{"currentpage":1,"firstResult":0,"maxresult":10,"pagecode":5,"pageindex":{"endPagecode":5,"startPagecode":1},"records":[{"abstractinfo":"以蒸馏水为研磨介质,采用行星式球磨机对平均粒径约为10μm的SiC粉料进行了球磨,对球磨粉料进行酸洗除铁及水洗,制备出平均粒径为351.5nm的SiC超细粉料,详细分析了粉料制各过程中的物理化学变化与机理.结果发现:粗分散体系长时间球磨所得超细粉体溶液形成肢体分散系,体系固相含量增加,颗粒平均<span style=\"color:red\">最小间距</span>减小,颗粒间的范氏引力倍增,易形成团聚体;超细粉料胶体溶液在酸洗过程中产生了硬团聚,主要是由于Fe2+氧化水化成为Fe(OH)3胶桥,将超细粉料钳住所致;另外,测试溶液接近SiC等电点时亦会导致颗粒团聚.酸洗去除胶桥、调解溶液pH值可有效消除团聚.","authors":[{"authorName":"申玉芳","id":"ca002c48-6b27-4d6e-b8ae-66d9ce2f0659","originalAuthorName":"申玉芳"},{"authorName":"邹正光","id":"e6c233ce-5c1e-4f6b-b10d-59be89c420fb","originalAuthorName":"邹正光"}],"doi":"10.3969/j.issn.1005-0299.2008.02.033","fpage":"278","id":"e2e4fb77-f386-457e-b123-2c2c5530e4ae","issue":"2","journal":{"abbrevTitle":"CLKXYGY","coverImgSrc":"journal/img/cover/CLKXYGY.jpg","id":"14","issnPpub":"1005-0299","publisherId":"CLKXYGY","title":"材料科学与工艺"},"keywords":[{"id":"80e9f8c8-115a-4dbd-a92a-3f1334782552","keyword":"SiC超细粉","originalKeyword":"SiC超细粉"},{"id":"848e959b-68e9-4b9e-8ed8-b0c420271264","keyword":"<span style=\"color:red\">最小间距</span>","originalKeyword":"最小间距"},{"id":"3251c7de-3f18-4a7a-a770-9b23a67ee7be","keyword":"Fe(OH)3胶桥","originalKeyword":"Fe(OH)3胶桥"},{"id":"f0d76020-e0e6-4b0a-b3bc-0d595e81a59a","keyword":"等电点","originalKeyword":"等电点"},{"id":"0889ed61-592f-4295-ad8b-3d18c8df5037","keyword":"机理","originalKeyword":"机理"}],"language":"zh","publisherId":"clkxygy200802033","title":"SiC超细粉制备机理研究","volume":"16","year":"2008"},{"abstractinfo":"采用具有粒子动态混合密实功能的SPACE系统,实现了高集料体积分数模型砂浆结构的生成.从而,以3种细集料粒径分布的模型砂浆(其中一种的粒径范围为0.125～1.34 mm,另外两种的粒径范围为0.25～5.00mm)结构为例,研究了集料细度和集料体积分数(ψ=40%～70%)对邻近集料表面最近<span style=\"color:red\">间距</span>分布的影响.结果表明,集料细度增加和集料体积分数增大都会使大尺度邻近集料表面最近<span style=\"color:red\">间距</span>出现的概率减小、小尺度邻近集料表面最近<span style=\"color:red\">间距</span>出现的概率增加,且峰值概率的位置向<span style=\"color:red\">小间距</span>方向偏移.另外,邻近集料表面最近<span style=\"color:red\">间距</span>的分区段累计概率结果分析表明,3种模型砂浆结构的邻近集料表面最近<span style=\"color:red\">间距</span>分布的57%以上小于10μm.最后,邻近集料表面最近<span style=\"color:red\">间距</span>的平均值的分析结果显示,当集料体积分数在40%～70%之间变化时,邻近集料表面最近<span style=\"color:red\">间距</span>的平均值在54.6～1.1μm之间变化;当砂浆中集料的体积分数在50%～70%之间变化时,邻近集料表面最近<span style=\"color:red\">间距</span>的平均值与集料的体积分数基本上呈线性关系;单位砂浆体积下集料的表面积的变化对邻近集料表面最近<span style=\"color:red\">间距</span>的平均值有影响,但二者之间的比值并非常数.","authors":[{"authorName":"陈惠苏","id":"5647791f-996c-422c-91d5-723b6437f9ec","originalAuthorName":"陈惠苏"},{"authorName":"孙伟","id":"20716f3d-41b5-4679-9ba7-196265a6a54a","originalAuthorName":"孙伟"},{"authorName":"蒋金洋","id":"0a66aeaa-2fd6-4525-a52a-166370b1968a","originalAuthorName":"蒋金洋"},{"authorName":"Stroeven