{"currentpage":1,"firstResult":0,"maxresult":10,"pagecode":5,"pageindex":{"endPagecode":5,"startPagecode":1},"records":[{"abstractinfo":"考察了特种氟硅橡胶在RP-3航空煤油介质环境中的老化行为,采用<span style=\"color:red\">傅里叶变换</span><span style=\"color:red\">衰减</span><span style=\"color:red\">全反射</span><span style=\"color:red\">红外光谱</span>(ATR-FTIR)对不同老化时间点内试样的特征基团进行了表征.利用<span style=\"color:red\">红外</span>差谱法研究了老化过程中各官能团相对含量的变化情况,结合材料的力学性能分析了特种氟硅橡胶耐RP-3航空煤油可能的老化机理:材料的老化初期,主要以物理老化为主,进入中后期则以化学老化为主.","authors":[{"authorName":"王荣华","id":"83dd2bc7-f2ab-4fc8-adc0-4584a3158c81","originalAuthorName":"王荣华"},{"authorName":"李晖","id":"eaf95d01-f2a8-4d98-ac5b-060b931daa32","originalAuthorName":"李晖"},{"authorName":"刘亚平","id":"d7cbfd12-185e-4bdb-87a2-0686684f57ef","originalAuthorName":"刘亚平"},{"authorName":"孙岩","id":"822ad232-e13b-4393-a84e-cdf818995b04","originalAuthorName":"孙岩"},{"authorName":"李倩倩","id":"99b59966-aeaf-459d-8673-86a2e65837cf","originalAuthorName":"李倩倩"},{"authorName":"王登霞","id":"451b9e43-3a90-4ad6-848a-de133b0ee72e","originalAuthorName":"王登霞"},{"authorName":"谢可勇","id":"2ac56644-5cde-417d-b372-9c2f20abac11","originalAuthorName":"谢可勇"}],"doi":"","fpage":"99","id":"aab3405e-723c-4a3a-9b0a-57af8875aa87","issue":"4","journal":{"abbrevTitle":"CLDB","coverImgSrc":"journal/img/cover/CLDB.jpg","id":"8","issnPpub":"1005-023X","publisherId":"CLDB","title":"材料导报"},"keywords":[{"id":"14d1fe13-a1bb-49df-9dd5-c8f0c7d2c537","keyword":"介质老化","originalKeyword":"介质老化"},{"id":"83d9fa04-07e2-4fef-8cfd-c48248a97515","keyword":"特种氟硅橡胶","originalKeyword":"特种氟硅橡胶"},{"id":"02b46c31-4e05-425b-afd2-b8c92caef7ff","keyword":"RP-3航空煤油","originalKeyword":"RP-3航空煤油"},{"id":"bbaf51c2-c2a6-435f-baae-d1ba7bce75af","keyword":"<span style=\"color:red\">傅里叶变换</span><span style=\"color:red\">衰减</span><span style=\"color:red\">全反射</span><span style=\"color:red\">红外光谱</span>","originalKeyword":"傅里叶变换衰减全反射红外光谱"},{"id":"6deda45b-bb18-4289-a04a-2cacc02ca134","keyword":"物理老化","originalKeyword":"物理老化"}],"language":"zh","publisherId":"cldb201404026","title":"特种氟硅橡胶耐介质老化行为规律研究","volume":"28","year":"2014"},{"abstractinfo":"<span style=\"color:red\">全反射</span><span style=\"color:red\">傅里叶变换</span>成像<span style=\"color:red\">光谱</span>仪在航空航天遥感等领域具有重要的应用.专门设置的柱面镜和准直系统,使得光路结构复杂,不仅增加了成像<span style=\"color:red\">光谱</span>议光学设计和安装调试、维护的难度,同时也增加了成像<span style=\"color:red\">光谱</span>议的重量和光能的损耗.提出了一种无成像镜实现成像<span style=\"color:red\">光谱</span>检测的结构,对其检测机理进行了研究.