{"currentpage":1,"firstResult":0,"maxresult":10,"pagecode":5,"pageindex":{"endPagecode":5,"startPagecode":1},"records":[{"abstractinfo":"利用扫描电镜(SEM)对铝合金6061在低浓度硫酸电解液中硬质阳极氧化膜的生长方式进行了研究.结果表明,氧化初期氧化膜在基体表面上呈点状生长,随着硬质阳极氧化反应的进行,点状氧化膜长大并沿基体表面逐渐铺展,同时在基体表面未氧化区域不断产生新的点状氧化膜.氧化膜以此种方式不断生长,直到基体表面被氧化膜覆盖为止.在此之后氧化膜生长与在传统硫酸浓度中的生长方式几乎相同,膜层厚度逐渐增加.在相同氧化时间和温度条件下,低硫酸浓度硬质阳极氧化膜的硬度和厚度都高于传统硫酸浓度的氧化膜.","authors":[{"authorName":"邓丽虹","id":"acb7779a-e4ef-4447-87eb-700fd320b60e","originalAuthorName":"邓丽虹"},{"authorName":"魏晓伟","id":"9da58b81-27d1-439d-a320-cc7d58a0f100","originalAuthorName":"魏晓伟"}],"doi":"","fpage":"434","id":"607ad89f-4a49-4d75-8f18-704ecf8dd9b8","issue":"6","journal":{"abbrevTitle":"FSYFH","coverImgSrc":"journal/img/cover/FSYFH.jpg","id":"25","issnPpub":"1005-748X","publisherId":"FSYFH","title":"腐蚀与防护"},"keywords":[{"id":"0362bbf4-316e-455b-a11d-ab4e13bbaaa3","keyword":"铝合金6061","originalKeyword":"铝合金6061"},{"id":"82fd7a5f-e6c8-4506-84ae-76a57d663fbb","keyword":"低浓度硫酸","originalKeyword":"低浓度硫酸"},{"id":"7a89b3b6-1ba6-445a-9df0-77c2c999c0b7","keyword":"氧化膜","originalKeyword":"氧化膜"},{"id":"d9b4f69f-c400-4f3b-9f49-d8558493b57e","keyword":"生长方式","originalKeyword":"生长方式"}],"language":"zh","publisherId":"fsyfh201106006","title":"铝合金6061在低浓度硫酸中硬质阳极氧化膜的生长方式","volume":"32","year":"2011"},{"abstractinfo":"利用电化学沉积的方法,在电解液中加入吡咯,制备了磷酸钙-聚吡咯复合涂层.结果表明:吡咯使涂层的生长方式发生了改变.未加入吡咯获得的单一的磷酸钙沉积陶瓷膜呈现无序排列,叶片状.电解液中加入吡咯后,陶瓷膜层有序排列,呈针状且整个膜层的晶粒增大.红外光谱分析表明,出现了C=C和N-H基团的伸缩振动吸收峰,说明吡咯已经由电解液中转移到涂层中.相分析表明:吡咯的加入并没有改变涂层的相组成,说明整个过程中仅有少量的吡咯进入涂层.","authors":[{"authorName":"马臣","id":"7eaf6c73-7e14-4c8a-a41e-7b9056bb0277","originalAuthorName":"马臣"},{"authorName":"曲立杰","id":"99ec6eb7-e847-4fa0-a64d-f262b60bd6de","originalAuthorName":"曲立杰"},{"authorName":"李慕勤","id":"2a8c1e8b-f1d7-4892-8feb-a22e83d90f4f","originalAuthorName":"李慕勤"},{"authorName":"杨士勤","id":"eec6b99f-d949-4cc0-be82-fc0e464afa39","originalAuthorName":"杨士勤"}],"doi":"","fpage":"696","id":"a51763e6-6b40-45c5-b36a-5582b6753b31","issue":"z2","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":"cf11a5f5-da17-4e04-b9c2-9a1ccffc5c27","keyword":"电沉积","originalKeyword":"电沉积"},{"id":"118caf30-2d58-4c42-bba9-0269e0368d9a","keyword":"吡咯","originalKeyword":"吡咯"},{"id":"2ca4ef3e-0e4e-4ab7-95d8-54fc3d59a854","keyword":"磷酸钙","originalKeyword":"磷酸钙"},{"id":"15286944-ced6-4ba5-b56a-22260e06c48a","keyword":"涂层","originalKeyword":"涂层"},{"id":"0185a4ee-bc1c-45c2-9492-7be7c1969717","keyword":"生长方式","originalKeyword":"生长方式"}],"language":"zh","publisherId":"xyjsclygc2007z2201","title":"吡咯对电沉积磷酸钙类复合涂层的生长方式的影响","volume":"36","year":"2007"},{"abstractinfo":"研究了Al-4.0Cu-0.45Mg-0.4Ag-0.25Er合金铸态晶界相的组成及其生长规律.结果表明:稀土Er在合金中主要以Al8Cu4Er相的形式存在,Mg和Ag固溶于α-Al.合金铸态组织由α-Al固溶体、Al8Cu4Er相和Al2Cu相组成.Al8Cu4Er相和Al2Cu相共生于α-Al固溶体晶界,形成离异型共晶组织.凝固过程中,Al8Cu4Er相优先依附于先共晶相α-Al形核,并且分别以枝晶生长和平面生长这2种方式有选择的进行生长,形成α-Al、Al8Cu4Er相和Al2Cu相的三元共晶组织.","authors":[{"authorName":"李云涛","id":"b304ea1a-548f-4500-82bb-1891183685ee","originalAuthorName":"李云涛"},{"authorName":"刘志义","id":"1e909145-9c1f-4aa1-a829-3576d293d824","originalAuthorName":"刘志义"},{"authorName":"马飞跃","id":"49df650a-09e4-4f58-b6de-2c5aa4de8930","originalAuthorName":"马飞跃"},{"authorName":"夏卿坤","id":"8d903083-f328-432c-bcd1-64e2073d518a","originalAuthorName":"夏卿坤"}],"doi":"","fpage":"1019","id":"92bd5880-cf3d-4222-8e98-b8908278f364","issue":"6","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":"f48b0a5a-ab43-41d3-82f6-4bb7027da534","keyword":"Al-Cu-Mg-Ag合金","originalKeyword":"Al-Cu-Mg-Ag合金"},{"id":"3af81abb-8796-4ec1-babe-1503fc11cba6","keyword":"稀土Er","originalKeyword":"稀土Er"},{"id":"a4dde1bf-c921-40d6-a33f-b93f95805e9a","keyword":"三元共晶","originalKeyword":"三元共晶"},{"id":"4dfef8b9-89e3-43f6-a755-7a10b4e04ca0","keyword":"生长方式","originalKeyword":"生长方式"}],"language":"zh","publisherId":"xyjsclygc200806018","title":"Al-Cu-Mg-Ag-Er合金晶界相组成及生长方式","volume":"37","year":"2008"},{"abstractinfo":"采用磁控溅射方法在钛合金(Ti6A14V)基体上制备了HA(+YSZ)复合涂层.利用X射线衍射仪(XRD)分析涂层的物相组成,扫描电镜(SEM)观察涂层的表面形貌,原子力显微镜(AFM)分析涂层的生长状况,划痕法测定涂层与基体的附着力.结果表明,用磁控溅射法可在Ti6Al4V基体上制备HA(+YSZ)复合涂层,涂层组成与靶材基本相似,涂层呈多孔状,划痕法测量涂层的附着力约为80N,涂层的生长模式为层状生长加岛状生长.","authors":[{"authorName":"施秋萍","id":"d746727c-5fbe-4a1e-bb13-ddb19a4b03a8","originalAuthorName":"施秋萍"},{"authorName":"赵玉涛","id":"1d8051c2-602e-435e-933e-5501e60aaadb","originalAuthorName":"赵玉涛"},{"authorName":"戴起勋","id":"143dc359-4285-40b3-a40c-ebe9adbf5157","originalAuthorName":"戴起勋"},{"authorName":"林东洋","id":"c01978b0-dd33-4df4-abd0-409d8a6b3c8a","originalAuthorName":"林东洋"},{"authorName":"罗平辉","id":"5d9271e1-6191-456a-bc39-387eeb648e63","originalAuthorName":