{"currentpage":1,"firstResult":0,"maxresult":10,"pagecode":5,"pageindex":{"endPagecode":5,"startPagecode":1},"records":[{"abstractinfo":"<span style=\"color:red\">燃烧</span>法是制备氧化物纳米材料的一种新方法,其中,<span style=\"color:red\">气</span><span style=\"color:red\">相</span><span style=\"color:red\">燃烧</span>法、<span style=\"color:red\">燃烧</span>火焰-化学<span style=\"color:red\">气</span><span style=\"color:red\">相</span>凝聚法已经实现了工业化生产;而一些新的工艺方法,如低温<span style=\"color:red\">燃烧</span>合成法、喷雾<span style=\"color:red\">燃烧</span>法、电控火焰合成法在制备纳米材料上也各有优缺点;<span style=\"color:red\">燃烧</span>法与其他技术的结合也在研究开发阶段.详细阐述了<span style=\"color:red\">燃烧</span>法的最新研究进展.","authors":[{"authorName":"程永亮","id":"89ca1809-ab52-48c9-8828-81a5222df0e8","originalAuthorName":"程永亮"},{"authorName":"宋武林","id":"b693f216-6501-4c28-bec6-c57247af047d","originalAuthorName":"宋武林"},{"authorName":"谢长生","id":"e57889c4-9e68-475d-abfa-32a083cfb164","originalAuthorName":"谢长生"}],"doi":"","fpage":"70","id":"29ed4e90-a9c2-4210-8946-7b0830daa691","issue":"7","journal":{"abbrevTitle":"CLDB","coverImgSrc":"journal/img/cover/CLDB.jpg","id":"8","issnPpub":"1005-023X","publisherId":"CLDB","title":"材料导报"},"keywords":[{"id":"97fd82e1-d7fd-4d4f-a18a-3f1457b360bc","keyword":"<span style=\"color:red\">燃烧</span>合成","originalKeyword":"燃烧合成"},{"id":"c8fbd1ff-add5-499a-ab2e-3f8dcbd2725b","keyword":"氧化物","originalKeyword":"氧化物"},{"id":"645abe79-aa48-48cf-8197-b88d28e1cdcb","keyword":"纳米粒子","originalKeyword":"纳米粒子"},{"id":"68bb2999-23f6-4c67-a480-f080399fce0e","keyword":"<span style=\"color:red\">气</span><span style=\"color:red\">相</span><span style=\"color:red\">燃烧</span>","originalKeyword":"气相燃烧"}],"language":"zh","publisherId":"cldb200307021","title":"<span style=\"color:red\">燃烧</span>法制备氧化物纳米材料的研究进展","volume":"17","year":"2003"},{"abstractinfo":"利用多重射流氢氧焰<span style=\"color:red\">燃烧</span>反应器,通过控制进料方式,以TiCl4和SiCl4为原料合成了具有典型核壳结构的纳米TiO2/SiO2复合颗粒,并分析了氢氧焰<span style=\"color:red\">燃烧</span>合成过程中核壳结构的形成机理.在纳米TiO2/SiO2复合颗粒中,无定形的SiO2均匀地包覆在晶态TiO2颗粒表面形成核壳结构,引入SiO2不但有效抑制TiO2晶粒的生长,而且抑制了锐钛相向金红石<span style=\"color:red\">相</span>的转变.在TiCl4和SiCl4次序进料时,TiCl4优先反应并通过成核生长生成TiO2纳米颗粒,SiCl4反应生成的SiO2通过在TiO2颗粒表面非均相成核生长,形成核壳结构的纳米复合颗粒.","authors":[{"authorName":"胡彦杰","id":"291e2704-9c60-4e65-9053-b90bead0ddb0","originalAuthorName":"胡彦杰"},{"authorName":"李春忠","id":"50e37b41-fdfe-477b-993b-97e0a9d37ce2","originalAuthorName":"李春忠"},{"authorName":"丛德滋","id":"757c9d53-2413-4caf-969c-f9555c32122a","originalAuthorName":"丛德滋"},{"authorName":"姜海波","id":"82524dd8-fbec-43cf-a8e6-c49aa056f260","originalAuthorName":"姜海波"},{"authorName":"赵尹","id":"aeee1424-4136-4edf-b73c-4a146bfcfad1","originalAuthorName":"赵尹"}],"doi":"10.3321/j.issn:1000-324X.2007.02.003","fpage":"205","id":"6a54fbd2-9728-4e6d-ae9b-c0d85085f2b8","issue":"2","journal":{"abbrevTitle":"WJCLXB","coverImgSrc":"journal/img/cover/WJCLXB.jpg","id":"62","issnPpub":"1000-324X","publisherId":"WJCLXB","title":"无机材料学报"},"keywords":[{"id":"774f767f-a239-4cc8-8051-761f338fd60a","keyword":"氢氧焰","originalKeyword":"氢氧焰"},{"id":"c40babdf-3c5a-4766-bdc0-70850d6606a4","keyword":"<span