Effect of cerium addition on microstructure and texture of aluminum foil for electrolytic capaci
Simulation of Microstructure Evolution

0.02
0.04 0.06
0.08
0.10
Microsegregation Pattern
C
Cr
MC
η
Fe
Nb
Ti
Laves
Experiment / Simulation Microsegregation and γ' precipitation in Ni-Cr-Al-Ta-W:
experiment
nucleation undercooling determined to ∆T=220K
A.Burtsev et al., EMRS proceedings (2002) M.Apel et al., Solar Energy Materials & Solar Cells 72 (2002) 201
Theoretical background: The phase field method
Multi-Phase Field Model Phase field equations
& φα = ∑ µαβ σ αβ α ,β π π2 2 2 φα φβ ∆Gαβ φβ ∇ φα − φα ∇ φβ + 2 φα − φβ + 2η η
Eutectic Fibres
NiAl-W
binary model
e.g. M.Apel et al., Journal of Crystal Growth 237-239 (2002) p. 154-158
Lamellar Eutectic Growth: Ternary alloy Al-Ag-Cu
e.g.G.Parieser et al, Steel research 72(2001) p.355
可降解锌基骨植入材料及其表面改性研究进展

第53卷第2期表面技术2024年1月SURFACE TECHNOLOGY·1·研究综述可降解锌基骨植入材料及其表面改性研究进展冯博玄1,谭晋韵2,裴佳1,袁广银1*(1.上海交通大学 轻合金精密成型国家工程研究中心和金属基复合材料国家重点实验室,上海 200240;2.复旦大学附属华山医院,上海 200040)摘要:医用锌及锌合金有望成为新一代可降解骨植入物材料来促进骨缺损的修复。
概述了可降解医用锌基材料的优势,包括较好的生物安全性和抗菌效果、能促进植入部位周围血管和新骨的生成以及骨相关基因的表达能力。
在此基础上,从基底材料、细胞种类及实验结果等方面系统总结了近年来关于可降解医用锌基材料生物相容性和降解行为的研究。
同时,归纳了可降解医用锌在临床修复骨缺损方面所面临的主要问题和挑战,包括较差的力学性能和较强的细胞毒性。
可降解医用锌较差的力学性能可以通过合金化进行改善,概述了多种新型医用锌合金的力学性能及其生物相容性。
表面改性是提高可降解医用锌基表面生物相容性和调控降解的有效手段。
从基底样品、表面改性手段、使用的细胞或动物模型以及细胞相容性和降解行为等方面,综述了近年来可降解锌基骨植入材料表面改性的研究现状,提出了可降解锌基骨植入材料表面改性目前所面临的难点问题,包括传统表面改性手段加剧了锌离子的释放或在表面改性后可降解医用锌的生物相容性改善功效不足,以及未来的发展方向。
关键词:可降解医用锌;骨植入材料;生物相容性;降解行为;表面改性中图分类号:O61;O62;Q25 文献标志码:A 文章编号:1001-3660(2024)02-0001-14DOI:10.16490/ki.issn.1001-3660.2024.02.001Research Progress of Biodegradable Zinc-based OrthopedicImplant Materials and Their Surface ModificationFENG Boxuan1, TAN Jinyun2, PEI Jia1, YUAN Guangyin1*(1. National Engineering Research Center of Light Alloy Net Forming & State Key Laboratory ofMetal Matrix Composite, Shanghai Jiao Tong University, Shanghai 200240, China;2. Huashan Hospital Affiliated to Fudan University, Shanghai 200040, China)ABSTRACT: In recent years, biodegradable metals, represented by magnesium (Mg), zinc (Zn), and iron (Fe), have received extensive attention from the biomedical and materials fields both domestically and internationally. This article outlined the requirements for ideal bone implant materials, and the advantages of biodegradable metals over other biodegradable materials, including mechanical performance, degradation performance, and biocompatibility. In addition, the degradation mechanism of biodegradable metal materials was summarized. Among them, Mg had been extensively investigated, but its rapid degradation rate lead to compromised mechanical properties and uncontrolled hydrogen evolution. Conversely, the degradation rate of Fe收稿日期:2023-01-04;修订日期:2023-02-25Received:2023-01-04;Revised:2023-02-25基金项目:国家自然科学基金(52130104,51971141);科技部重点研发专项(2021YFE0204900,2018YFE0115400)Fund:National Natural Science Foundation of China (52130104, 51971141); the National Key Research and Development Program of China (2021YFE0204900, 2018YFE0115400)引文格式:冯博玄, 谭晋韵, 裴佳, 等. 可降解锌基骨植入材料及其表面改性研究进展[J]. 表面技术, 2024, 53(2): 1-14.FENG Boxuan, TAN Jinyun, PEI Jia, et al. Research Progress of Biodegradable Zinc-based Orthopedic Implant Materials and Their Surface Modification[J]. Surface Technology, 2024, 53(2): 1-14.·2·表面技术 2024年1月was notably sluggish, approaching that of non-degradable materials. Zn and Zn alloys, due to their moderate degradation rate, good mechanical properties, and biological safety, were expected to become a new generation of biodegradable bone implant materials to promote bone defect repair. This article summarized the advantages of biodegradable Zn-based materials, including biological safety, antibacterial effects, and the ability to promote the generation of blood vessels and new bone around the implant site, as well as to promote the expression of bone-related genes. Based on this, recent research on the biocompatibility and degradation behavior of biodegradable Zn-based materials was systematically summarized from the aspects of substrate materials, cell types, and experimental results. At the same time, the main problems and challenges faced by the clinical application of biodegradable Zn for repairing bone defects were summarized, including poor mechanical properties and strong cytotoxicity. The poor mechanical properties of biodegradable Zn could be improved through alloying. This article outlined the mechanical properties and biocompatibility of various new medical Zn alloys. The potent cytotoxicity of biodegradable Zn used in medical applications arose from the local accumulation of Zn2+ ion generated during degradation. Zn2+ ion was reported to exhibit biphasic effect on cells. The low concentration of Zn2+ ion could promote the cell adhesion, proliferation, and differentiation. In contrast, the local high concentration of Zn2+ ion resulted from the rapid degradation rate of Zn implants at the initial stage of implantation, and some degradation products such as ZnO and Zn(OH)2 with poor biocompatibility always lead to cytotoxicity and inflammation surrounding the Zn implants, further delaying the regeneration and repair of bone defects. Zn still exhibited slight cytotoxicity after alloying, and surface modification was an effective means to improve the surface biocompatibility and regulate degradation of biodegradable Zn. This article reviewed the current research status of surface modi-fication of biodegradable Zn-based bone implant materials from the aspects of substrate samples, surface modification methods, cell or animal models used, and cell compatibility and degradation behavior, and proposed the current difficulties and future development directions of surface modification of biodegradable Zn-based bone implant materials. Surface modification of biodegradable Zn is still nascent, and there are scarce relevant studies with restricted advancement in the biocompatibility of biodegradable Zn. Traditional surface modification methods have increased the release of Zn2+ ion, resulting in higher cyto-toxicity. Alternatively, the efficacy of improving the biocompatibility of biodegradable Zn through surface modification has been insufficient. The future research direction of biodegradable Zn-based materials should focus more on surface modification methods such as phosphate and its composite coatings, as well as biodegradable polymer coatings.KEY WORDS: biodegradable zinc; bone implant material; biocompatibility; degradation behavior; surface modification每年由机械外伤导致的骨折、由炎症引发的骨组织坏死、由骨肿瘤引起的骨缺损等疾病的患者有数百万人[1-3]。
细胞培养用青霉素-链霉素产品说明书

细胞培养用青霉素-链霉素产品简介:细胞培养用青霉素-链霉素(Penicillin-Streptomycin for Cell Culture)为粉剂,是最常用的细胞培养用抗生素(即通常所谓的双抗)。
在细胞培养液中推荐的青霉素的工作浓度为100U/ml ,链霉素的工作浓度为0.1mg/ml 。
一个包装的细胞培养用青霉素-链霉素可以配制80L 细胞培养液。
保存条件:室温保存。
4ºC 保存可以使用更长时间。
注意事项:开瓶后需防止受潮。
本产品仅限于专业人员的科学研究用,不得用于临床诊断或治疗,不得用于食品或药品,不得存放于普通住宅内。
为了您的安全和健康,请穿实验服并戴一次性手套操作。
使用说明:细胞培养用青霉素-链霉素可以参考如下两种方法之一使用:1. 配制细胞培养液时加入细胞培养用青霉素-链霉素,然后再过滤除菌:配制细胞培养液时按照青霉素的工作浓度为100U/ml ,链霉素的工作浓度为0.1mg/ml 进行配制,配制完成后过滤除菌即可使用。
2. 配制青霉素-链霉素溶液(100X)母液,然后再添加到细胞培养液中:按照青霉素的含量为10KU/ml ,链霉素的含量为10mg/ml ,配制青霉素-链霉素溶液(100X)母液。
过滤除菌后即可按照100倍稀释加入到细胞培养液中使用。
配制的母液可以-20ºC 冻存。
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《废铅酸蓄电池回收技术规范》发布

68张文博等:钵基氧化物涂层的制备与研究进股2019年第4期[4] E.Carlos,Castano,J.Matthew,et al.Cerium-based oxide coatings[j].Curr.Opin.Solid.St.M..2015,19:69-76.[5]Gorte R J.Ceria in catalysis:From automotive applications to thewater-gas shift reaction[J].AIChE journal,2010,56(5):1126-1135.[6]Harvey T G.Cerium-based conversion coatings on aluminium alloys:a process review[J].Corrosion Engineering,Science and Technology,2013,48(4):248-269.[7]Fahrenholtz W G,O'Keefe M J.Zhou H,et al.Characterization ofcerium—based(*onversion coatings for corrosion protection of aluminum alloys]J].Surface and coatings Technology,2002,155(2-3):208-213.[8]Heller D K,Fahrenholtz W G,O'Keefe M J.The effect of post-treatment time and temperature on cerium-based conversion coatings on Al2O24-T3[J].Corrosion Science,2010,52(2):360-368.[9]Castano C E,Maddela S,O'Keefe M J,et al.A comparative study onthe corrosion resistance of cerium-based conversion coatings on AZ91D and AZ31B magnesium alloys[J].ECS Transactions,2012, 41(15):3-12.[10]X.Cui,Y.Yang,et al.Corrosion behaviors in physiological solutionof cerium conversion coatings on AZ31magnesium alloy|J].Appl.Surf.Sci.,2011,257:9703-9709.[11]W.F.Ng,M.H.Wong,F.T.Cheng.Cerium-based coating for enhancing the corrosion resistance of bio—degradable Mg implants[J].Mater.Chem.Phys.,2010,119:384-388.[12]Castano C E,O'Keefe M J,Fahrenholtz W G.Microstructural evolution of cerium-based coatings on AZ31magnesium alloys|J.Surface and Coatings Technology,2014.246:77-84.