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What is going on in magnesium alloys? 被引量:66
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作者 X.J. Wang D.K. Xu +10 位作者 R.Z. Wu X.B. chen Q.M. Peng L. Jin Y.C. Xin Z.Q. Zhang Y. Liu X.H. chen g. chen K.K. Deng H.Y. Wang 《Journal of Materials Science & Technology》 SCIE EI CAS CSCD 2018年第2期245-247,共3页
China has been developed into one of the most active regions in terms of both fundamental and applied research on magnesium (Mg) and its alloys in the world from a solid base laid by its prominent metallurgist and m... China has been developed into one of the most active regions in terms of both fundamental and applied research on magnesium (Mg) and its alloys in the world from a solid base laid by its prominent metallurgist and materials scientists over the past decades. Nowadays, a large number of young-generation researchers have been inspired by their predecessors and become the key participants in the fields of Mg alloys, which consequently led to the establishment of China Youth Scholar Society for Magnesium Alloys Research in 2015. Since then, the first two China Youth Scholars Symposiums on Mg Alloys Research had been held at Harbin (2015) and Chongqing (2016) China, respectively. A number of crucial research inter- ests related to fundamental and applied Mg research were discussed at the conferences and summarized in this short perspective, aiming to boost far-reaching initiatives for development of new Mg-based materials to satisfy the requirements for a broad range of industrial employments. Herein, four main aspects are included as follows: i) Plastic deformation mechanism and strengthening strategy, ii) Design and development of new Mg-based materials, iii) Key service properties, and iv) New processing technologies. 展开更多
关键词 Mg alloys Plastic deformation Strengthening Alloying design High performance Corrosion Fatigue behavior Creep Processing technologies Purification
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Formation of Re-containing Carbides in a Second Generation Directionally Solidified Ni Base Superalloy 被引量:1
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作者 T. Zhao D. Wang +2 位作者 J. Zhang g. chen L.H. Lou 《Journal of Materials Science & Technology》 SCIE EI CAS CSCD 2009年第3期361-364,共4页
The precipitates at grain boundary in a directionally solidified Ni base superalloy after heat treatment, aging at 975℃, and creep rupture test have been characterized. Besides the primary MC carbides and fine partic... The precipitates at grain boundary in a directionally solidified Ni base superalloy after heat treatment, aging at 975℃, and creep rupture test have been characterized. Besides the primary MC carbides and fine particles of u phase, the Re-containing M23C6 was observed. The precipitation kinetics revealed that the formation of M23C6 was associated with the dissolution of u phase and MC carbides. TEM image shows that the continuous precipitation of M23C6 particles effectively hinders the dislocation movement and strengthens the grain boundaries. The high strength of the alloy suggests that M23C6 carbides are beneficial to the properties although Re as an important matrix strengthening element was consumed. 展开更多
关键词 Ni-base Superalloys Directional solidification RHENIUM CARBIDE
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Influence of Planting Date on the Growth and Yield of Different Maturity Group of Soybeans in the Southeastern Coastal Plains of USA
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作者 P. Wiatrak g. chen 《Journal of Agricultural Science and Technology(B)》 2011年第2期251-265,共15页
Planting date is a critical component of soybean [Glycine max (L.) Merr.] production, under dry land conditions in the Southeastern Coastal Plain. The objectives of this study were to 1. Evaluate the effect of plant... Planting date is a critical component of soybean [Glycine max (L.) Merr.] production, under dry land conditions in the Southeastern Coastal Plain. The objectives of this study were to 1. Evaluate the effect of planting date on plant leaf area index (LAI) and normalized difference vegetation index (NDVI) at 60 and 90 days after planting (DAP), plant height and grain yield, and 2. Determine the optimum planting period by integrating the responses from vegetation growth to yield for soybean maturity group (MG) IV-VIII under dry land conditions in the Southeastern Coastal Plain. Planting dates were scheduled about 14-days intervals from late April to mid-July (2008) or late July (2009). Greatest grain yield for MG IV was obtained from planting in around mid-May in both years. The yield was greater for MG V planted in May and greater for MG VI-VIII planted in late April and May, but started to decline for planting in early June. Plant LAI and NDVI at 60 DAP were affected by both planting date and precipitation, but were poorly correlated with grain yield. However, plant LAI and NDVI were well correlated with yield and were greater for May planting dates at 90 DAP. These indiccs declined for soybean planted after May. Mature plant height decreased more rapidly with delayed planting. These results indicate that plant growth and yield decreased after May planting. Optimum planting period for all MGs was early to mid-May. 展开更多
关键词 SOYBEAN planting date leaf area index normalized difference vegetation index grain yield plant growth.
