{"currentpage":1,"firstResult":0,"maxresult":10,"pagecode":5,"pageindex":{"endPagecode":5,"startPagecode":1},"records":[{"abstractinfo":"介绍以第一原理<span style=\"color:red\">合金</span>电子理论为基础的系统<span style=\"color:red\">合金</span>科学(FP-SSA)框架中<span style=\"color:red\">Au3Cu</span><span style=\"color:red\">型</span><span style=\"color:red\">有序</span><span style=\"color:red\">合金</span>的特征原子势能(CAPE)配分函数.主要创新内容如下:以基本原子团{AiAu·[(I - i)<span style=\"color:red\">Au</span>,iCu]}和{AiCu·[(I- i)<span style=\"color:red\">Au</span>,iCu]}序列的中心特征原子AiAu和iCu为结构单元序列,替代原子对和原子团,建立了<span style=\"color:red\">合金</span>相的特征原子排列模型；以配位原子团[(I - i)<span style=\"color:red\">Au</span>,iCu]对作用于特征原子势场影响的方式替代原子对能量相互作用和原子团能量相互作用方式,以特征原子势能能级代替原子对能级和原子团能级,建立了<span style=\"color:red\">合金</span>相的“特征原子势能相加定律”,计算<span style=\"color:red\">合金</span>相及其组元的平均势能；在特征原子排列的简并因数与特征原子势能能级一致的条件下建立CAPE配分函数和计算组态熵.此函数揭示了当今流行的固溶体理论的不足之处,为建立特征Gibbs能配分函数奠定了基础.","authors":[{"authorName":"谢佑卿","id":"32d1838f-d86d-4516-9f42-70d383ac9f91","originalAuthorName":"谢佑卿"},{"authorName":"聂耀庄","id":"b6b9d8ad-057f-472e-a5a4-09014aad95e7","originalAuthorName":"聂耀庄"},{"authorName":"李小波","id":"828ad3bb-c44c-44b0-a0bb-c3b8274068a0","originalAuthorName":"李小波"},{"authorName":"刘心笔","id":"7f2dd550-07cf-4187-b409-55cf5b12d29e","originalAuthorName":"刘心笔"},{"authorName":"彭红建","id":"afd1d375-997d-4eca-8fc2-75f342ef239a","originalAuthorName":"彭红建"},{"authorName":"李艳芬","id":"c9994b4b-34bb-40c2-af42-345c60b2c75c","originalAuthorName":"李艳芬"}],"doi":"","fpage":"2489","id":"03dfae71-d6e7-448c-ac1a-6746c3ca3967","issue":"10","journal":{"abbrevTitle":"ZGYSJSXB","coverImgSrc":"journal/img/cover/ZGYSJSXB.jpg","id":"88","issnPpub":"1004-0609","publisherId":"ZGYSJSXB","title":"中国有色金属学报"},"keywords":[{"id":"69a5870f-2c04-41b5-ae84-233bc0355318","keyword":"<span style=\"color:red\">Au3Cu</span><span style=\"color:red\">型</span><span style=\"color:red\">有序</span><span style=\"color:red\">合金</span>","originalKeyword":"Au3Cu型有序合金"},{"id":"61c8954e-2f1a-4bf6-bcae-b8c122ab1801","keyword":"第一原理","originalKeyword":"第一原理"},{"id":"6f01f879-e9d6-4b40-b735-d046fb67771c","keyword":"系统<span style=\"color:red\">合金</span>科学","originalKeyword":"系统合金科学"},{"id":"5548db9c-0861-435e-be49-bce130661247","keyword":"特征原子","originalKeyword":"特征原子"},{"id":"f530e24b-ce37-4146-a985-da4544c59842","keyword":"势能","originalKeyword":"势能"},{"id":"697750ca-72aa-49d5-b36c-3c54d290c389","keyword":"配分函数","originalKeyword":"配分函数"}],"language":"zh","publisherId":"zgysjsxb201110016","title":"FP-SSA框架中<span style=\"color:red\">Au3Cu</span><span style=\"color:red\">型</span><span style=\"color:red\">有序</span><span style=\"color:red\">合金</span>相的特征原子势能配分函数","volume":"21","year":"2011"},{"abstractinfo":"依据<span style=\"color:red\">合金</span>特征晶体理论，固溶体中组元的原子状态分裂成若干特征原子状态，固溶体的晶格常数可由特征晶体的晶格常数相加定律、特征原子体积相加定律和特征原子状态相加定律求得。