期刊文献+
共找到10篇文章
< 1 >
每页显示 20 50 100
Formation mechanism of W phase and its effects on the mechanical properties of Mg-Dy-Zn alloys 被引量:1
1
作者 J.S.Chen C.J.Ji +4 位作者 Q.Y.Huang Y.Z.Zeng H.B.Xie p.chen B.Z.Sun 《Journal of Magnesium and Alloys》 2025年第5期2174-2189,共16页
The morphology and dimension of W phases play an important role in determining mechanical properties of Mg-RE-Zn(where RE denotes rare earth elements)alloys.In this study,theγ′platelet and W particle occurred in the... The morphology and dimension of W phases play an important role in determining mechanical properties of Mg-RE-Zn(where RE denotes rare earth elements)alloys.In this study,theγ′platelet and W particle occurred in the aged Mg-2Dy-0.5Zn(at.%)alloys were investigated by aberration-corrected scanning transmission electron microscopy.A novel formation mechanism of W phase was proposed,and its effects on the morphology and dimension of W particle,as well as mechanical properties of Mg-2Dy-0.5Zn alloys,were also discussed particularly.Different from other Mg-RE-Zn alloys,the nucleation and growth of W particle in Mg-Dy-Zn alloys mainly depend on the precipitatedγ′platelet.Primarily,a mass of Dy and Zn solute atoms concentrated nearγ′platelet or between two adjacentγ′platelets can meet the composition requirement of W particle nucleation.Next,the smaller interfacial mismatch between W andγ′facilitates the nucleation and growth of W particle.Thirdly,the growth of W particle can be achieved by consuming the surroundingγ′platelets.The nucleation and growth mechanisms make W particles exhibit rectangular or leaf-like and remain at the nanoscale.The coexistence ofγ′platelets and nanoscale W particles,and some better interfacial relationships between phases,lead to a high strength-ductility synergy of alloy.The findings may provide some fundamental guidelines for the microstructure design and optimization of new-type Mg-based alloys. 展开更多
关键词 Magnesium alloys Scanning transmission electron microscopy W particle Formation mechanism Mechanical properties
在线阅读 下载PDF
美国大豆生产、育种及产业现状 被引量:4
2
作者 李晓芝 张强 +3 位作者 赵双进 刘兵强 p.chen 张孟臣 《大豆科学》 CAS CSCD 北大核心 2011年第2期337-340,共4页
美国是目前世界上最大的大豆生产国,大豆种植面积(每年3 000万hm2以上)和总产(每年近8 000万t)均占世界的1/3左右;在大豆高产育种、品质育种、抗性育种等方面研究均居世界领先地位。分子育种已成为美国大豆品种改良的重要手段,美国第一... 美国是目前世界上最大的大豆生产国,大豆种植面积(每年3 000万hm2以上)和总产(每年近8 000万t)均占世界的1/3左右;在大豆高产育种、品质育种、抗性育种等方面研究均居世界领先地位。分子育种已成为美国大豆品种改良的重要手段,美国第一代转基因大豆育成引领了世界大豆育种方向。研究借鉴美国大豆生产、育种与推广的经验,对提升我国大豆国际竞争力具有积极意义。通过合作研究、考察、访谈等形式对美国大豆生产、育种及产业现状进行了分析研究。在此基础上,综述了目前美国大豆生产和育种研究现状与最新研究进展,大豆研究网络的构成与运行机制,相关技术服务与推广体系等方面内容。 展开更多
关键词 大豆 生产 育种
原文传递
紫外线对离子互补型自组装寡肽EAK16-II聚集状态的影响
3
作者 欧阳新平 p.chen 《华南理工大学学报(自然科学版)》 EI CAS CSCD 北大核心 2006年第8期51-54,共4页
借助原子力显微镜对离子互补型自组装寡肽EAK16-II在水溶液中自组装聚集形态受紫外线的影响进行了研究.研究结果表明,紫外线改变了该类寡肽在水溶液中自组装形成的纳米结构.当用波长为365 nm的紫外线照射2 h后,离子互补型自组装寡肽的... 借助原子力显微镜对离子互补型自组装寡肽EAK16-II在水溶液中自组装聚集形态受紫外线的影响进行了研究.研究结果表明,紫外线改变了该类寡肽在水溶液中自组装形成的纳米结构.当用波长为365 nm的紫外线照射2 h后,离子互补型自组装寡肽的聚集态从纤维状结构转变为球形结构.从成核模型分析,其原因是由于紫外线照射导致了自组装聚集体分子间作用力的破坏以及β片层向β转角的转变. 展开更多
关键词 自组装寡肽 聚集状态 紫外线 原子力显微镜
在线阅读 下载PDF
Effect of compressibility on the hypervelocity penetration 被引量:7
4
