{"currentpage":1,"firstResult":0,"maxresult":10,"pagecode":5,"pageindex":{"endPagecode":5,"startPagecode":1},"records":[{"abstractinfo":"根据改进分析型嵌入原子模型(MAEAM),通过计算钒的总能量随温度的变化关系确定其熔点为2160±10 K,与实验值(2175 K)一致.运用<span style=\"color:red\">分子</span><span style=\"color:red\">动力学</span><span style=\"color:red\">方法</span>(<span style=\"color:red\">MD</span>)从原子面密度函数、面结构因子、面径向分布函数三个方面研究了V(111)晶面的预熔现象和熔化情况,发现V(111)面在800 K左右开始出现预熔.","authors":[{"authorName":"阳喜元","id":"65cb1c41-93ef-46f7-be84-0bfe3daab678","originalAuthorName":"阳喜元"},{"authorName":"袁晓俭","id":"e393805e-c81d-4d59-822f-0c9c2d615543","originalAuthorName":"袁晓俭"},{"authorName":"胡望宇","id":"3c6371b5-46a6-4767-b6ac-bef197a40c8f","originalAuthorName":"胡望宇"}],"doi":"","fpage":"562","id":"8d6f04bb-91a0-4854-a366-06f713d7c28a","issue":"4","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":"abc904ec-8a9b-4b13-abb0-7df11bfcc85e","keyword":"预熔","originalKeyword":"预熔"},{"id":"ccb7489f-58cd-45ef-bb56-c1bed8b0a0db","keyword":"熔化","originalKeyword":"熔化"},{"id":"09a9f071-b55d-4781-b286-329a92dbe0a1","keyword":"V(111)面","originalKeyword":"V(111)面"},{"id":"5b3f1370-3c92-4215-807e-6ad944fe9a23","keyword":"MAEAM","originalKeyword":"MAEAM"},{"id":"1879ca0b-0fb4-4233-9a25-7095712a163a","keyword":"<span style=\"color:red\">分子</span><span style=\"color:red\">动力学</span><span style=\"color:red\">方法</span>(<span style=\"color:red\">MD</span>)","originalKeyword":"分子动力学方法(MD)"}],"language":"zh","publisherId":"xyjsclygc200604013","title":"用<span style=\"color:red\">分子</span><span style=\"color:red\">动力学</span>模拟研究V(111)晶面的熔化机理","volume":"35","year":"2006"},{"abstractinfo":"<span style=\"color:red\">分子</span><span style=\"color:red\">动力学</span>(<span style=\"color:red\">MD</span>)作为一种成熟的微观模拟<span style=\"color:red\">方法</span>,在微观研究领域已经得到广泛应用.耗散粒子<span style=\"color:red\">动力学</span>(DPD)是以<span style=\"color:red\">MD</span>为基础衍生出的介观模拟<span style=\"color:red\">方法</span>,突破了<span style=\"color:red\">MD</span>对计算能力要求过高的限制,实现了更大尺度上的模拟.在对1873K液态纯铁进行<span style=\"color:red\">MD</span>模拟的基础上,将<span style=\"color:red\">MD</span>体系与DPD体系进行了对应,实现了在液态纯铁体系中进行DPD模拟.","authors":[{"authorName":"沈通","id":"580639f9-963e-4533-9c0f-204cce853784","originalAuthorName":"沈通"},{"authorName":"吴永全","id":"dde9a231-1c37-443e-b4d5-ef7c0d18ea86","originalAuthorName":"吴永全"},{"authorName":"蒋国昌","id":"85f0a490-b5ad-4ee9-addd-3ce603647bb3","originalAuthorName":"蒋国昌"}],"doi":"10.3969/j.issn.1001-7208.2008.06.006","fpage":"23","id":"b207f8e7-f5a9-414b-a950-c5662ce08a62","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":"1e44155d-7f2b-4f30-a6b2-7cb341c91067","keyword":"液态纯铁","originalKeyword":"液态纯铁"},{"id":"21d3a9df-129a-4cc9-b748-6b7ce9bd473d","keyword":"<span style=\"color:red\">分子</span><span style=\"color:red\">动力学</span>","originalKeyword":"分子动力学"},{"id":"475c12f6-2fe2-45e1-bf01-d537214172bc","keyword":"耗散粒子<span