介绍了无序二元固溶体的9种晶格常数函数；确定了无序<span style=\"color:red\">Au-Cu</span><span style=\"color:red\">合金</span>及其组元的晶格常数函数；预计了<span style=\"color:red\">Au_3Cu</span>，AuCu，AuCu_<span style=\"color:red\">3</span>和相应<span style=\"color:red\">有序</span><span style=\"color:red\">合金</span>随成分变化的晶格常数、理论值与实验值符合较好．","authors":[{"authorName":"谢佑卿","id":"28672353-ca3c-493e-ac50-35552050946a","originalAuthorName":"谢佑卿"}],"categoryName":"|","doi":"","fpage":"1233","id":"e7599c4b-2c73-4b2a-85cf-480ef7b76d56","issue":"12","journal":{"abbrevTitle":"JSXB","coverImgSrc":"journal/img/cover/JSXB.jpg","id":"48","issnPpub":"0412-1961","publisherId":"JSXB","title":"金属学报"},"keywords":[{"id":"3b651273-c733-4800-8021-92cc1a0762ec","keyword":"<span style=\"color:red\">Au-Cu</span>系","originalKeyword":"Au-Cu系"},{"id":"0c431674-df07-4e59-989e-bfda494f9262","keyword":" disordered alloy","originalKeyword":" disordered alloy"},{"id":"d193ed90-2e93-4a7a-8817-c68a900f08eb","keyword":" ordered alloy","originalKeyword":" ordered alloy"},{"id":"c3745edb-ede5-495d-b53e-0b3474e2110d","keyword":"lattice constant","originalKeyword":"lattice constant"},{"id":"c7b05ebb-d9eb-4c7c-a164-97d720aa8d29","keyword":" atomic volume","originalKeyword":" atomic volume"}],"language":"zh","publisherId":"0412-1961_1998_12_9","title":"<span style=\"color:red\">Au-Cu</span>系中无序和<span style=\"color:red\">有序</span>相的晶格常数","volume":"34","year":"1998"},{"abstractinfo":"用XRD法研究了退火Fe73.5<span style=\"color:red\">Cu1Nb3</span>Si13.5B9<span style=\"color:red\">合金</span>中α-Fe(Si)晶化相的<span style=\"color:red\">有序</span>化过程.结果表明,Fe73.5<span style=\"color:red\">Cu1Nb3</span>Si13.5B9非晶<span style=\"color:red\">合金</span>在490℃,1h退火后,α-Fe(Si)晶化相是具<span style=\"color:red\">有</span>DO<span style=\"color:red\">3</span>结构的<span style=\"color:red\">有序</span>相,<span style=\"color:red\">有序</span>畴为球形,直径为7.0nm,它随退火温度的升高而长大,在590℃退火后达10.9nm,与α-Fe(Si)的尺寸相当.此时,α-Fe(Si)的<span style=\"color:red\">有序</span>度为0.8在850℃,1h退火后,α-Fe(Si)的DO<span style=\"color:red\">3</span>超点阵线条消失.在550℃等温退火时,α-Fe(Si)的DO<span style=\"color:red\">3</span><span style=\"color:red\">有序</span>畴先为椭球状,于60min退火后形成球状,直径为10nm.","authors":[{"authorName":"张湘义","id":"2274d714-3d7e-49ae-b2db-269680435ac7","originalAuthorName":"张湘义"},{"authorName":"郑炀曾","id":"b33eed66-d362-49e3-9134-3406d690e48e","originalAuthorName":"郑炀曾"}],"categoryName":"|","doi":"","fpage":"294","id":"c360b299-70f7-4177-b435-bcbc13cced7d","issue":"4","journal":{"abbrevTitle":"CLYJXB","coverImgSrc":"journal/img/cover/CLYJXB.jpg","id":"16","issnPpub":"1005-3093","publisherId":"CLYJXB","title":"材料研究学报"},"keywords":[{"id":"73019ccc-dbab-44d9-95dd-be8b71114d6e","keyword":"Fe_(73.5)<span style=\"color:red\">Cu_1Nb_3</span>Si_(13.5)B_9<span