meet that condition and, therefore can be mechanically tested.The mechanical testing can be performed in two ways:by heating the sample to a certain temperature above the solidus(remelting)or by cooling the liquid alloy to a certain temperature below the liquidus(solidification).The structures thus obtained are different,and so are the results of mechanical tests.First,we consider different techniques for measuring or estimating mechanical properties(strength at failure,yield strength,elongation to failure).These methods can be conditionally classified as tensile,shear(including torque)and compression tests performed upon remelting or solidification.In the second half of this chapter the strength and plastic properties of various model and commercial aluminium alloys will be presented.2.1.Techniques of testing metallic alloys in the semi-solid state2.1.1.Tensile tests2.1.1.1.Tensile tests upon remelting.The main difficulty during tensile tests of semi-solid samples is their very low strength and ductility due to the presence of liquid636 D.G.Eskin et al./Progress in Materials Science49(2004)629–711films at grain boundaries.Therefore,the conventional tensile testing machines cannot be directly used for studying the mechanical properties of mushy alloys.Thefirst tests of the strength of semi-solid materials go back to the beginning of the20th century when Norton[45]tested an aluminium alloy by suspending various weights to a solidifying sample.Tamman and Rocha[46]and Ver€o[47]used plane and notched cylindrical sample,respectively,to determine the tensile strength of binary and commercial alloys above solidus.It was shown that the ultimate tensile strength and ductility dropped at a temperature of solidus.A reliable testing machine for tensile tests of aluminium alloys above solidus was designed and used by Singer and Cottrell[48]for studying Al–Si alloys.These au-thors decided that the sample should be short and completely surrounded by ma-chine clamps in order to prevent shape distortion.The sample was tested in the horizontal direction.The determined property was the ultimate tensile strength,the elongation being almost zero.Researchers who studied hot cracking upon welding used mainlyflat-shaped specimens cut from sheets.Pumphrey and Jennings[49]heated a plane Al–Si specimen in a lead bath and tested it upon tension in the vertical direction at a rate of25mm/min.The temperature dependence of the ultimate tensile strength was constructed,but not for the elongation that scattered above solidus between0%and 3%.The analysis of literature data shows that to the end of1940s the techniques forassessing the ultimate tensile strength of semi-solid aluminium alloys were well-established.However,there were no reliable methods to measure the elongation or other plastic characteristics of alloys heated above their solidus.These techniques were developed in the1950s mainly due to the efforts of Russian scientists,e.g.Refs. [50,51].The main difficulties with respect to the measurement of elongation in the semi-solid state were(1)poor centring of the sample and,therefore,offset of the load and (2)low accuracy of measurements.The simplest way to solve thefirst problem is to use the scheme where the sample self-centres under gravity[11,50](Fig.1a).Pull rod is connected to the lower clamp through a hinge and has a light reservoir attached to its lower end.Lead pellets are fed to this reservoir at a constant rate until the sample fails.In all experiments the loading rate was10N/s.The ultimate tensile strength is determined by the ratio of thefinal load(plus the weight of the lower clamp)to the initial cross-section of the sample.The elongation was determined by measuring the distance l between two preliminary made marks on the sampleðEl¼ðl fÀl0Þ=l0Þ.The disadvantages of this technique are(1)no control of the strain rate and(2) lower measurable limit of the fracture stress($30kPa).However,the ease of tests and the reproducibility of results allowed Novikov[11] to perform very important measurements for various model and commercial alu-minium alloys.Later,another testing machine was designed[11]enabling one to control the tensile rate from0.3to25mm/min and to record the load.Fig.2a demonstrates an example of a tensile curve recorded for an Al–6%Cu alloy tested at 570°C (22°C above the solidus)and at a strain rate of 1mm/min.The typical feature of stress–strain curves for semi-solid testing is a well-pronounced branch of gradually decreasing stress,despite brittle fracture.Novikov [11]explained this phenomenon by the local deformation of solid bridges and extension of liquid intergranular films existing in the semi-solid sample.As a result,the effective cross-section of the sample decreases and the stress–strain curve shows the gradual de-crease of the stress.However,the corresponding elongation is fiction as the sample is already fractured.Therefore,the actual elongation is more reliable to determine by measurements in a microscope on the fractured sample after the test.Prokhorov and Bochai [51]have designed a testing machine in which a long,flat sample lies in the furnace on a copper support and is deformed mechanically.The Fig.1.Tensile machines for testing aluminium alloys upon remelting:(a)for evaluation of tensile strength and elongation to failure [11]1,upper clamp;2,axis;3,prism;4,lower clamp;5,pull rod;and 6,furnace;(b)Gleeble 1500/H10K-C low force tensile machine for testing semi-solid aluminium alloys [17](repro-duced by permission of H.G.Suzuki (National Institute for Metals Research,Tsukuba,Japan),D.Fer-guson (Dynamics Systems,Inc.,USA),and J.A Spittle (University of Wales,Swansea,UK)).D.G.Eskin et al./Progress in Materials Science 49(2004)629–711637load is applied through and measured by a dynamometer.The elongation of the sample is measured by an optical extensometer or by measuring the distance between marks on the sample.A large gauge length of the sample (200mm)provides for large measured absolute elongations and therefore increases the accuracy of determination of a rather small relative elongation.It is worth mentioning here that plane specimens cut from rolled or extruded billets are quite useful for studying semi-solid properties and sensitivity to hot cracking of welded joints and heat affected zones.But deformed samples should not be used for studying semi-solid properties and hot tearing of cast metals,because the mechanical properties and,in fact,the structures in the melting range of cast and deformed materials are different.Fig.2b demonstrates the typical difference in plastic behaviour of cast and deformed alloys tested in the semi-solid state.Two factors are acting in the opposite directions:the lower amount of eutectics in deformed material decreases the elongation in the semi-solid state,whereas the finer grain structure in this material should increase its plasticity in the semi-solid state [11].Recently,Gleeble 1500and 3500thermo-mechanical simulators (testing ma-chines)were used for studying mechanical properties of aluminium alloys upon remelting in the semi-solid state [52].The significant advantage of Gleeble-series testing set-ups is the use of Joule heat for rapid melting the sample.In combination with modern means of strain–stress and temperature acquisition and control,this increases the accuracy and reliability of measured results and assures more complete retention of the as-cast structure to the beginning of the test.Spittle et al.[17]describe the testing set-up based on a Gleeble 1500thermo-mechanical simulator.The Gleeble controls and heating facilities are joined with a low force mechanical rig,including a Hounsfield H10K-C servo-mechanical vertical testing machine with a range of interchangeable load cells from 10kN down to 10N and a special software to maintain the sample under a specified,near-zeroload Fig.2.(a)Typical stress–strain curve obtained for an Al–6%Cu alloy upon testing at 570°C at a rate of 1mm/min and (b)interrelation of elongation ðd Þcurves for cast (1)and deformed (2)samples tested in the semi-solid state upon remelting [11].638 D.G.Eskin et al./Progress in Materials Science 49(2004)629–711。

大角度晶界的英语

大角度晶界的英语

大角度晶界的英语Abstract:Macroscopic grain boundaries (MGBs) are a critical feature in polycrystalline materials, significantly influencing mechanical properties, thermal conductivity, and electrical conductivity. This paper delves into the characteristics, formation mechanisms, and the impact of MGBs on the performance of materials, with a focus on their rolein various applications.1. IntroductionGrain boundaries are interfaces between two crystalline grains in a polycrystalline solid. When the misorientation between grains is significant, these boundaries can be considered macroscopic, exhibiting distinct properties that differ from those of the bulk material. The study of MGBs is essential for understanding material behavior and optimizing performance in engineering applications.2. Characteristics of Macroscopic Grain BoundariesMacroscopic grain boundaries are characterized by their misorientation angles, which are typically greater than 15 degrees. They can be classified into several types based on the crystallographic relationship between the grains they separate:- Twin boundaries: Where the misorientation is a mirror reflection across the boundary plane.- Coincidence site lattice (CSL) boundaries: Where a high density of lattice points from both grains coincide at the boundary.- General boundaries: With no specific crystallographic relationship, these are the most common type.3. Formation MechanismsMGBs can form during various material processing techniques:- Recrystallization: After severe deformation, grains can grow, leading to the formation of MGBs.- Grain growth: During annealing, larger grains can consume smaller ones, resulting in increased misorientations at the boundaries.- Phase transformations: Changes in crystal structure during phase transitions can create MGBs.4. Impact on Material PropertiesThe presence of MGBs has a profound effect on the properties of polycrystalline materials:- Strength: MGBs can impede dislocation motion, increasing the material's strength.- Ductility: They can act as sites for crack initiation, affecting ductility.- Conductivity: MGBs can scatter electrons and phonons, reducing thermal and electrical conductivity.5. ApplicationsUnderstanding MGBs is crucial for optimizing materials in various applications:- Metalworking: Controlling grain size and boundary characteristics can enhance the mechanical properties of metals.- Electronics: In semiconductor devices, MGBs can influence carrier mobility and device performance.- Ceramics: MGBs in ceramics can affect fracture toughness and thermal shock resistance.6. Experimental Techniques for Studying MGBsSeveral experimental methods are used to study MGBs:- Scanning electron microscopy (SEM): Can reveal the morphology of MGBs.- Transmission electron microscopy (TEM): Provides detailed information on the atomic structure of boundaries.- Electron backscatter diffraction (EBSD): Allows for the determination of grain orientation and the identification of MGBs.7. Computational ModelingComputational techniques, such as molecular dynamics and phase-field modeling, are used to simulate MGB formation and behavior:- Molecular Dynamics (MD): Offers insights into atomic-scale processes at MGBs.- Phase-Field Modeling: Can predict the evolution of grain structures and boundary characteristics during processing.8. ConclusionMacroscopic grain boundaries play a critical role in determining the properties of polycrystalline materials. Understanding their characteristics, formation, and impact is essential for the development of advanced materials with tailored properties for specific applications. Future research should focus on developing new techniques to control MGBs and on multiscale modeling to predict their effects on material behavior.References1. Hull, D., & Bacon, D. J. (2011). Introduction to Dislocations (5th ed.). Butterworth-Heinemann.2. Humphreys, F. J., & Hatherly, M. (2004). Recrystallization and Related Annealing Phenomena (2nd ed.). Elsevier.3. Gottstein, G. (2002). Physical Foundations ofMaterials Science. Springer.4. Randle, V. (2017). Grain Boundary CharacterDistribution and its Applications. CRC Press.This document provides a comprehensive overview of macroscopic grain boundaries, discussing theircharacteristics, formation, and impact on material properties, as well as the experimental and computational techniques used to study them. It concludes with the significance of MGBs in material applications and the importance of future researchin this area.。

