{"currentpage":1,"firstResult":0,"maxresult":10,"pagecode":5,"pageindex":{"endPagecode":5,"startPagecode":1},"records":[{"abstractinfo":"针对厚度测量仪镀铬标准片的溯源性问题,采用自主设计的电解装置,实现了在45号钢基体表面局部镀铬,获得了厚度均匀的镀铬层,可以满足磁吸力厚度测量仪标准片的要求.","authors":[{"authorName":"缪华清","id":"6ade977f-6d40-461b-aaf6-106e4d73d8aa","originalAuthorName":"缪华清"},{"authorName":"袁学韬","id":"33a1c4a4-4bb4-4725-8e90-7b28a3422920","originalAuthorName":"袁学韬"},{"authorName":"<span style=\"color:red\">姚</span><span style=\"color:red\">晶晶</span>","id":"54f8d10b-428c-4314-bef7-f50757c33088","originalAuthorName":"姚晶晶"},{"authorName":"<span style=\"color:red\">姚</span>磊","id":"d14bda23-1f95-45bd-ac33-4a0a89c14e76","originalAuthorName":"姚磊"},{"authorName":"华志强","id":"89532c7b-d277-45b7-b806-15c6e8f571c1","originalAuthorName":"华志强"}],"doi":"","fpage":"286","id":"8df2a3ac-074c-4fbb-860d-c3bed5dd66ec","issue":"3","journal":{"abbrevTitle":"FSYFH","coverImgSrc":"journal/img/cover/FSYFH.jpg","id":"25","issnPpub":"1005-748X","publisherId":"FSYFH","title":"腐蚀与防护"},"keywords":[{"id":"47e9164b-e5cf-49dd-973c-c09c998dc432","keyword":"磁吸力厚度测量仪","originalKeyword":"磁吸力厚度测量仪"},{"id":"2b4b3531-9208-4cc2-ac9b-068c5474183f","keyword":"镀铬","originalKeyword":"镀铬"},{"id":"3ed14ede-bcde-4da0-8545-fa4db6f61f69","keyword":"厚度均匀性","originalKeyword":"厚度均匀性"}],"language":"zh","publisherId":"fsyfh201403019","title":"磁吸力厚度测量仪镀铬标准片制备方法","volume":"35","year":"2014"},{"abstractinfo":"为解决电解测厚仪锌基镀铜标准片的镀层结合力和溯源性差的问题,采用预浸活化碱性镀铜工艺取代氰化物镀铜工艺,解决了环保和标准片镀层结合力相矛盾的问题;应用自主设计的电解池,在锌基上获得厚度均匀、不完全包覆的镀铜层,满足了电解测厚仪锌基镀铜标准片的要求.","authors":[{"authorName":"缪华清","id":"8b1499f1-69ef-4b15-8b02-c1c73cfca25d","originalAuthorName":"缪华清"},{"authorName":"<span style=\"color:red\">姚</span>磊","id":"df56d1f0-2bc6-402e-a896-fd8070ed0381","originalAuthorName":"姚磊"},{"authorName":"<span style=\"color:red\">姚</span><span style=\"color:red\">晶晶</span>","id":"6ac35076-e31b-4136-976c-48136e446ee4","originalAuthorName":"姚晶晶"},{"authorName":"袁学韬","id":"4e02ce73-2658-4cdf-add2-929587d1460c","originalAuthorName":"袁学韬"},{"authorName":"华志强","id":"5fd0f721-1831-4b9e-ab3b-d436615ae280","originalAuthorName":"华志强"}],"doi":"","fpage":"508","id":"c8a3aadf-f347-464a-b3b1-70519805fcb0","issue":"5","journal":{"abbrevTitle":"FSYFH","coverImgSrc":"journal/img/cover/FSYFH.jpg","id":"25","issnPpub":"1005-748X","publisherId":"FSYFH","title":"腐蚀与防护"},"keywords":