Piet","id":"a1697583-bc34-4398-aafd-a8c62c3655a4","originalAuthorName":"Stroeven Piet"},{"authorName":"STROEVEN Martijn","id":"51b86764-725d-414f-b426-2a95341f26b4","originalAuthorName":"STROEVEN Martijn"}],"doi":"10.3321/j.issn:1000-3851.2005.04.018","fpage":"100","id":"aa5ff0ef-a8ef-4d6b-af6a-e207dc14b390","issue":"4","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":"8f38e9ad-9cf1-419d-9abe-5b6f1290d082","keyword":"数值模拟","originalKeyword":"数值模拟"},{"id":"80eb0e04-611f-44d8-b9b1-6856a24501ed","keyword":"邻近粒子表面最近<span style=\"color:red\">间距</span>","originalKeyword":"邻近粒子表面最近间距"},{"id":"cdfab319-ac08-4359-9348-4d4684fac7b0","keyword":"砂浆","originalKeyword":"砂浆"},{"id":"f16a841e-71e9-48a6-9cc2-024c96254e41","keyword":"集料","originalKeyword":"集料"},{"id":"28b64aef-f5b3-42f0-ba24-e2544f96faa6","keyword":"SPACE系统","originalKeyword":"SPACE系统"}],"language":"zh","publisherId":"fhclxb200504018","title":"砂浆中邻近集料表面最近<span style=\"color:red\">间距</span>分布的数值模拟","volume":"22","year":"2005"},{"abstractinfo":"分析了转炉炼钢过程能源消耗与工艺、设备、操作等因素的关系,建立了转炉工序能耗模型和应用模型,研究了转炉炼钢工序的<span style=\"color:red\">最小</span>能耗问题和与<span style=\"color:red\">最小</span>工序能耗相对应的工况条件.针对我国宝钢250 t转炉的设备条件和生产数据,给出转炉煤气的最大回收量为128.8 m3/t(钢),<span style=\"color:red\">最小</span>工序能耗为-18.90 kg/t(钢).","authors":[{"authorName":"郦秀萍","id":"51630794-21fb-4d29-9f75-4ccc3bc8022c","originalAuthorName":"郦秀萍"},{"authorName":"蔡九菊","id":"4b45bc1d-dd76-4d9a-8ae0-96dad9a9fbc3","originalAuthorName":"蔡九菊"},{"authorName":"殷瑞钰","id":"9ac3578f-4065-4d30-a445-c34d154cd362","originalAuthorName":"殷瑞钰"},{"authorName":"王鼎","id":"bcb514fe-de4b-4d89-91c9-10411c627258","originalAuthorName":"王鼎"},{"authorName":"周庆安","id":"5fcaad31-6b3a-45ce-82a0-5be4ec8b1924","originalAuthorName":"周庆安"}],"doi":"","fpage":"50","id":"d231b554-54ee-4642-a1c7-eedbade8493b","issue":"5","journal":{"abbrevTitle":"GT","coverImgSrc":"journal/img/cover/GT.jpg","id":"27","issnPpub":"0449-749X","publisherId":"GT","title":"钢铁"},"keywords":[{"id":"03b16c3f-0880-40df-95c5-ab5935fa4e59","keyword":"转炉","originalKeyword":"转炉"},{"id":"fd99c13d-15af-48e3-9b42-2fb7fbe6a946","keyword":"模型","originalKeyword":"模型"},{"id":"b2b6c4c4-4f58-4105-963e-adfe99a2e665","keyword":"工序能耗","originalKeyword":"工序能耗"},{"id":"43f0958d-2b01-4ee5-8d1f-5ea6bc0edb8b","keyword":"<span style=\"color:red\">最小</span>能耗","originalKeyword":"最小能耗"}],"language":"zh","publisherId":"gt200305013","title":"转炉炼钢工序<span style=\"color:red\">最小</span>能耗的研究","volume":"38","year":"2003"},{"abstractinfo":"为了比较分析强化传热中存在的熵产<span style=\"color:red\">最小</span>化和传递势容耗散<span style=\"color:red\">最小</span>化两种不同的方法,针对体点问题,根据这两种方法对导热系数分布进行了优化.