作者 W.J.Song X.W.Chen p.chen 《Acta Mechanica Sinica》 SCIE EI CAS CSCD 2018年第1期82-98,共17页
We further consider the effect of rod strength by employing the compressible penetration model to study the effect of compressibility on hypervelocity penetration.Meanwhile, we define different instances of penetratio... We further consider the effect of rod strength by employing the compressible penetration model to study the effect of compressibility on hypervelocity penetration.Meanwhile, we define different instances of penetration efficiency in various modified models and compare these penetration efficiencies to identify the effects of different factors in the compressible model. To systematically discuss the effect of compressibility in different metallic rod-target combinations, we construct three cases, i.e., the penetrations by the more compressible rod into the less compressible target, rod into the analogously compressible target, and the less compressible rod into the more compressible target. The effects of volumetric strain, internal energy, and strength on the penetration efficiency are analyzed simultaneously. It indicates that the compressibility of the rod and target increases the pressure at the rod/target interface. The more compressible rod/target has larger volumetric strain and higher internal energy. Both the larger volumetric strain and higher strength enhance the penetration or anti-penetration ability. On the other hand, the higher internal energy weakens the penetration or anti-penetration ability. The two trends conflict, but the volumetric strain dominates in the variation of the penetration efficiency, which would not approach the hydrodynamic limit if the rod and target are not analogously compressible. However, if the compressibility of the rod and target is analogous, it has little effect on the penetration efficiency. 展开更多
关键词 COMPRESSIBILITY Hypervelocity penetration Equation of state(EOS) SHOCKWAVE Bernoulli equation
在线阅读 下载PDF
An efficient SPH methodology for modelling mechanical characteristics of particulate composites 被引量:1
5
作者 Z.J.Zheng S.Kulasegaram +1 位作者 p.chen Y.Q.Chen 《Defence Technology(防务技术)》 SCIE EI CAS CSCD 2021年第1期135-146,共12页
Particulate composites are one of the widely used materials in producing numerous state-of-the-art components in biomedical,automobile,aerospace including defence technology.Variety of modelling techniques have been a... Particulate composites are one of the widely used materials in producing numerous state-of-the-art components in biomedical,automobile,aerospace including defence technology.Variety of modelling techniques have been adopted in the past to model mechanical behaviour of particulate composites.Due to their favourable properties,particle-based methods provide a convenient platform to model failure or fracture of these composites.Smooth particle hydrodynamics(SPH)is one of such methods which demonstrate excellent potential for modelling failure or fracture of particulate composites in a Lagrangian setting.One of the major challenges in using SPH method for modelling composite materials depends on accurate and efficient