style=\"color:red\">合金</span>","originalKeyword":"Fe_(73.5)Cu_1Nb_3Si_(13.5)B_9合金"},{"id":"94314a26-3691-4d59-a13f-0d8e38ed3ee4","keyword":"null","originalKeyword":"null"},{"id":"4e6c48f9-3cce-49f3-ba79-bd07161cdd98","keyword":"null","originalKeyword":"null"},{"id":"73789189-503f-460f-aef4-a0a218509144","keyword":"null","originalKeyword":"null"},{"id":"55bfb386-472e-4a57-83ee-f3b5fb702032","keyword":"null","originalKeyword":"null"}],"language":"zh","publisherId":"1005-3093_1995_4_4","title":"退火Fe_(73.5)<span style=\"color:red\">Cu_1Nb_3</span>Si_(13.5)B_9<span style=\"color:red\">合金</span>中α-Fe(Si)晶化相的<span style=\"color:red\">有序</span>化","volume":"9","year":"1995"},{"abstractinfo":"基于<span style=\"color:red\">合金</span>化的改性原理,以调整材料的长程<span style=\"color:red\">有序</span>度为改性思想,采用真空电弧熔炼/热压退火制备了四种Cr/Al复合<span style=\"color:red\">合金</span>化Fe<span style=\"color:red\">3</span>Si基<span style=\"color:red\">有序</span><span style=\"color:red\">合金</span>.通过XRD,SEM,EPMA等对<span style=\"color:red\">合金</span>进行了表征,并采用长程<span style=\"color:red\">有序</span>参数定量表征了退火得到的<span style=\"color:red\">有序</span>相的<span style=\"color:red\">有序</span>程度.结果表明:四种不同成分的<span style=\"color:red\">有序</span><span style=\"color:red\">合金</span>,具<span style=\"color:red\">有</span>不同的显微组织.随着Si含量降低<span style=\"color:red\">合金</span><span style=\"color:red\">有序</span>度下降,且Cr/Al的复合效应对这一趋势起到了促进作用,使得具<span style=\"color:red\">有</span>相同Si含量的Fe65Si25Cr5Al5<span style=\"color:red\">有序</span><span style=\"color:red\">合金</span>的<span style=\"color:red\">有序</span>度低于Fe<span style=\"color:red\">3</span>Si,分别为0.658和0.796.","authors":[{"authorName":"周琦","id":"473a430b-61cc-486d-ad1f-2a33c35c5227","originalAuthorName":"周琦"},{"authorName":"贾建刚","id":"62960858-4ec0-4ed5-a324-825329b356da","originalAuthorName":"贾建刚"},{"authorName":"臧树俊","id":"cf6a617a-964a-47ae-8b8a-ffad1a2cf084","originalAuthorName":"臧树俊"},{"authorName":"赵红顺","id":"ec7cce54-2155-4212-bf93-2432f05c635a","originalAuthorName":"赵红顺"},{"authorName":"吴海涛","id":"98f0799d-2b84-4f49-a1bd-f2489822b4c7","originalAuthorName":"吴海涛"}],"doi":"10.3969/j.issn.1001-4381.2012.01.017","fpage":"83","id":"4907211a-6a01-4614-bf6e-f31a481dd3c3","issue":"1","journal":{"abbrevTitle":"CLGC","coverImgSrc":"journal/img/cover/CLGC.jpg","id":"9","issnPpub":"1001-4381","publisherId":"CLGC","title":"材料工程"},"keywords":[{"id":"cc0e103e-43f7-4a06-abf0-65e1c4564e42","keyword":"Fe<span style=\"color:red\">3</span>Si","originalKeyword":"Fe3Si"},{"id":"9452447e-3ca1-4caa-9195-b273da7b3689","keyword":"Al","originalKeyword":"Al"},{"id":"c23b3748-5fc9-45da-8d59-bcae817b83c3","keyword":"Cr","originalKeyword":"Cr"},{"id":"b943f534-fb66-4b10-b35c-8e9fcf7e01f0","keyword":"真空熔炼","originalKeyword":"真空熔炼"},{"id":"ce9d9cc7-a6b1-4656-8c53-cb3bc2d2e8ce","keyword":"长程<span