{"currentpage":1,"firstResult":0,"maxresult":10,"pagecode":5,"pageindex":{"endPagecode":5,"startPagecode":1},"records":[{"abstractinfo":"以无机盐-硝酸氧锆为原料,采用醇-水加热-超临界干燥法制备了二氧化锆气凝胶.采用XRD、TEM和BET等手段对样品进行测试表征.研究结果表明:本方法可以制备具有高比表面、小粒径的二氧化锆气凝胶.气凝胶原粉的比表面最大,可达675.6m2/g.其晶相结构也不同于采用一般方法制备的ZrO2粉体.在焙烧温度低于700℃时,随着焙烧温度的升高,四方相的含量逐渐增大,到700℃时达到最大86%;经1000℃焙烧后尽管粒径>30nm,仍有约30%的ZrO2以四方相的形式存在.探讨了醇水加热法制备ZrO2气凝胶的成胶机理.","authors":[{"authorName":"","id":"48e31610-e77b-42c7-a600-47755c6175a1","originalAuthorName":"武志刚"},{"authorName":"赵永祥","id":"caf45632-9217-47d4-999a-75724676ba4d","originalAuthorName":"赵永祥"},{"authorName":"刘滇生","id":"40c2a2e6-4815-4f7e-8be8-3e91c9fc2722","originalAuthorName":"刘滇生"}],"doi":"","fpage":"389","id":"0050c917-54d8-471e-b6e7-fa5632f4826c","issue":"3","journal":{"abbrevTitle":"GNCL","coverImgSrc":"journal/img/cover/GNCL.jpg","id":"33","issnPpub":"1001-9731","publisherId":"GNCL","title":"功能材料"},"keywords":[{"id":"d2072415-cc03-43fd-a655-5fb081c53714","keyword":"ZrO2气凝胶","originalKeyword":"ZrO2气凝胶"},{"id":"029f6e67-1232-45a5-884f-f33fe32b7cb9","keyword":"醇水加热法","originalKeyword":"醇水加热法"},{"id":"96dff60b-c4a6-4a16-a1e3-3f9ab18ec32a","keyword":"硝酸氧锆","originalKeyword":"硝酸氧锆"},{"id":"bbabae5b-5d24-4679-9cff-ecb9b1c026d8","keyword":"超临界干燥","originalKeyword":"超临界干燥"}],"language":"zh","publisherId":"gncl200403044","title":"二氧化锆气凝胶制备和表征","volume":"35","year":"2004"},{"abstractinfo":"化技术和化材料是空间充气展开结构的一项合材料;热塑性(和轻度交联热固性)复合材料;铝/聚合物层合板.本文介绍了这几种材料的典型化技术,分别介绍了化体系的特点、研究现状以及该化技术相应的优势与局限性.","authors":[{"authorName":"刘宇艳","id":"68122908-d3fe-495e-a7ba-25ed30bfe56f","originalAuthorName":"刘宇艳"},{"authorName":"孟秋影","id":"e14cb1a9-f66d-4c5b-9944-5cc619d393e1","originalAuthorName":"孟秋影"},{"authorName":"谭惠丰","id":"6d2e3152-f077-4b09-a5fe-8011a51e7de2","originalAuthorName":"谭惠丰"},{"authorName":"杜星文","id":"8f3fcc95-4bc0-4d47-8491-a33690eb3fa8","originalAuthorName":"杜星文"}],"doi":"10.3969/j.issn.1001-4381.2008.02.018","fpage":"76","id":"c3cb1cc1-d85c-456c-a1e9-03c8c2d836d6","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":"862d0276-4dd1-465b-9341-f64db13e4cd9","keyword":"空间充气展开结构","originalKeyword":"空间充气展开结构"},{"id":"83d2d0c5-b3e0-45c4-ba13-41c58740e0c8","keyword":"化材料","originalKeyword":"刚化材料"},{"id":"b98188ea-f7b0-4e3b-999b-221523bb92cd","keyword":"化技术","originalKeyword":"刚化技术"}],"language":"zh","publisherId":"clgc200802018","title":"空间充气展开结构用化材料和化技术的研究现状","volume":"","year":"2008"},{"abstractinfo":"采用GPS卫星同步断电法对忠管道进行了断电电位测量,对结果进行了分析,评价了忠管道阴极保护系统的有效性,并提出了改进建议.