{"currentpage":1,"firstResult":0,"maxresult":10,"pagecode":5,"pageindex":{"endPagecode":5,"startPagecode":1},"records":[{"abstractinfo":"采用Potts模型Monte Carlo方法对3种现存的三维个体晶粒长大速率拓扑依赖性\n方程进行了仿真验证. 结果表明, Rivier速率方程认为晶粒\n体积变化率dVf/dt与晶粒面数f成线性关系, 与仿真\n结果明显不符, 不适用于描述三维晶粒长大过程的动力\n学. 当晶粒面数f≥8时, Yu-Liu速率方程和\nMacPherson-Srolovitz速率方程均与仿真结果很好吻合,\n表明这两者均可以用来定量描述三维晶粒长大过程的动力学;当\nf<8时, 这两个方程均与仿真结果有显著差异.","authors":[{"authorName":"王浩","id":"4520bc40-73ff-4fe0-ad04-dada21a66155","originalAuthorName":"王浩"},{"authorName":"刘国权","id":"3e4e217d-2a80-4b05-8197-b2e52e7e6750","originalAuthorName":"刘国权"},{"authorName":"秦湘阁","id":"66aa648a-1b1d-4499-86db-9dac627280d6","originalAuthorName":"秦湘阁"}],"categoryName":"|","doi":"","fpage":"13","id":"075a785f-8718-477c-a4ac-8719e1cf5f9b","issue":"1","journal":{"abbrevTitle":"JSXB","coverImgSrc":"journal/img/cover/JSXB.jpg","id":"48","issnPpub":"0412-1961","publisherId":"JSXB","title":"金属学报"},"keywords":[{"id":"b09e3662-9f08-4a8e-bd64-95f5706d5f51","keyword":"三维晶粒长大","originalKeyword":"三维晶粒长大"},{"id":"c24e1f7b-4f9f-4982-b5ad-c9fed7c85b04","keyword":"topology-dependent grain growth rate equation","originalKeyword":"topology-dependent grain growth rate equation"}],"language":"zh","publisherId":"0412-1961_2008_1_16","title":"三维晶粒长大速率方程的大尺度Potts模型Monte Carlo仿真验证","volume":"44","year":"2008"},{"abstractinfo":"The mechanism of grain structure evolution during directional solidification is a fundamental subject in material science. Within the published research there exist conflicting views on the mechanism of grain overgrowth. To study the effect of solidification rate on grain structure evolution, bi-crystals samples were produced in a nickel-base superalloy at different solidification rates. It was found that at the convergent grain boundaries those grains better aligned with respect to the heat flux more readily overgrew neighbouring grains with misaligned orientations and the effect became more pronounced as solidification rate was increased. However, at diverging grain boundaries the rate of overgrowth was invariant to the solidification rate. These experimental results were compared with models in the literature. Thus, a better insight into competitive grain growth in directional solidification processes was obtained.","authors":[],"categoryName":"|","doi":"","fpage":"1327","id":"5b699b94-a379-4092-a0fd-b84069e89008","issue":"5","journal":{"abbrevTitle":"SCS","id":"8e02334e-0007-4675-9eda-1bc1d39b75d9","issnPpub":"1674-7321","publisherId":"SCS","title":"Science China-Technological Sciences"},"keywords":[{"id":"7bd923d7-d135-4636-9177-8e9b0e49e2a9","keyword":"competitive grain growth;structure evolution;directional;solidification;nickel alloys;x-ray;selection;morphologies;orientation;prediction;evolution;alloy","originalKeyword":"competitive grain growth;structure evolution;directional;solidification;nickel alloys;x-ray;selection;morphologies;orientation;prediction;evolution;alloy"}],"language":"en","publisherId":"1674-7321_2012_5_1","title":"Effect of solidification rate on competitive grain growth in directional solidification of a nickel-base superalloy","volume":"55","year":"2012"},{"abstractinfo":"The effect of electropulsing on nanocrystalline grain growth in amorphous material is considered. A size-dependent growth rate of a nanoscale grain is revealed, which is due to the size-dependent electrical resistivity. A suspension effect is found when the density of electric current is at a critical value j(c). The formed grain may shrink when