具有高隔离度和任意功分比的平行带状功分器中英文对照翻译

具有高隔离度和任意功分比的平行带状功分器中英文对照翻译

A Parallel-Strip Ring Power Divider WithHigh Isolation and ArbitraryPower-Dividing RatioAbstract—In this paper, a new power divider concept, which provides high flexibility of transmission line characteristic impedance and port impedance, is proposed. This power divider is implemented on a parallel-strip line, which is a balanced transmission line. By implementing the advantages and uniqueness ofthe parallel-strip line, the divider outperforms the conventional divider in terms of isolation bandwidths. A swap structure of the two lines of the parallel-strip line is employed in this design, which is critical for the isolation enhancements. A lumped-circuit model of the parallel-strip swap including all parasitic effects has been analyzed. An equal power divider with center frequency of 2 GHz was designed to demonstrate the idea. The experimental results show that the equal power divider has 96.5%—10-dB impedance bandwidth with more than 25-dB isolation and less than 0.7-dB insertion loss. In order to generalize the concept with an arbitrary power ratio, we also realize unequal power dividers with the same isolation characteristics. The impedance bandwidth of the proposed power divider will increase with the dividing ratio, which is opposite to the conventional Wilkinson power divider. Unequal dividers with dividing ratios of 1 : 2 and 1 : 12 are designed and measured. Additionally, a frequency independent 1800 power divider has been realized with less than 20 phase errors.Index Terms—Arbitrary power-dividing ratio, parallel-strip line, ring structure, unequal power divider.I. INTRODUCTIONTHE WIKINSON power divider is one of the conventional and fundamental components in microwave engineering and exists in many microwave circuits. Both distributed and lumped Wilkinson power dividers have been applied in microwave integrated circuits and monolithic microwave integrated circuits [1]. Recently, extensive studies have been made to enhance the performances of the Wilkinson power divider, including size reductions by capacitive loading [2], folded circuitry [3] and resonating structure [4], [5], multiband operation [6], [7], unequal power dividing/combining [8], and active device [9] and waveguide implementations [10]. The power dividers discussed in this paper are focused on the isolation enhancement. The proposed divider is realized in the parallel-strip transmission line. Some parallel-strip circuits were reported with performance enhancement [11], [12]. The parallel-strip line provides more design flexibility than a micro-strip line, especially in realization of a high-impedance line and transitions.Many balanced circuits such as push–pull amplifiers, balanced mixers, frequency multipliers, and antenna arrays employ the Wilkinson power divider because of its simple design with high port-to-port isolation. Isolation is one of the important issuesin the design of the power divider and directional coupler. High isolation implies the minimization of unwanted coupling between active devices, as well as the elimination of unexpected distortions and oscillations. It is because it may provide a positivefeedback path for other frequencies, e.g., in Fig. 1, as unwanted oscillation at f1 may be set up outside of the operation frequency f0. Therefore, a wideband isolation operation is always preferred to suppress the coupling in other frequency bands.Fig. 1. Balanced circuit at frequency f0 and unwanted feedback at f1.The parallel-strip line belongs to a family of balanced transmission line. The conventional printed circuit board (PCB) fabrication technique is able to easily realize parallel-strip lines. It is a simple structure of a dielectric substrate sandwiched between two strip conductors. The signals flowing on the upper and lower strip conductors are always equal in magnitude and 1800out-of-phase. The quasi-TEM mode electric and magnetic fields distributions are closed to the micro-strip line. In this paper, a parallel-strip swap is employed to enhance isolation performance of the power divider. The swap is a passive microwave component. It forms a compact realization of 1800 phase shift by interchanging the connection of two conductors in the balanced transmission line. Various swaps were proposed for performance enhancement in a 1800 hybrid coupler [13]–[15].A new equal power divider, which is realized on a parallel-strip line with a ring-like structure, was first demonstrated in [16]. The four arms and two shunt resistors in the divider provide a high degree of freedom for choosing the circuit parameters. In this paper, the proposed concept is generalized to be arbitrary power dividing without an increase in design complexity. It shows a frequency-independent isolation characteristic, arbitrary power-dividing ratio without an external matching network, avoidance of a very thin strip line for achieving high characteristic impedance, and ease of realizing wideband 1800 dividing. While the conventional Wilkinson powerdivider exhibits limited isolation bandwidth, unequal Wilkinson power dividing relies on an external quarter-wave transformer for realizing unequal power dividing for the same port impedances.High characteristics impedance transmission lines are required for the unequal power divider. The unequal divider has been used with strict restrictions in design and fabrication because it requires a transmission line with very high impedance [8]. On the other hand, the very thin transmission line limits the power handling of the devices. To overcome this limitation in realizing characteristic impedance, the upper and lower strip lines of the parallel-strip line are offset so that it will be easier to highly increase the characteristic impedance. Three power dividers with power-dividing ratios of 1 : 1, 1 : 2, and 1 : 12 were designed, fabricated, and tested.Fig. 2. Schematic diagram of proposed power divider with four arms, a swap, and two shunt resistors.II. THEORETICAL ANALYSISThe structure of the proposed divider is illustrated in Fig. 2.In [13], the equal power divider has been analyzed using even and odd-mode analysis because of symmetry of the divider. For the same reason, the circuit parameters, such as port impedance and line impedances, should be the same as their corresponding parameters Z A=Z C, Z B=Z D, and Z2=Z3. In this paper, we try to generalize the analysis to an unequal power divider with an arbitrary dividing ratio.It consists of an 1800 swap, four quarter-wave-long arms (with characteristic impedances Z A, Z B, Z C, and Z D) and two shunt resistors with resistance . These five parameters determine the input impedances, isolation, and dividing ratio of the divider. In order to determine the arm characteristic impedances and resistor values, several parameters should be known, including port impedances Z1, Z2, and Z3 and power ratio K.Firstly, the impedance matching is considered. To achieve maximum power transfer, all the ports should be matched. The input impedance at port 1 is determined by Z A and Z C and port impedances Z2 and Z3.As illustrated in Fig. 3, it is assumed thata signal is injected to port 1 and will only pass through ports 2 and 3. There is no net current flowing from ports 2 to 3 due to port isolation between ports in the shaded region. Arms B and D with characteristic impedances Z B and Z D , respectively, the two shunt resistors, and the swap can thus be replaced by an open circuit in analysis. The two arms are connected in shunt; the input impedance at port 1 can be expressed as(1)The signal injected to port 2 can be divided into two parts, one flowing to port 1 and the other being absorbed by shunt resistors as shown in Fig. 4. Obviously, there is no net current flowing from arm to arm and port 3 in the shaded region, which can be replaced by an open circuit in analysis. The input impedance at port 2 can be given as(2)Similarly, the input impedance at port 3 can be expressed as(3)For the unequal power dividing and assuming the power ratio of ports 2 and 3 to be K, the power ratio can be determined by the ratio of input impedance of the arms A and C, as shown in Fig. 3, as follows:(4)123221)(-+=C A Z Z Z Z Z 12212)2(-+=B A Z R Z Z Z 12213)2(-+=D C Z R Z Z Z 32222232Z Z Z Z Z Z Z Z k A C A C ==By solving (1), (2), and (4), Z A and Z C are determined and are expressed in (5) and(6), respectively.Solving (4) and (1),(5)Solving (4) and (2),(6)Hence, the ratio of the square of Z B and Z D and shunt resistor can be determined by solving (2), (3), (5), and (6).Solving (5) and (2),(7)Solving (6) and (3),(8)There are four conditions, but five unknown parameters Z A , Z B, Z C , Z D , and R. Therefore, the solutions are singular, which implies there is no unique solution. The 31)1(Z Z k Z C +=21)11(Z Z k Z A +=)11(232kZ R Z D +=)1(222k Z R Z B +=infinite number of solutions provide a high degree of freedom when the divider is designed. For example, the divider can not only be designed for any port impedance without external matching circuits, but also provides unequal power dividing with equal port impedance.Isolation is a very important design issue. The symmetrical structure and the swap provide the possibility of frequency-independent isolation characteristics. Signals flowing through paths A –C and B –D should be equal in magnitude, but 1800 out-of -phase. In order to provide frequency-independent isolation, the phase difference between paths A –C and B –D should be frequency independent at 1800 out-of-phase and with equal amplitude, which is provided by the swap, and the characteristic impedance should be the sameZ A = Z D and Z B = Z C (9)Equation (9) represents the fifth condition for designing a divider with frequency-independent isolation and arbitrary power ratio. After combining the previous conditions, the parameters Z A , Z B, Z C , Z D , and R become unique. The design formulas can be summarized asR=2Z1 (10a)(10b)(10c)31)1(Z Z k Z Z C B +==21)11(Z Z k Z Z D A +==Fig. 5. Geometries of parallel-strip swap and parallel-strip line with equal physical length.III. PARALLEL SWAP AND DISCONTINUITYThe swap is the interchange between the two signal lines in the balance transmission line so that the signal is said to be ―reversed,‖ therefore, it provides 1800 phase shift without the existence of a delay line. It can be easily realized in some of the nonmicrostrip transmission lines such as a coplanar waveguide, coplanar strip line, and parallel-strip line. Fig. 5 shows the geometry of the parallel-strip swap. The upper and lower strip lines are connected by two vertical metical vias. The sections of the swap and parallel-strip line are simulated using Ansoft’s High Frequency Structure Simulator (HFSS). Within the entire simulation band, less than 0.5-dB extra insertion loss is introduced and 1800 phase shift is provided with less than 2 phase error, as shown in Fig. 6. The swap introduces discontinuity for the divider and always degrades the circuit performance. It is necessary to develop proper analysis models. The structure of parallel- strip swap with two shunt resistors used in the proposed divider is shown in Fig. 7. Two resistors are soldered across the two gaps at the upper and lower strip lines. These resistors are used to absorb the signal. They are necessary to provide proper impedance matching and port-to-port isolation, similar to the resistor in the Wilkinson power divider.Extra insertion loss and phase delay are introduced by the vertical via, which can be analyzed by a lumped-circuit model. The lump-circuit model of the swap with two shunt resistors (R S) is illustrated in Fig. 8. The parasitic capacitance (C S) is used to model the edge couplings between strips with different layers. The parasitic capacitance (C C) is used to model the total effect due to edge couplings between strips with the same layers and coupling between the vias. The parasitic inductance (L V) and resistance (R V) are introduced by vertical conductor in via-holes and soldering. Theparasitic components can be extracted from full-wave simulations so that the lumped model of the swap was done.The Z-parameter of the lumped equivalent model of the core in Fig. 8 is given by(11)Fig. 6. Simulated frequency responses of insertion loss and phase difference of a section of parallel-strip swap and line with same physical length.⎪⎪⎭⎫ ⎝⎛+--+=⎪⎪⎭⎫ ⎝⎛212121212221121121Z Z Z Z Z Z Z Z Z Z Z ZFig. 7. 3-D view of parallel-strip swap with two shunt resistors.Fig. 8. Lump equivalent model of parallel-strip line swap.where Z 1= R V + jwL V and Z 2= (1/ R S +1/jwC C )-1 Hence, the S-parameter converted from Z-parameters of the core is determined as follows:(12)(13) ))((020*********Z Z Z Z Z Z Z S S +++==))(()(020********Z Z Z Z Z Z Z S S ++-==The structure shown in Fig. 7 is simulated by the full-wave electromagnetic (EM) simulator HFSS, determining the optimum design of the vias on the substrate dielectric constant of 2.65 and thickness of 1.5 mm where all the gapwidthsFig. 