结果表明,三层PE管道相比于环氧粉末涂层管道更容易出现过保护现象,而且还容易受到干扰;电位是反应管道所处状态的主要指标,阴极保护系统的通电电位呈规律分布,但断电电位影响因素复杂,无明显规律.","authors":[{"authorName":"罗鹏","id":"18512348-d250-458d-bf3e-c0e9710d5a5c","originalAuthorName":"罗鹏"},{"authorName":"金鑫","id":"b3f412f6-6973-42ba-9881-3e553616f798","originalAuthorName":"金鑫"},{"authorName":"徐承伟","id":"784ec7f1-f012-452a-ba06-7609c0b10b0f","originalAuthorName":"徐承伟"},{"authorName":"薛致远","id":"48838684-38dc-4b1e-96e1-c13bc71f5694","originalAuthorName":"薛致远"},{"authorName":"高强","id":"aa4f9f94-5b47-40f2-a60b-5c90d1f80e89","originalAuthorName":"高强"},{"authorName":"张永盛","id":"dcf5fb27-5c7a-4933-98b7-981aca29f748","originalAuthorName":"张永盛"}],"doi":"","fpage":"224","id":"670a796f-6251-4fb3-8541-c3fb55741e13","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":"3ed78c05-3e52-49dd-a17f-0e442c522d84","keyword":"阴极保护","originalKeyword":"阴极保护"},{"id":"75cb2ded-b721-47f2-93b6-852438d3e430","keyword":"通电电位","originalKeyword":"通电电位"},{"id":"bbbc7c8f-15ec-440e-8d5b-7e5162d1c5e7","keyword":"断电电位","originalKeyword":"断电电位"}],"language":"zh","publisherId":"fsyfh201103016","title":"忠管道阴极保护断电电位测量结果分析","volume":"32","year":"2011"},{"abstractinfo":"模拟土壤施用稀土定位试验结果表明:黄土中各组份吸附稀土的能力为:无定形FexOy、紧结有机物>松结有机物>MnOx>晶形FexOy>永久负电荷;进入黄土的外源轻稀土,主要累积于紧结有机态(29.90~49.72%)、无定形氧化铁吸附态(26.81~46.76%),而累积于松结有机态的轻稀土受外源稀土的加入量影响较小(24.93~28.72%).当外源稀土用量在0.684~2.735mg/kg*季时,大豆地上部稀土无明显增加,而用量达13.674mg/kg时,地上部明显增加.黄土外源稀土的最佳用量为0.684mg/kg,此时,大豆增产43.82±15.08%、油菜增产17.92±9.07%.","authors":[{"authorName":"荆国芳","id":"fc1b92c6-600d-4fcd-8e1e-fa3dc5a1c9f5","originalAuthorName":"荆国芳"},{"authorName":"钱晓晴","id":"f0c35fa0-cdb7-47b9-b5f0-473802d2c771","originalAuthorName":"钱晓晴"}],"doi":"10.3969/j.issn.1004-0277.2002.02.011","fpage":"38","id":"8b89503d-85fe-42d8-a31b-5ee41eed9fc4","issue":"2","journal":{"abbrevTitle":"XT","coverImgSrc":"journal/img/cover/XT.jpg","id":"65","issnPpub":"1004-0277","publisherId":"XT","title":"稀土"},"keywords":[{"id":"d9808f7e-67c4-4266-9caf-60295c858dc6","keyword":"稀土","originalKeyword":"稀土"},{"id":"60f39a5b-d062-4283-92b6-49c319b6ff2e","keyword":"形态","originalKeyword":"形态"},{"id":"97b50517-dd4d-4380-b408-02394f1ee3bd","keyword":"生态效应","originalKeyword":"生态效应"}],"language":"zh","publisherId":"xitu200202011","title":"外源稀土在黄土中形态分布和生态效应研究","volume":"23","year":"2002"},{"abstractinfo":"验证已建立的刚性颗粒增强复合材料塑性细观损伤本构理论的合理性和可靠性.