[13]J.H.Park,W.S.Kim,D-H Jo,et al.Effect of Ce conversion underlayer coating on the photo-catalytic activity of TiO2sol-gel?lm deposited on hot-dip GI[J].J.Ind.En.g Chem.,2014,20:1965-1972.[14]P.Ji.J.Zhang,F.Chen,et al.Ordered mesoporous CeO2synthesized by nanocasting from cubic Ia3d mesoporous MCM-48silica:formation,characterization and photocatalytic activity[J..J.Phys.Chem.,200&112:17809-17813.[15J H.Gao,B.Qiao,T-J.Wang,et al.Cerium oxide coating of titaniumdioxide pigment to decrease its photocatalytic activity[J].Ind.Eng.Chem.Re.,2014,53:189-197.[16]Y.Chen,C.Qiu,C.Chen,et al.Facile synthesis of ceria nanospheres by Ce(OH)CC)3precursors[J].Mater.Lett.,2014.122:90-93.L17]S.Yabe,T.Sato.Cerium oxide for sunscreen cosmetics[J].J.Solid.State.Chem.,2003,171:7-11.[18]N.Iman a ka,T.Masui,H.Hirai,et al.Amorphous cerium-titaniumsolid solution phosphate as a novel family of band gap tunable sunscreen materials[j].Chem.Mater.,2003,15:2289-2291.[19]I.M.Allam,D.J.Rowcliffe.A dip process for thermal barrier coating on superalloys[J j.Thin Solid Films,1993,100:25-32.[20]X.Q.Cao,R.Vassen,D.Stoever.Ceramic materials for thermalbarrier coatings[J.J.Eur.Ceram.Soc.,2004,24:1-10.[21]J.Hierso,P.Boy,K.Vail6,et al.Nanostructured ceria based thin?lms(61lm)as cathode/electrolyte interfaces[J].J.Solid.Stat.eChem.,2013,197:113-119.[22]S.Suda.Nanocomposite glass abrasives L J J■J-Ceram.Soc.Jpn.,2014,122:244-249.[23]S-H.Lee,Z.Lu,S.V.Babu,et al.Chemical mechanical polishingof thermal oxide?Ims using silica particles coated with ceria[J].J.Mater.Res.,2002,17:2744-2749.[24]M.Femandez-Garcia,A.Martinez-Arias,J.C.Hanson.Nanostructured oxides in chemistry characterization and properties[j j.Chem.Re.,2004,104:4063-4104.[25]G.Zhang,Y.Guo,L.Lu,Z,et al.Synthesis and characterization ofCeOo thin film with well-ordered step edges[J].Mater.Lett.,2014,125:162-166.[26]Y.Yang,X.Du,Y.Chen,et al.Influences of the main anodic electroplating parameters on cerium oxide film[j」.Appl.Surf.Sci.,2014,305:330-336.[27]M.Vorokhta,1.Matol f nov6,M.Dubau,et al.HAXPES study ofCeO x thin?lm-silicon oxide interface[J].Appl.Surf.Sci.,2014,303:46-53.[28]S.Van Steenberge,W.P.Leroy,Depla D.Influence of oxygen?owand film thickness on the texture and microstructure of sputteredceria thin films[J].Thin.Solid.Films.,2014,553:2-6.《废铅酸蓄电池回收技术规范》发布记者8日从国家市场监督管理总局获悉:国家市场监督管理总局、国家标准化管理委员会日前批准发布《废铅酸蓄电池回收技术规范》。
2019年武汉理工大学材料学院博士研究生招生入围考试考生信息公示汇总表

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technology . 87:(1)83-94 (一作,JCR一区)2018.6
1.Nonhalogen Solvent-Processed Asymmetric Wide-
是
Bandgap Polymers for Nonfullerene Organic Solar Cells with Over 10% Efficiency, Adv. Funct. Mater, 2018, 28,
1049799924
全日制 非定向
天津科 技大学
高分子材 料与工程
武汉理 工大学
材料工程
戴红莲
武汉理工大学、 朱楚洪,
陆军军医大学基础医
学院
1.High energy storage properties and dielectric behavior
of (Bi0.5Na0.5)0.94Ba0.06Ti1-x(Al0.5Nb0.5)xO3 lead-
全日制 非定向
山东科 技大学
材料化学
山东科 技大学
材料加工 工程
韩颖超
王忠卫、曾荣昌 (山东科技大学)
nthanum magnesium hexaluminate thermal cycling lifetime
and CMAS corrosion behaviour,CERAMICS
INTERNATIONAL,2018年7月(一作,JCR一区)
2.Deposition and characterization of WC-Co hard-metal
coatings by high velocity oxy-fuel process combined with dry-
是(符合在国际重
氮氩比对模具钢表面镀CrAlN薄膜形貌和性能的影响

第51卷 第1期 表面技术2022年1月 SURFACE TECHNOLOGY ·105·收稿日期:2021-01-25;修订日期:2021-05-31 Received :2021-01-25;Revised :2021-05-31基金项目:湖北省教育厅科学技术项目(Q20181802)Fund :Supported by the Scientific Research Project of Education Department of Hubei Province (Q20181802) 作者简介:付泽钰(1996—),男,硕士研究生,主要研究方向为金属材料的表面处理。
Biography :FU Ze-yu (1996—), Male, Postgraduate, Research focus: surface treatment of metallic metaerials. 通讯作者:王天国(1978—),男,博士,教授,主要研究方向为表面工程技术和材料。
Corresponding author :WANG Tian-guo (1978—), Male, Doctor, Professor, Research focus: surface engineering technologies and materials. 引文格式:付泽钰, 王天国. 氮氩比对模具钢表面镀CrAlN 薄膜形貌和性能的影响[J]. 表面技术, 2022, 51(1): 105-112.FU Ze-yu, WANG Tian-guo. Effect of the Ratio of Nitrogen and Argon on the Microstructure and Properties of CrAlN Film Deposited on Die Steel Surface[J]. Surface Technology, 2022, 51(1): 105-112.氮氩比对模具钢表面镀CrAlN 薄膜形貌和性能的影响付泽钰,王天国(湖北汽车工业学院 材料科学与工程学院,湖北 十堰 442002)摘 要:目的 提高H13模具钢的表面性能,延长模具使用寿命。
霍夫梅斯特效应 超分子水凝胶的机械强度
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Tian-2012-Controlled synthesis
Applied Surface Science 258 (2012) 8431–8438Contents lists available at SciVerse ScienceDirectApplied SurfaceSciencej o u r n a l h o m e p a g e :w w w.e l s e v i e r.c o m /l o c a t e /a p s u scControlled synthesis of ZnO hollow microspheres via precursor-template method and its gas sensing propertyYu Tian a ,Jinchai Li b ,Hui Xiong a ,Jiangnan Dai a ,∗a Wuhan National Laboratory for Optoelectronics,College of Optoelectronic Science and Engineering,Huazhong University of Science and Technology,Wuhan 430074,China bKey Laboratory of Artificial Micro-and Nano-structures of Ministry of Education and School of Physics and Technology,Wuhan University,Wuhan 430072,Chinaa r t i c l ei n f oArticle history:Received 9October 2011Accepted 17December 2011Available online 26 December 2011Keywords:Gas sensor ZnOThermal evaporation Precursor template Ethanol sensinga b s t r a c tUsing Zn powder as precursor templates,ZnO hollow microspheres were successfully prepared by ther-mal evaporation method and characterized by X-ray diffraction analysis,scanning electron microscope and transmission electron microscope.It was found that different size and shape of precursor resulted in different ZnO nanostructures.When varying experimental conditions,such as air flow rate and working pressure,ZnO hollow spheres with different surface morphologies could be obtained.The advantages of the present synthetic technology are simple,relatively low cost,and high reproducibility.A gas sensor was fabricated from the as-prepared ZnO hollow microspheres and tested to the ethanol gas at different operating temperatures.© 2012 Published by Elsevier B.V.1.IntroductionControlled synthesis of semiconductor nanostructures in terms of size and shape has been strongly motivated and novel applica-tions can be investigated dependent on their structural properties [1–4].Among various semiconductor nanostructures,variety of nanostructures of ZnO has been investigated presenting it as richest family of nanostructures.ZnO has been extensively studied in vari-ous applications,including field-effect transistor [5],optical device [6],dye-sensitized solar cell [7],solid-state gas sensor [8]and so forth.Among these applications of nanostructured ZnO material,one of the most important applications is solid-state gas senor.ZnO is particularly applicable to gas sensors because of its typical prop-erties such as resistivity control over the range 10−3to 10−5cm,high electrochemical stability,absence of toxicity,and abundance in nature [8].ZnO sensors have many advantages such as low-cost and facile synthesis procedure compared to other materials [9].Generally speaking,ZnO gas sensors have been fabricated in the form of powders,pellets,thick and thin films.At present,numerous efforts have been paid to the synthesis of nanostructured ZnO such as nanorods [10],nanobelts [11],nano-tubes [12],nanocrystalline [13],flower-like microstructure [14],and twinned tabour-like structure [15]for gas sensor application.It has been shown that ZnO nanostructures can detect ethanol vapor [16–18],NO 2[11,19],H 2[11],NH 3[10],humidity [20],oxy-gen [21]and other gases.As ZnO gas sensor belongs to surface∗Corresponding author.Tel.:+862787793024;fax:+862787792735.E-mail address:daijiangnan@ (J.Dai).resistance control sensors,its sensitivity depends greatly on the surface microstructure,high surface area and permeable shell structure are thought to be good for electron depletion and effec-tive gas diffusion,therefore,sensing materials with hollow-sphere structure or porous shell structure would be good choice to increase the gas-sensing properties [22–24].To obtain such microstructures,synthesis methods always suffer from high temperature,expen-sive substrates,high cost,need of sophisticated equipments and rigorous experimental conditions.In this work,we mainly report on the preparation,characteriza-tion and sensing properties of ZnO hollow microspheres templated by Zn microspheres.And the effects of the size and shape of pre-cursor,air flow rate and working pressure on surface morphology of ZnO hollow spheres have been scrutinized in detail.In addition,their ethanol gas sensing study has also been carried out at var-ious operating temperatures and is found to be good gas sensing performance for detecting ethanol gas.2.Experimental2.1.Synthesis and characterization of the nanofibersIn our experiments,the preparation of Zn powder precursor template has been described in detail in our previous works [25,26].The shape and size of zinc powder precursor could alter in the synthesis process.ZnO nanostructures were synthesized via a sim-ple chemical vapor deposition process.The Si wafers were first covered with a thin layer of zinc particles to serve as substrates.Synthesis of the ZnO hollow microspheres and other nanos-tructures were performed in a quartz tube installed inside a0169-4332/$–see front matter © 2012 Published by Elsevier B.V.doi:10.1016/j.apsusc.2011.12.0908432Y.Tian et al./Applied Surface Science 258 (2012) 8431–8438Fig.1.