{"currentpage":1,"firstResult":0,"maxresult":10,"pagecode":5,"pageindex":{"endPagecode":5,"startPagecode":1},"records":[{"abstractinfo":"介绍了自制的摩擦力显微镜基本原理、结构及关键技术.该仪器能够同时或分别采集横向力和.法向力信号,进行多种微观力函数的程控采集,例如法向力与信号电流的对应关系,针尖与样品间的粘附力还介绍了uN级载荷定量设定方法等.利用该仪器研究了探针与金膜、光盘之间的接触式滑动的微观摩擦行为对微观接触状态进行了理论分析,提出了计算摩擦系数的方法","authors":[{"authorName":"路新春","id":"281e42fd-ce65-4a88-849c-ff9b2cd8468e","originalAuthorName":"路新春"},{"authorName":"王吉会","id":"ddf1c12a-da47-4c6f-af34-ea1714552c7d","originalAuthorName":"王吉会"},{"authorName":"戴长春","id":"2da4a273-5d79-472d-a90a-44c5419c65fc","originalAuthorName":"戴长春"},{"authorName":"<span style=\"color:red\">温</span><span style=\"color:red\">诗</span><span 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style=\"color:red\">铸</span>","id":"a5212a42-e543-45cb-8ab3-792f6827f943","originalAuthorName":"温诗铸"}],"doi":"10.3969/j.issn.1001-1560.2004.z1.002","fpage":"3","id":"98ca8ca0-30bc-4dc9-af2a-8fc2d145eadd","issue":"z1","journal":{"abbrevTitle":"CLBH","coverImgSrc":"journal/img/cover/CLBH.jpg","id":"7","issnPpub":"1001-1560","publisherId":"CLBH","title":"材料保护"},"keywords":[{"id":"9944196d-9229-46e6-bc4b-ca7639728299","keyword":"润滑","originalKeyword":"润滑"},{"id":"a1879499-cfe0-41a8-a674-f703b246f192","keyword":"磨损","originalKeyword":"磨损"},{"id":"adfe5fc3-1ca8-46a2-863d-c6b52ec58de9","keyword":"材料","originalKeyword":"材料"},{"id":"fcca83b1-5633-48a5-82dd-d57fa92afd83","keyword":"生物","originalKeyword":"生物"},{"id":"ada4202b-c739-4381-b0f8-8d20984d01ff","keyword":"表面工程","originalKeyword":"表面工程"}],"language":"zh","publisherId":"clbh2004z1002","title":"试述我国摩擦学研究的发展","volume":"37","year":"2004"},{"abstractinfo":"研究了油基金刚石悬浮液用作磁头抛光材料的抛光性能,用原子力显微镜和扫描电子显微镜观察了磁头抛光后的表面结果表明,纳米金刚石是一种理想的抛光材料,用于超高精度表面加工,其表面抛光质量要明显优于单用国外同类金刚石悬浮液抛光磁头的质量,纳米颗粒的作用十分明显,证实了纳米材料可用超精抛光材料.","authors":[{"authorName":"胡志孟","id":"9ae558ed-66ee-481d-be9a-3bf1aba448ce","originalAuthorName":"胡志孟"},{"authorName":"雒建斌","id":"22f44b23-5e01-4a94-a170-d3771a070495","originalAuthorName":"雒建斌"},{"authorName":"<span 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style=\"color:red\">温</span><span style=\"color:red\">诗</span><span