将上述本构理论的数值计算结果与SiC颗粒增强的铝基复合材料单轴拉伸实验结果进行比较.结果表明:由此本构模型得到的应力-应变理论曲线与拉伸实验所得的应力-应变曲线基本吻合,从而验证了该本构模型的合理性和可靠性.因此已建立的塑性细观损伤本构模型可用于数值计算,在一定程度上可预测颗粒增强复合材料的力学特性.在此基础上对大、小颗粒增强复合材料的延展性、空洞和颗粒体积分数演化规律等作了讨论.","authors":[{"authorName":"吴国民","id":"caab2819-e99c-4fc5-8f4d-6b19923fd48c","originalAuthorName":"吴国民"},{"authorName":"殷雅俊","id":"bdb5646b-fee1-4f09-b2e0-e0ccf6bf8553","originalAuthorName":"殷雅俊"}],"doi":"10.3321/j.issn:1000-3851.2005.05.003","fpage":"16","id":"afc0715b-f9a4-467d-bd25-4cd5ec674d62","issue":"5","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":"02ca7d0b-8fd2-40c6-a27a-0cb7be1aad5c","keyword":"颗粒增强复合材料","originalKeyword":"颗粒增强复合材料"},{"id":"43506929-0c02-4552-9936-b1c475477d5c","keyword":"细观损伤","originalKeyword":"细观损伤"},{"id":"c2c80041-0bcc-4b7f-87b6-4eba8ed58d2b","keyword":"塑性本构理论","originalKeyword":"刚塑性本构理论"},{"id":"88c1e48f-e34f-4115-b1bf-e919993ce3a3","keyword":"空洞演化","originalKeyword":"空洞演化"}],"language":"zh","publisherId":"fhclxb200505003","title":"颗粒增强复合材料塑性细观损伤本构模型的验证","volume":"22","year":"2005"},{"abstractinfo":"为了满足板材轧制过程在线控制快速计算的要求,首先建立了板材轧制平面应变塑性有限元能量泛函。其次,通过合理的简化建立了只考虑变形区的快速有限元模型,且对有限元建模的关键问题包括中性点、第一类速度奇异点和刚性区等进行了处理。最后,开发了板材轧制快速计算有限元程序,并且利用现场轧制数据测试了快速有限元程序的计算速度和精度,结果表明计算速度和精度满足在线快速计算的要求。","authors":[{"authorName":"张光亮","id":"bc6303e6-8b84-4d65-8672-d5ee15e5fb54","originalAuthorName":"张光亮"},{"authorName":"张士宏","id":"9da410b9-3b45-44e7-9853-9d700d62f223","originalAuthorName":"张士宏"},{"authorName":"刘劲松","id":"75dbd315-11f2-40ec-9f85-ced0db31886f","originalAuthorName":"刘劲松"},{"authorName":"张海渠","id":"6b30ea75-cd6e-4548-8981-625e7aad4746","originalAuthorName":"张海渠"},{"authorName":"李长生","id":"88830a0a-2707-4b41-99bc-930fc5fbe7bf","originalAuthorName":"李长生"}],"categoryName":"|","doi":"","fpage":"32","id":"34c2cb2a-08a5-4e65-9853-436b68135436","issue":"6","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":"7f8b6134-1932-4a93-8f0b-74c9734cb805","keyword":"板材轧制;塑性有限元法;在线控制","originalKeyword":"板材轧制;刚塑性有限元法;在线控制"}],"language":"zh","publisherId":"1001-0963_2009_6_8","title":"板材轧制过程轧制力塑性有限元快速计算","volume":"21","year":"2009"},{"abstractinfo":"为了满足板材轧制过程在线控制快速计算的要求,首先建立了板材轧制平面应变塑性有限元能量泛函.