way to treat interface and boundary conditions.In this paper,a masterslave method based multi-freedom constraints is proposed to impose essential boundary conditions and interfacial displacement constraints in modelling mechanical behaviour of composite materials using SPH method.The proposed methodology enforces the above constraints more accurately and requires only smaller condition number for system stiffness matrix than the procedures based on typical penalty function approach.A minimum cut-off value-based error criteria is employed to improve the computational efficiency of the proposed methodology.In addition,the proposed method is further enhanced by adopting a modified numerical interpolation scheme along the boundary to increase the accuracy and computational efficiency.The numerical examples demonstrate that the proposed master-slave approach yields better accuracy in enforcing displacement constraints and requires approximately the same computational time as that of penalty method. 展开更多
关键词 Particulate composites SPH Essential boundary condition Multi-point constraints Master-slave method
在线阅读 下载PDF
A high specific Young's modulus steel reinforced by spheroidal kappa-carbide 被引量:1
6
作者 p.chen J.Fu +6 位作者 X.Xu C.Lin J.C.Pang X.W.Li R.D.K.Misra G.D.Wang H.L.Yi 《Journal of Materials Science & Technology》 SCIE EI CAS CSCD 2021年第28期54-59,共6页
1.Introduction High strength steels continue to be developed for automotive applications to increase safety and reduce lightweight by downgauging[1,2].In addition,reducing density is another solution for the lightweig... 1.Introduction High strength steels continue to be developed for automotive applications to increase safety and reduce lightweight by downgauging[1,2].In addition,reducing density is another solution for the lightweight of automotive components[3,4].Aluminum addition could effectively reduce the density of steels,since it has a low atomic mass and invokes a lattice expansion[5]. 展开更多
关键词 CARBIDE STEEL strength
原文传递
Raiden大豆花叶病毒抗性的遗传和等位性试验
7
作者 谢国禄 p.chen 《国外作物育种》 2001年第4期86-86,共1页
关键词 Raiden大豆 花叶病毒 抗性遗性 等位性 RSV2
在线阅读 下载PDF
Controllable κ-carbide precipitation enables strength-ductility co-enhancement in Fe-Mn-Al-C low-density austenitic steel via grain boundary engineering
8
作者 J.H.Du p.chen +3 位作者 F.Zhang Z.P.Jia F.Shi X.W.Li 《Journal of Materials Science & Technology》 2025年第24期26-31,共6页
1.Introduction The precipitation of κ-carbides is critical for the deformation behavior of Fe-Mn-Al-C austenitic low-density steels[1-5].Ther-momechanical treatment can significantly influence the distribution,size,a... 1.Introduction The precipitation of κ-carbides is critical for the deformation behavior of Fe-Mn-Al-C austenitic low-density steels[1-5].Ther-momechanical treatment can significantly influence the distribution,size,and morphology of κ-carbides,and thus regulate the mechanical properties[1,4,6-8].Intragranular κ-carbides precipitate through either nucleation and growth mechanisms[9]or spinodal decomposition[3,5],depending on thermodynamic conditions. 展开更多
