{"currentpage":1,"firstResult":0,"maxresult":10,"pagecode":5,"pageindex":{"endPagecode":5,"startPagecode":1},"records":[{"abstractinfo":"马氏体用变按动力学分为变温相变和等温相变按热力学和界面动态分为热弹性相变、近似热弹性相变和非热弹性相变，其判据为（1）临界相变驱动力小，热滞小；（2）相界面能往复（正、逆）运动；（3）形状应变由弹性协作，马氏体内的弹性储存能对逆相变驱动力作出贡献按形核机制分为近似局域软模形核和层错形核，前者母相强化阻碍相变开动；后老母相强化不影响从，相变内耗峰出现的温度范围未见摸量的明显下降一级相变特性很弱的称为赝马氏体相变","authors":[{"authorName":"徐祖耀","id":"871a2e4a-7e74-4314-9c77-d26b7322dcf0","originalAuthorName":"徐祖耀"}],"categoryName":"|","doi":"","fpage":"45","id":"9b602887-298d-41ff-b20d-d7c0abe85964","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":"ed43cbc9-d811-4e3e-8d13-8ca81ff0d4aa","keyword":"马氏体相变的分类","originalKeyword":"马氏体相变的分类"},{"id":"16a333db-be14-4e4c-a5c7-a0ed8147703a","keyword":"semi-thermoelatic transformation","originalKeyword":"semi-thermoelatic transformation"},{"id":"1d2a715f-cbff-404c-ad53-0023f2eefd85","keyword":" <span style=\"color:red\">local</span> <span style=\"color:red\">soft</span> <span style=\"color:red\">mode</span>","originalKeyword":" local soft mode"},{"id":"788c9365-b577-4239-9683-6f4626da61be","keyword":" nucleation by stacking fault","originalKeyword":" nucleation by stacking fault"},{"id":"93d7013f-c350-47e6-bdf8-17436156c432","keyword":" quasi-martensitic transformation","originalKeyword":" quasi-martensitic transformation"}],"language":"zh","publisherId":"0412-1961_1997_1_3","title":"马氏体相变的分类","volume":"33","year":"1997"},{"abstractinfo":"Finite element analysis was performed to investigate the stresses within and around a <span style=\"color:red\">soft</span> hemispherical particle located on the surface of a hard matrix under a remote external tensile load. The purpose was to understand the effects of neodymium rich particles on the fatigue properties of Ti-55 alloy. Three case studies mere considered. First both particle and matrix mere perfect, second a crack existed within the particle, and third a crack was located in the matrix adjacent to the particle. Numerical results show that <span style=\"color:red\">soft</span> particles cause stress concentration in regions of the matrix adjacent to the particle, but that such stress concentrations are much weaker than those associated with a cavity. A crack within the particle increases the stress concentration in the matrix only a little when the crack is far from the interface. However, a crack in the matrix significantly increases <span style=\"color:red\">local</span> stress in the particle.","authors":[],"categoryName":"|","doi":"","fpage":"463","id":"f615e17f-edee-4b7c-a93a-2b41992af4ff","issue":"4","journal":{"abbrevTitle":"MSAT","id":"5c4ea523-f3ab-4618-9c21-537efff1d7fc","issnPpub":"0267-0836","publisherId":"MSAT","title":"Materials Science and Technology"},"keywords":[{"id":"b6a8a79f-cfa6-4908-bd23-2aecb09f79fa","keyword":"fatigue-crack initiation;finite-element;deformation;composites;alloy","originalKeyword":"fatigue-crack initiation;finite-element;deformation;composites;alloy"}],"language":"en","publisherId":"0267-0836_2000_4_2","title":"Effects of <span style=\"color:red\">soft</span> hemispherical particle on <span style=\"color:red\">local</span> surface stress of hard matrix","volume":"16","year":"2000"},{"abstractinfo":"The terahertz dielectric response of LuFe(2)O(4) is investigated by terahertz time-domain spectroscopy over a temperature range of 6-290 K. It is revealed that besides the central <span style=\"color:red\">mode</span> associated with the charge-ordered state, a <span style=\"color:red\">soft</span> TO(1) <span style=\"color:red\">mode</span> at below similar to 240 K is identified indicating the existence of displacing ferroelectricity, in addition to the charge-ordering-induced ferroelectricity at below 320 K. The anomaly of the <span style=\"color:red\">soft</span> <span style=\"color:red\">mode</span> at similar to 180 K reflects the magnetoelectric correlation between the <span style=\"color:red\">soft</span> TO(1) <span