(a)Schematic diagram of the experimental setup,(b)different Zn powder precursor template,(b 1):small size Zn powder,(b 2):flake-shaped Zn powder,(b 3):spherical Zn powder.conventional horizontal tube furnace,shown schematically in Fig.1a.The SEM images of zinc powder precursor with different shape and size have been shown in Fig.1b.Thereinto,Zn particles in Fig.1b 1possess of small size ranged of 30–80nm purchased from Sheenbow Trading Company Ltd in Guangzhou of China.Fig.1b 2shows the flake-shaped Zn powder particle mechanically deformed via a ball-milling process,Fig 1b 3shows the Zn microspheres.For the ZnO nanostructures growth,2g zinc powder (purity of ∼99.99%)and Si substrates with Zn precursor were located in a quartz boat,in which the substrates was located downstream 5mm away from the zinc source.The quartz boat was placed at the cen-ter region of the furnace.After the quartz tube was evacuated by a mechanical rotary pump,the central region of the furnace was heated to a settled temperature of 400◦C with a increasing rate of 10◦/min.High-purity Ar and air gases whose flow rates were sepa-rately controlled by two flowmeters at Ar 50sccm and air 80sccm,were introduced into the inner quartz tube.The synthesis process was carried out under the pressure of 20Pa and the temperature of the furnace was maintained at 465◦C for 60min.The power was then switched off,and then the furnace was allowed to cool.In this synthesis process,the substrate temperature,air flow and working pressure could alter in the synthesis process.2.2.Structure characterization techniquesThe surface morphologies of the products were characterized by Sirion FEG scanning electron microscopy (SEM,JEOL JSM 6700F at 10kV)equipped with energy dispersive X-ray spectroscopy (EDS).The chemical analyses of the products were investigated using D8advanced X-ray diffraction (XRD).The structures of the products were investigated by JEOL JEM 2010transmission elec-tron microscopy (TEM)and high-resolution transmission electron microscopy (HRTEM).2.3.Sensor fabrication and measurementsA proper amount of ZnO hollow spheres were slightly grinded together with several drops of water in an agate mortar.The formed slurry was coated onto an alumina tube with a diameter of 1mmand length of 4mm,being positioned with a pair of Au electrodes and four Pt wires on both ends of the tube.A Ni-Cr alloy coil through the tube was employed as a heater to control the oper-ating temperature by tuning the heating voltage.Gas sensing tests were performed by a WS-30A gas sensing measurement system (WeiSheng Electronics Science and Technology Co.,Ltd.,Henan Province,China).WS-30A is a static system using atmospheric air as the interference gas.Test gases with calculated amount are intro-duced into the test chamber by a syringe.Two electric fans installed in the chamber are used to make test gas homogeneous.After test,the chamber was removed for test gases to diffuse away.The sen-sor response to ethanol is defined as Ra/Rg,where Rg is the sensor resistance in a target gas and Ra is the sensor resistance in air,respectively.3.Results and discussionFig.2shows typical SEM images of three kinds of ZnO products grown with different shape and size Zn precursor.Sample 1(shown in Fig.2a 1and a 2),prepared by Zn nanoparticle (size:30–80nm)as precursor template,is chain-like ZnO structures.The length of these chains is about several micrometers.From the enlarged image,it is found that these chains are composed of many rhombus-like particles and the size of rhombus-like particle is about 100nm (inset in Fig.2a 2).And some nanorods are present among these chains;it is possibly that the rhombus-like particles grow too big to link together.Sample 2(shown in Fig.2b 1and b 2),prepared by flake-shaped Zn powder as precursor template,is flake-shaped ZnO structures,and there are well-aligned thin and short nanorods (diameter:about 40nm)growing on the surface of flake-shaped structure.The well-defined ZnO hollow microspheres can be clearly observed in Fig.2c 1and c 2(Sample 3),which is prepared by Zn microspheres as precursor template.It shows that most of the microspheres are partially broken,and many more are hollow or have porous holes.It can be seen that a large number of ZnO micro-spheres with a diameter distribution ranging in 5–22m and an average diameter of 14m exist on Si substrates.The diameters of these hollow microspheres are distinctly bigger than those of Zn microspheres.ZnO microsphere comprises numerous nanowiresY.Tian et al./Applied Surface Science258 (2012) 8431–84388433Fig.2.SEM images of ZnO samples prepared by using different Zn powder as precursor template at465◦C in1h,(a1and a2)ZnO nanostructures using small Zn powder as precursor template which the size range in30–80nm;(b1and b2)ZnO nanostructures usingflake-shaped Zn powder particle as precursor template;(c1,c2)hollow ZnO spheres using spherical Zn powder as precursor template.Thereinto,a2,b2and c2are the enlarged images of a1,b1and c1.pointing toward the center of microsphere on the outer and inner surfaces.The diameter and length of these nanowires are in the ranges of40–60nm and1.5–2m,respectively.It clearly imply that Zn precursor plays an important role to the synthesis of ZnO hol-low microspheres.And changing the shape and size of precursors could alter thefinal product morphology when all other processing parameters are kept the same.If there no using precursor-template on the Si wafers,only nanorods are present[25].The XRD patterns of three products are shown in Fig.3.It is found that all as-prepared samples are highly crystalline,and the diffraction peaks in every pattern can be indexed as the pure hexag-onal wurtzite ZnO structure with calculated lattice constants of about a=0.325nm and c=0.521nm.No peaks due to impurities are detected,indicating that all zinc powder precursors(thin layer on the Si substrate)have been thoroughly oxidized as pure ZnO during the reaction.The strong intensity of the(0002)peak indicates that the ZnO structures have preferential growth direction along the c-axis orientation.From the image,the intensity of the(0002)peaks about the three samples is enhanced from c to a,showing growth direction along the c-axis orientation of the sample1that has more preferential than those of the sample2and3.TEM was used to investigate the structure of the ZnO nanowires on the surface of the hollow microsphere synthesized at465◦C (Fig.2c2)in more detail.The TEM images in Fig.4a and b show that the wire is crystalline.Also,the SAED patterns of the ZnO structure (insets of Fig.4a)conform that they have crystalline growth along the[0001]direction.The HRTEM image in Fig.4b,with a lattice spacing of about0.26nm,is consistent with the lattice spacing for the(0002)plane of wurtzite ZnO.To explore the growth mechanism of the hollow ZnO micro-spheres,a series of experiments were performed in detail.To minimize the number of parameters affecting the ZnO hollow8434Y.Tian et al./Applied Surface Science 258 (2012) 8431–8438Fig.3.XRD patterns of obtained products a,b and c corresponding to the SEM images in Fig.2.microspheres,when altering one experiment parameter,all the other experiment parameters were kept constant.In each exper-iment,the spherical Zn powder particles were used as precursor template.At first,we have investigated the effect of growth temper-ature on surface morphology of the ZnO hollow microsphere [26].It is found that the increase in growth temperature transformed surface morphology from nanowires to club-shaped nanorods and nanograins.It showed that the growth temperature is another important factor on tailored surface morphology of ZnO hollow microsphere.Here we mainly investigated the effects of working pressure and air flow rate on surface morphology of ZnO hollow microsphere.Fig.5shows the images synthesized at lower deposition tem-perature 470◦C with variational working pressure keeping other experimental conditions constant.It is evident from the images that the nanostructure is variational with decreasing working pres-sure.At high working pressure (2×104Pa),there are few hollow sphere and the nanorods that promiscuously deposit on the surface