"罗平辉"}],"doi":"","fpage":"264","id":"3eac29ea-e450-47dc-a28a-189cfe81c048","issue":"z1","journal":{"abbrevTitle":"CLDB","coverImgSrc":"journal/img/cover/CLDB.jpg","id":"8","issnPpub":"1005-023X","publisherId":"CLDB","title":"材料导报"},"keywords":[{"id":"942a348e-11fb-466b-8296-d2831070d8c8","keyword":"复合涂层","originalKeyword":"复合涂层"},{"id":"07ba4704-2aad-4e55-bf99-da42e861eef8","keyword":"磁控溅射","originalKeyword":"磁控溅射"},{"id":"8ff14f91-5fff-4d02-81b4-384cf99b77a4","keyword":"微观形貌","originalKeyword":"微观形貌"},{"id":"0bb2e1c4-79bf-4341-b4a2-ae2eaf85614e","keyword":"生长方式","originalKeyword":"生长方式"}],"language":"zh","publisherId":"cldb2006z1084","title":"磁控溅射HA(+YSZ)/Ti6Al4V复合涂层的微观形貌和生长方式","volume":"20","year":"2006"},{"abstractinfo":"构造三维蒙特卡罗模型,研究了六边形基底薄膜生长的过程.在模型中针对每个原子考虑了原子沉积,原子扩散及原子脱附三个动力学过程,并认为这三个过程是相互独立的,即在同一计算步长中三个过程依据各自的概率发生.经过生长过程可视化的结果表明,薄膜原子之间的相互作用能、基底温度和沉积速率对薄膜的生长方式有显著的影响.这一结论得到了实验的验证.","authors":[{"authorName":"朱祎国","id":"bbc7ecb4-0587-4505-b979-bc865984bbbc","originalAuthorName":"朱祎国"}],"doi":"","fpage":"640","id":"d8a8d588-6e44-4ef7-8ff2-9dc2b62dbe92","issue":"6","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":"eb7fae3a-4ac6-444c-9ebe-f319e58116e2","keyword":"材料科学基础学科","originalKeyword":"材料科学基础学科"},{"id":"6bf518f2-5695-46c7-94be-ac908f2b1c7e","keyword":"薄膜生长","originalKeyword":"薄膜生长"},{"id":"4cf7e9df-26f7-40c1-828e-4bb15824079d","keyword":"三维Monte Carlo模型","originalKeyword":"三维Monte Carlo模型"},{"id":"40497ef0-7e47-4ea6-a5a0-e94f2cdc1777","keyword":"生长方式","originalKeyword":"生长方式"},{"id":"d0981d80-026d-41a6-b0b8-484ed6c923e2","keyword":"形貌","originalKeyword":"形貌"}],"language":"zh","publisherId":"clyjxb200906014","title":"薄膜生长的三维蒙特卡罗模型","volume":"23","year":"2009"},{"abstractinfo":"用热膨胀仪测定了12MnNiVR钢的连续冷却转变曲线,并结合显微组织观察和硬度测定,研究了低冷速下奥氏体向铁素体转变及向贝氏体转变的动力学,分析了铁素体转变及贝氏体转变的生长方式.实验钢在连续冷却过程中的计算相变动力学结果与实测相变数据吻合很好.研究结果表明实验钢在低冷速下冷却时奥氏体向铁素体转变,形核位置主要在晶棱处,生长方式主要为二维长大,奥氏体向贝氏体转变,形核位置主要在界面处,生长方式主要为一维长大.","authors":[{"authorName":"张志敏","id":"7343bbcd-1565-4047-93a5-9aa3c9284311","originalAuthorName":"张志敏"},{"authorName":"蔡庆伍","id":"b59fe407-b409-42e6-b122-d7209da071d3","originalAuthorName":"蔡庆伍"},{"authorName":"余伟","id":"23065a3f-7de2-4e3c-8e2b-9c9ac82e390a","originalAuthorName":"余伟"}],"doi":"","fpage":"143","id":"50e0fc1c-fc5f-4208-a731