style=\"color:red\">mode</span> and the spin/charge fluctuations revealed recently. Finally, the magnetic property at below similar to 240 K is discussed.","authors":[],"categoryName":"|","doi":"","fpage":"893","id":"9e0cfeee-a540-4b76-a287-0d756d321b70","issue":"4","journal":{"abbrevTitle":"APAS&P","id":"cde04357-7cb8-4746-b682-a64bfb9590d6","issnPpub":"0947-8396","publisherId":"APAS&P","title":"Applied Physics a-Materials Science & Processing"},"keywords":[{"id":"e5af614e-f6cc-4ffb-8a79-d558799a2a8d","keyword":"system lufe2o4;charge;polarization","originalKeyword":"system lufe2o4;charge;polarization"}],"language":"en","publisherId":"0947-8396_2009_4_1","title":"Terahertz spectroscopy of central and <span style=\"color:red\">soft</span> phonon modes in LuFe(2)O(4)","volume":"96","year":"2009"},{"abstractinfo":"Hydrogen induced cracking(HIC)of 0.3% C,1% Cr,1% Mn,1% Si high strength steel has been studied under simple <span style=\"color:red\">mode</span> Ⅰ,<span style=\"color:red\">mode</span> Ⅱ and(Ⅰ+Ⅱ)mixed <span style=\"color:red\">mode</span> loading conditions.Af- ter being hydrogen-charged in IN H_2SO_4 solution,the material behaved hydrogen embrittlement in all the cases studied.The threshold K_(ⅡH)/K_(ⅡX) of HIC under <span style=\"color:red\">mode</span> Ⅱ load- ing was 0.27,which was nearly the same as that K(ⅠH)/K_(ⅠX)=0.29 under <span style=\"color:red\">mode</span> Ⅰ loading. While the thresholds of-HIC under(Ⅰ+Ⅱ)mixed <span style=\"color:red\">mode</span> loading were 0.36,0.41 and 0.37 cor- responding to the K_Ⅱ/K_Ⅰ ratio of 0.27,0.4 and O.81.The results show that simple <span style=\"color:red\">mode</span> Ⅰ or <span style=\"color:red\">mode</span> Ⅱ loading is more susceptible to hydrogen embrittlement than(Ⅰ+Ⅱ)mixed <span style=\"color:red\">mode</span>. For explaining the experimental results,the effects of triaxial stress as well as plastic deformation ahead of crack tip has been discussed.","authors":[{"authorName":"GAO Hua XUE Lijue Shanghai University of Engineering Science","id":"0fc2502e-0847-47c0-b1ff-67364a271477","originalAuthorName":"GAO Hua XUE Lijue Shanghai University of Engineering Science"},{"authorName":"Shanghai","id":"2ae8191f-4894-4f7b-9b34-ae5b029ff299","originalAuthorName":"Shanghai"},{"authorName":"China Associate Professor","id":"6069ee5e-205d-49f4-8530-8131a398977c","originalAuthorName":"China Associate Professor"},{"authorName":"Dept.of Materials","id":"f1b295aa-d96f-4bdb-b19c-16749baba5df","originalAuthorName":"Dept.of Materials"},{"authorName":"Shanghai University of Engineering Science","id":"432efeba-b850-4e60-b69c-bf1c55c4844c","originalAuthorName":"Shanghai University of Engineering Science"},{"authorName":"350 Xianxia Road","id":"0aa0e7ce-407d-4f7c-bf45-b9c71285aea6","originalAuthorName":"350 Xianxia Road"},{"authorName":"Shanghai","id":"f099a3dd-13ab-4678-84d3-1809890c6432","originalAuthorName":"Shanghai"},{"authorName":"China","id":"49dd24c4-5e94-44f7-b3a9-1eba77707dd4","originalAuthorName":"China"}],"categoryName":"|","doi":"","fpage":"279","id":"8ababa1b-2beb-4095-93b0-f334d710ac9c","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":"49820a20-f454-4ea4-b2d0-c520ad9e0327","keyword":"(Ⅰ+Ⅱ)mixed <span style=\"color:red\">mode</span>","originalKeyword":"(Ⅰ+Ⅱ)mixed mode"},{"id":"cafc9217-7b27-49d9-b0e9-3e537d480a40","keyword":"null","originalKeyword":"null"}],"language":"en","publisherId":"1006-7191_1989_4_6","title":"(Ⅰ+Ⅱ)MIXED <span style=\"color:red\">MODE</span> HYDROGEN INDUCED CRACKING","volume":"2","year":"1989"},{"abstractinfo":"Complex structures can be regarded as bring derived from a few basic structures via the <span style=\"color:red\">local</span> twinning at the atomic level. Although quasicrystals and approximants are believed to be the B2 derivatives, the related B2 twinning <span style=\"color:red\">mode</span> is not known. This paper addresses this problem by analysing the twinning property of Al-Cu approximants in an