the density of applied electric current is higher than j(c). Numerical calculation shows that j(c) is about 2.59 x 10(3) A/mm(2) for nanocrystalline Ni80P20 alloy with grain size of 13 nm. (C) 1998 Acta Metallurgica Inc.","authors":[],"categoryName":"|","doi":"","fpage":"71","id":"df5f4b2a-e4d3-4019-bb73-13aa67ed205f","issue":"1","journal":{"abbrevTitle":"NM","id":"cc88b34d-fd3e-4cdd-8396-bdba97e827f1","issnPpub":"0965-9773","publisherId":"NM","title":"Nanostructured Materials"},"keywords":[{"id":"2eb0466b-f83f-42b5-88df-c9d618f39e77","keyword":"passing electric-current;structural relaxation;amorphous cu50ti50;crystallization;resistivity;alloys","originalKeyword":"passing electric-current;structural relaxation;amorphous cu50ti50;crystallization;resistivity;alloys"}],"language":"en","publisherId":"0965-9773_1998_1_1","title":"Suspension effect of nanocrystalline grain growth under electropulsing","volume":"10","year":"1998"},{"abstractinfo":"Grain growth process in nanocrystalline Ni-P alloys was investigated by use of differential scanning calorimetry and x-ray diffraction. Two exothermal peaks which result from grain growth processes of Ni3P and Ni crystallites, respectively, have been detected upon heating the nanocrystalline samples at constant heating rates. Activation energies for the two processes of grain growth were calculated by means of the relationship of grain growth temperature and heating rate using the Kissinger equation. Average interfacial energies of Ni3P/Ni3P grain boundary and Ni3P/Ni boundary were determined from the heat released during grain growth.","authors":[],"categoryName":"|","doi":"","fpage":"7345","id":"b371f36b-6a13-4168-a685-6e07d5804668","issue":"10","journal":{"abbrevTitle":"JOAP","id":"7dcf8a89-0513-40ee-be2d-759941dcef7e","issnPpub":"0021-8979","publisherId":"JOAP","title":"Journal of Applied Physics"},"keywords":[],"language":"en","publisherId":"0021-8979_1991_10_5","title":"GRAIN-GROWTH KINETICS AND INTERFACIAL ENERGIES IN NANOCRYSTALLINE NI-P ALLOYS","volume":"69","year":"1991"},{"abstractinfo":"A novel parameter is suggested for evaluating the fatigue crack growth rate in carbonsteels.Fatigue crack propagation tests of an annealed 0.42% carbon steel were carriedout under different conditions to investigate the relationship between this dominatingparameter and the crack opening displacement (COD).A new equation of fatiguecrack growth rate is formulated in terms of the suggested parameter.The physicalmeanings of the material parameters in this equation are explored experimentally.Considering the relation of crack growth and deformation properties,a simple andapplicable method is proposed to evaluate the fatigue crack growth rate.It is alsoobserved that the material parameters in the fatigue crack growth rate equation ofcarbon steels are related linearly to the material strength.The results are in a goodagreement with experimental results.","authors":[{"authorName":"X.S.Wang","id":"aadfdd1d-4401-4f9f-b0c2-4f024a356ffd","originalAuthorName":"X.S.Wang"},{"authorName":" S.Q.Zhu","id":"09a54693-f5cd-46ae-a229-ea5626c1f05e","originalAuthorName":" S.Q.Zhu"}],"categoryName":"|","doi":"","fpage":"271","id":"61c95c01-3cbb-4db7-b9f4-191887c99f51","issue":"4","journal":{"abbrevTitle":"JSXBYWB","coverImgSrc":"journal/img/cover/amse.jpg","id":"49","issnPpub":"1006-7191","publisherId":"JSXBYWB","title":"金属学报(英文版)"},"keywords":[{"id":"6903a57f-239a-49d8-acaa-c61b98b54e40","keyword":"crack opening displacement","originalKeyword":"crack