EI会议论文查询(共3篇)

上海健康医学院图书馆情报咨询部检索报告编号：2016—EI 检索报告2016 年月日，受（学院/部门）（老师/同学）委托，就其提供的已发表的 3 篇文献，查找了EV（EI）检索系统。

实际检索结果的统计数据见下表：EI检索系统收录（篇）核心文献（原光盘版）外围文献3所委托文献的具体检索结果如下：1.标题:Risk evaluation method in failure mode and effects analysis based on failure cause-effect chain作者: Geng, Xiu-Li ; Chu, Xue-Ning来源出版物: Jisuanji Jicheng Zhizao Xitong/Computer Integrated Manufacturing Systems, CIMS,2009文献类型：Journal article (JA)EI收录号：20100512678337（核心文献）2.标题:Evaluation of product outline design scheme based on customer requirements satisfaction degree作者: Geng, Xiu-Li; Chu, Xue-Ning ; Zhang, Zai-Fang来源出版物: Shanghai Jiaotong Daxue Xuebao/Journal of Shanghai Jiaotong University, 2009文献类型：Journal article (JA)EI收录号：20100512677965（核心文献）3.标题:Research on product configuration rules extraction based on variable precision rough set and incremental updating作者: Geng, Xiu-Li; Zhang, Zai-Fang; Chu, Xue-Ning来源出版物: Shanghai Jiaotong Daxue Xuebao/Journal of Shanghai Jiaotong University, 2010文献类型：Journal article (JA)EI收录号：20103313151543（核心文献）特出具此检索报告。

ei收录的会议论文(共8篇)ei收录的会议论文(共8篇)篇一：如何判断国际会议论文是否被EI收录★ 如何判断国际会议论文是否被EI收录？如何判断国际会议论文是否被EI收录？可能会遇到这样的情况，有些国际会议说明了EI收录，可到最后却并未收录，让人郁闷至极。

那么如何判断一个国际会议是否会被EI收录呢？除了看这个会议以往的被收录情况外，还有以下几个小经验：一、看会议论文的出版单位会议EI收录其实与主办方关系很小，甚至没有任何关系，第一要素主要取决于会议论文的出版单位，根据多年经验，特列举全球著名出版单位如下： 1.德国斯普林格出版社（SPRINGER）：100%EI收录； 2.美国机械工程学会出版社（ASME）：100%EI收录； 3.美国土木工程学会出版社（ASCE）：100%EI收录； 4.美国电子电气工程计算机学会出版社（IEEE CS）：99%EI收录； 5.美国电子电气工程出版社（IEEE）：90%EI收录； 6.英国工程技术出版社（IET）：90%EI收录； 7.法国Atlantis Press：70%。

二、考察会议主席的诚信度 1.国际一级学会发起：如IFAC、IEEE等。

如果IEEE发起的会议IEEE要占51%的注册费，因此，该类会议注册费均在500美元以上。

请注意中国2016年只有一个是IEEE发起的，即ICMA2016，其他均不是，2016年至今中国没有一个会议是IEEE发起；2.国家一级学会发起：如中国计算机学会、中国自动化学会、中国通讯学会等，如WCICA、CCC等；3.各大学校级领导：中国大学校级领导作为主席办国际会议具有中国特色（如ICTE等）；4.国际一级学会技术支持：如IEEE CS、IEEE、IET、ASME、ASCE等。

如ICIC、ICNC；5.其他学者。

掌握了会议论文的出版单位以及会议主席的诚信度以后，还要注意论文格式和英文摘要的书写方法。

三、注意事项 1.这里仅讨论的是EI收录的技巧，不是讨论会议的水平。

ei检索会议论文
您好！我可以帮助您进行EI检索会议论文。

EI（Engineering Index）是一种国际著名的工程领域文献数据库，涵盖了许多工程学科，如机械工程、电子工程、材料科学等。

它收录的论文主要来自各种会议和期刊。

要进行EI检索会议论文，您可以采取以下步骤：
1. 访问EI数据库（如Engineering Village、Web of Science）。

2. 找到检索界面，并选择期望的检索条件，例如关键词、作者、会议名称等。

3. 输入相应的检索信息，并点击检索按钮。

4. 筛选结果，可以根据相关性、时间、作者等进行排序。

5. 查看论文的详细信息，包括标题、作者、摘要等。

6. 如果需要，可以保存论文的相关信息或导出引用。

7. 根据需要，可以获取全文或通过链接找到论文所在的会议网站。

请注意，EI数据库需要付费订阅才能访问全部内容，如果您
没有订阅，只能访问部分免费内容。

希望以上信息对您有帮助！如有其他问题，请随时提问。

关于SCI、SSCI、AHCI及EI收录论文检索号的查询方法[大全5篇]第一篇：关于SCI、SSCI、A&HCI及EI收录论文检索号的查询方法附件10:关于SCI、SSCI、A&HCI及EI收录论文检索号的查询方法一、SCI、SSCI、A&HCI收录论文检索号查询1．进入学校图书馆主页。

