Metal-dependent Structure and Self Association of the RAG1 Zinc-Binding Domain

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金属材料专业英语词汇

金属材料专业英语词汇

Material Science 材料科学Material Science Definition 材料科学定义Machinability[məʃi:nə'biliti]加工性能Strength .[streŋθ]强度Corrosion & resistance durability.[kə'rəʊʒən] &[ri'zistəns] .[ 'djʊrə'bɪlətɪ] 抗腐蚀及耐用Special metallic features 金属特性Allergic, re-cycling & environmental protection 抗敏感及环境保护Chemical element 化学元素Atom of Elements 元素的原子序数Atom and solid material 原子及固体物质Atom Constitutes 原子的组织图Periodic Table 周期表Atom Bonding 原子键结合Metal and Alloy 金属与合金Ferrous & Non Ferrous Metal 铁及非铁金属Features of Metal 金属的特性Crystal Pattern 晶体结构Crystal structure, Space lattice & Unit cell 晶体结构,定向格子及单位晶格X – ray crystal analytics method X线结晶分析法Metal space lattice 金属结晶格子Lattice constant 点阵常数Mill's Index 米勒指数Metal Phase and Phase Rule金相及相律Solid solution 固熔体Substitutional type solid solution 置换固熔体Interstitial solid solution 间隙固熔体Intermetallic compound 金属间化合物Transformation 转变Transformation Point 转变点Magnetic Transformation 磁性转变Allotropic Transformation 同素转变Thermal Equilibrium 热平衡Degree of freedom 自由度Critical temperature 临界温度Eutectic 共晶Peritectic [.peri’tekti k] Temperature包晶温度Peritectic Reaction 包晶反应Peritectic Alloy 包晶合金Hypoeutectic Alloy 亚共晶体Hypereutectic Alloy 过共晶体Plastic Deformation 金属塑性Slip Plan 滑动面Distortion 畸变Work Hardening 硬化Annealing 退火Crystal Recovery 回复柔软Recrystallization 再结晶Properties & testing of metal 金属材料的性能及试验Chemical Properties 化学性能Physical Properties 物理性能Magnetism 磁性Specific resistivity & specific resistance 比电阻Specific gravity & specific density比重Specific Heat比热热膨胀系数 Coefficient of thermal expansion导热度 Heat conductivity机械性能 Mechanical properties屈服强度(降伏强度) (Yield strength)弹性限度、杨氏弹性系数及屈服点 elastic limit, Young’s module of elasticity to yield point伸长度 Elongation断面缩率 Reduction of area破坏性检验 destructive inspections渗透探伤法 Penetrate inspection磁粉探伤法 Magnetic particle inspection放射线探伤法 Radiographic inspection超声波探伤法 Ultrasonic inspection显微观察法 Microscopic inspection破坏的检验 Destructive Inspection冲击测试 Impact Test疲劳测试 Fatigue Test蠕变试验Creep Test潜变强度 Creeps Strength第一潜变期 Primary Creep第二潜变期 Secondary Creep第三潜变期 Tertiary Creep主要金属元素之物理性质 Physical properties of major Metal Elements工业标准及规格–铁及非铁金属 Industrial Standard – Ferrous & Non – ferrous Metal磁力 Magnetic简介 General软磁 Soft Magnetic硬磁 Hard Magnetic磁场 Magnetic Field磁性感应 Magnetic Induction导磁率[系数,性] Magnetic Permeability磁化率 Magnetic Susceptibility (Xm)磁力(Magnetic Force)及磁场 (Magnetic Field)是因物料里的电子 (Electron)活动而产生抗磁体、顺磁体、铁磁体、反铁磁体及亚铁磁体 Diamagnetism, Paramagnetic, Ferromagnetisms, Antiferromagnetism & Ferrimagnetisms抗磁体 Diamagnetism磁偶极子 Dipole负磁力效应 Negative effect顺磁体 Paramagnetic正磁化率 Positive magnetic susceptibility铁磁体 Ferromagnetism转变元素 Transition element交换能量 Positive energy exchange外价电子 Outer valence electrons化学结合 Chemical bond自发上磁 Spontaneous magnetization磁畴 Magnetic domain相反旋转 Opposite span比较抗磁体、顺磁体及铁磁体 Comparison of Diamagnetism, Paramagnetic & Ferromagnetism反铁磁体 Antiferromagnetism亚铁磁体 Ferrimagnetism磁矩 magnetic moment净磁矩 Net magnetic moment钢铁的主要成份 The major element of steel钢铁用"碳"之含量来分类 Classification of Steel according to Carbon contents铁相 Steel Phases钢铁的名称 Name of steel铁素体Ferrite渗碳体 Cementitle奥氏体 Austenite珠光体及共析钢 Pearlite &Eutectoid奥氏体碳钢 Austenite Carbon Steel单相金属 Single Phase Metal共释变态 Eutectoid Transformation珠光体 Pearlite亚铁释体 Hyppo-Eutectoid初释纯铁体 Pro-entectoid ferrite过共释钢 Hype-eutectoid粗珠光体 Coarse pearlite中珠光体 Medium Pearlite幼珠光体 Fine pearlite磁性变态点 Magnetic Transformation钢铁的制造 Manufacturing of Steel连续铸造法 Continuous casting process电炉 Electric furnace均热炉 Soaking pit全静钢 Killed steel半静钢 Semi-killed steel沸腾钢(未净钢) Rimmed steel钢铁生产流程 Steel Production Flow Chart钢材的熔铸、锻造、挤压及延轧 The Casting, Fogging, Extrusion, Rolling & Steel熔铸 Casting锻造 Fogging挤压 Extrusion延轧Rolling冲剪 Drawing & stamping特殊钢以元素分类Classification of Special Steel according to Element特殊钢以用途来分类 Classification of Special Steel according to End Usage 易车(快削)不锈钢 Free Cutting Stainless Steel含铅易车钢 Leaded Free Cutting Steel含硫易车钢 Sulphuric Free Cutting Steel硬化性能 Hardenability钢的脆性 Brittleness of Steel低温脆性 Cold brittleness回火脆性 Temper brittleness日工标准下的特殊钢材 Specail Steel according to JIS Standard铬钢–日工标准 JIS G4104 Chrome steel to JIS G4104铬钼钢钢材–日工标准 G4105 62 Chrome Molybdenum steel to JIS G4105镍铬–日工标准 G4102 63 Chrome Nickel steel to JIS G4102镍铬钼钢–日工标准 G4103 64 Nickel, Chrome & Molybdenum Steel to JIS G4103高锰钢铸–日工标准 High manganese steel to JIS standard片及板材 Chapter Four-Strip, Steel & Plate冷辘低碳钢片(双单光片)(日工标准 JIS G3141) 73 - 95 Cold Rolled (Low carbon) Steel Strip (to JIS G 3141)简介 General美材试标准的冷辘低碳钢片 Cold Rolled Steel Strip American Standard – American Society for testing and materials (ASTM)日工标准 JIS G3141冷辘低碳钢片 (双单光片)的编号浅释 Decoding of cold rolled(Low carbon)steel strip JIS G3141材料的加工性能 Drawing ability硬度 Hardness表面处理 Surface finish冷辘钢捆片及张片制作流程图表 Production flow chart cold rolled steel coil sheet冷辘钢捆片及张片的电镀和印刷方法 Cold rolled steel coil & sheet electro-plating & painting method冷辘(低碳)钢片的分类用途、工业标准、品质、加热状态及硬度表 End usages, industrial standard, quality, condition and hardness of cold rolled steel strip硬度及拉力 Hardness & Tensile strength test拉伸测试(顺纹测试) Elongation test杯突测试(厚度: 0.4公厘至 1.6公厘,准确至 0.1公厘 3个试片平均数 ) Erichsen test (Thickness: 0.4mm to 1.6mm, figure round up to 0.1mm)曲面(假曲率) Camber厚度及阔度公差 Tolerance on Thickness & Width平坦度(阔度大于 500公厘,标准回火 ) Flatness (width>500mm, temper: standard)弯度 Camber冷辘钢片储存与处理提示 General advice on handling & storage of cold rolled steel coil & sheet 防止生锈 Rust Protection生锈速度表 Speed of rusting焊接 Welding气焊 Gas Welding埋弧焊 Submerged-arc Welding电阻焊 Resistance Welding冷辘钢片(拉力: 30-32公斤/平方米)在没有表面处理状态下的焊接状况 Spot welding conditions for bared (free from paint, oxides etc) Cold rolled mild steel sheets(T/S:30-32 Kgf/ µ m2)时间效应(老化)及拉伸应变 Aging & Stretcher Strains日工标准(JIS G3141)冷辘钢片化学成份 Chemical composition – cold rolled steel sheet to JIS G3141冷辘钢片的"理论重量"计算方程式 Cold Rolled Steel Sheet – Theoretical mass 日工标准(JIS G3141)冷辘钢片重量列表 Mass of Cold-Rolled Steel Sheet to JIS G3141冷辘钢片订货需知Ordering of cold rolled steel strip/sheet其它日工标准冷轧钢片(用途及编号) JIS standard & application of other cold Rolled Special Steel电镀锌钢片或电解钢片Electro-galvanized Steel Sheet/Electrolytic Zinc Coated Steel Sheet电解/电镀锌大大增强钢片的防锈能力Galvanic Action improving Weather & Corrosion Resistance of the Base Steel Sheet上漆能力 Paint Adhesion电镀锌钢片的焊接 Welding of Electro-galvanized steel sheet点焊 Spot welding滚焊 Seam welding电镀锌(电解)钢片 Electro-galvanized Steel Sheet生产流程 Production Flow Chart常用的镀锌钢片(电解片)的基层金属、用途、日工标准、美材标准及一般厚度 Base metal, application, JIS & ASTM standard, and Normal thickness of galvanized steel sheet锌镀层质量 Zinc Coating Mass表面处理 Surface Treatment冷轧钢片 Cold-Rolled Steel Sheet/Strip热轧钢片 Hot-Rolled Sheet/Strip电解冷轧钢片厚度公差 Thickness Tolerance of Electrolytic Cold-rolled sheet热轧钢片厚度公差 Thickness Tolerance of Hot-rolled sheet冷轧或热轧钢片阔度公差 Width Tolerance of Cold or Hot-rolled sheet长度公差 Length Tolerance理论质量 Theoretical Mass锌镀层质量(两个相同锌镀层厚度) Mass Calculation of coating (For equal coating)/MM锌镀层质量(两个不同锌镀层厚度) Mass Calculation of coating (For differential coating)/MM镀锡薄铁片(白铁皮/马口铁) (日工标准 JIS G3303)简介 General镀锡薄铁片的构造 Construction of Electrolytic Tinplate镀锡薄钢片(白铁皮/马日铁)制造过程 Production Process of Electrolytic Tinplate锡层质量 Mass of Tin Coating (JIS G3303-1987)两面均等锡层 Both Side Equally Coated Mass两面不均等锡层 Both Side Different Thickness Coated Mass级别、电镀方法、镀层质量及常用称号Grade, Plating type, Designation of Coating Mass & Common Coating Mass镀层质量标记 Markings & Designations of Differential Coatings硬度 Hardness单相轧压镀锡薄铁片(白铁皮/马口铁) Single-Reduced Tinplate双相辗压镀锡薄钢片(马口铁/白铁皮) Dual-Reduction Tinplate钢的种类 Type of Steel常用尺寸 Commonly Used Size电器用硅 [硅] 钢片 Electrical Steel Sheet简介 General软磁材料 Soft Magnetic Material滞后回线 Narrow Hysteresis矫顽磁力 Coercive Force硬磁材料 Hard Magnetic Material最大能量积 Maximum Energy Product硅含量对电器用的低碳钢片的最大好处 The Advantage of Using Silicon low Carbon Steel晶粒取向(Grain-Oriented)及非晶粒取向(Non-Oriented) Grain Oriented & Non-Oriented电器用硅 [硅] 钢片的最终用途及规格 End Usage and Designations of Electrical Steel Strip电器用的硅 [硅] 钢片之分类 Classification of Silicon Steel Sheet for Electrical Use电器用钢片的绝缘涂层 Performance of Surface Insulation of Electrical Steel Sheets晶粒取向电器用硅钢片主要工业标准 International Standard – Grain-Oriented Electrical Steel Silicon Steel Sheet for Electrical Use晶粒取向电器用硅钢片 Grain-Oriented Electrical Steel晶粒取向,定取向芯钢片及高硼定取向芯钢片之磁力性能及夹层系数 (日工标准及美材标准) Magnetic Properties and Lamination Factor of SI-ORIENT-CORE& SI-ORIENT-CORE-HI B Electrical Steel Strip (JIS and AISI Standard)退火 Annealing电器用钢片用家需自行应力退火原因 Annealing of the Electrical Steel Sheet退火时注意事项 Annealing Precautionary碳污染 Prevent Carbon Contamination热力应先从工件边缘透入 Heat from the Laminated Stacks Edges提防过份氧化 No Excessive Oxidation应力退火温度 Stress –relieving Annealing Temperature绝缘表面 Surface Insulation非晶粒取向电力用钢片的电力、磁力、机械性能及夹层系数 Lamination Factors of Electrical, Magnetic & Mechanical Non-Grain Oriented Electrical电器及家电外壳用镀层冷辘 [低碳] 钢片 Coated (Low Carbon) Steel Sheets for Casing,Electricals & Home Appliances镀铝硅钢片 Aluminized Silicon Alloy Steel Sheet镀铝硅合金钢片的特色 Feature of Aluminized Silicon Alloy Steel Sheet用途 End Usages抗化学品能力 Chemical Resistance镀铝(硅)钢片–日工标准 (JIS G3314) Hot-aluminum-coated sheets and coils to JIS G 3314镀铝(硅)钢片–美材试标准 (ASTM A-463-77)35.7 JIS G3314镀热浸铝片的机械性能 Mechanical Properties of JIS G 3314 Hot-Dip Aluminum-coated Sheets andCoils公差 Size Tolerance镀铝(硅)钢片及其它种类钢片的抗腐蚀性能比较 Comparsion of various resistance of aluminized steel & other kinds of steel镀铝(硅)钢片生产流程 Aluminum Steel Sheet, Production Flow Chart焊接能力 Weldability镀铝钢片的焊接状态(比较冷辘钢片) Tips on welding of Aluminized sheet in comparasion with cold rolled steel strip钢板 Steel Plate钢板用途分类及各国钢板的工业标准包括日工标准及美材试标准 Type of steel Plate & Related JIS, ASTM and Other Major Industrial Standards钢板生产流程 Production Flow Chart钢板订货需知 Ordering of Steel Plate不锈钢 Stainless Steel不锈钢的定义 Definition of Stainless Steel不锈钢之分类,耐腐蚀性及耐热性Classification, Corrosion Resistant & Heat Resistance of Stainless Steel铁铬系不锈钢片Chrome Stainless Steel马氏体不锈钢Martensite Stainless Steel低碳马氏体不锈钢Low Carbon Martensite Stainless Steel含铁体不锈钢Ferrite Stainless Steel镍铬系不锈钢Nickel Chrome Stainless Steel释出硬化不锈钢Precipitation Hardening Stainless Steel铁锰铝不锈钢Fe / Mn / Al / Stainless Steel不锈钢的磁性Magnetic Property & Stainless Steel不锈钢箔、卷片、片及板之厚度分类Classification of Foil, Strip, Sheet & Plate by Thickness表面保护胶纸Surface protection film不锈钢片材常用代号Designation of SUS Steel Special Use Stainless 表面处理 Surface finish 薄卷片及薄片(0.3至 2.9mm 厚之片)机械性能Mechanical Properties of Thin Stainless Steel(Thickness from 0.3mm to 2.9mm) – strip/sheet 不锈钢片机械性能(301, 304, 631, CSP) Mechanical Properties of Spring use Stainless Steel不锈钢–种类,工业标准,化学成份,特点及主要用途Stainless Steel – Type, Industrial Standard, Chemical Composition, Characteristic & end usage of the most commonly used Stainless Steel不锈钢薄片用途例End Usage of Thinner Gauge不锈钢片、板用途例Examples of End Usages of Strip, Sheet & Plate不锈钢应力退火卷片常用规格名词图解General Specification of Tension Annealed Stainless Steel Strips耐热不锈钢Heat-Resistance Stainless Steel镍铬系耐热不锈钢特性、化学成份、及操作温度Heat-Resistance Stainless Steel铬系耐热钢Chrome Heat Resistance Steel镍铬耐热钢Ni - Cr Heat Resistance Steel超耐热钢Special Heat Resistance Steel抗热超级合金Heat Resistance Super Alloy耐热不锈钢比重表Specific Gravity of Heat – resistance steel plates and sheets stainless steel不锈钢材及耐热钢材标准对照表Stainless and Heat-Resisting Steels发条片 Power Spring Strip发条的分类及材料 Power Spring Strip Classification and Materials上链发条 Wind-up Spring倒后擦发条 Pull Back Power Spring圆面("卜竹")发条 Convex Spring Strip拉尺发条 Measure Tape魔术手环 Magic Tape魔术手环尺寸图 Drawing of Magic Tap定型发条 Constant Torque Spring定型发条及上炼发条的驱动力 Spring Force of Constant Torque Spring and Wing-up Spring定型发条的形状及翻动过程 Shape and Spring Back of Constant Torque Spring定型发条驱动力公式及代号The Formula and Symbol of Constant Torque Spring边缘处理 Edge Finish硬度 Hardness高碳钢化学成份及用途 High Carbon Tool Steel, Chemical Composition and Usage每公斤发条的长度简易公式 The Length of 1 Kg of Spring Steel Strip SK-5 & AISI-301每公斤长的重量 /公斤(阔 100-200公厘) Weight per one meter long (kg) (Width 100-200mm) SK-5 & AISI-301每公斤之长度 (阔 100-200公厘) Length per one kg (Width 100-200mm) SK-5 & AISI-301每公尺长的重量 /公斤(阔 2.0-10公厘) Weight per one meter long (kg) (Width 2.0-10mm) SK-5 & AISI-301每公斤之长度 (阔 2.0-10公厘) Length per one kg (Width 2.0-10mm)高碳钢片 High Carbon Steel Strip分类 Classification用组织结构分类 Classification According to Grain Structure用含碳量分类–即低碳钢、中碳钢及高碳钢 Classification According to Carbon Contains弹簧用碳钢片 Carbon Steel Strip For Spring Use冷轧状态 Cold Rolled Strip回火状态 Annealed Strip淬火及回火状态 Hardened & Tempered Strip/ Precision – Quenched Steel Strip贝氏体钢片 Bainite Steel Strip弹簧用碳钢片材之边缘处理 Edge Finished淬火剂 Quenching Media碳钢回火 Tempering回火有低温回火及高温回火 Low & High Temperature Tempering高温回火 High Temperature Tempering退火 Annealing完全退火 Full Annealing扩散退火 Diffusion Annealing低温退火 Low Temperature Annealing中途退火 Process Annealing球化退火 Spheroidizing Annealing光辉退火 Bright Annealing淬火 Quenching时间淬火 Time Quenching奥氏铁孻回火 Austempering马氏铁体淬火 Marquenching高碳钢片用途 End Usage of High Carbon Steel Strip冷轧高碳钢–日本工业标准 Cold-Rolled (Special Steel) Carbon Steel Strip to JIS G3311电镀金属钢片 Plate Metal Strip电镀金属捆片的优点Advantage of Using Plate Metal Strip金属捆片电镀层 Plated Layer of Plated Metal Strip镀镍 Nickel Plated镀铬 Chrome Plated镀黄铜 Brass Plated基层金属 Base Metal of Plated Metal Strip低碳钢或铁基层金属 Iron & Low Carbon as Base Metal不锈钢基层金属 Stainless Steel as Base Metal铜基层金属 Copper as Base Metal黄铜基层金属 Brass as Base Metal轴承合金 Bearing Alloy轴承合金–日工标准 JIS H 5401 Bearing Alloy to JIS H 5401锡基、铅基及锌基轴承合金比较表 Comparison of Tin base, Lead base and Zinc base alloy for Bearing purpose易溶合金 Fusible Alloy焊接合金 Soldering and Brazing Alloy软焊 Soldering Alloy软焊合金–日本标准 JIS H 4341 Soldering Alloy to JIS H 4341硬焊 Brazing Alloy其它焊接材料请参阅日工标准目录 Other Soldering Material细线材、枝材、棒材 Chapter Five Wire, Rod & Bar线材/枝材材质分类及制成品 Classification and End Products of Wire/Rod铁线(低碳钢线)日工标准 JIS G 3532 Low Carbon Steel Wires ( Iron Wire ) to JIS G 3532光线(低碳钢线),火线 (退火低碳钢线 ),铅水线 (镀锌低碳钢线)及制造钉用低碳钢线之代号、公差及备注 Ordinary Low Carbon Steel Wire, Annealed Low Carbon Steel Wire, Galvanized low Carbon Steel Wire & Low Carbon Steel Wire for nail manufacturing - classification, Symbol of Grade, Tolerance and Remarks.机械性能 Mechanical Properites锌包层之重量,铜硫酸盐试验之酸洗次数及测试用卷筒直径 Weight of Zinc-Coating, Number of Dippings in Cupric Sulphate Test and Diameters of Mandrel Used for Coiling Test冷冲及冷锻用碳钢线枝 Carbon Steel Wire Rods for Cold Heading & Cold Forging (to JIS G3507) 级别,代号及化学成份 Classification, Symbol of Grade and Chemical Composition直径公差,偏圆度及脱碳层的平均深度 Diameter Tolerance, Ovality and Average Decarburized Layer Depth冷拉钢枝材 Cold Drawn Carbon Steel Shafting Bar枝材之美工标准,日工标准,用途及化学成份 AISI, JIS End Usage and Chemical Composition of Cold Drawn Carbon Steel Shafting Bar冷拉钢板重量表 Cold Drawn Steel Bar Weight Table高碳钢线枝 High Carbon Steel Wire Rod (to JIS G3506)冷拉高碳钢线 Hard Drawn High Carbon Steel Wire (to JIS G3521, ISO-84580-1&2)化学成份分析表 Chemical Analysis of Wire Rod线径、公差及机械性能(日本工业标准 G 3521) Mechanical Properties (JIS G 3521)琴线(日本标准 G3522) Piano Wires (to G3522)级别,代号,扭曲特性及可用之线材直径 Classes, symbols, twisting characteristic and applied WireDiameters直径,公差及拉力强度 Diameter, Tolerance and Tensile Strength裂纹之容许深度及脱碳层 Permissible depth of flaw and decarburized layer常用的弹簧不锈钢线-编号,特性,表面处理及化学成份 Stainless Spring Wire – National Standard number, Characteristic, Surface finish & Chemical composition弹簧不锈钢线,线径及拉力列表Stainless Spring Steel, Wire diameter and Tensile strength of Spring Wire处理及表面状况 Finish & Surface各种不锈钢线在不同处理拉力比较表 Tensile Strength of various kinds of Stainless Steel Wire under Different Finish圆径及偏圆度之公差 Tolerance of Wire Diameters & Ovality铬镍不锈钢及抗热钢弹簧线材–美国材验学会 ASTM A313 – 1987 Chromium – Nickel Stainless and Heat-resisting Steel Spring Wire – ASTM A313 – 1987化学成份 Chemical Composition机械性能 Mechanical Properties305, 316, 321及 347之拉力表 Tensile Strength Requirements for Types 305, 316, 321 and 347 A1S1-302贰级线材之拉力表 Tensile Strength of A1S1-302 Wire日本工业标准–不锈钢的化学成份 (先数字后字母排列) JIS –Chemical Composition of Stainless Steel (in order of number & alphabet)美国工业标准–不锈钢及防热钢材的化学成份 (先数字后字母排列) AISI – Chemical Composition of Stainless Steel & Heat-Resistant Steel(in order of number & alphabet)易车碳钢 Free Cutting Carbon Steels (to JIS G4804 )化学成份 Chemical composition圆钢枝,方钢枝及六角钢枝之形状及尺寸之公差 Tolerance on Shape and Dimensions for Round Steel Bar, Square Steel Bar, Hexagonal Steel Bar易车(快削)不锈钢 Free Cutting Stainless Steel易车(快削)不锈钢种类 Type of steel易车(快削)不锈钢拉力表 Tensile Strength of Free Cutting Wires枝/棒无芯磨公差表 (μ) (μ = 1/100 mm) Rod/Bar Centreless Grind Tolerance易车不锈钢及易车钢之不同尺寸及硬度比较 Hardness of Different Types & Size of Free Cutting Steel 扁线、半圆线及异形线 Flat Wire, Half Round Wire, Shaped Wire and Precision Shaped Fine Wire 加工方法 Manufacturing Method应用材料 Material Used特点 Characteristic用途End Usages不锈钢扁线及半圆线常用材料 Commonly used materials for Stainless Flat Wire & Half Round Wire 扁线公差 Flat Wire Tolerance方线公差 Square Wire Tolerance。