关键词 deformation behavior Fe Mn Al C strength ductility co enhancement grain boundary engineering precipitation low density austenitic steel spinodal decomposition depending nucleation growth mechanisms
原文传递
STCF conceptual design report (Volume 1): Physics & detector 被引量:5
9
作者 M.Achasov X.C.Ai +457 位作者 L.P.An R.Aliberti Q.An X.Z.Bai Y.Bai O.Bakina A.Barnyakov V.Blinov V.Bobrovnikov D.Bodrov A.Bogomyagkov A.Bondar I.Boyko Z.H.Bu F.M.Cai H.Cai J.J.Cao Q.H.Cao X.Cao Z.Cao Q.Chang K.T.Chao D.Y.Chen H.Chen H.X.Chen J.F.Chen K.Chen L.L.Chen p.chen S.L.Chen S.M.Chen S.Chen S.p.chen W.Chen X.Chen X.F.Chen X.R.Chen Y.Chen Y.Q.Chen H.Y.Cheng J.Cheng S.Cheng T.G.Cheng J.P.Dai L.Y.Dai X.C.Dai D.Dedovich A.Denig I.Denisenko J.M.Dias D.Z.Ding L.Y.Dong W.H.Dong V.Druzhinin D.S.Du Y.J.Du Z.G.Du L.M.Duan D.Epifanov Y.L.Fan S.S.Fang Z.J.Fang G.Fedotovich C.Q.Feng X.Feng Y.T.Feng J.L.Fu J.Gao Y.N.Gao P.S.Ge C.Q.Geng L.S.Geng A.Gilman L.Gong T.Gong B.Gou W.Gradl J.L.Gu A.Guevara L.C.Gui A.Q.Guo F.K.Guo J.C.Guo J.Guo Y.P.Guo Z.H.Guo A.Guskov K.L.Han L.Han M.Han X.Q.Hao J.B.He S.Q.He X.G.He Y.L.He Z.B.He Z.X.Heng B.L.Hou T.J.Hou Y.R.Hou C.Y.Hu H.M.Hu K.Hu R.J.Hu W.H.Hu X.H.Hu Y.C.Hu J.Hua G.S.Huang J.S.Huang M.Huang Q.Y.Huang W.Q.Huang X.T.Huang X.J.Huang Y.B.Huang Y.S.Huang N.Hüsken V.Ivanov Q.P.Ji J.J.Jia S.Jia Z.K.Jia H.B.Jiang J.Jiang S.Z.Jiang J.B.Jiao Z.Jiao H.J.Jing X.L.Kang X.S.Kang B.C.Ke M.Kenzie A.Khoukaz I.Koop E.Kravchenko A.Kuzmin Y.Lei E.Levichev C.H.Li C.Li D.Y.Li F.Li G.Li G.Li H.B.Li H.Li H.N.Li H.J.Li H.L.Li J.M.Li J.Li L.Li L.Li L.Y.Li N.Li P.R.Li R.H.Li S.Li T.Li W.J.Li X.Li X.H.Li X.Q.Li X.H.Li Y.Li Y.Y.Li Z.J.Li H.Liang J.H.Liang Y.T.Liang G.R.Liao L.Z.Liao Y.Liao C.X.Lin D.X.Lin X.S.Lin B.J.Liu C.W.Liu D.Liu F.Liu G.M.Liu H.B.Liu J.Liu J.J.Liu J.B.Liu K.Liu K.Y.Liu K.Liu L.Liu Q.Liu S.B.Liu T.Liu X.Liu Y.W.Liu Y.Liu Y.L.Liu Z.Q.Liu Z.Y.Liu Z.W.Liu I.Logashenko Y.Long C.G.Lu J.X.Lu N.Lu Q.F.Lü Y.Lu Y.Lu Z.Lu P.Lukin F.J.Luo T.Luo X.F.Luo Y.H.Luo H.J.Lyu X.R.Lyu J.P.Ma P.Ma Y.Ma Y.M.Ma F.Maas S.Malde D.Matvienko Z.X.Meng R.Mitchell A.Nefediev Y.Nefedov S.L.Olsen Q.Ouyang P.Pakhlov G.Pakhlova X.Pan Y.Pan E.Passemar Y.P.Pei H.P.Peng L.Peng X.Y.Peng X.J.Peng K.Peters S.Pivovarov E.Pyata B.B.Qi Y.Q.Qi W.B.Qian Y.Qian C.F.Qiao J.J.Qin J.J.Qin L.Q.Qin X.S.Qin T.L.Qiu J.Rademacker C.F.Redmer H.Y.Sang M.Saur W.Shan X.Y.Shan L.L.Shang M.Shao L.Shekhtman C.P.Shen J.M.Shen Z.T.Shen H.C.Shi X.D.Shi B.Shwartz A.Sokolov J.J.Song W.M.Song Y.Song Y.X.Song A.Sukharev J.F.Sun L.Sun X.M.Sun Y.J.Sun Z.P.Sun J.Tang S.S.Tang Z.B.Tang C.H.Tian J.S.Tian Y.Tian Y.Tikhonov K.Todyshev T.Uglov V.Vorobyev B.D.Wan B.L.Wang B.Wang D.Y.Wang G.Y.Wang G.L.Wang H.L.Wang J.Wang J.H.Wang J.C.Wang M.L.Wang R.Wang R.Wang S.B.Wang W.Wang W.P.Wang X.C.Wang X.D.Wang X.L.Wang X.L.Wang X.P.Wang X.F.Wang Y.D.Wang Y.P.Wang Y.Q.Wang Y.L.Wang Y.G.Wang Z.Y.Wang Z.Y.Wang Z.L.Wang Z.G.Wang D.H.Wei X.L.Wei X.M.Wei Q.G.Wen X.J.Wen G.Wilkinson B.Wu J.J.Wu L.Wu P.Wu T.W.Wu Y.S.Wu L.Xia T.Xiang C.W.Xiao D.Xiao M.Xiao K.P.Xie Y.H.Xie Y.Xing Z.Z.Xing X.N.Xiong F.R.Xu J.Xu L.L.Xu Q.N.Xu X.C.Xu X.P.Xu Y.C.Xu Y.P.Xu Y.Xu Z.Z.Xu D.W.Xuan F.F.Xue L.Yan M.J.Yan W.B.Yan W.C.Yan X.S.Yan