{"currentpage":1,"firstResult":0,"maxresult":10,"pagecode":5,"pageindex":{"endPagecode":5,"startPagecode":1},"records":[{"abstractinfo":"用界面改性的方法研究了反渗透复合膜多孔支撑层/超薄功能层界面性质对反渗透复合膜性能的影响.用接触角表征极性即亲水性的变化,进行了ATR-IR的分析和测试.实验结果表明,多孔支撑层/超薄功能层界面的极性即亲水性与复合膜的产水率和脱盐率有明显的相关性,改性后的界面间形成了不同强度的氢键并对超薄功能层的N-H伸缩振动有影响.","authors":[{"authorName":"曹艳霞","id":"0ccc3189-f15f-44f5-be43-3c666e8325b1","originalAuthorName":"曹艳霞"},{"authorName":"郑国栋","id":"b72e1974-c9fb-46b0-8dd7-c92b0f794983","originalAuthorName":"郑国栋"},{"authorName":"徐纪平","id":"3daada89-a687-4537-9408-e90bc5d3e7d5","originalAuthorName":"徐纪平"},{"authorName":"沈家瑞","id":"6798045a-e782-4ecb-86a9-c1534d14c552","originalAuthorName":"沈家瑞"}],"doi":"","fpage":"142","id":"087aff9e-df1d-4bc2-9c58-4a9a75ae22c0","issue":"6","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":"f3f0f29c-25ab-40bd-8f4d-4d854975a6e6","keyword":"界面改性","originalKeyword":"内界面改性"},{"id":"4dfb17c6-3068-40cf-b741-fe5a5cd06369","keyword":"极性","originalKeyword":"极性"},{"id":"64a03819-8236-48e1-9c75-531ef9868b6f","keyword":"相关性","originalKeyword":"相关性"}],"language":"zh","publisherId":"gfzclkxygc200406036","title":"反渗透复合膜界面改性对其性能的影响研究--(Ⅱ)理论分析","volume":"20","year":"2004"},{"abstractinfo":"用界面改性的方法研究了多孔支撑层/超薄功能层界面性质对反渗透复合膜性能的影响.采用了甲酸、磷酸、盐酸和弱极性试剂异丙醇作为聚砜底膜表面改性试剂.实验结果表明,在实验采用的不同的改性条件下,复合膜的性能都出现了大幅度的提高,改变改性试剂时,复合膜的性能变化有着相似的规律.改变改性试剂的浓度和改性时间有同样的改性效果.","authors":[{"authorName":"曹艳霞","id":"52fbb999-fd35-4e0f-bf4e-98154c9ecb2e","originalAuthorName":"曹艳霞"},{"authorName":"郑国栋","id":"71984558-c97b-4332-8857-f90fd3830714","originalAuthorName":"郑国栋"},{"authorName":"徐纪平","id":"16a3110f-97ae-49e0-a049-17e4946ebd3a","originalAuthorName":"徐纪平"},{"authorName":"沈家瑞","id":"9f084331-5f54-4573-8a1e-950ab64f7956","originalAuthorName":"沈家瑞"}],"doi":"","fpage":"138","id":"8bade4f0-3eb3-4dca-8233-1e5edf5b6089","issue":"6","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":"f17aa2ad-381b-426d-8ced-1b24e8228e71","keyword":"界面","originalKeyword":"内界面"},{"id":"65464f30-3317-427c-b5fc-1f57b56d4427","keyword":"反渗透复合膜","originalKeyword":"反渗透复合膜"},{"id":"e278975c-2d55-4f15-ad69-a4446c326f73","keyword":"表面改性","originalKeyword":"表面改性"}],"language":"zh","publisherId":"gfzclkxygc200406035","title":"反渗透复合膜界面改性对其性能的影响研究--(Ⅰ)性能表征","volume":"20","year":"2004"},{"abstractinfo":"采和TEM、SEM及X-ray研究了生复合钢板的显微结构并对其弱界面进行了表征.