2．在页面下方“常用资源”中点击“Web of Knowledge”，进入ISI Web of Knowledge主页，点击上方标签“Web of Science”，进入检索页面，在页面下方引文数据库中勾选相应的数据库（SCI-EXPANDED或SSCI或A&HCI）。

3．在检索框中输入论文的英文标题，检索范围限定为题名，或在其他检索框中输入作者、地址等论文信息，点击“检索”，进入命中的结果页面。

λ如果是检索单篇论文，请点击论文题名进入论文的相关信息页面，其IDS号即为论文的检索号。

λ如果检索结果为多篇论文，请在检索到的结果页面选择所有符合条件的文章，勾选前面的方框后，在题名列表上方点击“添加到标记结果列表”，即可将所选文献添加到已标记列表中，再点击页面右上方的“标记结果列表()”，进入“Web of Science 标记记录”页面，在“第 1 步: 选择要输出的字段”方框中，勾选Author(s)作者、标题、来源、地址、IDS 编号，在“第2 步: 选择一个选项”方框中，点击“打印格式”，所出的页面中的ISI 文献传递号即为论文的检索号。

二、EI查询1．进入图书馆主页。

2.在页面左上侧列表中点击“电子资源”，进入跨库检索页面，点击右侧数据库列表中的“E”，选择“EI Engineering Village ”，进入EI主页，在相应的检索项中输入论文题名等论文信息，点击“serch”进行检索，获得相应的结果，再点击每篇文章后面的“Detailed”，进入文章信息的详细页面，其中的“Accession number”即为检索号。

Analysis of plastic and steel sleeve contact force on ANSYSAbstract. Plastic and steel sleeve contact force distribution, widely used in oil drilling mechanics,syringes, aerospace and so on. In this paper, plastic and steel ANSYS simulation compression sleeve contact deformation and contact force distribution state. Provide a valuable reference for the study of contact force fields Introduction.Keywords: Plastic; Steel Sleeve; Contact Force Distribution; ANSYS1.IntroductionResearch achievements have been in contact mechanics of fracturing technology to further enhance the domestic level, control production costs, such as high-voltage swing has made a significant contribution. To further raise the contact force distribution, we use ANSYS simulation packer seated, considering nonlinear contact problems characteristics and plastic tube sealing seat when the rubber material of the packer seat seal process numerical simulation analysis, find contacts Neri distribution.2.contact model analysis of the stress statePlastic tube axial compressive stress state , radial expansion . Research by the expansion of the inner wall of the steel sleeve plastic tube extrusion role radial pressure , the use of isolation method , a separate study on steel sleeve , steel sleeve in the space of stress state , as shown by the force of theinner wall of the steel sleeve case in Figure 1.Figure 1 A steel sleeve inner wall by the force.F is the axial pressure , pi is the radial pressure , a steel sleeve inner diameter , outer diameter is b,2.Stress analysis of thin-walled cylinderShown in Figure 1 , We know that the stress distribution is axisymmetric . Thus, the expression is to take the stress components:0,2)ln 23(,2)ln 1(22==+++-=+++=ϕρρϕϕρττρρσρρσC B AC B A( 2-1 ) Wherein the above formula, the radial stress , hoop stress and shear stress , A, B, C is a constant . Boundary conditions for the sleeve:⎪⎭⎪⎬⎫-=-=======b b a a b a q q ρρρρρρϕρρϕσσττ)(,)(0)(,0)( ( 2-2 )Steel sleeve are only subject to internal pressure problem , so the answer we get Lamea q ab b 112222---=ρσρ ( 2-3 ) a q ab b 112222-+-=ρσϕ………………………………………… ( 2-4 )Since the steel sleeve is axially symmetric problem, the calculation of circumferential strain was analyzed by the following formula()[]ρϕϕσσμσε+-=z E1( 2-5 )3.rubber deformation theory foundationStiffness is defined: refers to the displacement of the rubber in a certain range, the pressure on ( or tensile strength ) and its displacement ratio of the amount of variation is called static stiffness . Because rubber has such a static stiffness characteristics , variable compression deformation can restore the original state , radial axial pressure can occur after the expansion .F 1FF 2F 3X 2X 1X 3XFigure 2 Rubber compression load - displacement curveThe rubber is compressed to a range of the displacement amount after the pressure was slowly lifted uniform relationship between the rubber and the amount of displacement of the load suffered by the non-linear relationship shown in Figure 2 , the external force can be lifted back to the initial position of the rubber , there is no hysteresis with respect to the displacement of the load .From the above tests can be drawn: the use of plastic tube axial compressive contact force to do the test trials to meet assumptions.4.ANSYS simulation analysisUsing ANSYS mechanical model of the plastic tube in contact with the steel jacket for finite element analysis, the steel sleeve wall hoop stress strain distribution . According to the experimental method and the load characteristics , select three hollow plastic tube , the partition ring , fixed tube and pipe as the research object , create a structural model of the axis of symmetry shown in Figure 3 .A contact force analysis modelB jacket wall stress modelFigure 3 mechanical model to buildPlastic tube and steel casing for analysis model , the diagram shown in Figure A, axial compression cones , plastic squeeze tube radial expansion pipe wall , pipe deformation , thereby measure the contact stress . Figure B is a deformation of the casing after the force diagram , the spacer ring contact area without power, plastic tube extrusion severely deformed parts .Figure 4 Initial plastic tube with casing seat seal contact pressure distributionFigure 5 Plastic tube axial compression deformation maps Plastic tube under axial compression p = 100MPa role in axial compression cones shown in Figure 5 .As can be seen from Figure 5 , the plastic tube when the axial pressure reaches 100MPa, the compression distance of three plastic tube 61mm, at this time are the three plastic tube and the steel inner wall of the sleeve into contact to varying degrees , wherein the plastic tube and steel sets the maximum contact pressure , the value of 102MPa.The calculation results are shown in three different conditions are shown in Table 1.change of the three cartridges .80MPa contact pressure conditions change 100MPa contact pressure conditions changeFigure 6the greatest strain , the pressure on the top cones largest , more down smaller ; in cones and cones suffered under pressure mainly in the middle of the plastic tube , plastic tube in which the compression ratio cones bigger. This increases the axial pressure distribution , showing more obvious.5.ConclusionsPlastic cylinder with steel sleeve contact stress analysis for the song to the distribution, the lowest end of the maximum contact stress, and mainly for the plastic middle, followed by the middle of the plastic barrel, distribution showed a decreasing.References[1] Lubinski, A.,Althouse, W.S., Logan, J.L. Helical Buckling of Tubing sealed in Packers [J].JPT, 2012,14(3):pp655-670.[2] Hammerlindl, D.L. Movement, Forces and Stresses Associated with Combination Tubing Strings sealed in Packers[J]. PET, 2007,29(1): pp195-208.[3] Hammerlindl, D.J. Basic Fluid and Pressure Forces on oil well Tubular [J]. J.PET.Tech.,2009,32(3):pp153-159.[4] Hammerlindl, D.J.Packer-to-Tubing Forces for Intermediate Packers [J]. J. PET. Tech.,2010,32(2):pp515-527.[5] Cheatham, J.B., Pattillo, P.D. Helical Postbuckling Configuration of a WeightlessColumn Under the Action of an Axial Load [J]. SPE,J. 2010,(4):pp467-472.。