style=\"color:red\">铸</span>","id":"81db5cfa-43e0-45aa-8b73-dd6600fd6d16","originalAuthorName":"温诗铸"}],"doi":"10.3969/j.issn.1001-4381.2000.02.001","fpage":"3","id":"f4ce1720-c376-4a82-8aa0-c72270a76380","issue":"2","journal":{"abbrevTitle":"CLGC","coverImgSrc":"journal/img/cover/CLGC.jpg","id":"9","issnPpub":"1001-4381","publisherId":"CLGC","title":"材料工程"},"keywords":[{"id":"d00297cb-9e9a-45a3-9482-0554354dce60","keyword":"类金刚石薄膜","originalKeyword":"类金刚石薄膜"},{"id":"59c6264e-1c03-4261-b502-a6024a0fbedb","keyword":"IBAD","originalKeyword":"IBAD"},{"id":"d09977bd-d0ec-40ce-bf43-b83e43e4ac52","keyword":"纳米硬度","originalKeyword":"纳米硬度"}],"language":"zh","publisherId":"clgc200002001","title":"离子辅助轰击能量对类金刚石薄膜性能的影响","volume":"","year":"2000"},{"abstractinfo":"对外加直流电场作用下电流变液的拉伸、压缩和剪切特性进行了实验研究.实验结果表明,在外电场作用下,电流变液的压缩强度比剪切强度约高一个数量级,压缩强度是拉伸强度的2～3倍.压缩弹性模量约与压缩过程中电场强度的三次方成正比.压缩应力与电流变液本身性能、外加电压大小和压缩应变都有密切关系.拉伸屈服应力为剪切屈服应力的拉伸屈服应力和剪切屈服应力的3～4倍,据此计算得到剪切屈服应变角度在15°～18.5°之间.","authors":[{"authorName":"田煜","id":"59238f94-0489-40e0-93b4-3ec36d838606","originalAuthorName":"田煜"},{"authorName":"孟永钢","id":"bc2de4ac-d149-4df4-8a8e-c6110f70a0c4","originalAuthorName":"孟永钢"},{"authorName":"茅海荣","id":"f14a5b8a-0230-4ff5-9ad4-af72aed7fc05","originalAuthorName":"茅海荣"},{"authorName":"<span style=\"color:red\">温</span><span style=\"color:red\">诗</span><span style=\"color:red\">铸</span>","id":"bfaa3245-7ba4-4210-bb63-3410493b5264","originalAuthorName":"温诗铸"}],"doi":"10.3321/j.issn:1000-3851.2003.01.017","fpage":"91","id":"c71e481c-142a-46dc-8f92-f70c45bc534a","issue":"1","journal":{"abbrevTitle":"FHCLXB","coverImgSrc":"journal/img/cover/FHCLXB.jpg","id":"26","issnPpub":"1000-3851","publisherId":"FHCLXB","title":"复合材料学报"},"keywords":[{"id":"3b91d996-f38f-4d2b-8913-cf9473089bcc","keyword":"电流变液","originalKeyword":"电流变液"},{"id":"49a02a9a-9d1c-46d5-813c-b43054e0ea6d","keyword":"拉伸屈服应力","originalKeyword":"拉伸屈服应力"},{"id":"0f9a352e-dfa1-4764-b3c0-c97a6c8b7531","keyword":"压缩应力","originalKeyword":"压缩应力"},{"id":"2600d304-a7fe-41e5-802f-148dde0f29e7","keyword":"剪切屈服应力","originalKeyword":"剪切屈服应力"}],"language":"zh","publisherId":"fhclxb200301017","title":"电场作用下电流变液的拉伸、压缩和剪切特性","volume":"20","year":"2003"},{"abstractinfo":"报道了薄膜润滑的本质以及它与弹流润滑和边界润滑间关系的研究结果.根据各种特性膜厚度的变化分析了各润滑状态之间的转化关系,提出了润滑状态与宏观摩擦副所处状态关联与区分准则","authors":[{"authorName":"雒建斌","id":"b84012e8-65d6-4dff-99ab-6ce48f4409fe","originalAuthorName":"雒建斌"},{"authorName":"<span style=\"color:red\">温</span><span style=\"color:red\">诗</span><span