Al3Cu4 sample. Such an analysis leads to the recognition of the B2 chemical-twinning <span style=\"color:red\">mode</span> as 180 degrees/[111]B-2, which is responsible for the pentagonal atomic configuration in the Al-Cu approximants as well as for the pseudofivefold B2 twinning observed on quasicrystal surfaces.","authors":[],"categoryName":"|","doi":"","fpage":"501","id":"603a0e1d-f375-44f5-ae58-8552de20d48b","issue":"3","journal":{"abbrevTitle":"PMAOCMSDAMP","id":"e62fc53d-c8fd-4637-86db-12a39c2dbf47","issnPpub":"0141-8610","publisherId":"PMAOCMSDAMP","title":"Philosophical Magazine a-Physics of Condensed Matter Structure Defects and Mechanical Properties"},"keywords":[{"id":"ac16edd5-7533-4dcf-95d4-0c22ca61f3cc","keyword":"quasi-crystals","originalKeyword":"quasi-crystals"}],"language":"en","publisherId":"0141-8610_1999_3_1","title":"Chemical-twinning <span style=\"color:red\">mode</span> of the B2 structure in relation to Al-Cu approximants","volume":"79","year":"1999"},{"abstractinfo":"Fatigue threshold under mixed-<span style=\"color:red\">mode</span> I and II loading and elastic plane-strain conditions has been studied in dual-phase steels (DPS) of two types of volume fraction of martensite (V(m)) in laboratory air at room temperature. Near-threshold mixed-<span style=\"color:red\">mode</span> (I and II) fatigue crack growth occurs mainly by two mechanisms: shear <span style=\"color:red\">mode</span>, and tensile <span style=\"color:red\">mode</span>. Particular emphasis was placed on the influence of the <span style=\"color:red\">mode</span> II component. The mixed-<span style=\"color:red\">mode</span> threshold is controlled not only by <span style=\"color:red\">mode</span> I displacement but also by the <span style=\"color:red\">mode</span> II component. Apparent- and effective-bound curves (corrected closure) are obtained for the threshold condition and discussed in terms of the shape and size of the plastic region of crack tip; crack surface rubbing; and especially, roughness-induced closure and shear resistance of crack surface that resulted in an extremely high extrinsic-toughening contribution to the mixed-<span style=\"color:red\">mode</span> fatigue threshold values. The ratio of the threshold value of pure <span style=\"color:red\">mode</span> II to that of pure <span style=\"color:red\">mode</span> I (DELTAK(th,II)/DELTAK(th,I) attained highly to 1.9 times; the maximum hoop direction stress-intensity factor range of pure <span style=\"color:red\">mode</span> II branch crack tip is 2.2 times that of pure <span style=\"color:red\">mode</span> I. Obviously, the resistance of pure <span style=\"color:red\">mode</span> II crack growth here is far larger than that of pure <span style=\"color:red\">mode</span> I; the former is just to introduce the shear resistance of crack surface, the latter, to reduce the driving force of crack tip for crack closure. It is proposed that the apparent- and effective-bound curves are nonconservative risky and too conservative for design purposes, respectively. So, the threshold data should be obtained under the specific conditions found by concrete mechanical, microstructural, and environmental factors.","authors":[],"categoryName":"|","doi":"","fpage":"1713","id":"8d683d6d-d97f-4227-b983-fca3d20308b2","issue":"8","journal":{"abbrevTitle":"MAMTAMAMS","id":"3c00bd0a-9b64-4f42-89c3-0e640883446c","issnPpub":"1073-5623","publisherId":"MAMTAMAMS","title":"Metallurgical and Materials Transactions a-Physical Metallurgy and Materials Science"},"keywords":[{"id":"0fd63229-467a-415b-bcee-52302bb7c2ee","keyword":"superposition model;mild-steel;growth;propagation;behavior;microstructures;fracture","originalKeyword":"superposition model;mild-steel;growth;propagation;behavior;microstructures;fracture"}],"language":"en","publisherId":"1073-5623_1994_8_1","title":"MIXED-<span style=\"color:red\">MODE</span>-I AND MIXED-<span style=\"color:red\">MODE</span>-II