style=\"color:red\">动力学</span>","originalKeyword":"耗散粒子动力学"}],"language":"zh","publisherId":"shjs200806006","title":"1873K液态纯铁的<span style=\"color:red\">分子</span><span style=\"color:red\">动力学</span>和耗散粒子<span style=\"color:red\">动力学</span>研究","volume":"30","year":"2008"},{"abstractinfo":"采用<span style=\"color:red\">分子</span><span style=\"color:red\">动力学</span>模拟<span style=\"color:red\">方法</span>,应用Buckingham经验势模型,模拟纤锌矿相GaN的薄膜晶格生长.研究了GaN薄膜生长的早期阶段的形貌特点、生长规律、表面结构及<span style=\"color:red\">动力学</span>特性.模拟发现,N原子与Ga原子按照晶格特征吸附在衬底上,作层状分布趋势并且薄膜层从下到上晶态特征逐渐减弱.观察每层沉积原子数、空位比、沉积原子团簇质心高度与沉积原子均方位移随时间的变化规律,发现了随着时间步数增加,原子团簇逐渐达到稳定,在5000步时前3层都达到了较稳定状态,且N原子比Ga原子能更快地找到平衡位置.","authors":[{"authorName":"陈智辉","id":"f3289930-4c1e-4075-b590-ad5e4c667a44","originalAuthorName":"陈智辉"},{"authorName":"俞重远","id":"cf21cf38-f11f-4b18-a418-3ca906bb3219","originalAuthorName":"俞重远"},{"authorName":"芦鹏飞","id":"db11c1d4-4ed6-4c57-ac51-d71650cdf281","originalAuthorName":"芦鹏飞"},{"authorName":"刘玉敏","id":"c26b7887-3a39-43f2-9c98-05cc022f928a","originalAuthorName":"刘玉敏"},{"authorName":"王永钢","id":"7623f3d2-38e4-4388-91d9-14d4cfc38215","originalAuthorName":"王永钢"}],"doi":"","fpage":"2045","id":"7dd0b616-16a4-443d-8dc3-26c839d46d18","issue":"12","journal":{"abbrevTitle":"GNCL","coverImgSrc":"journal/img/cover/GNCL.jpg","id":"33","issnPpub":"1001-9731","publisherId":"GNCL","title":"功能材料"},"keywords":[{"id":"49a70d11-7936-4ffd-8469-da3b12216fde","keyword":"<span style=\"color:red\">分子</span><span style=\"color:red\">动力学</span>模拟","originalKeyword":"分子动力学模拟"},{"id":"3bdd4c05-41af-474e-8772-2994c54da895","keyword":"薄膜生长","originalKeyword":"薄膜生长"},{"id":"d390ebff-3e80-42af-8a5e-741286f24125","keyword":"Buckingham势","originalKeyword":"Buckingham势"},{"id":"ea348e29-7ece-4a42-83ab-2b255b55e8d8","keyword":"GaN","originalKeyword":"GaN"}],"language":"zh","publisherId":"gncl200812032","title":"<span style=\"color:red\">分子</span><span style=\"color:red\">动力学</span><span style=\"color:red\">方法</span>模拟GaN薄膜生长","volume":"39","year":"2008"},{"abstractinfo":"主要研究了利用<span style=\"color:red\">分子</span><span style=\"color:red\">动力学</span><span style=\"color:red\">方法</span>(<span style=\"color:red\">MD</span>)模拟等离子体与材料表面相互作用过程时<span style=\"color:red\">分子</span><span style=\"color:red\">动力学</span><span style=\"color:red\">方法</span>的参数对模拟结果的影响.详细分析了Berendsen热浴的应用时间、耦合强度和模拟时间量(单个轨迹的作用时间、弛豫时间)对模拟结果的影响,结果表明,热浴的应用时间对模拟结果的影响很大,而其它参数对模拟结果没有太大的影响.","authors":[{"authorName":"秦尤敏","id":"b24944a0-34ea-4cd7-b9fd-686a95f355d7","originalAuthorName":"秦尤敏"},{"authorName":"吕晓丹","id":"9083d726-268e-4f8b-8db7-b8320cfaf27a","originalAuthorName":"吕晓丹"},{"authorName":"宁建平","id":"a7eb8baa-36ff-43c9-aaa3-cb441fb3428c","originalAuthorName":"宁建平"},{"authorName":"张利纯","id":"8a7a6344-0618-4dfd-b3b3-e63