人工晶体学报, 2011, 40(4): 932-937.
非水解和水解溶胶-凝胶法制备TiO2薄膜的对比研究
包镇红 1, , 江伟辉 2, , 苗立锋 {"currentpage":1,"firstResult":0,"maxresult":10,"pagecode":5,"pageindex":{"endPagecode":5,"startPagecode":1},"records":[{"abstractinfo":"本文通过实验研究了冷凝式燃气热水器中烟气伴随有水蒸气凝结的受迫对流换热过程。着重介绍实验系统、测试方法和对塔板式换热器和肋片板式换热器的实验研究结果。实验表明，有水蒸气凝结时的烟气对流换热系数远大于无凝结时的换热系数，可提高数倍。在冷凝式换热器中,塔板式换热器的换热系数大于肋片板式换热器","authors":[{"authorName":"曹彦斌","id":"dbf669fc-5cbb-4363-a1e7-eac57ec7fb2d","originalAuthorName":"曹彦斌"},{"authorName":"艾效逸","id":"d326c93a-e479-4aa0-925b-30320074835a","originalAuthorName":"艾效逸"},{"authorName":"郭全","id":"908df1d3-a7f0-496c-83e2-8f3df6895069","originalAuthorName":"郭全"},{"authorName":"潘树源","id":"c241ac7f-1032-40db-89da-5ba3611748a5","originalAuthorName":"潘树源"},{"authorName":"","id":"b5dbe302-e049-4a8a-a270-4ae442c752fd","originalAuthorName":""},{"authorName":"傅忠诚","id":"3f95b7b6-37dc-4a51-801e-70d2ec9dd320","originalAuthorName":"傅忠诚"},{"authorName":"王随林","id":"1c153038-ecec-4259-a830-15b23fc704aa","originalAuthorName":"王随林"}],"doi":"","fpage":"729","id":"05aecca2-3ce6-400d-aea8-72b822cb054f","issue":"6","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":"d89ffb3c-8dae-4db0-8b02-a5aba0a4d803","keyword":"烟气对流换热","originalKeyword":"烟气对流换热"},{"id":"3ee4cd18-e575-4017-af6d-7a04bdaf5af7","keyword":"凝结","originalKeyword":"凝结"},{"id":"edfb03fc-5b6d-4f5d-8c31-6144329ab459","keyword":"肋片换热器","originalKeyword":"肋片换热器"}],"language":"zh","publisherId":"gcrwlxb200006020","title":"伴随有水蒸气凝结的烟气对流换热的实验研究","volume":"21","year":"2000"},{"abstractinfo":"提出了自傅里叶孤子概念.对自傅里叶孤子信号及自傅里叶高斯信号在光纤中的演变和传输进行了数值模拟和时频分析.结果表明,输入自傅里叶高斯信号,将演变成一类非自傅里叶孤子;三阶色散效应会影响由自傅里叶高斯信号所演变的孤子的震荡传输幅度,且引起孤子时域延迟、频谱不对称.","authors":[{"authorName":"殷德京","id":"ba1b2ca6-95d9-49c1-ba20-2318cc6e727a","originalAuthorName":"殷德京"}],"doi":"10.3969/j.issn.1007-5461.2009.04.021","fpage":"499","id":"dc0fd06c-9b69-42e8-ba36-242b96a2fe20","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 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"},"keywords":[{"id":"ef67afc8-f614-4302-921f-b804dc40ad96","keyword":"大气光学","originalKeyword":"大气光学"},{"id":"dd859d21-2b47-4856-82c2-bd0378f4dca1","keyword":"带宽","originalKeyword":"带宽"},{"id":"5f69bbc1-f2c8-4b4b-bfef-cd517ffafafa","keyword":"傅里叶变换","originalKeyword":"傅里叶变换"},{"id":"31ed8007-c9e2-4885-9e02-06bf7a2bbd0c","keyword":"湍流效应","originalKeyword":"湍流效应"}],"language":"zh","publisherId":"lzdzxb200603008","title":"滤波器带宽对傅里叶剪切干涉法精度的影响","volume":"23","year":"2006"},{"abstractinfo":"采用傅里叶级数有关理论,根据缠绕复合材料内部细观结构的特点,建立了缠绕复合材料刚度预测模型.