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SIMULATION OF STEEL COIL HEAT TRANSFER IN HPH FURNACE 被引量:3
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作者 M. Y. gu g. chen +1 位作者 M. C. Zhang X. C. Dai 《Acta Metallurgica Sinica(English Letters)》 SCIE EI CAS CSCD 2005年第5期647-652,共6页
The mathematical model has been estublished for the simulation of steel coil's heat transfer during annealing thermal process in HPH (high performance hydrogen) furnace. The equivalent radial thermal conductivity i... The mathematical model has been estublished for the simulation of steel coil's heat transfer during annealing thermal process in HPH (high performance hydrogen) furnace. The equivalent radial thermal conductivity is adopted by statistical analysis regression approach through the combination of a large quantity of production data collected in practice and theoretical analyses. The effect of the number of coils on circulating flow gas is considered for calculating the convection heat transfer coefficient, The temperature within the coil is predicted with the developed model during the annealing cycle including heating process and cooling process. The good consistently between the predicted results and the experimental data has demonstrated that the mathematical model established and the parameters identified by this paper are scientifically feasible and the effective method of calculation for coil equivalent radial heat transfer coefficient and circulating gas flow has been identified successfully, which largely enhances the operability and feasibility of the mathematic- model. This model provides a theoretical basis and an effective means to conduct studies on the impact that foresaid factors may imposed on the steel coil's temperature field, to analyze the stress within coils, to realize online control and optimal production and to increase facilily output by increasing heating and cooling rates of coils without producing higher thermal stress. 展开更多
关键词 FURNACE equivalent radial thermal conductivity convection heat transfer coefficient SIMULATION
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Iron Reduction and Adsorption on Shewanella Putrefaciens nearby Landfills in Northwest Florida 被引量:1
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作者 P.K. Subramaniam L. Martin +2 位作者 P. grasel K. Tawfiq g. chen 《Journal of Environmental Science and Engineering》 2010年第9期60-69,共10页
In Northwest Florida, the soil is mainly covered by poorly drained sandy soil of Myakka, which is characterized by a subsurface accumulation of humus and AI and Fe oxides. When organic rich landfill leachate is leaked... In Northwest Florida, the soil is mainly covered by poorly drained sandy soil of Myakka, which is characterized by a subsurface accumulation of humus and AI and Fe oxides. When organic rich landfill leachate is leaked to the iron rich soils, ferrous iron is released with the oxidation of organic compounds in the leachate. In this research, we investigated the activities of S. putrefaciens in reducing iron oxide in the iron rich soil of Northwest Florida with landfill leachate serving as the carbon source. S. putrefaciens had similar maximum specific growth rate and half saturation coefficients for all the leachate and soil samples. The average maximum specific growth rate was 0.008 hr^-1 and the average half saturation coefficient was 243.8 mg/L. Averagely, 2.2 mg ferrous iron was generated per mg COD consumed. In addition, adsorption of reduced ferrous iron on S. putrefaciens was further characterized. Ferrous iron adsorption on S. putrefaciens was a kinetic process, which increased with the increase of the reaction time. Equilibrium ferrous iron adsorption on S. putrefaciens can be reached after three hours. Ferrous iron had linear adsorption isotherms on S. putrefaciens for the pH range of 5 to 9. 展开更多
关键词 Ferrous iron S. putrefaciens REDUCTION adsorption.