style=\"color:red\">有序</span>参数","originalKeyword":"长程有序参数"}],"language":"zh","publisherId":"clgc201201017","title":"Cr/Al复合<span style=\"color:red\">合金</span>化Fe<span style=\"color:red\">3</span>Si基<span style=\"color:red\">有序</span><span style=\"color:red\">合金</span>及其<span style=\"color:red\">有序</span>度研究","volume":"","year":"2012"},{"abstractinfo":"采用X射线衍射和内耗测量研究了<span style=\"color:red\">Cu</span>-Zn-Al<span style=\"color:red\">合金</span>不同热处理条件对马氏体相变和母相<span style=\"color:red\">有序</span>态的影响。研究表明,“淬火-时效”试样从室温加热到320℃马氏体完全消失为止始终未发生逆相变。分级淬火短期等温试样出现B2?9R和DO_<span style=\"color:red\">3</span>?18R两种马氏体相变共存。随着等温时间的增长,B2?9R相变消失,与此同时DO_<span style=\"color:red\">3</span>?18R相变增强。然而,淬火后立即上淬到100—150℃等温的试样只出现B2?9R相变,即使等温时间增长也能继续保持。显然,从高温快冷不能抑制A2?B2<span style=\"color:red\">有序</span>,却可以抑制B2?DO_<span style=\"color:red\">3</span><span style=\"color:red\">有序</span>。虽然分级和上淬处理时母相所处的湿度相同,但其<span style=\"color:red\">有序</span>态却各异,足够的空位浓度是发生B2?DO_<span style=\"color:red\">3</span><span style=\"color:red\">有序</span>转变的必要条件。文中讨论了<span style=\"color:red\">Cu</span>-Zn-Al<span style=\"color:red\">合金</span>马氏体稳定化的可能机制。","authors":[{"authorName":"陈树川","id":"ec6a78f5-4987-450f-aa14-9ed1b2b370de","originalAuthorName":"陈树川"},{"authorName":"徐祖耀","id":"f25e3c5b-6016-4ffa-842b-1d16df437f61","originalAuthorName":"徐祖耀"},{"authorName":"杨凡","id":"15d6e17c-6897-4a08-8864-879aed7c6319","originalAuthorName":"杨凡"},{"authorName":"张骥华","id":"772ba9c7-cc7e-4c0f-b13d-baf9511bfc83","originalAuthorName":"张骥华"}],"categoryName":"|","doi":"","fpage":"5","id":"193a0251-d5c0-4b1f-bf58-5620ae112fba","issue":"4","journal":{"abbrevTitle":"JSXB","coverImgSrc":"journal/img/cover/JSXB.jpg","id":"48","issnPpub":"0412-1961","publisherId":"JSXB","title":"金属学报"},"keywords":[{"id":"bcd2e829-2dde-4073-9abf-c9ba8ab6f8d5","keyword":"马氏体稳定化","originalKeyword":"马氏体稳定化"},{"id":"52058a54-0b65-485e-a569-3e83479b409a","keyword":"A2→B2 ordering","originalKeyword":"A2→B2 ordering"},{"id":"5f2f5a4b-68fc-4293-a1cd-997daf4066c3","keyword":"vacancy concentration","originalKeyword":"vacancy concentration"}],"language":"zh","publisherId":"0412-1961_1991_4_3","title":"<span style=\"color:red\">Cu</span>-Zn-Al<span style=\"color:red\">合金</span>马氏体稳定化与母相<span style=\"color:red\">有序</span>态","volume":"27","year":"1991"},{"abstractinfo":"研究了Ti_<span style=\"color:red\">3</span>Al-Nb<span style=\"color:red\">合金</span>在高温下的<span style=\"color:red\">有序</span>化,冷却过程高温β相转变及时效过程亚稳定β相分解的行为,结果指出,在1060℃固溶处理时,<span style=\"color:red\">合金</span>形成初生α_2和β高温<span style=\"color:red\">有序</span>相;在固溶处理后的冷却过程中,<span style=\"color:red\">合金</span>发生β→α_2+ω<span style=\"color:red\">型</span>转变;在700℃时效过程中,<span style=\"color:red\">合金</span>发生(β+ω<span