{"currentpage":1,"firstResult":0,"maxresult":10,"pagecode":5,"pageindex":{"endPagecode":5,"startPagecode":1},"records":[{"abstractinfo":"采用SEM、XRD、动电位极化曲线及电化学阻抗等测试方法,研究了MB8镁合金微弧氧化过程中不同<span style=\"color:red\">终止</span><span style=\"color:red\">电压</span>下获得的陶瓷膜层的耐蚀性能.结果表明:<span style=\"color:red\">终止</span><span style=\"color:red\">电压</span>越高,膜层越厚;微火花阶段,膜层表面均匀、结晶细致,腐蚀电流密度较小,阻抗较大;弧放电阶段,膜层孔径变大,陶瓷层内显微缺陷增多,腐蚀电流密度增大,阻抗减小.由此得出结论:膜层耐蚀性能由膜层厚度与<span style=\"color:red\">终止</span><span style=\"color:red\">电压</span>共同决定,微火花放电末期膜层的耐蚀性能优于弧放电阶段的耐蚀性能.","authors":[{"authorName":"赵晴","id":"965be876-5217-49ec-a0bf-9256d093f752","originalAuthorName":"赵晴"},{"authorName":"章志友","id":"924be03b-dc8a-4c99-afc8-6b546680c7cf","originalAuthorName":"章志友"},{"authorName":"陈宁","id":"e7d3afe3-6be2-4729-93b6-5220bbad0eae","originalAuthorName":"陈宁"}],"doi":"10.3969/j.issn.1001-3660.2007.04.002","fpage":"4","id":"33b1d91e-2695-42e8-9448-1a8764b968f9","issue":"4","journal":{"abbrevTitle":"BMJS","coverImgSrc":"journal/img/cover/BMJS.jpg","id":"3","issnPpub":"1001-3660","publisherId":"BMJS","title":"表面技术   "},"keywords":[{"id":"d138d0f5-361c-4a79-9d17-c298e8d3f8ae","keyword":"微弧氧化","originalKeyword":"微弧氧化"},{"id":"54bcbde4-1ba4-4ada-b4cc-e8a14b98f31d","keyword":"镁合金","originalKeyword":"镁合金"},{"id":"0f8610f9-6120-413c-90d3-286c6d81eb6c","keyword":"耐蚀性","originalKeyword":"耐蚀性"},{"id":"33646809-bee8-493d-a199-fc344b876982","keyword":"<span style=\"color:red\">终止</span><span style=\"color:red\">电压</span>","originalKeyword":"终止电压"}],"language":"zh","publisherId":"bmjs200704002","title":"<span style=\"color:red\">终止</span><span style=\"color:red\">电压</span>对MB8镁合金微弧氧化膜耐蚀性的影响","volume":"36","year":"2007"},{"abstractinfo":"用组态相关推转壳模型Nilsson势研究了C．M．Parry组最近用EUROBALL谱仪观测到的127La高自旋态结构．实验上观测的127La的宇称和辛量子数为(π,α)=(+,-1/2)的带自旋达到(83/2)h．理论计算结果表明该带可能具有组态π(h11/2)2v(h11/2)6．并且几乎达到该带的带<span style=\"color:red\">终止</span>理论预言值 I=47.5h．该带的形变在I≤40h内处于正常形变区(ε2≈0.22，γ≈0°)，随着角动量的增加ν值逐渐增加，直到ν＝60°时带<span style=\"color:red\">终止</span>．","authors":[{"authorName":"董保国","id":"10f45003-283c-448e-81f6-6c7c91ea21b3","originalAuthorName":"董保国"},{"authorName":"郭宏超","id":"537fb03c-e03c-44fb-b4ed-3b48a019ad16","originalAuthorName":"郭宏超"},{"authorName":"I.Ragnarsson","id":"84f76bf9-33a5-4dca-a1a9-9faf9a1c126d","originalAuthorName":"I.Ragnarsson"}],"doi":"10.3969/j.issn.1007-4627.2000.04.006","fpage":"216","id":"13858167-4121-41c8-8122-cbbe6ed66518","issue":"4","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":"9ce5e984-3f73-42c9-9844-32740760b8cf","keyword":"带<span