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EFFECT OF CHEMICAL COMPOSITION AND PROCESSES ON THE TEXTURE OF HOT-ROLLED DEEP DRAWING STEEL SHEET 被引量:3
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作者 Y.Chen X.Chen +2 位作者 C.Y.Li x.y.li Y.L.Kang 《Acta Metallurgica Sinica(English Letters)》 SCIE EI CAS CSCD 2002年第3期324-330,共7页
A hot-rolled deep drawing(HDD)steel with high r-value and uniformdistribution of{111}texture in thickness was developed by hot rolling in ferrite region withlubricating between the roller and the steel.The experimenta... A hot-rolled deep drawing(HDD)steel with high r-value and uniformdistribution of{111}texture in thickness was developed by hot rolling in ferrite region withlubricating between the roller and the steel.The experimental results show that the carbon contentand finish rolling temperature have significant effects on beneficial texture{111},and lubricatingduring hot rolling at low temperature in alpha-region makes the distribution of the textureuniform.Three basic requirements needed to meet for HDD steel were concluded by comparing differentcarbon contents and hot rolling processes. 展开更多
关键词 ultra low carbon hot rolling in alpha-region lubricating R-VALUE {111}texture
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Experimental and numerical study of the effect of pulsatile flow on wall displacement oscillation in a flexible lateral aneurysm model 被引量:2
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作者 L.Z.Mu x.y.li +5 位作者 Q.Z.Chi S.Q.Yang P.D.Zhang C.J.Ji Y.He G.Gao 《Acta Mechanica Sinica》 SCIE EI CAS CSCD 2019年第5期1120-1129,共10页
This study experimentally and numerically investigated the effect of pulsatile flow of different frequencies and outflow resistance on wall deformation in a lateral aneurysm.A method for constructing a flexible aneury... This study experimentally and numerically investigated the effect of pulsatile flow of different frequencies and outflow resistance on wall deformation in a lateral aneurysm.A method for constructing a flexible aneurysm model was developed,and a self-designed piston pump was used to provide the pulsatile flow conditions.A fluid-structure interaction simulation was applied for comparison with and analysis of experimental findings.The maximum wall displacement oscillation increased as the pulsation frequency and outflow resistance increased,especially at the aneurysm dome.There is an obvious circular motion of the vortex center accompanying the periodic inflow fluctuation,and the pressure at the aneurysm dome at peak flow increased as the pulsatile flow frequency and terminal flow resistance increased.These results could explain why abnormal blood flow with high frequency and high outflow resistance is one of the risk factors for aneurysm rupture. 展开更多
关键词 LATERAL ANEURYSM In VITRO experiment PULSATILE flow Wall DISPLACEMENT OSCILLATION Fluid-structure interaction simulation