ca6c62270","originalAuthorName":"张利纯"},{"authorName":"赵成利","id":"3d829bf5-ef77-418c-8fbd-805f19e5c83b","originalAuthorName":"赵成利"},{"authorName":"贺平逆","id":"165764cf-5d36-4374-867e-0dfe793a4056","originalAuthorName":"贺平逆"},{"authorName":"","id":"b7cd2f4e-5c75-424f-8042-97c1154567ce","originalAuthorName":""},{"authorName":"苟富君","id":"48f1040f-49f8-444b-a08e-bf343141ff8a","originalAuthorName":"苟富君"}],"doi":"","fpage":"257","id":"d729d950-a0a2-4943-8d1b-2c330b01ac10","issue":"z2","journal":{"abbrevTitle":"CLDB","coverImgSrc":"journal/img/cover/CLDB.jpg","id":"8","issnPpub":"1005-023X","publisherId":"CLDB","title":"材料导报"},"keywords":[{"id":"0463fa75-f6b9-4c6d-b5cf-62226ace94b0","keyword":"<span style=\"color:red\">分子</span><span style=\"color:red\">动力学</span>","originalKeyword":"分子动力学"},{"id":"e46d3c75-1856-482b-9ee1-24ca6ae09bb2","keyword":"热浴","originalKeyword":"热浴"},{"id":"714f0f5a-93fc-4f38-a832-be307b3dd25a","keyword":"弛豫","originalKeyword":"弛豫"},{"id":"4ed3aadf-5d98-48f5-8536-713bab0ed860","keyword":"刻蚀","originalKeyword":"刻蚀"}],"language":"zh","publisherId":"cldb2009z2078","title":"<span style=\"color:red\">分子</span><span style=\"color:red\">动力学</span><span style=\"color:red\">方法</span>的模拟参数对结果的影响","volume":"23","year":"2009"},{"abstractinfo":"采用<span style=\"color:red\">动力学</span><span style=\"color:red\">方法</span>严格推导了A-Bf-1型逐步反应产物的<span style=\"color:red\">分子</span>量分布函数,结果与Flory通过概率算法所得的<span style=\"color:red\">分子</span>量分布函数完全一致.","authors":[{"authorName":"王志","id":"7e601eb8-a756-4907-9df9-d969d61f4c38","originalAuthorName":"王志"},{"authorName":"刘燕","id":"805e2e2a-35c1-4494-9779-dd7b6a321cc1","originalAuthorName":"刘燕"},{"authorName":"王霞","id":"597d7920-dba6-47a1-9603-86a52b1d4f40","originalAuthorName":"王霞"},{"authorName":"张以群","id":"840563da-6fab-41a3-8cbe-eadf3f19ffcd","originalAuthorName":"张以群"}],"doi":"","fpage":"37","id":"3a5c51c3-4e19-4535-a919-b3361233fcf5","issue":"5","journal":{"abbrevTitle":"GFZCLKXYGC","coverImgSrc":"journal/img/cover/GFZCLKXYGC.jpg","id":"31","issnPpub":"1000-7555","publisherId":"GFZCLKXYGC","title":"高分子材料科学与工程"},"keywords":[{"id":"726598e9-da21-4162-805c-ecc76f19c917","keyword":"A-Bf-1型缩聚反应","originalKeyword":"A-Bf-1型缩聚反应"},{"id":"984f4c0a-7bdf-4644-a8b8-45548ed627d8","keyword":"超支化高<span style=\"color:red\">分子</span>","originalKeyword":"超支化高分子"},{"id":"4a2979f4-c01c-4603-a257-ecdec7b1b43b","keyword":"<span style=\"color:red\">分子</span>量分布函数","originalKeyword":"分子量分布函数"},{"id":"9401db73-5712-478d-bb27-868db6b09a20","keyword":"环化反应","originalKeyword":"环化反应"}],"language":"zh","publisherId":"gfzclkxygc200505009","title":"<span style=\"color:red\">动力学</span><span style=\"color:red\">方法</span>获得A-Bf-1型超支化<span style=\"color:red\">分子</span>的<span style=\"color:red\">分子</span>量分布函数","volume":"21","year":"2005"},{"abstractinfo":"利用嵌入原子模型,采用<span style=\"color:red\">分子</span><span style=\"color:red\">动力学</span><span style=\"color:red\">方法</span>计算了贵金属Au低指数晶面及部分简单高指数晶面的表面能.