style=\"color:red\">气</span><span style=\"color:red\">相</span><span style=\"color:red\">燃烧</span>","originalKeyword":"气相燃烧"},{"id":"1c658a9e-0084-4f5c-8410-d9e0b00ccca6","keyword":"核壳结构","originalKeyword":"核壳结构"},{"id":"893b94ed-ca40-42a8-90e9-28f5fe65d261","keyword":"TiO2","originalKeyword":"TiO2"},{"id":"811bfec3-2680-4ce3-be16-b9f5f407d25a","keyword":"SiO2","originalKeyword":"SiO2"}],"language":"zh","publisherId":"wjclxb200702003","title":"氢氧焰<span style=\"color:red\">燃烧</span>合成核壳结构纳米TiO2/SiO2复合颗粒及机理分析","volume":"22","year":"2007"},{"abstractinfo":"根据机械合金化和界面固<span style=\"color:red\">相</span>扩散反应的基本原理,开创性地提出了机械碾压法加化学镀配料加氢化<span style=\"color:red\">燃烧</span>合成的三步合成工艺,制备出高容量的Mg-Ni储氢合金.研究表明,<span style=\"color:red\">气</span><span style=\"color:red\">相</span><span style=\"color:red\">燃烧</span>过程中的温度、压力及保温时间对<span style=\"color:red\">燃烧</span>产物的组成有较大的影响,通过对反应过程的分析得出了合成Mg-Ni合金箔的反应机理.热分析测试表明所得Mg-Ni合金箔在220℃放氢,放氢量为2.6wt%.","authors":[{"authorName":"贾志华","id":"668c48c0-4b88-45a9-b079-73a2f7cc1c41","originalAuthorName":"贾志华"},{"authorName":"王玉平","id":"49c7a225-e77f-409e-9867-eaaa9d6e0a0c","originalAuthorName":"王玉平"},{"authorName":"刘文斌","id":"39f54b00-a748-4efa-99c3-40145aa83c3f","originalAuthorName":"刘文斌"}],"doi":"","fpage":"121","id":"024db37d-5420-423f-bbaa-03f951748e0d","issue":"10","journal":{"abbrevTitle":"CLDB","coverImgSrc":"journal/img/cover/CLDB.jpg","id":"8","issnPpub":"1005-023X","publisherId":"CLDB","title":"材料导报"},"keywords":[{"id":"3e06c888-de3d-4cd4-94d5-0764198adb53","keyword":"储氢","originalKeyword":"储氢"},{"id":"687c8018-8d06-4811-a4e0-38382b0c09f2","keyword":"<span style=\"color:red\">气</span><span style=\"color:red\">相</span><span style=\"color:red\">燃烧</span>","originalKeyword":"气相燃烧"},{"id":"1b51bca7-17c0-47b2-bd9f-2ac8da4ec039","keyword":"Mg-Ni合金","originalKeyword":"Mg-Ni合金"}],"language":"zh","publisherId":"cldb200510032","title":"Mg-Ni储氢合金箔的制备及储氢性能研究","volume":"19","year":"2005"},{"abstractinfo":"采用TTM法与型线定点法相结合的方式生成带涡流器环形<span style=\"color:red\">燃烧</span>室贴体网格,在任意曲线坐标系中对其三维两相反应流场进行数值模拟,采用的紊流、<span style=\"color:red\">燃烧</span>以及辐射模型分别为:标准k-ε方程,EBU-Arrhenius公式,六通量热辐射模型等.在同位网格系下气<span style=\"color:red\">相</span>采用SIMPLE算法求解,<span style=\"color:red\">气</span>液两<span style=\"color:red\">相</span>流动用PSIC法模拟.