该模型将缠绕复合材料特征单元的刚度作为一个刚度场,利用二维傅里叶级数展开得到描述该刚度场的函数.算例的结果表明,本文中所建立的模型可以预测缠绕复合材料整体刚度特性,同时通过傅里叶级数各阶展开项的叠加可以反映材料内部细观结构对缠绕复合材料刚度特性的影响.","authors":[{"authorName":"李俭","id":"5c9a163a-8e20-4d2b-9bd2-6d7f1c09be48","originalAuthorName":"李俭"},{"authorName":"温卫东","id":"b1d1f5a6-a965-4ebc-a45c-d358efe5fcc7","originalAuthorName":"温卫东"},{"authorName":"崔海涛","id":"ca6cefc6-117a-41df-a523-277836d1ac89","originalAuthorName":"崔海涛"}],"doi":"","fpage":"169","id":"62bc2493-08a5-4898-9109-49f98ff44b46","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":"63fb7dd7-9d46-4f6e-b9b2-171cb6ee7229","keyword":"缠绕","originalKeyword":"缠绕"},{"id":"ddffdea1-691f-4cd8-aa4a-95a45d946ed0","keyword":"复合材料","originalKeyword":"复合材料"},{"id":"ea9399a7-c918-46af-a357-2faa400d5354","keyword":"刚度","originalKeyword":"刚度"},{"id":"02a94a08-68d9-4fa0-ba95-124bc33db514","keyword":"预测模型","originalKeyword":"预测模型"},{"id":"eb47b871-ce60-4c4c-80ee-6f8b4a73f1d8","keyword":"傅里叶级数","originalKeyword":"傅里叶级数"}],"language":"zh","publisherId":"fhclxb200805028","title":"基于傅里叶级数的缠绕复合材料刚度预测方法","volume":"25","year":"2008"},{"abstractinfo":"用分步傅里叶变换方法数值求解非线性薛定谔方程,研究了一阶自傅里叶光孤子信号在光纤传输中的相互作用特性,证明了算法内部不存在理论误差.数值模拟结果表明:1)一阶自傅里叶孤子对中的相互作用表现不同于一阶标准孤子对,它类似于二阶或准二阶孤子之间的相互作用特性.两孤子经历一段周期性的相互吸引后,出现强烈的相互排斥.2)孤子相互作用特性不足以用孤子的阶去区分或分类,在同一阶的孤子中,不同的脉宽对孤子的相互作用有显著不同的影响.3)微弱的三阶色散效应有利于抑制一阶自傅里叶孤子间的相互作用.","authors":[{"authorName":"殷德京","id":"19ff89d9-ea5a-430c-a26b-cef288af1fb5","originalAuthorName":"殷德京"}],"doi":"10.3969/j.issn.1007-5461.2012.06.014","fpage":"741","id":"9400e358-5fb0-4032-b477-61861159faa1","issue":"6","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":"6913d0e1-9cf4-4a5b-b894-acf2fb589190","keyword":"纤维与波导光学","originalKeyword":"纤维与波导光学"},{"id":"8cbdc7bc-5dd5-469e-b94d-7ec2b3d3173e","keyword":"自傅里叶孤子","originalKeyword":"自傅里叶孤子"},{"id":"81570af2-6290-44c1-90cf-f774a635cb30","keyword":"分步傅里叶变换方法","originalKeyword":"分步傅里叶变换方法"},{"id":"bb330cd0-a44b-4e2b-ad73-60db1386a1b6","keyword":"相互作用","originalKeyword":"相互作用"},{"id":"4cb46a27-10f8-41c8-b16e-a0f9568afcfb","keyword":"三阶色散","originalKeyword":"三阶色散"}],"language":"zh","publisherId":"lzdzxb201206014","title":"自傅里叶光孤子的相互作用特性","volume":"29","year":"2012"},{"abstractinfo":"在对傅里叶红外光谱仪与传统的色散型光谱分析仪进行比较的基础上,综述了基于该装置的高温红外光谱发射率测量技术的国内外发展现状.