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STUDY ON DYNAMIC J-INTEGRAL OF MECHANICAL HETEROGENEOUS WELDED JOINT
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作者 F.Q.Tian D.Y.He +2 位作者 x.y.li Y.W.Shi D.Zhang 《Acta Metallurgica Sinica(English Letters)》 SCIE EI CAS CSCD 2004年第6期934-939,共6页
Welded joint is a mechanical heterogeneous body, and mechanical heterogeneity has great effect on dynamic fracture behaviour of welded joints. In the present investigation, dynamic response curve and dynamic J-integra... Welded joint is a mechanical heterogeneous body, and mechanical heterogeneity has great effect on dynamic fracture behaviour of welded joints. In the present investigation, dynamic response curve and dynamic J-integral of practical undermatched welded joint and whole base and whole weld three-point-bend (TPB) models containing longitudinal crack are com- puted. Dynamic J-integral is evaluated using virtual crack extension (VCE) method and the computation is performed using MARC finite element code. Because of the effect of inertia, dynamic load response curve of computed model waves periodically. Dynamic J-integral evaluated by VCE method is path independent. The effect of inertia has little influence on dynamic J-integral curve. The value of dynamic J-integral of undermatched welded joint is lower than that of whole base metal and higher than that of whole weld metal. The results establish the foundation of safety evaluation for dynamic loaded welded structures. 展开更多
关键词 virtual crack extension welded joint dynamic response curve dynamic J-integral
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剪切波分裂的复量分析:实例研究
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作者 x.y.li 王广福 《地球物理学进展》 CSCD 1991年第4期110-110,共1页
把复分量分析方法应用于4组剪切波数据:美国克恩县Lost Hills地区四分量单偏移距VSP;巴黎盆地单一震源、二分量多偏移距VSP;Lost Hills地区四分量反射测线二澳大利亚的G^an Creek煤矿煤层内的跨孔测量.在所有上述实例中,分裂的快剪切波... 把复分量分析方法应用于4组剪切波数据:美国克恩县Lost Hills地区四分量单偏移距VSP;巴黎盆地单一震源、二分量多偏移距VSP;Lost Hills地区四分量反射测线二澳大利亚的G^an Creek煤矿煤层内的跨孔测量.在所有上述实例中,分裂的快剪切波(或槽波)的偏振可由地震波特性的色标记录剖面估算.特别是在测线内和测线外震源复分量色标剖面上和源无关的一致性偏振允许可以求得剪切波的偏振涌,而无需旋转仪器和震源的轴.我们的结论是:复分量分析方法有助于由地震剖面识别和估计剪切波的分裂,帮助进行地层解释,并可简化各向异性介质中多分量反射资料的处理过程. 展开更多
关键词 剪切波 偏移距 各向异性介质 槽波 巴黎盆地 地震剖面 复分 处理过程 可由 矿煤层
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剪切波分裂的复量分析:理论
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作者 x.y.li 王广福 《地球物理学进展》 CSCD 1991年第4期109-109,共1页
采用复数运算,把实部和虚部作为两个相互垂直的坐标轴是处理向量偏振数据的一种自然方法。这就是把多分量数据由通常的笛尔卡坐标变换到极坐标,这样做就可计算瞬时振幅和瞬时极性。我们把这种方法称之为复分量分析,波动过程可以用能够... 采用复数运算,把实部和虚部作为两个相互垂直的坐标轴是处理向量偏振数据的一种自然方法。这就是把多分量数据由通常的笛尔卡坐标变换到极坐标,这样做就可计算瞬时振幅和瞬时极性。我们把这种方法称之为复分量分析,波动过程可以用能够表示波动类型各自特征的瞬时特性来表示。这种方法对于用瞬时特性检验剪切波的分裂特别适用,剪切波分裂时的瞬时振幅有几个局部极大值,而瞬时极性是矩形和半三角形的一个组合.剪切波的分裂可由瞬时振幅和偏振的显示来识别,分裂的剪切波的快波的极性和两个剪切波之间的延时可用色标显示来定量.瞬时特性的显示为叠加在一个极性色标显示上的波纹线.采用色标改善了剪切波分裂的识别能力和量化精度. 展开更多
关键词 剪切波 瞬时极 波纹线 局部极大值 色标 波动过程 坐标变换 复分 快波 可由
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Amplitude analysis of the decays D^(0)→π^(+)π^(−)π^(+)π^(−)and D^(0)→π^(+)π^(−)π^(0)π^(0)