会议论文ei检索查询(共7篇)会议论文ei检索查询(共7篇)篇一：什么样的会议论文能够被SCI或者EI检索什么样的会议论文能够被SCI或者EI检索！（转载）管理提醒: 本帖被 kidy008 从新人展示移动到本区现在检索很多，包括SCI，SCIE，EI，ISTP，ACM。

关于哪些会被检索，很多人关注，写个短文供大家参考，当然不保证绝对正确，基本都差不多。

1.SCI检索 SCI检索包括SCI的3500多个期刊，大部分都是很著名的刊物，国内的e文刊物只有科学通报，中国科学，《计算机科学技术学报》（英文）等寥寥几种被SCI检索。

一些非常著名的会议可能会被SCI检索，但事先一般都会被某个刊物出版（一般为springer的）然后再被检索。

查询自己论文是否被SCI检索可以到在图书馆主页里面的：Web of Science Proceedingsfull fill the essential function, stress the shape beauty, and saving ater. The quality of the sanitary implement has been requested to include exact size tolerance, fine external appearance, physics function, flushing function etc. Flushing function is the ability that the bedpan ejects filth, ashes it clearly hile controlling the amount of ater. Without question, flush function is one of the uppermost functions. According to the flushing ay, bedpan can be divided into ash-don type, siphonic type and ejecting siphonic type. Wash-don bedpan rush out filth by the impact of the ater, the poer is decided by potential energy of the ater in tank subtracts losing energy. Siphonic bedpan?s flush poer primarily relies on siphonic poer. III. THE STRUCTURE DESIGN OF SIPHONIC BEDPAN?S FLOW CHANNEL As mentioned above, under the condition of piping ater-filled, hatever means e adopt, it ill not produce the siphonic phenomenon if air is interfused. So e should make sure that the piping section dimension is appropriate, as figure 1 shos, the diameter of D-E segment is degressive. According to the statics and hydromechanics theories, hile the fluid in piping flosstably, the physical volume flux is constant at any section of the pipe. So the smaller of the pipe section, the higher of the current velocity of the fluid. So the diameter change could result in the ater velocity change in the D-E segment. Figure 1. The structure design of siphonic bedpan?s flo channel Thus at the beginning of the siphonic bedpan?s flo channel, the flushing velocity of the ater being higher and higher, form the E-F segment in advance, expedite siphonic process, reduce the amount of ater, attained the purpose of saving ater. The D-E segment is rising, and its section diameter is generally among 55-65 mm. The ability of rushing out filth ill be eakend ith larger diameter, the result may increase ater amount. While the drainage amount in forepart ill be influenced ith smaller diameter, it ill cause the ater surface rising, and result in siphonic phenomenon later. The E-F segment is a hump segment, its perfect section diameter generally among 45-55 mm. The F-G segment is a increasing segment, the diameter is being bigger from small, and the section is being large, it ill loer segment?s the current length increase, velocity of in the addition fluid, make make siphonic siphonic phenomenon keep more time, And its section diameter is generally among 55-60 mm.IV. THREE-DIMENSIONAL STEADY NUMERIC SIMULATION FOR FLOWING IN BEDPAN Bedpan?s geometrical modeling is the most plicated in sanitary implements, its CAD model include plicated surface and characteristics, these may result in many difficulties during the numeric simulation and influence the result. Considering the siphonic bedpan?s hole flo channel as puting area, and the difficulty to set up the CAD model in ADINA, so this paper make use of Pro/E to conduct the parameterization model of the siphonic bedpan. The ater arp is 200 mm high, and the pipe diameter in the largest section is 80 mm. Then the modelis imported into ADINA8.3 through IGES data format. In ADINA, e still need to predigest the physics model before adding load and boundary conditions. Detailed information is as follos: Load: velocity method is defined such a volume fraction F, defining the value of the point having fluid as 1, the value of the point having no fluid as 0. Thus, in a mesh unit, the F average value represents the a that fluid contained the unit. If the average value is 1, the mesh is filled ith the fluid, if the average value is 0, then for empty mesh. If the value is beteen 0 and 1, the mesh is free surface mesh. So it has advantages of easy realization, small calculation quantity, high-precision etc, and can handle plex nonlinear problem such as free surface folding, free surface filling ater etc. When the model involves flo theories of the to phases or multi-phase, it introduces the single fluid model to solve problem. Namely, in the ater-air to phase flo field, ater and air obey the same team momentum