of the sphere,shown in Fig.5a.While working pressure is decreas-ing (8×103Pa),some hollow sphere with small rhombus-shaped grain are present,shown in Fig.5b.Surface morphology (Fig.5c)gradually tends to regular distributing while working pressure is 1×102Pa.The pressure is adjacent to 20Pa where our previous experimental condition has been used.From the results,when working pressure is high,the inside zinc vapor pressure may not be enough to break the shells,resulting in the presence of compound Zn/ZnO.So it is thought that the optimized working pressure is about 20Pa.XRD patterns from the products obtained at differentworking pressure are shown in Fig.6.Thereinto,a 1and b 1are the XRD patterns of as-deposited spheres when working pressure is 2×104Pa and 8×103Pa,respectively.The peaks belonging to Zn and ZnO are present.And the peaks belonging to hexagonal Zn are decreasing when working pressure is 8×103Pa,which implied the quantity of ZnO in the spheres is increasing.Fig.6c 1displays the XRD pattern when working pressure is 1×102Pa.All the peaks can be well indexed to wurtzite ZnO.No other peak is observed in the XRD spectra,revealing that the Zn precursor almost transformed into ZnO hollow spheres with the wurtzite structure.It also indi-cates that working pressure of 1×102Pa is appropriate to oxidize Zn precursor into ZnO hollow microspheres.From the above results,working pressure influenced not only the type of the product but also its surface morphology of hollow microsphere.High working pressure is difficult to synthesize hollow ZnO microsphere.This is because the interior Zn vapor is not enough to damage the thin ZnO shell compared to outer high pressure.So the optimized working pressure is 20Pa for hollow ZnO microsphere synthesis.The effect of air flow rate is unconspicuous compared to those of growth temperature and working pressure.At the low air flow rate (60sccm),it is consistent with a low supersaturation,thus forming the long needle-shaped nanowires with small roots on the sur-face of ZnO hollow microspheres,shown in Fig.7a.As increasing the air flow rate to 80sccm,the supersaturation will be increased.Therefore,the increasing air flow rate introduces the higher super-saturation corresponding to the growth ZnO nanowires with big roots,and even big nanorods (as shown in Fig.7b).For the con-stant temperature,the desorption probability of adsorb atoms may not change.So it will lead to the higher growth rate with higher oxygen flow rate,which needs to be further verified by the other experiments.And the effects of other experimental conditions are unconspicuous so they do not list here.In our chemical vapor deposition experiment,ZnO crystal growth may undergo the following process.The schematic illustra-tion for the formation of ZnO hollow spheres is depicted in Fig.8.At different stages,SEM images are shown in the schematic illus-tration.The growth of ZnO hollow spheres should be a vapor-solid process rather than a vapor-liquid-solid process,because no cata-lyst was used during the synthesis.At the initial growth stage when air was introduced into the tube at 400◦C,ZnO nanocrystals are formed on the primary zinc microsphere surface,forming a dense ZnO nanocrystals on the surface of Zn microsphere.Additional Zn powder is quickly vaporized and delivered into the precursor tem-plate by the carrier gas Ar and reaction with air when temperature rises rapidly,and then adsorbs on the surface of the sphere to form an absorbed layer of Zn atoms,then to act as the seeds for subse-quent nanorods/nanowires growth.Because the shell is very dense and seamless,the inside Zn vapor pressure will be high enough to break the thin shells and Zn in the interior will beevaporated,Fig.4.(a)TEM images of ZnO nanowires on the surface of the hollow sphere,the inset is the corresponding electron diffraction pattern;(b)HRTEM image of the corresponding TEM images.Y.Tian et al./Applied Surface Science258 (2012) 8431–84388435Fig.5.SEM images of the as-prepared products obtained at different working pressure while keeping other reaction conditions the same as in a typical synthesis:(a1,b1and c1)Low-and(a2,b2and c2)high-magnification images of microspheres of the as-obtained products synthesized at2×104Pa,8×103Pa and2×102Pa,respectively(the insets show the enlarged views of the surface morphologies).resulting in the formation of hollow ZnO microsphere with a small open mouth.As far as known,the temperature at the deposition region is higher than zinc’s melting temperature(419.5◦C),the interior Zn will eventually be sublimated with rising temperature. The nanocrystalline on the surface of ZnO sphere shell are very ben-eficial to the preferred aligned growth of ZnO nanorods/nanowires. With the concentration of the Zn vapor coming from additional Zn powder reaches a stable saturation status,it approximately under-goes an equilibrium condition for the growth of well-aligned ZnO nanorods/nanowires with uniform size and morphology.Like the nanorods/nanowires grown on the outer surface,the nanostruc-tures on the inner surface are also grown from the ZnO nanocrystals. After growth for one hour,a completely hollow ZnO sphere is formed.SEM images coming from different growth stage experi-ments also indirectly sustain our growth mechanism.The gas sensing properties of as-prepared ZnO hollow sphere with nanowires on the surface for the detection of ethanol was investigated.Fig.9a shows the schematic illustration of the sensor element.In order to determine the optimum operating tempera-ture,the response of the ZnO hollow spheres gas sensor to100ppm ethanol gas was tested as shown in Fig.9b.It seems that the sensor shows the largest responses to ethanol when operated at420◦C. Therefore,the temperature of420◦C was chosen for further exam-ining the gas sensing characteristics of the ZnO hollow spheres.The gas sensitivities of the sensors with different concentrations(from 1to200ppm)of ethanol gas were tested.The gas sensitivity(S)was defined as the resistance ratio Ra/Rg.As shown in Fig.9c,it can be seen clearly that gas sensitivity was enhanced with rising concen-tration of ethanol gas.It is known that the gas sensing mechanism for semiconducting metal oxides can be ascribed to the change in8436Y.Tian et al./Applied Surface Science 258 (2012) 8431–8438Fig.6.XRD patterns of obtained products a 1,b 1and c 1synthesized at 2×104Pa,8×103Pa and 2×102Pa.electrical conductivity resulting from the chemical interaction of gas molecules with the surface of semiconductor metal oxides.The mechanism of enhanced sensing of ZnO hollow sphere sensor can be explained as follows:The oxygen vacancy (V O )in ZnO nanowires grown on the surface of sphere acts as an electron donor in ZnO to provide electrons to the conduction band of ZnO and makes ZnO nanowires an n-type semiconductor [27].The exposed surface of nanowires adsorbs the oxygen molecules from the ambient gas components,which capture electrons from the conduction band and form O −,as in eqs 1.So oxygen adsorption plays an important role in electrical transport properties of ZnO [28].O 2(g)+2e −→2O −(ads)(1)After sufficient adsorption of oxygen,depletion layers were formed on the surface regions of nanowires,which caused the carrier concentration to decrease and consequently increased the resistance.In addition,the surface effect of nanomaterials,namely,a high surface-to-volume ratio results in the high quantity of sur-face atoms of thin nanowires grown on the surface of the spheres,which can lead to the insufficiency of surface atomiccoordinationFig.7.ZnO microspheres surface morphologies formed at different air flow rates which include (a)nanowires with small roots (b)nanowires with bigroots.Fig.8.A schematic drawing of the possible formation mechanism of hollow microspheres at diverse duration:(a)Zn precursor (b)formation of Zn/ZnO core/shell structure (c)formation of hollow microsphere (d)ZnO microspheres with different surface morphologies.Y.Tian et al./Applied Surface Science258 (2012) 8431–84388437Fig.9.