结果 发现:生复合钢板的显微结构是由低碳马氏体板条沿轧面和轧向近于平行排列构成的,其复合结构为(100)织构取向带嵌于(111)织构基体中形成的层状结构,弱界面为(100)/(100)板条晶问界面.","authors":[{"authorName":"蔡大勇","id":"a6172228-7fd7-4ca4-b509-7bdd5f097679","originalAuthorName":"蔡大勇"},{"authorName":"张春玲","id":"7074c458-2e9d-4d1a-87dd-bd4944c23886","originalAuthorName":"张春玲"},{"authorName":"荆天辅","id":"9793054a-0fc0-4054-be53-4e1801264dc8","originalAuthorName":"荆天辅"}],"doi":"10.3969/j.issn.1001-0777.2000.05.008","fpage":"23","id":"d9237ee9-c200-4c37-b597-e4e2fdb583e1","issue":"5","journal":{"abbrevTitle":"WLCS","coverImgSrc":"journal/img/cover/WLCS.jpg","id":"64","issnPpub":"1001-0777","publisherId":"WLCS","title":"物理测试"},"keywords":[{"id":"b2a1a256-1edf-4456-bb2f-9980cbeead66","keyword":"生复合钢板","originalKeyword":"内生复合钢板"},{"id":"af7bda98-b770-4738-b6b6-b6342611d919","keyword":"弱界面","originalKeyword":"弱界面"},{"id":"eeca3e87-6a56-4a20-951d-1b67724d9e34","keyword":"织构","originalKeyword":"织构"}],"language":"zh","publisherId":"wlcs200005008","title":"生复合钢板中弱界面的测定","volume":"","year":"2000"},{"abstractinfo":"为了揭示团状流中夹带液滴的产生机理,本文建立了气液团状流界面波运动模型。该模型可以预测界面波沿壁面的运动规律及界面波特性(波幅、波速)的变化特点,理论解释团状流扰动性大的特点。结果表明:当气速较小或液速较大时,界面波在运动过程中存在反转现象,当进入环状流时,反转现象消失。界面波波速与最大波幅均随气、液速度的增大而增大,而临界波幅主要受气速的影响。通过与实验结果对比,证明该模型可以较好地反映界面波在团状流条件下的运动特点。","authors":[{"authorName":"王科","id":"0ed60553-78c0-4cdc-bfae-a65180f92473","originalAuthorName":"王科"},{"authorName":"马江","id":"42b6c6c9-96aa-4cfb-b64c-58b05529a2db","originalAuthorName":"马江"},{"authorName":"白博峰","id":"ee620047-d954-4527-afa9-00708f7a9a36","originalAuthorName":"白博峰"}],"doi":"","fpage":"2116","id":"d8f832f7-62b7-4564-95b3-faf56891a91a","issue":"12","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":"401ed6ad-c4b1-481d-a495-25fc6c0a7cda","keyword":"团状流","originalKeyword":"团状流"},{"id":"84f99bd7-9631-4cc3-9a47-6d613829cb80","keyword":"界面波","originalKeyword":"界面波"},{"id":"875d9c30-eb85-4eb4-8bb6-d76e850c5b54","keyword":"动力学模型","originalKeyword":"动力学模型"},{"id":"139ff688-7f10-49d2-bf91-f639b60f1bdd","keyword":"液泛","originalKeyword":"液泛"}],"language":"zh","publisherId":"gcrwlxb201212025","title":"气液团状流界面波运动模型研究","volume":"33","year":"2012"},{"abstractinfo":"根据聚合物改性砂浆不同的界面破坏形式,提出了表征界面粘接特性的聚强度和界面结合强度概念,并通过二者的总体宏现效应-粘接强度试验探讨了乙烯-醋酸乙酸共聚物、双级配填料和水泥对砂浆聚强度和界面结合强度的影响.试验表明,在本试验务件下乙烯-醋酸乙酸共聚物的最佳掺量范围为1.5%~3.5%.当聚合物掺量低于3.5%时,随着聚合物掺量的增加,聚合物改性砂浆的粘接强度增大,破坏形式为聚破坏;当聚合物掺量高于3.5%时,聚合物改性砂浆界面的结合强度降低,导致粘接强度降低,破坏形式为界面破坏.