{"currentpage":1,"firstResult":0,"maxresult":10,"pagecode":5,"pageindex":{"endPagecode":5,"startPagecode":1},"records":[{"abstractinfo":"The martensitic transformation behavior of FeMnGe alloy (0-6 wt% Gel was investigated by resistivity and dilation methods. Ge depresses the martensitic transformation of FeMn alloy. The effect of Ge on starting temperature of martensitic transformation (M-s) temperature of FeMn alloy is -12 K/wt% Ge. Comparing Ge (4S(2)4p(2)) with Si (3S(2)3p(2)) and Al (3S(2)3P(1)), which have similar outer shells of electrons, we found that their effects on the M-s of FeMn alloy are completely different. The result suggests that the outer shell of electron is not the main factor governing the M-s temperature of FeMn alloy, although it is essential in the alloy's antiferromagnetic transition.","authors":[],"categoryName":"|","doi":"","fpage":"329","id":"df475b01-f8fb-4156-9a76-10448f1bb164","issue":"2","journal":{"abbrevTitle":"JOMR","id":"155c387a-c8cb-4083-85f3-6b58aeef4116","issnPpub":"0884-2914","publisherId":"JOMR","title":"Journal of Materials Research"},"keywords":[{"id":"463276c9-9d28-4008-b555-b9e3334eb77b","keyword":"shape memory alloys;transition","originalKeyword":"shape memory alloys;transition"}],"language":"en","publisherId":"0884-2914_2000_2_1","title":"Martensitic transformation behavior of FeMnGe alloys","volume":"15","year":"2000"},{"abstractinfo":"Martensitic transformation in Ni(2+x)Mn(1-x)Ga alloys is known to be controlled by the soft tetragonal elastic constant C' of the high-temperature austenitic phase. The temperature (T) and composition (x) dependence of C'(T, x) are calculated using the first-principles exact muffin-tin orbitals method. We show that the temperature factor of C' is dominated by the phonon-smearing term. The competition between the negative alloying effect (partial derivative C'/partial derivative x < 0) and the positive temperature effect (partial derivative C'/partial derivative T > 0) is found to lead to nearly constant C'(T(M)(x), x) at the critical temperature TM(x). We demonstrate that a proper account of the temperature and composition dependence of C'(T, x) is indispensable for reasonable theoretical TM(x) values. VC 2011 American Institute of Physics. [doi: 10.1063/1.3603935]","authors":[],"categoryName":"|","doi":"","fpage":"","id":"a51efcb4-3438-4b44-91d5-75dfe8e75f75","issue":"26","journal":{"abbrevTitle":"APL","id":"5e3c428a-be96-46d5-bcb9-94a4fce832b0","issnPpub":"0003-6951","publisherId":"APL","title":"Applied Physics Letters"},"keywords":[{"id":"d15316f6-f8d5-4c7c-adc2-a87bec35395a","keyword":"phase","originalKeyword":"phase"}],"language":"en","publisherId":"0003-6951_2011_26_2","title":"Interplay between temperature and composition effects on the martensitic transformation in Ni(2+x)Mn(1-x)Ga alloys","volume":"98","year":"2011"},{"abstractinfo":"gamma-Fe(5.90-10.9 at. % N) nanoparticles ranging in diameters from 30 to 100 nm were prepared by laser-induced pyrolysis of mixtures of Fe(CO)(5) and NH3. During the quenching from high temperature to room temperature and even down to 4.2 K, no martensitic transformation occurred in these particles. Based on the effects of surface tension and refinement of grain size on the yield strength of the nanoparticles, the dependencies of nucleation driving force and the martensite-start temperature on the particle size was revealed, from a viewpoint of thermodynamics of martensitic transformation in the gamma-Fe(N) nanoparticles. It is suggested that the yield strength increment due to the surface tension and to the very fine crystallite grains is probably the predominant aspect responsible for inhibiting the nucleation of martensite and drastic decrease of the martensite-start temperature of the nanoparticles. High pressure of 0.5 - 4.0 GPa were adopted to induce the martensitic transition of the gamma-Fe nanoparticles. It is found that the extent of martensitic transformation increased with the increasing pressures, most individual gamma-Fe particles were partially transformed to martensite after pressurization.","authors":[],"categoryName":"|","doi":"","fpage":"313","id":"d4cb5fab-1cdb-4592-8f91-a9fe362e510c","issue":"3","journal":{"abbrevTitle":"NM","id":"cc88b34d-fd3e-4cdd-8396-bdba97e827f1","issnPpub":"0965-9773","publisherId":"NM","title":"Nanostructured Materials"},"keywords":[{"id":"c4b5bba9-5827-4fd5-bba7-f06bc143af5f","keyword":"small particles;nucleation;powders;metals;alloys;ms","originalKeyword":"small particles;nucleation;powders;metals;alloys;ms"}],"language":"en","publisherId":"0965-9773_1996_3_1","title":"Investigation on the martensitic transformation in gamma-Fe(N) nanoparticles","volume":"7","year":"1996"},{"abstractinfo":"Face centered cubic (fcc) gamma-Fe (5.9-10.4at.