{"currentpage":1,"firstResult":0,"maxresult":10,"pagecode":5,"pageindex":{"endPagecode":5,"startPagecode":1},"records":[{"abstractinfo":"研究了不同<span style=\"color:red\">电磁</span><span style=\"color:red\">组合</span><span style=\"color:red\">场</span>对AZ61镁合金凝固组织的影响.结果表明,在静磁场作用下,镁合金的凝固组织为等轴晶,晶界上的结晶相成网状分布;在静磁场与工频交流电<span style=\"color:red\">组合</span><span style=\"color:red\">场</span>作用下,其凝固组织与只施加静磁场时类似,基本为等轴晶,但由于交流电的施加晶粒明显得到细化,晶界上结晶相的网状结构也变得细小;而在镁合金凝固过程中同时施加静磁场和直流电流<span style=\"color:red\">组合</span><span style=\"color:red\">场</span>时,由于<span style=\"color:red\">组合</span><span style=\"color:red\">场</span>产生的熔体内部的定向力作用的结果,凝固组织主要为蔷薇状晶粒,组织得到明显的净化,其晶界上结晶相的网状结构彻底消失,以不连续的薄条状和点状形态分布.","authors":[{"authorName":"许光明","id":"85019d1c-dc1c-4655-86d9-96c2a4c8e78c","originalAuthorName":"许光明"},{"authorName":"李金涛","id":"ea191c3f-0a7a-4125-869b-50c79be56a62","originalAuthorName":"李金涛"},{"authorName":"崔建忠","id":"f50f4a11-a4a7-4c45-a122-2a7bc6892bd4","originalAuthorName":"崔建忠"}],"doi":"","fpage":"2195","id":"c2439ad5-4a53-4395-ba86-3990bbde8086","issue":"12","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":"06284316-94d0-44cf-8134-5341e890fdbe","keyword":"AZ61镁合金","originalKeyword":"AZ61镁合金"},{"id":"3ae31c10-e5cc-4778-94f8-d621358e4cf3","keyword":"<span style=\"color:red\">电磁</span><span style=\"color:red\">组合</span><span style=\"color:red\">场</span>","originalKeyword":"电磁组合场"},{"id":"d4f8d511-fa17-4e68-b65c-03a8037cb3fc","keyword":"结晶相","originalKeyword":"结晶相"}],"language":"zh","publisherId":"xyjsclygc200912028","title":"<span style=\"color:red\">电磁</span><span style=\"color:red\">组合</span><span style=\"color:red\">场</span>对镁合金凝固组织的影响","volume":"38","year":"2009"},{"abstractinfo":"利用坐标变换理论,推导出椭圆形和梯形变换空间的<span style=\"color:red\">电磁</span>参数分布,设计出<span style=\"color:red\">组合</span>型目标的<span style=\"color:red\">电磁</span>超材料隐身斗篷.在频率为400MHz的平面横电波(TE 波)垂直入射的条件下,对该斗篷的隐身性能进行数值仿真分析.结果表明,在隐身斗篷的作用下,目标模型内部几乎没有<span style=\"color:red\">电磁</span>波进入,斗篷以外的<span style=\"color:red\">电磁</span>场也没有明显的变化,这些现象与理论预测的结果基本一致,体现了所设计的斗篷良好的隐身性能,由此验证了根据坐标变换设计的超材料,在理论上具有控制<span style=\"color:red\">电磁</span>波传播路径并且不改变外界波<span style=\"color:red\">场</span>的特性.","authors":[{"authorName":"刘冶","id":"574b92ef-fc44-4558-99d4-c7ef8620700f","originalAuthorName":"刘冶"},{"authorName":"李竹影","id":"4b2d3a5e-404f-4c73-96cc-8a99263419ac","originalAuthorName":"李竹影"},{"authorName":"张旺洲","id":"7275a84b-6033-4cc5-8982-b7de47728519","originalAuthorName":"张旺洲"},{"authorName":"孙禹宏","id":"dc82f5b5-873e-4c46-a14d-093a517030af","originalAuthorName":"孙禹宏"}],"doi":"10.3969/j.issn.1001-9731.2013.15.023","fpage":"2235","id":"54678814-258b-43eb-903f-f03cb90080d0","issue":"15","journal":{"abbrevTitle":"GNCL","coverImgSrc":"journal/img/cover/GNCL.jpg","id":"33","issnPpub":"1001-9731","publisherId":"GNCL","title":"功能材料"},"keywords":[{"id":"89130e45-6141-4397-8c49-0b9454b98b62","keyword":"超材料","originalKeyword":"超材料"},{"id":"160ee707-97b1-4145-8178-0a31ce1ddcbd","keyword":"坐标变换","originalKeyword":"坐标变换"},{"id":"a6978497-b498-427a-96c5-53e5a898484b","keyword":"隐身","originalKeyword":"隐身"},{"id":"90141ff0-4c40-4acc-874c-1c8b377dda49","keyword":"斗篷","originalKeyword":"斗篷"},{"id":"8e4f8720-ff8d-4c5d-b900-360366e03f61","keyword":"<span