在详细介绍各具特色的装置结构、工作原理、测量温度范围和测量水平的同时,评述了这项技术的特点和局限性,并对其未来发展趋势进行了展望.","authors":[{"authorName":"何小瓦","id":"88a187ff-b6ca-4419-80da-e1d6aaffb772","originalAuthorName":"何小瓦"},{"authorName":"戴景民","id":"3e1a3583-095d-49ec-84bd-ebc53c34508d","originalAuthorName":"戴景民"},{"authorName":"辛春锁","id":"7de618cc-d2f7-4bee-97b8-02010f019442","originalAuthorName":"辛春锁"},{"authorName":"王宗伟","id":"78a30c8f-b5ff-4620-addd-1f47d961bc30","originalAuthorName":"王宗伟"},{"authorName":"徐辉","id":"93d23d4b-c176-45f2-b01b-576c94024488","originalAuthorName":"徐辉"}],"doi":"10.3969/j.issn.1007-2330.2007.05.004","fpage":"13","id":"54d2d3b4-8e16-4bfa-a77e-1fa02d85bb5c","issue":"5","journal":{"abbrevTitle":"YHCLGY","coverImgSrc":"journal/img/cover/YHCLGY.jpg","id":"77","issnPpub":"1007-2330","publisherId":"YHCLGY","title":"宇航材料工艺 "},"keywords":[{"id":"805568c2-060e-4e13-b799-6d103a502061","keyword":"光谱发射率","originalKeyword":"光谱发射率"},{"id":"dcb251de-0a8e-4dd7-a2ca-8a76129f1e15","keyword":"发射率测量","originalKeyword":"发射率测量"},{"id":"96d0bca4-9a7c-4ae7-8549-fe4355995fa4","keyword":"高温环境","originalKeyword":"高温环境"},{"id":"f4f99223-2f7e-4131-a66f-6b5d57bbf0e8","keyword":"FT-IR","originalKeyword":"FT-IR"}],"language":"zh","publisherId":"yhclgy200705004","title":"基于傅里叶光谱仪在高温环境下材料光谱发射率测试技术","volume":"37","year":"2007"},{"abstractinfo":"利用XRD线形傅氏分析方法定量分析TA15合金在750、800和925℃热压缩变形后的位错亚结构.结果表明:利用 XRD 线性傅氏分析的方法可以比较方便地定量表征位错信息;位错类型主要为基面(0002)、柱面(1010)和锥面(1011)型位错.在750℃、1s-1变形条件下,随应变量的增加,直到60%变形量时,位错密度仍在增加.而在800℃、1s-1变形条件下,位错密度先增加后降低.各变形条件下位错密度均在1010～1011cm-2的范围:750℃变形后,各晶面的位错密度随应变量增加而增加,但是基面(0002)和锥面(1011)位错随应变量的增加的速度更快,说明此温度下基面和锥面位错更易滑移:800℃变形后锥面位错密度随着应变量增加稍有增加,而柱面(1010)和基面(0002)的变化很大.","authors":[{"authorName":"刘勇","id":"f9f872bc-2a74-4157-8f74-b185563f6efc","originalAuthorName":"刘勇"},{"authorName":"朱景川","id":"a01988ff-8bdf-4db2-81d2-083950cdceaa","originalAuthorName":"朱景川"},{"authorName":"王洋","id":"333a6294-16cd-4bf5-8449-c7bcb6ad76bc","originalAuthorName":"王洋"},{"authorName":"占家军","id":"ca7da949-5761-458d-9904-5736f7341861","originalAuthorName":"占家军"}],"doi":"","fpage":"1505","id":"164ca2f6-a1ab-4b53-894f-c5d799bdb5fb","issue":"9","journal":{"abbrevTitle":"XYJSCLYGC","coverImgSrc":"journal/img/cover