equation. In the puting area, each controlling volume is filling ith ater and air, and their volume fraction?s addition should be 1, namely, a?aa?1 Among above, ?a? denotes the volume fraction, subscript and ?a? denote ater and air respectively. Once the ater and air?s volume fractions are knon, all their unknon quantity and characteristic parameter can be denoted by average volume fraction. Tracking the ater-air interface can be solved by nether consecutiveequation. ?a?t ?Va?0 Thereinto, ?V? denotes velocity vector.B. Boundary conditions The material property and the boundary conditions are as follos: Gas phase is air, and its density is 1.293 kg/m3, viscosity is 1.7894×10-5 kg/Flushing proces The figure 4 shos floing field distributions at different moment. Figure 4. Distributing of flo at different moment by simulation for the variational section bedpan In the figuresabove, areas in red colour represent ater, areas in navy blue represent air, other colours represent the mixture of ater and air. Contrasting the flo field distribution of the constant section bedpan to the variational section bedpan, e ill found, to the constant section bedpan, pipe?s tiptopduring hile 0-5s, to ater the variational caput hasn?t section gotten bedpan, across ater the caput has already gotten across during 0-1s and in 5.6 s, ater because in hen the arp the ater has floed caput out got pletely. across the pipe?s This mainly tiptop, the siphonic phenomenon happens. Water arp?s outflo increases largely. This makes ater level drop rapidly and reach loest level in arp, and then the siphonic phenomenon stops, ater velocity bees loer, ater that has not gotten across the pipe?s tiptop start to turn back, and finally bee level off. 2) Pressure distribution The figure 5 shos pressure distribution at different moment for the variational section bedpan. In the folloing figures, to the constant section bedpan, the minus pressure is -695.4 Pa, hile to the variational section bedpan, the minus pressure is -1733 Pa, this difference shos the strong function of siphon. Figure 5. Pressure distributing at different moment for the variational section bedpan 3) Velocity distribution As the figure 6 shos, velocity for the variational section bedpan is averagely larger than the velocity for the constant section bedpan, consequently, it provide effective gist for variational section bedpan, it can easily achieve effectively flushing aim pared to the constant section bedpan. Besides, it indirectly indicates that the variational section bedpan can easily achieve the function of saving ater. Figure 6. The velocity distribution of the to kind sections bedpan pipe VI. CONCLUSIONS This paper studied on the structure optimization of the siphonic bedpan?s flo channel, recurringto finite element softare ADINA, three-dimensional steady flo numeric simulation of ater floing in bedpan is carried out, the VOF analysis on siphonic bedpan?s flushing process has also been carried out. The results can help technics designers find out the disfigurement essentially, enhance the precision in the porcelain sanitation field. Further more, it ill shorten the exploiting time and expense of the ne product consumedly, bring remarkable economic benefit to producing enterprise. ACKNOWLEDGMENT America The preferred spelling is ithout an “e” of the ord “acknoledgment” in after the “g”. Avoid the stilted expression, “One of us thanks . . .” Instead, try “R.B.G. thanks”. Put applicable sponsor acknoledgme nts here; DO NOT place them on the first page of your paper or as a footnote. REFERENCES Yue bangguo, “Talking about bedpan?s flushing filth function and saving ater,” Chinaare, 2001 Wu ziniu, The basic elements of puting hydromechanics. Beijing: the Science Press. 2001. 1-8. Hong fangen, “Kinetic object round free surface floing field value simulation and experimentation research,” Doctor Degree thesis. Wuxi, Jiangsu, China: Chinese atercraft science research center. 2001.4. C.W. Hirt, B.D. Nichols. Volume of fluid method for the dynamics of free boundaries. Journal of Computational Physics, 1981, 39:201-225. Lin huzong, Phantasmagoric floing science-multiphase hydromechanics. Beijing: the book concern of Qinghua University, Guangzhou: the book concern of Jinan University. Wang youcheng, Shao min, The theory and numeric method on finite element analysis. Beijing: the book concern of Qinghua University, 1997. 