{"currentpage":1,"firstResult":0,"maxresult":10,"pagecode":5,"pageindex":{"endPagecode":5,"startPagecode":1},"records":[{"abstractinfo":"研究了热-剪切循环条件下Sn-3.5Ag-0.5Cu钎料/Cu界面的显微结构,分析了界面金属间化合物的生长行为,并与<span style=\"color:red\">恒温</span><span style=\"color:red\">时效</span>后的Sn-3.5Ag-0.5Cu/Cu界面进行了对比.结果表明:<span style=\"color:red\">恒温</span><span style=\"color:red\">时效</span>至100 h,Sn-3.5Ag-0.5Cu/Cu界面上已形成Cu6Sn5和Cu3Sn两层金属间化合物;而热-剪切循环至720周Sn-3.5Ag-0.5Cu/Cu界面上只存在Cu6Sn5金属间化合物层,无Cu3Sn层生成,在界面近域的钎料内,颗粒状的Ag3Sn聚集长大成块状;在热-剪切循环和<span style=\"color:red\">恒温</span><span style=\"color:red\">时效</span>过程中,界面金属间化合物的形态初始都为扇贝状,随着<span style=\"color:red\">时效</span>时间的延长逐渐趋于平缓,最终以层状形式生长.","authors":[{"authorName":"王烨","id":"c0cf369a-0818-4aea-9eeb-1d152d20df9b","originalAuthorName":"王烨"},{"authorName":"黄继华","id":"e1dd1ea4-078d-4f99-9e4d-bd42cf7d794e","originalAuthorName":"黄继华"},{"authorName":"张建纲","id":"cb3b419c-8d4f-405c-a90d-1611a89049e4","originalAuthorName":"张建纲"},{"authorName":"齐丽华","id":"c1506cd5-547d-41ee-a829-2d327a8c8513","originalAuthorName":"齐丽华"}],"doi":"","fpage":"495","id":"92101fa4-1d32-45a2-904f-e1c7664ce454","issue":"3","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":"d4e85fe6-84df-47b9-8e37-86c421a17f77","keyword":"热-剪切循环","originalKeyword":"热-剪切循环"},{"id":"99f61ef8-8840-4b97-9821-e9b871544208","keyword":"<span style=\"color:red\">恒温</span><span style=\"color:red\">时效</span>","originalKeyword":"恒温时效"},{"id":"e2df0df1-3073-4b44-93d6-82c3cb9f9757","keyword":"Sn-3.5Ag-0.5Cu/Cu界面","originalKeyword":"Sn-3.5Ag-0.5Cu/Cu界面"},{"id":"d09936aa-5186-44d6-8797-4abcea33abec","keyword":"金属间化合物","originalKeyword":"金属间化合物"}],"language":"zh","publisherId":"zgysjsxb200603019","title":"Sn-3.5Ag-0.5Cu/Cu界面的显微结构","volume":"16","year":"2006"},{"abstractinfo":"论文介绍了一种漆包线漆<span style=\"color:red\">恒温</span>涂漆的控制方法,实践证明该方法对提高涂漆工艺稳定性和漆包线质量有很好效果.","authors":[{"authorName":"周军","id":"5497bce9-8336-42a6-8857-3ec4a981f06d","originalAuthorName":"周军"}],"doi":"10.3969/j.issn.1009-9239.2002.05.014","fpage":"35","id":"d6967b65-f0d7-440f-ae43-568f7f335356","issue":"5","journal":{"abbrevTitle":"JYCL","coverImgSrc":"journal/img/cover/JYCL.jpg","id":"50","issnPpub":"1009-9239","publisherId":"JYCL","title":"绝缘材料"},"keywords":[{"id":"7b95c872-e8ea-4263-b263-90b82cae330f","keyword":"漆包线","originalKeyword":"漆包线"},{"id":"901bf705-ab5d-4a64-84bb-291178f51414","keyword":"漆包线漆","originalKeyword":"漆包线漆"},{"id":"9dd974d8-b89f-4ef8-9967-02af04d6292d","keyword":"生产工艺","originalKeyword":"生产工艺"},{"id":"167b9eff-73e8-42ec-bfc3-cdea79e0aed9","keyword":"控制方法","originalKeyword":"控制方法"}],"language":"zh","publisherId":"jycltx200205014","title":"漆包线漆的<span style=\"color:red\">恒温</span>控制方法","volume":"35","year":"2002"},{"abstractinfo":"本文对于用分析法计算钢材加热时间的几个公式(Д.B.