B.F.Yang C.Yang H.J.Yang H.R.Yang H.T.Yang J.F.Yang S.L.Yang Y.D.Yang Y.H.Yang Y.S.Yang Y.L.Yang Z.W.Yang Z.Y.Yang D.L.Yao H.Yin X.H.Yin N.Yokozaki S.Y.You Z.Y.You C.X.Yu F.S.Yu G.L.Yu H.L.Yu J.S.Yu J.Q.Yu L.Yuan X.B.Yuan Z.Y.Yuan Y.F.Yue M.Zeng S.Zeng A.L.Zhang B.W.Zhang G.Y.Zhang G.Q.Zhang H.J.Zhang H.B.Zhang J.Y.Zhang J.L.Zhang J.Zhang L.Zhang L.M.Zhang Q.A.Zhang R.Zhang S.L.Zhang T.Zhang X.Zhang Y.Zhang Y.J.Zhang Y.X.Zhang Y.T.Zhang Y.F.Zhang Y.C.Zhang Y.Zhang Y.Zhang Y.M.Zhang Y.L.Zhang Z.H.Zhang Z.Y.Zhang Z.Y.Zhang H.Y.Zhao J.Zhao L.Zhao M.G.Zhao Q.Zhao R.G.Zhao R.P.Zhao Y.X.Zhao Z.G.Zhao Z.X.Zhao A.Zhemchugov B.Zheng L.Zheng Q.B.Zheng R.Zheng Y.H.Zheng X.H.Zhong H.J.Zhou H.Q.Zhou H.Zhou S.H.Zhou X.Zhou X.K.Zhou X.P.Zhou X.R.Zhou Y.L.Zhou Y.Zhou Y.X.Zhou Z.Y.Zhou J.Y.Zhu K.Zhu R.D.Zhu R.L.Zhu S.H.Zhu Y.C.Zhu Z.A.Zhu V.Zhukova V.Zhulanov B.S.Zou Y.B.Zuo 《Frontiers of physics》 SCIE CSCD 2024年第1期1-154,共154页
The superτ-charm facility(STCF)is an electron–positron collider proposed by the Chinese particle physics community.It is designed to operate in a center-of-mass energy range from 2 to 7 GeV with a peak luminosity of... The superτ-charm facility(STCF)is an electron–positron collider proposed by the Chinese particle physics community.It is designed to operate in a center-of-mass energy range from 2 to 7 GeV with a peak luminosity of 0.5×10^(35) cm^(–2)·s^(–1) or higher.The STCF will produce a data sample about a factor of 100 larger than that of the presentτ-charm factory—the BEPCII,providing a unique platform for exploring the asymmetry of matter-antimatter(charge-parity violation),in-depth studies of the internal structure of hadrons and the nature of non-perturbative strong interactions,as well as searching for exotic hadrons and physics beyond the Standard Model.The STCF project in China is under development with an extensive R&D program.This document presents the physics opportunities at the STCF,describes conceptual designs of the STCF detector system,and discusses future plans for detector R&D and physics case studies. 展开更多
关键词 electron–positron collider tau-charm region high luminosity STCF detector conceptual design
原文传递
New Catalysts for ROMP
10
作者 H.Berke C.Frech +4 位作者 A.Lhamazares O.Blacque H.W.Schmalle C.Adlhart p.chen 《复旦学报(自然科学版)》 CAS CSCD 北大核心 2005年第5期625-626,共2页
1 Introduction Ring Opening Metathesis Polymerization(ROMP)is based on the olefin metathesis reaction,which requires transition metal catalysts.Mainly molybdenum,tungsten and ruthenium based catalysts have up to now b... 1 Introduction Ring Opening Metathesis Polymerization(ROMP)is based on the olefin metathesis reaction,which requires transition metal catalysts.Mainly molybdenum,tungsten and ruthenium based catalysts have up to now been used.The“in-between”metal rhenium was only rarely applied in olefin metathesis reactions,and not at all in ROMP processes.We have found that cationic phosphine substituted dinitrosyl rhenium complexes 1a and 1b effectively catalyze ROMP of norbonene,dicyclopentadiene and of cyclooctene.See Fig.1. 展开更多
关键词 ROMP RHENIUM morbene DFT
在线阅读 下载PDF
上一页 1 下一页 到第
使用帮助 返回顶部