篇四：论文怎样写才能被EI检索论文怎样写才能被EI收录 2016年06月12日星期五上午 10:15 从2002年起《吉林大学学报0253-4827 Applied Mathematics and Mechanics 0890-5487 China Ocean Engineering 1004-5341 China Welding1004-9541 Chinese Journal of Chemical Engineering 1022-4653 Chinese Journal of Electronics 1000-9345 Chinese Journal of Mechanical Engineering 学报网站 1671-7694 Chinese Optics Letters 学报网站 1673-7350 Frontiers of Computer Science in China 期刊网址 1006-6748 High Technology Letters 1674-4799 International Journal of Minerals, Metallurgy and Materials 1004-0579 Journal of Beijing Institute of Technology 学报编辑部 1005-9784 Journal of Central South University of Technology 学报网站 1672-5220 Journal of Donghua University 1005-9113 Journal of Harbin Institute of Technology 1001-6058 Journal of Hydrodynamics 1005-0302 Journal of Materials Science and Technology 1002-0721 Journal of Rare Earths 1674-4926 Journal of Semiconductors 学报编辑部 1007-1172 Journal of Shanghai Jiaotong University 1003-7985 Journal of Southeast University 1004-4132 Journal of Systems Engineering and Electronics 1009-6124 Journal of Systems Science and Complexity 1003-2169 Journal of Thermal Science1000-2413 Journal of Wuhan University of Technology -Materials Science Edition 1673-565X Journal of Zhejiang University SCIENCE A 1674-5264 Mining Science and Technology 1001-0521 Rare Metals 1006-9291 Science in China, Series B: Chemistry 1672-1799 Science in China, Series G: Physics, Astronomy 1005-8885 The Journal of China Universities of Posts and Telemunications 1005-1120 Transactions of Nanjing University of Aeronautics and Astronautics 1003-6326 Transactions of Nonferrous Metals Society of China 1006-4982 Transactions of Tianjin University 1007-0214 Tsinghua Science and Technology Editor Information 1001-1455 爆炸与冲击 0254-0037 北京工业大学学报 1001-5965 北京航空航天大学学报学报编辑部 1001-053X 北京科技大学学报学报编辑部 1001-0645 北京理工大学学报学报编辑部 1007-5321 北京邮电大学学报学报编辑部 1000-1093 兵工学报 1001-4381 材料工程 1005-0299 材料科学与工艺 1009-6264 材料热处理学报学报网站 1005-3093 材料研究学报 1001-1595 测绘学报学报编辑部1007-7294 船舶力学 1000-8608 大连理工大学学报 1004-499X 弹道学报 1000-2383 地球科学学报网站 1005-0388 电波科学学报1000-6753 电工技术学报 1007-449X 电机与控制学报 1000-1026 电力系统自动化学报网站 1006-6047 电力自动化设备 1001-0548 电子科技大学学报 0372-2112 电子学报 1009-5896 电子与信息学报 1005-3026 东北大学学报 1001-0505 东南大学学报 1000-3851 复合材料学报 1003-6520 高电压技术 1000-7555 高分子材料科学与工程 1002-0470 高技术通讯1003-9015 高校化学工程学报1000-5773 高压物理学报 1000-4750 工程力学 0253-231X 工程热物理学报 1001-9731 功能材料学报网站 1006-2793 固体火箭技术0254-7805 固体力学学报 1005-0086 光电子.激光 1000-0593 光谱学与光谱分析 1004-924X 光学精密工程学报网站 0253-2239 光学学报学报网站 0454-5648 硅酸盐学报 1001-2486 国防科技大学学报 1006-7043 哈尔滨工程大学学报学报网站 0367-6234 哈尔滨工业大学学报 0253-360X 焊接学报 1005-5053 航空材料学报1000-8055 航空动力学报编辑部网站 1000-6893 航空学报学报网站 0258-0926 核动力工程 1001-9014 红外与毫米波学报1000-2472 湖南大学学报 1000-565X 华南理工大学学报编辑部网站1671-4512 华中科技大学学报0438-1157 化工学报学报网站1002-0446 机器人学报网站 0577-6686 机械工程学报学报网站1671-5497 吉林大学学报学报编辑部 1003-9775 计算机辅助设计与图形学学报 1006-5911 计算机集成制造系统编辑部网站0254-4164 计算机学报 1000-1239 计算机研究与发展学报网站1007-4708 计算力学学报 1001-246X 计算物理 1007-9629 建筑材料学报 1000-6869 建筑结构学报 1671-7775 江苏大学学报（自然科学版） 1009-3443 解放军理工大学学报（自然科学版） 0412-1961 金属学报 0258-1825 空气动力学学报 1000-8152 控制理论与应用学报网站 1001-0920 控制与决策 0459-1879 力学学报学报网站0253-9993 煤炭学报学报网站1003-6059 模式识别与人工智能1004-0595 摩擦学学报 1672-6030 纳米技术与精密工程 1005-2615 南京航空航天大学学报 1005-9830 南京理工大学学报 1000-0925 内燃机工程 1000-0909 内燃机学报 1002-6819 农业工程学报学报编辑部 1000-1298 农业机械学报学报编辑部 1001-4322 强激光与粒子束学报编辑部 1000-0054 清华大学学报 0253-2409 燃料化学学报 1006-8740 燃烧科学与技术 1000-985X 人工晶体学报无机材料期刊网 1000-9825 软件学报学报编辑部 1006-2467 上海交通大学学报 1000-2618 深圳大学学报（理工版） 0371-0025 声学学报1000-7210 石油地球物理勘探 1000-0747 石油勘探与开发0253-2697 石油学报 1001-8719 石油学报:石油加工学报网站1672-9897 实验流体力学学报网站 1001-6791 水科学进展0559-9350 水利学报学报编辑部 1003-1243 水力发电学报1009-3087 四川大学学报学报编辑部 0254-0096 太阳能学报学报编辑部 0493-2137 天津大学学报学报编辑部 1001-8360 铁道学报1000-436X 通信学报 0253-374X 同济大学学报 1000-131X 土木工程学报学报网站 1674-4764 土木建筑与环境工程学报编辑部1001-4055 推进技术 1000-324X 无机材料学报 1671-8860 武汉大学学报1001-2400 西安电子科技大学学报学报网站 0253-987X 西安交通大学学报 1000-2758 西北工业大学学报 0258-2724 西南交通大学学报学报网站 1002-185X 稀有金属材料与工程 1000-6788 系统工程理论与实践 1001-506X 系统工程与电子技术1007-8827 新型炭材料 1000-6915 岩石力学与工程学报学报网站 1000-4548 岩土工程学报 1000-7598 岩土力学期刊编辑部 0254-3087 仪器仪表学报 1005-0930 应用基础与工程科学学报学报网站 1000-6931 原子能科学技术 1008-973X 浙江大学学报 1672-7126 真空科学与技术学报 1004-6801 振动测试与诊断 1004-4523 振动工程学报1000-3835 振动与冲击学报网站 0258-8013 中国电机工程学报1001-7372 中国公路学报 0258-7025 中国激光学报网站1000-1964 中国矿业大学学报 1673-5005 中国石油大学学报1001-4632 中国铁道科学 1004-0609 中国有色金属学报学报网站1672-7207 中南大学学报（自然科学版）学报网站 0254-4156 自动化学报学报网站篇五：如何判断国际会议论文是否被EI收录★ 如何判断国际会议论文是否被EI收录？如何判断国际会议论文是否被EI收录？可能会遇到这样的情况，有些国际会议说明了EI收录，可到最后却并未收录，让人郁闷至极。

