{"currentpage":1,"firstResult":0,"maxresult":10,"pagecode":5,"pageindex":{"endPagecode":5,"startPagecode":1},"records":[{"abstractinfo":"介绍了材质为16MnR的液化石油气球罐破裂情况,得出硫化物应力腐蚀是球罐产生裂纹的主要原因.提出了球罐维修和防腐蚀工艺措施,经年检和实践运行证明措施取得良好的效果.","authors":[{"authorName":"高中科","id":"6ed9011f-7a13-450e-a7be-3065ee0aade0","originalAuthorName":"高中科"},{"authorName":"慕细豹","id":"a0dd8d56-0268-4d13-b363-413838bbbcdd","originalAuthorName":"慕细豹"},{"authorName":"孙坚","id":"34730378-bbff-4ca3-bc09-a372890db335","originalAuthorName":"孙坚"},{"authorName":"库勤峰","id":"cafc17cb-b1b6-46a7-9c7a-287348fd2e2d","originalAuthorName":"库勤峰"}],"doi":"10.3969/j.issn.1005-748X.2007.08.015","fpage":"429","id":"d1241773-3911-439a-a9c4-27de4ff25ae7","issue":"8","journal":{"abbrevTitle":"FSYFH","coverImgSrc":"journal/img/cover/FSYFH.jpg","id":"25","issnPpub":"1005-748X","publisherId":"FSYFH","title":"腐蚀与防护"},"keywords":[{"id":"a5365f24-8364-41c8-be33-7ab148b22e7a","keyword":"液化石油气球罐","originalKeyword":"液化石油气球罐"},{"id":"4201e38e-8ee3-4362-87e6-b631c7205b6e","keyword":"失效原因","originalKeyword":"失效原因"},{"id":"1f9db69c-8402-4fc5-888c-797775aa5474","keyword":"<span style=\"color:red\">焊缝</span><span style=\"color:red\">缺</span><span style=\"color:red\">隙</span>","originalKeyword":"焊缝缺隙"},{"id":"22afc7f3-8288-491c-b09d-5aae86acfd53","keyword":"补焊工艺","originalKeyword":"补焊工艺"}],"language":"zh","publisherId":"fsyfh200708015","title":"液化石油气球罐裂纹原因分析及防护对策","volume":"28","year":"2007"},{"abstractinfo":"用传统氧化物法制备了<span style=\"color:red\">缺</span>铁组分为Y2.3Ca0.7Zr0.3V0.2Fe4.5-δO12（<span style=\"color:red\">缺</span>铁量δ=0.05）的石榴石铁氧体（YCaZrVIG）,用XRD、SEM对样品进行物相和微结构表征。研究了烧结温度对YCaZrVIG铁氧体物相组成、烧结性能、微观结构及电磁性能的影响。结果表明,烧结后的YCaZrVIG铁氧体为单相的石榴石结构;适当提高烧结温度,有利于气孔的排除和致密化;1400℃－1450℃烧结的YCaZrVIG铁氧体晶粒形状规则,晶界清晰,结构较致密。随烧结温度的提高,YCaZrVIG铁氧体的晶粒尺寸先增大后减小,1420℃烧结的YCaZrVIG铁氧体结构致密,气孔相对较少,晶粒大小均匀且尺寸最大（约20μm）,电磁性能较佳,ε=14.3,tanδε=4.4×10^-4,4πMs=165mT,Br=51mT,Hc=48A.m^-1（0.6Oe）。","authors":[{"authorName":"黄银寅","id":"111e15f7-5d7a-4028-964f-89be32720e19","originalAuthorName":"黄银寅"},{"authorName":"杨建","id":"6590328b-de74-4a55-abf2-f0473988049e","originalAuthorName":"杨建"},{"authorName":"金宇龙","id":"8129d772-a433-49db-bef0-cd35a77a9626","originalAuthorName":"金宇龙"},{"authorName":"王加仟","id":"52776c24-0d12-40c1-9c98-33fe6fd2ea33","originalAuthorName":"王加仟"},{"authorName":"丘泰","id":"cce7a91f-52fd-4630-a7e3-f87954baad14","originalAuthorName":"丘泰"}],"doi":"","fpage":"885","id":"364a91ab-d4f7-4eba-9b37-79ea86c2919b","issue":"6","journal":{"abbrevTitle":"CLKXYGCXB","coverImgSrc":"journal/img/cover/CLKXYGCXB.jpg","id":"13","issnPpub":"1673-2812","publisherId":"CLKXYGCXB","title":"材料科学与工程学报"},"keywords":[{"id":"28cdf46b-a23e-4882-8a10-1e488e4f9bea","keyword":"石榴石铁氧体","originalKeyword":"石榴石