%N) ultrafine particles ranging in size from 30 to 100 nm prepared at room temperature by laser induced pyrolysis of Fe(CO)(5) and NH3. It is found that these austenitic particles did not transform to martensite when subsequently quenched to 77 K or 4.2 K, which is greatly lower than the martensite-start temperature of the bulk alloy with the same composition. Many planar defects, which can serve as the favorable martensitic nucleation sites in bulk austenite alloy, have been observed in these particles. Taking into account the size effect of the ultrafine particles on the martensitic transformation, a modification for the conventional martensitic transformation has been made to interpret the stabilization behavior of the ultrafine gamma-Fe(N) particles. It is indicated that the strengthening of the particles due to the reduction of the particle size and refinement of grain size may play important roles in both inhibiting the homogeneous nucleation and martensitic transformation occurred in the ultrafine particles.","authors":[],"categoryName":"|","doi":"","fpage":"4468","id":"9a9ffb78-ab10-4ceb-ab9b-cac3acd63286","issue":"8","journal":{"abbrevTitle":"JJOAPP1PBC&RP","id":"eab64340-273c-46fd-a8d5-cbb40895fbed","issnPpub":"0021-4922","publisherId":"JJOAPP1PBC&RP","title":"Japanese Journal of Applied Physics Part 1-Regular Papers Brief Communications & Review Papers"},"keywords":[{"id":"45936d17-e1ff-4697-a4e8-78f36d44a734","keyword":"ultrafine particles;particles size;martensitic transformation;gamma-Fe(N);thermodynamics;laser synthesis;size;dependence;powders;metals;alloys;ms","originalKeyword":"ultrafine particles;particles size;martensitic transformation;gamma-Fe(N);thermodynamics;laser synthesis;size;dependence;powders;metals;alloys;ms"}],"language":"en","publisherId":"0021-4922_1996_8_1","title":"Thermodynamic interpretation of the martensitic transformation in ultrafine gamma-Fe(N) particles","volume":"35","year":"1996"},{"abstractinfo":"An approach for the thermodynamics of the thermoelastic martensitic transformation in β-Cu base alloys is suggested.Driving forces for martensitic transformation,T_0 and M_s tempera- tures in Cu-Zn,Cu-Al and Cu-Zn-Al alloys were calculated and the calculated M_s are in good agreement with the experimental ones.Ordering of the parent phase lowers M_s(T_0)in Cu-Zn and Cu-Zn-Al alloys,but raises M_s(T_0)in Cu-Al alloys.Two methods for the es- timation of the critical driving force for the thermoelastic martensitic transformation are also introduced.","authors":[{"authorName":"XU Zuyao (T.Y.Hsu) ZHOU Xiaowang~** Department of Materials Science","id":"50c67556-4bf3-4ac7-96af-e03878efb73d","originalAuthorName":"XU Zuyao (T.Y.Hsu) ZHOU Xiaowang~** Department of Materials Science"},{"authorName":"Shanghai Jiaotong University","id":"592109f6-ee5b-4e1f-89b7-54564173dc8a","originalAuthorName":"Shanghai Jiaotong University"},{"authorName":"Shanghai","id":"d71d5e8b-3330-4ccf-a88d-f4895679a0b7","originalAuthorName":"Shanghai"},{"authorName":"China Now at Department of Materials Strength (Department No.1)","id":"90428e55-9ea1-426d-aa03-b40407fc2842","originalAuthorName":"China Now at Department of Materials Strength (Department No.1)"},{"authorName":"Shanghai Research Institute of Materials","id":"c4e1a24d-7811-493d-be41-0d15d2b8cf57","originalAuthorName":"Shanghai Research Institute of Materials"},{"authorName":"Shanghai","id":"ca37ff78-16a5-4654-b87d-751dbfad832c","originalAuthorName":"Shanghai"},{"authorName":"200030 China","id":"5fc2cb57-90ec-44b6-a56f-b54247f52325","originalAuthorName":"200030 