一类新型镁材料——镁基金属有机骨架材料

一类新型镁材料——镁基金属有机骨架材料

2018年第37卷第9期 CHEMICAL INDUSTRY AND ENGINEERING PROGRESS·3437·化 工 进展一类新型镁材料——镁基金属有机骨架材料韩森建,王海增(中国海洋大学化学化工学院,山东 青岛 266100)摘要:镁基金属有机骨架材料(Mg-MOFs )是近年来逐渐受到关注的一类新型功能材料,其种类与结构多样化,使其在很多领域中展现出了潜在的应用价值,为镁资源的开发利用开拓了一个新的领域。

本文从Mg-MOFs 的种类、特点、制备方法、应用以及稳定性5个方面展开论述。

详细阐述了Mg-MOFs 在催化、药物缓释、光学材料、气体储存、气体吸附和分离等方面的应用,着重介绍了Mg-MOFs 的储氢能力和对二氧化碳的吸附能力及对不同混合物的选择分离能力。

提出了今后Mg-MOFs 的研究重点:优化Mg-MOFs 的制备条件,降低制备难度及成本;选择新的配体源及溶剂,开发具有结构稳定、高比表面积、功能多样的Mg-MOFs ,扩大其在气体吸附与选择性分离方向的应用;将Mg-MOFs 应用于复合材料中,拓宽其应用范围。

关键词:镁基金属有机骨架材料;羧酸配体;储氢;分离中图分类号:O6-1 文献标志码:A 文章编号:1000–6613(2018)09–3437–09 DOI :10.16085/j.issn.1000-6613.2017-2174A new material of magnesium complexes——magnesium based metalorganic frameworksHAN Senjian , WANG Haizeng(College of Chemistry and Chemical Engineering, Ocean University of China, Qingdao 266100, Shandong, China)Abstract :Magnesium based metal organic frameworks (Mg-MOFs), as a new kind of functional material, have recently drawn much research attention. Due to the diversified specie and structures, Mg-MOFs have shown potential applications in many fields, which provide a new research area for the development and utilization of magnesium resources. Five aspects on Mg-MOFs are discussed in this article, including the main types, characteristics, preparation method, applications and stability. The applications of Mg-MOFs in catalysis, drug delivery, optical properties, gas storage, adsorption and separation are elaborated, and the capacities of hydrogen storage, carbon dioxide adsorption and selective uptake are presented emphatically. In addition, the prospects and challenges in the future are pointed out. For instance: optimizing the preparation conditions of Mg-MOFs to reduce the process difficulty and costs; selecting new ligands and solvent to prepare Mg-MOFs of high surface area, developing varieties of functional Mg-MOFs with structural stability to expand their applications in gas adsorption and separation, and applying Mg-MOFs to the composite materials to extend their application range.Key words: magnesium based metal organic frameworks (Mg-MOFs); ligands of carboxylic acid; storage hydrogen gas; separation我国镁资源总储量世界第一,包括固态镁资源和液态镁资源[1]。

4氨基安替比林4AAP和2氨基54吡啶134噻二唑4APTD分子在银电极表面

4氨基安替比林4AAP和2氨基54吡啶134噻二唑4APTD分子在银电极表面

摘要上世纪70年代中期发展起来的表面增强拉曼散射光谱(surfaceenhancedRRmRnscattering,SERS),具有超高的灵敏度,可以探测到吸附在特定金属表面的单层分子,目前已广泛地应用在研究吸附界面的表面状态、生物大分子的构型、构象和界面取向以及结构分析等领域。

原位表面增强拉曼散射光谱(in.situSERS)技术可以现场研究表面吸附和界面反应,是一种在线、实时的原位技术。

自组装单层(Self-assembledmonolayers,SAMs)是溶液(或气态)分子通过分子间作用力在固体基底上自发形成的一类排列规则、热力学稳定的单层膜,该膜具有均匀一致,高密度堆积和缺陷少等特点。

该技术常用于表面分析并为表面及界面现象的研究提供分子膜板。

而电化学交流阻抗是一种暂态、原位的电化学测试技术,目前在电极过程、金属的腐蚀机理及缓蚀剂性能评价等方面得到广泛应用,是评价缓蚀剂膜性能和监测膜完整性的有效方法。

用量少、操作方便的金属缓蚀剂在金属防腐领域得到越来越广泛的关注,但不同类型缓蚀剂的缓蚀机理到目前为止还不甚明了,且同种缓蚀剂在不同环境下对同种金属或处于相同环境中的不同金属的缓蚀机理也不尽相同,金属缓蚀剂的缓蚀机理对我们应用金属缓蚀剂具有指导意义,因此对其的研究还将是一个重点。

表面增强拉曼散射光谱(SERS)技术和电化学方法联用可以在分子水平现场监测电极表面吸附分子的吸附行为和其缓蚀性能的关系,从而帮助理解缓蚀剂分子的缓蚀机理。

根据上述设想本论文开展了以下几方面的工作:1.利用表面增强拉曼散射(SERS)光谱原位考察不同电位下4.氨基安替比林(4.AAP)在电极表面的吸附机理以及其组装液pH值对其与银作用方式的影响。

依据密度泛函数(DFT)理论预测4-AAP分子振动模式及其SERS光谱归属。

结果表明:在开路电位下,组装层中的4-AAP分子以N15和03为位点,由苯环倾斜和比林环垂直的方式吸附在银表面;但随着外加电压负移,4-AAP分子的苯环趋于垂直吸附而比林环则逐渐以平行方式靠近银表面。

MOFS材料

MOFS材料
28
课后作业
通过学校图书馆的ACS及RSC数据库,任选 一篇关于MOFs材料的光、电、磁、吸附、催化 等性能方面的研究论文,仔细研读后,写出一篇 不少于200字的读后感。
29
MOFs材料设计原理
30
MOFs 包括两个重要的组分:结点(connectors, 网络结构中的节点)和联接体(linkers,联接网络结构 结点间的化学键或包含多个化学键的有机官能团)。 在多孔MOF中,人们通常把金属离子看作为结点,配 体作为联接体。
24
目前,国际上许多化学家、物理学家和材料学 家的研究结果表明,MOFs 多孔材料在气体的储存、 催化剂、分离及光电磁材料等方面具有重要的应用 价值。
另外,金属位在大量的分子识别过程中起关键 性的作用,因为金属位能产生高度的选择性和分子 的储存和传送。
MOFs材料经常具有不饱和金属位和大的比表 面积,这在化学工业有着广阔的应用前景。
BDC groups (C: shaded circles). (b) The same with four ZnO4 tetrahedra shaded. (c) The same with the C6 octahedron shaded. (d) The BDC anion (O: open circles, C: shaded circles). (e) The link (the phenyl of the BDC anion).
manipulations are very easy.

A major disadvantage of this approach is that the
outcomes are often difficult to be predicted since no

金属有机骨架材料MOFs及其应用ppt课件.ppt

金属有机骨架材料MOFs及其应用ppt课件.ppt
• we choose MIL-101 as the stationary phase and xylene isomers and ethy-lbenzene (EB) as the targets for separation.
Gu, Z. Y. Yan, X. P. Angewandte Chemie-International Edition 49, 1477-1480 (2010)
Hydrogen Storage in Microporous rganic Frameworks
Rosi, N. L. Eckert, J. Eddaoudi, M. O'Keeffe, M.Yaghi, O. M. science 300, 1027-1029 (2003)
MOF-5的储氢性能
实验流程图
吸附性能
富集效果
105ppb
2030ppb
Metal–Organic Framework MIL-101 for HighResolution Gas-Chromatographic Separation of
Xylene Isomers and Ethylbenzene
• We show the first fabrication of the MOFcoated capillary column for high-resolution GC separation.
78K
298K
Rowsell, J. L. C. Spencer, E. C. Eckert, J. Yaghi, O. M. science 309, 1350-1354 (2005)
Metal Organic Frameworks as Adsorbents for Trapping and Preconcentration of Organic Phosphonates

金属有机配位聚合物的制备及其性能的测试

金属有机配位聚合物的制备及其性能的测试

南京航空航天大学硕士学位论文摘要金属-有机配位聚合物是由金属中心离子与有机配体自组装而形成的。

金属-有机配位聚合物新颖的多样结构导致其许多特殊的性能。

由于含硫芳基多齿配体本身结构的多样性,在与金属离子配位时,可以组装出结构新颖和功能独特的配合物。

它们表现出不同寻常的光、电、磁等性质,在非线性光学,磁性和催化材料等方面具有潜在的应用前景。

本课题为含硫金属-有机配位聚合物的合成和性能表征。

文中对到目前为止的金属-有机配位聚合物的研究成果进行了系统的总结。

本论文分别以对苯二胺和对苯二酚为有机小分子,与二硫化碳在碱性条件下反应,在反复实验的基础上,找到了合适的反应条件,冷凝回流合成出了以硫为配位原子的有机配体。

用均相法和溶剂热合成法,将生成的配体与过渡金属在含有表面活性剂的条件下混合发生配位反应,制备了相应的含硫过渡金属配位聚合物,考察各反应因素对配位聚合物形貌的影响。