[{"id":"0c7577e0-4c49-4a01-ac16-51c458b8803f","keyword":"电解式测厚仪","originalKeyword":"电解式测厚仪"},{"id":"08976888-6cd4-4599-90b5-e495372a7e21","keyword":"锌基体","originalKeyword":"锌基体"},{"id":"ab9cb490-370e-4def-9039-26cdda9c237f","keyword":"电镀铜","originalKeyword":"电镀铜"}],"language":"zh","publisherId":"fsyfh201405025","title":"电解式测厚仪锌基镀铜厚度标准片制备","volume":"35","year":"2014"},{"abstractinfo":"以<span style=\"color:red\">姚</span>冲大型钼多金属矿床为例，阐明了大别山北麓地区区域和矿床地质特征。通过在该地区开展岩矿石物性标本测试、综合物探剖面性研究（可控源音频大地电磁方法和频谱激电方法试验），试验及测试结果表明，<span style=\"color:red\">姚</span>冲钼矿床中含矿岩体为中低阻，高极化特征，<span style=\"color:red\">姚</span>冲钼矿床为斑岩体外接触带成矿，在深部高阻岩体的外侧存在一个低阻异常体，经钻孔验证，该低阻异常体为花岗斑岩体（脉）外接触带含辉钼矿的中元古界片麻岩。频谱激电法反演结果更进一步印证了物性测试结果和可控源音频大地电磁测深结果的准确性。因此，此次综合物探方法试验结果表明，可控源音频大地电磁测深和频谱激电法在该地区寻找斑岩型钼矿床是有效的，可为今后在该区域寻找斑岩型矿床提供技术参考。","authors":[{"authorName":"李冰","id":"dc65a649-28dc-47d8-8db1-024312fc7661","originalAuthorName":"李冰"},{"authorName":"尚建阁","id":"e954eef9-d05f-408d-803f-97fed70d75fe","originalAuthorName":"尚建阁"},{"authorName":"刘清泉","id":"75897a79-3e77-4a84-80f5-09a97fb9c23a","originalAuthorName":"刘清泉"},{"authorName":"张智慧","id":"719cd997-9746-4138-b915-4a97127e02ee","originalAuthorName":"张智慧"},{"authorName":"丁云河","id":"7a366c93-fb58-43c3-b4e6-d4bc8c2136c2","originalAuthorName":"丁云河"},{"authorName":"魏明君","id":"bd762cc1-2563-4e53-b048-019c2e67f404","originalAuthorName":"魏明君"},{"authorName":"王蒙","id":"749d2edf-03af-4586-815c-096d984d0f12","originalAuthorName":"王蒙"}],"doi":"10.11792/hj20150106","fpage":"21","id":"b4817cdb-b4dd-4360-829e-8de7f5bc0efe","issue":"1","journal":{"abbrevTitle":"HJ","coverImgSrc":"journal/img/cover/HJ.jpg","id":"44","issnPpub":"1001-1277","publisherId":"HJ","title":"黄金"},"keywords":[{"id":"d499d377-380d-4b7a-a3b8-4cdf4d28c530","keyword":"可控源音频大地电磁测深","originalKeyword":"可控源音频大地电磁测深"},{"id":"caea6518-fc2a-4427-b346-39df7c03d3c1","keyword":"频谱激电法","originalKeyword":"频谱激电法"},{"id":"0b1253cc-6352-4895-b452-6c6a5719c227","keyword":"斑岩型钼矿床","originalKeyword":"斑岩型钼矿床"},{"id":"164d2631-4e52-4d0a-9df6-1eb451f2e78b","keyword":"<span style=\"color:red\">姚</span>冲钼多金属矿床","originalKeyword":"姚冲钼多金属矿床"}],"language":"zh","publisherId":"huangj201501007","title":"综合物探方法寻找斑岩型钼矿床的应用试验研究---以<span style=\"color:red\">姚</span>冲钼多金属矿床为例","volume":"","year":"2015"},{"abstractinfo":"用SHS技术制备的纳米共<span style=\"color:red\">晶晶</span>须复相陶瓷具有较大的断裂韧性和较高的塑性形变行为,其组织结构以纳米共<span style=\"color:red\">晶晶</span>须为基体.