对波长632.8 nm、940 nm和3000 nm进行<span style=\"color:red\">光谱</span>检测的仿真实验表明,其<span style=\"color:red\">光谱</span>测量误差小于1％.","authors":[{"authorName":"赵远","id":"e2797d66-3274-44f8-8176-c45cf9ce4201","originalAuthorName":"赵远"},{"authorName":"赵光兴","id":"56216dbf-2ff8-4a04-8d4c-7196d41e2231","originalAuthorName":"赵光兴"}],"doi":"10.3969/j.issn.1007-5461.2014.04.015","fpage":"502","id":"d035f2b3-8f6d-4593-9cf6-0b6064f31e24","issue":"4","journal":{"abbrevTitle":"LZDZXB","coverImgSrc":"journal/img/cover/LZDZXB.jpg","id":"53","issnPpub":"1007-5461","publisherId":"LZDZXB","title":"量子电子学报   "},"keywords":[{"id":"52159e1f-5eb1-4e46-b64e-926f222d85aa","keyword":"<span style=\"color:red\">光谱</span>学","originalKeyword":"光谱学"},{"id":"62305a72-0469-45c6-9a78-3b0d75835051","keyword":"<span style=\"color:red\">全反射</span><span style=\"color:red\">傅里叶变换</span>成像<span style=\"color:red\">光谱</span>仪","originalKeyword":"全反射傅里叶变换成像光谱仪"},{"id":"7e30be62-e342-4b22-8fb6-86e5dd4c6a19","keyword":"成像镜","originalKeyword":"成像镜"},{"id":"255d3d85-7ef8-4d2b-b300-dacca5d134bd","keyword":"<span style=\"color:red\">光谱</span>检测","originalKeyword":"光谱检测"}],"language":"zh","publisherId":"lzdzxb201404015","title":"无成像镜<span style=\"color:red\">全反射</span><span style=\"color:red\">傅里叶变换</span>成像结构<span style=\"color:red\">光谱</span>检测的机理","volume":"31","year":"2014"},{"abstractinfo":"利用偏振<span style=\"color:red\">傅里叶变换</span><span style=\"color:red\">红外</span>(FTIR)<span style=\"color:red\">光谱</span>仪测量目标<span style=\"color:red\">红外</span>偏振特性,需要对偏振FTIR<span style=\"color:red\">光谱</span>仪进行定标,计算出<span style=\"color:red\">红外</span>辐射目标的绝对<span style=\"color:red\">光谱</span>能量分布.利用黑体进行偏振FTIR<span style=\"color:red\">光谱</span>仪定标时,发现不同偏振检测方向的仪器响应有一定偏差,即仪器存在偏振敏感性.通过对仪器偏振特性的定标检测,得到仪器偏振响应函数和偏置特性曲线,应用定标结果,将会消除<span style=\"color:red\">红外</span>偏振仪器自身的偏振敏感性对目标偏振特性的影响,为提高目标的<span style=\"color:red\">红外</span>偏振探测精度打下基础.","authors":[{"authorName":"龚忠清","id":"43f5ba9e-dc2e-403a-a596-182c9ef99a7e","originalAuthorName":"龚忠清"},{"authorName":"孙晓兵","id":"aa2f121f-0402-463c-aee5-58919ecfd3df","originalAuthorName":"孙晓兵"},{"authorName":"张荞","id":"28fa2a66-4d6d-423e-9237-5b5eb808413b","originalAuthorName":"张荞"},{"authorName":"洪津","id":"92cd9a4d-8e4c-4b24-807b-6ffc9898b656","originalAuthorName":"洪津"}],"doi":"10.3969/j.issn.1007-5461.2011.02.003","fpage":"142","id":"5b8f3415-4108-46e6-82d3-129e27eb6331","issue":"2","journal":{"abbrevTitle":"LZDZXB","coverImgSrc":"journal/img/cover/LZDZXB.jpg","id":"53","issnPpub":"1007-5461","publisherId":"LZDZXB","title":"量子电子学报   "},"keywords":[{"id":"ae681201-f5b4-4086-9b88-c964e393dd6b","keyword":"傅里叶光学","originalKeyword":"傅里叶光学"},{"id":"114399c3-eb84-43c6-961d-77f57e4e3373","keyword":"仪器响应函数","originalKeyword":"仪器响应函数"},{"id":"aff827e1-1c0b-4d57-b0dc-ddd5954aed2e","keyword":"定标","originalKeyword":"定标"},{"id":"8bd71308-bd62-40d2-93ff-104cfb92ea08","keyword":"偏振","originalKeyword":"偏振"},{"id":"33dde52a-a7a3-43fa-ae68-5b1cfdc0f9f2","keyword":"<span style=\"color:red\">红外</span>","originalKeyword":"红外"}],"language":"zh","publisherId":"lzdzxb201102003","title":"偏振<span style=\"color:red\">傅里叶变换</span><span style=\"color:red\">红外光谱</span>仪定标研究","volume":"28","year":"2011"},{"abstractinfo":"用<span style=\"color:red\">衰减</span><span style=\"color:red\">全反射</span><span style=\"color:red\">红外光谱</span>(FTIR-ATR)技术研究了纳米SiO2粒子在紫外光固化复合涂层中的迁移现象,并对影响纳米SiO2粒子在涂层中分布梯度的因素进行了半定量分析.研究结果表明,纳米SiO2粒子在光固化过程中向涂层接触空气的表面迁移,在表面层富集.当纳米SiO2粒子含量较高、分子量较小、接枝率较高,或者在极性较大的基体树脂中时,迁移较快,分布梯度较大.","authors":[{"authorName":"邱玮丽","id":"a5f43deb-7470-47ee-b026-3b3a05ade189","originalAuthorName":"邱玮丽"},{"authorName":"马晓华","id":"31872c66-53dd-4585-9e70-c3f78c3ae9d8","originalAuthorName":"马晓华"},{"authorName":"杨清河","id":"f2654b05-745e-40c4-bf6b-f2d4c130b791","originalAuthorName":"杨清河"},{"authorName":"付延鲍","id":"bfce92e4-222d-47bc-80e9-da4ff5bf7937","originalAuthorName":"付延鲍"},{"authorName":"宗祥福","id":"0163aed7-7158-4577-8fdf-ad6c3bfe6a15","originalAuthorName":"宗祥福"}],"doi":"10.3321/j.issn:1000-3851.2004.04.011","fpage":"54","id":"9108aae6-c4fc-4d78-8c87-96ef45657110","issue":"4","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":"35559a06-bece-488a-a750-b0d3151da25d","keyword":"<span style=\"color:red\">衰减</span><span style=\"color:red\">全反射</span><span style=\"color:red\">红外光谱</span>(FTIR-ATR)","originalKeyword":"衰减全反射红外光谱(FTIR-ATR)"},{"id":"01a94818-91ae-4ac7-ba4a-9cb5dd076a19","keyword":"纳米SiO2","originalKeyword":"纳米SiO2"},{"id":"5f8be849-853b-4f43-a091-e7efc27c291c","keyword":"紫外光固化复合涂层","originalKeyword":"紫外光固化复合涂层"}],"language":"zh","publisherId":"fhclxb200404011","title":"用<span style=\"color:red\">衰减</span><span style=\"color:red\">全反射</span><span style=\"color:red\">红外光谱</span>研究纳米SiO2粒子在复合涂层中的迁移现象","volume":"21","year":"2004"},{"abstractinfo":"采用自蔓延燃烧法制备了Ti0.9Mn0.05Fe0.05O2-δ催化剂,运用原位漫<span style=\"color:red\">反射</span><span style=\"color:red\">傅里叶变换</span><span style=\"color:red\">红外光谱</span>对该催化剂的NO和NH3稳态吸附以及NO和NH3瞬态反应进行了详细地分析与讨论.结果表明,相比于Lewis酸性位,150oC时Br?nsted酸性位吸附的NH3更具有SCR活性；与双齿硝酸盐和桥式硝酸盐相比, NO吸附产生的单齿硝酸盐是主要的中间物种；该SCR反应遵循Eley-Rideal和Langmuir-Hinshelwood机理,但以后者为主.