通过对两种<span style=\"color:red\">燃烧</span>室的计算结果与实验值比较表明本计算方法合理,所得的计算结果可为环形<span style=\"color:red\">燃烧</span>室的优化设计提供指导数据.","authors":[{"authorName":"蔡文祥","id":"39ef9afd-5cc7-4f2d-9eda-b550f8a887cf","originalAuthorName":"蔡文祥"},{"authorName":"赵坚行","id":"e7b3e1e7-6c58-43a7-a835-130c3c10a29d","originalAuthorName":"赵坚行"},{"authorName":"张靖周","id":"c1171029-70bc-4488-9443-4bf169568039","originalAuthorName":"张靖周"}],"doi":"","fpage":"179","id":"f2ace13b-a829-4e9f-8ed0-40101f73f863","issue":"z2","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":"770b907e-3888-4a71-bbf4-c756c721a24e","keyword":"数值模拟","originalKeyword":"数值模拟"},{"id":"7950cce6-a0d4-4b7f-896d-0eb7047a34d3","keyword":"两相反应流","originalKeyword":"两相反应流"},{"id":"e8dbab81-bcbb-4a01-93f2-1d6fdb2d8452","keyword":"<span style=\"color:red\">燃烧</span>室","originalKeyword":"燃烧室"},{"id":"908b40c1-b363-4d81-a4a0-eb0df62187fa","keyword":"涡流器","originalKeyword":"涡流器"},{"id":"2f30d535-4bae-42e7-9569-27c82a38efae","keyword":"贴体网格","originalKeyword":"贴体网格"}],"language":"zh","publisherId":"gcrwlxb2006z2047","title":"环形<span style=\"color:red\">燃烧</span>室内<span style=\"color:red\">气</span><span style=\"color:red\">相</span><span style=\"color:red\">燃烧</span>及两<span style=\"color:red\">相</span>流动计算","volume":"27","year":"2006"},{"abstractinfo":"本文建立了分级进风<span style=\"color:red\">燃烧</span>室高温<span style=\"color:red\">气</span>固两<span style=\"color:red\">相</span>流动的实验装置.利用三维激光粒子动态分析仪(PDA),测量了<span style=\"color:red\">燃烧室内有气</span><span style=\"color:red\">相</span><span style=\"color:red\">燃烧</span>的高温<span style=\"color:red\">气</span>固流动的两<span style=\"color:red\">相</span>瞬时速度场.得到了平均轴向与切向速度、轴向与切向脉动速度均方根值和轴向-切向脉动速度关联量的分布.","authors":[{"authorName":"郑晓川","id":"2f9c56d0-19e0-418d-9e89-551156826fac","originalAuthorName":"郑晓川"},{"authorName":"袁书生","id":"93511142-1768-4dff-a968-f4cbda795011","originalAuthorName":"袁书生"},{"authorName":"张健","id":"f748c3ea-d774-47ef-9c1f-b89c3d38a6a1","originalAuthorName":"张健"},{"authorName":"张洪涛","id":"76d0e047-6ffa-4478-add8-e405b873b765","originalAuthorName":"张洪涛"},{"authorName":"周力行","id":"e0a60b2b-8e73-440a-bb3e-73deb91eea8e","originalAuthorName":"周力行"}],"doi":"","fpage":"1066","id":"9ff3c70a-5251-449d-a6e4-9a3632a0e501","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":"7f2254b1-7ac5-470a-90ec-58261eed4584","keyword":"分级<span style=\"color:red\">燃烧</span>","originalKeyword":"分级燃烧"},{"id":"b7807099-c310-4981-b60c-c0da1f97025d","keyword":"高温<span style=\"color:red\">气</span>固两<span style=\"color:red\">相</span>流","originalKeyword":"高温气固两相流"},{"id":"b0a31f3c-c28f-446f-bfea-18447802b8c2","keyword":"PDA测量","originalKeyword":"PDA测量"}],"language":"zh","publisherId":"gcrwlxb200606053","title":"分级进风<span style=\"color:red\">燃烧</span>室内高温<span style=\"color:red\">气</span>固两<span style=\"color:red\">相</span>流动的PDA测量","volume":"27","year":"2006"},{"abstractinfo":"通过直接数值模拟的方法研究了旋流<span style=\"color:red\">燃烧</span>器中三维正庚烷喷雾<span style=\"color:red\">燃烧</span>,为实际喷雾蒸发和<span style=\"color:red\">燃烧</span>问题提供参考.