运用Mori-Tanaka方法研究了复合共<span style=\"color:red\">晶晶</span>须的等效本征应变,并得到了复合共<span style=\"color:red\">晶晶</span>须的应力应变关系.通过应力应变关系计算出复合共<span style=\"color:red\">晶晶</span>须的刚度,复合共<span style=\"color:red\">晶晶</span>须为横观各向同性,具有5个独立的弹性常数.根据复相陶瓷的应变均值,考虑复合共<span style=\"color:red\">晶晶</span>须方位的随机性,计算出材料的有效弹性模量和泊松比,复相陶瓷材料为各向同性体.","authors":[{"authorName":"倪新华","id":"d4a27666-cb33-4203-a99c-622672d7e992","originalAuthorName":"倪新华"},{"authorName":"刘协权","id":"476140cb-ec03-4973-b03d-929d9beaca1c","originalAuthorName":"刘协权"},{"authorName":"赵忠民","id":"dc1ef99f-25ee-445c-a62b-58d0da1f23cb","originalAuthorName":"赵忠民"}],"doi":"","fpage":"597","id":"1b35fe4b-79e2-4e21-b2f4-cdb07beac094","issue":"z1","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":"5424a8dd-674e-477b-b97b-a60008656435","keyword":"纳米共<span style=\"color:red\">晶晶</span>须","originalKeyword":"纳米共晶晶须"},{"id":"dfb9476f-ff4d-4acb-b73d-52a0a2e7e528","keyword":"刚度预报","originalKeyword":"刚度预报"},{"id":"18ade8d8-d3b4-46a3-83d5-46cf73f1c4a8","keyword":"Mori-Tanaka方法","originalKeyword":"Mori-Tanaka方法"},{"id":"f92d2f4e-2db7-493e-a8cb-576041d5dd54","keyword":"横观各向同性","originalKeyword":"横观各向同性"},{"id":"da5424d2-bc12-4364-9c2a-7f2153cf438a","keyword":"各向同性","originalKeyword":"各向同性"}],"language":"zh","publisherId":"xyjsclygc2005z1161","title":"纳米共<span style=\"color:red\">晶晶</span>须复相陶瓷的刚度预报","volume":"34","year":"2005"},{"abstractinfo":"从理论上分析TA15钛合金动态再结<span style=\"color:red\">晶晶</span>粒生长驱动力,提出动态再结<span style=\"color:red\">晶晶</span>粒生长等效反驱动力的概念.基于动态再结<span style=\"color:red\">晶晶</span>粒生长驱动力,建立(描述动态再结<span style=\"color:red\">晶晶</span>粒尺寸演变)的晶粒生长速率模型及晶粒尺寸模型.以TA15钛合金动态再结<span style=\"color:red\">晶晶</span>粒尺寸实验测定数据为例,采用遗传算法(GA)优化尺寸模型参数.结果表明,模型计算结果与实验数据能够达到较好的吻合,平均误差为7.4%.","authors":[{"authorName":"欧阳德来","id":"7e729ecb-f68e-40c8-a11b-3a24e0938efb","originalAuthorName":"欧阳德来"},{"authorName":"鲁世强","id":"aff73040-f173-4485-ae39-e4698a16f6fb","originalAuthorName":"鲁世强"},{"authorName":"崔霞","id":"d602e91f-c94a-4d11-ac90-93e0341de3b5","originalAuthorName":"崔霞"},{"authorName":"吴超","id":"7a6ab0e9-8485-483d-bed4-86db1dbeb463","originalAuthorName":"吴超"},{"authorName":"李鑫","id":"f5a5ac3d-d464-41a2-a2b3-201b020876f9","originalAuthorName":"李鑫"}],"doi":"","fpage":"1162","id":"3db81805-6e50-4f36-a7d9-8302eb4cae16","issue":"7","