(a)Schematic illustration of the sensor element and(b)response of the ZnO hollow sphere sensor to100ppm of ethanol at different operating temperatures(c)the sensor response of the hollow ZnO microsphere to different concentration of ethanol at420◦C(d)the corresponding response-recovery curves of the ZnO hollow sphere sensor.and high surface energy.Therefore,the surfaces are highly active, which promotes further adsorption of oxygen in the ambient atmo-sphere.When ethanol gas molecules approach the ZnO surface, they will react with the adsorbed O−,which results in electrons being released to the surface layer of ZnO.The relevant reaction which occurs on the surface could be as follows:C2H5OH(ads)+6O−→2CO2+3H2O+6e−(2) Thus,ZnO hollow sphere sensor has good gas sensitivity to ethanol gas due to larger quantity of V O and higher surface-to-volume ratio,namely,a larger effective surface areas of thin nanowires assembled on the ZnO spheres.4.ConclusionsIn summary,a precursor-template method was demonstrated for the synthesis of hollow ZnO spheres with high surface area, which were composed of different surface morphologies by alter-ing growth experimental conditions such as growth temperature, airflow and working pressure.On the basis of the controls of Zn precursor shape and size,the precursor plays a critical role on the formation of the ZnO hollow sphere.The obtained ZnO hollow spheres exhibited good gas sensing performance toward ethanol gas due to the high surface area and hollow structure,suggest-ing the ZnO nanomaterial is a promising candidate for detecting ethanol gas.However,further effort is in great need and in progress for developing a gas sensor with the selectivity for other gases.AcknowledgmentThis work is funded by the National Natural Science Foundation of China(grant nos.51002058,10975109,61006046). 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Effect of annealing temperature on microstructural evolution and mechanical property of Ti alloy
Short CommunicationEffect of the annealing temperature on the microstructural evolution and mechanical properties of TiZrAlValloyR.Jing a ,⇑,S.X.Liang a ,b ,C.Y.Liu a ,M.Z.Ma a ,R.P.Liu a ,⇑a State Key Laboratory of Metastable Materials Science and Technology,Yanshan University,Qinhuangdao 066004,China bCollege of Equipment Manufacture,Hebei University of Engineering,Handan 056038,Chinaa r t i c l e i n f o Article history:Received 13December 2012Accepted 15June 2013Available online 27June 2013a b s t r a c tThis study aimed to evaluate the effects of the annealing temperature on the structural evolution and mechanical properties of TiZrAlV alloy.The microstructural evolution and mechanical properties of the alloy were investigated by X-ray diffraction,metallographic analysis,tensile testing,and microhardness testing.The results showed that the thickness of the a phase that precipitated from the parent phase was sensitive to the annealing temperature.With increased annealing temperature,the a -phase tended to exhibit equiaxed grains,except for the specimen annealed at 1050°C.The tensile strength of the equi-axed a grains were also demonstrated to have higher tensile strength than those of the lamellar a phase.The optimal mechanical properties of the alloy was obtained after annealing at 850°C,i.e.,r b =1245MPa,r 0.2=1006MPa,and e =16.89%.Ó2013Elsevier Ltd.All rights reserved.1.IntroductionTitanium-based alloys are increasingly being used as structural materials in the aerospace and automotive industries because of their remarkable advantages,such as exceptional strength-to-weight ratio,good hardenability,good elevated temperature performance,excellent fatigue/crack-propagation behavior,and corrosion resistance [1,2].Compared with other conventional stainless steel or structural materials,the mechanical properties of Ti alloys enable their weight to be reduced to about 40%in aerospace and automotive applications [3,4].Currently,the main-stream Ti structural material is the a +b phase Ti–6Al–4V alloy because of its better physical and mechanical properties than com-mercial-purity Ti and other Ti alloys.The a +b phase Ti–6Al–4V alloy is often used in aerospace applications,pressure vessels,blades and discs of aircraft turbines and compressors,surgical implants,etc.[5–8].The mechanical properties of dual-phase Ti alloys are closely related to their microstructure.The metallurgical processes such as thermo-mechanical processing and different heat treatment methods,which bring modifications in the micro-structure,can strongly influence their mechanical properties of these alloys [9].The majority of commercially used dual-phase Ti alloys are usually thermo-mechanically processed and subjected to different heat treatments to obtain the ideal microstructure for the desired application.In general,these alloys exist as two typical microstructures,namely,Widmanstätten lath precipitateof the hexagonal close-packed a phase distributed in a matrix of body-centered cubic b phase,and the combination of some equi-axed a -phase grains distributed in a transformed b phase.In general,Ti alloys have low hardness (HV 300–320)and yield strength (880–900MPa)[10].Previous studies [11]have used zir-conium,which has similar chemical properties to Ti,as an alloying element to strengthen Ti–6Al–4V alloy,even though zirconium is considered a neutral element [12,13].The addition of 20%(by mass)Zr to Ti–6Al–4V alloy has been experimentally found to in-crease the alloy strength and microhardness with acceptable elon-gation.In this work,different microstructures of the alloy were obtained by controlling the annealing process.The mechanical properties of the alloy were found to be very sensitive to the annealing temperature.2.Experimental procedureThe alloy used for this study is prepared by electromagnetic induction melting the mixture of sponge Ti (99.7wt%),sponge Zr (Zr +Hf P 99.5wt%),industrially pure Al (99.5wt%)and V (99.9wt%)under an argon atmosphere.Table 1shows the chemical composition of the studied alloy.The alloy was then flipped and re-melted three times to ensure a homogeneous chemical compo-sition.The ingot used in the experiment was homogenized at 1000°C for 12h,followed by cooling to room temperature.Then the ingot underwent multiple breakdowns after being held at 1000°C above the b transus temperature for 90min to completely break the coarse grains.The ingot was held at 900°C for 90min and then subjected to the final heat forging in the a +b phase0261-3069/$-see front matter Ó2013Elsevier Ltd.All rights reserved./10.1016/j.matdes.2013.06.039Corresponding authors.Tel.:+863358074723;fax:+863358074545.E-mail addresses:qwe_jr@ (R.Jing),riping@ (R.P.Liu).982R.Jing et al./Materials and Design52(2013)981–986Fig.1.DSC curve of TiZrAlV alloy.region,and the ingot was lathed into bar40mm in diameter.Thesamples(approximately10mmÂ10mmÂ70cm)were cut fromthe bar using wire-electrode cutting and used for subsequentannealing trials.Differential scanning calorimetry(DSC)was used to determinethe phase transition temperatures with a heating rate°C/min which was adopted the standard of ASTM:F2004–05(2010).The nominal a?a+b transus temperature andb?b transus temperature for TiZrAlV alloy are about789and946°C,respectively,as shown in Fig.1.Heat treatment wasperformed in a tubular vacuum furnace under a protective argonpatterns of TiZrAlV alloy:(a)forging,(b)annealing treatment at different temperatures,and(c)detail of33–43°of forging and annealingsignified that the alloy only formed the solid solution phase and that no other intermetallic compound and/or phase existed (Fig.2a).A comparison of the XRD patterns at different annealing temperatures (Fig.2b)revealed that the phase composition of all annealed alloys consisted of a and b phases.With increased annealing temperature,the b phase (110)reflection peak near 38°gradually broadened and the intensity of the (110)diffraction peak increased.However,at 1050°C annealing temperature,the b phase (200)peak disappeared.The XRD patterns also showed that the proportion of a and b phases evidently changed with the chan-ged in annealing temperature.This phenomenon may be caused by the difference of the migration rate of the atom under the high temperature.Generally,with the temperature increasing,the fre-quencies of the atoms migration are also increased gradually.In the insulation process,the moving distancesof Al atom (which is a -stabilized element)and V atom (which is b -stabilized element)were different,and in the subsequent cooling process,the b phase transformed into the a phase which caused the Al atom enriched in the b phase lattice and changed the b phase lattice parameters.Therefore,it may make the intensity of the b phase (110)reflection peak increase and the (002)reflection peak decrease when the annealing temperature was heated to 1050°C.Furthermore,the annealing holding time was shorter (30min),in this process,the a phase transformed into the b phase may be incomplete at an-nealed treatment at 1000°C,while annealed temperature was in-creased to 1050°C,the a phase may be completely transformed into the b phase,therefore,in the specimen annealed at 1000°C the initial a phase was also existed,but the specimen which was annealed at 1050°C did not exist the initial a phase.This may re-sult that the differences of a phase between 1000°C and 1050°C is obviously.Fig.3shows