opening displacement"},{"id":"8d77f92a-df31-4336-8060-3fa4fa39eed7","keyword":"null","originalKeyword":"null"},{"id":"dd006637-ef76-4576-9a75-20354647f5cf","keyword":"null","originalKeyword":"null"},{"id":"91d28554-1abc-4083-aef0-a60d92736fa3","keyword":"null","originalKeyword":"null"}],"language":"en","publisherId":"1006-7191_2001_4_9","title":"A NOVEL PARAMETER FOR EVALUATING THE FATIGUE CRACK GROWTH RATE IN CARBON STEELS","volume":"14","year":"2001"},{"abstractinfo":"From single phase to two-phase alloys, creep crack growth behavior of Fe-15Cr-25Ni austenitic steels has been examined for different grain sizes at 973 and 1123 K. The creep crack growth rate increases with increasing grain size. An equation was found to describe the relation between the initiation time t(i) or rupture time t(r) and grain size d: t(r(i)) . d(beta) = C. The precipitation of grain boundary carbide decreases the effect of grain size on creep crack growth. Different grain size dependences on creep crack growth in other materials were also analysed. A damage model based on constrained cavity growth was shown to provide good predictions on the grain size effect on creep crack growth behavior.","authors":[],"categoryName":"|","doi":"","fpage":"450","id":"6d7b0e6a-077a-4c22-ac0e-fadf166dd18f","issue":"5","journal":{"abbrevTitle":"MTJ","id":"2d4614a6-de1c-4df9-ba6b-a783f09d7b2d","issnPpub":"0916-1821","publisherId":"MTJ","title":"Materials Transactions Jim"},"keywords":[{"id":"94fa5239-e5c8-4ee4-a6f6-6fd06f093b22","keyword":"creep;crack growth rate;rupture time;grain size;austenitic steel","originalKeyword":"creep;crack growth rate;rupture time;grain size;austenitic steel"}],"language":"en","publisherId":"0916-1821_1993_5_1","title":"GRAIN-SIZE DEPENDENCE OF CREEP CRACK-GROWTH IN NI-CR AUSTENITIC STEELS","volume":"34","year":"1993"},{"abstractinfo":"Abstract: Growth process of δ-phase was studied during the solidification of carbon steel. Through analyzing the solute diffusion around cylindrical crystals in the melt, the mathematic representation of lateral growth rate of cylindrical crystals was confirmed; the calculation and analysis of lateral growth rate were carried out. In order to validate the theoretical calculation and analysis, the growth process of δ-phase during the solidification was in-situ observed using a confocal scaning laser microscope (CSLM) and the growth rates were measured through CSLM images. The results show that lateral growth rates of δ-phase in the carbon steel first rapidly decrease with the increase of the radius of the cylindrical crystal, and then slowly fall down or maintain invariable. The radius of δ-phase is the primary factor to affect the growth rate. The higher the temperature gradient is, the bigger the growth rate is. However, the effect of the temperature gradient is feeble. Good correlation is obtained between theoretical analysis and experiment results in absolute values of lateral growth rate and change rule.","authors":[{"authorName":"CHANG Guo-wei","id":"16d2b16a-1e62-4775-965d-e6303774f69a","originalAuthorName":"CHANG Guo-wei"},{"authorName":"CHEN Shu-ying","id":"f80f6bd3-433b-41aa-b358-dc365a96301a","originalAuthorName":"CHEN Shu-ying"},{"authorName":"LI Qing-chun","id":"7b64a668-dda0-4852-bf60-efbd0bdbcf99","originalAuthorName":"LI Qing-chun"},{"authorName":"YUE Xu-dong","id":"c334a3bd-1135-4753-bd5f-db7c2aa0a5d7","originalAuthorName":"YUE Xu-dong"},{"authorName":"JIN Guang-can","id":"402679a9-a449-4846-a5ce-7d17dc3d8016","originalAuthorName":"JIN