style=\"color:red\">电磁</span>波","originalKeyword":"电磁波"}],"language":"zh","publisherId":"gncl201315023","title":"<span style=\"color:red\">组合</span>型<span style=\"color:red\">电磁</span>隐身斗篷的超材料设计与仿真","volume":"44","year":"2013"},{"abstractinfo":"<span style=\"color:red\">组合</span><span style=\"color:red\">电磁</span>场是指通过2个或者2个以上励磁线圈,产生2个或2个以上交互作用的<span style=\"color:red\">电磁</span>场,并将交互作用的<span style=\"color:red\">电磁</span>场作用于材料制备过程.<span style=\"color:red\">组合</span><span style=\"color:red\">电磁</span>场在金属凝固过程中的应用可为开发新材料、优化材料制备工艺、提高金属材料制品的综合质量和解决金属材料在制备过程中的技术难题提供新的手段和方法.<span style=\"color:red\">组合</span>磁场在材料凝固过程中的应用必将成为材料研究领域的新方向.","authors":[{"authorName":"朱庆丰","id":"bea4c6d5-5f29-45f8-bbf4-b6aabb05fbd0","originalAuthorName":"朱庆丰"},{"authorName":"赵志浩","id":"59001798-add7-45f2-8548-52a11ea3d690","originalAuthorName":"赵志浩"},{"authorName":"王静","id":"15169f2a-e9c1-4e86-809f-ae71304e201a","originalAuthorName":"王静"},{"authorName":"崔建忠","id":"69a32c6e-dda0-43e9-b2cc-0635e281951b","originalAuthorName":"崔建忠"}],"doi":"","fpage":"109","id":"7519d0cc-52db-458f-97e4-1702ae73bdd1","issue":"5","journal":{"abbrevTitle":"CLDB","coverImgSrc":"journal/img/cover/CLDB.jpg","id":"8","issnPpub":"1005-023X","publisherId":"CLDB","title":"材料导报"},"keywords":[{"id":"0630b658-11ea-498e-a8ff-9d290e23460a","keyword":"<span style=\"color:red\">组合</span>磁场","originalKeyword":"组合磁场"},{"id":"4a396bfa-d9f1-4c08-93ea-610fab338665","keyword":"<span style=\"color:red\">电磁</span>悬浮","originalKeyword":"电磁悬浮"},{"id":"7ee06e0b-2905-4c27-b285-25a24575845c","keyword":"<span style=\"color:red\">电磁</span>振荡","originalKeyword":"电磁振荡"},{"id":"f190150b-44d7-4739-b92f-cf50da7c31fd","keyword":"异相位<span style=\"color:red\">电磁</span>连铸","originalKeyword":"异相位电磁连铸"}],"language":"zh","publisherId":"cldb200705028","title":"<span style=\"color:red\">组合</span><span style=\"color:red\">电磁</span>场在材料凝固过程中的应用和发展","volume":"21","year":"2007"},{"abstractinfo":"利用经典<span style=\"color:red\">电磁</span>理论导出光<span style=\"color:red\">场</span>中线性动量的守恒定律,并获得光散射力和梯度力的一般表达式,进而解释光<span style=\"color:red\">场</span>辐射压及尺寸远小于光波长的任意形状的生物微粒子在激光光<span style=\"color:red\">场</span>中所受的散射力和梯度力.