铁氧体"},{"id":"98562481-766f-405e-a5fb-57249c01dd38","keyword":"YCaZrVIG","originalKeyword":"YCaZrVIG"},{"id":"71920c2b-6360-405b-9d5f-2cf93bdfe508","keyword":"烧结温度","originalKeyword":"烧结温度"},{"id":"ee9b8610-93c4-42f4-ad72-ad437ffe2602","keyword":"微观结构","originalKeyword":"微观结构"},{"id":"3e117fb0-76d7-4ed6-a9e9-65a271c558e6","keyword":"电磁性能","originalKeyword":"电磁性能"}],"language":"zh","publisherId":"clkxygc201106016","title":"<span style=\"color:red\">缺</span>铁YCaZrVIG铁氧体的电磁性能","volume":"29","year":"2011"},{"abstractinfo":"基于化学式为Mg0.65Zn0.35Mn0.1Fe1.9-xO4-8的Mg-Mn-Zn铁氧体材料,采用具有高化学均匀性的柠檬酸有机凝胶法制备技术来研究少量<span style=\"color:red\">缺</span>铁(Iron deficient,x=0,0.05,0.1)对Mg-Mn-Zn铁氧体烧结密度、微观结构和磁性能的影响.实验表明:与符合化学计量比的Mg-Mn-Zn铁氧体相比,少量<span style=\"color:red\">缺</span>铁的Mg-Mn-Zn铁氧体具有更高的相对烧结密度和起始磁导率,然而具有较高的磁损耗;相对高的烧结密度和较大的晶粒尺寸导致了高的起始磁导率,较大的晶粒尺寸以及观察到的在少量<span style=\"color:red\">缺</span>铁样品晶界上析出的富镁锌方铁体(Wustite)相可能是造成少量<span style=\"color:red\">缺</span>铁Mg-Mn-Zn铁氧体具有较高磁损耗的原因.","authors":[{"authorName":"范积伟","id":"be0d18de-5290-45eb-8645-cc212eb30009","originalAuthorName":"范积伟"},{"authorName":"赵慧君","id":"89c412e0-158d-4ce4-8b9b-3789cbea2cec","originalAuthorName":"赵慧君"}],"doi":"","fpage":"1","id":"cc9ff111-3ea0-4482-8370-250bd3329515","issue":"z1","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":"c024c56b-05e3-4a9b-a2df-5d9a214de2d4","keyword":"Mg-Mn-zn铁氧体","originalKeyword":"Mg-Mn-zn铁氧体"},{"id":"99e20bfa-fdfe-4ce3-9ddd-a92f0e619a79","keyword":"少量<span style=\"color:red\">缺</span>铁","originalKeyword":"少量缺铁"},{"id":"784a5685-b34d-47df-8728-e193e48733c5","keyword":"烧结密度","originalKeyword":"烧结密度"},{"id":"33d0167c-81f8-4953-9c14-8f219a5c5d76","keyword":"起始磁导率","originalKeyword":"起始磁导率"},{"id":"178fd778-ba32-4cc5-9d94-552c5560f38c","keyword":"磁损耗","originalKeyword":"磁损耗"}],"language":"zh","publisherId":"xyjsclygc2008z1001","title":"少量<span style=\"color:red\">缺</span>铁对Mg-Mn-Zn铁氧体性能的影响","volume":"37","year":"2008"},{"abstractinfo":"统计了生产中的光亮镀镍溶液在镀层质量最佳时的248套主成分的分析数据,拟订了三个主要成分:硫酸镍(A)、氯化镍(B)、和硼酸(C)及成分比值A/B、A/C和B/C的诊断标准,并绘成了诊断图.应用此图来判定镀液成分的丰<span style=\"color:red\">缺</span>并指导生产中投料,获得了满意的效果.","authors":[{"authorName":"丘星初","id":"bdc0cf5a-4a4b-43cf-bd66-67ad107b4be9","originalAuthorName":"丘星初"},{"authorName":"丘山","id":"f2dbb2f3-33c7-4342-ba85-af89787e485d","originalAuthorName":"丘山"}],"doi":"10.3969/j.issn.1001-3849.2000.03.008","fpage":"25","id":"c32fcc55-357f-4920-b267-b9f3392e28a8","issue":"3","journal":{"abbrevTitle":"DDYJS","coverImgSrc":"journal/img/cover/DDYJS.jpg","id":"20","issnPpub":"1001-3849","publisherId":"DDYJS","title":"电镀与精饰   "},"keywords":[{"id":"c9ed4b6d-fbc0-46dc-b4db-6ac87b383d45","keyword":"镀液成分丰<span