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":"e6bcf597-d265-45d7-8e43-18833ddd5fca","keyword":"驱动力","originalKeyword":"驱动力"},{"id":"f755513f-c7ce-4125-989f-1d84f4359c6f","keyword":"晶粒生长模型","originalKeyword":"晶粒生长模型"},{"id":"b5c7a19e-8b55-414f-8819-7d06477b4923","keyword":"TA15钛合金","originalKeyword":"TA15钛合金"}],"language":"zh","publisherId":"xyjsclygc201007007","title":"TA15钛合金动态再结<span style=\"color:red\">晶晶</span>粒生长模型","volume":"39","year":"2010"},{"abstractinfo":"探讨MGH956合金冷轧薄板中粗大再结<span style=\"color:red\">晶晶</span>粒的形成原因,以及合金中的弥散颗粒对再结晶过程的作用和影响.结果表明MGH956合金中存在的细小弥散Y2O3颗粒,抑制了再结晶的形核过程,使合金中仅形成少量形核核心,在1300℃左右高温退火中,少量形核核心迅速长大,因此形成了粗大的再结<span style=\"color:red\">晶晶</span>粒组织.","authors":[{"authorName":"杨峥","id":"54d86f44-08e6-4060-8ba7-909ac2480965","originalAuthorName":"杨峥"},{"authorName":"田耘","id":"dc6484ca-c336-420f-a156-10fcfe0ad19a","originalAuthorName":"田耘"},{"authorName":"柳光祖","id":"732d663d-afd8-4aa0-a535-4d44da72107b","originalAuthorName":"柳光祖"}],"doi":"","fpage":"1","id":"6b6c4ed8-295a-4b82-a921-4d38917b3818","issue":"5","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":"44d1a563-a3f0-4fbd-97da-28f0fb84b248","keyword":"MGH956合金","originalKeyword":"MGH956合金"},{"id":"e7784ba0-0268-4fad-820f-5bfa2db95e35","keyword":"氧化物弥散强化","originalKeyword":"氧化物弥散强化"},{"id":"5c42823f-addd-4e12-8ce8-2f5a6834fa0c","keyword":"再结晶","originalKeyword":"再结晶"}],"language":"zh","publisherId":"jsrclxb201005001","title":"MGH956合金冷轧薄板粗大再结<span style=\"color:red\">晶晶</span>粒形成机理","volume":"31","year":"2010"},{"abstractinfo":"测试了30钢经50％强形变后在不同温度下再结晶形核的时间，根据公式G=G。e-Q/RT计算了再结<span style=\"color:red\">晶晶</span>核的激活能。","authors":[{"authorName":"贲永志","id":"4cde65d4-a757-4ea6-ab5e-396c042a8909","originalAuthorName":"贲永志"}],"doi":"10.3969/j.issn.1001-0777.2001.03.007","fpage":"24","id":"614a9dab-75e6-46b8-9d10-0d75833b91fb","issue":"3","journal":{"abbrevTitle":"WLCS","coverImgSrc":"journal/img/cover/WLCS.jpg","id":"64","issnPpub":"1001-0777","publisherId":"WLCS","title":"物理测试"},"keywords":[{"id":"55e76cda-2c8f-405e-a915-3faa9e810bcd","keyword":"强形变30钢","originalKeyword":"强形变30钢"},{"id":"315cef17-6443-421c-b01c-336a93f756e9","keyword":"再结晶","originalKeyword":"再结晶"},{"id":"ac4abb4f-cd8d-479e-a5d6-4b0f22e5349b","keyword":"激活能","originalKeyword":"激活能"}],"language":"zh","publisherId":"wlcs200103007","title":"强形变30钢再结<span style=\"color:red\">晶晶</span>核的激活能","volume":"","year":"2001"},{"abstractinfo":"以晶界迁移机制进行再结晶的材料,其稳定动态再结<span style=\"color:red\">晶晶</span>粒尺寸D取决于形变Zener-Hol1omon参数(Z因子).