理论分析表明光散射力是由于偶极子散射导致<span style=\"color:red\">电磁</span>波动量变化产生,而梯度力为作用在感应偶极子上的洛伦兹力,激光对微粒的作用力与光束束腰半径、粒子的大小、粒子及周围媒质的折射率和激光功率等系统参数的有关.","authors":[{"authorName":"李忠明","id":"7aefae35-d767-470d-8b5b-3ea5f86f0e99","originalAuthorName":"李忠明"},{"authorName":"张镇西","id":"7f885463-1b00-4d53-bd8c-40943dc816f4","originalAuthorName":"张镇西"}],"doi":"10.3969/j.issn.1007-5461.2007.02.016","fpage":"211","id":"28f08c9a-560e-4cff-88fb-a381c078ee98","issue":"2","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":"c2685520-5924-4356-a77d-328971935bd0","keyword":"光的<span style=\"color:red\">电磁</span>理论","originalKeyword":"光的电磁理论"},{"id":"78f79e88-a211-4a34-9da1-8cdf38ac09cf","keyword":"光<span style=\"color:red\">场</span>辐射力","originalKeyword":"光场辐射力"},{"id":"542eb8ee-6455-4c69-846e-84b8f445afbd","keyword":"理论分析","originalKeyword":"理论分析"},{"id":"1d1e0372-2ab6-4114-96aa-5493de50cc6f","keyword":"生物细胞","originalKeyword":"生物细胞"}],"language":"zh","publisherId":"lzdzxb200702016","title":"光<span style=\"color:red\">场</span>力的<span style=\"color:red\">电磁</span>理论分析","volume":"24","year":"2007"},{"abstractinfo":"采用数值模拟方法分析了<span style=\"color:red\">电磁</span>连铸复合式结晶器内的流<span style=\"color:red\">场</span>.对静磁场磁感应强度不同时<span style=\"color:red\">组合</span>磁场下的流<span style=\"color:red\">场</span>进行了比较,在此基础上,分析了<span style=\"color:red\">电磁</span>连铸复合式结晶器的工作原理.分析结果表明:<span style=\"color:red\">电磁</span>连铸复合式结晶器不仅具有<span style=\"color:red\">电磁</span>制动和软接触两种功能,而且能够控制弯月面区域的速度,使其保持在合适的范围内.从而有效地防止了<span style=\"color:red\">电磁</span>制动结晶器在需要较大制动强度时对弯月面制动过死及软接触结晶器弯月面波动剧烈易引起卷渣的弊端.","authors":[{"authorName":"钱忠东","id":"8931840e-c31b-4b7d-8412-ab2535b07b3b","originalAuthorName":"钱忠东"},{"authorName":"李本文","id":"07da8fc2-b7bd-4458-86ef-c7e1198d1a6c","originalAuthorName":"李本文"},{"authorName":"李东辉","id":"dec07403-1b95-407a-8d95-880cc6a2ef28","originalAuthorName":"李东辉"},{"authorName":"王恩刚","id":"9d617e5c-302e-45d0-9e7c-77b6073ea9d6","originalAuthorName":"王恩刚"},{"authorName":"赫冀成","id":"c761ab5d-1769-4dfb-a325-83b2a169a9de","originalAuthorName":"赫冀成"}],"categoryName":"|","doi":"","fpage":"1223","id":"d78ec408-f6b8-4d23-bb63-b4bd6c298a4c","issue":"11","journal":{"abbrevTitle":"JSXB","coverImgSrc":"journal/img/cover/JSXB.jpg","id":"48","issnPpub":"0412-1961","publisherId":"JSXB","title":"金属学报"},"keywords":[{"id":"368711ac-7c0a-4523-a195-7999c6a0aaaa","keyword":"连铸","originalKeyword":"连铸"},{"id":"9efc4a84-ab60-423c-8116-8a21cf8e3f6d","keyword":"null","originalKeyword":"null"},{"id":"0d5c3f58-0656-4815-94a0-108ecdfd9fdc","keyword":"null","originalKeyword":"null"}],"language":"zh","publisherId":"0412-1961_2001_11_5","title":"<span style=\"color:red\">电磁</span>连铸复合式结晶器内钢液流<span style=\"color:red\">场</span>的数值模拟","volume":"37","year":"2001"},{"abstractinfo":"采用数值模拟方法分析了<span style=\"color:red\">电磁</span>连铸复合式结晶器内的流<span style=\"color:red\">场</span>.对静磁场磁感应强度不同时<span style=\"color:red\">组合</span>磁场下的流<span style=\"color:red\">场</span>进行了比较,在此基础上,分析了<span style=\"color:red\">电磁</span>连铸复合式结晶器的工作原理.