style=\"color:red\">铸</span>","id":"628bdf4d-9b10-4019-aa55-c4ed3810f040","originalAuthorName":"温诗铸"},{"authorName":"史兵","id":"199ef67b-8934-43be-bdcc-ca139ce54927","originalAuthorName":"史兵"}],"categoryName":"|","doi":"","fpage":"120","id":"c6600028-9f18-408a-95fa-a375b01ebd94","issue":"2","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":"a1178ec4-2daa-4511-aec4-e4d3051c91e5","keyword":"薄膜润滑","originalKeyword":"薄膜润滑"},{"id":"6e9d2d00-ff21-4b30-ad43-1ab50511c98a","keyword":"null","originalKeyword":"null"},{"id":"b260b164-301d-4c49-8e21-ffe154d7b9f5","keyword":"null","originalKeyword":"null"},{"id":"fb686d08-5b78-443f-8a88-11bcf90992cb","keyword":"null","originalKeyword":"null"}],"language":"zh","publisherId":"1005-3093_1997_2_15","title":"润滑的状态转化","volume":"11","year":"1997"},{"abstractinfo":"构建了对电流变液对电场的动态响应过程进行研究的测试系统.此系统的响应快于其它用于同样研究的系统,可以达到0.01ms的响应速度.使用这个测试系统对电流变液的极化和退极化过程以及在不同剪切速率下对电场的动态响应进行了研究表明,基于NaY沸石和硅油的电流变液对电场的上升响应时间常数在毫秒量级,且与剪切速率的-3/4次方成正比,与其它研究人员的理论描述基本一致.直流电场关闭时,在1ms左右电流变液就回复到了原有零电场状态.剪切速率越高,电流变液回复所需时间也越短.另外发现剪切应力有0.3ms左右时间延迟.","authors":[{"authorName":"田煜","id":"7a99a373-cc98-4bb5-b1cf-722d5f5b553b","originalAuthorName":"田煜"},{"authorName":"孟永钢","id":"13f06bbb-c951-4398-ac88-bd8581c35a8d","originalAuthorName":"孟永钢"},{"authorName":"<span style=\"color:red\">温</span><span style=\"color:red\">诗</span><span style=\"color:red\">铸</span>","id":"d6e7a7ed-15c0-4dee-8996-f01ffa40537d","originalAuthorName":"温诗铸"}],"doi":"","fpage":"180","id":"f9a3acbe-a89e-43df-8268-f08dec73da4e","issue":"2","journal":{"abbrevTitle":"GNCL","coverImgSrc":"journal/img/cover/GNCL.jpg","id":"33","issnPpub":"1001-9731","publisherId":"GNCL","title":"功能材料"},"keywords":[{"id":"3add1a02-ee25-40a6-a4af-e3896ea65daf","keyword":"电流变液","originalKeyword":"电流变液"},{"id":"57566f82-83ca-4662-a50a-3d58952e3641","keyword":"动态响应","originalKeyword":"动态响应"},{"id":"4af87a41-4d42-4baf-b808-89987499c868","keyword":"响应时间常数","originalKeyword":"响应时间常数"}],"language":"zh","publisherId":"gncl200202022","title":"基于NaY沸石和硅油的电流变液的动态响应实验研究","volume":"33","year":"2002"},{"abstractinfo":"探讨了小方坯在步进冷床下线的<span style=\"color:red\">温</span>降过程.理论推导了小方坯辐射散热的计算公式,并利用有限元软件对连<span style=\"color:red\">铸</span>小方坯冷却模型进行了数值模拟,对比分析了不同条件对<span style=\"color:red\">铸</span>坯<span style=\"color:red\">温</span>降的影响,结果表明<span style=\"color:red\">铸</span>坯<span style=\"color:red\">温</span>降过程主要由热辐射散热决定.通过考虑不同影响因素及实际生产条件的差异,得出了小方坯在步进冷床下线的<span style=\"color:red\">温</span>降时间估算公式,用于指导相关工程设计.","authors":[{"authorName":"李东辉","id":"4627b8aa-211c-48c1-bd02-6e106cd60d26","originalAuthorName":"李东辉"}],"doi":"10.13228/j.boyuan.issn1005-4006.20160013","fpage":"35","id":"6cf0e215-e3e0-4a88-95b3-d1c59999ef81","issue":"5","journal":{"abbrevTitle":"LZ","coverImgSrc":"journal/img/cover/LZ.jpg","id":"52","issnPpub":"1005-4006","publisherId":"LZ","title":"连铸"},"keywords":[{"id":"841050ad-2dc1-455e-b5b8-b94e93bdd849","keyword":"连<span 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style=\"color:red\">铸</span>生产提供了一个计算机\"实验平台\".