最后,通过FTIR,EDS,SEM,TEM,紫外-可见等分析手段对配体和配合物进行表征,发现所合成的镉(Ⅱ)配位聚合物具有半导体的性质。

关键词:金属-有机配位聚合物,溶剂热合成,二硫化碳,配体,表征iABSTRACTMetal-organic coordination polymers are a type of self-assembly formed by organic ligands and metal ions. Diversified structures of the coordination polymers result in unusual properties of the novel materials. Duo to the structure multiformity of multidentate organic ligand with the sulfur and aryl, they can assemble out complexes of novel structures and unique fuctions if coordinated with metal ions. They have shown distinctive optical, electrical, and magnetic properties, thus they have a potential applied prospect in nonlinear optics, magnetic and catalytic materials.The subject is to synthesize and analyze the property of sulfur metal-organic coordination polymers. In this dissertation, we do the summary of the development and achievements of metal-organic coordination polymers. In this paper, we use p-phenylenediamine or p-dihydroxybenzene as small organic molecules to react with carbon bisulfide in alkaline condition. We find out the appropriate reaction condition on the basis of repeated experiments, and synthesize organic ligand with the sulfur as coordination atom in the condition of refluxing. Then we use the acquired ligands to react with transition metal ions under surfactant by solvothermal and homogeneous techniques and get the corresponding transition metal complexes with the sulfur atom. We have explored the influences of all kinds of synthesis factors for their morphologies. Finally, through analytical methods such as FTIR, EDS, SEM, TEM, UV-vis, we characterize the ligands and complexes, and suggest that the Cd(Ⅱ) complex is a semi-conductor.Keywords: metal-organic coordination polymers, solvothermal synthesis, carbon bisulfide, ligand, characterizeii图表清单图清单图1.1 金属-有机配位聚合物的金属中心 (5)图1.2 组装金属-有机配位聚合物使用的多齿配体 (6)图3.1 配体合成实验装置图 (19)图4.1 实验Pt-02-04配体L的红外谱图 (34)图4.2 实验Pt′-03-04配体L′的红外谱图 (35)图4.3 实验Pt-02-04配体L的能谱分析图 (35)图4.4 实验Pt′-03-04配体L′的能谱分析图 (36)图4.5 均相法合成的Cd(Ⅱ)配位聚合物TEM图(PEG-400, 5%) (37)图4.6 均相法合成的Cd(Ⅱ)配位聚合物TEM图(PEG-400, 2%) (38)图4.7 特殊形貌的Ni(Ⅱ)配位聚合物的SEM图 (39)图4.8 特殊形貌的Co(Ⅱ)配位聚合物的SEM图 (40)图4.9 特殊形貌的Cd(Ⅱ)配位聚合物的SEM图 (40)图4.10 特殊形貌的Cu(Ⅰ)配位聚合物的SEM图 (41)图 4.11 不同温度下所得Cd(Ⅱ)配位聚合物的SEM图 (a)120℃ (b) 150℃ (43)图 4.12不同降温速率下所得Cu(Ⅰ)配位聚合物的SEM图 (a)5℃/h (b)2℃/h (44)图4.13 添加不同的表面活性剂所得产物的SEM图 (45)图4.14添加不同量的表面活性剂所得产物的SEM图 (46)图4.15 Cd(Ⅱ)配位聚合物液态紫外可见图 (47)图4.16 Cd(Ⅱ)配位聚合物的能谱分析图 (48)Ⅱ配位聚合物(A)固态紫外-可见图;(B)吸收系数与光子能图4.17 Cd()量的关系图 (49)表清单表1.1 几个对应金属-有机配位聚合物的基本概念 (4)vi南京航空航天大学硕士学位论文表3.1 实验所用药品 (17)表3.2 合成配体主要药品物性 (18)表3.3 仪器及设备 (19)表3.4 以对苯二胺为有机小分子R合成配体 (20)表3.5 以对苯二酚为有机小分子R′合成配体 (21)表3.6 均相法合成配位聚合物的实验结果 (23)表3.7 溶剂热合成配位聚合物的实验结果 (24)vii承诺书本人郑重声明:所呈交的学位论文,是本人在导师指导下,独立进行研究工作所取得的成果。