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作者 M.Ablikim M.N.Achasov +642 位作者 P.Adlarson O.Afedulidis X.C.Ai R.Aliberti A.Amoroso Q.An Y.Bai O.Bakina I.Balossino Y.Ban H.-R.Bao V.Batozskaya K.Begzsuren N.Berger M.Berlowski M.Bertani D.Bettoni F.Bianchi E.Bianco A.Bortone I.Boyko R.A.Briere A.Brueggemann H.Cai X.Cai A.Calcaterra G.F.Cao N.Cao S.A.Cetin J.F.Chang W.L.Chang G.R.Che G.Chelkov C.Chen C.H.Chen Chao Chen G.Chen H.S.Chen M.L.Chen S.J.Chen S.L.Chen S.M.Chen T.Chen X.R.Chen X.T.Chen Y.B.Chen Y.Q.Chen Z.J.Chen Z.Y.Chen S.K.Choi X.Chu G.Cibinetto F.Cossio J.J.Cui H.L.Dai J.P.Dai A.Dbeyssi R.E.de Boer D.Dedovich C.Q.Deng Z.Y.Deng A.Denig I.Denysenko M.Destefanis F.De Mori B.Fang S.S.Fang W.X.Fang Y.Fang Y.Q.Fang R.Farinelli L.Fava F.Feldbauer G.Felici C.Q.Feng J.H.Feng Y.T.Feng K.Fischer M.Fritsch C.D.Fu J.L.Fu Y.W.Fu H.Gao Y.N.Gao Yang Gao S.Garbolino I.Garzia P.T.Ge Z.W.Ge C.Geng E.M.Gersabeck B.Ding X.X.Ding Y.Ding Y.Ding J.Dong L.Y.Dong M.Y.Dong X.Dong M.C.Du S.X.Du Z.H.Duan P.Egorov Y.H.Fan J.Fang JA.Gilman K.Goetzen L.Gong W.X.Gong W.Gradl S.Gramigna M.Greco M.H.Gu Y.T.Gu C.Y.Guan Z.L.Guan A.Q.Guo L.B.Guo M.J.Guo R.P.Guo Y.P.Guo A.Guskov J.Gutierrez K.L.Han T.T.Han X.Q.Hao F.A.Harris K.K.He K.L.He F.H.Heinsius C.H.Heinz Y.K.Heng C.Herold T.Holtmann P.C.Hong G.Y.Hou X.T.Hou Y.R.Hou Z.L.Hou B.Y.Hu H.M.Hu J.F.Hu T.Hu Y.Hu G.S.Huang K.X.Huang L.Q.Huang X.T.Huang Y.P.Huang T.Hussain F.H\"olzken N.H\"usken N.in der Wiesche M.Irshad J.Jackson S.Janchiv J.H.Jeong Q.Ji Q.P.Ji W.Ji X.B.Ji X.L.Ji Y.Y.Ji X.Q.Jia Z.K.Jia D.Jiang H.B.Jiang P.C.Jiang S.S.Jiang T.J.Jiang X.S.Jiang Y.Jiang J.B.Jiao J.K.Jiao Z.Jiao S.Jin Y.Jin M.Q.Jing X.M.Jing T.Johansson S.Kabana N.Kalantar-Nayestanaki X.L.Kang X.S.Kang M.Kavatsyuk B.C.Ke V.Khachatryan A.Khoukaz R.Kiuchi O.B.Kolcu B.Kopf M.Kuessner X.Kui A.Kupsc W.K\"uhn J.J.Lane P.Larin L.Lavezzi T.T.Lei Z.H.Lei H.Leithoff M.Lellmann T.Lenz C.Li C.Li C.H.Li Cheng Li D.M.Li F.Li G.Li H.Li H.B.Li H.J.Li H.N.Li Hui Li J.R.Li J.S.Li K.Li L.J.Li L.K.Li Lei Li M.H.Li P.R.Li Q.M.Li Q.X.Li R.Li S.X.Li T.Li W.D.Li W.G.Li X.Li X.H.Li X.L.Li x.y.li Y.G.Li Z.J.Li Z.X.Li C.Liang H.Liang H.Liang Y.F.Liang Y.T.Liang G.R.Liao L.Z.Liao Y.P.Liao J.Libby A.Limphirat D.X.Lin T.Lin B.J.Liu B.X.Liu C.Liu C.X.Liu F.Liu F.H.Liu Feng Liu G.M.Liu H.Liu H.B.Liu H.H.Liu H.M.Liu Huihui Liu J.B.Liu J.Y.Liu K.Liu K.Y.Liu Ke Liu L.Liu L.C.Liu Lu Liu M.H.Liu P.L.Liu Q.Liu S.B.Liu T.Liu W.K.Liu W.M.Liu X.Liu X.Liu Y.Liu Y.Liu Y.B.Liu Z.A.Liu Z.D.Liu Z.Q.Liu X.C.Lou F.X.Lu H.J.Lu J.G.Lu X.L.Lu Y.Lu Y.P.Lu Z.H.Lu C.L.Luo M.X.Luo T.Luo X.L.Luo X.R.Lyu Y.F.Lyu F.C.Ma H.Ma H.L.Ma J.L.Ma L.L.Ma M.M.Ma Q.M.Ma R.Q.Ma X.T.Ma X.Y.Ma Y.Ma Y.M.Ma F.E.Maas M.Maggiora S.Malde A.Mangoni Y.J.Mao Z.P.Mao S.Marcello Z.X.Meng J.G.Messchendorp G.Mezzadri H.Miao T.J.Min R.E.Mitchell X.H.Mo B.Moses N.Yu.Muchnoi J.Muskalla Y.Nefedov F.Nerling I.B.Nikolaev Z.Ning S.Nisar Q.L.Niu W.D.Niu Y.Niu S.L.Olsen Q.Ouyang S.Pacetti X.Pan Y.Pan A.Pathak P.Patteri Y.P.Pei