Guang-can"}],"categoryName":"|","doi":"","fpage":"28","id":"7fe2ba51-30c0-45ed-83e3-5207d057eb8c","issue":"4","journal":{"abbrevTitle":"GTYJXBYWB","coverImgSrc":"journal/img/cover/GTYJXBEN.jpg","id":"1","issnPpub":"1006-706X","publisherId":"GTYJXBYWB","title":"钢铁研究学报(英文版)"},"keywords":[{"id":"e66ff7bd-b9c9-422a-840e-a34edc8a935d","keyword":"Key words: cell growth ","originalKeyword":"Key words: cell growth "},{"id":"f43a05ef-ddfa-4f97-8abf-7f5a73f43bb8","keyword":" solidification process ","originalKeyword":" solidification process "},{"id":"54ee7352-594f-4cea-9638-ddcd1a3f01f9","keyword":" carbon steel ","originalKeyword":" carbon steel "},{"id":"4a8fb7ed-59ef-45ea-a08a-d93e8d00a0eb","keyword":" in-situ observation","originalKeyword":" in-situ observation"}],"language":"en","publisherId":"1006-706X_2012_4_11","title":"Lateral Growth Rate of Cells in Melt","volume":"19","year":"2012"},{"abstractinfo":"A single phase HfNi5 nanocrystalline (NC) sample was prepared by quenching a Hf11Ni89 alloy with the melt-spinning technique. A randomly oriented HfNi5 nanophase material with an average grain size of about 10 nm was formed in the as-quenched state. Differential scanning calorimetry (DSC), transmission electron microscopy (TEM), and X-ray diffraction (XRD) analysis were used for the investigation of the thermal stability and grain growth of the NC HfNi5 sample. On heating the NC sample at a constant heating rate, two exothermal peaks appear in the DSC curve, corresponding to a grain-growth process of the HfNi5 nanophase prior to a precipitation process of Ni solid solution. It was found the grain-growth temperature of the NC HfNi5 phase is approximately equal to the crystallization temperature of the same compositional amorphous alloy. The average grain boundary energy in the NC sample calculated by means of the calorimetric results, is about 0.36J/m(2). Activation energies for the grain growth and Ni precipitation are calculated by using the Kissinger equation. It was obtained that the value of the activation energy for the HfNi5 nanophase grain growth is close to that for the volume self-diffusion in Hf. The grain growth mechanism and the thermal stability of the NC material are also discussed.","authors":[],"categoryName":"|","doi":"","fpage":"2641","id":"45f7b94b-818c-4c99-be95-424a7b028e37","issue":"7","journal":{"abbrevTitle":"AMEM","id":"4f81a190-bef1-4aad-9252-7d3fd7514903","issnPpub":"0956-7151","publisherId":"AMEM","title":"Acta Metallurgica Et Materialia"},"keywords":[{"id":"9cd3076f-4d27-4e3c-bec4-d8256d263b37","keyword":"ni-p alloys;nanocrystalline","originalKeyword":"ni-p alloys;nanocrystalline"}],"language":"en","publisherId":"0956-7151_1995_7_1","title":"THERMAL-STABILITY AND GRAIN-GROWTH OF A MELT-SPUN HFNI5 NANOPHASE ALLOY","volume":"43","year":"1995"},{"abstractinfo":"The available experimental results have been summarized concerning the effect of grain size on minimum creep rate.There are two types of creep rate-grain size relations.One is that there is a criti- cal grain size above which creep rate is independent of grain size,below which creep rate increases with the decrease of grain size.The other is that there is an intermediate grain size at which creep resistance is optimum.The first relation usually occurs at higher temperatures(>0.5 T_m),and intermediate stress ranges,while the second relation at interme- diate temperature ranges(0.4-0.5 T_m)and higher stresses.For the two types of creep rate-grain size