1 A new model of metal plasticity and fracture with pressure and lode dependence(MIT)

1 A new model of metal plasticity and fracture with pressure and lode dependence(MIT)

A new model of metal plasticity and fracturewith pressure and Lode dependenceYuanli Bai *,Tomasz WierzbickiImpact and Crashworthiness Lab,Massachusetts Institute of Technology,77Massachusetts Avenue,Room 5-218,Cambridge,MA 02139,USAReceived 28June 2007;received in final revised form 28August 2007Available online 14September 2007AbstractClassical metal plasticity theory assumes that the hydrostatic pressure has no or negligible effect on the material strain hardening,and that the flow stress is independent of the third deviatoric stress invariant (or Lode angle parameter).However,recent experiments on metals have shown that both the pressure effect and the effect of the third deviatoric stress invariant should be included in the con-stitutive description of the material.A general form of asymmetric metal plasticity,considering both the pressure sensitivity and the Lode dependence,is postulated.The calibration method for the new metal plasticity is discussed.Experimental results on aluminum 2024-T351are shown to validate the new material model.From the similarity between yielding surface and fracture locus,a new 3D asymmetric fracture locus,in the space of equivalent fracture strain,stress triaxiality and the Lode angle parameter,is postulated.Two methods of calibration of the fracture locus are discussed.One is based on classical round specimens and flat specimens in uniaxial tests,and the other one uses the newly designed but-terfly specimen under biaxial testing.Test results of Bao (2003)[Bao,Y.,2003.Prediction of ductile crack formation in uncracked bodies.PhD Thesis,Massachusetts Institute of Technology]on alumi-num 2024-T351,and test data points of A710steel from butterfly specimens under biaxial testing validated the postulated asymmetric 3D fracture locus.Ó2007Elsevier Ltd.All rights reserved.Keywords:Pressure effect;Lode dependence;Yield surface;Fracture locus;Calibration method0749-6419/$-see front matter Ó2007Elsevier Ltd.All rights reserved.doi:10.1016/j.ijplas.2007.09.004*Corresponding author.E-mail address:byl@ (Y.Bai).Available online at International Journal of Plasticity 24(2008)1071–10961072Y.Bai,T.Wierzbicki/International Journal of Plasticity24(2008)1071–10961.IntroductionThe classical J2theory of metal plasticity assumes that the effect of hydrostatic pressure r m on plasticflow is negligible,and further assumes that theflow stress is independent of the third stress invariant of the stress deviator.For application to ductile fracture,these assumptions must be carefully examined.Ductile fracture is a local phenomenon and the state of stress and strain in potential fracture locations must be determined with great accuracy.Fracture initiation is often preceded by large plastic deformation and there are considerable stress and strain gradients around the point of fracture.In these situations, the infinitesimal J2theory of plasticity is not accurate enough,and more refined plasticity models has to be introduced.The soil and rock mechanics community has long recognized a need for incorporating the hydrostatic and deviatoric(Lode angle parameter)stress invariants into a constitutive descriptions(see for example Bardet,1990;Menetrey and Willam,1995).More recently Bigoni and Piccolroza(2003)proposed a general failure surface for geomaterials in the space of principal stresses that reduces in limiting cases to the Tresca hexagon or the von Mises circle.The Sandia GeoModel(Fossum and Brannon,2006)is also formulated in the space of three invariants.The developments in geomaterials was proceeding over the decades independently of metal plasticity with the latter lagging behind the former.Based on an extensive experimental study,Richmond and Spitzig(Richmond and Spit-zig,1980;Spitzig and Richmond,1984)werefirst to demonstrate the effect of hydrostatic pressure on yielding of aluminum alloys.This conclusion has recently been confirmed by Wilson(2002),who studied notched2024-T351aluminum bars in tension.The concept of a shrinking yield surface with hydrostatic pressure was put forward independently by Gur-son(1975)and later by Needleman and Tvergaard(1984)in their studies of ductile frac-ture by the nucleation,growth and coalescence of voids.The common shortcoming of these various theories of porous plasticity has been an ill-defined calibration procedure.In general,the hydrostatic pressure is controlling the size of the yield surface while the Lode angle parameter is responsible for its shape.The determination of an adequate shape of the yield surface has become an issue in the sheet metal forming industry.It was found a long time ago that the von Mises plane stress ellipse does not lead to a correct prediction of the necking instability.There are an abundance of various modifications and generaliza-tions of the plane stress yield curve to bring the prediction closer to reality(Karafillis and Boyce,1993;Barlat et al.,1991,1997,2005;Vegter and van den Boogaard,2006).How-ever,most of the above theories included the effect of an in-plane anisotropy and the con-nection between the shape of yield condition and the Lode angle parameter has only been noticed recently.In particular,the effect of the Lode angle parameter(or the third devia-toric stress invariant)on plastic yielding has been studied by Cazacu and Barlat(2004), Cazacu et al.(2006),Racherla and Bassani(2007).Their models incorporate the difference in strength under compression and tension.They showed that the forming limit diagram of sheets was sensitive in that difference.However,their models did not have enoughflexibil-ity to predict plane strain yielding.Such a generalization is proposed in the present paper.The paper is divided into two parts.Thefirst part is concerned with a development of a more general plasticity model.Results of21tests on three groups of specimens are ana-lyzed through afinite element simulation.It is shown that the parameters of the J2plas-ticity model with power hardening rule,determined from one test,can not predict correctly the load–displacement responses in the all remaining tests.A new plasticitymodel with correction for the hydrostatic pressure and the Lode parameter brings a per-fect correlation with test results.Percentage-wise,the correction for the hydrostatic pres-sure is small.Physically,it could be attributed to the effect of hydrostatic pressure on metal crystal dislocations.The magnitudes of correction due to the deviatoric state parameter (Lode angle parameter)is large and in some cases reaches20%.The effect of hydrostatic pressure is consistent with earlierfinding of other authors(Richmond and Spitzig,1980; Spitzig and Richmond,1984;Wilson,2002).The new yield surface is asymmetric in the space of principal stresses losing three planes of symmetry as compared to the Tresca yield condition with six plane of symmetry,so it is asymmetric in any of the Tresca’s six sym-metry planes.The second part of the paper deals with the determination of the3D locus of the frac-ture initiation points.The locus is determined experimentally from two types of test pro-cedures.One is based on classical round specimens orflat specimens in uniaxial tests,and the other one uses a series of tests on a double curvature butterfly specimen subjected to bi-axial loading under different combination of tension/shear and compression/shear.The test points are thenfitted to a smooth surface which describes the dependence of the equiv-alent strain to fracture on the average stress triaxiality and the normalized third invariant of the deviatoric stress tensor(or Lode angle parameter).Again,it is shown that the best fit of test data is provided by a surface which is asymmetric with respect to the Lode angle parameter.2.Characterization of the stress stateThe extended metal plasticity model and the3D fracture locus will be formulated in terms of three invariants of the stress tensor[r],defined respectively byp¼Àr m¼À13trð½r Þ¼À13ðr1þr2þr3Þ;ð1Þq¼ r¼ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi32½S :½Sr¼ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi12½ðr1Àr2Þ2þðr2Àr3Þ2þðr3Àr1Þ2r;ð2Þr¼92½S Á½S :½S1=3¼272detð½S Þ!1=3¼272ðr1Àr mÞðr2Àr mÞðr3Àr mÞ!1=3;ð3Þwhere[S]is the deviatoric stress tensor,½S ¼½r þp½I ;ð4Þ[I]is the identity tensor and r1,r2and r3denote principal stresses.Note that the param-eter p is positive in compression,but r m is positive in tension.It is convenient to work with the dimensionless hydrostatic pressure g,defined byg¼Àpq¼r mr:ð5ÞThe parameter g,often referred to as the triaxiality parameter,has been extensively used in the literature on ductile fracture(McClintock,1968;Rice and Tracey,1969;Hancock and Mackenzie,1976;Mackenzie et al.,1977;Johnson and Cook,1985;Bao,2003).The sec-ond important parameter is the Lode angle h.The geometrical represent of Lode angle is Y.Bai,T.Wierzbicki/International Journal of Plasticity24(2008)1071–10961073shown in Fig.1.The Lode angle h is related to the normalized third deviatoric stress invariant n (see Malvern,1969;Xu and Liu,1995)throughn ¼r q3¼cos ð3h Þ:ð6ÞSince the range of the Lode angle is 06h 6p /3,the range of n is À16n 61.Further-more,the Lode angle h can be normalized byh ¼1À6h p ¼1À2parccos n :ð7ÞThe range of h is À16 h 61.The parameter h will be called the Lode angle parameter hereinafter.Now,all stress directions (or called loading conditions)can be characterized by the above defined set of parameters ðg ; h Þ.Various stress states encountered in ‘‘classi-cal ”specimens used for plasticity and fracture testing can be uniquely characterized by the above defined set of parameters ðg ; h Þ,as shown in Table 1.The analytical expressions for the stress triaxiality g ,the parameter h in terms of measurable quantities are all listed in Table 1.Special attention is given to the plane stress state.It was shown by Wierzbicki and Xue (2005)that the condition r 3=0uniquely relates the parameters g and n (or h )through n ¼cos p 2ð1À h Þh i ¼À272g g 2À13:ð8ÞA plot of Eq.(8)is shown in Fig.2.Points corresponding to 10types of ‘‘classical ”spec-imens and tests are marked by circles.The function h (Eq.(8))has three roots correspond-ing to pure shear (g =0, h ¼0)and the transverse plastic plane strain (g ¼Æ1ffiffi3p , h ¼0).3.A new form of metal plasticityThe plasticity theory to be developed in this section is valid under several assumptions.Firstly,the homogeneity and material isotropy are assumed.Secondly,the material is taken to be elastic–plastic with isotropic hardening.The extension to the combined isotro-pic/kinematic hardening could be made following the procedures suggested by Khan (for example Khan and Jackson,1999).Finally,the plastic incompressibility is assumed.1074Y.Bai,T.Wierzbicki /International Journal of Plasticity 24(2008)1071–10963.1.Effect of hydrostatic pressure on yieldThe concept of pressure dependent yield condition goes back to Coulomb–Mohr,and Drucker and Prager (1952).This concept,originally developed for soil and granular mate-rials,was shown more recently in a number of publications (Richmond and Spitzig,1980;Brownrigg et al.,1983;Spitzig and Richmond,1984;Bru ¨nig,1999)to be applicable to metal plasticity.According to the above theories,the initial and current yield function is taken in this paper to be a linear function of the normalized pressure,g ,r yld ¼ r ð e p ÞÀa I 1¼ r ð e p Þ1À3ar m p !¼ r ð e p Þð1À3ag Þ;ð9ÞTable 1Ten types of classical specimens for plasticity and fracture calibrationNo.Specimen type Analytical expressions for stress triaxiality g a The Lode angle parameter h 1Smooth round bars,tension 1312Notched round bars,tension (Bridgman,1952)13þffiffiffi2p ln 1þa 2R ÀÁ13Plastic plane strain,tension ffiffi3p 304Flat grooved plates,tension (Bai et al.,2006b )ffiffi3p 31þ2ln 1þt 4R ÀÁÂÃ05Torsion or shear 006Cylinders,compression À13À17Equi-biaxial plane stress tension 23À18Equi-biaxial plane stress compression À2319Plastic plane strain,compression Àffiffi3p 3010Notched round bars,compression À13þffiffiffi2p ln 1þa 2R ÀÁÂÃÀ1a In the expressions of g ,R is the radius of a notch or a groove,a is the radius of a round bar at the notch,t is the thickness of a flat grooved plate at the groove.Y.Bai,T.Wierzbicki /International Journal of Plasticity 24(2008)1071–109610751076Y.Bai,T.Wierzbicki/International Journal of Plasticity24(2008)1071–1096where I1=3r m and e p is the equivalent plastic strain.The proportionality parameter a should be calibrated from tests.In Eq.(9),thefirst strain hardening term, rð e pÞ,represents the stress–strain curve in zero hydrostatic pressure,for example in the torsion test.In prac-tice,tensile tests of a smooth round bar or a dog-bone specimen are very commonly used to calibrate the stress–strain curve.Therefore,more generally,Eq.(9)can be rewritten asr yld¼ rð e p;g Þ½1À3aðgÀg Þ ¼ rð e pÞ½1Àc gðgÀg Þ ;ð10Þwhere rð e pÞis material strain hardening function from the reference test,and g is the ref-erence value of stress triaxiality from the reference test,for example,g =1/3for smooth round bar tensile test,g =À1/3for cylindrical specimen compressive test,g =0for tor-sion test and so on.Here,c g is a material constant need to be calibrated,which represents the hydrostatic pressure effect on material plasticity.It should also be noted that the effect of pressure on plasticity does not have to be linear.Experimental data for ices showed a non-linear pressure effect(Karr et al.,1989).A linear function is proposed in this paper for metals.The present concept of pressure dependent yield function for metals should not be con-fused with Gurson type of softening(Gurson,1975;Needleman and Tvergaard,1984)due to the nucleation,growth and linkage of voids.In a simple tensile test,it is difficult to tell what physical mechanism is responsible for the observed softening-the suppression of dis-location motion or the growth of material porosity with deformation.The physically based Eq.