9. Simulated S-parameters of the parallel-strip line swap using lumped model and full-wave EM simulation. (a) Magnitude response. (b) Phase response.are 0.2 mm and the radius of the metallic via is 0.55 mm. Deembedding of the parameters has been performed by utilizing the microwave circuit simulator, Agilent Technologies’s Advanced Design System (ADS). Both EM and circuit simulationsof the parallel-strip swaps with 70.71- terminations are shown in Fig. 9. Good agreement of both the magnitudes and phases responses are achieved within the frequency band of interest. The values of parasitic elements are L V =2.181 nH,C S=0.2939 pF, C C=0.3878 pF, and R V =0.2624Ω. The model circuit is analyzed and, hence, the scattering matrix representing the parallel-strip swap with shunt resistor (R S) is, therefore, obtained, and the entire circuit can thus be easily modeled in the circuit simulation.IV. RESULTS OF SIMULATION AND EXPERIMENTA. Equal Power DividerThe power dividers are fabricated in a conventional printed circuit technique and the dividers designed for demonstration are built on a substrate with a dielectric constant of 2.65 and a thickness of 1.5 mm, as shown in Fig. 10. The derivation in Section II is based on an ideal transmission line model. This analysis provides initial design parameters. Discontinuities or parasitic elements such as T-junctions and steps will be introduced. EM optimization is required to determine all circuit parameters with the best performance.Fig. 10. Implementation of proposed equal power divider on PCB. (a) Upper layer. (b) Bottom layer. are built on a substrate with a dielectric constant of 2.65 and a thickness of 1.5 mm, as shown in Fig. 10. The derivation in Section II is based on an ideal transmission line model. This analysis provides initial design parameters. Discontinuities or parasiticelements such as T-junctions and steps will be introduced. EM optimization isrequired to determine all circuit parameters with the best performance.All the port impedances are designed at 50 , i.e., Z1=Z2=Z3=50Ω The designparameters of an equal power divider are Z A=Z B=Z C= Z D = 70.71Ωand R=100Ω.By removing portion of the ground of a micro-strip line, the parabolic tapered transition between the parallel-strip line and micro-strip line [11] was employed for connecting the coaxial connector for measurement purposes with less than 0.1-dB insertion loss within the entire tested frequency band. However, an approximate 0.5-dB extra insertion loss will be introduced if a subminiature A (SMA) connector is directly connected to the SMA connector. Fig. 11 shows both simulated and measured results of the equal power divider. The EM simulation tool is Ansoft’s HFSS. The measured insertion loss from ports 1 to 2 and 3 are less than 3.7 dB within the operation frequency band, as shown in Fig. 11(a). Some mismatches come from an inaccurate prediction of the vertical structure from the EM simulator and soldering. The mismatches in return losses shown in Fig. 11(b) are due to unexpected errors from soldering between the divider and SMA connectors. The ring-like structure implies similar input and output impedance characteristics, as shown in Fig. 10. The total usable impedance bandwidth is wider than that of the conventional Wilkinson power divider. Due to the imbalances of the two paths, e.g., electrical delay and insertion loss in the swap, the isolation has a finite value. Fortunately, the isolation can still provide great improvement over the conventional divider.The impedance bandwidths of return loss lower than 10 dB of the proposed divider is measured at 96.5%, as observed in Fig. 11(b). In Fig. 11(c), the proposed divider demonstrates more than 25 dB in the entire frequency band in the measurement, while a conventional Wilkinson power divider shows approximately 33% isolation bandwidth of more than 20-dB isolation. Good agreement between experimental and simulated results can be observed.B. Unequal Power DividersApart from the equal power divider, two unequal power dividers with ratios of 1 : 2 and 1 : 12 are realized. The impedance bandwidth is usually reduced with the dividing ratio in the conventional Wilkinson power divider; however, the bandwidth of the proposed divider is increased with a power ratio of . The relation is shown in Fig. 12. Figs. 13 and 14 show the frequency responses of -parameters and the dividing ratio of the 1 : 2 power divider. The design parameters are Z A=Z D=61.24Ω, ZB=ZC= 86.61Ω, and R=100Ω. Measured results agree withEMsimulation.Within the 125% operation bandwidth with lower than 10-dB return loss, more than 26-dB port-to-port isolation is achieved and the average divider ratio is approximately 2.07.Fig. 11. Simulated and measured results of proposed equal power divider.(a) Insertion losses. (b) Return losses. (c) Isolation.A high dividing ratio implies the existence of some high characteristicimpedance transmission lines. The implementation ofhigh characteristic impedance remains challenge because of theFig. 15. Cross section and 3-D view of offset parallel-strip line.Fig. 16. Relationship of characteristics impedance and normalized offset distance with different normalized strip width, where z denotes characteristics impedance, w denotes width of the strip line, d denotes offset distance, and h denotes substrate thickness.technique of extremely thin micro-strip line fabrication. The realization of the unequal power divider may be limited by fabrication of the thin strip line and low power-handling capacity of the divider.In order to easily realize a high-impedance transmission line, a micro-strip defected ground structure was proposed for the 1 : 4 unequal divider [8]. In [17], thecharacteristics impedance parallel- strip line was increased by offsetting the upper and lower strip lines in the finite ground micro-strip line for stopband enhancement. Similarly, the characteristics impedance of a parallel-strip line can be increased by offsetting the strip lines, as shown in Fig. 15. Fig. 16 shows the relationship between characteristics impedances and normalized circuit parameters on the same substrate. It is obvious that the characteristics impedance (z) increases with offset distance (d) without use of very narrow strip lines. A high characteristic impedance parallel-strip line can be realized by offsetting the upper and lower strip lines andit does not need a very narrow line.In the 1 : 12 power divider, two arms with high characteristic impedance are realized by offsetting the parallel-strip line. Figs. 17 and 18 show its -parameters and the dividing ratio varied with frequency. The design parameters are Z A=Z D=50.04Ω, Z B=Z D=180.27Ω, and R=100Ω. Good agreement of both simulated and measured results are obtained. Within the 150% operation bandwidth with lower than 10-dBreturn loss, more than 24-dB port-to-port isolation is achieved and the average divider ratio is approximately 12.68.Fig. 17. Simulated and measured S-parameters of 1 : 12 proposed divider.Fig. 18. Simulated and measured dividing ratio of 1 : 12 proposed divider.C. Frequency-Independent 180 Power DividerConventionally, the symmetric power divider is used for in-phase powerdividing/combining. A power divider with wideband 1800 out-of-phase operation is needed for many balanced circuit such as a push–pull amplifier and balanced mixer. The 1800 hybrid or the power divider with a 1800 delay line is used for such purpose.A 1800 divider can be easily realized by adding an extra section of delay line. However, a delay line limits the bandwidth of phase balances. The conventional 1800 hybrid coupler or Wilkinson power divider with a delay line may not fulfill actual application demands and may degrade system performance. With a similar approach to [12], the frequency-independent 1800 differential phase between ports 2 and 3 is realized by tapering the lower line in port 2 and the upper line in port 3, the parallel-strip line-to-micro-strip line transition, which is used for measurement, is formed as shownin Fig. 19. All circuit parameters are the same as the equal power divider in Section IV. The magnitudes of simulated and measured -parameters are close to that of the equal power divider, as shown in Fig. 11. A frequency-independent 1800 phase difference is observed, as shown in Fig. 20. A small phase error within 2 is introduced due to the thickness of the substrate of the PCB, while it can be minimized by using a thinner substrate with a lower dielectric constant. Similarly, the 1800 unequal power divider with an arbitrary dividing ratio can be realized via the same technique.Fig. 19. Implementation of proposed 1800 equal power divider on PCB. (a) Upper layer. (b) Bottom layer.Fig. 20. Phase response of 1800 equal power divider.V. CONCLUSIONA novel power divider with better isolation than the conventional Wilkinson power divider has been presented. Design formulas for the proposed divider have been proven analytically. The ring-like structure provides design flexibility such as unequal power dividing without extra impedance matching networks. The equal and unequal power dividers were designed and tested with out-performed isolation characteristics. Additionally, a 1800 equal power divider was realized by making use of the balanced structure of the parallel-strip line. Similarly, a 1800unequal power divider can be designed. The proposed design leads to realization of a new geometrical configuration for a high-performance power-divider concept.R EFERENCES[1] L. H. Lu, P. Bhattacharya, L. P. B. Katehi, and G. E. Ponchak, ―X-band and K-band lumped Wilkinson power dividers with a micromachined technology,‖ in IEEE MTT-S Int. Microw. Symp. Dig., 2000, pp. 287–290.[2] K. Hettak, G. A. Morin, and M. G. Stubbs, ―Compact MMIC CPW and asymmetric CPS branch-line couplers and Wilkinson dividers using shunt and seri es stub loading,‖ IEEE Trans. Microw. Theory Tech., vol. 53, no. 5, pp. 1624–1635, May 2005.[3] L. Chiu, T. Y. Yum, Q. Xue, and C. H. Chan, ―The folded hybrid ring and its applications in balance devices,‖ in IEEE Eur. Microw. Conf., 2005, pp. 1–4.[4] K. M. Shum, Q. Xue, and C. H. Chan, ―Curved PBG cell and its applications,‖in Asia–Pacific Microw. Conf., 2001, pp. 767–770.[5] D. J. Woo and T. K. Lee, ―Suppression of harmonics in Wilkinson power divider using dual-band rejection by asymmetric DGS,‖ IEEE Trans. Microw. Theory Tech., vol. 53, no. 6, pp. 2139–2144, Jun. 2005.[6] L. Wu, Z. Sun, H. Yilmaz, and M. Berroth, ―A dual-frequency Wilkinson power divider,‖ IEEE Trans. Microw. Theory Tech., vol. 54, no. 1, pp. 278–284, Jan. 2006.[7] M. Chongcheawchamnan, S. Patisang, M. Krairiksh, and I. D. Robertson, ―Tri-band Wilkinson power divider using a three-section transmission-line transformer,‖ IEEE Microw. Wireless Compon. Lett.,to be published.[8] J. S. Lim, S. W. Lee, C. S. Kim, J. S. Park, D. Ahn, and S. W. Nam, ―A 4 : 1 unequal Wilkinson power divider,‖ IEEE Microw. Wireless Compon. Lett., vol. 11, no. 3, pp. 124–126, Mar. 2001.[9] L. H. Lu, Y. T. Liao, and C. R. Wu, ―A miniaturized Wilkinson power divider withCMOSactive inductors,‖ IEEE Microw.Wireless Compon. Lett., vol. 15, no. 11, pp. 775–777, Nov. 2005.[10] X. Xu, R. G. Bosisio, and K. Wu, ―A new six-port junction based on substrate integrated waveguide technology,‖ IEEE Trans. Microw. Theory Tech., vol. 53, no. 7, pp. 2267–2273, Jul. 2006.[11] S. G. Kim and K. Chang, ―Ultrawide-band transitions and new microwave components using double-sided parallel-strip lines,‖ IEEE Trans. Microw. Theory Tech., vol. 52, no. 9, pp. 2148–2152, Sep. 2004.[12] L. Chiu, T. Y. Yum, Q. Xue, and C. H. Chan, ―A wide band compact parallel-strip 180_ Wilkinson power divider for push-pull circuitries,‖ IEEE Microw. Wireless Compon. Lett., vol. 16, no. 1, pp. 49–51, Jan. 2006.[13] C. W. Kao and C. H. Chen, ―Novel uniplanar 180 hybrid-ring couplers with spiral-type phase inverters,‖ IEEE Microw. Guided Wave Lett., vol. 10, no. 10, pp. 412–414, Oct. 2000.[14] B. R. Heimer, L. Fan, and K. Chang, ―Uniplanar hybrid couplers using asymmetrical coplanar striplines,‖ IEEE Trans. Microw. Theory Tech., vol. 45, no. 12, pp. 2234–2240, Dec. 1997.[15] T. Q. Wang and K. Wu, ―Size-reduction and band-broadening design technique of uniplanar hybrid ring coupler using phase inverter for M(H)MIC’s,‖ IEEE Trans. Microw. Theory Tech., vol. 47, no. 2, pp.198–206, Feb. 1999.[16] L. Chiu and Q. Xue, ―A new parallel-strip power divider with enhanced isolation performance,‖ in Proc. Asia–Pacific Microw. Conf., Dec. 2006, pp. 411–416.[17] S. Sun and L. Zhu, ―Stopband-enhanced and size-miniaturized lowpass filters using high-impedance property of offset finite-ground microstrip line,‖ IEEE Trans. Microw. Theory Tech., vol. 53, no. 9, pp.2844–2850, Sep. 2005.具有高隔离度和任意功分比的平行带状功分器摘要:在这篇文章中,提出了一种新型的功率分配器概念,并提及传输线特性阻抗和端口阻抗的高弹性。