FATIGUE THRESHOLD AND CRACK CLOSURE IN DUAL-PHASE STEELS","volume":"25","year":"1994"},{"abstractinfo":"Nominal <span style=\"color:red\">mode</span> I and mixed <span style=\"color:red\">mode</span> I/II fatigue tests were carried out using the intermetallic compound Ni3Al(CrB) in the form of single crystal specimens. The effects of crystal orientation and load <span style=\"color:red\">mode</span> on fatigue crack initiation and growth were studied. The fracture surfaces of the single crystals were characterized by a cleavage-like appearance and cracking occurred either on a single {111} plane or on multiple {111} planes irrespective of whether <span style=\"color:red\">mode</span> I or mixed <span style=\"color:red\">mode</span> I/II loadings were applied. It was found that the crack initiation and growth behaviour are dependent on both crystal orientation and applied loading <span style=\"color:red\">mode</span>. The cracking behaviour predicted by three mixed <span style=\"color:red\">mode</span> fracture criteria (MTS, SED and G criteria) in polycrystalline materials under mixed <span style=\"color:red\">mode</span> loading can be understood from the present results on single crystals.","authors":[],"categoryName":"|","doi":"","fpage":"883","id":"3da3bf8d-c448-410c-b3da-e30b87030a44","issue":"6","journal":{"abbrevTitle":"F&FOEM&S","id":"04d17cf7-69ae-4c5c-a2e8-0caa835d6fbb","issnPpub":"8756-758X","publisherId":"F&FOEM&S","title":"Fatigue & Fracture of Engineering Materials & Structures"},"keywords":[{"id":"f13f57e4-6428-409a-a6bf-e8cbf6687955","keyword":"fatigue cracking;mixed <span style=\"color:red\">mode</span> loading;crystallographic orientation;resolved shear stress;Ni3Al(CrB) single crystals;growth;alloy","originalKeyword":"fatigue cracking;mixed mode loading;crystallographic orientation;resolved shear stress;Ni3Al(CrB) single crystals;growth;alloy"}],"language":"en","publisherId":"8756-758X_1997_6_1","title":"<span style=\"color:red\">Mode</span> I and mixed <span style=\"color:red\">mode</span> I/II fatigue cracking in Ni3Al(CrB) single crystals","volume":"20","year":"1997"},{"abstractinfo":"We have observed an interface vibrational <span style=\"color:red\">mode</span> in CdSe/ZnTe superlattices (SL's) by Raman scattering. The frequency of this interface <span style=\"color:red\">mode</span> lies above the optical-phonon bands of bulk CdSe and ZnTe compounds, and the ion displacements in the <span style=\"color:red\">mode</span> are sharply localized at the Zn-Se interfaces of the SL's. When the force constants of all four kinds of bonds in the SL's are taken to have thc same values as in the corresponding bulk compounds, the frequency of this interface <span style=\"color:red\">mode</span>, 222 cm-1, calculated using the linear-chain model is consistent with the experimental result, 222 cm-1. Both the smaller masses and the larger force constants of the interface bonds in the SL's rather than the mass effect alone, suggested previously, favor the appearance of the interface modes.","authors":[],"categoryName":"|","doi":"","fpage":"12141","id":"932a5037-45e9-4370-91b2-5b735f35123d","issue":"20","journal":{"abbrevTitle":"PRB","id":"41d73232-e732-4216-a5f7-4b352bb955cf","issnPpub":"0163-1829","publisherId":"PRB","title":"Physical Review B"},"keywords":[{"id":"bab67aea-9ead-4664-a56c-9855f187bd1a","keyword":"phonons","originalKeyword":"phonons"}],"language":"en","publisherId":"0163-1829_1992_20_1","title":"INTERFACE VIBRATIONAL-<span style=\"color:red\">MODE</span> IN CDSE/ZNTE SUPERLATTICES","volume":"45","year":"1992"},{"abstractinfo":"The thin foil specimen of a ferrite-austenite duplex stainless steel was tensiled under transmis- sion electron microscope(TEM).It was found that both in ferrite and austenite the <span style=\"color:red\">local</span> deformation band at crack tip was formed near to the crack propagating direction.Its forma- tion was related with the crack