China"}],"categoryName":"|","doi":"","fpage":"401","id":"dfe2831e-5719-47d1-945a-7dd55cb4d4e1","issue":"6","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":"62344c6a-23e4-4888-9135-15447192caf6","keyword":"β-Cu base alloy","originalKeyword":"β-Cu base alloy"},{"id":"6fad6de8-8d8c-4769-afd7-4fe447ac4472","keyword":"null","originalKeyword":"null"},{"id":"3858010e-39d5-47ee-a12b-e0b7414038a4","keyword":"null","originalKeyword":"null"}],"language":"en","publisherId":"1006-7191_1991_6_1","title":"THERMODYNAMICS OF MARTENSITIC TRANSFORMATION IN β-Cu BASE ALLOYS","volume":"4","year":"1991"},{"abstractinfo":"A dynamic process of the martensitic transformation in(Y,Mg)-PSZ ceramics was observed in situ using TEM.Under the effect of contact stress between tetragonal(t)-ZrO_2 precipi- tates,a group of substructural martensite variants may occur priorly and then another one was induced by the elastic strain relaxation,both form(100)_m twins further.In addition,the crystallography of the martensitic transformation was also discussed.","authors":[{"authorName":"DAI Zurong LI Baocheng Taiyuan Institute of Mechanical Engineering","id":"5718dba2-674e-444f-b8f3-55c04d24ee75","originalAuthorName":"DAI Zurong LI Baocheng Taiyuan Institute of Mechanical Engineering"},{"authorName":"Taiyuan","id":"b1bb347a-2154-4885-ad0a-08dba184cb4b","originalAuthorName":"Taiyuan"},{"authorName":"ChinaWU Houzheng CHEN Yuru LIU Wenxi Tianjin University","id":"1250a7ce-caec-4d99-9135-75e46dc6dd60","originalAuthorName":"ChinaWU Houzheng CHEN Yuru LIU Wenxi Tianjin University"},{"authorName":"Tianjin","id":"a6cb606b-95a7-4b24-b7d0-ac1003b1f9ef","originalAuthorName":"Tianjin"},{"authorName":"China","id":"6d7eb666-4198-495e-84b6-6cbcc32c4d50","originalAuthorName":"China"}],"categoryName":"|","doi":"","fpage":"471","id":"0441c0c2-ff26-400b-83ad-8c1ff9582ec0","issue":"6","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":"3a07cc51-6834-4946-b9fd-95a181d71e43","keyword":"ceramics","originalKeyword":"ceramics"},{"id":"fdfe9c44-f867-4a92-a9ae-d383e1b59e5a","keyword":"null","originalKeyword":"null"},{"id":"c4be5ca9-4f47-473c-a1a4-6917b8a8de06","keyword":"null","originalKeyword":"null"}],"language":"en","publisherId":"1006-7191_1991_6_2","title":"THE MARTENSITIC TRANSFORMATION IN(Y,Mg)-PSZ CERAMICS","volume":"4","year":"1991"},{"abstractinfo":"The kinetics of the reversible martensitic transformation in a Cu-Zn-Al-Mn-Ni shape memory alloy has been studied by means of differential scanning calorimetry.The apparent activation energy has been calculated and the kinetic equations of positive and adverse martensitic transformation have been established with the variations of temperature and time.","authors":[{"authorName":"GENG Guili","id":"ab0e2585-eda5-4e42-a425-1deee1c7e737","originalAuthorName":"GENG Guili"},{"authorName":"BAI Yujun","id":"a0801985-8fe5-4010-93d9-f4524ab3b43e","originalAuthorName":"BAI Yujun"},{"authorName":"PENG Qifeng(Institute for Materials Engineering","id":"67553f06-b758-4fa7-b44a-3885b28801be","originalAuthorName":"PENG Qifeng(Institute for Materials Engineering"},{"authorName":"Shandong University of Technology","id":"d3641003-cf77-4f34-b261-b05829ca7536","originalAuthorName":"Shandong University of Technology"},{"authorName":"Jinan 250014","id":"ed7a1e6d-ed85-476b-aa5e-63aeb637b685","originalAuthorName":"Jinan 250014"},{"authorName":"China) Manuscript received 30 May 1995","id":"44907840-7f8e-4214-9c9d-6fe37fe4f0ba","originalAuthorName":"China) Manuscript received 30 May 1995"}],"categoryName":"|","doi":"","fpage":"56","id":"67f0d978-9a38-4f36-9d16-3803d3105156","issue":"1","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":"0fe433b7-0a29-4f65-bb07-145db2fb1856","keyword":":shape memory alloy","originalKeyword":":shape memory alloy"},{"id":"61b66f74-9ce0-4025-950c-009db94d9bc7","keyword":"null","originalKeyword":"null"},{"id":"f2a7e6fe-425e-4d61-851a-263a6ec4bde0","keyword":"null","originalKeyword":"null"},{"id":"93399b89-d117-45dc-8553-c665800c5a10","keyword":"null","originalKeyword":"null"}],"language":"en","publisherId":"1006-7191_1996_1_5","title":"DSC STUDY OF MARTENSITIC TRANSFORMATION KINETICS IN A Cu-Zn-Al-Mn-Ni SHAPE MEMORY ALLOY","volume":"9","year":"1996"},{"abstractinfo":"The microstructural changes associated with the tetragonal to monoclinic martensitic transformation