style=\"color:red\">缺</span>","originalKeyword":"镀液成分丰缺"},{"id":"31448d83-25af-41f1-bed8-e2d4985b899a","keyword":"诊断图","originalKeyword":"诊断图"},{"id":"05ab1998-2c6c-42f9-81a0-9841bfefe40e","keyword":"光亮镀镍溶液","originalKeyword":"光亮镀镍溶液"}],"language":"zh","publisherId":"ddjs200003008","title":"图法诊断光亮镀镍溶液主成分的丰<span style=\"color:red\">缺</span>","volume":"22","year":"2000"},{"abstractinfo":"采用氧化物法陶瓷工艺,对Li0.45Ni0.2Ti0.1Fe2.25O4铁氧体材料进行了<span style=\"color:red\">缺</span>铁配方、<span style=\"color:red\">缺</span>铁并添加烧结助剂等两方面的研究.结果表明:<span style=\"color:red\">缺</span>铁及添加Bi2O3都没有在锂铁氧体中形成杂相,烧结后陶瓷样品物相组成单一,结晶状况良好；这两种配方变化对材料微观形貌均有改善作用,其中同时<span style=\"color:red\">缺</span>铁并添加烧结助剂作用更为明显,该样品具有良好的综合性能,表观密度p为4.72 g·cm-3,介电损耗为5.4×10-4,饱和磁化强度4πM,为2275 Gs,剩磁比R为0.853,矫顽力Hc为2.9Oe,能够满足移相器对锂铁氧体材料的性能要求.","authors":[{"authorName":"唐可","id":"536506b9-20ed-4e86-8116-a81e91253dc1","originalAuthorName":"唐可"},{"authorName":"杨洪杰","id":"d4a719eb-fc65-4ae6-973c-2c32a545b551","originalAuthorName":"杨洪杰"}],"doi":"","fpage":"959","id":"239f985e-672d-4565-aee2-8709ad4bfc5d","issue":"5","journal":{"abbrevTitle":"RGJTXB","coverImgSrc":"journal/img/cover/RGJTXB.jpg","id":"57","issnPpub":"1000-985X","publisherId":"RGJTXB","title":"人工晶体学报"},"keywords":[{"id":"2e21ab1f-7bbb-4b93-82d1-26e83423b0c1","keyword":"锂铁氧体","originalKeyword":"锂铁氧体"},{"id":"b2f69ec1-e994-49d7-af2f-9d9f19469554","keyword":"<span style=\"color:red\">缺</span>铁","originalKeyword":"缺铁"},{"id":"56abbb20-de99-40fb-a0b5-b7a67e80be5c","keyword":"Bi2O3","originalKeyword":"Bi2O3"},{"id":"ee0622cb-a04f-4aeb-a497-fad53e77aea3","keyword":"微观形貌","originalKeyword":"微观形貌"},{"id":"71f29fe2-a9ed-440a-bff2-4a3c8e54d6f3","keyword":"介电性能","originalKeyword":"介电性能"},{"id":"8f9acf23-c469-4f5c-a30d-190344d50a21","keyword":"磁性能","originalKeyword":"磁性能"}],"language":"zh","publisherId":"rgjtxb98201305037","title":"<span style=\"color:red\">缺</span>铁配方及烧结助剂对锂铁氧体显微结构及电磁性能的影响","volume":"42","year":"2013"},{"abstractinfo":"利用在束核谱学实验技术, 建立了169Re基于9/2-[514]组态的强耦合转动带. 该带在已知的奇A Re核中具有最大的低自旋旋称劈列. 对于奇A Re中的9/2-[514]转动带, 研究了它们的能量旋称劈列和M1跃迁矩阵元相对旋称劈列与核形状偏离轴对称的关系, 揭示了非常<span style=\"color:red\">缺</span>中子的奇A Re核具有相当的负三轴形变.","authors":[{"authorName":"周小红","id":"677579da-e5b1-45d6-9d7a-f3bee7fc787c","originalAuthorName":"周小红"},{"authorName":"张玉虎","id":"18417873-fcfd-4abc-9a26-53a3c1c87363","originalAuthorName":"张玉虎"},{"authorName":"宋立涛","id":"080ff8de-aa53-45b9-9ea6-f070b51996d2","originalAuthorName":"宋立涛"},{"authorName":"郑勇","id":"40e6ac3c-2267-4d99-911b-cb4a1bb3fe76","originalAuthorName":"郑勇"},{"authorName":"徐岩冰","id":"cada417a-2eae-45eb-9b05-430538a5256e","originalAuthorName":"徐岩冰"}],"doi":"10.3969/j.issn.1007-4627.2004.04.017","fpage":"326","id":"27a40c86-14bf-4fbe-aac4-9240800418d1","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":"ad2a3121-b3c9-45df-a335-4d0c58d31363","keyword":"三轴形变","originalKeyword":"三轴形变"},{"id":"6e1d5368-b1d9-4cc6-b742-4cf4f1139d5e","keyword":"旋称劈列","originalKeyword":"旋称劈列"},{"id":"2a4f833f-f381-4606-9514-b6d6a62cb733","keyword":"奇A核","originalKeyword":"奇A核"}],"language":"zh","publisherId":"yzhwlpl200404017","title":"非常<span