另外, O2的存在有利于NO的氧化和配位态NH3的活化.","authors":[{"authorName":"陈婷","id":"698d74d6-09d9-4b36-bae6-1edbc1df6bef","originalAuthorName":"陈婷"},{"authorName":"管斌","id":"447a1485-0bcb-4f88-91ef-7598b77b78bb","originalAuthorName":"管斌"},{"authorName":"林赫","id":"d7540d4f-faf9-4ac5-b571-03ffea87f59f","originalAuthorName":"林赫"},{"authorName":"朱霖","id":"cb7f8f17-2199-46c1-a209-5a547d93461e","originalAuthorName":"朱霖"}],"doi":"10.1016/S1872-2067(12)60730-X","fpage":"294","id":"decf4848-539c-4136-8716-699003cfb0a2","issue":"3","journal":{"abbrevTitle":"CHXB","coverImgSrc":"journal/img/cover/CHXB.jpg","id":"18","issnPpub":"0253-9837","publisherId":"CHXB","title":"催化学报   "},"keywords":[{"id":"4d8dad31-5c47-464d-9424-442aa5c570fe","keyword":"氮氧化物","originalKeyword":"氮氧化物"},{"id":"c607470a-bb0b-467b-a9e4-2661a02ab8d2","keyword":"氨","originalKeyword":"氨"},{"id":"fff2dd33-1b62-4680-87b5-f603eb96d923","keyword":"锰铁基催化剂","originalKeyword":"锰铁基催化剂"},{"id":"032f23d7-c8c4-483b-a306-7760b0a21d3d","keyword":"低温选择性催化还原","originalKeyword":"低温选择性催化还原"},{"id":"0ac77db7-d05f-4893-8b91-5487a5b50c02","keyword":"原位漫<span style=\"color:red\">反射</span><span style=\"color:red\">傅里叶变换</span><span style=\"color:red\">红外光谱</span>","originalKeyword":"原位漫反射傅里叶变换红外光谱"}],"language":"zh","publisherId":"cuihuaxb201403005","title":"原位漫<span style=\"color:red\">反射</span><span style=\"color:red\">傅里叶变换</span><span style=\"color:red\">红外光谱</span>研究锰铁基催化剂上低温选择性催化还原反应机理","volume":"","year":"2014"},{"abstractinfo":"在直线扫描式高精度<span style=\"color:red\">傅里叶变换</span><span style=\"color:red\">红外</span>(FTIR)<span style=\"color:red\">光谱</span>仪系统的研制过程中,为了达到<span style=\"color:red\">光谱</span>图的质量和分辨率要求,提出了一种利用DSP芯片TMS320F28335作为控制器,直线电机运动平台带动动镜的系统设计方法.介绍了FTIR的优点以及TMS320F28335的性能特点,分析了FTIR系统的原理,详细阐述了电机控制系统的设计方案,给出了DSP、电机驱动器以及电机模块之间的硬件接口电路和软件实现方法.实验证明,该电机控制系统具有很好的稳定性和很高的运动精度,其位置运动精度能够达到0.1 μm,保证动镜做稳定可靠的直线运动.","authors":[{"authorName":"王伟","id":"373de64c-a62a-4e73-b47c-d894bb182147","originalAuthorName":"王伟"},{"authorName":"陆亦怀","id":"724ea2c5-b931-44c8-9f6e-702274f7bb30","originalAuthorName":"陆亦怀"},{"authorName":"陆钒","id":"ef781c93-d8d9-44ef-85a4-eb933ef4bd72","originalAuthorName":"陆钒"},{"authorName":"张天舒","id":"b1290521-0bdc-427e-9e98-5acfeab28a1b","originalAuthorName":"张天舒"},{"authorName":"付毅宾","id":"ca23ac3a-35cb-4aef-b012-a01040efe404","originalAuthorName":"付毅宾"}],"doi":"10.3969/j.issn.1007-5461.2015.01.002","fpage":"8","id":"a747afd8-4471-4611-8dc5-3aad101d9b6a","issue":"1","journal":{"abbrevTitle":"LZ","coverImgSrc":"journal/img/cover/LZ.jpg","id":"52","issnPpub":"1005-4006","publisherId":"LZ","title":"连铸"},"keywords":[{"id":"26f5cdb2-c864-4b8c-845f-4b8d7a9e64d6","keyword":"光电子学","originalKeyword":"光电子学"},{"id":"de233221-a03e-43ac-abf2-0fc922d5ade6","keyword":"<span