布得林,Б.B.斯塔尔克,И.Д.塞米金)作了批判性的介绍,分别指出了它们的不足之处。按照<span style=\"color:red\">恒温</span>介质中物体加热过程的分析,推导了物体加热时间的计算公式,它与以前各公式相比,具有下列各特点: 1)没有忽略加热的开始阶段所占的时间; 2)不仅适用于“薄材”而且适用于“厚材”的加热计算; 3)不仅可以计算物体在加热过程中的平均温度,而且可以计算中心及表面温度。 根据推导的结果,支中进而在理论上讨论了几个因素(温度、物体尺寸、物体物理性质)对加热时间的影响。最后也涉及到了关于炉子生产率的讨论。","authors":[{"authorName":"任世铮","id":"f1e94b4c-d287-47cc-9b23-4d73bfa888b5","originalAuthorName":"任世铮"}],"categoryName":"|","doi":"","fpage":"22","id":"4bd14e3b-6f36-46ad-815f-b5009e07cfe3","issue":"1","journal":{"abbrevTitle":"JSXB","coverImgSrc":"journal/img/cover/JSXB.jpg","id":"48","issnPpub":"0412-1961","publisherId":"JSXB","title":"金属学报"},"keywords":[],"language":"zh","publisherId":"0412-1961_1959_1_6","title":"<span style=\"color:red\">恒温</span>炉中的辐射加热","volume":"4","year":"1959"},{"abstractinfo":"本文叙述并讨论了几种固溶处理过的高钼不锈钢在不同温度<span style=\"color:red\">时效</span>过程中,组织结构变化的情况.16-6Cr-Mo不锈钢在800-1000℃保温,δ-铁素体首先在原来的γ/α相界上形成,然后或者由奥氏体晶粒四周向着中心,或者由晶粒一端向着另外一端推进,最后奥氏体将退缩到晶粒中心或者一个晶粒隅上消失.在600-700℃保温,则发现有层片状铁素体在奥氏体晶粒内形成,然后逐渐增多长大,最后全部代替了奥氏体.在16-6Cr-Mo、16-2.5-6及16-5-6Cr-Ni-Mo不锈钢中,从铁素体内沉淀出来的细小碳化物是一种过渡组织,在x相的成核与长大过程中,它们将不断地进行溶解.16-15-6 Cr-Ni-Mo不锈钢属奥氏体型,在不同温度进行固溶处理,奥氏体都很稳定,在随后的<span style=\"color:red\">恒温</span>处理过程中,只有碳化物从奥氏体内析出.在这几种钢中碳化物及x相的析出,均能显著地改变钢的硬度.在所研究的两种复相不锈钢中,都观察到有由于x相析出所引起的沉淀硬化现象.","authors":[{"authorName":"刘嘉乐","id":"23e2d8e1-1741-459f-bc46-e5d3b85f3f3d","originalAuthorName":"刘嘉乐"},{"authorName":"庄育智","id":"78746fe4-78a4-4913-86f3-0fca16d58a82","originalAuthorName":"庄育智"}],"categoryName":"|","doi":"","fpage":"24","id":"9b29a10f-6159-458c-aa9f-f055aa384004","issue":"1","journal":{"abbrevTitle":"JSXB","coverImgSrc":"journal/img/cover/JSXB.jpg","id":"48","issnPpub":"0412-1961","publisherId":"JSXB","title":"金属学报"},"keywords":[],"language":"zh","publisherId":"0412-1961_1960_1_8","title":"含钼不锈钢的<span style=\"color:red\">恒温</span>分解","volume":"5","year":"1960"},{"abstractinfo":"将球团矿分别在900℃<span style=\"color:red\">恒温</span>和升温试验条件下还原，研究了球团矿的还原膨胀行为；分析了2种温度条件下球团膨胀机理；对比了2种条件下的试验结果，观察分析了还原后球团的外观和微观组织形貌，得到了导致2种温度条件下球团膨胀差异的原因。研究结果表明：<span style=\"color:red\">恒温</span>还原球团的最大膨胀值为18.3%，升温还原时为8.3%，<span style=\"color:red\">恒温</span>还原球团的膨胀行为更加明显；裂纹和气孔的形成以及金属铁的析出形态差异是造成膨胀差异的主要原因。