通过仿真分析,可部分或全部取代现场试浇,节约了人材物的投入,带来可观的经济效益.","authors":[{"authorName":"史荣","id":"67f547a9-6da2-45df-ba9e-e77bca5c9114","originalAuthorName":"史荣"},{"authorName":"崔小朝","id":"da4af244-0bed-457e-a9d3-7ff75aa58880","originalAuthorName":"崔小朝"},{"authorName":"刘才","id":"25f87bbc-79c8-4872-a459-13273ced08a8","originalAuthorName":"刘才"},{"authorName":"杜艳平","id":"fb1fa4aa-b403-498c-8269-5101ce9d08e9","originalAuthorName":"杜艳平"},{"authorName":"杜建新","id":"f54b5530-ac6d-4342-bde3-2dfa7c71e26d","originalAuthorName":"杜建新"}],"doi":"10.3969/j.issn.1005-4006.2001.01.008","fpage":"21","id":"25f798cc-8fc4-4125-affa-02bb4efcc4c3","issue":"1","journal":{"abbrevTitle":"LZ","coverImgSrc":"journal/img/cover/LZ.jpg","id":"52","issnPpub":"1005-4006","publisherId":"LZ","title":"连铸"},"keywords":[{"id":"f3789186-8d96-4b20-9629-ef815c1e5a43","keyword":"","originalKeyword":""}],"language":"zh","publisherId":"lz200101008","title":"连<span style=\"color:red\">铸</span>过程液固<span style=\"color:red\">温</span>耦合计算机仿真软件","volume":"","year":"2001"},{"abstractinfo":"连<span style=\"color:red\">铸</span>过程中,坯壳表面回<span style=\"color:red\">温</span>的发生机制主要有两种.一种是由于二冷区换热方式的差异性;另一种是由于放热强度和换热强度的差异性.拉坯速度、冷却强度及冷却段长度均对坯壳回<span style=\"color:red\">温</span>有着重要的影响.其中拉坯速度及冷却强度的影响可通过二冷优化配水来减缓,而冷却段长度的影响需要在设计之初优化连铸机二冷区设计的合理性.","authors":[{"authorName":"韩占光","id":"124c72c8-8723-445b-a24b-f6fe763a9612","originalAuthorName":"韩占光"}],"doi":"","fpage":"11","id":"7b0109ed-c6d6-4766-a5b3-f1fbc72b99a8","issue":"3","journal":{"abbrevTitle":"LZ","coverImgSrc":"journal/img/cover/LZ.jpg","id":"52","issnPpub":"1005-4006","publisherId":"LZ","title":"连铸"},"keywords":[{"id":"c8d6bfc8-8f05-4e0e-86e9-ad48158abb3a","keyword":"连<span style=\"color:red\">铸</span>","originalKeyword":"连铸"},{"id":"893de129-b670-48fb-9d7e-faf217864ba2","keyword":"二冷区","originalKeyword":"二冷区"},{"id":"d0b3724a-056e-42ee-9573-8099f8a2b140","keyword":"回<span style=\"color:red\">温</span>","originalKeyword":"回温"},{"id":"3560ee10-7086-4077-979b-617b090727f8","keyword":"冷却制度","originalKeyword":"冷却制度"},{"id":"c7c25b06-0dd6-4656-8358-4d90c26fdd95","keyword":"冷却段长度","originalKeyword":"冷却段长度"}],"language":"zh","publisherId":"lz201403003","title":"连<span style=\"color:red\">铸</span>坯壳表面温度回<span style=\"color:red\">温</span>机制及影响因素","volume":"","year":"2014"}],"totalpage":1075,"totalrecord":10749}