数值计算和理论分析的结果表明,根据<span style=\"color:red\">最小</span>传递势容耗散原理得到的结果优于<span style=\"color:red\">最小</span>熵产原理得到的结果.其原因在于传递势容耗散<span style=\"color:red\">最小</span>的优化目标是提高热量传递效率,而熵产<span style=\"color:red\">最小</span>的优化目标实际上是减少可用能损失.","authors":[{"authorName":"程新广","id":"229cec52-c285-4f3f-9f57-2bf6a31c3d61","originalAuthorName":"程新广"},{"authorName":"孟继安","id":"47a5337d-317f-4e0d-9dc6-4eadc1d1e74b","originalAuthorName":"孟继安"},{"authorName":"过增元","id":"cb92029f-bf5c-448f-907e-94be914af0b4","originalAuthorName":"过增元"}],"doi":"","fpage":"1034","id":"78a02742-40ac-4d92-a220-edcef2471da9","issue":"6","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":"0c5136aa-8b5e-42cc-9397-4d0ce247bb17","keyword":"<span style=\"color:red\">最小</span>熵产","originalKeyword":"最小熵产"},{"id":"12d25830-fede-49e5-8330-6c9ebd2f41c9","keyword":"<span style=\"color:red\">最小</span>传递势容耗散","originalKeyword":"最小传递势容耗散"},{"id":"07fb69dc-876e-4196-8c07-1058325003bc","keyword":"强化传热","originalKeyword":"强化传热"},{"id":"e63baa3c-0c43-473a-9082-fe243ad435b0","keyword":"导热系数","originalKeyword":"导热系数"}],"language":"zh","publisherId":"gcrwlxb200506043","title":"导热优化中的<span style=\"color:red\">最小</span>传递势容耗散与<span style=\"color:red\">最小</span>熵产","volume":"26","year":"2005"},{"abstractinfo":"在不同温度梯度及生长速度下测量了Ａｌ－Ａｌ３Ｎｉ共晶合金<span style=\"color:red\">间距</span>选择范围. 实验结果表明, 在一定生长速度下, 共晶<span style=\"color:red\">间距</span>存在一容许范围. 其宽度随生长速度的增加减小, 在某一温梯度下, 共晶<span style=\"color:red\">间距</span>与生长速度的关系满足λ＾ｎｕ＝常数ｎ＝１．７－２．０）的关系, 温度梯度增加, 其最大, <span style=\"color:red\">最小</span>及平均<span style=\"color:red\">间距</span>离略有减小. 同时, Ａｌ－Ａｌ３Ｎｉ合金的<span style=\"color:red\">间距</span>选择范围与初始生长速度无关.","authors":[{"authorName":"庄艳歆","id":"70852d9e-aa5b-4f70-9b88-58ba72635ad2","originalAuthorName":"庄艳歆"},{"authorName":"胡壮麒","id":"5beb701b-6ddb-4c72-8fb7-471f9952e9ca","originalAuthorName":"胡壮麒"},{"authorName":"朱丽红","id":"330c003d-bc6a-4243-9b5e-a918ae655ae8","originalAuthorName":"朱丽红"},{"authorName":"张修睦","id":"b62b386e-5ae4-47d3-b2a7-a47c655aa977","originalAuthorName":"张修睦"}],"categoryName":"|","doi":"","fpage":"353","id":"658bce31-9db9-4599-8225-069149f7c096","issue":"4","journal":{"abbrevTitle":"JSXB","coverImgSrc":"journal/img/cover/JSXB.jpg","id":"48","issnPpub":"0412-1961","publisherId":"JSXB","title":"金属学报"},"keywords":[{"id":"edf50bb7-dc59-4b33-9c2a-d7ab83811512","keyword":"<span