tip Schmid factor,dislocation shielding,latent hardening and hardening coefficient.When the crack tip emitted dislocations to a slip system by the action of pure <span style=\"color:red\">mode</span> Ⅱ stress resolute,and the decreasing rate of hardening coefficient was suitable,lo- cal deformation band was easy to form.","authors":[{"authorName":"YAO Kefu University of Science and Technology Beijing","id":"57ccead7-9d11-4e85-91ed-a16a7e4d7d1c","originalAuthorName":"YAO Kefu University of Science and Technology Beijing"},{"authorName":"Beijing","id":"8fde0e6f-fa1b-44b8-8fa5-b2b4582526c4","originalAuthorName":"Beijing"},{"authorName":"ChinaTANG Naivong CHEN Nanping Tsinghua University","id":"eea8cc24-b6d7-44e4-aef3-cfd96847102d","originalAuthorName":"ChinaTANG Naivong CHEN Nanping Tsinghua University"},{"authorName":"Beijing","id":"215e1912-c540-4acb-9a1a-d377717127b3","originalAuthorName":"Beijing"},{"authorName":"China","id":"7394117d-4506-4dab-9580-7d7e4be2b62e","originalAuthorName":"China"}],"categoryName":"|","doi":"","fpage":"147","id":"832eda0e-86f0-41ab-9d06-f304deaeb125","issue":"3","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":"acdde4d5-1153-4e63-b3b9-3a5d2289f7f7","keyword":"crack tip","originalKeyword":"crack tip"},{"id":"7a668516-0c01-4dc2-a867-9a03e0f71b9d","keyword":"null","originalKeyword":"null"},{"id":"0294b5e6-92f6-4558-985c-5624771608f4","keyword":"null","originalKeyword":"null"}],"language":"en","publisherId":"1006-7191_1992_3_5","title":"TEM OBSERVATION OF <span style=\"color:red\">LOCAL</span> DEFORMATION BAND AT CRACK TIP","volume":"5","year":"1992"},{"abstractinfo":"<FONT face=Verdana>There are significant effects of process parameters on internal qualities of bloom, and these process parameters are as follows: position and reduction amount, reduction distribution, reduction rate, and so on. Developing a control model is the key to apply <span style=\"color:red\">soft</span> reduction technology successfully. As the research object, 360 mm×450 mm bloom caster in PISCO (Panzhihua Iron and Steel Co) has been studied, and the research method for control model of dynamic <span style=\"color:red\">soft</span> reduction has been proposed. On the basis of solidification and heat transfer model, the position of <span style=\"color:red\">soft</span> reduction and reduction distribution of each frame are determined according to the bloom temperature distribution and solid fraction in bloom center calculated. Production practice shows that the ratio of center porosity which is less than or equal to 10, increased to 9727%, ratio of central segregation which is less than or equal to 05, increased to 8091%, and ratio of central carbon segregation index which is more than or equal to 110, decreased to 4% with the applying model of dynamic <span style=\"color:red\">soft</span> reduction.</FONT>","authors":[{"authorName":"CHEN Yong","id":"474ef6e9-68c3-42e6-b216-a84530c9025a","originalAuthorName":"CHEN Yong"},{"authorName":"JI Cheng","id":"fc51be4c-35fc-4acb-8e4d-7850251e7bbc","originalAuthorName":"JI Cheng"},{"authorName":"ZHU Miaoyong","id":"82350722-1fb0-47d9-8f4b-7f79dbf86b1d","originalAuthorName":"ZHU Miaoyong"},{"authorName":"WU Guorong","id":"79fb43d1-5104-44fd-9c75-2c1ef2fe4791","originalAuthorName":"WU Guorong"}],"categoryName":"|","doi":"","fpage":"31","id":"74aca0d0-8adc-44a6-a6c8-4f51aeabb3e9","issue":"9","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":"fbbca9d7-8633-41d4-bb57-91c04997316d","keyword":"bloom continuous casting;dynamic <span style=\"color:red\">soft</span> reduction;control model;center porosity;central segregation","originalKeyword":"bloom continuous casting;dynamic soft reduction;control model;center porosity;central segregation"}],"language":"en","publisherId":"1006-706X_2010_9_6","title":"Control Model of Bloom Dynamic <span style=\"color:red\">Soft</span> Reduction","volume":"17","year":"2010"}],"totalpage":138,"totalrecord":1374}