Numerical Simulation of Temperature Field in the CyclonePingyang Xiao a and Zhenwei Zhang bSchool of Mechanical Engineering and Automation, Northeastern University, Shenyang, Liaoning, 110004, Chinaa xpypaper@,b zzw1658@Keywords: Separator, Numerical Simulation, Temperature Field.Abstract. This paper mainly focuses on the numerical simulation of temperature field in the cyclone separation. The authors took advantage of RSM turbulence model of software FLUENT to imitate the temperature field. This thesis puts forward the temperature distribution of the cyclone, and figures out that the overall temperature is 373°C. Temperature difference in different region is less than one centigrade degree with the maximum temperature in the cone part and the minimum temperature in inlet tube and cylinder part of the cyclone, what’s more, the temperature is relatively higher near the wall. The air compression can lead the higher temperature in the lower part, so the cone part has the highest temperature. The higher temperature near the wall is caused by the friction between the wall and flow.IntroductionThis paper mainly focuses on the flow field phenomenon of gas-solid separation process in CLT/A type cyclone separator about the potato granules drying system. The simulation is established based on the discrete coupling model, the assumption of which is that the model needs the constant temperature. It is really necessary to simulate the temperature field of CLT/A type cyclone as the temperature of hot air is relatively high in the drying system and the internal temperature conditions can not be determined.Physical modelThe cylindrical volume is relatively large in the cyclone group of CLT/A 8.4×4 type shown in Fig.1. The cyclone separator is divided into four sub-cylinders, which show symmetrical layout and the structure is identical. Therefore the simulation only focuses on the single cylinder.Fig. 1 Structure group graph of Fig. 2 Three-dimensional solid modelCLT / A 8.0 × 4-type cyclone of the CLT / A-type cycloneThe three-dimensional model can be obtained by taking advantage of powerful modeling capabilities of solid surface of UG about CLT/A type cyclone shown in Fig. 2.Finite element modelThe three-dimensional solid model established by UG can be imported into GAMBIT so as to be meshed. Multiple Boolean operations should be carried out on the solid model in order to be facilitated to mesh in GAMBIT, which can lead to the establishment of two entities form. The overall body of Volom1 is consisted of exhaust volute and exhaust pipe. The overall body of Volom2 is consisted of entrance pipe and cone below the cylinder. Then the model is exported in the .step format, and then the model will be imported into GAMBIT. The total model is shown in Fig. 3. Meshing should be conducted in the several parts of model in order to generate the better structured grid. The operations in GAMBIT can be shown as flowing.(1) Establish the auxiliary plane and split the intake pipe with the Split command.(2) The cylinder can be divided into two parts with a plane parallel to Y-axis at Y=2260mm, theupper of which is ring cylinder and the lower part is cylinder.Fig. 3 Physical model of cyclone in GAMBIT Fig. 4 Mesh diagram of CLT / A-type cycloneThe entire cyclone is divided into four parts: intake pipe, outtake pipe, lower half part of the cylinder and the upper half part of the cylinder. The meshing can be imposed on them separately. Meshing is the premise process of numerical simulation and also the discrete process of calculating region. The number of the grid has nothing to do with the final result according to the theory of CFD, and when the intensity of the grid reaches a certain value, it has little effect on the simulation result by continuing encryption [1]. However, in practice, if the mesh is too sparse, it is difficult to describe some detail in the flow field. What’s more, the computing speed can be greatly affected if the number of the meshing is too large. Therefore the number select of the grids can both guarantee the accuracy requirements and avoid excessive consumption of the system resources [2]. This paper adopts the complex grids according to the complexity of the flow field and variability of local feature. The hexahedral grid can be generated, which is the main structure, by taking advantage of Hex/Wedge-type structured grid and Cooper barrel pattern. This kind of grid matches well with the flow field, and is conductive to process of coupling conditions in the numerical simulation region. The meshing can be drawn as Fig. 4.Boundary conditionsThe gas phase can be simplified in order to facilitate solving the multiphase flow inside the cyclone[3].(1) Gas flow is steady-state in cyclone;(2) The gas flow rate is low( generally less than 30m/s), and the gas can be seen as incompressiblefluid;(3) The inlet air flows evenly, and in a fully developed turbulent state;(4) No gas exhausts from the dust exhaust at the bottom of the cyclone.Set the boundary conditions as following:(1) Inlet boundary: the inlet air temperature is 373.15K, and the density is 1.225 kg/m3. The viscosityis 18.1×10-6 . The entrance speed is known, so the inlet boundary is set as the velocity inlet boundary condition. Assuming that the inlet turbulent is developed fully, and the gas inlet velocity is set as 15 m/s evenly distribution throughout the inlet section. The turbulence intensity is set as I and the hydraulic diameter is set as D. Flow Reynolds number is shown as Eq. 1.4e 61.225150.252R 2.5725101810UD ρµ−××===××. (1) Hydraulic diameter is set as Eq. 2. 220.460.2070.2940.460.207HD ab D a b ××===++. (2)Turbulence Intensity is set as Eq. 3. 