EDTA辅助水热法合成硫化铋晶体

EDTA辅助水热法合成硫化铋晶体

EDTA辅助水热法合成硫化铋晶体沈林;殷俊霞;汪朝晖;汪效祖【摘要】以Bi( NO3)3·5H2O和Na2S2O3·5H2O为原料,用乙二胺四乙酸(EDTA)辅助水热法合成了纳米或微米级的Bi2S3晶体(1),其结构、形貌和光谱性能经XRD,FE-SEM和UV-Vis表征.结果表明:溶液的pH对1的形貌有显著的影响,随着pH的增大,1由纳米棒组成的微米球逐渐转变为微米级片状结构;1出现蓝移.%Nano- or micro-scaled Bi2S3 crystals(l) were synthesized byEDTA(ethylenediamine tet-ra-acetic acid)-assisted hydrothermal method from Bi(NO3)3 ? 5H2O and Na2S2O3 ? 5H2O. The structure, topography and spectrum property of 1 were characterized by XRD, FE-SEM and UV-Vis. The results showed that the pH value of solution played a key role in the formation of 1 topography, the micro-spheres composed of nanorods transform into micro-plate structures as pH value increasing. 1 shows blue shift.【期刊名称】《合成化学》【年(卷),期】2012(020)002【总页数】4页(P231-234)【关键词】硫化铋晶体;乙二胺四乙酸;纳米材料;水热合成【作者】沈林;殷俊霞;汪朝晖;汪效祖【作者单位】南京工业大学材料化学工程国家重点实验室,江苏南京210009;南京工业大学材料化学工程国家重点实验室,江苏南京210009;南京工业大学材料化学工程国家重点实验室,江苏南京210009;南京工业大学材料化学工程国家重点实验室,江苏南京210009【正文语种】中文【中图分类】O614.53;O753硫属半导体材料,由于独特的物理化学性质和潜在应用价值引起了人们的广泛关注。