具有合适配比的双级配填料可增强砂浆粘接强度,但大粒径填料的增加会降低砂浆与基材界面的结合强度,导致砂浆的粘接强度降低,在本试验条件下填料A/填料B的比例取1:2为宜.聚合物改性砂浆的粘接强度随水泥掺量的增加而增大,并在掺量为30%时出现拐点,故在本试验条件下水泥掺量取30%较佳.","authors":[{"authorName":"马保国","id":"9cb63faf-82db-4f59-8a1e-c2c659e7517f","originalAuthorName":"马保国"},{"authorName":"吴媛媛","id":"3f05238c-bb7a-4e29-bdb7-c091fd5cf46e","originalAuthorName":"吴媛媛"},{"authorName":"张风臣","id":"e115d0e4-cf7d-4511-bf52-1cc2ebcb0779","originalAuthorName":"张风臣"},{"authorName":"尹耿","id":"4497dc73-712d-4571-a0c1-d702cb1b5e8c","originalAuthorName":"尹耿"},{"authorName":"戴璐","id":"350759a4-bd65-4c8a-8af6-3e4829e805fc","originalAuthorName":"戴璐"}],"doi":"","fpage":"62","id":"ec91c8fd-6121-4f49-9101-a23cb50f02ef","issue":"12","journal":{"abbrevTitle":"CLDB","coverImgSrc":"journal/img/cover/CLDB.jpg","id":"8","issnPpub":"1005-023X","publisherId":"CLDB","title":"材料导报"},"keywords":[{"id":"d575b99b-648f-4163-89e1-04cf86b6582c","keyword":"聚合物改性砂浆","originalKeyword":"聚合物改性砂浆"},{"id":"9b392609-3542-4aea-a87e-799a06c90f6f","keyword":"界面粘接特性","originalKeyword":"界面粘接特性"},{"id":"ef3f215c-0ee2-49c1-93f3-309e4a44bf71","keyword":"粘接强度","originalKeyword":"粘接强度"},{"id":"baca2d3c-edb4-4fba-94f6-f869aeaa9104","keyword":"聚强度","originalKeyword":"内聚强度"},{"id":"dc2dfe1a-ed7f-42e1-a2f4-45fa27ef4647","keyword":"界面结合强度","originalKeyword":"界面结合强度"}],"language":"zh","publisherId":"cldb200912019","title":"聚合物改性砂浆界面粘接特性的研究","volume":"23","year":"2009"},{"abstractinfo":"通过在全比例水模型上进行模拟,研究了结晶器宽度、拉坯速度、浸入式水口结构及水口浸入深度等工艺参数对板坯结晶器钢/渣界面波动和界面最大流速的影响.结果表明:单独增大结晶器宽度或拉坯速度,结晶器钢/渣界面波动和界面最大流速都将增大;而浸入式水口结构和水口浸入深度对钢/渣界面波动和界面最大流速的影响较复杂,其中,15°凸型水口通用性较好.","authors":[{"authorName":"舒志浩","id":"488c5b16-2164-4bde-a151-81d1b691bf27","originalAuthorName":"舒志浩"},{"authorName":"侯泽旺","id":"f1802522-d0a4-4628-a54d-9cfac9e80be4","originalAuthorName":"侯泽旺"}],"doi":"","fpage":"40","id":"44ba5570-1811-4241-a249-f5cd972703e8","issue":"3","journal":{"abbrevTitle":"GTFT","coverImgSrc":"journal/img/cover/gtft1.jpg","id":"28","issnPpub":"1004-7638","publisherId":"GTFT","title":"钢铁钒钛"},"keywords":[{"id":"e1fcae78-504b-4b16-8517-f23e268049d8","keyword":"板坯连铸","originalKeyword":"板坯连铸"},{"id":"97eebbe8-4bef-47c5-982b-fb71fce25fbd","keyword":"结晶器","originalKeyword":"结晶器"},{"id":"3de0b14c-2611-4d90-b0f7-17cfe2c60dfc","keyword":"钢/渣界面","originalKeyword":"钢/渣界面"},{"id":"ed2dfaf4-44f0-460b-8dad-2fdc05d28a00","keyword":"界面波动","originalKeyword":"界面波动"},{"id":"49b4f2f3-05fe-4b09-b4b5-882e42cdc91a","keyword":"界面最大流速","originalKeyword":"界面最大流速"}],"language":"zh","publisherId":"gtft201203009","title":"板坯结晶器钢/渣界面流态的水模拟","volume":"33","year":"2012"},{"abstractinfo":"研究了反应注塑(RTM)成型的复合材料不同层次界面的特点,并分别采用冷等离子处理和超声处理对RTM成型的复合材料界面性能进行改性.