at cryogenic temperatures in sintered CeO2-ZrO2 ceramics containing 15.5-16.5 mol% CeO2 have been studied by means of TEM observations. X-ray diffraction analysis indicates that the stress-induced martensitic phase increases with decreases in both temperature and CeO2 content. The effects of martensitic morphologies, anti-phase boundaries (APBs) and various dislocation features on mechanical properties are also discussed in the paper.","authors":[],"categoryName":"|","doi":"","fpage":"41101","id":"5eac2f35-3e51-4210-82f1-6ef99e58dfa1","issue":"1","journal":{"abbrevTitle":"C","id":"238cf93a-294c-4fc3-8d79-138864b128c7","issnPpub":"0011-2275","publisherId":"C","title":"Cryogenics"},"keywords":[{"id":"f8e19214-dc76-4bf1-816c-757d230f4ef3","keyword":"martensitic transformation;ZrO2-based ceramics;cryogenic temperatures;mechanical-properties;phase-transformation;tetragonal phase;zirconia;system","originalKeyword":"martensitic transformation;ZrO2-based ceramics;cryogenic temperatures;mechanical-properties;phase-transformation;tetragonal phase;zirconia;system"}],"language":"en","publisherId":"0011-2275_1996_1_1","title":"Martensitic transformation in ZrO2-based ceramics at cryogenic temperatures","volume":"36","year":"1996"},{"abstractinfo":"Instead of conventional quenching martensitic transformation from beta-Ti to alpha-Ti, unusual martensitic transformation from alpha-Ti to beta-Ti induced by rapid heating has been achieved simply by using an electric current pulse. A large amount of the high-temperature martensitic phase remained in a Ti-6Al-4V alloy. We verified that such transformation is structurally and kinetically achievable, which agrees well with the phenomenological crystallographic theory of martensitic transformation. (C) 2004 American Institute of Physics.","authors":[],"categoryName":"|","doi":"","fpage":"4872","id":"416e0002-ccfd-4926-bc4b-403a81aa210a","issue":"24","journal":{"abbrevTitle":"APL","id":"5e3c428a-be96-46d5-bcb9-94a4fce832b0","issnPpub":"0003-6951","publisherId":"APL","title":"Applied Physics Letters"},"keywords":[{"id":"5c0dc6fc-261a-47be-ab89-9e54cf81246a","keyword":"cobalt;particles","originalKeyword":"cobalt;particles"}],"language":"en","publisherId":"0003-6951_2004_24_1","title":"Martensitic transformation from alpha-Ti to beta-Ti on rapid heating","volume":"84","year":"2004"},{"abstractinfo":"The internal friction of alloys in martensite state is believed to be an M/M interface one, which can be explained by an expression deduced from the theory of dislocation internal fric- tion.The internal friction during martensitic transformation consists of two parts,including those of the M/M interface and of the phase transformation.The latter is further composed of two portions,the major one produced by reverse martensitic transformation and the other from stress-induced martensite.It was also found that the degradation of damping properties of the CuZnAl alloys is related to the dislocation,which is introduced from the exciting pro- cess,and tends to be of stable value after certain excitements.","authors":[{"authorName":"CHENG Yixuan CHEN Jiqin FANG Xiaomin L(?) Weiping Zhejiang University","id":"fc1312a3-31dd-451c-9d65-7b9e0ff984a3","originalAuthorName":"CHENG Yixuan CHEN Jiqin FANG Xiaomin L(?) Weiping Zhejiang University"},{"authorName":"Hangzhou","id":"08b3d478-382a-4f17-8189-c656e716ac0d","originalAuthorName":"Hangzhou"},{"authorName":"China","id":"96bfe88c-d44a-4a6c-b23d-70650945c269","originalAuthorName":"China"}],"categoryName":"|","doi":"","fpage":"441","id":"51cca94f-e022-4410-9498-36a4f1635366","issue":"6","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":"362c8a3d-ceb1-4a7f-9000-41a0126de2bf","keyword":"damping property","originalKeyword":"damping property"},{"id":"fe79e170-6a41-47fd-9c8b-5400f20a7206","keyword":"null","originalKeyword":"null"},{"id":"0ef966bf-7f7c-4710-943d-e082d1e96392","keyword":"null","originalKeyword":"null"},{"id":"d2b0acd0-8e19-4d50-bcad-e0a65169e123","keyword":"null","originalKeyword":"null"}],"language":"en","publisherId":"1006-7191_1991_6_4","title":"DAMPING PROPERTIES OF MARTENSITE AND MARTENSITIC TRANSFORMATION IN CuZnAl ALLOYS","volume":"4","year":"1991"}],"totalpage":641,"totalrecord":6408}