(10)explains a relative difference in the stress–strain curves obtained in tests with various stress triaxialities,which can be measured experimentally by a few simple tests.At the same time,the material softening in the GTN model(Needleman and Tverg-aard,1984)is an illusive concept because the reference state is the undamaged stress–strain curve for the matrix material,which can not be found from any simple tests.The revers-ibility of the softening is another issue even though(Spitzig and Richmond,1984)did not address it directly.It is implicitly assumed that the dislocation suppression is reversible. This means that when in the loading process the hydrostatic pressure is brought back to the original value,the material will regain its initial strength.It is useful to design a test program involving a controlled change of the triaxiality to distinguish the two types of softening as discussed above.One such test could,for example,would involve two-stage tensile tests on notched round bars.After some plastic deformation the test is stopped and the gauge section of a specimen is re-machined to a larger radius.Such tests are being planned by the present authors.3.2.Lode dependenceThe dependence of the yield condition on the Lode angle parameter can best be explained by comparing the von Mises and Tresca yield condition.In the polar coordinate system,the equivalent stress becomes the radial coordinate while the circumferential coor-dinate is the Lode angle h.In the deviatoric stress plane,the von Mises yielding condition is represented by a circle.The Tresca yielding is a hexagon inscribed on the von Mises cir-cle,as shown in Fig.3.To take the third deviatoric stress invariant into account,a new term considering the effect of the Lode angle is introduced into Eq.(10).The following yield criterion is proposed:r yld ¼ r ð e p Þ½1Àc g ðg Àg 0Þ c s h þðc ax h Àc s h Þc Àc m þ1m þ1 !;ð11Þwhere c and c ax h are two parameters defined by c ¼cos ðp =6Þ1Àcos ðp =6Þ1cos ðh Àp =6ÞÀ1 !¼6:4641½sec ðh Àp =6ÞÀ1 ;ð12Þc ax h ¼c t h for h P 0;c c h for h <0:(ð13ÞEq.(11)defines a class of function that define the shape of the yield surface.The term cos(h Àp /6)in the definition of the parameter c represents the difference between von Mises and Tresca in the deviatoric stress plane,which is obtained from the geometrical construction by comparing the von Mises circle and the Tresca hexagon.After modifica-tion and normalization,the range of c is 06c 61,in which c =0is corresponding to plane strain or shear condition,and c =1is corresponding to axial symmetry.In Eq.(11),the leading term is linear with respect to the parameter c ,the higher order power term c m þ1m þ1 is introduced to make the yield surface smooth and differentiable with respect to Lode angle h around c =1.The parameter m is a non-negative integer.There are fourmaterial constants,c t h ,c s h ,c c h and m ,need to be calibrated.The values of c t h ,c s h ,and c c h are relative,and at least one of them is equal to unity.This depends on which type of ref-erence test is used to calibrate the strain hardening function rð p Þ.For example,if a smooth round bar tensile test is used,then c t h ¼1;if a torsion test is used,then c s h ¼1;if a cylinder specimen compressive test is used,then c c h ¼1.It can be proved that the postulated yield function (Eq.(11))is smooth and differentia-ble.The convexity of yield surface is controlled by the ratios of three parameters c t h ,c c h andc s h .Compared with von Mises and Tresca yield conditions,this yield surface can be plotted in the deviatoric stress plane,as shown in Fig.3.Examples of yield loci are shown in Fig.4for the case of plane stress.By suitably choosing model parameters,some limiting cases are obtained.For example,assuming either c g =0and c t h ¼c s h ¼c c h ¼1or m =0gives the von Mises yield condition,Y.Bai,T.Wierzbicki /International Journal of Plasticity 24(2008)1071–10961077while taking c g =0and c s h ¼ffiffiffi3p =2;c t h ¼c c h ¼1;m ¼þ1gives the Tresca yield criterion.If the parameter c g ¼0in above two cases,then one will get Drucker and Prager yield function (1952)and pressure-modified Tresca yield function.Most of metal plasticity the-ories assume that,in the deviatoric stress plane,the yield function is symmetric for uniaxial tension and uniaxial compression,which are corresponding to h ¼1and h ¼À1respec-tively (for example,Tresca,1864;Mises,1913;Barlat et al.,1991;Karafillis and Boyce,1993).This restriction can be removed in the present model by setting c t h ¼c c h .It shouldbe noted that the flattening property of the von Mises ellipse,which is needed for right prediction of the Forming Limit Curves,was introduced by many authors in the space of principal stresses using non-quadratic yield function (Hosford,1972;Karafillis and Boyce,1993;Barlat et al.,1991,1997),often under plane stress assumption.Vegter and van den Boogaard (2006)modeled the plane stress yield locus by fitting Brezier curves into four test points.Working on the deviatoric plane with the Lode angle dependence is another way of controlling the shape of the yield surface in a simple and elegant way.3.3.The deviatoric associated flow ruleThe yield surface,given by Eq.(11),can be visualized in the space of three principle stresses (r 1,r 2,r 3),see Fig.5.According to the conventional associated flow rule,d e plij ¼d k o f o r ij ;ð14Þwhere the plastic potential is defined byf ¼q À r ð e p Þ½1Àcg ðg Àg 0Þ c sh þðc ax h Àc s h Þc Àc m þ1m þ1 !;ð15ÞFig.4.Examples of yield locus for plane stress condition.(Here,c t h ¼1,and the effect of hydrostatic pressure is dis-activated,c g =0).1078Y.Bai,T.Wierzbicki /International Journal of Plasticity 24(2008)1071–1096d k is the equivalent plastic strain increment,and q is defined by Eq.(2).To implement a yield function intofinite element codes,a necessary step is to derive the expression for thenormal direction(orflow direction)with respect to yield locus,o fij .From the yield func-tion,Eq.(15),one can geto f o r ij ¼o qo r ijþ rð e pÞc g c shþðc axhÀc shÞcÀc mþ1mþ1!o go r ijÀ rð e pÞ½1Àc gðgÀg ÞÂðc axhÀc shÞð1Àc mÞo co r ij;ð16Þwhere o qo r ij ,o go r ijand o co r ijcan be expressed by the following equations.o q o r ij ¼32qs ij;ð17Þo g o r ij ¼13qd ijÀ3g2q2s ij;ð18Þo c o r ij ¼3ffiffiffi3p2Àffiffiffi3p!tanðhÀp=6ÞcosðhÀp=6Þ1q sin3hd ij3þcos3h2qs ijÀ32q2s ik s kj:ð19ÞAlthough the plasticity is pressure sensitive,experiments show that the plastic dilatancy of metals is negligible(Spitzig and Richmond,1984).To satisfy the assumption of plasticincompressibility,thefirst term13q d ij in Eq.(18)should be removed.Therefore,what isused in the present paper is aflow rule with deviatoric associativity,see Eq.(20),rather than the conventional associatedflow rule,Eq.(16).d e pl ij¼d k32qs ijÀ rð e pÞc g c shþðc axhÀc shÞcÀc mþ1mþ1!3g2q2s ij &À rð e pÞ½1Àc gðgÀg Þ ðc axh Àc shÞð1Àc mÞÂ3ffiffiffi3p2Àffiffiffi3p!tanðhÀp=6ÞcosðhÀp=6Þ1q sin3hd ij3þcos3h2qs ijÀ32q2s ik s kj):ð20ÞFig.5.A postulated3D yield surface.Y.Bai,T.Wierzbicki/International Journal of Plasticity24(2008)1071–10961079Clearly,the presence of additional terms in Eq.(20)indicate that the direction of plastic flow is normal to the yield surface in the deviatoric plane but not to von Mises yield sur-face.In this issue,the present formulation can be classified as an intermediateflow rule between the non-associatedflow rule and the conventional‘‘fully”associated one.(It should be noted that if this model is used to model other non-metallic porous materials, which are plastic compressible,then a fully associatedflow rule as previous stated is nec-essary).This new form of metal plasticity has been implemented into Abaqus user material subroutine VUMAT using the classical mapping return algorithm.The following numer-ical simulations are run with the material subroutine.4.Experimental calibration of2024-T351aluminumA power function is introduced to describe the isotropic stain hardening for metal plasticity.rð e pÞ¼Aðe þ e pÞn for r P r y;ð21Þwhere is thefirst yield strain.There are nine parameters,A, ,n,c g,g ,c th ,c sh,c ch,and m,in the present plasticity model.To validate and calibrate the model,four types of tests are required.Thefirst test is the smooth round bar tensile test,from which the baseline stress–strain curve(parameters:A, and n)can be determined.Also,the reference parametersare uniquely defined:g =1/3and c th ¼1.The second test is the notched round bars tensiletest.Introducing a geometric notch to a smooth round bar increases the hydrostatic pres-sure in the materials inside the neck.Wilson(2002)conducted this type of test on alumi-num2024-T351,and calibrated the pressure effect on metal plasticity,but the effect of Lode angle was not taken into account.The third test is the tensile test offlat groovedplates,which can be used to calibrate the parameter c sh .The fourth test is the cylindricalspecimens’upsetting test,which can be used to calibrate the last two parameters c ch andm.The corresponding stress states of these four types of tests are also respectively marked as A,B,C and D in Fig.3.The analysis and a description of experimental study of thefirst three types of tests were described in the earlier report(Bai et al.,2006b)in detail.In this paper,emphasis is put on the numerical simulation study and plastic model calibration.4.1.Smooth and notched round bars tensile testsSmooth round bar tensile tests were used to calibrate the stress–strain curve.There are three steps involved.Firstly,the engineering stress–strain curve r E(e E)is obtained from the force–displacement curve P(u)recorded during the test.Secondly,the true stress–strain curve rð eÞis calculated from the engineering stress–strain curve using the classical trans-formation law, r¼r Eð1þe EÞand e¼lnð1þe EÞ.In this step,only the data point before specimen necking can be used because the transformation equations are valid only up to necking initiation.Approximately,one can take the peak point of the force–displacement curve as the necking initiation point.Thirdly,a power function(Eq.(21))is used tofit the true stress–strain curve obtained from the test.This curve is then extrapolated to get the approximate true stress–strain curve after necking.Two methods are available to determine more precisely the true stress–strain curve after necking.If the continuous measurements of the neck geometry are available,then the Bridgman correction is applicable.Alternatively,the inverse method could be used in 1080Y.Bai,T.Wierzbicki/International Journal of Plasticity24(2008)1071–1096which the stress–strain curve after necking is adjusted to get good agreement of the mea-sured force–displacement curve.For the present material,the neck was not deep and it was not necessary to adjust the stress–strain curve after necking.A group of tensile tests of smooth and notched round bars were conducted,refer to Fig.6.The diameter of smooth round bar specimens is9mm.For notched round bar spec-imens,the diameter of the minimal cross-section is8mm,and two radii of notches are assigned,equal to12mm and4mm,respectively.The diameters in specimens shoulder are all equal to15mm,and the length of gauge section for this group of specimens is 25.5mm.The selected material is aluminum2024-T351.To diminish a possible effect of material anisotropic,all the specimens discussed in this paper are machined from the roll-ing direction(or90°direction)of a same material block.Furthermore,Bao(2003)has shown that the effect of anisotropy of2024-T351aluminum alloy is negligible.Two to four tests are conducted for each case.The stress–strain curve was calibrated from a smooth round bar tensile test,so g =1/3. To calibrate the pressure dependence coefficient c g,thefinite element models of the spec-imens were constructed with the Lode angle terms switched off.Round bar specimens are discretized by4-node axisymmetric elements.Finite element models of Abaqus/explicit are built,in which the user material subroutine VUMAT is used.The measured force–dis-placement curves are shown in Figs.7and8.In order to study possible mesh dependency, calculations were run usingfine(0.1mm)and coarse(0.2mm)meshes.The maximal dif-ference of the force–displacement response was less than0.5%,meaning that thefinite ele-ment solution was convergent.All the results presented in this paper use thefine mesh size. From Figs.7and8,one can see that without any corrections,the force–displacement response of the smooth round bar simulation agrees with the experimental results very well,but the notched round bar simulations over-predict the force–displacement curves about3–6%.Similar reduction in the material strength were also reported by Bru¨nig (1999)and Kuroda(2004).The reason is that the material points inside a notched round bar are subjected to higher pressure than the smooth round bar.This phenomenon shows the effect of hydrostatic pressure on stress–strain curve.By changing the coefficient c g iteratively,a value of c g=0.09is obtained,which makes the force–displacement curvesFig.6.A group of smooth and notched round bar specimens.。