style=\"color:red\">终止</span>","originalKeyword":"带终止"},{"id":"011511d7-bf32-4441-adba-635c08323c7e","keyword":"转动带","originalKeyword":"转动带"},{"id":"96b92360-8cd9-49a7-9941-f5b87f398251","keyword":"组态相关推转壳模型","originalKeyword":"组态相关推转壳模型"}],"language":"zh","publisherId":"yzhwlpl200004006","title":"127La转动带及带<span style=\"color:red\">终止</span>","volume":"17","year":"2000"},{"abstractinfo":"研究了微弧氧化处理中起始<span style=\"color:red\">电压</span>U始、<span style=\"color:red\">终止</span><span style=\"color:red\">电压</span>U终对陶瓷层的影响,发现<span style=\"color:red\">电压</span>是决定微弧氧化陶瓷层生长厚度及表面粗糙度的关键.结果表明:当起始<span style=\"color:red\">电压</span>U始相等时,<span style=\"color:red\">终止</span><span style=\"color:red\">电压</span>U终(或△U)愈高,陶瓷层厚度愈厚;当<span style=\"color:red\">终止</span><span style=\"color:red\">电压</span>U终相等时,起始<span style=\"color:red\">电压</span>U始愈高,陶瓷层厚度也愈厚.试样的表面粗糙度随微弧氧化处理<span style=\"color:red\">终止</span><span style=\"color:red\">电压</span>U终的升高而增加,与U始变化的关系不明显.","authors":[{"authorName":"陈宏","id":"814364c6-d2e5-4e60-b756-79b409aabada","originalAuthorName":"陈宏"},{"authorName":"郝建民","id":"63d61e6e-542a-4e11-b9fe-3d6d33de64e6","originalAuthorName":"郝建民"},{"authorName":"王利捷","id":"486a56a5-2257-4d8a-af29-bce82b8c8dd5","originalAuthorName":"王利捷"}],"doi":"10.3969/j.issn.1001-3660.2004.03.007","fpage":"17","id":"123ec152-b428-4b7c-8fd4-7b968caf1786","issue":"3","journal":{"abbrevTitle":"BMJS","coverImgSrc":"journal/img/cover/BMJS.jpg","id":"3","issnPpub":"1001-3660","publisherId":"BMJS","title":"表面技术   "},"keywords":[{"id":"40b1bc59-a5eb-45b3-a308-1fd8664ffaee","keyword":"镁合金","originalKeyword":"镁合金"},{"id":"8592b28c-582e-4ec3-90b2-355dc63938a6","keyword":"微弧氧化","originalKeyword":"微弧氧化"},{"id":"1bf6eb69-fd03-4e0c-a775-23c47212e304","keyword":"陶瓷层","originalKeyword":"陶瓷层"},{"id":"b259078f-09ce-49ad-9468-07901c050e74","keyword":"粗糙度","originalKeyword":"粗糙度"},{"id":"ab914b1b-6606-4fe2-943e-43f74aa50b13","keyword":"<span style=\"color:red\">电压</span>","originalKeyword":"电压"}],"language":"zh","publisherId":"bmjs200403007","title":"镁合金微弧氧化处理<span style=\"color:red\">电压</span>对陶瓷层的影响","volume":"33","year":"2004"},{"abstractinfo":"采用 MMS300热模拟试验机对 GCr15轴承钢的热变形工艺进行模拟，研究变形<span style=\"color:red\">终止</span>温度对其显微组织的影响。结果表明，变形<span style=\"color:red\">终止</span>温度在770～870℃内变化时，其显微组织均为片层状珠光体＋沿晶界分布的先共析碳化物，并且先共析碳化物周围存在铁素体薄膜。随着变形<span style=\"color:red\">终止</span>温度的升高，晶粒尺寸和珠光体团的尺寸均增加，珠光体的片层间距略微减小，硬度增加。通过回归分析获得维氏硬度与片层间距倒数的拟合方程 HV＝38．3S －1＋92．7。变形<span style=\"color:red\">终止</span>温度在810～870℃内升高时，碳化物的网状程度增加。