style=\"color:red\">傅里叶变换</span><span style=\"color:red\">红外光谱</span>仪","originalKeyword":"傅里叶变换红外光谱仪"},{"id":"b1685fd2-4662-45a7-86b9-b17acd0fc693","keyword":"TMS320F28335","originalKeyword":"TMS320F28335"},{"id":"284846ee-e31c-4109-90dc-ae9fedb1a550","keyword":"动镜","originalKeyword":"动镜"},{"id":"c28661b7-da70-4e30-8e62-9468511f1f08","keyword":"电机","originalKeyword":"电机"}],"language":"zh","publisherId":"lzdzxb201501002","title":"基于DSP的<span style=\"color:red\">傅里叶变换</span><span style=\"color:red\">红外光谱</span>仪动镜控制系统设计","volume":"32","year":"2015"},{"abstractinfo":"折射式扫描干涉仪与传统干涉仪相比具有高稳定性和高光通量等优点,但其光程的改变是由补偿光楔的运动产生的,其结构也导致了不同波长的光经过的光程不同,从而导致了由干涉图<span style=\"color:red\">变换</span>出来的<span style=\"color:red\">光谱</span>在波数上有偏差.采用的波数校正方法很好的解决了这一问题,并具有很高的精度.","authors":[{"authorName":"熊伟","id":"473b12c8-826d-49c9-afde-413194c79660","originalAuthorName":"熊伟"},{"authorName":"方勇华","id":"20521440-30de-4cad-ae99-3800429782ed","originalAuthorName":"方勇华"},{"authorName":"荀毓龙","id":"5a985f70-266e-4a5d-a615-078c1f77eafe","originalAuthorName":"荀毓龙"},{"authorName":"黄烨","id":"5c9a9085-31b3-4e82-9920-042ace4be788","originalAuthorName":"黄烨"},{"authorName":"黄斌","id":"93f89929-3aee-4f1d-92a2-a40902a3a7a8","originalAuthorName":"黄斌"}],"doi":"10.3969/j.issn.1007-5461.2005.02.007","fpage":"165","id":"ea5d794f-0738-4027-89c2-1e9405e0a1d6","issue":"2","journal":{"abbrevTitle":"LZDZXB","coverImgSrc":"journal/img/cover/LZDZXB.jpg","id":"53","issnPpub":"1007-5461","publisherId":"LZDZXB","title":"量子电子学报   "},"keywords":[{"id":"f4cd5ec5-8dde-4135-9bda-531bd416d4d1","keyword":"应用光学","originalKeyword":"应用光学"},{"id":"e8aeffa4-c243-4ece-a7cd-dcc48b3fe050","keyword":"波数","originalKeyword":"波数"},{"id":"29a7b639-ddba-41c3-984c-741067373020","keyword":"校正","originalKeyword":"校正"},{"id":"de991fc6-243f-4b18-9cb6-49c1a5807fd5","keyword":"干涉","originalKeyword":"干涉"}],"language":"zh","publisherId":"lzdzxb200502007","title":"<span style=\"color:red\">傅里叶变换</span><span style=\"color:red\">红外光谱</span>信息处理中的波数校正","volume":"22","year":"2005"},{"abstractinfo":"采用原位漫<span style=\"color:red\">反射</span><span style=\"color:red\">傅里叶变换</span><span style=\"color:red\">红外光谱</span>研究了CH4和CO2在不同粒径的Ni/SiO2催化剂上的吸附及活化. 