《金属基复合材料》第二章,界面及相容性

《金属基复合材料》第二章,界面及相容性

2.2 Definition of interface (界面的定义)
It is a micro-region between matrix and reinforcements where the chemical composition is changed markedly and load can be transferred. It is a new phase which has a certain thickness and structure of which has obvious difference as compared to reinforcement or matrix. So called interfacial phases.
Type of interfacial binding force:(界面结合力有三类) 1) Mechanical combining force —— Friction,
(机械结合——摩擦力)
2) Physical combining force —— Vanderwaals force and hydrogen bond,(物理结合——范德华力和氢键)
metal matrix composite materials cannot be considered in isolation, they are mutually related. Chemical interactions and reactions between the matrix and the reinforcement component determine the interface adhesion, modify the characteristics of the composite components and affect the mechanical characteristics significantly. In high temperature use of MMCs the microstructure has to remain stable for long service periods. Thermal stability and failure is determined by changes in the microstructure and at the interfaces, e.g. reaction and precipitation processes. Thermal stress of MMCs can take place both isothermally and cyclically. The effects show differences. During a cyclic load of monolithic materials, especially at high temperature gradients and cycle speeds, a high probability of failure by thermal fatigue is to be expected, e.g. short-fiber reinforced aluminum alloys possess good thermal shock stability. The formation of the interface between the matrix and the reinforcing phase has a substantial influence on the production and characteristics of the metallic composite materials. The adhesion between both phases is usually determined by the interaction between them. During the production of the molten matrix e.g. by infiltration, wettability becomes significant.

金属有机框架物简介

金属有机框架物简介

金属-有机框架化合物简介金属-有机框架化合物(Metal-Organic Frameworks,MOFs)通常是指以有机配体为连接体(linkers)和以金属离子或簇为节点(nodes),通过配位键组装形成的具有周期性结构的配位化合物。

由于MOFs材料在荧光、催化、气体吸附与分离、质子导体、药物运输等方面具有潜在的应用价值,近十几年来,发展非常迅速,大量结构新颖的MOFs被不断的设计合成出来。

随着现代配位化学和晶体工程的发展,MOFs之间的键合作用已经不再仅局限于配位键作用,还囊括了其他作用力,比如:氢键作用,范德华力,芳香环之间的π-π作用等。

这些丰富的作用力使得MOFs结构和功能更加多元化、复杂化。

近几年来,计算机技术和仿真技术被应用到MOFs的研究中,在它们的帮助下,越来越多的新型MOFs材料不断的被合成出来。

与传统的多孔材料相比,MOFs材料的优势在于结构和功能的可设计性和调控性。

在理想情况下,通过合理设计配体和选择金属离子构筑的次级构建单元(SBUs),就可以合成目标结构和功能的MOFs。

虽然,目前每年有很多结构新颖性能特别的MOFs被合成报道,然而,在很多情况下,看似合理的设计,却很难实现。

这与MOFs的自主装过程有关。

在MOFs的合成过程中,除了配体和金属离子的影响外,还有其他的影响因素,比如:反应温度、溶剂、pH值、压力、配体和金属盐的比例与浓度等,每一个反应条件的改变,都有可能影响MOFs 的自主装过程,从而影响MOFs的结构,进而可能影响MOFs的性能。

总之,在通常情况下,根据金属离子构筑的SBUs和有机配体的几何构型可以预测MOFs最终的框架结构。

例如:平面方格结构可以通过4-连接平面构型SBU和直线型2-连接配体形成,如:MOF-118;类金刚石结构则可以通过四面体构型的4-连接SBU和直线型2-连接配体形成;立方结构框架则可以通过6-连接的SBU和直线型2-连接配体形成,如:MOF-5;T d八面体结构可以通过3-连接配体和轮桨状的4-连接SBU构筑,如:HKUST-1 (Figure1.1)。

刘一男考研词汇速记指南-完整版

刘一男考研词汇速记指南-完整版

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illuminate luminous aluminum lure luxury luxurious marathon media medieval medium immediate module mod e mod el mould mosaic napkinopera drama partner partnership partd epartd eparture partial impartial particle particular impart peakpoke spear pierce spur pyramid peek aspect inspect expect respect irrespective respective perspective spectacl e spectacular speculate suspect suspicion suspicious prospect specimen prosper prosperity prosperity prosperous d espited espise pence pension compensate pennydispensable indispensable expensive expend spend finance financialfinefiscalpolishrallyallyalliance coalitionraprelyreligion religious reliable liablerifle safeguard guard ward guarantee warrant ward robe steward saint sanction sane insane scan scanty skim schedule table series insertd esert assert exert sham shameashamed shop shop floor shopping skull sharp sarcastic satire shark slaveslitsliceslotslyslip slope slippery lubricate snoopy snobbish strain constrain constraint restrain 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anthropol ogist trialturbine turmoil ultimate ultimatum ultraviolet worship shapeassist consist consistent insist persist resist transistor attend tend tend ency extend extent intend tend er trend trench entrench tedious tedium antenna cognitive cognition recognize electric electronelectronic electrical electricity eminent prominent menacemineund ermine entertain entertainment attainretain sustain sustainable d etain maintain maintenance contain content tame exhibit inhibit prohibit multiple multiply multitud e multimedia第八章中国好谐音admire admirable admiration agony ache nostalgy nostalgic alcohol ambition ambitious annoy anxiety anxious arithmetic awkward bachelor banquet bare barely barren pare bark embark barge barley barn bizarre blunt blund er brochure bull buffet category ceaseclue clumsy coal curse curriculum d amn cond emn d emosbureaucracy d emonstrate epid emic diamond dilute dinosaurd onated ose drastic drugdump dwarf economy economic economical economics eliteend orse end owfad efeeble famine fertile fertilize fertilizer sterile glamour glamorous grant hazard hud dle idiot illusion indulge injure ivory jungle lame lameness lease liege allegiance lod ge loyalloyalty alloy marvelous marvel meltweld merciful mercy militant military mist moist mystery mysterious myth naughty nuisance oath parasite paradigm panic poultry plow propagand a propagate porcelain queer weird retrieve rhythm rumor tumor scene scenery scenario scheme screw scrutiny slaughter sleeve smuggle spoil sponge sponsor。