style=\"color:red\">间距</span>","originalKeyword":"间距"},{"id":"2b381525-0592-4606-98e0-069c12ebe812","keyword":"null","originalKeyword":"null"},{"id":"59b06ebb-133d-4f15-a13b-395e7934bcf2","keyword":"null","originalKeyword":"null"},{"id":"fe3de7c5-d5e2-46fa-b188-c24ca4ce9c92","keyword":"null","originalKeyword":"null"}],"language":"zh","publisherId":"0412-1961_1999_4_12","title":"控制参数对Al—Al3Ni共晶合金<span style=\"color:red\">间距</span>的影响","volume":"35","year":"1999"},{"abstractinfo":"本文根据层片状共晶生长理论，利用时间相关模型对存在对流作用的Al-CuAl2共晶层片<span style=\"color:red\">间距</span>进行数值求解<span style=\"color:red\">最小</span>和最大层片<span style=\"color:red\">间距</span>（&lambda;o和&lambda;max）的计算结果与实验结果符合较好，熔体的流动使Al-CuAl2共晶稳态生长的层片<span style=\"color:red\">间距</span>增加；当层片<span style=\"color:red\">间距</span>超过&lambda;max时，层片组织处于非稳态：共晶生长速率越低，液相流动的影响越大","authors":[{"authorName":"张伟强","id":"690a3b40-0649-43b4-876a-13e638902217","originalAuthorName":"张伟强"},{"authorName":"杨院生","id":"0ae1e4b9-569b-4c2f-bc33-fb9397c11f01","originalAuthorName":"杨院生"},{"authorName":"胡壮麒","id":"c6401b06-8025-491f-9519-dd77cc1aea09","originalAuthorName":"胡壮麒"}],"categoryName":"|","doi":"","fpage":"1","id":"2006ff9c-4fa1-4ac2-baa2-da974c3a4fa7","issue":"1","journal":{"abbrevTitle":"JSXB","coverImgSrc":"journal/img/cover/JSXB.jpg","id":"48","issnPpub":"0412-1961","publisherId":"JSXB","title":"金属学报"},"keywords":[{"id":"2e0a38eb-bfec-4224-99bc-021d5e822475","keyword":"共晶","originalKeyword":"共晶"},{"id":"f09601a5-cdea-49b2-8b2d-510f5de025a3","keyword":" lamellar spacing","originalKeyword":" lamellar spacing"},{"id":"c46c38ed-c583-4b69-9797-14ef18d5eae7","keyword":" fluid flow","originalKeyword":" fluid flow"},{"id":"60d524e9-fed1-4ae8-afbe-ab32b669e1b9","keyword":" stability","originalKeyword":" stability"}],"language":"zh","publisherId":"0412-1961_1998_1_3","title":"Al-CuAl_2共晶层片<span style=\"color:red\">间距</span>的数值模拟","volume":"34","year":"1998"},{"abstractinfo":"<span style=\"color:red\">最小</span>二乘法是求解精确晶格参数的基本方法.讨论了使用和不使用校正函数情形下的科恩<span style=\"color:red\">最小</span>二乘法,给出了所有晶系的法方程、晶格参数、误差估计的计算公式,以及计算晶格参数、校正函数参数的阻尼<span style=\"color:red\">最小</span>二乘迭代算法,该方法具有普适性,有大的收敛范围和快的收敛速度.作为应用例子,计算了数个不同晶系晶体的晶格参数,说明<span style=\"color:red\">最小</span>二乘法是获得高精度晶格参数的计算方法;用阻尼<span