M.Pelizaeus H.P.Peng Y.Y.Peng K.Peters J.L.Ping R.G.Ping S.Plura V.Prasad F.Z.Qi H.Qi H.R.Qi M.Qi T.Y.Qi S.Qian W.B.Qian C.F.Qiao J.J.Qin L.Q.Qin X.S.Qin Z.H.Qin J.F.Qiu S.Q.Qu Z.H.Qu C.F.Redmer K.J.Ren A.Rivetti M.Rolo G.Rong Ch.Rosner S.N.Ruan N.Salone A.Sarantsev Y.Schelhaas K.Schoenning M.Scodeggio K.Y.Shan W.Shan X.Y.Shan J.F.Shangguan L.G.Shao M.Shao C.P.Shen H.F.Shen W.H.Shen X.Y.Shen B.A.Shi H.C.Shi J.L.Shi J.Y.Shi Q.Q.Shi R.S.Shi S.Y.Shi X.Shi X.D.Shi J.J.Song T.Z.Song W.M.Song Y.J.Song Y.X.Song S.Sosio S.Spataro F.Stieler Y.J.Su G.B.Sun G.X.Sun H.Sun H.K.Sun J.F.Sun K.Sun L.Sun S.S.Sun T.Sun W.Y.Sun Y.Sun Y.J.Sun Y.Z.Sun Z.Q.Sun Z.T.Sun C.J.Tang G.Y.Tang J.Tang Y.A.Tang L.Y.Tao Q.T.Tao M.Tat J.X.Teng V.Thoren W.H.Tian Y.Tian Z.F.Tian I.Uman Y.Wan S.J.Wang B.Wang B.L.Wang Bo Wang D.Y.Wang F.Wang H.J.Wang J.P.Wang K.Wang L.L.Wang M.Wang Meng Wang N.Y.Wang S.Wang S.Wang T.Wang T.J.Wang W.Wang W.Wang W.P.Wang X.Wang X.F.Wang X.J.Wang X.L.Wang X.N.Wang Y.Wang Y.D.Wang Y.F.Wang Y.L.Wang Y.N.Wang Y.Q.Wang Yaqian Wang Yi Wang Z.Wang Z.L.Wang Z.Y.Wang Ziyi Wang D.Wei D.H.Wei F.Weidner S.P.Wen Y.R.Wen U.Wiedner G.Wilkinson M.Wolke L.Wollenberg C.Wu J.F.Wu L.H.Wu L.J.Wu X.Wu X.H.Wu Y.Wu Y.H.Wu Y.J.Wu Z.Wu L.Xia X.M.Xian B.H.Xiang T.Xiang D.Xiao G.Y.Xiao S.Y.Xiao Y.L.Xiao Z.J.Xiao C.Xie X.H.Xie Y.Xie Y.G.Xie Y.H.Xie Z.P.Xie T.Y.Xing C.F.Xu C.J.Xu G.F.Xu H.Y.Xu Q.J.Xu Q.N.Xu W.Xu W.L.Xu X.P.Xu Y.C.Xu Z.P.Xu Z.S.Xu F.Yan L.Yan W.B.Yan W.C.Yan X.Q.Yan H.J.Yang H.L.Yang H.X.Yang T.Yang Y.Yang Y.F.Yang Y.F.Yang Y.X.Yang Z.W.Yang Z.P.Yao M.Ye M.H.Ye J.H.Yin Z.Y.You B.X.Yu C.X.Yu G.Yu J.S.Yu T.Yu X.D.Yu C.Z.Yuan J.Yuan L.Yuan S.C.Yuan Y.Yuan Z.Y.Yuan C.X.Yue A.A.Zafar F.R.Zeng S.H.Zeng X.Zeng Y.Zeng Y.J.Zeng Y.J.Zeng X.Y.Zhai Y.C.Zhai Y.H.Zhan A.Q.Zhang B.L.Zhang B.X.Zhang D.H.Zhang G.Y.Zhang H.Zhang H.C.Zhang H.H.Zhang H.H.Zhang H.Q.Zhang H.Y.Zhang J.Zhang J.Zhang J.J.Zhang J.L.Zhang J.Q.Zhang J.W.Zhang J.X.Zhang J.Y.Zhang J.Z.Zhang Jianyu Zhang L.M.Zhang Lei Zhang P.Zhang Q.Y.Zhang S.H.Zhang Shulei Zhang X.D.Zhang X.M.Zhang X.Y.Zhang Y.Zhang Y.Zhang Y.T.Zhang Y.H.Zhang Y.M.Zhang Yan Zhang Z.D.Zhang Z.H.Zhang Z.L.Zhang Z.Y.Zhang Z.Y.Zhang G.Zhao J.Y.Zhao J.Z.Zhao L.Zhao Lei Zhao M.G.Zhao R.P.Zhao S.J.Zhao Y.B.Zhao Y.X.Zhao Z.G.Zhao A.Zhemchugov B.Zheng J.P.Zheng W.J.Zheng Y.H.Zheng B.Zhong X.Zhong H.Zhou J.Y.Zhou L.P.Zhou X.Zhou X.K.Zhou X.R.Zhou X.Y.Zhou Y.Z.Zhou J.Zhu K.Zhu K.J.Zhu L.Zhu L.X.Zhu S.H.Zhu S.Q.Zhu T.J.Zhu W.D.Zhu Y.C.Zhu Z.A.Zhu J.H.Zou J.Zu 《Chinese Physics C》 SCIE CAS CSCD 2024年第8期6-33,共28页