the microstructure of the annealing temperatures.The specimens ited Widmanstätten morphology (Fig.3a),i.e.,chaotic arrangement of slender a lath and b annealing temperature to 1000°C,the b peared and the a lath gradually (Fig.3b–e).In this process,the alloy axed trend with increased annealing have caused the increased equiaxed a phase the annealing process.First,the lamellar a ‘‘interleaved,’’which restricts the other a longitudinal direction.Consequently,a only along the transverse direction,which promotes the thickening of the a lamellar.Second,the new a phase that precipitates from the parent phase grows along a specific habit plane and has a cer-tain orientation relationship with the primary a phase.Thus,the new precipitated a phase growing along the longitudinal direction is hindered such that the equiaxed degree is increased.Obasi [14]also indicated that the phase transformation in Ti alloys during heating (a ?b )and cooling (b ?a )is governed by the so-called Burgers orientation relationship {0002}a ||{110}b and h 11À20i a ||h 111i b with 6possible b -orientations during the a ?b phase transformation and 12possible a orientations that can transform from a single parent b grain during b ?a phase transformation.However,when the annealing temperature reached 1050°C,the alloy revealed the typical basketweave mor-phology (Fig.3f),i.e.,a crisscross slender a lath.b grain boundaries and some parallel lamellar the grain boundaries (the Widmanstätten microstructure)observed in this process.In most diffusion phase and precipitation processes,the nucleations of the heterogeneously occurs at some preferential nucleation the matrix such as the grain boundary,dislocation,phase [15].When the annealing temperature (e.g.,Optical microstructure of TiZrAlV alloy under different annealing temperature:(a)800°C,(b)850°C,(c)900°C,(d)950°C,(e)1000°C,and Fig.4.True stress–strain curve of the studied alloy under different conditions.the thickness of the a lath became limited.Therefore,the thicknessof the new precipitated a phase after annealing at1050°C was smaller than that after annealing at1000°C.The mechanical properties of the alloy were evaluated through uniaxial tensile tests.Fig.4and Table2show the true stress–strain curves and mechanical properties of the specimens at different annealing temperatures.The mechanical properties of the ZrTiAlV alloy evidently depended on the annealing temperature and micro-structure.When the annealing temperatures were between800 and1000°C,the yield strength r0.2and ultimate strength r b de-creased from1009and1290MPa to978and1181MPa,respec-tively.The elongation only slightly changed after annealing at of the residual b phase during the annealing process as well as the thickness of the a lath.The main factors influencing the mechanical properties of an-nealed samples in which only the a and b phases exist are the phase content,size,and morphology of the a phase[16–18].Because of the limited number of independent slips modes,the hcp structure of Ti exhibits a vary strong grain-boundary,or Hall–Petch strength-ening at room temperature.The thickness of the a grain boundary directly influences the strength mismatch between the a+b matrix and the grain boundary[19].Consider the case of b processed microstructures.Some of the microstructural features involved with progressively increasing length scales are width of the a-laths, the colony size,and the b grain size(feature sizes may range from sub-micron to millimeters).Depending on the thermo-mechanical treatment the alloy is subjected to,such as cooling rates from +b dual phase region or above the b-transus,these features can vary significantly.Quantifying them over the diverse range length scales involved becomes rather important.Thus,to investi-gate the effect of the annealing temperature on the microstructure and mechanical properties,the specimens prepared at different annealing temperatures were subjected to SEM analysis,as shown Fig.6.The measured thicknesses of the a lath from the SEM images are shown in Fig.7a.With increased annealing temperature Fig.5.Microhardness of annealed specimens under different conditions.SEM images of TiZrAlV alloy under different annealing temperature:(a)800°C,(b)850°C,(c)900°C,(d)950°C,(e)1000°C,and(f)from 800°C to 1000°C,the thickness of the a lath in the annealed samples increased from 1.07l m to 4.22l m.When the annealing temperature reached 1050°C,the thickness was reduced to 1.12l m.According to the Hall–Petch equation,(i.e.,r =r 0+kd À1/2,where d is the thickness of the a lath),the strength of an annealed alloy is related to the a lath thickness,as shown in Fig.7b.On one hand,the change of the a lath thickness moved the distance of dis-location to the phase boundary,which resulted in increased num-ber of dislocations piling up such that the stress concentration was more severe.On the other hand,reducing the a lath thickness increased the density of the phase boundary in the same cross-sectional area.Consequently,the movement of the dislocation obstacle increased.Thus,based on the OM images,SEM images,and true stress–strain curve,the slender a lath obtained at 800°C and 1050°C increased the strength of the specimens and made dis-location movement difficultly.Moreover,with increased equiaxed a -phase degree,the strength of the annealed specimens gradually decreased.This result implied that the strength of the processed alloy lamellar a phase microstructure was higher than that of processed equiaxed a -phase microstructure.The magnitude of the titanium alloy tensile elongation is con-nected with the non-uniform degree of the tensile micro deforma-tion zone,as well as the length and the spacing of slip bands.With the spacing of slip bands decreasing,the plastic deformability in-crease before the material fracture [20].Compared with the lamel-lae microstructure,the slip bands spacing of the duplex microstructure is smaller,thus this microstructure possess a high-er ability of deformation.When sample was annealed at 850°C,the feature of microstructure presented the duplex microstructure (Fig.3b),therefore,the elongation reached the largest value in this experiment i.e.16.89%.4.ConclusionThe phase transition,microstructure evolution,and their effects on the mechanical properties of TiZrAlV alloy were investigated.The conclusions were as follows:(1)TiZrAlV alloy exhibited an a +b phase after high-tempera-ture annealing.The intensity of the b (110)diffraction peak increased with increased annealing temperature.However,the intensity of the b (200)diffraction peak gradually decreased with increased annealing temperature.When the temperature reached 1050°C,the b (200)diffraction peak completely disappeared.(2)The thickness of the a phase was sensitive to the annealingtemperature.With increased annealing temperature,the a phase tended to exhibit equiaxed grains,except for speci-mens annealed at 1050°C.After annealing at 1000°C,the maximum thickness was 4.22l m.(3)The mechanical properties of the annealed specimens weresensitive to the morphology of the precipitated a phase and yo the annealing temperature.The optimal mechanical properties of the alloy were obtained after annealing at 850°C,i.e.,r b =1245MPa,r 0.2=1006MPa,and e =16.89%.AcknowledgmentsThis work was supported by the SKPBRC (Grant No.2010CB731600),NSFC (Grant No.51121061/51171160/51171163).References[1]Eylon D,Vassel A,Combres Y,Boyer RR,Bania PJ,Schutz RW.Issues in thedevelopment of beta titanium alloys.JOM 1994;46:14–5.[2]Ivasishin 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新材料英文文献
新材料英文文献Microstructural evolution taking place duringequal-channel angular pressing was studied in a commercial Al-6Mg-03Sc alloy at 523 K(250℃)(~0.5T)The structural changes are mainl associated with development of microshearbands(MSBs)that are continuously formed by strain accumulation and microstructural heterogeneities in each pass.which result in frag mentation of coarse original grainsNewultrafine grains(UFGs)with moderate-to-high angle boundary misorien tations are concurrently evolved in the interiors of MSBs accompanied by rigid body rotation at medium-to-large strains.Such strain-induced grain refinement process occurs verv slowly and incompletely in the present heavily alloved Alallovleading to formation of a mixed microstructurei.e.the UFGs in colonyand some weaklymisoriented fragments of original grainsThe microstructure evolved at 12 is characterized bv a bimodal crvstallite size distribution with two peaks at d0.2 to 0.3 um and d0.6 to 0.7 um.and the fraction of high angle boundaries ofabout 0.35+0.05.The main factors promoting dynamic formation of UFGs and the effects of thermal processes on it during severe plastic deformation are discussed in detail.研究了工业用Al-6 Mg-03 Sc合金在523 K(250℃)等通道转角挤压过程中的显微组织演变)(~0.5T)结构变化主要与微剪切带(MSB)的发育有关这是连续形成的应变积累和微观结构的不均匀性在每个通道。