分析结果表明:<span style=\"color:red\">电磁</span>连铸复合式结晶器不仅具有<span style=\"color:red\">电磁</span>制动和软接触两种功能,而且能够控制弯月面区域的速度,使其保持在合适的范围内.从而有效地防止了<span style=\"color:red\">电磁</span>制动结晶器在需要较大制动强度时对弯月面制动过死及软接触结晶器弯月面波动剧烈易引起卷渣的弊端.\n","authors":[{"authorName":"钱忠东","id":"6d8782dd-4f21-4e21-ab4f-88a304ba1cf1","originalAuthorName":"钱忠东"},{"authorName":"李本文","id":"cd7dd809-5ff6-4fc3-b7eb-bdfed916714a","originalAuthorName":"李本文"},{"authorName":"李东辉","id":"871ec942-643a-4123-b12f-8c628de535dd","originalAuthorName":"李东辉"},{"authorName":"王恩刚","id":"c6594bd4-71f1-4029-a155-7a6c96b11db7","originalAuthorName":"王恩刚"},{"authorName":"赫冀成","id":"95de1f6f-e47f-4201-b091-981b5a63cc59","originalAuthorName":"赫冀成"}],"doi":"10.3321/j.issn:0412-1961.2001.11.019","fpage":"1223","id":"500e6373-7e9c-4996-afb2-1f31c05aef70","issue":"11","journal":{"abbrevTitle":"JSXB","coverImgSrc":"journal/img/cover/JSXB.jpg","id":"48","issnPpub":"0412-1961","publisherId":"JSXB","title":"金属学报"},"keywords":[{"id":"4b25bd53-dffb-4a80-a15c-694678ffe005","keyword":"连铸","originalKeyword":"连铸"},{"id":"74d23822-e938-4a1a-b41b-b4a47deeaaca","keyword":"复合式结晶器","originalKeyword":"复合式结晶器"},{"id":"c61b6f5a-2a7a-4a34-b9db-155205da4dc1","keyword":"钢液流<span style=\"color:red\">场</span>","originalKeyword":"钢液流场"},{"id":"cd860a45-5f45-41ba-8c8f-7b1433adac57","keyword":"数值模拟","originalKeyword":"数值模拟"}],"language":"zh","publisherId":"jsxb200111019","title":"<span style=\"color:red\">电磁</span>连铸复合式结晶器内钢液流<span style=\"color:red\">场</span>的数值模拟","volume":"37","year":"2001"},{"abstractinfo":"对圆坯连铸结晶器<span style=\"color:red\">电磁</span>搅拌<span style=\"color:red\">电磁</span>场及流<span style=\"color:red\">场</span>进行了数值模拟.分析了不同搅拌频率对结晶器内<span style=\"color:red\">电磁</span>场及流<span style=\"color:red\">场</span>分布的影响,得出了<span style=\"color:red\">电磁</span>场及流<span style=\"color:red\">场</span>特性与搅拌频率的关系.研究表明搅拌频率的变化对<span style=\"color:red\">电磁</span>场及流<span style=\"color:red\">场</span>的影响比较大,采用合适的<span style=\"color:red\">电磁</span>搅拌频率可以在连铸坯内获得较大的<span style=\"color:red\">电磁</span>搅拌强度.","authors":[{"authorName":"王学兵","id":"8bc3bb1b-e3ba-40a3-82a2-c1b569f55401","originalAuthorName":"王学兵"},{"authorName":"胡坤太","id":"7f69050f-de5a-4e13-b3bb-b3e9dcffbcbf","originalAuthorName":"胡坤太"},{"authorName":"仇圣桃","id":"5a23f910-a554-4349-a460-255399f5d49b","originalAuthorName":"仇圣桃"},{"authorName":"任子平","id":"4b161df6-0e56-497f-87cd-724049423c1c","originalAuthorName":"任子平"}],"doi":"","fpage":"38","id":"cb495198-754a-42e9-be84-b4c4d82cfa8b","issue":"2","journal":{"abbrevTitle":"LZ","coverImgSrc":"journal/img/cover/LZ.jpg","id":"52","issnPpub":"1005-4006","publisherId":"LZ","title":"连铸"},"keywords":[{"id":"1608818b-4df6-439b-b516-1912b642f3e4","keyword":"结晶器","originalKeyword":"结晶器"},{"id":"c63dbf01-da97-4fac-a6ec-730932a7f3f9","keyword":"<span