结果表明,在不同粒径的催化剂上,检测到有CH4解离生成的CHx(x=1～3)物种,以及催化剂表面吸附的CHx物种与表面- OH 作用生成的CHx-O物种. CH4的裂解强烈依赖于催化剂表面Ni颗粒的大小,在粒径8 nm左右的Ni颗粒上,CH4较易解离;CO2难以直接在Ni/SiO2催化剂表面发生解离吸附,但CH4解离生成的吸附H对CO2的解离吸附具有明显的促进作用;CH4与CO2共吸附时,较小粒径的Ni可以促进CO2与表面氧物种发生反应,生成单齿表面碳酸盐物种.","authors":[{"authorName":"郭建忠","id":"70135b23-ba89-4bbd-8c13-3c59e2e3deec","originalAuthorName":"郭建忠"},{"authorName":"侯昭胤","id":"8b222d14-cb03-4d46-ac4c-2de196ec34c6","originalAuthorName":"侯昭胤"},{"authorName":"高静","id":"f3671e5d-ddc2-4fe6-a95f-0c2a0b8d2bc8","originalAuthorName":"高静"},{"authorName":"郑小明","id":"fa6e91ed-3620-4dd2-b67a-de0dff9b7776","originalAuthorName":"郑小明"}],"doi":"","fpage":"22","id":"89eb3746-b0ef-4efb-b3da-2268c3bd7bb1","issue":"1","journal":{"abbrevTitle":"CHXB","coverImgSrc":"journal/img/cover/CHXB.jpg","id":"18","issnPpub":"0253-9837","publisherId":"CHXB","title":"催化学报   "},"keywords":[{"id":"7c4dc028-e8dd-4de6-8099-d99f07ce204d","keyword":"甲烷","originalKeyword":"甲烷"},{"id":"1ecac8b6-3536-45ca-b9b8-6654b4697148","keyword":"二氧化碳","originalKeyword":"二氧化碳"},{"id":"91c42382-f3d4-41bd-b99a-1ddeb931d5ab","keyword":"镍","originalKeyword":"镍"},{"id":"4cf2eac0-437b-43b6-b57b-c76f437b1fcd","keyword":"二氧化硅","originalKeyword":"二氧化硅"},{"id":"e8cddc31-4c50-430a-9525-198c691cd8db","keyword":"负载型催化剂","originalKeyword":"负载型催化剂"},{"id":"b28d5b4c-543f-4be3-9f05-682807eae0c8","keyword":"吸附","originalKeyword":"吸附"},{"id":"c78a986c-90a1-4d9b-9d97-5f6043787af9","keyword":"活化","originalKeyword":"活化"},{"id":"548fd9b3-1130-4bb4-bb31-feab10b93bc9","keyword":"<span style=\"color:red\">红外光谱</span>","originalKeyword":"红外光谱"}],"language":"zh","publisherId":"cuihuaxb200701006","title":"不同粒径的Ni/SiO2催化剂上CH4和CO2吸附活化的漫<span style=\"color:red\">反射</span><span style=\"color:red\">傅里叶变换</span><span style=\"color:red\">红外光谱</span>研究","volume":"28","year":"2007"},{"abstractinfo":"将<span style=\"color:red\">红外</span><span style=\"color:red\">衰减</span><span style=\"color:red\">全反射</span>法(ATR-FTIR)和图谱差示法用于橡胶产品的材质和故障分析.在对橡胶产品进行材质分析时,虽然AIR-FT-IR法可无损地直接检测样品,但在所采集的<span style=\"color:red\">红外光谱</span>图中常含有各种有机和无机添加剂的谱峰,这给橡胶制品的材质分析带来了困难.对所测样品的表面分别用有机溶剂和无机酸处理可排除它们的干扰,最终表明,所分析橡胶产品的成分分别是聚氯乙烯(PVC)和苯乙烯-氢化丁二烯-苯乙烯嵌段共聚物(SEBS)；对存在故障的橡胶产品可采用图谱差示法求出引起故障原因的物质的<span style=\"color:red\">红外光谱</span>,对于本次分析的样品故障而言,它们分别是抗氧剂和阻燃剂使用不当所致.","authors":[{"authorName":"张小俊","id":"14cb6902-2c28-4290-9ecb-25ff6cb907a8","originalAuthorName":"张小俊"},{"authorName":"姚杰","id":"2759b8fb-250d-47ac-83c0-75e2f0a795d0","originalAuthorName":"姚杰"}],"doi":"","fpage":"127","id":"bcb0c822-db6e-4cdb-a54f-51c63807b7d7","issue":"7","journal":{"abbrevTitle":"GFZCLKXYGC","coverImgSrc":"journal/img/cover/GFZCLKXYGC.jpg","id":"31","issnPpub":"1000-7555","publisherId":"GFZCLKXYGC","title":"高分子材料科学与工程"},"keywords":[{"id":"2db9ba28-1b09-4faa-bb6b-730f590588d2","keyword":"<span style=\"color:red\">红外</span><span