作者建立了反映D-Z间关系的理论模型,进行了St41钢平面应变热变形动态再结晶实验,探讨了动态再结<span style=\"color:red\">晶晶</span>粒细化的机理.该理论模型为Sellars的经验公式提供了物理基础.研究结果表明,提高形变储存能是细化动态再结<span style=\"color:red\">晶晶</span>粒的重要途径.","authors":[{"authorName":"何宜柱","id":"ba287636-6540-4bed-a886-b721bf5ffe1f","originalAuthorName":"何宜柱"},{"authorName":"陈大宏","id":"50b292f4-177b-4274-8e3f-c1723fb1cdda","originalAuthorName":"陈大宏"},{"authorName":"雷廷权","id":"742b1adb-dfbc-4b18-a6f1-7f0ddac81f4c","originalAuthorName":"雷廷权"},{"authorName":"齐藤良行","id":"ea17fa72-a35d-498e-abd3-d53e9a4e009b","originalAuthorName":"齐藤良行"}],"doi":"","fpage":"26","id":"ca7d9da9-f977-4916-862c-df141e6045e7","issue":"1","journal":{"abbrevTitle":"GTYJXB","coverImgSrc":"journal/img/cover/GTYJXB.jpg","id":"30","issnPpub":"1001-0963","publisherId":"GTYJXB","title":"钢铁研究学报"},"keywords":[{"id":"c7d56a72-26d2-4dfd-9490-a2befb836545","keyword":"动态再结晶","originalKeyword":"动态再结晶"},{"id":"5df29481-adc8-4328-8aa8-d757d20e8479","keyword":"晶粒尺寸","originalKeyword":"晶粒尺寸"},{"id":"03fb77e1-4c1c-4692-bb72-84cea579a5a2","keyword":"Zener-Hol1omon参数","originalKeyword":"Zener-Hol1omon参数"},{"id":"160c30f2-ed43-4bfa-a727-854b8ddff143","keyword":"热变形","originalKeyword":"热变形"}],"language":"zh","publisherId":"gtyjxb200001007","title":"形变Z因子与动态再结<span style=\"color:red\">晶晶</span>粒尺寸间的理论模型","volume":"34","year":"2000"},{"abstractinfo":"基于γ-基多孪<span style=\"color:red\">晶晶</span>体微结构及滑移系和形变孪晶空间晶体学位向分布的变形机制,提出了分析晶体屈服应力对外载轴和片层界面夹角间的依赖关系及影响因素的细观力学解析模型.分析了α2相中柱面和锥面上滑移系的启动对多孪<span style=\"color:red\">晶晶</span>体屈服应力的影响.模拟计算和分析结果表明:当θ=0°时,位错滑移方向跨越片层界面,α2相中柱面滑移系开动;当θ=45°时,滑移方向平行片层界面;当θ=90°方向时,γ相中与片层界面斜交的孪晶开动,而α2相中锥面滑移系由于其临界剪切应力(CRSS)很大而并不开动.多孪<span style=\"color:red\">晶晶</span>体中孪晶与普通位错、柱面与孪晶及锥面与柱面之间的CRSS比值关系可确定为k:e:z=1:3:18.","authors":[{"authorName":"苏继龙","id":"58a0020e-e645-4253-9362-5ba5f06f7c23","originalAuthorName":"苏继龙"},{"authorName":"胡更开","id":"71c778d3-2345-4af7-af7b-a42fb67b0c53","originalAuthorName":"胡更开"}],"doi":"","fpage":"1500","id":"54365ce0-6ee3-4d09-9ea1-814e96f9bf06","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":"1d1c9c7f-dd37-4427-92d8-bb7796085e50","keyword":"γ-基合金","originalKeyword":"γ-基合金"},{"id":"53b6f9be-da32-41d9-bb77-262eb54dc0fe","keyword":"多孪<span