style=\"color:red\">电磁</span>搅拌","originalKeyword":"电磁搅拌"},{"id":"d41b5e51-2069-483e-a168-0f9f2bed8a23","keyword":"频率","originalKeyword":"频率"},{"id":"5c9937da-8712-444d-8df9-e865824173a5","keyword":"<span style=\"color:red\">电磁</span>场","originalKeyword":"电磁场"},{"id":"fbf0892e-bd8f-464c-af85-136567fc4976","keyword":"流<span style=\"color:red\">场</span>","originalKeyword":"流场"}],"language":"zh","publisherId":"lz200802012","title":"圆坯连铸结晶器<span style=\"color:red\">电磁</span>搅拌<span style=\"color:red\">电磁</span>场、流<span style=\"color:red\">场</span>的数值模拟","volume":"","year":"2008"},{"abstractinfo":"建立了板坯结晶器<span style=\"color:red\">电磁</span>搅拌过程<span style=\"color:red\">电磁</span>场与流<span style=\"color:red\">场</span>计算的三维数学模型,采用SIMPLER方法对2对极和4对极条件下的<span style=\"color:red\">电磁</span>场与流<span style=\"color:red\">场</span>进行了数值求解.结果表明:磁感应强度B和<span style=\"color:red\">电磁</span>力F都呈现出关于结晶器中心对称的规律;结晶器两侧每一对N、S极之间的水平面内,<span style=\"color:red\">电磁</span>力都呈现圆周状分布的规律;板坯宽面边缘的<span style=\"color:red\">电磁</span>力较大,而板坯窄面边缘和中心区域的<span style=\"color:red\">电磁</span>力较小;与4对极相比,2对极产生的磁感应强度和<span style=\"color:red\">电磁</span>力大,钢液的流速大,搅拌强度大;无结晶器<span style=\"color:red\">电磁</span>搅拌时,铸坯边缘的纵断面的流场主要分成四个回流区;而有结晶器<span style=\"color:red\">电磁</span>搅拌时,左侧的两个回流区基本消失,右侧两个回流区减小.","authors":[{"authorName":"陈荣","id":"f07ab9bc-1f7b-4470-b1c1-b9a9f45d8840","originalAuthorName":"陈荣"},{"authorName":"沈厚发","id":"e1984bd9-f152-4586-9ad8-fab4d9f83db0","originalAuthorName":"沈厚发"}],"doi":"","fpage":"1","id":"578861d4-c876-4cd9-9c9f-df54a7706bd8","issue":"3","journal":{"abbrevTitle":"LZ","coverImgSrc":"journal/img/cover/LZ.jpg","id":"52","issnPpub":"1005-4006","publisherId":"LZ","title":"连铸"},"keywords":[{"id":"095f2a33-ca48-4e2b-8d0a-694e13c974c0","keyword":"板坯连铸","originalKeyword":"板坯连铸"},{"id":"74732df7-0ff0-47fd-b555-1c1f5016a72a","keyword":"结晶器","originalKeyword":"结晶器"},{"id":"e1132929-a664-41ad-b697-4832029fa59a","keyword":"<span style=\"color:red\">电磁</span>搅拌","originalKeyword":"电磁搅拌"},{"id":"192a5aa2-f214-4b8d-ab8d-5ee3206e87fb","keyword":"流<span style=\"color:red\">场</span>","originalKeyword":"流场"},{"id":"a282f0f0-0a12-4325-90ee-72e3bedb5c89","keyword":"数值模拟","originalKeyword":"数值模拟"}],"language":"zh","publisherId":"lz201003001","title":"板坯结晶器<span style=\"color:red\">电磁</span>搅拌<span style=\"color:red\">电磁</span>场与流<span style=\"color:red\">场</span>的数值模拟","volume":"","year":"2010"},{"abstractinfo":"建立了板坯结晶器<span style=\"color:red\">电磁</span>搅拌过程<span style=\"color:red\">电磁</span>场与流<span style=\"color:red\">场</span>计算的三维数学模型，采用SIMPLER方法对2对极和4对极条件下的<span style=\"color:red\">电磁</span>场与流<span style=\"color:red\">场</span>进行了数值求解。