结果表明,RTM成型复合材料不同层次界面性能是不同的,通过冷等离子体和超声处理可以提高树脂对纤维增强体的浸润性,进而可以改善复合材料的界面性能,而界面的好坏直接影响RTM成型复合材料的力学性能.","authors":[{"authorName":"秦伟","id":"921267ff-8255-4a5f-a12e-312326f9bb7f","originalAuthorName":"秦伟"},{"authorName":"张志谦","id":"e41518bf-cf53-4585-96a3-3af6bef27331","originalAuthorName":"张志谦"},{"authorName":"吴晓宏","id":"6e688a71-6362-4158-8799-753aaeb8b9e8","originalAuthorName":"吴晓宏"},{"authorName":"王福平","id":"934c7b70-825b-426d-ad34-e23bd20664e4","originalAuthorName":"王福平"}],"doi":"","fpage":"206","id":"23a86331-0529-4531-aa11-07eda7095663","issue":"6","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":"1fecad1b-d4a0-4df7-bd66-e42d1b507827","keyword":"RTM工艺","originalKeyword":"RTM工艺"},{"id":"9380a1a6-7caf-4d8b-adcd-79a67d85fdbb","keyword":"冷等离子体处理技术","originalKeyword":"冷等离子体处理技术"},{"id":"690074e0-6793-4145-a7d2-ba486fba145c","keyword":"超声处理","originalKeyword":"超声处理"},{"id":"dfe12ea7-d301-4481-9dd2-146768e823f6","keyword":"界面性能","originalKeyword":"界面性能"}],"language":"zh","publisherId":"gfzclkxygc200306053","title":"RTM成型复合材料的界面改性","volume":"19","year":"2003"},{"abstractinfo":"对具有吸收-透射性边界面的梯度折射率半透明介质层,建立了介质内热辐射传递与边界面辐射换热的数理模型,并采用数值弯曲光线跟踪法求解介质的热辐射传递.通过数值模拟,分析了正弦折射率下,边界面的反射特性、吸收率以及介质层光学厚度对介质内热辐射平衡温度场及热流分布的影响.结果表明,边界面的反射特性与吸收率对介质辐射换热均有重要影响,吸收率的影响与边界面反射特性、介质层光学厚度及环境条件相关,呈现特征不同的作用.","authors":[{"authorName":"夏新林","id":"b3884b79-d553-4540-8acc-df04c8f2796d","originalAuthorName":"夏新林"},{"authorName":"任德鹏","id":"f0b6678f-8095-4f8f-b683-4c9aef805929","originalAuthorName":"任德鹏"},{"authorName":"谈和平","id":"debbc85f-1a6d-4d8c-8e88-789bbb50dbe5","originalAuthorName":"谈和平"}],"doi":"","fpage":"653","id":"2f28c842-10e5-418c-8727-0de6e33dd9c8","issue":"4","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":"48bb9157-1dc2-49e8-91c1-89200ede2c84","keyword":"梯度折射率介质","originalKeyword":"梯度折射率介质"},{"id":"134c5749-9bf2-4e7f-a52f-80fbd794048e","keyword":"吸收-透射界面","originalKeyword":"吸收-透射界面"},{"id":"ac12c0ee-a192-4486-abd5-cd2ff1d385af","keyword":"热辐射平衡","originalKeyword":"热辐射平衡"},{"id":"00347c68-ba36-4803-8e1f-9e2e8097fd47","keyword":"数值弯曲光线跟踪法","originalKeyword":"数值弯曲光线跟踪法"}],"language":"zh","publisherId":"gcrwlxb200504034","title":"吸收-透射界面下正弦折射率介质辐射换热","volume":"26","year":"2005"},{"abstractinfo":"提出了一种利用拉伸法和剪切法测定生复合板钢板弱界面拉伸强度及剪切强度的测试方法.