GROWTH OF INORGANIC THIN FILMS USING SELF-ASSEMBL

GROWTH OF INORGANIC THIN FILMS USING SELF-ASSEMBL

专利名称:GROWTH OF INORGANIC THIN FILMSUSING SELF-ASSEMBLED MONOLAYERS ASNUCLEATION SITES发明人:ENGSTROM, James, R.,KILLAMPALLI, Aravind, S.,MA, Paul, F.申请号:US2005021384申请日:20050617公开号:WO06/009807P1公开日:20060126专利内容由知识产权出版社提供摘要:Systems and methods for preparing inorganic-organic interfaces using organo-transition metal complexes and self -assembled monolayers as organic surfaces. In one embodiment, a silicon wafer is cleaned and reacted with stabilized pirhana etch to provide an oxide surface. The surface is reacted with the trichlorosilyl end of alkyltrichlorosilanes to prepare self assembling monomers (SAMs). The alkyltrichlorosilanes have the general formula R1-R-SiC13, where R1 is -OH, -NH2, -COOH, -SH, COOCH3, -CN, and R is a conjugated hydrocarbon, such as (CH2)n where n is in the range of 3 to 18. The functionalized end of the SAM can optionally modified chemically as appropriate, and is then reacted with metal-bearing species such as tetrakis(dimethylamido)titanium,Ti[N(CH3)2]4, (TDMAT) to provide a titanium nitride layer.申请人:ENGSTROM, James, R.,KILLAMPALLI, Aravind, S.,MA, Paul, F.地址:20 Thornwood Drive, Suite 105 Ithaca, NY 14850-1265 US,355 Warren Road Ithaca, NY 14850 US,134 Summerhill Drive, Apt.1 Ithaca, NY 14850 IN,135 Acalanes Dr., Apt.14 Sunnyvale, CA 94086 US国籍:US,US,IN,US代理机构:MILSTEIN, Joseph, B., Ph.D 更多信息请下载全文后查看。

新型铋基金属有机框架的合成及其光催化产氢性能

新型铋基金属有机框架的合成及其光催化产氢性能
© 2019, Dalian Institute of Chemical Physics, Chinese Academy of Sciences. Published by Elsevier B.V. All rights reserved.
Metal-organic frameworks (MOFs) composed of metal-oxo clusters and polydentate organic linkers represent an intriguing class of porous crystalline material with many attractive properties such as porosity, large surface area, and structural and functional tunability [1]. Because of these unique advantages, MOFs have been widely investigated for gas storage and separation, sensors, drug delivery, and catalysis [2]. Some photo-responsive MOFs exhibiting semiconductor behavior have been developed as photocatalysts for promising solar energy conversion. In particular, solar-driven water splitting is of great significance when considering that hydrogen evolution

金属有机骨架UiO-66 在催化领域的应用

金属有机骨架UiO-66 在催化领域的应用

CHEMICAL INDUSTRY AND ENGINEERING PROGRESS 2019年第38卷增刊1收稿日期:2019–07–11;修改稿日期:2019–07–30。

基金项目:国家自然科学基金(21808142);上海应用技术大学中青年科技发展基金(ZQ2018-3)。

第一作者:于吉行(1995—),男,硕士,研究方向为工业催化。

E-mail :yuzihang168@ 。

通信作者:俞俊,副教授,硕士生导师,研究方向为工业催化。

E-mail :yujun@ 。

引用本文:于吉行, 俞俊, 薛晓雅, 等. 金属有机骨架UiO-66在催化领域的应用[J]. 化工进展, 2019, 38(s1): 144–151.Citation: YU Jihang, YU Jun, XUE Xiaoya, et al. Applications in the field of catalysis of metal organic framework UiO-66[J]. Chemical Industry and Engineering Progress, 2019, 38(s1): 144–151. ·144·化 工 进展DOI :10.16085/j.issn.1000–6613.2019–1106金属有机骨架UiO-66在催化领域的应用于吉行,俞俊,薛晓雅,韩颖,毛海舫,毛东森(上海应用技术大学化学与环境工程学院,上海 201418)摘要:金属有机骨架(MOFs )经过二十多年的快速发展,已经合成了成千上万种,然而MOFs 材料普遍具有较低的稳定性,在一定程度上限制了MOFs 的发展。

UiO-66的合成是MOFs 材料稳定性的一个突破,其在催化领域的发展尤为迅速。

本文首先介绍了理想及实际状态下UiO-66的结构特征,并说明了配体缺失导致的节点空位处的元素组成。

然后综述了利用UiO-66特殊的结构特征或将其功能化用于催化反应的研究,包括节点空位、功能化节点空位、负载金属纳米颗粒、功能化配体等。

铁死亡与胰腺癌的关系研究进展

铁死亡与胰腺癌的关系研究进展

铁死亡与胰腺癌的关系研究进展张辉1,冯俊凯1,赵凯1,马艳波21 山西医科大学第一临床医学院,太原030000;2 山西医科大学第一医院肝胆胰腺外科摘要:铁死亡是一种非凋亡性细胞死亡模式,其中心事件包括铁代谢异常、脂质代谢异常、脂质过氧化和质膜破裂等。

胰腺癌中铁死亡相关调控机制涉及铁死亡相关转录因子、自噬、免疫微环境。

铁死亡对胰腺癌的治疗也有影响,铁死亡失调常导致化疗耐药和治疗失败;使用纳米颗粒进行药物递送是癌症治疗的一个重要领域,近年来已经开发出许多纳米探针结合铁死亡疗法来进行抗肿瘤治疗;某些中药成分可促进铁死亡,从而发挥抗肿瘤作用。

关键词:胰腺癌;铁死亡;脂质过氧化doi:10.3969/j.issn.1002-266X.2023.19.022中图分类号:R735.9 文献标志码:A 文章编号:1002-266X(2023)19-0086-04胰腺癌发病率居我国男性恶性肿瘤第7位,居女性恶性肿瘤第11位[1]。

胰腺癌肿瘤微环境中,广泛纤维化、血管缺乏、免疫抑制和缺氧的基质环境,不仅促进肿瘤生长和侵袭,还使其对抗肿瘤药物产生耐受抵抗[2]。

因此患者预后较差,临床上迫切需要新的治疗方法来改善预后。

铁死亡是一种由细胞内微环境氧化扰动引发,受谷胱甘肽过氧化物酶4(GPX4)调控,可被铁螯合剂和亲脂性抗氧化剂抑制的非凋亡性细胞死亡模式[3],在神经变性、自身免疫疾病、恶性肿瘤等发生发展中起着重要的调节作用。

本文就铁死亡机制的最新进展以及充分利用铁死亡机制治疗胰腺癌的新策略进行综述,旨在为胰腺癌的临床治疗提供新的思路。

1 铁死亡中心事件铁死亡由铁代谢、脂质代谢异常、脂质过氧化和质膜破裂等中心事件组成[4]。

多不饱和脂肪酸的脂质过氧化在推动细胞铁死亡中起重要作用。

乙酰辅酶A合成酶长链家庭成员4与溶血磷脂酰胆碱酰基转移酶3是合成膜磷脂的关键酶,最后在脂肪氧合酶作用下生成脂质氢过氧化物。

铁死亡的活性氧(ROS)可由多种来源产生,如铁介导的芬顿反应、线粒体电子传递链等。

单个氢原子在金属钼中占位与迁移行为的计算机模拟研究

单个氢原子在金属钼中占位与迁移行为的计算机模拟研究

单个氢原子在金属钼中占位与迁移行为的计算机模拟研究摘要:氢原子的扩散与高性能材料金属钼的蠕变性等机械性能息息相关。

为进一步推进氢原子在金属钼中迁移性能的机理研究,并增加人们从微观尺度上对原子在晶格中的迁移行为的认识,本文应用第一性原理计算方法研究了氢原子在金属钼中的迁移扩散机理,首先计算了原子在钼超胞中的四面体间隙和八面体间隙中的结合能,得到间隙氢原子与钼超胞的结合能分别为-2.525V和-2.355V。

其次还计算了氢原子在各种迁移初始状态到最终状态需要越过的能垒,得到氢原子从八面体到八面体间隙、八面体到四面体间隙和四面体到四面体间隙的能垒分别为1.22eV、1.25eV和0.25eV。

结果表明氢原子更倾向于待在四面体间隙,氢原子在金属钼中的最有效扩散路径为四面体-四面体,迁移能垒为0.25eV。

关键词:间隙氢原子掺杂;钼;第一性原理;原子扩散1 研究背景钼的熔点高达2620℃,钼合金常用于托卡马克(tokamaks)核反应堆[1]的制造(一种环形型容器,采用磁约束实现受控核聚变)。

在托卡马克(tokamaks)核反应堆释放出的高能量、低原子数的原子会对合金材料产生冲击,对合金的耐久性影响巨大[2]。

钼具有优异的耐溅射腐蚀性能、良好的传热性能和优异的机械性能。

钼合金被认为是最有前途的等离子体表面材料之一[3]。

钼的应用领域也在不断扩大,并越来越多地应用于新兴材料。

点缺陷[4-5]对材料特性的影响是不言而喻的。

周立颖利用基于密度泛函理论的第一性原理计算了表面附近空位、和掺杂的形成能,以及它们对原子在该表面附近吸附和扩散的彩响[6],表明在掺杂体系中,原子更容易替代表面第2层原子的位置,且近邻吸附子的吸附能升高,原子从表面上到表面下层扩散的能垒分别显示出相对于干净表面,空位缺陷的形成使得原子在表面附近的扩散更加容易,而掺杂使得原子在表面上的扩散更加困难。