<span style=\"color:red\">气</span><span style=\"color:red\">相</span><span style=\"color:red\">燃烧</span>模型采用自适应单步反应机理,液<span style=\"color:red\">相</span>采用拉格朗日方法跟踪,液滴蒸发采用无限传导蒸发模型.本文研究了<span style=\"color:red\">气</span><span style=\"color:red\">相</span>和液<span style=\"color:red\">相</span>时均特性.结果发现<span style=\"color:red\">燃烧</span>和中心回流区(CRZ)之间有相互促进作用;同向旋流导致更强的中心回流区(CRZ),但是会有更小的外部回流区(ORZ);富预混<span style=\"color:red\">燃烧</span>会有更高的化学反应速率,并且蒸发冷却的影响更为明显;湍流入流会导致更高的液滴散布和更小的液滴直径.","authors":[{"authorName":"杨建山","id":"83c39947-e8f2-4cc1-bd3e-38ea51dea9d4","originalAuthorName":"杨建山"},{"authorName":"罗坤","id":"fe06cbad-87d0-492a-81b1-71f3f05d1bf8","originalAuthorName":"罗坤"},{"authorName":"邵长孝","id":"c42aae77-35c1-414d-94c7-7178c65a368f","originalAuthorName":"邵长孝"},{"authorName":"樊建人","id":"e09118a6-7a94-4db6-b794-0fcadd8268e0","originalAuthorName":"樊建人"}],"doi":"","fpage":"335","id":"e417f119-5332-4e38-91d4-0316f2770175","issue":"2","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":"85a76304-dd68-4d34-83fb-629e1541600a","keyword":"液雾<span style=\"color:red\">燃烧</span>","originalKeyword":"液雾燃烧"},{"id":"4c204c6b-d07a-44e9-9cd5-8d7a353cc93f","keyword":"直接数值模拟","originalKeyword":"直接数值模拟"},{"id":"b17df0f8-5599-4d78-8b78-7ec5790b9933","keyword":"旋流<span style=\"color:red\">燃烧</span>","originalKeyword":"旋流燃烧"},{"id":"f4dfbf18-edb0-4b5d-9023-17a5e3d8a57e","keyword":"时均特性","originalKeyword":"时均特性"}],"language":"zh","publisherId":"gcrwlxb201502023","title":"<span style=\"color:red\">气</span>液两<span style=\"color:red\">相</span>旋流<span style=\"color:red\">燃烧</span>的时均统计特性","volume":"36","year":"2015"},{"abstractinfo":"本文利用三维PDA测量了预混段减小的斗山巴布科克旋流<span style=\"color:red\">燃烧</span>器<span style=\"color:red\">气</span>、固两<span style=\"color:red\">相</span>流动特性，并与设计的斗山巴布科克旋流<span style=\"color:red\">燃烧</span>器PDA测量结果对比，得出：预混段减小的<span style=\"color:red\">燃烧</span>器在x／d=0．1，0．3截面存在回流区，并将设计<span style=\"color:red\">燃烧</span>器回流区的位置由一二次风之间推迟至外二次风区域；预混段减后的<span style=\"color:red\">燃烧</span>器与设计<span style=\"color:red\">燃烧</span>器相比，轴向、径向、切向平均速度在二次风区域产生的峰值远离<span style=\"color:red\">燃烧</span>器轴线；在x／d=O．1—0．5截面，预混段减小的<span style=\"color:red\">燃烧</span>器与设计<span style=\"color:red\">燃烧</span>器相比一次风区域颗粒体积流量的峰值变大，二次风区域颗粒体积流量的峰值变小，在<span style=\"color:red\">燃烧</span>器出口附近回流区内的颗粒体积流量明显降低。","authors":[{"authorName":"曾令艳","id":"f2b94d6c-a575-476e-96a5-dd63681c2d67","originalAuthorName":"曾令艳"},{"authorName":"李争起","id":"bc326248-41df-4515-8531-01df8f1084ca","originalAuthorName":"李争起"},{"authorName":"赵广播","id":"97358fbf-413a-4ab0-a8d8-67e6e134ae3e","originalAuthorName":"赵广播"},{"authorName":"周航","id":"8175a248-536e-4f8e-bee5-40d29a178aed","originalAuthorName":"周航"},{"authorName":"张福成","id":"e23c56e2-a2a7-4a15-8bdd-e47ad8025754","originalAuthorName":"张福成"}],"doi":"","fpage":"1953","id":"5133eafb-3329-4dd4-8ecb-bb21507e7dec","issue":"11","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":"38088c84-90b0-4052-8942-cdd5fce5b375","keyword":"<span