style=\"color:red\">最小</span>二乘法计算了ChuG校正函数的参数,表明该方法是获得校正函数参数的有效方法.","authors":[{"authorName":"张庆礼","id":"ce01ff48-6c76-42e1-bdd8-787ad9709028","originalAuthorName":"张庆礼"},{"authorName":"王宜申","id":"55c3e905-75ae-4fad-a526-708ba2f88e56","originalAuthorName":"王宜申"},{"authorName":"肖进","id":"09a84918-c610-41be-bb62-49ff40b7e247","originalAuthorName":"肖进"},{"authorName":"李冬青","id":"fc776fa7-fdb2-48cc-9a68-1f5a9f465325","originalAuthorName":"李冬青"},{"authorName":"殷绍唐","id":"20400f75-806a-460c-a71c-4e2a5e097e8c","originalAuthorName":"殷绍唐"}],"doi":"10.3969/j.issn.1007-5461.2009.02.010","fpage":"177","id":"24ddce29-5fdd-4926-9704-e581e560e29f","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":"b76c58bf-b8fd-4f32-8384-5eb45b7a7564","keyword":"材料","originalKeyword":"材料"},{"id":"da8fe6db-c924-463a-bf44-fb908a06172a","keyword":"晶格参数","originalKeyword":"晶格参数"},{"id":"1b3d33c2-b7d7-4977-94f2-e18db770cf56","keyword":"科恩<span style=\"color:red\">最小</span>二乘法","originalKeyword":"科恩最小二乘法"},{"id":"04a0bcb0-91e7-4c38-a463-17552fbed53d","keyword":"法方程","originalKeyword":"法方程"},{"id":"29c6d49d-0fab-4ecd-b0a1-dbc8d6bb3e11","keyword":"衍射角校正函数","originalKeyword":"衍射角校正函数"},{"id":"c6258769-92e4-4351-b3c0-6cac0b964d64","keyword":"阻尼<span style=\"color:red\">最小</span>二乘法","originalKeyword":"阻尼最小二乘法"}],"language":"zh","publisherId":"lzdzxb200902010","title":"<span style=\"color:red\">最小</span>二乘法计算晶格参数","volume":"26","year":"2009"},{"abstractinfo":"根据<span style=\"color:red\">最小</span>方差预测理论， 提出了用<span style=\"color:red\">最小</span>方差预测 法预测岩土工程变形， 对其建模机 理和准则进行了论述， 并对预测模型的优化方法进行了研究和探讨。 在实际应用中， 将 <span style=\"color:red\">最小</span>方差预测法与其它预 测方法进行了比较。 结果表明， 该方法建模简便， 计算简单， 模型更 新优化快， 能取得较高的预测精度。","authors":[{"authorName":"王国辉","id":"4c6ac675-504c-48f5-aafd-aaf2f8d15b70","originalAuthorName":"王国辉"},{"authorName":"马莉","id":"72310b03-ad63-43fc-974b-6577fcc2cf59","originalAuthorName":"马莉"},{"authorName":"杨腾峰","id":"a890afa5-5bd8-4aea-8973-8e545145e319","originalAuthorName":"杨腾峰"},{"authorName":"侯永会","id":"3f4da4a8-ace0-484e-bf2b-cf47460715a7","originalAuthorName":"侯永会"},{"authorName":"李卫国","id":"82c4cda5-c015-4d29-9e63-3df0471b1256","originalAuthorName":"李卫国"}],"doi":"","fpage":"162","id":"55d54030-2332-40d2-8069-ec7396cfbeec","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":"420170d5-c300-479c-871c-47e925e63545","keyword":"<span style=\"color:red\">最小</span>方差预测","originalKeyword":"最小方差预测"},{"id":"f19306ef-ebad-40b4-affa-7007550d684e","keyword":"变形预测","originalKeyword":"变形预测"},{"id":"856f63d2-9358-4c66-8416-93da210cf25a","keyword":"模型优化","originalKeyword":"模型优化"}],"language":"zh","publisherId":"zgysjsxb200101036","title":"<span style=\"color:red\">最小</span>方差预测法预测岩土工程变形","volume":"11","year":"2001"},{"abstractinfo":"采取在静子叶片表面埋入微型压力传感器的方法,对叶尖、叶中和叶根三个截面上的动态压力进行测量,实验研究了六个轴向<span style=\"color:red\">间距</span>下压气机的旋转失速特性.