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JOURNAL OF RARE EARTHS,Vol.28,No.1,Feb.2010,p.134F j y I M I S &T y j ()I M T y R &D j W NG y (f 6@63)DOI 6S ()666Effect of cerium addition on microstr ucture and texture of aluminum foil for electr olytic capacitor sWANG Haiy an (王海燕)1,2,L I Wenx ue (李文学)1,REN Hu iping(任慧平)1,HUANG L iy in g (黄丽颖)1,WAN G Xia ngy ang(王向阳)1(1.School of Material and Metall urgy Engineering,Inner Mongolia University of Science and Technology,Baotou 014010,China;2School of Materials S cience and En-gineering,University of Science and Technology B eijing,Beijing 100083,China)Received 23October 2008;revised 27August 2009Abstract:Anode foil of aluminum electrolytic capacitor,which requires large surface area for high capacitance,were prepared by rolling,an-nealing and electrochemical etching.Effects of cerium addition on the capacitance of aluminum electrolytic capacitors were investigated.Mi-crostructure of the aluminum foil surface was observed by optical microscopy (OM)and scanning electron microscopy (SEM).Electron back scattered diffraction (EBSD)was also employed to reveal texture evolvement of cold-rolled aluminum foil after annealed.The results showed that addition of cerium contributed to higher <100>texture and higher etch pit density as well.Moreover,the distribution of etch tunnels was more uniformcompared with that without cerium addition.Perfect specificsurface area was obtained with 0.0074%addition of cerium.Keywords:electrolytic capacitor;aluminum foil;rare earthsAluminum electrolytic capacitors are widely used in all types of electronic equipments.High voltage electrolytic ca-pacitors consist of an electrolyte put on an anode made from a 40–100μm thin high-purity aluminum foil with an oxide layer serving as dielectric [1].The capacitance of dielectrics depends on the dielectric constant,the thickness,and the surface area.Among those factors,especially for aluminum electrolytic capacitors,the enlargement of the surface area is most effective from the practical viewpoint because of the trend toward capacitor size miniaturization [2,3].The effective surface can be greatly increased through an etching process that forms narrow channels along the crystallographic <001>directions into the foils.Thus,with regard to the cube-tex-ture in the aluminum foils for electrolytic capacitors,produc-tion has to be optimized so as to provide maximum number of cube-nuclei as well as good growth prospect of the cube-orientation [1,4].A strongly textured material consisting of grains with <001>direction parallel to the sheet normal is favorable.In practical application this is achieved by pro-ducing sheets with a strong cube-texture {001}<100>.To increase the surface area,investigation of pit formation seems very important.Many studies have discussed the pits using high-purity aluminum foils during DC etching in HCl solutions,including the shape,morphology of pitting corro-sion,the tunnel pit growth and the effect of impurities on etching behavior [5].In addition,since the thickness of these foils is only 100–110μm,the tunnel length must be con-trolled to less than 50μm,in order to form a non-piercing layer after etching on double surfaces of Al foil [6].Thus,it is necessary to study the principle of tunnel growth to controltunnel length of pits and maintain a non-piercing layer.It has been recognized that the solution composition in-duces certain mechanical,physical and chemical changes,which can lead to activation of chemical and electrochemical reactions,thus result in accelerated material removal and corrosion [7].In general,hydrochloric acid is used for the etching solution,but the size and distribution of etch pits are not uniform with low density as a result of high corrosive-ness.However,effect of solution composition,especially for rare earth element on pitting corrosion,has not been exten-sively or systematically studied,it can be expected that addi-tion of rare earth during electrochemical etching of alumi-num may induce optimum etch structure,and produces high surface of aluminum foil.Therefore,to increase the specific internal area by reducing the rate of dissolution concentrated on local area and producing dense etch pits,studies of rare earth addition was carried out in this work.1ExperimentalHigh-purity (>99.9972%)aluminum foils with different cerium additions of 0.006wt.%,0.0074wt.%,and 0.012wt.%were used.The impurities in the aluminum are as follows (wt.%):Fe 0.00071,Si 0.00070,Cu 0.00125,Zn 0.00014,and Ti 0.00005.The thickness of aluminum ingot was 18mm,after homogenized treatment,reheating,hot rolling and reversibly cold rolling with a thickness reduction of as much as 98%to a final thickness of 0.11mm.Finally,all speci-mens were isothermally annealed for various times in salt bath furnace.For DC electrolytic etching test,specimensound at ion it em:P ro e ct supported b the nne r ongolia mporta nt cie nc e e chnolog Pro ec t 20071911a nd nner ongolia e chnolog ese arch evelopment Pro ec tCorre sponding a uthor :A H ai an E-ma il:w ind :10.101/1002-07210900-1WANG Haiyan et al.,Effect of cerium addition on microstructure and texture of aluminum foil for electrolytic capacitors 135were cut into 10mm ×55mm,and exposed with an area of 1cm 2to the etching solution.The rest of the specimen was masked with polyester tape.All the specimens were pre-treated in HCl+H 2SO 4(3:1)solution and then rinsed with deionized water before electrolytic etching test.Surface morphology of the recrystallized foils and etch tunnels were observed by means of optical microscopy and scanning electron microscopy (SEM).The evolution of cube-texture during isothermal annealing of the cold rolled foils was tracked by crystallographic texture using electron back scattered diffraction (EBSD)micro texture analysis [8].2Results and discussionFig.1(a –d)show the shape and distribution of the etch pit formed in the solutions with cerium additions of 0wt.%,0.006wt.%,0.0074wt.%,and 0.012wt.%respectively.It is found that there are noticeable differences in the morpholo-gies of etch pits,depending on the additive.The intensity of the cube-orientation {001}<100>changed with the increas-ing of cerium content.As shown in Fig.1(a),when cerium is not applied,about 20%of the tunnels observed at 15μm become alive in the process of tunnel growth,while more tunnels are observed with cerium addition and the survival rate increases in Fig.1(b),(c)and (d).Compared with those with additives,the density of etch pits is low in pure alumi-num foil.The length,widths and depths of individual pits weremeasured for each specimen.As shown in Fig.1,under the conditions without additive and with 0.006wt.%Ce,0.0074wt.%Ce,and 0.012wt.%Ce,the density of etch pit is 0.9×105,3.2×105,4.3×105and 6.1×105pits/cm 2,and the av-erage size is 14.0,12.2,9.0and 8.6μm,respectively.The number of etch pits generated in the etching solutions with rare earth additives is about twice as much as that formed without additive as shown in Fig.1(a).This system is typical of the Al-RE (rare earth)series.Ce-rium exists as stable intermetallic compounds in aluminum,and with a negative enthalpy of mixing in the liquid phase [9].There are some kinds of micro impurity,such as Fe,Si,Mn in aluminum,Ce will form compound of CeFe 2Al 10,CeSi 2A13,CeMn 4Al 8,Ce 2Mn 7Al 10,(CeMg)Al 2,etc.[10]These com-pounds can purify the matrix and eliminate the obstruction of impurity,especially the effect of Fe on nucleation and growth of cube orientation grains during annealing process,and thus increase the cube orientation of aluminum foil,which agrees with the etch pits measurement shown in Fig.1.Fig.2shows the texture evolution of samples with differ-ent rare earth contents cold-rolled and annealed at 530°C for 600s.In Fig.2(a),some minor intensities of cube-orienta-tion {001}<100>are observed.By contrast,with cerium addition,the texture has changed in Fig.2(b).The ODF (ΔΦ=5°)is characterized by very sharp cube-orientation dominating over the rolled texture,for the aluminum foil with 0.0074wt.%pare to the Fig.2(b),the 0.019wt.%Ce addition showed weaker cube-orientationtextureFig.1Recrystallized microstructureof aluminumfoil without Ce (a),with 0.006wt.%Ce (b),with 0.0074wt.%Ce(c)and with 0.012wt.%Ce(d)F T x f f 53f 6(),%()%()ig.2e tureevolution o the samples a terannealed at 0o C or 00s without Ce a with 0.0074wt.Ce b and with 0.012wt.Ce c136JOURNAL OF RARE EARTHS,Vol.28,No.1,Feb.2010(Fig.2(c)).To sum up,annealed samples with cerium addi-tion have higher intensity of cube-orientation {001}<100>and the cube texture reaches the maximum with 0.0074wt.