style=\"color:red\">缺</span>中子 Re核的负三轴形变研究","volume":"21","year":"2004"},{"abstractinfo":"通过重离子核反应与在束γ谱的实验技术, 对A=130<span style=\"color:red\">缺</span>中子核区122Cs与134Ce核的高自旋态进行了研究, 所用核反应分别为107Ag(19F, 1p3n)与 122Sn(16O,4n). 实验结果扩展了122Cs 与134Ce的能级纲图. 在122Cs中发现可能是属于手征二重带的结构, 而在134Ce核的高自旋态结构中呈现出重要的具有不同γ形变的形状共存特性.","authors":[{"authorName":"朱胜江","id":"27076966-ea78-4f99-b79a-725164379ab6","originalAuthorName":"朱胜江"},{"authorName":"禹英男","id":"6ba62fd8-e28c-43a1-b623-d6bd2eede346","originalAuthorName":"禹英男"},{"authorName":"甘翠云","id":"87867b16-93f1-44fd-aa3d-61105d98a0f7","originalAuthorName":"甘翠云"},{"authorName":"朱凌燕","id":"c86a35cc-14ea-4ef4-8708-28ab4e4d9ade","originalAuthorName":"朱凌燕"},{"authorName":"M·萨哈伊","id":"8cc953bc-9679-475b-9476-b348d5d682c0","originalAuthorName":"M·萨哈伊"},{"authorName":"肖树冬","id":"2602bf61-d2a7-40c7-9697-70a27f5be24f","originalAuthorName":"肖树冬"},{"authorName":"李明亮","id":"9902fa9b-4b30-448b-8907-4be6f6f17b04","originalAuthorName":"李明亮"},{"authorName":"车兴来","id":"8291c275-c04f-46ff-8029-2015d72fa627","originalAuthorName":"车兴来"},{"authorName":"温书贤","id":"0eb203ca-70bb-48dd-b6ad-4695a5a19255","originalAuthorName":"温书贤"},{"authorName":"竺礼华","id":"b0b0fc97-0f84-4552-82ff-58dcfddd7060","originalAuthorName":"竺礼华"},{"authorName":"吴晓光","id":"25816354-d8cf-4170-afc1-7064eec95dfb","originalAuthorName":"吴晓光"},{"authorName":"李广生","id":"3c777410-25c2-4979-8a8b-d08dfc36138b","originalAuthorName":"李广生"}],"doi":"10.3969/j.issn.1007-4627.2004.04.014","fpage":"315","id":"5f6553b3-ccf6-4888-b9d8-e06d367aa4c3","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":"24baf915-43e9-4ddf-b0a7-063453452f85","keyword":"核结构","originalKeyword":"核结构"},{"id":"9e1935cb-088b-49af-a311-033b870e2eb2","keyword":"高自旋态","originalKeyword":"高自旋态"},{"id":"f93aa092-8074-406e-a595-3ff4bf56d60b","keyword":"手征二重带","originalKeyword":"手征二重带"},{"id":"95e42c66-f571-4a41-b6f0-e90129d25c5a","keyword":"形状共存","originalKeyword":"形状共存"}],"language":"zh","publisherId":"yzhwlpl200404014","title":"A=130区<span style=\"color:red\">缺</span>中子核122Cs与134Ce高自旋态研究","volume":"21","year":"2004"},{"abstractinfo":"本文针对膜蒸馏实验中开放式的窄空气<span style=\"color:red\">隙</span>,研究其内流动与换热机理.研究发现,对于开放式的大宽<span style=\"color:red\">隙</span>比(120:1)空气<span style=\"color:red\">隙</span>,即使其厚度仅为 1 mm,也会形成向上流动的流场,其流动状态为层流,温度分布为直线分布.空气<span style=\"color:red\">隙</span>内按实验结果求得的热流密度大于按导热公式计算的结果.