实验结果表明:轴向<span style=\"color:red\">间距</span>对压气机失速点的流量系数影响很大,转静子轴向<span style=\"color:red\">间距</span>减少,压气机失速推迟;压气机刚进入旋转失速的模态与轴向<span style=\"color:red\">间距</span>有关,轴向<span style=\"color:red\">间距</span>较大时,压气机首先进入多团全叶高旋转失速,当轴向<span style=\"color:red\">间距</span>为21%CR时,压气机直接进入单团全叶高旋转失速;轴向<span style=\"color:red\">间距</span>不同,近失速点的压力扰动也存在差别.","authors":[{"authorName":"李传鹏","id":"160e5ddc-d758-463e-9301-5844cd2807a4","originalAuthorName":"李传鹏"},{"authorName":"胡骏","id":"dbd138ff-67f5-4094-990b-690e70e4615b","originalAuthorName":"胡骏"},{"authorName":"王英锋","id":"41e54909-3313-417f-8a23-cbcbc05deff6","originalAuthorName":"王英锋"},{"authorName":"张燎原","id":"2896c752-f9ed-48a7-a66c-02f1d949fbb8","originalAuthorName":"张燎原"}],"doi":"","fpage":"246","id":"94efc969-7c4f-46a5-a5ac-62f7a8208564","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":"697b7925-7fa5-4839-930e-295beffd0e20","keyword":"轴向<span style=\"color:red\">间距</span>","originalKeyword":"轴向间距"},{"id":"7587cea3-ae37-4cc2-88aa-dc979fedf438","keyword":"失速模态","originalKeyword":"失速模态"},{"id":"e4d56323-616e-4b39-97dd-a4082b3d88df","keyword":"失速特性","originalKeyword":"失速特性"}],"language":"zh","publisherId":"gcrwlxb200502020","title":"轴向<span style=\"color:red\">间距</span>对压气机失速特性的影响","volume":"26","year":"2005"},{"abstractinfo":"利用金相显微镜观察合金的显微组织并测量枝晶臂<span style=\"color:red\">间距</span>,采用电化学工作站研究不同镍含量ZA35合金的电化学腐蚀性能.结果表明,元素镍的加入对合金组织细化和耐蚀性能具有重要影响,当加入量为0.5％时所得ZA35-0.5Ni合金组织最为细化,为团絮状组织,二次枝晶臂<span style=\"color:red\">间距</span><span style=\"color:red\">最小</span>,仅为12.84μm,比ZA35合金减小23％.该合金在3.5％NaCl溶液中的耐蚀性能高,腐蚀电流密度较ZA35合金减小85％.","authors":[{"authorName":"刘敬福","id":"49436fec-c5c4-43fd-933e-4836abaadb3f","originalAuthorName":"刘敬福"},{"authorName":"冯立丽","id":"25409100-3bea-467e-9994-257941a3aac7","originalAuthorName":"冯立丽"}],"doi":"10.3969/j.issn.2095-1744.2016.04.007","fpage":"26","id":"dd8e1a88-9182-4dc8-9769-f64569cb0612","issue":"4","journal":{"abbrevTitle":"YSJSGC","coverImgSrc":"journal/img/cover/YSJSGC.jpg","id":"76","issnPpub":"2095-1744","publisherId":"YSJSGC","title":"有色金属工程"},"keywords":[{"id":"524e9a5d-6aaf-4ff8-9eff-74c1f84b36b1","keyword":"ZA35合金","originalKeyword":"ZA35合金"},{"id":"989abe95-46b2-45ab-91ce-173914e8237b","keyword":"镍","originalKeyword":"镍"},{"id":"c2a73552-e1e2-440d-9cc5-cc29ba8433f7","keyword":"枝晶臂<span style=\"color:red\">间距</span>","originalKeyword":"枝晶臂间距"},{"id":"79485320-8e9c-470d-af0a-ad045eeada4e","keyword":"电化学性能","originalKeyword":"电化学性能"}],"language":"zh","publisherId":"ysjs201604007","title":"ZA35-xNi合金的枝晶臂<span style=\"color:red\">间距</span>和电化学性能","volume":"6","year":"2016"}],"totalpage":547,"totalrecord":5468}