style=\"color:red\">衰减</span><span style=\"color:red\">全反射</span>法","originalKeyword":"红外衰减全反射法"},{"id":"d494f084-facc-4beb-ac41-a6f3cff753e7","keyword":"聚氯乙烯","originalKeyword":"聚氯乙烯"},{"id":"62df658f-198b-4599-a0a4-06da46b40e40","keyword":"苯乙烯-氢化丁二烯-苯乙烯嵌段共聚物","originalKeyword":"苯乙烯-氢化丁二烯-苯乙烯嵌段共聚物"},{"id":"bd0c947b-09d2-4c52-9247-d12a3f2f61c7","keyword":"材质分析","originalKeyword":"材质分析"},{"id":"cac61d05-0d58-4a6b-9bbd-845c3113213f","keyword":"故障分析","originalKeyword":"故障分析"}],"language":"zh","publisherId":"gfzclkxygc201307031","title":"<span style=\"color:red\">红外</span><span style=\"color:red\">衰减</span><span style=\"color:red\">全反射</span>法(ATR)在橡胶产品分析中的应用","volume":"29","year":"2013"},{"abstractinfo":"通过测试2种不同高弹改性沥青的宏观性能发现,高弹1#改性沥青的延度和针入度随时间推移明显降低,软化点呈升高趋势,-10℃低温弯曲应变显著下降,而高弹2#改性沥青宏观力学性能并没有发生明显衰变;采用<span style=\"color:red\">红外</span><span style=\"color:red\">衰减</span><span style=\"color:red\">全反射</span>法(ATR)结合<span style=\"color:red\">红外光谱</span>定量分析法对2种不同高弹改性沥青的组分析出问题进行了研究,发现高弹1#在60℃的温度下随时间延长逐渐从改性沥青表面析出,且析出迁移量逐渐增加,而高弹2#基本不发生组分析出,其组分抗迁移能力优于高弹1#.证明高弹1#改性沥青宏观性能衰变的原因是由于高弹改性剂随时间延长逐渐析出至沥青表面所致.","authors":[{"authorName":"李璐","id":"3ad3d03f-be1b-41fe-945b-f371a84e97ba","originalAuthorName":"李璐"},{"authorName":"郝增恒","id":"237064d1-d864-4130-8da1-a2060a3a1812","originalAuthorName":"郝增恒"},{"authorName":"王民","id":"8d5225b6-939c-4832-8449-a0969168f5c7","originalAuthorName":"王民"},{"authorName":"李睿","id":"4e1adac2-4993-4d95-b0cf-27b2d6229324","originalAuthorName":"李睿"},{"authorName":"盛兴跃","id":"ed9cb0bc-a807-4d82-9117-d1d32f382780","originalAuthorName":"盛兴跃"}],"doi":"10.16865/j.cnki.1000-7555.2016.03.023","fpage":"124","id":"c49d5d2a-b519-45f7-bc1b-26af1120f4d8","issue":"3","journal":{"abbrevTitle":"GFZCLKXYGC","coverImgSrc":"journal/img/cover/GFZCLKXYGC.jpg","id":"31","issnPpub":"1000-7555","publisherId":"GFZCLKXYGC","title":"高分子材料科学与工程"},"keywords":[{"id":"09facde8-5bec-4bf8-9fb4-33e843031d50","keyword":"<span style=\"color:red\">红外</span><span style=\"color:red\">衰减</span>全发射法","originalKeyword":"红外衰减全发射法"},{"id":"03215af9-7f3b-452b-b99b-6ebfd356e848","keyword":"高弹改性沥青","originalKeyword":"高弹改性沥青"},{"id":"331db471-b770-4c04-abd2-fcbe01fad241","keyword":"组分析出","originalKeyword":"组分析出"},{"id":"d42fd19a-2c33-4680-82f7-598a854cc0ba","keyword":"定量分析","originalKeyword":"定量分析"}],"language":"zh","publisherId":"gfzclkxygc201603023","title":"基于<span style=\"color:red\">红外</span><span style=\"color:red\">衰减</span><span style=\"color:red\">全反射</span>法的高弹改性沥青组分析出表征","volume":"32","year":"2016"}],"totalpage":2122,"totalrecord":21214}