结果表明，磁感应强度B和<span style=\"color:red\">电磁</span>力F都呈现出关于结晶器中心对称的规律；结晶器两侧每一对N、S极之间的水平面内，<span style=\"color:red\">电磁</span>力都呈现圆周状分布的规律；板坯宽面边缘的<span style=\"color:red\">电磁</span>力较大，而板坯窄面边缘和中心区域的<span style=\"color:red\">电磁</span>力较小；与4对极相比，2对极产生的磁感应强度和<span style=\"color:red\">电磁</span>力大，钢液的流速大，搅拌强度大；无结晶器<span style=\"color:red\">电磁</span>搅拌时，铸坯边缘的纵断面的流场主要分成四个回流区；而有结晶器<span style=\"color:red\">电磁</span>搅拌时，左侧的两个回流区基本消失，右侧两个回流区减小。","authors":[{"authorName":"陈荣\t沈厚发","id":"80825e4c-bda5-46e3-ae8b-3ec4af0cbf6f","originalAuthorName":"陈荣\t沈厚发"}],"categoryName":"|","doi":"","fpage":"1","id":"8931e7b2-ca2c-4ddb-a1c2-7c29213cd8b9","issue":"3","journal":{"abbrevTitle":"LZ","coverImgSrc":"journal/img/cover/LZ.jpg","id":"52","issnPpub":"1005-4006","publisherId":"LZ","title":"连铸"},"keywords":[{"id":"38913ced-1603-46e9-84f9-a026517bad0e","keyword":"板坯连铸;结晶器;<span style=\"color:red\">电磁</span>搅拌;流<span style=\"color:red\">场</span>;数值模拟","originalKeyword":"板坯连铸;结晶器;电磁搅拌;流场;数值模拟"}],"language":"zh","publisherId":"1005-4006_2010_3_9","title":"板坯结晶器<span style=\"color:red\">电磁</span>搅拌<span style=\"color:red\">电磁</span>场与流<span style=\"color:red\">场</span>的数值模拟","volume":"1","year":"2010"},{"abstractinfo":"采用数值模拟的方法对<span style=\"color:red\">电磁</span>净化中间包内钢液的流动特征进行了模拟研究.结果表明:旋转室内的钢液在<span style=\"color:red\">电磁</span>力作用下产生水平旋转流动,促进了夹杂物的碰撞、聚合及上浮;旋转室的旋转切向出流以一定角度进入分配室内,所形成的偏流引起钢液流动的非对称性,易在分配室内形成水平环流状流动特征.分配室内设置T形坝控流装置可减轻流<span style=\"color:red\">场</span>结构的非对称性,分配室内的流动更为均匀.","authors":[{"authorName":"赵利荣","id":"57e457d0-7813-4296-9462-edfd4efb759c","originalAuthorName":"赵利荣"},{"authorName":"王赟","id":"4cd60382-e1b8-4f71-a61a-b8eee8942d8b","originalAuthorName":"王赟"},{"authorName":"钟云波","id":"51ada530-59c9-47cd-990c-53eb3ef67d4e","originalAuthorName":"钟云波"},{"authorName":"王贺利","id":"56567eeb-09f9-4988-b706-35c0459fd705","originalAuthorName":"王贺利"},{"authorName":"王保军","id":"2427e1bf-4733-43fb-b65e-3bf1338baf5c","originalAuthorName":"王保军"},{"authorName":"雷作胜","id":"2a7c316f-5907-4170-a366-776fef0ce7d1","originalAuthorName":"雷作胜"},{"authorName":"任维丽","id":"78d0397e-19a3-4299-b9e1-a43011fa8488","originalAuthorName":"任维丽"}],"doi":"10.3969/j.issn.1001-7208.2008.06.010","fpage":"46","id":"6126be40-dce0-45a9-a0a4-1ff3e976a454","issue":"6","journal":{"abbrevTitle":"SHJS","coverImgSrc":"journal/img/cover/SHJS.jpg","id":"59","issnPpub":"1001-7208","publisherId":"SHJS","title":"上海金属"},"keywords":[{"id":"e869e2f5-cc22-4159-bf51-7b9fc544a891","keyword":"连铸中间包","originalKeyword":"连铸中间包"},{"id":"e061cf06-4196-4cf2-8feb-04219dcc8b63","keyword":"<span style=\"color:red\">电磁</span>净化","originalKeyword":"电磁净化"},{"id":"d47d5a48-66a1-49cf-b832-517cd5c0aa09","keyword":"流<span style=\"color:red\">场</span>","originalKeyword":"流场"},{"id":"b919cb50-4974-47e2-a645-6fe7ae77ecb4","keyword":"数值模拟","originalKeyword":"数值模拟"}],"language":"zh","publisherId":"shjs200806010","title":"<span style=\"color:red\">电磁</span>净化中间包内流<span style=\"color:red\">场</span>的数值模拟","volume":"30","year":"2008"}],"totalpage":1114,"totalrecord":11138}