同时,采用Levenberg-Marquardt算法,建立了Au表面能的BP神经网络模型;结合<span style=\"color:red\">分子</span><span style=\"color:red\">动力学</span>模型的计算数据,通过大量数据的自学习训练,完成神经网络模型对Au高指数晶面表面能的预测.计算结果表明:该<span style=\"color:red\">方法</span>具有较高的预测精度,能正确预言低指数晶面表面能的排序,Au各晶面的表面能随其晶面与(111)密排面夹角的增大呈现先增大后减小的特点.","authors":[{"authorName":"汤伟","id":"9306a353-a8b3-4f77-8645-a7fc049f7bc4","originalAuthorName":"汤伟"},{"authorName":"朱定一","id":"2f0bd22c-01bf-4b0d-8583-6d98a4321a52","originalAuthorName":"朱定一"},{"authorName":"陈丽娟","id":"fc25f5aa-8f61-4b7e-bd45-b085e6721754","originalAuthorName":"陈丽娟"},{"authorName":"关翔锋","id":"1b3a0643-4f81-49e0-9aad-4d65e355c4fb","originalAuthorName":"关翔锋"}],"doi":"","fpage":"105","id":"5bad73f3-1323-4af8-b6c9-76eac61190f1","issue":"1","journal":{"abbrevTitle":"ZGYSJSXB","coverImgSrc":"journal/img/cover/ZGYSJSXB.jpg","id":"88","issnPpub":"1004-0609","publisherId":"ZGYSJSXB","title":"中国有色金属学报"},"keywords":[{"id":"d5048ca7-cb6e-4abf-ba9a-fe1783649352","keyword":"表面能","originalKeyword":"表面能"},{"id":"622d3d68-7d7b-44f3-b196-63fa2ec89e68","keyword":"嵌入原子势","originalKeyword":"嵌入原子势"},{"id":"450bfce2-9090-47e3-b09d-1b780333e33d","keyword":"人工神经网络","originalKeyword":"人工神经网络"},{"id":"12477496-89dd-4462-897f-c4519bf0bac8","keyword":"Levenberg-Marquardt算法","originalKeyword":"Levenberg-Marquardt算法"}],"language":"zh","publisherId":"zgysjsxb200501018","title":"基于<span style=\"color:red\">分子</span><span style=\"color:red\">动力学</span>结合神经网络的Au表面能计算<span style=\"color:red\">方法</span>","volume":"15","year":"2005"},{"abstractinfo":"<span style=\"color:red\">分子</span>马达是一类将化学能转化为机械能的微小机器.对二维模型的研究表明,非保守力在体系与外界能量交换中发挥重要作用.四态模型较好地反映了马达<span style=\"color:red\">力学</span>化学过程的各个状态及相应的构象变化.","authors":[{"authorName":"赵同军","id":"16933635-ebf2-475b-9a26-4964eb1fcd19","originalAuthorName":"赵同军"},{"authorName":"李微","id":"5cbcb87b-0cd2-4363-94b8-5c211b50158f","originalAuthorName":"李微"},{"authorName":"韩英荣","id":"b500a529-8786-4007-a785-854154524931","originalAuthorName":"韩英荣"},{"authorName":"卓益忠","id":"a5e126a5-2a23-4362-8193-d87b39e37fc8","originalAuthorName":"卓益忠"}],"doi":"10.3969/j.issn.1007-4627.2004.02.029","fpage":"177","id":"3aa3f1d2-5ea9-43b7-8130-189c7315c2b3","issue":"2","journal":{"abbrevTitle":"YZHWLPL","coverImgSrc":"journal/img/cover/YZHWLPL.jpg","id":"78","issnPpub":"1007-4627","publisherId":"YZHWLPL","title":"原子核物理评论   "},"keywords":[{"id":"13400856-ac5d-415b-b3ff-614a2f32bd7b","keyword":"<span style=\"color:red\">分子</span>马达","originalKeyword":"分子马达"},{"id":"83cd56c9-30cc-47e2-bae7-c943da79d34d","keyword":"布朗马达","originalKeyword":"布朗马达"},{"id":"a0fb59d7-fda0-4ae6-8b70-f16ffdfe6a9d","keyword":"<span