与810℃相比，变形<span style=\"color:red\">终止</span>温度为770℃和790℃时，碳化物的网状程度较严重。","authors":[{"authorName":"李振兴","id":"ac9d2eb6-51d4-44c4-ae8e-36f1afaf31fb","originalAuthorName":"李振兴"},{"authorName":"李长生","id":"3a680359-77fa-4899-badd-395fa0c36b9c","originalAuthorName":"李长生"},{"authorName":"马永强","id":"73b98e58-c212-4466-8d4d-e01ffa4bd6ec","originalAuthorName":"马永强"},{"authorName":"李涛","id":"85b6dbe3-944d-4a2e-a331-23a44fe62f82","originalAuthorName":"李涛"},{"authorName":"张建","id":"b2c3e580-9334-4691-9e31-7ebf5e834cc5","originalAuthorName":"张建"}],"doi":"10.11868/j.issn.1001-4381.2015.10.005","fpage":"28","id":"b8645cd8-1529-4d80-85c6-899c309b24cc","issue":"10","journal":{"abbrevTitle":"CLGC","coverImgSrc":"journal/img/cover/CLGC.jpg","id":"9","issnPpub":"1001-4381","publisherId":"CLGC","title":"材料工程"},"keywords":[{"id":"7b76757b-5738-4ce0-9272-9fd0b6a8e65e","keyword":"GCr15 轴承钢","originalKeyword":"GCr15 轴承钢"},{"id":"ff755fa8-b9fb-40da-a721-59adf1c499cd","keyword":"变形<span style=\"color:red\">终止</span>温度","originalKeyword":"变形终止温度"},{"id":"ccbe4495-ab44-48fe-8502-4b7a0170d58a","keyword":"珠光体","originalKeyword":"珠光体"},{"id":"8a45ee90-d0e5-4eb8-b866-846b39074e09","keyword":"网状碳化物","originalKeyword":"网状碳化物"},{"id":"0cfd6244-a5d0-4fac-9b68-9bd8bd28eff9","keyword":"片层间距","originalKeyword":"片层间距"}],"language":"zh","publisherId":"clgc201510005","title":"变形<span style=\"color:red\">终止</span>温度对 GCr15轴承钢显微组织的影响","volume":"","year":"2015"},{"abstractinfo":"对缩短胶接面长度以提高起裂载荷的复合材料加筋壁板长桁<span style=\"color:red\">终止</span>端新型混合连接设计进行了研究.采用经试验验证的有限元方法,对长桁<span style=\"color:red\">终止</span>端混合连接的传载与失效机制进行分析,并研究了胶接面长度对结构起裂载荷的影响规律.研究结果表明:新型混合连接设计中紧固件提供的法向约束以及剪切载荷传递路径可显著提升<span style=\"color:red\">终止</span>端结构的起裂载荷,并增强<span style=\"color:red\">终止</span>端处界面的抑制损伤扩展能力;结构的起裂载荷随着胶接面的缩短而提高;当胶接面前缘退至连接区末排紧固件之后,可避免结构在最终破坏前发生界面失效,结构强度由蒙皮的机械连接强度决定.","authors":[{"authorName":"钟小丹","id":"d8087f5d-a9fc-4020-80df-8e8e94bdd720","originalAuthorName":"钟小丹"},{"authorName":"陈普会","id":"f8209291-80d2-4ff3-843f-cc5ae8278e91","originalAuthorName":"陈普会"}],"doi":"","fpage":"197","id":"e7df5419-44c5-4fef-9cb7-a10f4c0762cf","issue":"6","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":"f690ff3d-f908-4f9d-8a58-7aff04df380f","keyword":"复合材料","originalKeyword":"复合材料"},{"id":"1b0809f2-a723-4c5d-9464-1af08446206b","keyword":"加筋壁板","originalKeyword":"加筋壁板"},{"id":"16ddb762-e877-4783-b234-91e569b1f3e9","keyword":"长桁<span style=\"color:red\">终止</span>端","originalKeyword":"长桁终止端"},{"id":"7c4083db-b75d-4601-9cd4-736bf7f49505","keyword":"混合连接","originalKeyword":"混合连接"},{"id":"891b8315-d0a9-4d8d-8696-76635b0a29d5","keyword":"脱胶","originalKeyword":"脱胶"}],"language":"zh","publisherId":"fhclxb201306029","title":"复合材料加筋壁板长桁<span style=\"color:red\">终止</span>端混合连接设计分析","volume":"30","year":"2013"},{"abstractinfo":"在试验轧机上对X80管线钢进行了热轧试验，并采用超快冷结合层流冷却的冷却方式对试验钢进行了冷却，结合组织观测，系统研究了超快冷<span style=\"color:red\">终止</span>温度对力学性能的影响。