Using e^(+)e^(−)annihilation data corresponding to an integrated luminosity of 2.93 fb^(−1)taken at the center-of-mass energy√s=3.773 GeV with the BESIII detector,a joint amplitude analysis is performed on the decays... Using e^(+)e^(−)annihilation data corresponding to an integrated luminosity of 2.93 fb^(−1)taken at the center-of-mass energy√s=3.773 GeV with the BESIII detector,a joint amplitude analysis is performed on the decays D^(0)→π^(+)π^(−)π^(+)π^(−)and D^(0)→π^(+)π^(−)π^(0)π^(0)(non-η).The fit fractions of individual components are obtained,and large interferences among the dominant components of the decays D^(0)→a_(1)(1260)π,D^(0)→π(1300)π,D^(0)→ρ(770)ρ(770),and D^(0)→2(ππ)_(S)are observed in both channels.With the obtained amplitude model,the CP-even fractions of D^(0)→π^(+)π^(−)π^(+)π^(−)and D^(0)→π^(+)π^(−)π^(0)π^(0)(non-η)are determined to be(75.2±1.1_(stat).±1.5_(syst.))%and(68.9±1.5_(stat).±2.4_(syst.))%,respectively.The branching fractions of D^(0)→π^(+)π^(−)π^(+)π^(−)and D^(0)→π^(+)π^(−)π^(0)π^(0)(non-η)are measured to be(0.688±0.010_(stat.)±0.010_(syst.))%and(0.951±0.025_(stat.)±0.021_(syst.))%,respectively.The amplitude analysis provides an important model for the binning strategy in measuring the strong phase parameters of D^(0)→4πwhen used to determine the CKM angleγ(ϕ_(3))via the B^(−)→DK^(−)decay. 展开更多
关键词 BESIII D^(0)meson decays amplitude analysis CP-even fraction
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Stabilizing nanograined Fe-Cr alloy by Si-assisted grain boundary segregation 被引量:1
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作者 X.F.Xu x.y.li B.Zhang 《Journal of Materials Science & Technology》 SCIE EI CAS CSCD 2023年第3期223-233,共11页
Intentional solute segregation at grain boundary(GB)can effectively stabilize the nanograined alloys by reducing the excess energy and mobility of GB,but it usually works for binary alloys with sufficient GB segregati... Intentional solute segregation at grain boundary(GB)can effectively stabilize the nanograined alloys by reducing the excess energy and mobility of GB,but it usually works for binary alloys with sufficient GB segregation tendency.Here,we found that the segregation of Cr can be enhanced in a nanostruc-tured Fe-8Cr alloy with insufficient GB segregation tendency through the interaction of another solute Si(1.0 wt.%).After surface mechanical grinding treatment and subsequent annealing,the nanograined Fe-8Cr-1Si is more thermally stable than the nanograined Fe-8Cr,which is mainly attributed to the Si-enhanced Cr segregation as observed by Super-X energy-dispersive X-ray spectroscopy(EDS)mapping system.With the grain refinement to nanoscale,the thermal stability is further improved due to the in-crease of Cr content at GBs and the precipitates formed at appropriate high temperatures.The present finding provides guidance for the development of advanced nanostructured ternary alloys. 展开更多
关键词 SEGREGATION Grain boundary Fe-Cr-Si alloy NANOCRYSTALLINE Thermal stability
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Compression Stability of Reversed Austenite in 9Ni Steel 被引量:7
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作者 S.H.Chen M.J.Zhao +1 位作者 x.y.li L.J.Rong 《Journal of Materials Science & Technology》 SCIE EI CAS CSCD 2012年第6期558-561,共4页