-1895eff57949","issue":"4","journal":{"abbrevTitle":"CLRCLXB","coverImgSrc":"journal/img/cover/CLRCLXB.jpg","id":"15","issnPpub":"1009-6264","publisherId":"CLRCLXB","title":"材料热处理学报"},"keywords":[{"id":"28d42fde-ebcf-459a-b77d-af789d2008e0","keyword":"12MnNiVR钢","originalKeyword":"12MnNiVR钢"},{"id":"9f27e97f-a71a-4225-962f-3bb7955b6d62","keyword":"连续冷却转变","originalKeyword":"连续冷却转变"},{"id":"fef0328c-9afa-4dac-82e3-66fc93352b89","keyword":"相变动力学","originalKeyword":"相变动力学"},{"id":"1d453080-c476-4dc1-abcc-f0dcbb0aa440","keyword":"生长方式","originalKeyword":"生长方式"}],"language":"zh","publisherId":"jsrclxb201304028","title":"12MnNiVR钢的连续冷却转变行为及相变动力学","volume":"34","year":"2013"},{"abstractinfo":"
通过电磁悬浮(EML)熔炼设备对Al-70%Si合金进行深过冷处理, 利用高速摄影仪(HSC)和SEM分别对凝固过程和凝固后的组织进行了观测, 研究了不同过冷度下初生Si的生长规律. 结果表明, 过冷度对初生Si的生长有很大影响. 当过冷度较小时, 初生Si为粗大的长条状, 有特殊的边和面, 且具有明显的孪晶痕迹, 表现出小平面生长的特征; 当过冷度较大时, 初生Si为细小的枝晶和球状晶, 表面光滑, 表现出非小平面生长的特征; 当过冷度居于中间时, 初生Si为粗大的块状和规则排列的枝晶状, 块状有特殊的边和面, 枝晶表面光滑, 表现出小平面和非小平面混合生长的特征. 随着过冷度的增加, 初生Si的生长方式由小平面生长转变为中间方式生长, 再由中间方式生长转变为非小平面生长, 生长方式间发生转变的临界过冷度分别为122 和230 K.
","authors":[{"authorName":"严军辉","id":"c50c4716-7626-4d9c-b9bd-514d4d31eaaf","originalAuthorName":"严军辉"},{"authorName":"坚增运","id":"3aa40412-58bf-4448-8c8f-ec4556a5c72d","originalAuthorName":"坚增运"},{"authorName":"朱满","id":"88886935-8184-411a-a37b-60e2020a497e","originalAuthorName":"朱满"},{"authorName":"常芳娥","id":"ce542981-9a81-4dea-bf2d-9f7ac8a583eb","originalAuthorName":"常芳娥"},{"authorName":"许军锋","id":"717be7eb-904e-43e7-9ca0-ff7b2f58f36c","originalAuthorName":"许军锋"}],"categoryName":"Orginal Article","doi":"10.11900/0412.1961.2015.00553","fpage":"931","id":"eb782f60-a24a-445e-8e14-66be46d132a0","issue":"8","journal":{"abbrevTitle":"JSXB","coverImgSrc":"journal/img/cover/JSXB.jpg","id":"48","issnPpub":"0412-1961","publisherId":"JSXB","title":"金属学报"},"keywords":[{"id":"adeacf78-b1c9-487c-8455-06cdac8d5732","keyword":"Al-70%Si合金","originalKeyword":"Al-70%Si合金"},{"id":"a0966754-9c33-443f-b0cd-7d9e24c37631","keyword":"电磁悬浮","originalKeyword":"电磁悬浮"},{"id":"8880efe8-b676-429c-982d-65417ed46653","keyword":"高速摄影仪","originalKeyword":"高速摄影仪"},{"id":"835d8703-eb1f-4a4d-bdae-58c1db1122e1","keyword":"深过冷","originalKeyword":"深过冷"},{"id":"405c90c0-e598-403a-b9d8-5656cf7e0dd8","keyword":"初生Si","originalKeyword":"初生Si"},{"id":"6768d42b-c70f-4d40-8dff-4c746c657888","keyword":"生长方式","originalKeyword":"生长方式"}],"language":"zh","publisherId":"C20150553","title":"深过冷Al-70%Si合金的凝固特性与微观组织*","volume":"52","year":"2016"},{"abstractinfo":"通过电磁悬浮(EML)熔炼设备对Al-70%Si合金进行深过冷处理,利用高速摄影仪(HSC)和SEM分别对凝固过程和凝固后的组织进行了观测,研究了不同过冷度下初生Si的生长规律.