弹性力学专业英语英汉互译词汇

弹性力学专业英语英汉互译词汇

弹性力学elasticity弹性理论theory of elasticity均匀应力状态homogeneous state of stress 应力不变量stress invariant应变不变量strain invariant应变椭球strain ellipsoid均匀应变状态homogeneous state ofstrain 应变协调方程equation of straincompatibility 拉梅常量Lame constants各向同性弹性isotropic elasticity旋转圆盘rotating circular disk 楔wedge开尔文问题Kelvin problem 布西内斯克问题Boussinesq problem艾里应力函数Airy stress function克罗索夫--穆斯赫利什维Kolosoff-利法Muskhelishvili method 基尔霍夫假设Kirchhoff hypothesis 板Plate矩形板Rectangular plate圆板Circular plate环板Annular plate波纹板Corrugated plate加劲板Stiffened plate,reinforcedPlate 中厚板Plate of moderate thickness 弯[曲]应力函数Stress function of bending 壳Shell扁壳Shallow shell旋转壳Revolutionary shell球壳Spherical shell [圆]柱壳Cylindrical shell 锥壳Conical shell环壳Toroidal shell封闭壳Closed shell波纹壳Corrugated shell扭[转]应力函数Stress function of torsion 翘曲函数Warping function半逆解法semi-inverse method瑞利--里茨法Rayleigh-Ritz method 松弛法Relaxation method莱维法Levy method松弛Relaxation 量纲分析Dimensional analysis 自相似[性] self-similarity影响面Influence surface接触应力Contact stress赫兹理论Hertz theory协调接触Conforming contact滑动接触Sliding contact滚动接触Rolling contact压入Indentation各向异性弹性Anisotropic elasticity颗粒材料Granular material散体力学Mechanics of granular media 热弹性Thermoelasticity超弹性Hyperelasticity粘弹性Viscoelasticity对应原理Correspondence principle 褶皱Wrinkle塑性全量理论Total theory of plasticity 滑动Sliding微滑Microslip粗糙度Roughness非线性弹性Nonlinear elasticity大挠度Large deflection突弹跳变snap-through有限变形Finite deformation格林应变Green strain阿尔曼西应变Almansi strain弹性动力学Dynamic elasticity运动方程Equation of motion准静态的Quasi-static气动弹性Aeroelasticity水弹性Hydroelasticity颤振Flutter弹性波Elastic wave简单波Simple wave柱面波Cylindrical wave水平剪切波Horizontal shear wave竖直剪切波Vertical shear wave 体波body wave无旋波Irrotational wave畸变波Distortion wave膨胀波Dilatation wave瑞利波Rayleigh wave等容波Equivoluminal wave勒夫波Love wave界面波Interfacial wave边缘效应edge effect塑性力学Plasticity可成形性Formability金属成形Metal forming耐撞性Crashworthiness结构抗撞毁性Structural crashworthiness 拉拔Drawing破坏机构Collapse mechanism 回弹Springback挤压Extrusion冲压Stamping穿透Perforation层裂Spalling塑性理论Theory of plasticity安定[性]理论Shake-down theory运动安定定理kinematic shake-down theorem静力安定定理Static shake-down theorem 率相关理论rate dependent theorem 载荷因子load factor加载准则Loading criterion加载函数Loading function加载面Loading surface塑性加载Plastic loading塑性加载波Plastic loading wave简单加载Simple loading比例加载Proportional loading 卸载Unloading卸载波Unloading wave冲击载荷Impulsive load阶跃载荷step load脉冲载荷pulse load极限载荷limit load中性变载nentral loading拉抻失稳instability in tension 加速度波acceleration wave本构方程constitutive equation 完全解complete solution名义应力nominal stress过应力over-stress真应力true stress等效应力equivalent stress流动应力flow stress应力间断stress discontinuity应力空间stress space主应力空间principal stress space静水应力状态hydrostatic state of stress 对数应变logarithmic strain工程应变engineering strain等效应变equivalent strain应变局部化strain localization应变率strain rate应变率敏感性strain rate sensitivity 应变空间strain space有限应变finite strain塑性应变增量plastic strain increment 累积塑性应变accumulated plastic strain 永久变形permanent deformation内变量internal variable应变软化strain-softening理想刚塑性材料rigid-perfectly plasticMaterial 刚塑性材料rigid-plastic material理想塑性材料perfectl plastic material 材料稳定性stability of material 应变偏张量deviatoric tensor of strain 应力偏张量deviatori tensor of stress 应变球张量spherical tensor of strain 应力球张量spherical tensor of stress 路径相关性path-dependency线性强化linear strain-hardening应变强化strain-hardening随动强化kinematic hardening各向同性强化isotropic hardening强化模量strain-hardening modulus幂强化power hardening 塑性极限弯矩plastic limit bendingMoment 塑性极限扭矩plastic limit torque弹塑性弯曲elastic-plastic bending 弹塑性交界面elastic-plastic interface 弹塑性扭转elastic-plastic torsion粘塑性Viscoplasticity非弹性Inelasticity理想弹塑性材料elastic-perfectly plasticMaterial 极限分析limit analysis极限设计limit design极限面limit surface上限定理upper bound theorem上屈服点upper yield point下限定理lower bound theorem下屈服点lower yield point界限定理bound theorem初始屈服面initial yield surface后继屈服面subsequent yield surface屈服面[的]外凸性convexity of yield surface 截面形状因子shape factor of cross-section沙堆比拟sand heap analogy 屈服Yield 屈服条件yield condition屈服准则yield criterion屈服函数yield function屈服面yield surface塑性势plastic potential 能量吸收装置energy absorbing device 能量耗散率energy absorbing device 塑性动力学dynamic plasticity 塑性动力屈曲dynamic plastic buckling 塑性动力响应dynamic plastic response 塑性波plastic wave运动容许场kinematically admissibleField 静力容许场statically admissibleField 流动法则flow rule速度间断velocity discontinuity滑移线slip-lines滑移线场slip-lines field移行塑性铰travelling plastic hinge 塑性增量理论incremental theory ofPlasticity米泽斯屈服准则Mises yield criterion 普朗特--罗伊斯关系prandtl- Reuss relation 特雷斯卡屈服准则Tresca yield criterion洛德应力参数Lode stress parameter莱维--米泽斯关系Levy-Mises relation亨基应力方程Hencky stress equation赫艾--韦斯特加德应力空Haigh-Westergaard 间stress space洛德应变参数Lode strain parameter德鲁克公设Drucker postulate盖林格速度方程Geiringer velocityEquation结构力学structural mechanics结构分析structural analysis结构动力学structural dynamics拱Arch三铰拱three-hinged arch抛物线拱parabolic arch圆拱circular arch穹顶Dome空间结构space structure空间桁架space truss雪载[荷] snow load风载[荷] wind load土压力earth pressure地震载荷earthquake loading弹簧支座spring support支座位移support displacement支座沉降support settlement超静定次数degree of indeterminacy机动分析kinematic analysis结点法method of joints截面法method of sections结点力joint forces共轭位移conjugate displacement影响线influence line三弯矩方程three-moment equation单位虚力unit virtual force刚度系数stiffness coefficient柔度系数flexibility coefficient力矩分配moment distribution力矩分配法moment distribution method 力矩再分配moment redistribution分配系数distribution factor矩阵位移法matri displacement method 单元刚度矩阵element stiffness matrix 单元应变矩阵element strain matrix总体坐标global coordinates贝蒂定理Betti theorem高斯--若尔当消去法Gauss-Jordan eliminationMethod 屈曲模态buckling mode复合材料力学mechanics of composites复合材料composite material 纤维复合材料fibrous composite单向复合材料unidirectional composite泡沫复合材料foamed composite颗粒复合材料particulate composite 层板Laminate夹层板sandwich panel正交层板cross-ply laminate斜交层板angle-ply laminate 层片Ply多胞固体cellular solid 膨胀Expansion压实Debulk劣化Degradation脱层Delamination脱粘Debond纤维应力fiber stress层应力ply stress层应变ply strain层间应力interlaminar stress比强度specific strength强度折减系数strength reduction factor 强度应力比strength -stress ratio 横向剪切模量transverse shear modulus 横观各向同性transverse isotropy正交各向异Orthotropy剪滞分析shear lag analysis短纤维chopped fiber长纤维continuous fiber纤维方向fiber direction纤维断裂fiber break纤维拔脱fiber pull-out纤维增强fiber reinforcement致密化Densification最小重量设计optimum weight design 网格分析法netting analysis混合律rule of mixture失效准则failure criterion蔡--吴失效准则Tsai-W u failure criterion 达格代尔模型Dugdale model断裂力学fracture mechanics概率断裂力学probabilistic fractureMechanics格里菲思理论Griffith theory线弹性断裂力学linear elastic fracturemechanics, LEFM弹塑性断裂力学elastic-plastic fracturemecha-nics, EPFM 断裂Fracture 脆性断裂brittle fracture解理断裂cleavage fracture蠕变断裂creep fracture延性断裂ductile fracture晶间断裂inter-granular fracture 准解理断裂quasi-cleavage fracture 穿晶断裂trans-granular fracture 裂纹Crack裂缝Flaw缺陷Defect割缝Slit微裂纹Microcrack折裂Kink椭圆裂纹elliptical crack深埋裂纹embedded crack[钱]币状裂纹penny-shape crack预制裂纹Precrack短裂纹short crack表面裂纹surface crack裂纹钝化crack blunting裂纹分叉crack branching裂纹闭合crack closure裂纹前缘crack front裂纹嘴crack mouth裂纹张开角crack opening angle,COA 裂纹张开位移crack opening displacement,COD裂纹阻力crack resistance裂纹面crack surface裂纹尖端crack tip裂尖张角crack tip opening angle,CTOA裂尖张开位移crack tip openingdisplacement, CTOD裂尖奇异场crack tip singularityField裂纹扩展速率crack growth rate稳定裂纹扩展stable crack growth定常裂纹扩展steady crack growth亚临界裂纹扩展subcritical crack growth 裂纹[扩展]减速crack retardation 止裂crack arrest 止裂韧度arrest toughness断裂类型fracture mode滑开型sliding mode张开型opening mode撕开型tearing mode复合型mixed mode撕裂Tearing 撕裂模量tearing modulus断裂准则fracture criterionJ积分J-integralJ阻力曲线J-resistance curve断裂韧度fracture toughness应力强度因子stress intensity factor HRR场Hutchinson-Rice-RosengrenField 守恒积分conservation integral 有效应力张量effective stress tensor 应变能密度strain energy density 能量释放率energy release rate内聚区cohesive zone塑性区plastic zone张拉区stretched zone热影响区heat affected zone, HAZ 延脆转变温度brittle-ductile transitiontempe- rature 剪切带shear band剪切唇shear lip无损检测non-destructive inspection 双边缺口试件double edge notchedspecimen, DEN specimen 单边缺口试件single edge notchedspecimen, SEN specimen 三点弯曲试件three point bendingspecimen, TPB specimen 中心裂纹拉伸试件center cracked tensionspecimen, CCT specimen 中心裂纹板试件center cracked panelspecimen, CCP specimen 紧凑拉伸试件compact tension specimen,CT specimen 大范围屈服large scale yielding 小范围攻屈服small scale yielding 韦布尔分布Weibull distribution 帕里斯公式paris formula空穴化Cavitation应力腐蚀stress corrosion概率风险判定probabilistic riskassessment, PRA 损伤力学damage mechanics 损伤Damage连续介质损伤力学continuum damage mechanics 细观损伤力学microscopic damage mechanics 累积损伤accumulated damage脆性损伤brittle damage延性损伤ductile damage宏观损伤macroscopic damage细观损伤microscopic damage微观损伤microscopic damage损伤准则damage criterion损伤演化方程damage evolution equation 损伤软化damage softening损伤强化damage strengthening损伤张量damage tensor损伤阈值damage threshold损伤变量damage variable损伤矢量damage vector损伤区damage zone疲劳Fatigue 低周疲劳low cycle fatigue应力疲劳stress fatigue随机疲劳random fatigue蠕变疲劳creep fatigue腐蚀疲劳corrosion fatigue疲劳损伤fatigue damage疲劳失效fatigue failure疲劳断裂fatigue fracture 疲劳裂纹fatigue crack疲劳寿命fatigue life疲劳破坏fatigue rupture疲劳强度fatigue strength 疲劳辉纹fatigue striations 疲劳阈值fatigue threshold 交变载荷alternating load 交变应力alternating stress 应力幅值stress amplitude 应变疲劳strain fatigue应力循环stress cycle应力比stress ratio安全寿命safe life过载效应overloading effect 循环硬化cyclic hardening 循环软化cyclic softening 环境效应environmental effect 裂纹片crack gage裂纹扩展crack growth, crackPropagation裂纹萌生crack initiation 循环比cycle ratio实验应力分析experimental stressAnalysis工作[应变]片active[strain] gage基底材料backing material应力计stress gage零[点]飘移zero shift, zero drift 应变测量strain measurement应变计strain gage应变指示器strain indicator应变花strain rosette应变灵敏度strain sensitivity 机械式应变仪mechanical strain gage 直角应变花rectangular rosette引伸仪Extensometer应变遥测telemetering of strain 横向灵敏系数transverse gage factor 横向灵敏度transverse sensitivity 焊接式应变计weldable strain gage 平衡电桥balanced bridge粘贴式应变计bonded strain gage粘贴箔式应变计bonded foiled gage粘贴丝式应变计bonded wire gage 桥路平衡bridge balancing电容应变计capacitance strain gage 补偿片compensation technique 补偿技术compensation technique 基准电桥reference bridge电阻应变计resistance strain gage 温度自补偿应变计self-temperaturecompensating gage半导体应变计semiconductor strainGage 集流器slip ring应变放大镜strain amplifier疲劳寿命计fatigue life gage电感应变计inductance [strain] gage 光[测]力学Photomechanics光弹性Photoelasticity光塑性Photoplasticity杨氏条纹Young fringe双折射效应birefrigent effect等位移线contour of equalDisplacement 暗条纹dark fringe条纹倍增fringe multiplication 干涉条纹interference fringe 等差线Isochromatic等倾线Isoclinic等和线isopachic应力光学定律stress- optic law主应力迹线Isostatic亮条纹light fringe光程差optical path difference 热光弹性photo-thermo -elasticity 光弹性贴片法photoelastic coatingMethod光弹性夹片法photoelastic sandwichMethod动态光弹性dynamic photo-elasticity 空间滤波spatial filtering空间频率spatial frequency起偏镜Polarizer反射式光弹性仪reflection polariscope残余双折射效应residual birefringentEffect 应变条纹值strain fringe value应变光学灵敏度strain-optic sensitivity 应力冻结效应stress freezing effect 应力条纹值stress fringe value应力光图stress-optic pattern暂时双折射效应temporary birefringentEffect 脉冲全息法pulsed holography透射式光弹性仪transmission polariscope 实时全息干涉法real-time holographicinterfero - metry 网格法grid method全息光弹性法holo-photoelasticity 全息图Hologram全息照相Holograph全息干涉法holographic interferometry 全息云纹法holographic moire technique 全息术Holography全场分析法whole-field analysis散斑干涉法speckle interferometry 散斑Speckle错位散斑干涉法speckle-shearinginterferometry, shearography 散斑图Specklegram白光散斑法white-light speckle method 云纹干涉法moire interferometry [叠栅]云纹moire fringe[叠栅]云纹法moire method 云纹图moire pattern离面云纹法off-plane moire method参考栅reference grating试件栅specimen grating分析栅analyzer grating面内云纹法in-plane moire method 脆性涂层法brittle-coating method条带法strip coating method坐标变换transformation ofCoordinates计算结构力学computational structuralmecha-nics 加权残量法weighted residual method 有限差分法finite difference method 有限[单]元法finite element method 配点法point collocation里茨法Ritz method广义变分原理generalized variationalPrinciple 最小二乘法least square method胡[海昌]一鹫津原理Hu-Washizu principle赫林格-赖斯纳原理Hellinger-ReissnerPrinciple 修正变分原理modified variationalPrinciple 约束变分原理constrained variationalPrinciple 混合法mixed method杂交法hybrid method边界解法boundary solution method 有限条法finite strip method半解析法semi-analytical method协调元conforming element非协调元non-conforming element混合元mixed element杂交元hybrid element边界元boundary element 强迫边界条件forced boundary condition 自然边界条件natural boundary condition 离散化Discretization离散系统discrete system连续问题continuous problem广义位移generalized displacement 广义载荷generalized load广义应变generalized strain广义应力generalized stress界面变量interface variable 节点node, nodal point [单]元Element角节点corner node边节点mid-side node内节点internal node无节点变量nodeless variable 杆元bar element桁架杆元truss element 梁元beam element二维元two-dimensional element 一维元one-dimensional element 三维元three-dimensional element 轴对称元axisymmetric element 板元plate element壳元shell element厚板元thick plate element三角形元triangular element四边形元quadrilateral element 四面体元tetrahedral element曲线元curved element二次元quadratic element线性元linear element三次元cubic element四次元quartic element等参[数]元isoparametric element超参数元super-parametric element 亚参数元sub-parametric element节点数可变元variable-number-node element 拉格朗日元Lagrange element拉格朗日族Lagrange family巧凑边点元serendipity element巧凑边点族serendipity family无限元infinite element单元分析element analysis单元特性element characteristics 刚度矩阵stiffness matrix几何矩阵geometric matrix等效节点力equivalent nodal force 节点位移nodal displacement节点载荷nodal load位移矢量displacement vector载荷矢量load vector质量矩阵mass matrix集总质量矩阵lumped mass matrix相容质量矩阵consistent mass matrix 阻尼矩阵damping matrix瑞利阻尼Rayleigh damping刚度矩阵的组集assembly of stiffnessMatrices载荷矢量的组集consistent mass matrix质量矩阵的组集assembly of mass matrices 单元的组集assembly of elements局部坐标系local coordinate system局部坐标local coordinate面积坐标area coordinates体积坐标volume coordinates曲线坐标curvilinear coordinates静凝聚static condensation合同变换contragradient transformation 形状函数shape function试探函数trial function检验函数test function权函数weight function样条函数spline function代用函数substitute function降阶积分reduced integration零能模式zero-energy modeP收敛p-convergenceH收敛h-convergence掺混插值blended interpolation等参数映射isoparametric mapping双线性插值bilinear interpolation小块检验patch test非协调模式incompatible mode节点号node number单元号element number带宽band width带状矩阵banded matrix变带状矩阵profile matrix带宽最小化minimization of band width 波前法frontal method子空间迭代法subspace iteration method 行列式搜索法determinant search method 逐步法step-by-step method纽马克法Newmark威尔逊法Wilson拟牛顿法quasi-Newton method牛顿-拉弗森法Newton-Raphson method 增量法incremental method初应变initial strain初应力initial stress切线刚度矩阵tangent stiffness matrix 割线刚度矩阵secant stiffness matrix 模态叠加法mode superposition method 平衡迭代equilibrium iteration子结构Substructure子结构法substructure technique 超单元super-element网格生成mesh generation结构分析程序structural analysis program 前处理pre-processing后处理post-processing网格细化mesh refinement应力光顺stress smoothing组合结构composite structure。