随着点缺陷理论研究方法逐渐成熟[7-9],可以深入研究材料的微缺陷结构和原子扩散机理,有助于进一步研究钼及合金的析出强化,相成核,生长动力学和老化强化机制。

有机合成(孟祥豹)ch5有机金属试剂

有机合成(孟祥豹)ch5有机金属试剂

Organometallic Compounds有机金属试剂有机金属试剂主族金属试剂:Li,Na, Mg, Cu, Zn, Cd过渡金属有机化合物:Pd,W,Mo,Ni,Sn稀土金属有机化合物: Sm,La,Yb,Ru,Rh,ScI. Concepts and principles Compounds with C-M bond. M = metalAs electrophilic reagents,attacked by nucleophilesAs nucleophilicreagents, attackelectrophiles Organometellic compoundsOrganometellic compoundsThe reactivity depends on the nature of the metal atom. Electropositive characterA. Preparation1. From metals and organic halides2. Metal-halogen exchangeSolventEquilibrium 利于形成与电负性更大的碳原子相连的有机金属试剂3. Metal-metal exchange4. Metalation of hydrocarbonsEquilibrium/ 利于形成含更小电正性金属的试剂A acidic C-H bond, formation a stable carbanionB. General reactions of organometallic compounds1. Substitution ( nucleophilic )2. Addition to double bondsNucleophiliesII. Organomagnesium compounds(Grignard reagents)♣1901, Grignard reagent was discovered; ♣1912, Nobel PrizeX = Cl, Br, IR = alkyl, aryl, alkenylPreparation:Order of reactivity: RI > RBr > RCl >> RF ♦Magnesium metal♦Alkyl halide: ♦Solvent: 乙醚, THF ,(丁醚, 异戊醚),甲基叔丁基醚⨯♦O 2, CO 2, H 2O should be rigorously excluded 1o RX > 2o RX > 3o RX♦反应的引发:碘或者CH 2Br 2♦反应的淬灭:氯化铵水溶液Vinyl halidesAcetylenic halidesAlkyl Chlorides Reactions of Grignard reagentsA. Formation of carbon-carbon bonds 1. Formation of Hydrocarbons 延长碳链烷基化卤代烃、磺酸酯、硫酸酯2. Formation of AlcoholsTertiary alcoholPrimary alcoholSecondary alcohol酮甲醛醛格氏试剂与醛酮的反应提供了一条由简单醇制备复杂醇的路线收率-----电性因素立体因素√Less bulky Grignard reagent is preferableAlternative methods for synthesizing alcoholsa. With acyl halides控制投料比,可控制产物的结构状态低温, 等当量投料立体位阻?b. With carboxylic esters3o 醇有两个相同烃基的醇甲酸酯对称的仲醇2o 醇六甲基磷酰胺HMPA有两个相同取代基的二醇c. With epoxide增加两个碳的醇不对称环氧化物3. Formation of Aldehydes原酸酯4. Formation of Ketones腈酰胺5. Formation of Caboxylic acids 与CO 2的反应B. Reaction at elements other than carbon1. Hydroperoxides 氢过氧化物2. Thiols过氧醇硫醇3. Sulfinic acids4. Alkyl Iodides烷基亚磺酸5. Amines6. Derivatives of phosphorus, boron, and siliconC. Some abnormal reactions of Grignard reagents1. Allylic and Benzylic Grignard reagentMajorminorAllyl Grignard reagentAllylic-type Grignard reagentReaction through six-membered cyclic transition stateBenzylic Grignard reagentsPyrrole2-position3-positionIndole2. 1,4 -Additionα, β-不饱和醛, 1,2-additionGrignard reagent, with a large bulky group1, 2-addition1,4-addition75%25%α, β-不饱和酮, 1,4-additionOrganic SynthesisA large bulky group in 4-positionA large bulky group in α-positionCu +, Cu 2+催化1,4-加成反应CuCl, Cu(OAc)2,CuCN3. Undesirable reactions of Grignard reagentDecomposition of Grignard reagentα-Hydrogen atomenolizationAs a baseReductionA hydrogen atom at β-carbonHydride-ion transferSix-memberedCyclic transition stateStereoselectivityMechanism of Grignard Reaction Barbier reactionIII. Organolithium compounds♦作为强碱;♦作为强的亲核试剂, 活性高于Grignard 试剂;♦发生一些不同于Grignard 试剂的反应Wurtz coupling reaction♦RX/Li干燥, 溶剂, 隔绝空气, 温度低温反应♦金属-卤素交换芳基、乙烯基卤代物♦锂-氢交换较强酸性的烃C-H键涉及有机锂试剂的实验装置RLi 过滤、转移装置反应装置无水溶剂蒸馏转移装置涉及有机锂试剂的实验装置B. ReactionsSimilar as the Grignard reagents, but more effective.The differences from Grignard reagentsLess readily prevented by steric hindrance from reacting at carbonyl groups.1. Reaction with Carbonyl Groups2. 1,2-addition , with unsaturated ketones1,4-addition1,2-addition3. Wurtz coupling 烃基取代反应4. Carbon dioxide 形成羧酸、酮的反应羧酸5. Addition to cyclic ether6. Reaction with Carboxylic DerivativesIV. Organocopper compoundsA. PreparationOrganocoper compoundsLithium organocuprates二烷基铜锂试剂R = alkyl, alkenyl, arylB. Reactions1. With alkyl halides较少重排、消除副反应2. Coupling reaction with Carbonyl halides形成酮,温和,收率较高3. Reaction with α-Bromo-ketones酮的α-烃化碱催化, 与卤代烃反应/ 消除, 缩合烷基铜锂试剂仅与卤代烃反应, 而不与醛酮羰基反应4. With α,β-unsaturated carbonyl compoundsReacts exclusively by 1,4-addition, Michael addition---------高度的区域选择性, 将烷基、芳基引入α、β-不饱和羰基化合物的β-位RMgBr: 1,2-and 1,4-additionRLi: 1,2-addition R2CuLi: 1, 4-additionCis-加成5. Addition to Epoxides反应条件温和,生成增加2个碳的醇;加成反应的位点α, β-不饱和环氧化物1, 4-additionTrans-addition活性顺序:酰氯> 醛> 环氧化物>RX>酮>酯>腈6. Copper(I) catalyzed formation of cyclopropanesA copper-carbene complex may be involved V. Organocadmium compoundsA. Preparation金属试剂与金属离子交换, 生成更稳定的金属试剂R = alkyl, aryl 反应活性比RMgX, RLi低, 毒性B. ReactionDo not react with ketones and esters.分子中引入酮基, 对其它功能团没有影响VI. Organozinc compounds A. Preparation1. With acyl chlorideB. ReactionsKetones2. With aldehydes and ketonesReformatsky reaction3. With nitriles4. The Simmons-Smith reactionCarbenoidZinc-copper alloyVII. Organonickel compoundsA. PreparationThe 3-allyl complex dimerizationAllyl halideB. ReactionsCoupling reaction with alkyl halidesDihydrocoumarinsTerpenesB. ReactionsVIII. Organoferric compoundsA. PreparationCollman’s reagentCarbonyl complexSynthesis of cyclic ketonesFerrocene二茂铁。

构筑手性金属有机骨架的方法及其在不对称催化中的应用

构筑手性金属有机骨架的方法及其在不对称催化中的应用

构筑手性金属有机骨架的方法及其在不对称催化中的应用刘丽丽;台夕市;刘美芳;郭焕美;晁明珠【期刊名称】《化工进展》【年(卷),期】2015(000)004【摘要】手性金属有机骨架(MOF)具有独特的结构、不对称催化和手性拆分等性能,引起了催化学者的极大重视。

系统地介绍了国内外有关手性MOF的合成方法,即:①非手性物质在晶体生长过程中自组装;②使用手性化合物来诱导合成;③通过手性有机基团与金属离子配位将手性成分嵌入金属有机骨架;④表面修饰的方法,第3种方法是最常用的合成手性MOF的方法。

重点阐述了近年来手性MOF在不对称催化领域的最新研究成果,希望能为手性MOF研究者设计、合成更优良的手性MOF催化剂提供参考。

未来手性MOF催化的主要目标在于合成性能更加高效、稳定的新型手性MOF催化剂,并应用于大规模工业生产中,在温和条件下实现较高的转化数和对映体选择性。

%Chiral metal-organic frameworks (MOFs) have attracted growing interest for their potential use in asymmetric catalysis and chiral separation,and on a more basic level,have called for the creation of new topologies in inorganic materials over the past few years. The synthesis methods of chiral MOF arediscussed,includingⅠself-assembly based on achiral organic ligands;Ⅱ synthesis by chiral template;Ⅲ synthesis by chiral ligands;Ⅳ post-synthesis modification. “Synthesis by chiral ligands” is widely used in creating chiral MOFs. Accordingly,some applications of various chiral MOFs as catalysts are elaborated,hoping to offer some help to the designer of chiralMOFs. Usually as an asymmetric catalyst,chiral MOFs are capable of being very active for many reactions, such as epoxidation and Aldol reaction. The future main objective of chiral MOFs catalysis is to synthesize more excellent chiral MOF catalysts and be used in large-scale industrial production, achieving higher enantioselectivity and larger turn-over number under mild conditions.【总页数】10页(P997-1006)【作者】刘丽丽;台夕市;刘美芳;郭焕美;晁明珠【作者单位】潍坊学院化学化工与环境工程学院,山东潍坊 261061;潍坊学院化学化工与环境工程学院,山东潍坊 261061;潍坊学院化学化工与环境工程学院,山东潍坊 261061;潍坊学院化学化工与环境工程学院,山东潍坊 261061;潍坊学院化学化工与环境工程学院,山东潍坊 261061【正文语种】中文【中图分类】O643.3;O627【相关文献】1.不对称催化氢化反应中立体选择性探讨--在均相不对称催化氢化反应中,催化剂的手性膦配体结构对立体选择性的影响 [J], 刘跃发2.手性金属有机骨架(CMOF)在不对称催化方面的应用 [J], 曾庆兰; 郑兴莉; 尹晓刚3.C2-对称面手性RuPHOX-Ru催化的不对称氢化反应及其在手性药物合成中的应用 [J], 李万亮4.噻唑烷类手性配体在催化不对称硅氢化反应中的应用Ⅲ.高分子酮的催化不对称硅氢化反应 [J], 姚金水;周立国;李弘;何炳林5.手性二茂铁基β-氨基醇的合成及其在催化硼氢化钠/碘对潜手性酮的不对称还原反应中的应用 [J], 时憧宇;杜玲枝因版权原因,仅展示原文概要,查看原文内容请购买。

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ZDD and a fragment of RAG1 including only the RING finger sequence have been expressed in E. coli as fusion proteins with maltose binding protein (MBP). These proteins are referred to as MBP-ZDD and MBP-RF, respectively. We have recently described the cloning, expression, and purification of MBPZDD and MBP-RF. In addition, the proteolytic cleavage of the MBP-ZDD chimera to generate the ZDD fragment, and its subsequent purification, was done as previously reported [5]. N-terminal amino acid sequencing was done at the W.M. Keck Foundation Biotechnology Resource Laboratory, and electrospray mass spectrometry was done by Walter McMurray at the Yale University School of Medicine. The Zn2-coordinated form of ZDD (Zn 2-ZDD) was produced by dialysis of the native ZDD against nitrogen-saturated 20 mM Tris-HCl (pH 7.5), 100 mM NaCl, 5 mM 2-mercaptoethanol (BME), and 1 mM EDTA at 4˚C for 17 hours. The Zn2-Cd1 form of ZDD was generated by dialysis of Zn2-ZDD against nitrogen-saturated 20 mM Tris-HCl (pH 7.5), 100 mM NaCl, 5 mM BME supplemented with one molar equivalent of CdCl2 at 4˚C for 12 hours. The metal to protein stoichiometry was determined by atomic absorption spectroscopy using an Instrumentation Laboratory IL157 spectrometer. The concentration of metal ions in the RAG1 proteins was measured in solutions of 3 to 10 µM protein. These were compared to either a Zn or Cd calibration curve ranging from 1 to 15 µM, which was measured prior to each protein sample.
B.
Circular Dichroism Spectroscopy
Circular dichroism (CD) spectra were collected on an AVIV model 62DS spectropolarimeter using a 0.2 mm path length cell. Protein samples were dialyzed against buffer containing 20 mM sodium phosphate (pH 7.0), 50 mM NaCl, 1mM BME. Five separate spectra with a step size of 0.5 nm and a 1.5 nm bandwidth were averaged to obtain the final spectrum for each protein sample. The temperature during the scans was maintained at 25˚C with a water-jacketed cuvette holder. The molar ellipticity was determined using protein concentrations obtained from amino acid analysis. Thermal denaturation studies were done by collecting data at a single wavelength and increasing the temperature in 1˚C increments, equilibrating for 60 sec, and using a 30 sec signal integration time. The melting temperatures (Tm) were determined from the temperature at which the slope of the first derivative of the data was at a minimum.
I. Introduction
Structural zinc-binding domains are often characterized by the requirement of zinc coordination for proper protein folding [1]. One specific class of zinc-binding motif that will be discussed here is the zinc C3HC4 motif, also known as the RING finger [2]. To date at least eighty proteins include a sequence of approximately 50 residues consistent with a RING finger motif. This conserved sequence, with minor variations in some cases, is defined as follows: C-X2-C-loopI-C-X-H-X2-C-X2-C-loopII-C-X 2-C, where X represents any amino acid. A common function attributable to the RING finger module has remained elusive, although a role in protein-protein interactions has been speculated [2]. One of the first RING finger sequences was identified in RAG1, a protein expressed in developing lymphocytes by recombination activating gene-1 [3]. RAG1, along with RAG2, is an essential component of the V(D)J recombination reaction, which produces the genetic sequence encoding for the variable regions of the T cell receptor and immunoglobulin chains. Briefly, V(D)J recombination is accomplished via selection and assembly of gene segments known as variable (V), joining (J), and sometimes diversity (D) in an ordered and precisely regulated process (for a review see [4]). The RING finger sequence of RAG1 is present within the N-terminal third of the protein, which contains a total of 1040 residues in the murine form. Besides the RING finger sequence, we have recently identified the presence of two C2H2 zinc finger sequences within RAG1 [5]. A domain in RAG1 containing one of the zinc finger modules plus the RING finger forms a highly specific dimer, as characterized by a variety of biophysical techniques [5]. The dimerization of this zinc-binding domain provides further support for the participation of RING fingers in protein-protein interactions. This dimerization domain of RAG1, previously referred to as R121, will be referred to here as ZDD, zinc-binding dimerization domain. Here we focus on the role of metal binding to the ZDD dimer. In particular, we have investigated the stabilities of different species of ZDD with varying metal-to-protein stoichiometries. Combined with the metal-binding studies, we have further investigated dimer
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