结果表明,过冷度对初生Si的生长有很大影响.当过冷度较小时,初生Si为粗大的长条状,有特殊的边和面,且具有明显的孪晶痕迹,表现出小平面生长的特征;当过冷度较大时,初生Si为细小的枝晶和球状晶,表面光滑,表现出非小平面生长的特征;当过冷度居于中间时,初生Si为粗大的块状和规则排列的枝晶状,块状有特殊的边和面,枝晶表面光滑,表现出小平面和非小平面混合生长的特征.随着过冷度的增加,初生Si的生长方式由小平面生长转变为中间方式生长,再由中间方式生长转变为非小平面生长,生长方式间发生转变的临界过冷度分别为122和230 K.","authors":[{"authorName":"严军辉","id":"c2d4c6ca-53fd-4c9a-b396-66bf133fb0ab","originalAuthorName":"严军辉"},{"authorName":"坚增运","id":"2fe4f481-ccdc-428f-9e89-fe97ebce86e1","originalAuthorName":"坚增运"},{"authorName":"朱满","id":"f9c4e7bc-7527-467b-bf5d-1bdec4e9a16f","originalAuthorName":"朱满"},{"authorName":"常芳娥","id":"9a60574e-bd9f-4627-903f-69dc98dc4b58","originalAuthorName":"常芳娥"},{"authorName":"许军锋","id":"ebfe7b4a-f5e4-4beb-a7e1-81d9546a56db","originalAuthorName":"许军锋"}],"doi":"10.11900/0412.1961.2015.00553","fpage":"931","id":"5bb517a5-7222-48dc-b125-c311bb3679c6","issue":"8","journal":{"abbrevTitle":"JSXB","coverImgSrc":"journal/img/cover/JSXB.jpg","id":"48","issnPpub":"0412-1961","publisherId":"JSXB","title":"金属学报"},"keywords":[{"id":"a7f9241c-5aed-46d8-a390-7fbc8de16077","keyword":"Al-70%Si合金","originalKeyword":"Al-70%Si合金"},{"id":"38f5840b-9824-46d7-adf2-1681a3a9a0f5","keyword":"电磁悬浮","originalKeyword":"电磁悬浮"},{"id":"a2aef034-71e0-4745-aa9b-337c8748681c","keyword":"高速摄影仪","originalKeyword":"高速摄影仪"},{"id":"f6efb894-8a83-474e-8b1d-26c34e73f1d6","keyword":"深过冷","originalKeyword":"深过冷"},{"id":"74ecb7d9-a240-43e5-a45b-8030fa98b7dd","keyword":"初生Si","originalKeyword":"初生Si"},{"id":"eab6d238-749a-498d-b9be-d42f51f443f0","keyword":"生长方式","originalKeyword":"生长方式"}],"language":"zh","publisherId":"jsxb201608005","title":"深过冷Al-70%Si合金的凝固特性与微观组织","volume":"52","year":"2016"},{"abstractinfo":"利用区熔定向凝固设备制备了Tb0.3Dy0.7Fe1.95合金,研究了不同定向凝固生长速度下Tb0.3Dy0.7Fe1.95合金的轴向择优取向、晶体的生长方式、结晶形貌的变化规律以及它们之间的关系.结果表明,随着定向凝固生长速度V从低速10μm/s逐步增大到380μm/s,Tb0.3Dy0.7Fe1.95合金的轴向择优取向从<110>方向转变为<311>及<110>、<211>、<533>多种混合轴向取向,之后又转变为原来的<110>方向,当V≥350μm/s后,轴向择优取向变得不明显.在整个过程中出现了2个不稳定过渡阶段,即180μm/s