style=\"color:red\">燃烧</span>器","originalKeyword":"燃烧器"},{"id":"381d98dc-3325-41a5-b74f-aea3f4eeffde","keyword":"<span style=\"color:red\">气</span>固两<span style=\"color:red\">相</span>流动","originalKeyword":"气固两相流动"},{"id":"5fe24637-4ec9-4559-b5fb-2c84f175559c","keyword":"三维PDA","originalKeyword":"三维PDA"}],"language":"zh","publisherId":"gcrwlxb201111040","title":"预混段长度对旋流<span style=\"color:red\">燃烧</span>器<span style=\"color:red\">气</span>固两<span style=\"color:red\">相</span>流动特性的影响","volume":"32","year":"2011"},{"abstractinfo":"在自行设计的多重射流<span style=\"color:red\">燃烧</span>反应器基础上,通过氢气和空气预混合辅助<span style=\"color:red\">燃烧</span>方法,用四氯化钛作为前驱体<span style=\"color:red\">气</span><span style=\"color:red\">相</span>水解合成了纳米二氧化钛颗粒.并通过TEM、XRD、TG-DTA、X荧光半定量分析和UV-Vis吸收光谱对所制得的粒子进行了表征.以三氯乙烯(TCE)气体为模拟污染物,考察了粒子的<span style=\"color:red\">气</span><span style=\"color:red\">相</span>光催化性能.在连续流动式玻璃反应器中,反应时间为2h时,所制样品对三氯乙烯的降解率和商品TiO2<span style=\"color:red\">相</span>当.","authors":[{"authorName":"李根深","id":"24ae4678-0d32-4ef2-8479-1984f7ffc331","originalAuthorName":"李根深"},{"authorName":"蔡平雄","id":"f05091ea-ab5e-434f-9533-5eaf2f330eca","originalAuthorName":"蔡平雄"},{"authorName":"干路平","id":"e19c5098-70b1-4a89-8b95-9fd027b035f8","originalAuthorName":"干路平"},{"authorName":"李春忠","id":"e93f3cfb-3d8e-41f4-866a-2fd30e83f9b9","originalAuthorName":"李春忠"},{"authorName":"丛德滋","id":"e3de06bd-667a-4dd5-9773-84926a928f78","originalAuthorName":"丛德滋"}],"doi":"","fpage":"1990","id":"3c95aa90-576a-4b0b-95bc-a84982f110dc","issue":"z1","journal":{"abbrevTitle":"GNCL","coverImgSrc":"journal/img/cover/GNCL.jpg","id":"33","issnPpub":"1001-9731","publisherId":"GNCL","title":"功能材料"},"keywords了平均轴向与切向速度、轴向与切向脉动速度均方根值和轴向-切向脉动速度关联量的分布.","authors":[{"authorName":"郑晓川","id":"2f9c56d0-19e0-418d-9e89-551156826fac","originalAuthorName":"郑晓川"},{"authorName":"袁书生","id":"93511142-1768-4dff-a968-f4cbda795011","originalAuthorName":"袁书生"},{"authorName":"张健","id":"f748c3ea-d774-47ef-9c1f-b89c3d38a6a1","originalAuthorName":"张健"},{"authorName":"张洪涛","id":"76d0e047-6ffa-4478-add8-e405b873b765","originalAuthorName":"张洪涛"},{"authorName":"周力行","id":"e0a60b2b-8e73-440a-bb3e-73deb91eea8e","originalAuthorName":"周力行"}],"doi":"","fpage":"1066","id":"9ff3c70a-5251-449d-a6e4-9a3632a0e501","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":"7f2254b1-7ac5-470a-90ec-58261eed4584","keyword":"分级<span