style=\"color:red\">型</span>)亚稳→(α_2+β)稳定分解。","authors":[{"authorName":"李东","id":"66c2fad5-43ae-4617-9048-063b20c35455","originalAuthorName":"李东"},{"authorName":"周敬","id":"b66cc9c9-fb67-439b-81a6-f18d4c713f14","originalAuthorName":"周敬"},{"authorName":"常昕","id":"2a8b064d-fb70-46c4-b424-42402161520f","originalAuthorName":"常昕"},{"authorName":"关少轩","id":"8b4c8726-d0ff-48b2-9337-2827a8d9b577","originalAuthorName":"关少轩"}],"categoryName":"|","doi":"","fpage":"57","id":"7224f126-da16-410c-bc34-0021d8aef7e6","issue":"6","journal":{"abbrevTitle":"JSXB","coverImgSrc":"journal/img/cover/JSXB.jpg","id":"48","issnPpub":"0412-1961","publisherId":"JSXB","title":"金属学报"},"keywords":[{"id":"ce922631-96bb-42f5-8106-e0ac75d85e61","keyword":"Ti_<span style=\"color:red\">3</span>Al-Nb<span style=\"color:red\">合金</span>","originalKeyword":"Ti_3Al-Nb合金"},{"id":"e953bc23-1b1b-4e50-8cce-aff802d181ef","keyword":"ordering transformation","originalKeyword":"ordering transformation"},{"id":"b02e1147-a4ee-44a0-9bd3-faae6296a6fd","keyword":"α_2","originalKeyword":"α_2"},{"id":"6aee46ea-3bd5-4091-ab37-b26fe19dd23a","keyword":"β","originalKeyword":"β"},{"id":"64ec3c24-16a0-4f33-afb3-313d25c4609d","keyword":"ω","originalKeyword":"ω"}],"language":"zh","publisherId":"0412-1961_1990_6_7","title":"Ti_<span style=\"color:red\">3</span>Al-Nb<span style=\"color:red\">合金</span>的<span style=\"color:red\">有序</span>转变","volume":"26","year":"1990"},{"abstractinfo":"研究了热处理工艺条件对非化学计量比的Ni48Mn31Ga21<span style=\"color:red\">合金</span>的结构<span style=\"color:red\">有序</span>度的影响.结果表明:对于非化学计量Ni48Mn31Ga21<span style=\"color:red\">合金</span>,其结构<span style=\"color:red\">有序</span>化处Ζ理工艺宜选用900℃×4d+400℃×50h.","authors":[{"authorName":"陈小丽","id":"f5e1d429-49b1-4f28-af3a-d40f1e338c0f","originalAuthorName":"陈小丽"},{"authorName":"卢斌","id":"d7c91e8d-3311-4209-983f-62648d22068b","originalAuthorName":"卢斌"},{"authorName":"刘岩","id":"de374b52-19a5-4e4e-8d40-4701792aa2e6","originalAuthorName":"刘岩"},{"authorName":"王花宾","id":"febe19bd-c786-40c2-8ba1-20c850cee537","originalAuthorName":"王花宾"},{"authorName":"刘吉轩","id":"63f54d8e-60c1-4d5b-9fd1-b55819f38002","originalAuthorName":"刘吉轩"},{"authorName":"吴标理","id":"c6ce8af0-dc5f-4094-9e15-bd327b3032ca","originalAuthorName":"吴标理"}],"doi":"","fpage":"1620","id":"dd1bb2a4-105d-49a4-bc22-54fdd6ef31f2","issue":"z1","journal":{"abbrevTitle":"GNCL","coverImgSrc":"journal/img/cover/GNCL.jpg","id":"33","issnPpub":"1001-9731","publisherId":"GNCL","title":"功能材料"},"keywords":[{"id":"f72bfc7d-df07-4a67-967c-34693b5791d9","keyword":"Heusler<span style=\"color:red\">合金</span>","originalKeyword":"Heusler合金"},{"id":"0972cbbe-36cd-4126-ad56-145b9209fcc3","keyword":"热处理","originalKeyword":"热处理"},{"id":"74c59a5e-10c1-4c66-b833-048578454024","keyword":"XRD分析","originalKeyword":"XRD分析"},{"id":"e72973fc-b555-4ac1-be49-9970d9891dd7","keyword":"<span