结果表明：在超快冷<span style=\"color:red\">终止</span>温度为670℃时，组织中发现了多边形铁素体，试验钢屈强比较低；随着超快冷<span style=\"color:red\">终止</span>温度的降低，析出物粒子逐渐增多，尺寸逐渐细小且弥散，试验钢的强度和低温韧性逐渐提高，断后伸长率先升高后降低。","authors":[{"authorName":"周晓光","id":"dddd47b0-46b0-4785-b0e2-8187c8b33f70","originalAuthorName":"周晓光"},{"authorName":"刘振宇","id":"90d59ba6-9d87-476c-82dc-86a0196026fe","originalAuthorName":"刘振宇"},{"authorName":"吴迪","id":"a7f1f176-2cdf-45ad-a7de-b59c416798eb","originalAuthorName":"吴迪"},{"authorName":"王国栋","id":"dd92a87d-c986-44a2-8407-a7afc1aca1ce","originalAuthorName":"王国栋"}],"doi":"","fpage":"5","id":"11901f86-019c-4d3c-b633-f2d47baed6e8","issue":"10","journal":{"abbrevTitle":"JXGCCL","coverImgSrc":"journal/img/cover/JXGCCL.jpg","id":"45","issnPpub":"1000-3738","publisherId":"JXGCCL","title":"机械工程材料"},"keywords":[{"id":"1573634a-c613-46f3-b58e-9989e8754bea","keyword":"超快冷","originalKeyword":"超快冷"},{"id":"d02ccd6d-5c69-46dd-a9c2-2b39ee934d4b","keyword":"管线钢","originalKeyword":"管线钢"},{"id":"f533b6db-39fa-4977-963c-a1fae518f0de","keyword":"显微组织","originalKeyword":"显微组织"},{"id":"75004cd4-5f09-4545-aced-fe1464d476a8","keyword":"力学性能","originalKeyword":"力学性能"}],"language":"zh","publisherId":"jxgccl201210002","title":"超快速冷却<span style=\"color:red\">终止</span>温度对X80管线钢组织和性能的影响","volume":"36","year":"2012"},{"abstractinfo":"<span style=\"color:red\">电压</span>加载方式会影响微弧氧化过程及膜层性能。利用自制的具有多种输出脉冲形式的电源，在不同的<span style=\"color:red\">电压</span>增量下加载对AZ91D镁合金微弧氧化，研究了加载方式对微弧氧化过程及膜层性能的影响。结果表明：随着<span style=\"color:red\">电压</span>增量的增加，成膜速率增大，膜层粗糙度变大，表面的孔径增大、孔隙率增加；膜层的最终厚度主要取决于<span style=\"color:red\">终止</span><span style=\"color:red\">电压</span>，而<span style=\"color:red\">终止</span><span style=\"color:red\">电压</span>相同时，<span style=\"color:red\">电压</span>增量越大，平均耗能越小；微弧氧化的不同阶段应采用不同的<span style=\"color:red\">电压</span>增量，开始阶段将其恒定为10v／min，当<span style=\"color:red\">电压</span>达到350V后改增量为5V／min直至<span style=\"color:red\">终止</span><span style=\"color:red\">电压</span>，这种加载方式制膜时的成膜效率、能耗及膜层耐蚀性、表面性能等综合结果较好。","authors":[{"authorName":"彭飞","id":"cb87fcb3-93ac-4700-a4b5-50d4b880f72a","originalAuthorName":"彭飞"},{"authorName":"马跃洲","id":"22dc6d3e-28d7-4327-bd8f-a789b0fc6ce1","originalAuthorName":"马跃洲"},{"authorName":"王鹏","id":"8da3b5dd-9c8f-4b88-a23a-7ba79ec1f9ef","originalAuthorName":"王鹏"},{"authorName":"杨亮","id":"a3e4052a-0ffe-4a73-b7a2-1c11d93d4a34","originalAuthorName":"杨亮"},{"authorName":"田明辉","id":"13168a25-19bd-40cb-97b9-53f21e4ca880","originalAuthorName":"田明辉"}],"doi":"","fpage":"12","id":"f9b69a59-7e7d-4b6e-96e4-0422253b1cc7","issue":"7","journal":{"abbrevTitle":"CLBH","coverImgSrc":"journal/img/cover/CLBH.jpg","id":"7","issnPpub":"1001-1560","publisherId":"CLBH","title":"材料保护"},"keywords":[{"id":"d1a11c8f-32da-40d4-bc4f-458274e0ef8e","keyword":"微弧氧化","originalKeyword":"微弧氧化"},{"id":"c764ed3c-9276-4a21-b3a7-3c773791500a","keyword":"<span