%Ce.With further addition of Ce,cube texture density weak-ens.In order to develop greater understanding of texture evolvement,{111}pole figures,determined from EBSP,for the above specimens with different rare earth contents cold-rolled and annealed at 530°C,are shown in Fig.3,where separate measurements were made on small and large grains.The sample of cold rolled and annealed high purity alu-minum had a random texture with few grains exhibiting cube,S and Cu orientations (see Fig.3(a)),while addition of 0.0074wt.%cerium resulted in sharp cube texture,i.e.,more than 90%{100}<001>orientations with little other texture component are observed in Fig.3(b).With more Ce addi-tions,Fig.3(c)indicates that the orientations are similar to those of the grains shown in Fig.3(b),i.e.,cube texture with minor other texture components.However,the cube texture is less sharp,the contour line tend to sparse,with other ori-entations starting to be presented.It is known that addition of rare earth can refine crys-tal [11,12],and induce boundary corrosion,since higher bound-ary density reduces segregation of impurity atoms and dis-tribution inhomogeneity of current density.Therefore,it is possible to increase the specific electric capacity through de-creasing the grain size under special corrosion conditions [4].With increasing rare earth content,higher defect density and corresponding local concentration of corrosion current den-sity around grain boundaries induce preferred corrosion of rge corrosion holes or channels will appear frequently along the grain boundaries,which lead to the in-homogeneity of corroded structure.Taking the microstructure and texture evolution into ac-count,we conclude that control of cerium addition produces different recrystallization textures during annealing of cold-rolled aluminum,from which the favorite corrosion orienta-tion can be found.When aluminum is electrochemically etched,cubic pits are initially formed and turned into tunnels as the pits grow up.The SEM images of the aluminum etched pit shown in Fig.4corroborate the microstructural evolvement.Fig.4(a)shows that the tunnel length is approximately 20μm.Fig.4(b)indicates that many dark and small tunnels distribute along the tunnel depth in the etched aluminum foils with 0.0074wt.%Ce addition.It is easy to verify that cerium additive induces higher density of small etch pits and contributes their further growth into tunnels by enhancing the mass transport inside one-dimensional tunnel structure.Uniform tunnel length distribution increases the surface area which favors capacitance.It should be noted,however,that large etch pit forms in Fig.4(c)which is rooted in the connections of many small pits ,thus the tunnel wall along its depth will pare to the smaller pits,the surface of tunnel will decrease,as a result of blocking of small pits or tunnels by oxides with the increasing of cerium.The specific capaci-tance obtained by using alternating current impedance [13]shows that the capacitance at first increases,and then de-creases with increasing rare earth addition,it means that the content of rare earth should be controlled to certain extent,and the highest specific surface area was obtained from the specimen with 0.0074wt.%Ce.The effect of cerium on the corrosion of aluminum has been investigated by incorporating cerium into aluminum substrates and observing the subsequent anodic oxidation behavior of the alloys [14].The corrosion resistance of alumi-Fig.3{111}pole figures for sample after annealed at 530°C for600s without Ce (a),with 0.0074wt.%Ce (b)and with 0.012wt.%Ce(c)F S M f f (),%()%()ig.4E images o the aluminum oil without Ce a with 0.0074wt.Ce b and with 0.012wt.Ce cWANG Haiyan et al.,Effect of cerium addition on microstructure and texture of aluminum foil for electrolytic capacitors137num in aqueous media can be attributed to rapid formation of surface oxide film[15].Hydrochloric acid is used as etching solution,and Cl–plays an important role in spot corrosion and development,which has great effect on the oxide scale dissolution of the aluminum foil surface.Cl–is adsorbed on the special location of oxide surface,dissolves the oxide scales and formed Al(OH)2Cl,Al(OH)Cl2,AlCl2+,AlCl3, Al(OH)Cl+,finally produces etch pits on the surface of Al. Cerium and aluminium are oxidized at the alloy/film inter-face and incorporated into the anode film.In general,the oxide layer spread over the macroscopic surface,improves active hole forming[16],thus increases the specific internal area.However,when the content of cerium keeps increasing, the distribution inhomogeneity induces the substantial in-crease of chemistry activity,and results in large number of etching pits,which generates film breakdown over alumi-num surface.During the growth of tunnel,metal dissolution occurs from its surface,while the tunnel sidewalls are cov-ered with oxide film which restrain corrosion,which results in inferior capacitance[17].As mentioned above,we can estimate that the introduction of cerium reduces the thickness of oxide film on aluminum metal and induces the nucleation of etch pits.Therefore,ad-dition of rare earth has certain potential to be used for the application of aluminum electrolytic capacitors,and the in-volved researches are still underway to be carried out.3ConclusionsCerium was introduced to control the etch pits and tunnel length distribution on aluminum foil for electrolytic capaci-tors.The dissolution of cerium during electrochemical etch-ing might induce the optimum etch structure,produce high surface area and finally increase the capacitance,since addi-tion of cerium prohibited initial oxide film formation during etching but favors the formation of corrosion pits.In this work,the most perfect surface area was obtained when the addition of Ce reached0.0074wt.%.References:[1]Engler O,Huh M Y.Evolution of the cube texture in high pu-rity aluminum capacitor foils by continuous recrystallization and subsequent grain growth.Mater.Sci.Eng.A,1999,271(1): 371.[2]Scherer J,Magnussen O M,Ebel T,Behm R J.Initial stages ofthe anodic etching of aluminum foils studied by atomic force microscopy.Corros.Sci.,1999,41(1):35.[3]Oh H J,Lee J H,Ahn H J,Jeong Y S,Park N J,Kim S S,ChiC S.Etching characteristics of high-purity aluminum in hy-drochloric acid solutions.Mater.Sci.Eng.A,2007,449-451(25):348.[4]Mao Weimin,Chen Lei,Sa Liman,Yu Yongning,Li Yunfeng.Influence of grain boundaries on corrosion structure of low voltage aluminum foil.T he Chinese Journal of Nonferrous Metals(in Chin.),2004,14(1):1.[5]Osawa N,Fukuoka K.Pit nucleation behavior of aluminiumfoil for electrolytic capacitors during early stage of DC etching.Corros.Sci.,2000,42(3):585.[6]Wang Mei,He Yedong.Growth and passivation of aluminumetch tunnels at on-off controlling direct current in6wt.%HCl solution.Rare Metals,2008,27(2):205.[7]Liu Guili,Zhang Guoying,Li Rongde.Electronic theoreticalstudy of the interaction between rare earth elements and impu-rities at grain boundaries in steel.J.Rare Earths,2003,21(3): 372.[8]Baker I,Li J.An EBSP study of isothermally-annealed cold-rolled nickel.Microscopy Research and T echnique,2004,63: 289.[9]Kang Y B,Peltona A D,Chartranda P,Fuerst C D.Criticalevaluation and thermodynamic optimization of the Al-Ce,Al-Y, Al-Sc and Mg-Sc binary put.Coupling Phase Diagrams Thermochem.,2008,32:413.[10]Deng Yunlai,Zhang Xinmin,Liu Chunming,Chen Zhiyong,Zhou Zhuoping.The effect of trace RE on the evolution of tex-tures in high voltage aluminum capacitor foils.Functional Material,2002,33(1):60.[11]Li Chunlong,Wang Yunsheng,Chen Jianjun,Liu Chengjun,Jiang Maofa.Effects of rare earth on structure and mechanical properties of clean BNbRE steel.J.Rare Earths,2005,23(4): 470.[12]Lin Qin,Guo Feng,Zhu Xingyuan.Behaviors oflanthanum and ce-rium on grain boundaries in carbon manganese clean steel.J.Rare Earths,2007,25(4):485.[13]Wang Xiangyang.Study of the Electrolytic Etching of Ce Alumi-num Foil for Gigh Voltage Anode of Electrolytic Capacitor.Inner mongolia:InnerMongoliaUniv.Sci.&Tech.,2008.5.[14]Tomcsany L,V arga K,Bartik Ietal.Study of the interaction ofCl–with A passive film on Al and initiation of pitting corrosion.Electrochim.A cta,1989,34(5):855.[15]Mishra A K,Balasubramaniam R.Corrosion inhibition of alu-minium by rare earth chlorides.Mater.Chem.Phy s.,2007, 103(2-3):385.[16]Crossland A C,Thompson G E,Skeldon P,Wood G C,SmithC J E,Habazaki H,Shimizu K.Anodic oxidation of Al-Ce Al-loys and inhibitive behavior of Cerium species.Corros.Sci., 1998,40(6):871.[17]Kang J W,Shin Y H,Tak Y S.Growth of etch pits formedduring sonoelectrochemical etching of aluminum.Electro-chimica A cta,2005,51(5):1012.。