style=\"color:red\">动力学</span>","originalKeyword":"动力学"},{"id":"cfa7a848-8202-4c7d-bfd9-cd03b01d1101","keyword":"棘齿","originalKeyword":"棘齿"}],"language":"zh","publisherId":"yzhwlpl200402029","title":"<span style=\"color:red\">分子</span>马达<span style=\"color:red\">动力学</span>","volume":"21","year":"2004"},{"abstractinfo":"为了预测聚己内酰胺(PA6)与聚烯烃热塑性弹性体(POE)的相容性及其共混物的玻璃化转变温度(Tg)、<span style=\"color:red\">力学</span>性能和结合能,采用<span style=\"color:red\">分子</span><span style=\"color:red\">动力学</span>(<span style=\"color:red\">MD</span>)和介观<span style=\"color:red\">动力学</span>(MesoDyn)模拟<span style=\"color:red\">方法</span>对PA6/POE共混物进行了研究.结果表明:通过温度-比容曲线可以得到PA6/POE共混体系的Tg分别对应于PA6与POE的Tg,PA6/POE为不相容体系；MesoDyn模拟了共混物的介观形貌与<span style=\"color:red\">动力学</span>演变过程,通过比较混合物的有序度参数的大小判断混合物为不相容体系.本模拟<span style=\"color:red\">方法</span>可以作为预测聚合物共混物性能的有利工具,也可以为高聚物配方设计提供理论指导.","authors":[{"authorName":"张彦飞","id":"3ac2aa1e-d616-4f10-be09-37c990564b2c","originalAuthorName":"张彦飞"},{"authorName":"兰艳花","id":"e43bbba5-dae3-433b-b76b-1d489860ac0f","originalAuthorName":"兰艳花"},{"authorName":"付一政","id":"703cc85b-ea09-4a82-803c-24a3b5b25a38","originalAuthorName":"付一政"},{"authorName":"赵贵哲","id":"767fb0ca-76b1-4da5-8337-7e13f6bb6a46","originalAuthorName":"赵贵哲"},{"authorName":"胡国胜","id":"ade7f979-a801-419f-9fc6-66b7ef7f73cd","originalAuthorName":"胡国胜"}],"doi":"10.3969/j.issn.1001-4381.2013.07.009","fpage":"44","id":"88b98545-0158-428b-b8c4-01fd28fa9b24","issue":"7","journal":{"abbrevTitle":"CLGC","coverImgSrc":"journal/img/cover/CLGC.jpg","id":"9","issnPpub":"1001-4381","publisherId":"CLGC","title":"材料工程"},"keywords":[{"id":"4034568e-0996-47f8-8215-fa31a1c51579","keyword":"聚己内酰胺","originalKeyword":"聚己内酰胺"},{"id":"7f0510ca-0383-435b-93bd-a45903043cd8","keyword":"聚烯烃热塑性弹性体","originalKeyword":"聚烯烃热塑性弹性体"},{"id":"537a8579-81a3-4627-97db-7ab198c3622e","keyword":"<span style=\"color:red\">分子</span><span style=\"color:red\">动力学</span>","originalKeyword":"分子动力学"},{"id":"6171676f-bb7a-4c67-9812-b37e12d7286d","keyword":"介观<span style=\"color:red\">动力学</span>","originalKeyword":"介观动力学"},{"id":"64d5d04a-482b-42f6-b4cb-991a82a04cf9","keyword":"相容性","originalKeyword":"相容性"}],"language":"zh","publisherId":"clgc201307009","title":"PA6/POE共混物的<span style=\"color:red\">分子</span><span style=\"color:red\">动力学</span>与介观<span style=\"color:red\">动力学</span>模拟","volume":"","year":"2013"},{"abstractinfo":"本文采用<span style=\"color:red\">分子</span><span style=\"color:red\">动力学</span>(<span style=\"color:red\">MD</span>)模拟来计算纳米流体比较重要的热物性:热导率和粘度,与已有实验结果比较符合较好,为进一步研究纳米流体传热效率提供了依据.","authors":[{"authorName":"范庆梅","id":"286af4d2-afc2-4aeb-84a6-2b7cee00a771","originalAuthorName":"范庆梅"},{"authorName":"卢文强","id":"3efacb34-d072-4c8a-8a7d-8bea5a997c29","originalAuthorName":"卢文强"}],"doi":"","fpage":"268","id":"43b31891-e6e2-46ed-9585-500556ea2b66","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":"cc84c053-ec35-494c-a3dd-70798772dd4e","keyword":"纳米流体","originalKeyword":"纳米流体"},{"id":"03600b04-0917-40af-8b4b-f02b923e5b1e","keyword":"<span