本文给出的数值模拟结果与实验结果吻合较好.","authors":[{"authorName":"高虹","id":"14875ef9-a8e7-4fc7-a14f-cfdf3d86eb01","originalAuthorName":"高虹"},{"authorName":"田瑞","id":"f419bbf4-11c3-4e35-83e5-d2fba9a5966f","originalAuthorName":"田瑞"},{"authorName":"杨晓宏","id":"00dd86fe-fae1-4b23-a49a-c3dd08a7663f","originalAuthorName":"杨晓宏"},{"authorName":"李嵩","id":"c7244f56-81c7-4717-bcb4-82b2f659ef0d","originalAuthorName":"李嵩"}],"doi":"","fpage":"2087","id":"207765d0-3e6c-40c9-9732-b9f53b5c1cf5","issue":"12","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":"23c20b59-bfa2-4519-b877-24e99608a541","keyword":"膜蒸馏","originalKeyword":"膜蒸馏"},{"id":"74ce2b9d-7041-4a31-8f70-f9817b4abd8c","keyword":"空气<span style=\"color:red\">隙</span>","originalKeyword":"空气隙"},{"id":"ad554bb5-ed9c-4622-acd9-ee06cc259c2e","keyword":"自然对流","originalKeyword":"自然对流"},{"id":"d9aee07d-be4c-4cf4-89b2-304e8f1ff2f4","keyword":"数值模拟","originalKeyword":"数值模拟"}],"language":"zh","publisherId":"gcrwlxb200912030","title":"气<span style=\"color:red\">隙</span>式膜蒸馏中空气<span style=\"color:red\">隙</span>内流动与换热研究","volume":"30","year":"2009"},{"abstractinfo":"介绍宝钢1550热镀锌机组<span style=\"color:red\">焊缝</span>跟踪和物料跟踪控制系统的配置和功能,以及系统应用软件的功能和现场使用情况.","authors":[{"authorName":"祃丽婷","id":"03e2dce2-cff4-407d-96ee-2660d3c3740e","originalAuthorName":"祃丽婷"}],"doi":"10.3969/j.issn.1001-7208.2004.06.007","fpage":"29","id":"4c9e66ad-82bd-4595-9cdd-00eafc85c9bc","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":"66cc4863-7c24-43f7-ab75-385a1898043f","keyword":"<span style=\"color:red\">焊缝</span>跟踪","originalKeyword":"焊缝跟踪"},{"id":"b32b26cb-fa8b-43f0-86fe-0d78615993ea","keyword":"物料跟踪","originalKeyword":"物料跟踪"},{"id":"ab649312-2076-450f-b702-9b8a1d1ad1a2","keyword":"人机接口","originalKeyword":"人机接口"},{"id":"0fbcf516-f30a-4c36-8689-2fdddef7f19b","keyword":"<span style=\"color:red\">焊缝</span>同步检测装置","originalKeyword":"焊缝同步检测装置"}],"language":"zh","publisherId":"shjs200406007","title":"<span style=\"color:red\">焊缝</span>跟踪和物料跟踪","volume":"26","year":"2004"},{"abstractinfo":"","authors":[{"authorName":"孔令晓","id":"6f1f7ba5-8049-4f1f-bc06-38fe934cc629","originalAuthorName":"孔令晓"},{"authorName":"孔瑞祥","id":"2ea8dd2f-1488-4a7d-90ee-492cf6956855","originalAuthorName":"孔瑞祥"}],"doi":"10.3969/j.issn.1000-6826.2000.03.007","fpage":"11","id":"b9c30c03-95f8-4f0c-b8ce-3d8def918cad","issue":"3","journal":{"abbrevTitle":"JSSJ","coverImgSrc":"journal/img/cover/3abe017a-2574-4821-8152-4ae974ef0471.jpg","id":"47","issnPpub":"1000-6826","publisherId":"JSSJ","title":"金属世界"},"keywords":[{"id":"f3f86589-25cb-40ff-8992-443bd4ca58e8","keyword":"","originalKeyword":""}],"language":"zh","publisherId":"jssj200003007","title":"当心<span style=\"color:red\">缺</span>钾","volume":"","year":"2000"}],"totalpage":304,"totalrecord":3034}