用于反无人机的双频八木天线的设计

用于反无人机的双频八木天线的设计

_用于反无人机的双频八木天线的设计摘要近年来,随着民用消费机无人机技术的发展和完善,使得操控无人机的门槛降低,一些发达地区已经开始禁飞无人机,现有民用无人机系统的遥控与数传系统所使用频段为2.4GHz与5.8GHz ,故制作小型化、高性能的双频八木天线具有很好的工程意义。

八木天线是一种最为常见的定向天线,它具有结构简单、方向性强、增益高等特点,被广泛应用在无线通信系统中。

但八木天线的缺点也很明显,体积过于庞大。

微带天线自问世以来因为其体积小巧、重量轻等优点很快得到学者们的关注,微带准八木天线便是微带天线和八木天线的产物。

微带准八木天线具有传统八木天线方向性强增益高等优点,同时拥有制作简单成本低等优势。

因此研究微带准八木天线有着极其重要的现实意义。

本文从八木天线和微带天线的基本理论入手,设计了一款双频微带准八木天线,其工作频段为2.4GHz-2.5GHz,另一个频段为5.7GHz-5.85GHz,在高频段的增益能达到5.5dB,低频段的增益相对较低。

关键词:反无人机;准八木天线;双频段;微带天线AbstractIn recent years, with the development and perfection of civil consumer UA V technology, the threshold of controlling UA V has been lowered. Some developed areas have begun to ban UA Vs, The frequency bands used in remote control and data transmission systems of existing civil UA V systems are 2.4 GHz and 5.8 GHz, Therefore, making a miniaturized and high performance dual-band Yagi antenna is of great engineering significance.Yagi antenna is one of the most common directional antennas, It has the characteristics of simple structure, strong directivity and high gain, and is widely used in wireless communication systems. But the shortcomings of Yagi antenna are also obvious, and its size is too large. Since its advent, microstrip antenna has attracted the attention of scholars because of its compact size and light weight. Microstrip quasi-Yagi antenna is the product of microstrip antenna and Yagi antenna. Microstrip quasi-Yagi antenna has the advantages of high directivity, high gain, simple fabrication and low cost. Therefore, the study of microstrip quasi-Yagi antenna has extremely important practical significance.This paper starts with the basic theory of Yagi antenna and microstrip antenna, A dual-band microstrip quasi-Yagi antenna is designed. Its working band is 2.4 GHz-2.5 GHz, and the other band is 5.7 GHz-5.85 GHz, The gain can reach 5.5dB in high frequency band, but it is relatively low in low frequency band.Key word:Anti UA V; Yagi antenna; Dual band; microstrip antenna目录第1章绪论 (1)1.1研究背景及意义 (1)1.2国内外研究现状 (1)1.3论文主要研究内容和章节安排 (5)1.3.1本文的主要研究内容 (5)1.3.2本文的内容安排 (5)第2章天线的基本理论 (6)2.1天线主要性能参数 (6)2.1.1天线的阻抗特性 (6)2.1.2天线的方向特性 (7)2.1.3天线的极化特性 (8)2.2天线的带宽 (9)2.3微带天线基本理论 (9)2.4本章小结 (11)第3章八木天线的基本原理 (12)3.1八木天线的结构 (12)3.2八木天线的工作原理 (13)3.3八木天线分析方法 (14)3.4本章小结 (17)第4章双频微带八木天线的设计与仿真分析 (18)4.1双频微带八木天线的设计 (18)4.2双频微带八木天线仿真分析 (20)4.3双频微带八木天线仿真优化 (23)4.4双频微带八木天线的加工与测试 (24)4.4.1双频微带八木天线的加工 (24)4.4.2双频微带八木天线的实物测试 (24)4.4.3实物测试误差分析 (25)4.5本章小结 (25)第5章结论与展望 (26)5.1总结 (26)5.2将来工作的方向 (26)参考文献 (27)致谢.......................................................第1章绪论1.1研究背景及意义随着无线通信技术发展迅猛,人们的的生活发生了翻天覆地的改变,如今,天线不在是军用产物或者收看电视频道的大锅盖,其领域逐渐进入日常的工作和生活中。