relations,the increase of the creep rates with the de- crease of grain size for small grain sizes is all due to grain boundary sliding.For large grain sizes,a dis- location climb mechanism is dominant in creep deformation for the first relation,while a Hall-Perch grain boundary strengthening effect is believed to play an important role by dislocation glide mechanism for the second relation.","authors":[{"authorName":"LI Pei'en ** Institute of Materials Science and Engineering","id":"e40c6329-7ed8-44a4-9890-2e14279f7bf8","originalAuthorName":"LI Pei'en ** Institute of Materials Science and Engineering"},{"authorName":"Shanghai Jiaotong University","id":"4361bd10-f54c-458e-b92a-b3320afa646f","originalAuthorName":"Shanghai Jiaotong University"},{"authorName":"Shanghai 200030","id":"2fdc20e7-ebab-4e6a-9c6d-31b9cb1ff9ed","originalAuthorName":"Shanghai 200030"},{"authorName":"China+ To whom correspondence should be addressed.","id":"39b14400-db67-4e4f-8312-986dcdb02167","originalAuthorName":"China+ To whom correspondence should be addressed."}],"categoryName":"|","doi":"","fpage":"119","id":"20a0a2c9-cbbe-4323-a9bb-da5fdff60672","issue":"2","journal":{"abbrevTitle":"CLKXJSY","coverImgSrc":"journal/img/cover/JMST.jpg","id":"11","issnPpub":"1005-0302 ","publisherId":"CLKXJSY","title":"材料科学技术(英文)"},"keywords":[{"id":"0075c70d-ed70-4b02-9753-7bbaa31fd532","keyword":"grain size","originalKeyword":"grain size"},{"id":"e5abcdfc-2374-49d6-9672-f9facd6c3650","keyword":"null","originalKeyword":"null"}],"language":"en","publisherId":"1005-0302_1992_2_1","title":"On Grain Size Dependence of Minimum Creep Rate","volume":"8","year":"1992"},{"abstractinfo":"A two-dimensional mesoscale cellular automaton algorithm is developed to Simulate curvature-driven grain growth during materials processing. In the present model, a deterministic switch rule for the grain growth is adopted, and thus the kinetics of the grain growth can be simulated quantitatively. In addition, the grain-boundary energy is dependent oil the misorientation between neighboring grains. At mesoscale, the simulations show that each grain displays a unique growth behavior. The growth behavior of individual grains can be categorized into four types: (1) grains with monotonically increasing equivalent diameters, (2) grains that first grow and then begin to shrink, (3) grains with almost constant diameters, and (4) grains that decrease in size. Furthermore, an oscillation grain-growth in the present mesoscale cellular automation simulations. This Simulated growth behavior is observed individual grain-growth behavior has not been reported in the literature.","authors":[],"categoryName":"|","doi":"","fpage":"119","id":"6b232b2b-c681-4f1d-9bd9-b2ef6c9a8d73","issue":"1","journal":{"abbrevTitle":"MAMTBMAMPS","id":"1e3b53b7-9441-4ffb-b571-357d5a6a4f9b","issnPpub":"1073-5615","publisherId":"MAMTBMAMPS","title":"Metallurgical and Materials Transactions B-Process Metallurgy and Materials Processing Science"},"keywords":[{"id":"acf0324f-984c-4a13-90a6-a42fc48c743c","keyword":"vertex dynamics simulation;computer-simulation;2 dimensions;solidification;kinetics;recrystallization;boundary;alloys","originalKeyword":"vertex dynamics simulation;computer-simulation;2 dimensions;solidification;kinetics;recrystallization;boundary;alloys"}],"language":"en","publisherId":"1073-5615_2006_1_1","title":"A mesoscale cellular automaton model for curvature-driven grain growth","volume":"37","year":"2006"}],"totalpage":550,"totalrecord":5495}