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Tunable Fiber Gratings and Their Applications
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作者 Z. Fang L. Zhao +5 位作者 L. Li K. gao Y. Zhou J. geng R. Qu g. chen 《光学学报》 EI CAS CSCD 北大核心 2003年第S1期223-224,共2页
Some practical research topics on tunable fiber gratings in author's group are presented, including tuning speed, tuning range, tuning characteristics of gratings in HB fiber, and the tunability of the line-width.... Some practical research topics on tunable fiber gratings in author's group are presented, including tuning speed, tuning range, tuning characteristics of gratings in HB fiber, and the tunability of the line-width. The applications of fiber gratings in communication and sensing are also discussed. 展开更多
关键词 been of in as FBG were Tunable Fiber Gratings and Their Applications than have EDFA for that
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Measurement of the integrated Luminosities of cross-section scan data samples around theψ(3770)mass region
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作者 M. Ablikim M. N. Achasov +398 位作者 S. Ahmed M. Albrecht M. Alekseev A. Amoroso F. F. An Q. An Y. Bai O. Bakina R. Baldini Ferroli Y. Ban K. Begzsuren D. W. Bennett J. V. Bennett N. Berger M. Bertani D. Bettoni F. Bianchi E. Boger I. Boyko R. A. Briere H. Cai X. Cai O. Cakir A. Calcaterra g. F. Cao S. A. Cetin J. Chai J. F. Chang W. L. Chang g. Chelkov g. chen H. S. chen J. C. chen M. L. chen P. L. chen S. J. chen X. R. chen Y. B. chen X. K. Chu g. Cibinetto F. Cossio H. a. Dai, J. F. Dai A. Dbeyssi D. Dedovich Z. Y. Deng A. Denig I. Denysenko M. Destefanis F. De Mori Y. Ding C. Dong J. Dong L. Y. Dong M. Y. Dong Z. L. Dou S. X. Du P. F. nuan J. Fang S. S. Fang Y. Fang R. Farinelli L. Fava S. Fegan F. Feldbauer g. Felici C. Q. Feng E. Fioravanti M. Fritsch C. D. Fu Q. gao X. L. gao Y. gao, Y. g. gao Z. gao B. garillon I. garzia A. gilman K. goetzen L. gong W. X. gong W. gradl M. greco L. M. gu M. H. gu Y. T. gu A. q. guo L. B. guo R. P. guo Y. F. guo A. guskov Z. Haddadi S. Han X. Q. Hao F. A. Harris Z. L. He X. O. He F. H. Heinsius T. Held Y. K. Heng T. Holtmann Z. L. Hou H. M. Hu J. F. gu T. Hu Y. Hu g. S. Huang J. S. Huang X. T. Huang X. Z. Huang Z. L. guang T. Hussain W. Ikegami Andersson M Irshad Q. Ji Q. P. Ji X. B. Ji X. L. Ji X. S. Jiang X. Y. Jiang J. B. Jiao Z. Jiao D. P. Jin S. Jin Y. Jin T. Johansson A. Julin N. Kalantar-Nayestanaki X. S. Kang M. Kavatsyuk B. C. Ke T. Khan A. Khoukaz P. Kiese R. Kliemt L. Koch O. B. Kolcu B. Kopf M. Kornicer M. Kuemmel M. Kuessner A. Kupsc M. Kurth W. Kiihn J. S. Lange M. Lara P. Larin L. Lavezzi S. Leiber H. Leithofi C. Li cheng Li D. M. Li F. Li F. Y. Li g. Li H. B. Li H. J. Li J. C. Li J. W. Li K. J. Li Kang Li Ke Li Lei Li P. L. Li P. R. Li Q. Y. Li T. Li W. D. Li W. g. Li X. L. Li X. N. Li X. Q. Li Z. B. Li H. Liang Y. F. Liang Y. T. Liang g. R. Liao L. Z. Liao J. Libby C. X. Lin D. X. Lin S. Liu B. J. Liu C. X. Liu D. Liu D. Y. Liu F. H. Liu Fang Liu Feng Liu H. B. Liu