1/851/8e 0.16(R )100%0.16(2.5710)7.34%I −−=×=××=.(3) (2) Outlet boundary: outlet boundary is set as outflow boundary. Assuming that the flow condition isin fully developed condition, namely the flow situation can be obtained by the pulling of flow field. The air exhaust can be set as the outflow, and the weight of the flow is set as one. The dust exhaust is set as outflow, and the weight of the flow is set as zero.(3) Wall conditions: take the standard wall function, namely the wall has no-slip boundary [4]. Theroughness parameter of wall is set as 0.5.(4) The overlapping circle is set as interface surface, which connects the exhaust pipe and cylinder.Fig. 5 Total temperature fieldNumerical simulation analysisTemperature distribution at various locations in CLT/A type cyclone can be intuitively obtained through numerical simulation shown in the Fig. 5. The entrance temperature is relatively low, and temperature can increase with moving downward along the cone. The value can reach the highest at the bottom of cone. The exhaust temperature can decrease along the exhaust pipe, but is still higher than inlet air temperature. The temperature change reason is shown as following: the air enters the air intake with the number of 100, and the flow can be compressed by centrifugal force caused by the rotation. In addition, the temperature can be increased due to the friction between the flow and wall. The temperature continues to rise owing to the further impact of compression and friction when reaches the cone wall. The final flow will be excluded through the exhaust pipe with some pressure decrease lower than the cone and bigger than the cylinder and inlet, namely the temperature is center. However the temperature change is small, and the left table stays at 3.73e+2 from start to finish shown from the color column. The temperature is about 100℃ in the cyclone with only less than one temperature change. Therefore temperature change is small.Fig. 6 and Fig. 7 respectively show the temperature distribution in Y=0 section about static and total temperature in CLT/A type cyclone separator. The static temperature distribution has the same situation with the total temperature distribution in the Y=0 cross section in the cyclone, and specific temperature change region inside the cyclone can be clear obtained. The temperature of air intake and cylinder is the lowest with the maximum temperature in the cone part, and the temperature of exhaust pipe stays centre. The exhaust pipe temperature can decrease further. Temperature distribution shows a symmetrical situation in both sides of the exhaust pipe or inside the exhaust pipe in cyclone with only little difference near the wall, which shows the vortex shape. The small difference is caused by the local turbulence accompanied by the rotation flow inside cyclone.Fig. 6 Y=0 Static temperature Fig. 7 Y=0 Total temperatureFig. 8 and Fig. 9 respectively show the temperature distribution in X=0 section about static and total temperature in CLT/A type cyclone separator. Temperature distribution of each parts of the X=0 cross section can be seen clearly in the picture. Internal temperature distribution of X=0 section has the same situation with the total temperature distribution in cyclone. The cylinder part below the exhaust pipe has almost the same temperature distribution with the lower cone compared with the section Y=0 with only obvious difference in the position above the air exhaust, the reason for which is that the asymmetry caused the flow’s entrance from the unilateral line.Fig. 8 X=0 Static temperature Fig. 9 X=0 Total temperatureTemperature distribution can be respectively obtained in the section Z=0.5, Z=0.75, Z=1, Z=1.25, Z=1.5, Z=1.75 and Z=2 in the cyclone shown in Fig. 10, which also shows that temperature near the wall is relatively high, the reason for which is that friction between the flow and wall and compression effect of centrifugal force can lead the enhancement of temperature. Temperature gradient of each cross-section shows circular ring, better symmetry and a certain degree irregularity that can be caused by the different local turbulence.Fig. 10 The temperature distribution on Z = 0.5, 0.75, 1, 1.25, 1.5, 1.75, 2 cross sectionConclusionThis thesis puts forward the temperature distribution of the cyclone with type of CLT/A, and figures out that the overall temperature is about 373°C. Temperature difference in different region is less than one centigrade degree with the maximum temperature in the cone part and the minimum temperature in inlet tube and cylinder part of the cyclone, what’s more, the temperature is relatively higher near the wall. The air compression can lead the higher temperature in the lower part, so the cone part has the maximum temperature which is caused by the strengthen impact of air compression. The higher temperature near the wall is caused by the friction between the wall and flow. The total temperature in the cyclone stays a constant value with almost no change and local difference can be obtained.References[1] F. Boysan, B. Ewan and J. Swithenbank: Experimental and Theoretical Studies of Cyclone Separator Aerodynamics: (Chem E Symp Series, P. 305-320, 1983).[2] W. Q. Tao. Modern Process of Heat Transfer Calculation: (Science Press, 2002).[3] G. L. Gao. Thermal Engineering and Fluid Mechanics: (China Electric Power Press, P. 130-131,China 1997).[4] Y. Mao, L. Pang, X. W. Wang et al. Numerical Simulation of Three-dimensional Turbulence inCyclone: (Petroleum Refining and Chemical Industry, V. 33(2), P. 1-6, China 2002).Advanced Mechanical Design10.4028//AMR.479-481Numerical Simulation of Temperature Field in the Cyclone 10.4028//AMR.479-481.462。