该方法具有测试简单、数据准确的特点.","authors":[{"authorName":"蔡大勇","id":"280ccfcb-a536-4d3e-93d5-89d392b0d43c","originalAuthorName":"蔡大勇"},{"authorName":"张春玲","id":"27c703ef-0b47-4d4d-a49e-58d0e19bcae9","originalAuthorName":"张春玲"},{"authorName":"荆天辅","id":"f96e65c5-8dbc-4d05-8694-08f7e4163f98","originalAuthorName":"荆天辅"}],"doi":"10.3969/j.issn.1001-0777.2000.02.011","fpage":"41","id":"df1a60ed-1189-4766-9569-cf8a8b6acc9f","issue":"2","journal":{"abbrevTitle":"WLCS","coverImgSrc":"journal/img/cover/WLCS.jpg","id":"64","issnPpub":"1001-0777","publisherId":"WLCS","title":"物理测试"},"keywords":[{"id":"ad47c23c-0cde-4dc7-a6b0-879725eff0e0","keyword":"生复合板","originalKeyword":"内生复合板"},{"id":"cefc7e46-05ac-4ee0-93f8-e4687c51307c","keyword":"弱界面","originalKeyword":"弱界面"},{"id":"842a587f-0d92-4fe8-ae72-725d2cfd121d","keyword":"界面结合强度","originalKeyword":"界面结合强度"}],"language":"zh","publisherId":"wlcs200002011","title":"一种生复合板弱界面结合强度的测试方法","volume":"","year":"2000"},{"abstractinfo":"利用VOF方法和Lagrange两相流模型描述了吹氩结晶器钢/渣界面\n行为, 并用水模型实验检验了数值模拟结果.\n在此基础上考察了吹氩量、拉速、结晶器宽度、水口浸入深度及气泡尺寸对钢\n/渣界面卷混的影响规律. 结果表明:拉速为1.8 m/min时,\n增大吹氩量, 结晶器的上回流区逐渐消失,\n气泡对界面的扰动则不断加剧;吹氩量一定时,\n拉速由1.2 m/min增至2.2 m/min的过程中, 气泡的冲\n击深度增加, 氩气泡对钢液流型和界面形状的影响减弱;\n增加水口浸入深度对抑制吹氩下界面波动作\n用明显, 而结晶器宽度对此影响较小;\n气泡尺寸显著影响钢/渣界面行为.","authors":[{"authorName":"曹娜","id":"d3c15a9f-db00-43d5-a4c0-81451b0ad27b","originalAuthorName":"曹娜"},{"authorName":"朱苗勇","id":"4b23e277-1024-45ac-a115-591aeb970acb","originalAuthorName":"朱苗勇"}],"categoryName":"|","doi":"","fpage":"79","id":"ebfb65d4-92a9-4549-873b-cb29c37288c3","issue":"1","journal":{"abbrevTitle":"JSXB","coverImgSrc":"journal/img/cover/JSXB.jpg","id":"48","issnPpub":"0412-1961","publisherId":"JSXB","title":"金属学报"},"keywords":[{"id":"a0604d92-1b41-4652-904c-c22b81145ced","keyword":"连铸","originalKeyword":"连铸"},{"id":"7bf5ce8c-06d4-45ce-ae06-37c7b4fbb724","keyword":"mold","originalKeyword":"mold"},{"id":"d39c8610-1a22-4217-8046-610a4f23d2fe","keyword":"blowing argon gas","originalKeyword":"blowing argon gas"}],"language":"zh","publisherId":"0412-1961_2008_1_13","title":"吹氩板坯连铸结晶器钢/渣界面行为的数值模拟","volume":"44","year":"2008"}],"totalpage":3747,"totalrecord":37469}