由此得出，为了得到与实际生产相近的还原膨胀行为，球团矿应该在升温条件或模拟的生产条件下进行还原试验。","authors":[{"authorName":"白明华","id":"ee2314a7-87e5-475a-a9ef-1b204ddeab24","originalAuthorName":"白明华"},{"authorName":"符远翔","id":"e9bd0528-86a6-4f4a-ba8a-5424ea5f44a1","originalAuthorName":"符远翔"}],"doi":"10.13228/j.boyuan.issn0449-749x.20140479","fpage":"35","id":"912cbaad-89c2-4598-bc18-57dc3c1c450e","issue":"6","journal":{"abbrevTitle":"GT","coverImgSrc":"journal/img/cover/GT.jpg","id":"27","issnPpub":"0449-749X","publisherId":"GT","title":"钢铁"},"keywords":[{"id":"e93fb09e-5b22-45b3-aec5-b19fe744dcb3","keyword":"直接还原","originalKeyword":"直接还原"},{"id":"0a67fca1-0c33-43f5-925f-292d091b21df","keyword":"球团矿","originalKeyword":"球团矿"},{"id":"108efef0-af02-4f15-a7cc-84c1a703b89f","keyword":"升温条件","originalKeyword":"升温条件"},{"id":"69f66fee-5eae-477f-adb7-f9dcc3944d30","keyword":"<span style=\"color:red\">恒温</span>条件","originalKeyword":"恒温条件"},{"id":"5aa456ef-36f3-4bca-a6b6-f9a3e987a352","keyword":"还原膨胀率","originalKeyword":"还原膨胀率"}],"language":"zh","publisherId":"gt201506007","title":"球团矿<span style=\"color:red\">恒温</span>和升温直接还原膨胀行为试验","volume":"","year":"2015"},{"abstractinfo":"通过对４０Ｃｒ，Ｔ１０钢的同材或异材<span style=\"color:red\">恒温</span>超塑焊接接头的断口分析，提出超塑焊接接头是由冶金结合的焊合区及机械结合区、显微空隙等焊接缺陷构成的接头构成模型，可供超塑焊接工艺及质量检测参考．","authors":[{"authorName":"杨蕴林","id":"9c470d14-374a-4983-be3b-b22a8d126e23","originalAuthorName":"杨蕴林"},{"authorName":"李志","id":"f39c8fe3-bab2-4fa0-971b-5bca0bf7cadb","originalAuthorName":"李志"},{"authorName":"李炎","id":"6815ba7a-febd-489f-92cf-f7414b4faf59","originalAuthorName":"李炎"}],"categoryName":"|","doi":"","fpage":"384","id":"0732e332-a5f5-4f05-8923-59cbdba0774a","issue":"20","journal":{"abbrevTitle":"JSXB","coverImgSrc":"journal/img/cover/JSXB.jpg","id":"48","issnPpub":"0412-1961","publisherId":"JSXB","title":"金属学报"},"keywords":[{"id":"f66db98b-9e61-4340-b44c-3f406b10851b","keyword":"超塑焊接","originalKeyword":"超塑焊接"},{"id":"0262bae5-bd9f-493c-adaf-709d31bbba20","keyword":"null","originalKeyword":"null"},{"id":"be471293-c68a-4ccd-bf14-e0bcdb1355f6","keyword":"null","originalKeyword":"null"}],"language":"zh","publisherId":"0412-1961_1995_20_2","title":"<span style=\"color:red\">恒温</span>超塑焊接接头断口分析","volume":"31","year":"1995"},{"abstractinfo":"通过<span style=\"color:red\">恒温</span>烘烤对氨-不锈钢热管<span style=\"color:red\">恒温</span>特性进行了试验研究,其中烘烤温度为270℃.试验结果发现,烘烤过程中有不凝性气体产生,约占总工质质量的0.8％;不凝性气体对热管的影响只与热管工作温度有关,温度低时影响较大,温度升高影响迅速减小;此外,烘烤过程中热管表现出热管效应,与同尺寸同工况下的铝棒相比,氨-不锈钢热管传热能力优越,对温度变化反应灵敏,最高有效导热系数约为壳体材料的159倍,有效导热系数和密度之比约为壳体材料的309.9倍.","authors":[{"authorName":"段彦军","id":"860dc898-ab38-48b0-83d3-295d7ee70fa6","originalAuthorName":"段彦军"},{"authorName":"王焕光","id":"cd3c72ca-876f-49c2-86fd-324b78fae7a5","originalAuthorName":"王焕光"},{"authorName":"陶毓伽","id":"f87e8b9c-05b5-463a-9a5b-502bcae445a2","originalAuthorName":"陶毓伽"},{"authorName":"淮秀兰","id":"6389987a-22ec-4ca8-809e-9eddaa7650e7","originalAuthorName":"淮秀兰"},{"authorName":"曲伟","id":"5864ac67-ef98-433a-b122-f68f7d062f55","originalAuthorName":"曲伟"}],"doi":"","fpage":"1523","id":"a6002639-53dc-4270-93e9-97499f4b48ad","issue":"8","journal":{"abbrevTitle":"GCRWLXB","coverImgSrc":"journal/img/cover/GCRWLXB.jpg","id":"32","issnPpub":"0253-231X","publisherId":"GCRWLXB","title":"工程热物理学报   "},"keywords":[{"id":"0a854bec-ab7e-474b-900c-29c94e20bff8","keyword":"氨-不锈钢热管","originalKeyword":"氨-不锈钢热管"},{"id":"65052c96-005e-4129-9f04-13d548510231","keyword":"热管效应","originalKeyword":"热管效应"},{"id":"ce801eac-8c80-4a5e-8abc-f72f94777984","keyword":"不凝性气体","originalKeyword":"不凝性气体"},{"id":"00161354-8025-45c1-a93e-6491c72d554d","keyword":"有效导热系数","originalKeyword":"有效导热系数"},{"id":"ce03b34e-291d-4e0f-9764-a92beda8fe64","keyword":"相变","originalKeyword":"相变"}],"language":"zh","publisherId":"gcrwlxb201308030","title":"氨-不锈钢热管<span style=\"color:red\">恒温</span>特性试验研究","volume":"34","year":"2013"},{"abstractinfo":"本文主要针对预氧化聚碳硅烷纤维的<span style=\"color:red\">恒温</span>烧结过程进行了基础方面的研究.采用XPS、TG-DTG-DTA、IR对预氧化聚碳硅烷原纤维进行标定;采用日本精密天平连续跟踪纤维质量变化情况,探讨了烧结过程中温度对纤维失重及收缩的影响;采用IR、SEM和数码相机分析了纤维<span style=\"color:red\">恒温</span>烧结过程中微观结构和宏观形貌的变化情况,并对预烧结纤维进行了二次烧结.","authors":[{"authorName":"王浩","id":"8fd2440b-78b3-4686-a2d3-144496646bca","originalAuthorName":"王浩"},{"authorName":"李效东","id":"4e108de7-c710-422c-ae82-c99f80ebcc1f","originalAuthorName":"李效东"},{"authorName":"冯春祥","id":"f4e265f8-ddcd-4703-93b3-93fd2d49612f","originalAuthorName":"冯春祥"},{"authorName":"彭平","id":"8f2311d4-676d-4630-8eaa-cbe4144301a2","originalAuthorName":"彭平"},{"authorName":"陈革","id":"fdf2d1da-1c29-4670-a338-c8abfe43fb87","originalAuthorName":"陈革"}],"doi":"10.3969/j.issn.1673-2812.2002.02.016","fpage":"206","id":"d4830982-e4ac-4dcb-9cca-3f1536a7ecdc","issue":"2","journal":{"abbrevTitle":"CLKXYGCXB","coverImgSrc":"journal/img/cover/CLKXYGCXB.jpg","id":"13","issnPpub":"1673-2812","publisherId":"CLKXYGCXB","title":"材料科学与工程学报"},"keywords":[{"id":"c5feaa68-cff8-4b31-932d-00b204ed8cf1","keyword":"预氧化","originalKeyword":"预氧化"},{"id":"27fa86f5-3cba-4be4-91a1-6d275bd854aa","keyword":"聚碳硅烷纤维","originalKeyword":"聚碳硅烷纤维"},{"id":"ab312be6-f6ed-4368-8ffb-4b449dfcf181","keyword":"<span style=\"color:red\">恒温</span>烧结","originalKeyword":"恒温烧结"},{"id":"a7830750-d27b-4788-921e-f637a270fbfc","keyword":"碳化硅纤维","originalKeyword":"碳化硅纤维"}],"language":"zh","publisherId":"clkxygc200202016","title":"预氧化聚碳硅烷纤维的<span style=\"color:red\">恒温</span>烧结","volume":"20","year":"2002"},{"abstractinfo":"利用热失重技术,取适量聚丙烯餐盒专用粒料在290℃、300℃、310℃、320℃、330℃下<span style=\"color:red\">恒温</span>一定时间,得到聚丙烯的热失重曲线.分别计算聚丙烯在一定温度下,<span style=\"color:red\">恒温</span>失重5％、10％、15％时所经历的时间.并通过阿累尼乌斯方程进行线性拟合,得到聚丙烯失重5％、10％、15％的寿命方程.