style=\"color:red\">电压</span>加载方式","originalKeyword":"电压加载方式"},{"id":"16c16a52-3219-49f1-9400-af3a4a5bfeb2","keyword":"AZ91D镁合金","originalKeyword":"AZ91D镁合金"},{"id":"b5a0cc34-b0b4-49e7-8169-cc7367ee1074","keyword":"<span style=\"color:red\">电压</span>增量","originalKeyword":"电压增量"},{"id":"8a9268f2-2591-42cb-82b1-42397d51d0ab","keyword":"耐蚀性","originalKeyword":"耐蚀性"}],"language":"zh","publisherId":"clbh201207007","title":"<span style=\"color:red\">电压</span>加载方式对镁合金微弧氧化过程及膜层性能的影响","volume":"45","year":"2012"},{"abstractinfo":"由于设计要求或设计限制条件，壁板的长桁常常在翼肋或机身框附近、机翼的前后梁附近、机翼与机身的开口附近、机翼的油箱附近等部位<span style=\"color:red\">终止</span>。在面内载荷作用下，截面形状突变和传载路径偏移在端头处会产生应力集中，极易引起缘条／蒙皮界面脱胶分层。对三种构型的长桁<span style=\"color:red\">终止</span>端典型件在单向拉、压载荷下的破坏机制进行了试验研究与数值模拟，结果表明，拉伸时的失效是由面外剥离应力与层间剪应力的共同作用所致，而压缩时的失效主要是由层间剪应力所致。","authors":[{"authorName":"周凯华","id":"d37d50a6-2201-4fd3-b10d-844461062ed2","originalAuthorName":"周凯华"},{"authorName":"陈普会","id":"2a0bccc3-d35d-4d51-ab09-74cc9fff7533","originalAuthorName":"陈普会"},{"authorName":"柴亚南","id":"9d6d0f31-6947-4494-bea1-185dd89e4397","originalAuthorName":"柴亚南"}],"doi":"","fpage":"212","id":"5b1f3481-aa70-461a-bede-157331048aa5","issue":"6","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":"4b8bf07f-e88a-42bf-9d10-933ad97100c7","keyword":"复合材料","originalKeyword":"复合材料"},{"id":"6b443b59-6fb5-4cb5-84bb-b712c2e6ca12","keyword":"加筋板","originalKeyword":"加筋板"},{"id":"604b2d24-7ba5-4ae7-9971-641acd0e6125","keyword":"长桁<span style=\"color:red\">终止</span>端","originalKeyword":"长桁终止端"},{"id":"074d3aff-4fc9-4842-baab-eb04a8c6e403","keyword":"脱胶","originalKeyword":"脱胶"},{"id":"f7b53787-dfaa-4008-b3d5-d1d220c0118e","keyword":"失效机制","originalKeyword":"失效机制"}],"language":"zh","publisherId":"fhclxb201206034","title":"复合材料加筋板长桁<span style=\"color:red\">终止</span>端失效机制","volume":"29","year":"2012"},{"abstractinfo":"针对体心立方(bcc)结构金属及合金{112}〈111〉孪生的ω点阵机制,利用点阵模型详解了bcc结构金属及合金{112}〈111〉孪晶形核、长大和<span style=\"color:red\">终止</span>全过程.模型揭示了孪晶可以通过ω→bcc转变过程形成孪晶核胚,再通过孪晶核胚生长或合并的方式长大,最终与特殊位向ω相作用受阻而停止.