/XYJSCLYGC.jpg","id":"69","issnPpub":"1002-185X","publisherId":"XYJSCLYGC","title":"稀有金属材料与工程"},"keywords":[{"id":"a521d85d-e71c-4f0e-8a91-bb4b2d729fd0","keyword":"TA15合金","originalKeyword":"TA15合金"},{"id":"c5c93aed-4d20-40f0-9592-bcae56bdf2f9","keyword":"热压缩变形","originalKeyword":"热压缩变形"},{"id":"d6345368-b954-4b85-9cf7-2ce039992eb9","keyword":"XRD线性傅氏分析方法","originalKeyword":"XRD线性傅氏分析方法"},{"id":"76906d41-2c9b-42ec-950d-744047239ccb","keyword":"位错","originalKeyword":"位错"}],"language":"zh","publisherId":"xyjsclygc200809001","title":"XRD线形傅氏分析方法研究TA15合金热压缩变形后的位错","volume":"37","year":"2008"},{"abstractinfo":"对一阶自傅里叶孤子与一阶标准孤子光信号在光纤中传输的相互作用特性进行了数值模拟研究.所用方法为算法内部不存在理论误差的分步傅立叶变换法.结果表明:同为一阶孤子,若振幅不同,三阶色散效应导致的线性延时性不同,振幅越大,延时越多;孤子的近程相互作用会进一步改变孤子的群速度,甚至可以依据两孤子的先后排列方向而决定减速还是增速.","authors":[{"authorName":"殷德京","id":"b410abf6-4573-495c-9867-6ac1e06ece1c","originalAuthorName":"殷德京"}],"doi":"10.3969/j.issn.1007-5461.2014.03.013","fpage":"335","id":"43a4c50e-7b96-4c20-8555-63aab81ba450","issue":"3","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":"7b24841d-8f99-482d-b591-96b7b6cf0d4f","keyword":"纤维与波导光学","originalKeyword":"纤维与波导光学"},{"id":"1567a68a-aeaf-4c72-9c17-38624f0dc024","keyword":"自傅里叶孤子","originalKeyword":"自傅里叶孤子"},{"id":"ee81cd42-02e3-44f4-a88e-fd7cd56706dd","keyword":"分步傅里叶变换方法","originalKeyword":"分步傅里叶变换方法"},{"id":"0e3f2ec0-ee17-4969-98d4-86f15184fb88","keyword":"相互作用","originalKeyword":"相互作用"}],"language":"zh","publisherId":"lzdzxb201403013","title":"三阶色散下的自傅里叶孤子与标准孤子相互作用","volume":"31","year":"2014"},{"abstractinfo":"将热分析-傅里叶红外光谱-气相色谱-质谱组成同步联用检测系统,对果胶在N2气和N2/O2氛围中,243、270和335℃3个温度点的热解产物经傅里叶红外光谱和GC-MS进行同步分析,在2种氛围下共检测鉴别了26种热分解产物.","authors":[{"authorName":"刘春波","id":"f5012373-4c52-42d1-9e96-e9262f32818f","originalAuthorName":"刘春波"},{"authorName":"曾晓鹰","id":"d3c48b3d-14b5-4823-ab4f-0cf2daf4d70c","originalAuthorName":"曾晓鹰"},{"authorName":"王昆淼","id":"51560f63-3e76-44c0-99cd-815b8c2d416a","originalAuthorName":"王昆淼"},{"authorName":"赵伟","id":"112852ba-6541-4b79-a674-e18923730d67","originalAuthorName":"赵伟"},{"authorName":"韩敬美","id":"e695e448-e0d7-46b4-b37f-ae33f864bd93","originalAuthorName":"韩敬美"},{"authorName":"何沛","id":"6300a824-60dc-4867-8092-05a3ba99f3ff","originalAuthorName":"何沛"},{"authorName":"陈永宽","id":"22f9bfd4-ebbd-4aa3-b99f-773d9caa25ae","originalAuthorName":"陈永宽"},{"