The effect of compressive stress on the stability of reversed austenite in gNi steel was investigated by uni- axial and hydrostatic compression. It was found that the uniaxial compressive pressure promoted the Υ-α t... The effect of compressive stress on the stability of reversed austenite in gNi steel was investigated by uni- axial and hydrostatic compression. It was found that the uniaxial compressive pressure promoted the Υ-α transformation, while the hydrostatic pressure suppressed the -Υ-α transformation. The pressure dependent transformation behavior can be explained according to thermodynamic analysis. 展开更多
关键词 9Ni steel MARTENSITE Reversed austenite Hydrostatic pressure Uniaxial compressive pressure
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Orientation dependence of mechanically induced grain boundary migration in nano-grained copper 被引量:1
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作者 J.X.Hou x.y.li K.Lu 《Journal of Materials Science & Technology》 SCIE EI CAS CSCD 2021年第9期30-34,共5页
Tensile tests were carried out on gradient nanograined copper samples to investigate the grain orientation dependence of mechanically induced grain boundary migration(GBM) process. The relationship between GBM and the... Tensile tests were carried out on gradient nanograined copper samples to investigate the grain orientation dependence of mechanically induced grain boundary migration(GBM) process. The relationship between GBM and the orientations of nanograins relative to loading direction was established by using electron backscatter diffraction. GBM is found to be more pronounced in the grains with higher Schmid factors where dislocations are easier to slip. As a result, the fraction of high angle grain boundaries decreases and that of low angle grain boundaries increases after GBM. 展开更多
关键词 Grain boundary migration Orientation dependence TEXTURE Nano-grain COPPER
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Transition of deformation mechanisms from twinning to dislocation slip in nanograined pure cobalt
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作者 Y.W.Qi Z.P.Luo +1 位作者 x.y.li K.Lu 《Journal of Materials Science & Technology》 SCIE EI CAS CSCD 2022年第26期124-129,共6页
Deformation mechanisms of nanograined and submicron-grained pure cobalt processed by means of high strain rate shear deformation at cryogenic temperatures were studied.Microstructural analysis revealed a transition of... Deformation mechanisms of nanograined and submicron-grained pure cobalt processed by means of high strain rate shear deformation at cryogenic temperatures were studied.Microstructural analysis revealed a transition of governing deformation mechanism from deformation twinning and dislocation slip in submicron-grains to and dislocations slip in nanograins.Microhardness tests illustrated that the Hall-Petch relation slope changes consequently with the transition of deformation mechanism. 展开更多
关键词 NANOGRAIN COBALT Deformation mechanism Hall-Petch relation
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