其次,通过合理的简化建立了只考虑变形区的快速有限元模型,且对有限元建模的关键问题包括中性点、第一类速度奇异点和刚性区等进行了处理.最后,开发了板材轧制快速计算有限元程序,并且利用现场轧制数据测试了快速有限元程序的计算速度和精度,结果表明计算速度和精度满足在线快速计算的要求.","authors":[{"authorName":"张光亮","id":"cd9a1639-4231-45d5-9f95-2a666115e081","originalAuthorName":"张光亮"},{"authorName":"张士宏","id":"9efa32db-fb88-4038-b77c-adabc4eb4c3f","originalAuthorName":"张士宏"},{"authorName":"刘劲松","id":"a5c70bfa-9001-4ffa-b661-c670e6eabe91","originalAuthorName":"刘劲松"},{"authorName":"张海渠","id":"41bc2ae8-9170-4943-87d9-f68950a1b2df","originalAuthorName":"张海渠"},{"authorName":"李长生","id":"74d58b04-ae35-4787-bea2-7d703aa9e898","originalAuthorName":"李长生"}],"doi":"","fpage":"32","id":"3c7cc817-66c1-42ef-9aab-d0f786b69f05","issue":"6","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":"621d02dc-4d98-4336-bb35-7ae6dfaf8302","keyword":"板材轧制","originalKeyword":"板材轧制"},{"id":"3727e566-75ee-468f-a887-3592861220ee","keyword":"塑性有限元法","originalKeyword":"刚塑性有限元法"},{"id":"ac49a1a8-1dee-4159-a68f-ad423e622e4a","keyword":"在线控制","originalKeyword":"在线控制"}],"language":"zh","publisherId":"gtyjxb200906008","title":"板材轧制过程轧制力塑性有限元快速计算","volume":"21","year":"2009"},{"abstractinfo":"分析与探讨了高温玻璃的应力流动模型及其材料参数的温度相关性。利用粘塑性力学模型,基于三维有限元软件DEFORM 3D建立非球面透镜高温模压有限元模型,对光学玻璃L-BAL42球形预制件模压成非球面透镜的整个过程进行了数值仿真,发现非球面透镜应力分布规律:透镜边缘处应力最大,在和模阶段应力快速增加,导致透镜边缘处最易破碎,结果得到实验的验证。采用较大的模压速度及冷却速度将导致残余应力增加,同时分析了透镜非球面偏差变化规律。最后在模具设计时将非球面偏差补偿进去,发现非球面透镜偏差减少,由正偏差变为负偏差。","authors":[{"authorName":"张小兵","id":"acdaaafb-1d57-4199-a58b-b10026bfd6f6","originalAuthorName":"张小兵"}],"doi":"","fpage":"68","id":"0cf3ab32-a23c-4a51-b293-acb9d2170919","issue":"2","journal":{"abbrevTitle":"BQCLKXYGC","coverImgSrc":"journal/img/cover/BQCLKXYGC.jpg","id":"4","issnPpub":"1004-244X","publisherId":"BQCLKXYGC","title":"兵器材料科学与工程 "},"keywords":[{"id":"e0a0f244-1bb9-4be6-8312-69fe596770d2","keyword":"非球面","originalKeyword":"非球面"},{"id":"5c391287-977d-4916-890f-73513924296a","keyword":"粘塑性模型","originalKeyword":"粘刚塑性模型"},{"id":"f0a4a2b2-474b-45bb-87ee-1af2286e366c","keyword":"三维模压成型模型","originalKeyword":"三维模压成型模型"}],"language":"zh","publisherId":"bqclkxygc201502018","title":"基于粘塑性模型非球面透镜三维模压成型模拟","volume":"","year":"2015"},{"abstractinfo":"采用塑性有限元解析计算了无孔型轧制轧件自由表面