style=\"color:red\">晶晶</span>体","originalKeyword":"多孪晶晶体"},{"id":"9815cdf9-11ea-4a29-83ba-e7ec7734f9ec","keyword":"滑移系","originalKeyword":"滑移系"},{"id":"e78fce67-5ab0-4ef1-aff0-e224d50aff1a","keyword":"屈服应力","originalKeyword":"屈服应力"},{"id":"f0afe430-3bcb-4b9e-8a9d-b283f55d3c4f","keyword":"细观力学","originalKeyword":"细观力学"}],"language":"zh","publisherId":"zgysjsxb200510004","title":"α2相滑移系对γ-TiAl基多孪<span style=\"color:red\">晶晶</span>体屈服强度的影响","volume":"15","year":"2005"},{"abstractinfo":"7075铝合金在热变形过程中主要发生连续动态再结晶，在温度为250~450℃、应变速率为0.1~1 s?1的条件下，对多组圆柱试样进行热模拟压缩实验。采用金相定量法对热变形后材料的显微组织晶粒度进行测量，建立7075铝合金热变形时动态再结<span style=\"color:red\">晶晶</span>粒度演化模型。结果表明：根据唯象理论的指数模型，利用线性回归方法求得7075铝合金热塑性变形组织晶粒度的演化模型；将该模型导入到有限元软件中能够预报7075铝合金热变形过程的连续动态再结<span style=\"color:red\">晶晶</span>粒度；预报结果与实验结果非常接近，说明将该演化模型导入有限元软件中可以较为准确地预测7075铝合金热变形过程动态再结<span style=\"color:red\">晶晶</span>粒度。","authors":[{"authorName":"杨栋","id":"0954a426-a3a8-4149-9dde-4ed09bc70bce","originalAuthorName":"杨栋"},{"authorName":"陈文琳","id":"877c98b5-4ff4-473a-b98c-1c9143b0433e","originalAuthorName":"陈文琳"},{"authorName":"王少阳","id":"1d07377d-b654-4cc6-9df9-8ce4daa6f887","originalAuthorName":"王少阳"},{"authorName":"马勇","id":"87e9b092-9558-4405-b58f-573b2d1f1669","originalAuthorName":"马勇"},{"authorName":"张金鹏","id":"e3b80b5f-ef60-419f-8bc7-31620f47fa8e","originalAuthorName":"张金鹏"},{"authorName":"周瑞","id":"084f8c3e-8a8d-4c3f-b44a-d836ad109667","originalAuthorName":"周瑞"},{"authorName":"赵亚培","id":"541efb7d-9f2e-481a-b4c4-9f9f18226815","originalAuthorName":"赵亚培"},{"authorName":"王欣芳","id":"b54433e8-c56b-4415-a69e-9cc839af056b","originalAuthorName":"王欣芳"}],"doi":"","fpage":"2747","id":"66baf603-c374-4efc-9fa3-e5429a951988","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":"6d3d0c02-e10f-4d68-8da5-d83a44a34365","keyword":"7075铝合金","originalKeyword":"7075铝合金"},{"id":"7a2fa632-3189-4284-a74a-bd4da9378f39","keyword":"热压缩","originalKeyword":"热压缩"},{"id":"e3df2bdc-e951-469a-95cd-c04e3eef03c5","keyword":"连续动态再结晶","originalKeyword":"连续动态再结晶"},{"id":"70458dd8-0997-43e6-b951-4a2a0b929eae","keyword":"有限元","originalKeyword":"有限元"},{"id":"876b8ff6-9349-49f2-985e-c3f82663fa6d","keyword":"组织晶粒度预报","originalKeyword":"组织晶粒度预报"}],"language":"zh","publisherId":"zgysjsxb201310004","title":"7075铝合金热变形时动态再结<span style=\"color:red\">晶晶</span>粒度演化模型","volume":"","year":"2013"}],"totalpage":75,"totalrecord":741}