style=\"color:red\">有序</span>化","originalKeyword":"有序化"}],"language":"zh","publisherId":"gncl2004z1454","title":"Heusler<span style=\"color:red\">型</span>Ni2MnGa<span style=\"color:red\">合金</span>的<span style=\"color:red\">有序</span>化处理","volume":"35","year":"2004"},{"abstractinfo":"本文将原子位形几率波理论推广到三元复式格子体系,研究了(A~ⅢB~Ⅴ)_(1-x)C_(2x)~(Ⅳ)<span style=\"color:red\">型</span><span style=\"color:red\">合金</span>最稳定超晶格的原子排列,由理论得到十九种基态<span style=\"color:red\">有序</span>结构,揭示了原子<span style=\"color:red\">有序</span>分布的形成规律。","authors":[{"authorName":"王世范","id":"1f9c6302-0b14-4c53-9777-aa7f6b7be622","originalAuthorName":"王世范"},{"authorName":"倪军","id":"7cfa3e4e-95ab-43ab-af43-cb55ab437a9a","originalAuthorName":"倪军"},{"authorName":"段文晖","id":"6615f93a-20b0-4462-82ac-d4e762470205","originalAuthorName":"段文晖"}],"categoryName":"|","doi":"","fpage":"194","id":"b02abd8c-269e-4757-84b1-4a1d6d8ef596","issue":"3","journal":{"abbrevTitle":"CLYJXB","coverImgSrc":"journal/img/cover/CLYJXB.jpg","id":"16","issnPpub":"1005-3093","publisherId":"CLYJXB","title":"材料研究学报"},"keywords":[{"id":"e1464ee2-c9f6-4313-bc76-f84cb485fba9","keyword":"原子位形几率波","originalKeyword":"原子位形几率波"},{"id":"54a4f3cb-ef31-47aa-9e73-20e983e11892","keyword":"material design","originalKeyword":"material design"},{"id":"788a5779-100a-471f-a5a1-3e61c92c2441","keyword":"ordered structure","originalKeyword":"ordered structure"}],"language":"zh","publisherId":"1005-3093_1993_3_10","title":"(A~ⅢB~V)_(1-x)C_(2x)~Ⅳ <span style=\"color:red\">型</span>三元<span style=\"color:red\">合金</span>的<span style=\"color:red\">有序</span>结构","volume":"7","year":"1993"},{"abstractinfo":"研究了<span style=\"color:red\">有序</span>态Ni<span style=\"color:red\">3</span>Fe<span style=\"color:red\">合金</span>在不同氢气压力中和在不同电流密度电解渗氢时<span style=\"color:red\">合金</span>的拉伸性能.结果表明:随着氢气压力或电流密度的增加,<span style=\"color:red\">合金</span>的延伸率先快速下降,随后逐渐趋于恒定:<span style=\"color:red\">合金</span>的氢脆因子与氢气压力或电流密度之间呈相同的依赖关系.<span style=\"color:red\">有序</span>态Ni<span style=\"color:red\">3</span>Fe<span style=\"color:red\">合金</span>在氢气中的脆化机制是催化反应生成的氢原子进入<span style=\"color:red\">合金</span>所致,<span style=\"color:red\">合金</span>的脆化程度与进入<span style=\"color:red\">合金</span>的氢原子数量<span style=\"color:red\">有</span>关.","authors":[{"authorName":"陈业新","id":"839511ad-1ca9-4a3a-8df8-584b400dd069","originalAuthorName":"陈业新"},{"authorName":"朱再飞","id":"9a4ed432-a3ef-4027-8aed-7ea5d3b9b5a1","originalAuthorName":"朱再飞"},{"authorName":"万晓景","id":"b85ce15a-b08d-48d3-80ef-738d0d29bc95","originalAuthorName":"万晓景"}],"doi":"","fpage":"2109","id":"c25581f5-9b47-48e3-be4c-3f6d9e19c7c5","issue":"12","journal":{"abbrevTitle":"XYJSCLYGC","coverImgSrc":"journal/img/cover/XYJSCLYGC.jpg","id":"69","issnPpub":"1002-185X","publisherId":"XYJSCLYGC","title":"稀有金属材料与工程"},"keywords":[{"id":"121ebc2f-c1f3-4977-9b52-feacaf546682","keyword":"<span