style=\"color:red\">燃烧</span>","originalKeyword":"分级燃烧"},{"id":"b7807099-c310-4981-b60c-c0da1f97025d","keyword":"高温<span style=\"color:red\">气</span>固两<span style=\"color:red\">相</span>流","originalKeyword":"高温气固两相流"},{"id":"b0a31f3c-c28f-446f-bfea-18447802b8c2","keyword":"PDA测量","originalKeyword":"PDA测量"}],"language":"zh","publisherId":"gcrwlxb200606053","title":"分级进风<span style=\"color:red\">燃烧</span>室内高温<span style=\"color:red\">气</span>固两<span style=\"color:red\">相</span>流动的PDA测量","volume":"27","year":"2006"},{"abstractinfo":"通过直接数值模拟的方法研究了旋流<span style=\"color:red\">燃烧</span>器中三维正庚烷喷雾<span style=\"color:red\">燃烧</span>,为实际喷雾蒸发和<span style=\"color:red\">燃烧</span>问题提供参考.<span style=\"color:red\">气</span><span style=\"color:red\">相</span><span style=\"color:red\">燃烧</span>模型采用自适应单步反应机理,液<span style=\"color:red\">相</span>采用拉格朗日方法跟踪,液滴蒸发采用无限传导蒸发模型.本文研究了<span style=\"color:red\">气</span><span style=\"color:red\">相</span>和液<span style=\"color:red\">相</span>时均特性.结果发现<span style=\"color:red\">燃烧</span>和中心回流区(CRZ)之间有相互促进作用;同向旋流导致更强的中心回流区(CRZ),但是会有更小的外部回流区(ORZ);富预混<span style=\"color:red\">燃烧</span>会有更高的化学反应速率,并且蒸发冷却的影响更为明显;湍流入流会导致更高的液滴散布和更小的液滴直径.","authors":[{"authorName":"杨建山","id":"83c39947-e8f2-4cc1-bd3e-38ea51dea9d4","originalAuthorName":"杨建山"},{"authorName":"罗坤","id":"fe06cbad-87d0-492a-81b1-71f3f05d1bf8","originalAuthorName":"罗坤"},{"authorName":"邵长孝","id":"c42aae77-35c1-414d-94c7-7178c65a368f","originalAuthorName":"邵长孝"},{"authorName":"樊建人","id":"e09118a6-7a94-4db6-b794-0fcadd8268e0","originalAuthorName":"樊建人"}],"doi":"","fpage":"335","id":"e417f119-5332-4e38-91d4-0316f2770175","issue":"2","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":"85a76304-dd68-4d34-83fb-629e1541600a","keyword":"液雾<span style=\"color:red\">燃烧</span>","originalKeyword":"液雾燃烧"},{"id":"4c204c6b-d07a-44e9-9cd5-8d7a353cc93f","keyword":"直接数值模拟","originalKeyword":"直接数值模拟"},{"id":"b17df0f8-5599-4d78-8b78-7ec5790b9933","keyword":"旋流<span style=\"color:red\">燃烧</span>","originalKeyword":"旋流燃烧"},{"id":"f4dfbf18-edb0-4b5d-9023-17a5e3d8a57e","keyword":"时均特性","originalKeyword":"时均特性"}],"language":"zh","publisherId":"gcrwlxb201502023","title":"<span style=\"color:red\">气</span>液两<span style=\"color:red\">相</span>旋流<span style=\"color:red\">燃烧</span>的时均统计特性","volume":"36","year":"2015"},{"abstractinfo":"本文利用三维PDA测量了预混段减小的斗山巴布科克旋流<span style=\"color:red\">燃烧</span>器<span style=\"color:red\">气</span>、固两<span style=\"color:red\">相</span>流动特性，并与设计的斗山巴布科克旋流<span style=\"color:red\">燃烧</span>器PDA测量结果对比，得出：预混段减小的<span style=\"color:red\">燃烧</span>器在x／d=0．1，0．3截面存在回流区，并将设计<span style=\"color:red\">燃烧</span>器回流区的位置由一二次风之间推迟至外二次风区域；预混段减后的<span style=\"color:red\">燃烧</span>器与设计<span style=\"color:red\">燃烧</span>器相比，轴向、径向、切向平均速度在二次风区域产生的峰值远离<span style=\"color:red\">燃烧</span>器轴线；在x／d=O．1—0．