的变形,探讨了件辊接触面摩擦因子的取值对计算结果的影响,并与实测值进行了对比,得到了相关结论.","authors":[{"authorName":"韦东滨","id":"c2e07a95-9c8f-4e40-b40d-b0cfa25c7b8f","originalAuthorName":"韦东滨"},{"authorName":"徐建中","id":"9b09b986-2fa7-4214-a024-5c9ade315baa","originalAuthorName":"徐建中"},{"authorName":"吴迪","id":"feff9146-1019-4e54-be4f-4c59ee50329b","originalAuthorName":"吴迪"},{"authorName":"白光润","id":"7600bd0f-2e4c-417a-b6b0-a0137cb5e514","originalAuthorName":"白光润"}],"doi":"10.3969/j.issn.1001-1447.1999.04.010","fpage":"40","id":"3c4efa8d-212b-4942-8b76-4a01ad9b04c5","issue":"4","journal":{"abbrevTitle":"GTYJ","coverImgSrc":"journal/img/cover/GTYJ.jpg","id":"29","issnPpub":"1001-1447","publisherId":"GTYJ","title":"钢铁研究"},"keywords":[{"id":"ac956b8f-d70d-4d7d-be2b-b8b595dae865","keyword":"无孔型轧制","originalKeyword":"无孔型轧制"},{"id":"7d6ef12a-2e46-487d-ba3a-04a2c722c97b","keyword":"自由表面形状","originalKeyword":"自由表面形状"},{"id":"58874faa-a5c6-4c8f-bf22-296c13a4f557","keyword":"塑性有限元","originalKeyword":"刚塑性有限元"}],"language":"zh","publisherId":"gtyj199904010","title":"无孔型轧制轧件自由表面形状的塑性有限元分析","volume":"","year":"1999"},{"abstractinfo":"采用塑性有限元法(FEM)建立宝钢2050粗轧区孔型立辊调宽过程轧制模型.计算所得多块带钢轧制力值与现场实测结果吻合良好,模拟的带钢头尾形状与现场实际结果吻合也很好,并建立立轧稳态狗骨形状计算的数学模型.同时研究得出立辊孔型角度对狗骨高及轧制力的影响规律.","authors":[{"authorName":"李学通","id":"167c5874-3d5c-4818-aa56-a00f45a98864","originalAuthorName":"李学通"},{"authorName":"杜凤山","id":"0cc702ac-0a36-4e25-aa74-7e3c14b344db","originalAuthorName":"杜凤山"},{"authorName":"吴建峰","id":"763c8aad-a609-401c-8634-12689a6aa663","originalAuthorName":"吴建峰"}],"doi":"10.3969/j.issn.1001-7208.2005.01.008","fpage":"31","id":"76854ebe-a841-475f-bb2c-24a437411cb6","issue":"1","journal":{"abbrevTitle":"SHJS","coverImgSrc":"journal/img/cover/SHJS.jpg","id":"59","issnPpub":"1001-7208","publisherId":"SHJS","title":"上海金属"},"keywords":[{"id":"74d0329e-9e0a-4039-b35f-22f3dbb8c473","keyword":"热轧带钢","originalKeyword":"热轧带钢"},{"id":"104658b6-0416-4c36-86cc-7cc8c02780cb","keyword":"孔型立辊","originalKeyword":"孔型立辊"},{"id":"e61ce7b6-6409-42a6-afa6-5e82108aa0bc","keyword":"调宽轧制","originalKeyword":"调宽轧制"},{"id":"48629ef2-c4d2-4dd7-a371-645257bc698a","keyword":"塑性有限元法","originalKeyword":"刚塑性有限元法"}],"language":"zh","publisherId":"shjs200501008","title":"孔型立辊调宽轧制的三维塑性有限元研究","volume":"27","year":"2005"}],"totalpage":26,"totalrecord":259}