ei会议论文(共3篇)ei会议论文(共3篇)篇一：EI会议论文EI会议论文四大检索系统 SCI、EI、ISTP、ISR是世界四大重要检索系统，其收录文章的状况是评价国家、单位和科研人员的成绩、水平以及进行奖励的重要依据之一。

我国被四大系统收录的论文数量逐年增长。

学校在”1512工程”建设及科技成果奖励方案中均十分重视四大系统，也已成为教师和科研人员提升自己的努力方向。

何为EI 3千到8千元不等。

一般用作：硕士毕业、博士毕业、评副教授、评正教授使用。

作者在国际会议或者国际杂志上发表论文被EI收录后，国内一些权威机构可以出具EI收录证书给作者。

EI类型现在EI数据库的收录的文献只分为两类：会议检索与期刊检索，其判断如下： A 会议论文：Conference article一般来说，期刊论文的质量略高于会议论文。

EI会议与核心的比较A.横向比较（数量级）：一篇EI检索论文，约等于中国国内的核心期刊3-5篇。

B.纵向比较（质量级）：ISTP，属于国际级出版物；核心期刊属于国家级出版物。

C.立体比较（实效性）：高级职称晋升要求本专业相关刊物上公开发表教学、科研论文5篇，其中被SCI、ISTP、EI收录全文收录3篇以上，并撰写15万字以上公开出版发行的专著或教材。

EI会议发表途径金笔杆中心能够帮助解决这个困惑，。

录用时间快，文章质量高，保证入库。

篇二：EI学术论文检索、EI会议论文核心检索入口EI论文检索入口华译网论文翻译专业机构汇集EI检索地址如下，本文后附有华译网EI 论文翻译价格和英文论文外籍校对价格，欢迎大家惠顾。

EI论文检索入口常用网址如下：英特网EI官方网址：/Kns55/brief/Result_CPFD.htm 清华大学图书馆：/service/SCIcenter/eiall.html 《工程索引》（The Engineering Index，简称EI）是美国工程信息公司（Engineering information Inc.）出版的著名工程技术类综合性检索工具。