材料学织构类型中英文

材料学织构类型中英文

材料学织构类型中英文Material Science: The Fabric of Structural TypesThe field of material science encompasses a vast and intricate realm, where the very essence of the physical world is unraveled and understood. At the heart of this discipline lies the study of structural types, a captivating exploration of the intricate patterns and arrangements that define the properties and behaviors of various materials. From the crystalline structures of metals to the amorphous networks of glasses, the diversity of structural types is a testament to the ingenuity and complexity of the natural world.One of the most fundamental structural types in material science is the crystalline structure. Characterized by the orderly and repetitive arrangement of atoms or molecules, crystalline materials exhibit a high degree of long-range order and symmetry. This organization allows for the efficient packing of atoms, resulting in the unique physical and chemical properties that define materials such as metals, ceramics, and many minerals. The study of crystalline structures, including their formation, defects, and phase transformations, is crucial in understanding the behavior and applications of a wide range of materials.Alongside the crystalline structure, another prominent structural type is the amorphous structure. Unlike their crystalline counterparts, amorphous materials lack the long-range order and symmetry that define the crystalline state. Instead, they exhibit a more random and disordered arrangement of atoms or molecules, often resulting in unique mechanical, optical, and thermal properties. Glasses, polymers, and certain types of ceramics are examples of amorphous materials, each with its own distinct applications and characteristics.The study of structural types in material science extends beyond the binary classification of crystalline and amorphous. There exist a multitude of intermediate and hybrid structures that exhibit characteristics of both, blending the properties of order and disorder. These include semi-crystalline materials, where regions of crystalline order coexist with amorphous domains, and nanocrystalline structures, which feature nanometer-scale crystalline grains embedded in an amorphous matrix.The importance of understanding structural types in material science cannot be overstated. The arrangement and organization of atoms and molecules within a material directly influence its physical, chemical, and mechanical properties, making the study of structural types a crucial aspect of material design and engineering. By unraveling the complexities of these structural types, researchers andengineers can tailor the properties of materials to meet the ever-evolving demands of modern technology and industry.One of the primary tools used in the study of structural types is X-ray diffraction. This powerful analytical technique allows researchers to probe the atomic-scale structure of materials, revealing the intricate patterns and arrangements that define their properties. Through the analysis of diffraction patterns, scientists can identify the specific structural types present in a material, as well as quantify the degree of crystallinity, the size and orientation of grains, and the presence of defects or impurities.In addition to X-ray diffraction, other advanced characterization techniques, such as electron microscopy, neutron scattering, and spectroscopic methods, have become indispensable in the field of material science. These tools provide a multifaceted understanding of structural types, enabling researchers to investigate the relationship between atomic-scale structure and macroscopic properties.The applications of structural type analysis in material science are vast and far-reaching. In the realm of electronics, the understanding of crystalline and amorphous structures has paved the way for the development of semiconductors, superconductors, and advanced optoelectronic devices. In the field of materials science, the tailoringof structural types has led to the creation of high-performance alloys, ceramics, and composites with enhanced mechanical, thermal, and corrosion-resistant properties.Moreover, the study of structural types has implications far beyond the realm of traditional materials. In the emerging field of biomaterials, researchers are exploring the use of naturally occurring and biomimetic structures to develop cutting-edge medical devices, tissue engineering scaffolds, and drug delivery systems. The intricate structural types found in biological materials, such as bone, teeth, and spider silk, have inspired the development of novel materials with exceptional strength, toughness, and biocompatibility.As the field of material science continues to evolve, the study of structural types will undoubtedly remain at the forefront of scientific inquiry. With the ongoing advancements in characterization techniques, computational modeling, and materials synthesis, the understanding of structural types is poised to unlock new frontiers in materials design and engineering. From the development of next-generation energy storage devices to the creation of smart and responsive materials, the exploration of structural types will undoubtedly shape the future of our technological landscape.In conclusion, the study of structural types in material science is a multifaceted and captivating field, one that delves into the very heartof the physical world. From the ordered arrangements of crystalline structures to the intricate patterns of amorphous materials, the diversity of structural types is a testament to the remarkable complexity and versatility of the materials that surround us. As we continue to push the boundaries of our understanding, the exploration of structural types will undoubtedly remain a crucial and dynamic aspect of material science, guiding us towards a future where the very fabric of our world is woven with the insights and innovations of this remarkable discipline.。

热动专业英语词典

热动专业英语词典
criterion=标准
critical pressure=临界压力
crossflow=交叉流,横向冲刷
crude oil=原油
culm=煤屑
cycle efficiency=循环效率
cyclone furnace=旋风炉
debris=有机残余物,残骸
decane=葵烷
decay=分解
induced draft fan=引风机
industrial steam generator(boiler)=工业锅炉
inert=惰性
inferior=低级的,劣质的
ingredients=成分
ingress=进入,入口
in-line=顺列
in-line arrangement=顺列布置
inorganic=无机的
ion=离子
jurisdiction=权限
lattice=晶格结构
lb/h=磅/小时
lbf/in2=英制压力单位,磅/平方英寸
leakage air=漏风
lean gas=贫气
lignite=褐煤
liquefaction=液化
locally expensive fuels=当地廉价燃料
bituminous=烟煤
blade=叶片
blast furnace=高炉
blowdown=排污
boiler=锅炉
bottom water seal=炉底水封
Btu/h=英热单位/小时
bulk=大块的
burner=燃烧器
burner zone=燃烧器区域
butane=丁烷
capacity=出力,功率

Fabrication and testing of large free-form surfaces

Fabrication and testing of large free-form surfaces

TMT 1.4-m PM segments
JWST 1.3-m PM segments
Applications for freeform aspheres
Correction optics for wide field systems
Three-mirror anastigmat uses axisymmetric Cassegrain-type primarysecondary combination, slightly off axis Tertiary mirror is fully off axis
Interferometer with axisymmetric null corrector
Subaperture interferometry for small optics
Annular subapertures Zygo Verifire Asphere
Off axis subapertures QED SSI
Other TMA designs are fully off axis Designs often start with off axis portion of axisymmetric parent, then are
allowed to depart