该机制说明了{112}〈111〉类型孪晶是一种相变孪晶.","authors":[{"authorName":"吴松全","id":"e138004b-5733-44f7-82de-e994b0cbd107","originalAuthorName":"吴松全"},{"authorName":"杨义","id":"8814f259-7689-436f-a64f-fada74a7e93b","originalAuthorName":"杨义"},{"authorName":"李阁平","id":"48ac2c5b-6648-4722-9078-c6758dcc9ce0","originalAuthorName":"李阁平"},{"authorName":"平德海","id":"24dbdafe-9e50-48fa-bf15-79bcdd7e7c7c","originalAuthorName":"平德海"},{"authorName":"胡青苗","id":"c3d8dc2e-485c-47a2-8489-ed75bbc8f345","originalAuthorName":"胡青苗"},{"authorName":"杨锐","id":"89fc07e3-2848-44e5-8bb0-b465124889ac","originalAuthorName":"杨锐"}],"doi":"10.11900/0412.1961.2015.00309","fpage":"249","id":"05bfcd11-c40c-49ec-9834-3e96bf5dc193","issue":"2","journal":{"abbrevTitle":"JSXB","coverImgSrc":"journal/img/cover/JSXB.jpg","id":"48","issnPpub":"0412-1961","publisherId":"JSXB","title":"金属学报"},"keywords":[{"id":"97aec010-552b-480f-9310-b14d754465e4","keyword":"金属和合金","originalKeyword":"金属和合金"},{"id":"98d62dc8-4334-4102-9879-1d6f487a6aed","keyword":"孪晶","originalKeyword":"孪晶"},{"id":"4dffa57b-ff18-43bb-804a-859e62c0f03b","keyword":"相变","originalKeyword":"相变"},{"id":"b7c9e940-83d4-464e-9b26-c79cbbe44f38","keyword":"ω点阵","originalKeyword":"ω点阵"}],"language":"zh","publisherId":"jsxb201602016","title":"{112}〈111〉孪生的形核和长大及<span style=\"color:red\">终止</span>的ω点阵机制","volume":"52","year":"2016"},{"abstractinfo":"通过在硅橡胶绝缘材料上施加交直流<span style=\"color:red\">电压</span>，研究工频交流<span style=\"color:red\">电压</span>叠加在直流<span style=\"color:red\">电压</span>上时对绝缘间隙的局部放电幅值与重复率的影响。结果表明：当交流<span style=\"color:red\">电压</span>纹波振幅低于其局部放电<span style=\"color:red\">终止</span><span style=\"color:red\">电压</span>时，相比没有叠加交流纹波的直流<span style=\"color:red\">电压</span>，其大放电脉冲的数量增加，而重复率则远低于交流<span style=\"color:red\">电压</span>频率。","authors":[{"authorName":"曹馨予","id":"af7ac280-50ea-44f2-97c5-a27f0f011794","originalAuthorName":"曹馨予"},{"authorName":"王刚","id":"9fe83228-3a99-43d8-9d8c-bc34a8034940","originalAuthorName":"王刚"},{"authorName":"赵毅","id":"ef0054cc-9b09-47b9-971c-ccc8522ec472","originalAuthorName":"赵毅"}],"doi":"10.16790/j.cnki.1009-9239.im.2016.12.012","fpage":"62","id":"ee4fe46c-d6c1-4b8a-9316-028f620c09a4","issue":"12","journal":{"abbrevTitle":"JYCL","coverImgSrc":"journal/img/cover/JYCL.jpg","id":"50","issnPpub":"1009-9239","publisherId":"JYCL","title":"绝缘材料"},"keywords":[{"id":"c0a15d29-2482-4493-9cbc-58e3f12bd97f","keyword":"高压直流输电","originalKeyword":"高压直流输电"},{"id":"d5d74b1c-8450-428a-b9ae-4289ed9b41fb","keyword":"交流<span style=\"color:red\">电压</span>纹波","originalKeyword":"交流电压纹波"},{"id":"d7820808-53ef-42cd-b85a-48c5ac0fa68a","keyword":"复合绝缘子","originalKeyword":"复合绝缘子"},{"id":"2729924f-cf29-4b00-a31f-b159924e4720","keyword":"局部放电","originalKeyword":"局部放电"}],"language":"zh","publisherId":"jycltx201612013","title":"交直流<span style=\"color:red\">电压</span>叠加对绝缘子局部放电影响的研究","volume":"","year":"2016"}],"totalpage":406,"totalrecord":4060}