style=\"color:red\">分子</span><span style=\"color:red\">动力学</span>(<span style=\"color:red\">MD</span>)模拟","originalKeyword":"分子动力学(MD)模拟"},{"id":"6d464d46-e2e0-4c25-9d03-cd12c137617e","keyword":"热导率","originalKeyword":"热导率"},{"id":"a827e9c3-0c26-4d9b-ae8e-56ad3b0ae122","keyword":"粘度","originalKeyword":"粘度"}],"language":"zh","publisherId":"gcrwlxb200402026","title":"纳米流体热导率和粘度的<span style=\"color:red\">分子</span><span style=\"color:red\">动力学</span>模拟计算","volume":"25","year":"2004"},{"abstractinfo":"为了预测聚烯烃弹性体(POE)与不同聚酰胺(PA6、PA11和PA1010)的相容性及共混物的<span style=\"color:red\">力学</span>性能和介观形貌,采用<span style=\"color:red\">分子</span><span style=\"color:red\">动力学</span>(<span style=\"color:red\">MD</span>)和介观<span style=\"color:red\">动力学</span>(MesoDyn)模拟<span style=\"color:red\">方法</span>对不同种类的POE/PA共混物进行了研究.结果表明,3种共混体系中PA11/POE共混物的拉伸模量、体积模量及剪切模量都较小,韧性比较好,<span style=\"color:red\">力学</span>性能和结合能最好；MesoDyn模拟结果表明,PA11与POE相容性最好.本模拟<span style=\"color:red\">方法</span>可以作为预测聚合物共混物性能的有利工具,也可以为高聚物配方设计提供理论参考.","authors":[{"authorName":"张彦飞","id":"9865528d-9cbd-4c87-8388-6293e4d75977","originalAuthorName":"张彦飞"},{"authorName":"兰艳花","id":"a1af158d-9f3b-45e1-b38e-0f8eda26a16e","originalAuthorName":"兰艳花"},{"authorName":"付一政","id":"c18ca19c-2544-4c42-80d9-04e59110b213","originalAuthorName":"付一政"},{"authorName":"刘亚青","id":"4eff8d08-bca6-4ad7-a2cd-8c364cc5814c","originalAuthorName":"刘亚青"},{"authorName":"胡国胜","id":"d95b8b1e-2e98-4da2-94f3-8ec53a53a733","originalAuthorName":"胡国胜"}],"doi":"","fpage":"182","id":"eafc1aa7-a887-40d4-b100-389b339bc3de","issue":"2","journal":{"abbrevTitle":"GFZCLKXYGC","coverImgSrc":"journal/img/cover/GFZCLKXYGC.jpg","id":"31","issnPpub":"1000-7555","publisherId":"GFZCLKXYGC","title":"高分子材料科学与工程"},"keywords":[{"id":"9a7f93b2-4ce8-4a57-8b9e-1b41f63f2222","keyword":"聚烯烃弹性体","originalKeyword":"聚烯烃弹性体"},{"id":"c169aa76-85fa-414c-baa6-d1581ccc1941","keyword":"聚酰胺","originalKeyword":"聚酰胺"},{"id":"853fb051-e226-4b5c-a5d1-71ba8989d81b","keyword":"<span style=\"color:red\">分子</span><span style=\"color:red\">动力学</span>","originalKeyword":"分子动力学"},{"id":"8f382c45-c28f-4c40-9bcb-9e7ccaee511a","keyword":"介观<span style=\"color:red\">动力学</span>","originalKeyword":"介观动力学"},{"id":"47cf8298-e92a-4a2d-aaa2-c2747aa77ac9","keyword":"<span style=\"color:red\">力学</span>性能","originalKeyword":"力学性能"},{"id":"84771e90-39e1-46ee-b6b8-f63b6bcc25b8","keyword":"结合能","originalKeyword":"结合能"}],"language":"zh","publisherId":"gfzclkxygc201302046","title":"POE/PA共混物性能的<span style=\"color:red\">分子</span><span style=\"color:red\">动力学</span>与介观<span style=\"color:red\">动力学</span>模拟","volume":"29","year":"2013"}],"totalpage":8476,"totalrecord":84752}