Initial shaping for “standard” optics
that it always fits the surface. • Used for > 200 m^2 of axisymmetric aspheres • Software change to allow operation on freeform aspheres
2. Grinding and polishing tools don’t fit, limiting ability to make smooth surfaces
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Large Scale Fabrication of Quasi-Aligned ZnO Stacking NanoplatesXueli Cao,Haibo Zeng,*Ming Wang,Xijin Xu,Ming Fang,Shulin Ji,and Lide Zhang*Key Laboratory of Materials Physics,Institute of Solid State Physics,Chinese Academy of Sciences,Hefei 230031,Anhui,People’s Republic of ChinaRecei V ed:January 14,2008;In Final Form:February 28,2008The large scale fabrication of quasi-aligned ZnO stacking nanoplates was achieved for the first time by low-temperature solution growth with assistance of citrate.Each nanoplate is composed of two or several parallel stacking nanosheets in back-to-back way with the same central axis.These nanosheets are of single crystalline and with two large surfaces as ((0001)planes.Remarkably,these stacking nanoplates approximately vertically stand on the substrate by their side small planes,and their surface morphology and verticality can be further adjusted by the molar ratio of citrate to Zn 2+ions.The formation mechanism was considered according to the effect of introduced ions on the nucleation and growth process.These ZnO nanoplates with multilayer stacking and vertical alignment features have large specific surface area and c plane exposure and hence would have great potential advantages for correlative properties.ZnO nanostructures have attracted more and more interest because of their expected excellent exhibition in a great deal of properties and relevant applications.1Remarkably,some are strongly dependent on the particular exposed surface of the nanostructures,such as luminescence,photocatalytic,and sens-ing properties.2,3Some properties of ZnO nanostructures are strongly preferential to the c planes.For example,Ye et al.4have reported that the ZnO nanoplates have good photocatalytic activity,and the thinner nanoplates have higher performance.These results demonstrated that the c planes have higher photocatalytic activity than the side surfaces in ZnO.On the basis of this consideration,the method to fabricate the c plane-dominated ZnO nanostructures in which the relative surface area of the c plane is larger than that of others has emerged but still is a challenge.Generally,for ZnO,the highest surface energy of the c plane advances the growth along the c -axis,and results in the familiar nanowires in which the relative surface area of the c plane is very low.5,6Although c plane-dominated ZnO nanoplates have been reported recently,7there still remains a significant challenge to directly fabricate mul-tilayer ZnO nanoplate arrays in large scale with c plane-dominated surface,especially to those standing on the substrates.Here,we report the quasi-aligned ZnO stacking nanoplates for the first time,which were fabricated in large scale by citrate-assisted low-temperature solution method.These multilayer stacking and vertical alignment features enable them to possess great c -dominated planes,and the surface morphology and verticality can be further adjusted by the molar ratio of citrate ion/Zn 2+.The novel ZnO nanostructures are expected to have promising applications in c -dominated preferential properties.For example,the stacking ZnO nanoplates on substrates may be served as effective and convenient recycled photocatalysts.An aqueous solution composed of 0.01M hydrated zinc nitrate [Zn(NO 3)2‚6H 2O],0.01M hexamethylenetetramine (HMT,C 6H 12N 4),and trisodium citrate (molar ratio of citrate ion/Zn 2+0.02or 0.05)of reagent grade was first used as the nutrient solution.Silicon substrates were washed with acetone in an ultrasonic bath and etched by piranha solution (3:1concentrated H 2SO 4/30%H 2O 2).Quasi-aligned ZnO stacking nanoplate arrays were grown on the silicon substrate using a simple two-step process.In the first step,the colloidal ZnO nanocrystals were spin-coated on the substrate several times.Between coatings,the silicon substrate was annealed at 150°C to ensure particle adhesion to the substrate surface.ZnO nanocrystals were prepared according to the previously reported method of Pacholski.8After the silicon substrate was coated with ZnO nanocrystals,the seeded substrates were placed upside-down in a sealed bottle containing the nutrient solution.Then,the bottle was put into an oven and maintained at 80°C for 6h.Finally,the products on the silicon substrates were washed with deionized water several times and then dried for further characterization.The morphology and structure of the products were examined by field emission scanning electron microscopy (FE-SEM,FEI,Sirion 200),high-resolution transmission electron microscopy (HRTEM,JEOL 2010),and X-ray diffraction (XRD,Philips X’Pert Pro diffractometer with Cu K R Radiation).For the photocatalytic activity evaluation,the concentration of photo-degrated methylene blue was recorded by a spectrophotometer (SP-2000UV).The organic dyes (primal solution: 1.0×10-4M,30mL)and the catalysts (10mg)were thoroughly stirred in the dark to reach the adsorption equilibrium of the organic dyes with the catalyst and then exposed to light from a UV light (18W).Figure 1shows the XRD patterns of the samples fabricated with different citrate concentration.Without citrate in the nutrient solution,the sample represents the normal c -axis *To whom all correspondence should be addressed.E-mail:(H.Z)hbzeng@;(L.Z.)ldzhang@.Fax:+865515591434.Tel:+865515591465.52672008,112,5267-5270Published on Web 03/13/200810.1021/jp800499r CCC:$40.75©2008American Chemical Societypreferential orientation (Figure 1a).When citrate ion/Zn 2+molar ratio is 0.02(Figure 1b),the intensities of (100)and (002)peaks are similar,which suggests no obvious orientation in this sample.When increasing the citrate ion/Zn 2+molar ratio to 0.05,the XRD pattern exhibits very distinct (100)preferential orientation,as shown in Figure 1c,which implies that this sample may have special nanostructure:the ZnO (100)plane would be parallel to the substrate.These results indicate that the molar ratio of citrate ion/Zn 2+could greatly change the ZnO preferential growth orientation,inducing the evolvement from the (001)orientation without citrate,to the unconspicuous orientation with the citrate ion/Zn 2+molar ratio of 0.02and the (100)orientation with that of 0.05.Figure 2a shows a typical low-magnification FE-SEM image of the sample with a molar ratio of citrate ion/Zn 2+of 0.02.Obviously,ZnO nanoplates with uniform size have been fabricated in large scale.Cross-sectional image (Figure 2b)shows that the nanoplates form a monolayer array on the substrate,which is derived from the ZnO seed layer and stands on the substrate in a certain gradient.From the high magnifica-tion FE-SEM image (Figure 2c),almost all the nanoplates are composed of a large thin and a small thin nanosheet in back-to-back stacking way,which are of smooth and hexagonal morphologies.The diameter and the thickness of nanosheet are of about 1µm and 200nm,respectively.An enlarged FE-SEMimage (Figure 2c)also shows that there are some small hexagonal steps on one side of the plate.The TEM image and the selected area electron diffraction (SAED)(Figure 2d)patterns show the same result and also reveal that the top and bottom large surfaces of the nanoplate are ((0001)planes and {1-100}small side facets.The result suggests that citrate molecules slow down the crystal growth along the (001)orientation,which provides a simple approach to control the dominated special surface.By increasing the molar ratio of citrate ion/Zn 2+from 0.02to 0.05,we can also prepare large scale uniform nanoplate arrays,as shown in Figure 3a.However,several obvious differences can be observed in the sample with 0.05citrate ion/Zn 2+molar ratio compared to the sample with 0.02molar ratio.First,as shown in Figure 3,panels b and c,the stacking nanoplate has become multilayer.Second,the multilayer stacking nanoplate arrayshaveFigure 1.XRD patterns of the samples by low-temperature solution growth without citrate (a),growth with citrate ion/Zn 2+molar ratio of 0.02(b),and 0.05(c).Figure 2.FE-SEM (a -c)and TEM (d)images of ZnO double-layer stacking nanoplates corresponding to citrate ion/Zn 2+molar ratio of 0.02.The inset is the SAEDpattern.Figure 3.FE-SEM images of ZnO multilayer stacking nanoplates corresponding to citrate ion/Zn 2+molar ratio of 0.05,the low magnification FE-SEM (a),the high magnification FE-SEM (b),and the cross-sectional FE-SEM image (c).5268J.Phys.Chem.C,Vol.112,No.14,2008Lettersbetter verticality than double-layer stacking nanoplate arrays.Third,the ZnO nanoplate surface becomes rough and porous at citrate ion/Zn 2+of 0.05molar ratio compared to that of 0.02molar ratio.These multilayer stacking and rough surface will induce much larger specific surface area.These features will stimulate great application potential in c -plane related properties when combined with those well-standing nanoplates.The typical nanowire arrays were obtained by the normal solution growth without citrate assistance,as shown in Figure 4.According to the great differences in orientation and morphology between stacking nanoplate arrays and nanowire arrays,we learn that the citrate ion in nutrient solution plays a vital role in the nucleation and growth process.In principle,a crystal growth process consists of nucleation and growth,which is affected by the intrinsic crystal structure and the external conditions including the kinetic energy barrier,temperature,time and capping molecules,and so on.9The crystal structures of the nanoplates involved in the work are all hexagonal in nature.In general,for the materials of hexagonal nanoplates the anisotropic growth along the c -axis is available to form the one-dimensional nanostructures.5However,the hexagonal nanoplates reported here have been fabricated by the citrate-assisted low-temperature solution method.As we know,citrate is an important biological ligand for metal ions.It can form a strong complex with Ca 2+,Mg 2+,Zn 2+,Fe 2+,Au +,and Ag +ions.10While the citrate was introduced to the growth solution,the period for the formation of ZnO nuclei was remarkably changed.Zn 2+will form [Zn(C 6H 5O 7)412-]10-with citrate ion,which can bind to the positive charged Zn 2+terminated (0001)polar plane more strongly than to another nonpolar surface due to the Coulombic force.Such adsorption would slow down crystal growth along the [001]direction.11On the other hand,the citrate adsorption would slow down the surface energy,which could result in the (0001)surface not becoming the highest-energy surface.According,the intrinsically anisotropic growth of ZnO along the <001>direction is substantially suppressed and the platelike ZnO is formed,which is similar to the formation of the ZnO nanodisks.12Citrate again plays an important role in the formation of quasi-aligned ZnO stacking nanoplates by possible bonding to the Zn 2+(0001)surface through the -COO -and -OH groups and suppressing growth along the <001>direction;crystal growth then proceeds sideways,leading to the formation of stacking nanoplates.Different from the orientated column-to-plate,11,13the stacking nanoplates we synthesized are concave in center.From the detailed examination of the top and bottom of the back-to-back double nanoplate,the surface is quite different:one side is smooth and another is rough (Figure 2c).Around the roughsurface center,there are some fine step edges gradually sticking out and these lead to the concave in center.A single hexagonal plate can be further developed into multilayer plates along the steps.According to the above analyses,it was clearly demonstrated that the citrate adsorption can significantly change the ZnO growth orientation.Along with the increase of the molar ratio of citrate ion/Zn 2+,the orientation of products has changed from (001)to (100),and the morphology has changed from nanowires into stacking nanoplates.Besides the orientation and the morphology,the molar ratio of citrate/Zn 2+also strongly affected the verticality of the arrays.With the increase of the molar ratio of citrate ion/Zn 2+,the verticality of the ZnO nanoplate arrays was greatly improved.The seed layer on the substrate has a nonperfect c -orientation,in the early stages of growth;ZnO crystals grew along the fastest growth orientation along the <10-10>direction,and these crystals are not aligned.But as the platelike randomly oriented crystals grew further,they began to overlap and their growth became physically limited as the misaligned nanoplate began to impinge on other neighboring crystals,giving rise to the preferred orientation of the nanoplate arrays.When the citrate ion/Zn 2+has been increased to 0.05,large existence of complex compounds with citrate and Zn 2+finally results in the obviously (100)orientation nanoplate arrays,which are represented in the XRD pattern.If the citrate ion concentration is further increased,the impingement of the neighboring crystals also increases,so the verticality of the multilayer ZnO nanoplate arrays improves.The surface of the ZnO becomes rough and porous along with the increase of the molar ratio of citrate ions to zinc concentra-tion.This “etching”effect is similar to the results reported by Wang et al.14The comparison of photocatalytic activity of different samples is illustrated in Figure 5.Under the same conditions,the double and multilayer stacking nanoplates have much greater photo-catalytic activity in the decomposition of methylene blue compared to the common nanowire arrays.With the conversion of ZnO nanostructure from nanowire to the nanoplate,especially the multistacking nanoplate,the photocatalytic efficiency was greatly improved.This finding is exciting for exploration of photocatalysts with high efficiency but is reasonable according to its large specific surface area and large exposure of active c plane.These results further demonstrate that such standing ZnO stacking nanoplates have great potential applications in specific surface area and c plane-related properties.As to the origins of high photocatalytic efficiency of typical multistacking nanoplate arrays,two factors should be noted.The first one is thelargeFigure 4.FE-SEM image of ZnO nanowires without citrate in the growthprocess.Figure 5.Photodegradation efficiency of methylene blue by the double-layer stacking ZnO nanoplates (a),multilayer stacking ZnO nanoplates (b),and normal ZnO nanowires (c).Letters J.Phys.Chem.C,Vol.112,No.14,20085269specific surface area,which greatly enhances the light-harvesting due to the longer surface light path and reduced reflectance, and the pollutant-adsorption on the enlarged surface.Further-more,the dominated c surface could also greatly improve the performance.Yamaguchi and co-workers15have reported that photocatalytic activity of ZnO film strongly depends on the specified crystal faces that are exposed.Our results give an indication that the polar c surfaces have higher photocatalytic activity,compared with nonpolar planes,at least in the decomposition of methylene blue.This is coincident with the high surface energy of c planes.In summary,through addition of citrate ions in the growth nutrition large scale hexagonal ZnO stacking nanoplate arrays have been obtained for the first time,which are approximately vertical on substrate.It also reveals that the top and bottom wide surface of the nanoplate are((0001)planes and{1-100} side facets.These c-dominated ZnO nanoplates standing on silicon substrate have a large active surface area exposed to the environment.Also,we have clearly demonstrated that ZnO stacking nanoplate arrays with the dominated c planes show a much higher photocatalytic activity in decomposition of meth-ylene blue,compared with common nanowire arrays.The novel ZnO nanostructures are expected to have promising applications in other fields.Acknowledgment.This work supported by the Major Research Plan of the National Natural Science Foundation of China(10604055)and the National Basic Research Program of China(Grant2007CB936601)References and 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