5截面，预混段减小的<span style=\"color:red\">燃烧</span>器与设计<span style=\"color:red\">燃烧</span>器相比一次风区域颗粒体积流量的峰值变大，二次风区域颗粒体积流量的峰值变小，在<span style=\"color:red\">燃烧</span>器出口附近回流区内的颗粒体积流量明显降低。","authors":[{"authorName":"曾令艳","id":"f2b94d6c-a575-476e-96a5-dd63681c2d67","originalAuthorName":"曾令艳"},{"authorName":"李争起","id":"bc326248-41df-4515-8531-01df8f1084ca","originalAuthorName":"李争起"},{"authorName":"赵广播","id":"97358fbf-413a-4ab0-a8d8-67e6e134ae3e","originalAuthorName":"赵广播"},{"authorName":"周航","id":"8175a248-536e-4f8e-bee5-40d29a178aed","originalAuthorName":"周航"},{"authorName":"张福成","id":"e23c56e2-a2a7-4a15-8bdd-e47ad8025754","originalAuthorName":"张福成"}],"doi":"","fpage":"1953","id":"5133eafb-3329-4dd4-8ecb-bb21507e7dec","issue":"11","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":"38088c84-90b0-4052-8942-cdd5fce5b375","keyword":"<span style=\"color:red\">燃烧</span>器","originalKeyword":"燃烧器"},{"id":"381d98dc-3325-41a5-b74f-aea3f4eeffde","keyword":"<span style=\"color:red\">气</span>固两<span style=\"color:red\">相</span>流动","originalKeyword":"气固两相流动"},{"id":"5fe24637-4ec9-4559-b5fb-2c84f175559c","keyword":"三维PDA","originalKeyword":"三维PDA"}],"language":"zh","publisherId":"gcrwlxb201111040","title":"预混段长度对旋流<span style=\"color:red\">燃烧</span>器<span style=\"color:red\">气</span>固两<span style=\"color:red\">相</span>流动特性的影响","volume":"32","year":"2011"},{"abstractinfo":"在自行设计的多重射流<span style=\"color:red\">燃烧</span>反应器基础上,通过氢气和空气预混合辅助<span style=\"color:red\">燃烧</span>方法,用四氯化钛作为前驱体<span style=\"color:red\">气</span><span style=\"color:red\">相</span>水解合成了纳米二氧化钛颗粒.并通过TEM、XRD、TG-DTA、X荧光半定量分析和UV-Vis吸收光谱对所制得的粒子进行了表征.以三氯乙烯(TCE)气体为模拟污染物,考察了粒子的<span style=\"color:red\">气</span><span style=\"color:red\">相</span>光催化性能.在连续流动式玻璃反应器中,反应时间为2h时,所制样品对三氯乙烯的降解率和Name":"徐纲","id":"63aa5f8b-e9ea-429d-a287-1f432d2c7e0f","originalAuthorName":"徐纲"},{"authorName":"聂超群","id":"649428a4-6686-4e5f-bec3-2c73445f96c9","originalAuthorName":"聂超群"},{"authorName":"黄伟光","id":"1ebf8940-a943-47e9-8ed1-9b2bbe63b2ed","originalAuthorName":"黄伟光"},{"authorName":"陈静宜","id":"7b9ad1c6-4209-440d-97fd-f22dedf26da0","originalAuthorName":"陈静宜"}],"doi":"","fpage":"141","id":"6243e938-c161-4957-8b00-e1d8402f318d","issue":"1","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":"c89497c2-1517-4166-8c41-a417ca9043b9","keyword":"燃气轮机<span style=\"color:red\">燃烧</span>室","originalKeyword":"燃气轮机燃烧室"},{"id":"b6534950-8a57-4fbd-a7db-b93741630252","keyword":"低热值煤气","originalKeyword":"低热值煤气"}],"language":"zh","publisherId":"gcrwlxb200301044","title":"燃气轮机<span style=\"color:red\">燃烧</span>室<span style=\"color:red\">燃烧</span>天然<span style=\"color:red\">气</span>和<span style=\"color:red\">燃烧</span>中低热值煤气的比较","volume":"24","year":"2003"}],"totalpage":4521,"totalrecord":45206}