authorName":"缪明明","id":"789c0353-ebed-4f89-9e89-5866b0d2d3b8","originalAuthorName":"缪明明"},{"authorName":"刘志华","id":"61d04ec1-7d72-4ed4-9dad-40ef5a2f1a79","originalAuthorName":"刘志华"}],"doi":"10.3724/SP.J.1095.2012.00572","fpage":"1218","id":"431bf04c-e7f6-4c1b-9969-58f916234e38","issue":"10","journal":{"abbrevTitle":"YYHX","coverImgSrc":"journal/img/cover/YYHX.jpg","id":"73","issnPpub":"1000-0518","publisherId":"YYHX","title":"应用化学"},"keywords":[{"id":"f9f3d36d-d61b-401e-8b49-cb142c912fab","keyword":"同步热分析","originalKeyword":"同步热分析"},{"id":"6063d881-55d3-4a39-b44e-2bcd768f1407","keyword":"傅里叶红外光谱","originalKeyword":"傅里叶红外光谱"},{"id":"6e504aa6-6fc4-4ef3-ba51-4c1bbcafb1e9","keyword":"气相色谱-质谱","originalKeyword":"气相色谱-质谱"},{"id":"b489f259-738f-4b8c-b597-a4105d0cdabf","keyword":"果胶热分解","originalKeyword":"果胶热分解"}],"language":"zh","publisherId":"yyhx201210020","title":"热分析-傅里叶红外光谱-气相色谱-质谱联用技术分析果胶的热分解产物","volume":"29","year":"2012"},{"abstractinfo":"大挠度剪切理论下复合材料夹层圆柱扁壳的稳定性控制方程是一组非线性高阶常系数偏微分方程, 其中包含四个独立的函数,它们分别为横向挠度w、参考曲面的法线转角Φx、Φy和应力函数F.本文中将这四个独立的函数表示为广义傅里叶级数,选用了两个变量分离的梁本征函数之积构成广义傅里叶级数的通项,通过梁本征函数中的待定常数使所选级数预先满足简支、固支或弹性支持边界条件.然后把以广义傅里叶级数表示的独立函数代入控制方程中便将这个非线性高阶常系数偏微分方程转化为非线性代数方程组,这样便可以寻求不同的通用程序进行求解.从而为复合材料叠层、夹层板壳在复杂边界条件下的弯曲、振动和稳定问题的求解探索出了一种通用的、有效的方法.","authors":[{"authorName":"张志民","id":"c90f68c7-9d52-4e71-8072-abfa2f1f9cdc","originalAuthorName":"张志民"},{"authorName":"刘宏增","id":"6e388228-dbf4-4412-9d05-85792e887e6b","originalAuthorName":"刘宏增"},{"authorName":"张恒","id":"70a6173f-572c-4c05-a68f-768a2a369b90","originalAuthorName":"张恒"}],"doi":"10.3321/j.issn:1000-3851.1998.02.020","fpage":"0","id":"17454d59-8b05-41a4-9c6a-c45e07351e3e","issue":"2","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":"0e166b34-8094-4121-8f61-c76eceef8058","keyword":"复合材料夹层扁壳","originalKeyword":"复合材料夹层扁壳"},{"id":"105b6842-2490-48fc-80d5-357fe5273d3a","keyword":"广义傅里叶级数","originalKeyword":"广义傅里叶级数"},{"id":"b21294bf-7d2a-4565-966b-39eecb294145","keyword":"梁本征函数","originalKeyword":"梁本征函数"},{"id":"299a80a1-69d2-445b-b56a-73108ee9bad8","keyword":"大挠度","originalKeyword":"大挠度"},{"id":"0336cc1b-aa78-4415-8750-c72033ec3ad7","keyword":"剪切理论","originalKeyword":"剪切理论"}],"language":"zh","publisherId":"fhclxb199802020","title":"大挠度剪切理论下复合材料夹层圆柱扁壳的广义傅里叶级数解法","volume":"15","year":"1998"}],"totalpage":68,"totalrecord":673}