style=\"color:red\">有序</span>态Ni<span style=\"color:red\">3</span>Fe","originalKeyword":"有序态Ni3Fe"},{"id":"82b99b24-af2b-44b9-af1d-4e99a00c72f1","keyword":"氢脆","originalKeyword":"氢脆"},{"id":"5a6d2bbd-1260-4b10-9967-37bd72f59ed7","keyword":"力学性能","originalKeyword":"力学性能"}],"language":"zh","publisherId":"xyjsclygc200812009","title":"氢对<span style=\"color:red\">有序</span>态Ni<span style=\"color:red\">3</span>Fe<span style=\"color:red\">合金</span>脆性的影响","volume":"37","year":"2008"},{"abstractinfo":"研究了室温下不同<span style=\"color:red\">有序</span>度的Ni<span style=\"color:red\">3</span>Fe在真空和氢气气氛中的力学性能及断口形貌特征.结果表明:具<span style=\"color:red\">有</span>不同<span style=\"color:red\">有序</span>度的Ni<span style=\"color:red\">3</span>Fe在真空中拉伸时,均不发生环境氢脆;但在氢气中氢对其<span style=\"color:red\">有</span>强烈的脆化作用,且其敏感性随着<span style=\"color:red\">有序</span>度的增加而加剧.扫描电镜观察表明:在真空中或H2中拉伸时,无序Ni<span style=\"color:red\">3</span>Fe的断口都为韧性穿晶断口,而在氢气中拉伸时,1000 h<span style=\"color:red\">有序</span>化Ni<span style=\"color:red\">3</span>Fe为100%沿晶脆性断口,但是<span style=\"color:red\">有序</span>化60 h和200 h的Ni<span style=\"color:red\">3</span>Fe的断口为穿晶和沿晶混合断口.","authors":[{"authorName":"陈爱萍","id":"cdb87d56-552b-4b38-b1b3-53a1abf242f3","originalAuthorName":"陈爱萍"},{"authorName":"陈业新","id":"611ad46c-7a2e-42d9-a443-ae34655fd67d","originalAuthorName":"陈业新"},{"authorName":"万晓景","id":"d62ee6f0-4df7-43b1-9e89-d8db668d0b06","originalAuthorName":"万晓景"},{"authorName":"王建国","id":"fd2ca722-dfd6-4187-a9bc-43b50e769dcc","originalAuthorName":"王建国"},{"authorName":"程晓英","id":"6157097d-af2f-403f-aabd-4733fe3fb6b8","originalAuthorName":"程晓英"}],"doi":"10.3321/j.issn:1005-3093.2003.01.013","fpage":"74","id":"a3bbd6d1-ed3a-4fa5-9540-d9f1b3ccb0a5","issue":"1","journal":{"abbrevTitle":"CLYJXB","coverImgSrc":"journal/img/cover/CLYJXB.jpg","id":"16","issnPpub":"1005-3093","publisherId":"CLYJXB","title":"材料研究学报"},"keywords":[{"id":"ffb91179-d315-442c-b292-ff6058ebad56","keyword":"材料科学基础学科","originalKeyword":"材料科学基础学科"},{"id":"d967a689-f792-4033-a8a7-3efe0a2c0012","keyword":"金属间化合物","originalKeyword":"金属间化合物"},{"id":"16348e1e-3579-4adc-bf27-07193a8fa2f0","keyword":"环境氢脆","originalKeyword":"环境氢脆"},{"id":"b220801d-c83c-4713-a18d-bc19447a1c2a","keyword":"<span style=\"color:red\">有序</span>度","originalKeyword":"有序度"},{"id":"37764e24-5998-4df2-b262-47546885ed50","keyword":"Ni<span style=\"color:red\">3</span>Fe","originalKeyword":"Ni3Fe"}],"language":"zh","publisherId":"clyjxb200301013","title":"<span style=\"color:red\">有序</span>度对Ni<span style=\"color:red\">3</span>Fe<span style=\"color:red\">合金</span>环境氢脆的影响","volume":"17","year":"2003"}],"totalpage":16653,"totalrecord":166530}