最终将失重10％时的寿命当作聚丙烯餐盒的使用寿命,并由此推测聚丙烯餐盒在微波炉中的使用次数约为9.7千次.","authors":[{"authorName":"李洋","id":"9f10c74c-97fe-4197-a192-5005e77d6515","originalAuthorName":"李洋"},{"authorName":"刘洋","id":"edf48fc2-ebd4-4523-92e8-1f500f760001","originalAuthorName":"刘洋"},{"authorName":"匡莉","id":"e5d5e16e-b9d7-489f-afb4-34707f908fe2","originalAuthorName":"匡莉"},{"authorName":"高建国","id":"57023c28-2089-464f-89bf-82a28e7292a1","originalAuthorName":"高建国"},{"authorName":"陈敏剑","id":"178193dc-0dfc-4941-a669-a42e992ae62b","originalAuthorName":"陈敏剑"},{"authorName":"宋国君","id":"dc7a6dec-3347-4e49-bd70-69fab7b87276","originalAuthorName":"宋国君"},{"authorName":"李培耀","id":"5ea63e8a-7977-4659-9d3b-f8c2326b4d9a","originalAuthorName":"李培耀"}],"doi":"","fpage":"37","id":"b1d9bf28-57d2-4b05-b5f8-2c7828916bde","issue":"4","journal":{"abbrevTitle":"HCCLLHYYY","coverImgSrc":"journal/img/cover/HCCLLHYYY.jpg","id":"42","issnPpub":"1671-5381","publisherId":"HCCLLHYYY","title":"合成材料老化与应用"},"keywords":[{"id":"85fb4cb3-4796-472b-bac6-62c156e73b7d","keyword":"热失重","originalKeyword":"热失重"},{"id":"fa12b679-e439-4df4-8579-2be43293c9d0","keyword":"聚丙烯","originalKeyword":"聚丙烯"},{"id":"cdb3034b-cc1b-4f15-83fd-a266d9dacd10","keyword":"阿累尼乌斯方程","originalKeyword":"阿累尼乌斯方程"},{"id":"a384dddc-cade-4a53-9ab4-dab89e751386","keyword":"寿命方程","originalKeyword":"寿命方程"}],"language":"zh","publisherId":"hccllhyyy201604009","title":"TG<span style=\"color:red\">恒温</span>法评测聚丙烯餐盒的使用次数","volume":"45","year":"2016"},{"abstractinfo":"用电阻测定及X射线衍射法研究了共晶成分Au-Si合金快速凝固箔带在等温<span style=\"color:red\">时效</span>时的相变过程,提出了由非晶态至平衡态的四阶段转变顺序,分析了各亚稳相的结构和电子浓度特征,说明在等温<span style=\"color:red\">时效</span>过程中亦可生成Hume-Rothery电子化合物及尺寸因素化合物。","authors":[{"authorName":"李松瑞","id":"eda1e050-2e94-448c-ad39-eab5ca66d5ee","originalAuthorName":"李松瑞"},{"authorName":"高世谷","id":"48292fe8-9db5-4d89-97ac-a300fb1b0f5d","originalAuthorName":"高世谷"},{"authorName":"高秀娟","id":"0f1b8d07-bccf-439a-8158-9c2920d83d69","originalAuthorName":"高秀娟"}],"categoryName":"|","doi":"","fpage":"407","id":"5dd1680b-5e4f-4ac0-9e47-198f6a2fb5f0","issue":"5","journal":{"abbrevTitle":"JSXB","coverImgSrc":"journal/img/cover/JSXB.jpg","id":"48","issnPpub":"0412-1961","publisherId":"JSXB","title":"金属学报"},"keywords":[{"id":"23ff69ea-e4ff-4ed3-baa6-362ae190940a","keyword":"Au-Si非晶态","originalKeyword":"Au-Si非晶态"},{"id":"1f80f5f4-850b-40a7-b281-02dfeeeb5419","keyword":"isothermal phase transformation","originalKeyword":"isothermal phase transformation"},{"id":"f1441f8e-f823-4717-89ac-2e477426dc8a","keyword":"null","originalKeyword":"null"}],"language":"zh","publisherId":"0412-1961_1988_5_22","title":"Au-Si非晶态合金的<span style=\"color:red\">恒温</span>相变","volume":"24","year":"1988"}],"totalpage":435,"totalrecord":4341}