H. L Liu H. M. Liu Huanhuan Liu Huihui Liu J. B. Liu J. Y. Liu K. Liu K. Y. Liu Ke Liu L. D. Liu Q. Liu S. B. Liu X. Liu Y. B. Liu Z. A. Liu Zhiqing Liu Y. F. Long X. C. Lou H. J. Lu J. g. Lu Y. Lu Y. P. Lu C. L. Luo M. X. Luo X. L. Luo S. Lusso X. R. Lyu F. C. Ma H. L. Ma L. L. Ma M. M. Ma Q. M. Ma X. N. Ma X. Y. Ma Y. M. Ma F. E. Maas M. Maggiora Sc Q. A. Malik A. Mangoni Y. J. Mao Z. P. Mao S. Mareello Z. X. Meng J. g. Messehendorp g. Mezzadri J. Min T. J. Min R. E. Mitchell X. H. Mo Y. J. Mo C. Morales Morales g. Morello N. Yu. guchnoi H. Muramatsu A. Mustafa S. Nakhoul Y. Nefedov F. Nerling I. B. Nikolaev Z. Ning S. Nisar S. L. Niu X. Y. Niu S. L. Olsen Q. Ouyang S. Paeetti Y. Pan M. Papenbrock P. Patteri M. Pelizaeus J. Pellegrino H. P. Peng Z. Y. Peng K. Peters J. Pettersson J. L. Ping R. g. Ping A. Pitka R. Poling V. Prasad H. R. Qi M. Qi T. Y. Qi S. Qian C. F. Qiao N. Qin X. S. Qin Z. H. Qin J. F. Qiu K. H. Rashid C. F. Redmer M. Richter M. Ripka M. Rolo g. Rong Ch. Rosner X. D. Ruan A. Sarantseve M. Savrie C. Sehnier K. Sehoenning W. Shan X. Y. Shan M. Shao C. P. Shen P. X. Shen X. Y. Shen H. Y. Sheng X. Shi J. J. Song W. M. Songa X. Y. Song S. Sosio Sc C. Sowa S. Spataro g. X. Sun J. F. Sun L. Sun S. S. Sun X. H. Sun Y. J. Sun Y. K Sun Y. Z. Sun Z. J. Sun Z. T. Sun Y. T Tan C. J. Tang g. Y. Tang X. Tang I. Tapan M. Tiemens B. Tsednee I. Uman g. S. Varner B. Wang B. L. Wang C. W. Wang D. Wang D. Y. Wang Dan Wang K. Wang L. L. Wang L. S. Wang M.Wang Meng Wang P. Wang P. L. Wang W. P. Wang X. F. Wang Y. Wang Y. F. Wang Y. Q. Wang Z. Wang Z. g. Wang Z. Y. Wang Zongyuan Wang T. Weber D. H. Wei P. Weidenkaff S. P. Wen U. Wiedner M. Wolke L. H. Wu L. J. Wu Z. Wu L. Xia X. Xia Y. Xia D. Xiao Y. J. Xiao Z. J. Xiao Y. g. Xie Y. H. Xie X. A. Xiong Q. L. Xiu g. F. Xu J. J. Xu L. Xu Q. J. Xu Q. N. Xu X. P. Xu F. Yan L. Yan W. B. Yan W. C. Yan Y. H. Yan H. J. Yang H. X. Yang L. Yang S. L. Yang Y. H. Yang Y. X. Yang Yi- fan Yang M. Ye M. H. Ye J. H. Yin Z. Y. You B. X. Yu C. X. Yu J. S. Yu C. Z. Yuan Y. Yuan A. Yuncu A. A. Zafar A. Zallo Y. Zeng Z. Zeng 《Chinese Physics C》 SCIE CAS CSCD 2018年第6期1-8,共8页
To investigate the nature of the Ψ(3770) resonance and to measure the cross section for e^+e^-→DD, a cross-section scan data sample, distributed among 41 center-of-mass energy points from 3.73 to 3.89 GeV, was ta... To investigate the nature of the Ψ(3770) resonance and to measure the cross section for e^+e^-→DD, a cross-section scan data sample, distributed among 41 center-of-mass energy points from 3.73 to 3.89 GeV, was taken with the BESIII detector operated at the BEPCII collider in the year 2010. By analyzing the large angle Bhabha scattering events, we measure the integrated luminosity of the data sample at each center-of-mass energy point. The total integrated luminosity of the data sample is 76.16±0.04±0.61 pb^-1, where the first uncertainty is statistical and the second systematic. 展开更多
关键词 Bhabha scattering events integrated luminosity BESⅢ
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