{"currentpage":1,"firstResult":0,"maxresult":10,"pagecode":5,"pageindex":{"endPagecode":5,"startPagecode":1},"records":[{"abstractinfo":"对配合比和加工制作过程完全相同聚乙烯醇(PVA)纤维增强水泥基复合材料,通过采用一种对试件断面抛光,涂荧光粉的显微成像法对PVA纤维在水泥基材料中的分布状况进行量化测定;通过3点弯曲试验并结合测定结果研究了纤维分布对材料弯曲性能的影响.纤维测定结果表明:荧光显微成像法在划分网格适当的条件下可以准确的量化测定PVA纤维的分布,3点弯曲试验和纤维分布测定结果表明:纤维分布对材料的开裂强度没有影响,但是却决定了开裂强度到弯曲强度的提高幅度和弯曲韧度.纤维分布越均匀,提高幅度和弯曲韧度越大,同时材料的弯曲强度及相应的挠度也越大.","authors":[{"authorName":"牛恒茂","id":"d71f6aa6-34e9-4762-b142-3242c49d032f","originalAuthorName":"牛恒茂"},{"authorName":"武文红","id":"5709d138-d34d-44f8-9eaa-72e8ae6c3350","originalAuthorName":"武文红"},{"authorName":"<span style=\"color:red\">米</span><span style=\"color:red\">力</span>","id":"158ba819-cb9a-4b36-99d1-1ffc1d50a984","originalAuthorName":"米力"}],"doi":"","fpage":"325","id":"be4f8a8f-d251-4380-9737-c07c35b7335b","issue":"2","journal":{"abbrevTitle":"GSYTB","coverImgSrc":"journal/img/cover/GSYTB.jpg","id":"36","issnPpub":"1001-1625","publisherId":"GSYTB","title":"硅酸盐通报   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style=\"color:red\">米</span>、喉部镶嵌鈹青铜的风洞喷管内壁的研制过程。采用的是硫酸盐—氯化物混和型电铸镍溶液。对设计所要求的镍层机械、物理性能、电铸镍—鈹青铜搭接形式与其疲劳强度进行了测","authors":[{"authorName":"陈钧武","id":"aea4a160-1e84-48c2-b29f-17709001212b","originalAuthorName":"陈钧武"}],"categoryName":"|","doi":"","fpage":"234","id":"a251075c-9987-40fe-b2ef-1cecb9e59232","issue":"3","journal":{"abbrevTitle":"ZGFSYFHXB","coverImgSrc":"journal/img/cover/中国腐蚀封面19-3期-01.jpg","id":"81","issnPpub":"1005-4537","publisherId":"ZGFSYFHXB","title":"中国腐蚀与防护学报"},"keywords":[],"language":"zh","publisherId":"1005-4537_1984_3_18","title":"1.8<span style=\"color:red\">米</span>风洞喷管内壁的电铸制造","volume":"4","year":"1984"},{"abstractinfo":"分别用<span style=\"color:red\">米</span>氏散射和瑞利散射对钧瓷内小气泡和分相液滴的散射进行模拟计算,以对比两种计算方法的差异.通过对比计算,解析了钧瓷乳光产生的机理.计算结果表明,对于单个颗粒的散射,气泡的散射远远大于分相.气泡和分相的散射都是各向异性,并且波长越短,散射越强.但它们对短波选择的程度随粒子半径变化是不同的,小气泡是单调的,而分相液滴会有极值出现.","authors":[{"authorName":"杨高林","id":"f0e158bf-c14c-490b-9245-c904038d2b99","originalAuthorName":"杨高林"},{"authorName":"孙洪巍","id":"96a43b5a-eb49-4c7f-8bd6-678cb7730eda","originalAuthorName":"孙洪巍"},{"authorName":"李国霞","id":"f9c5b6e1-80d1-4127-aca3-1e915d0e0158","originalAuthorName":"李国霞"},{"authorName":"赵维娟","id":"1302f0a3-05ce-4bf6-ac43-4759e2776b3b","originalAuthorName":"赵维娟"},{"authorName":"李融武","id":"6cd487b6-4651-4fbe-9e4b-9d6ef14d0a6e","originalAuthorName":"李融武"}],"doi":"","fpage":"120","id":"88abb26c-a489-414e-ad55-8c8c4e36a72c","issue":"10","journal":{"abbrevTitle":"CLDB","coverImgSrc":"journal/img/cover/CLDB.jpg","id":"8","issnPpub":"1005-023X","publisherId":"CLDB","title":"材料导报"},"keywords":[{"id":"47799de8-0020-4a17-acc0-d802d9af1f5e","keyword":"<span style=\"color:red\">米</span>氏散射","originalKeyword":"米氏散射"},{"id":"07b02678-cdd2-42b1-8677-25024c0d83d6","keyword":"瑞利散射","originalKeyword":"瑞利散射"},{"id":"23acdb46-f8fb-4f33-b750-d21a126ca203","keyword":"钧瓷","originalKeyword":"钧瓷"},{"id":"59357c99-9bc3-4e96-8a3f-49c078cbd7d1","keyword":"分相","originalKeyword":"分相"},{"id":"7a44a77a-ef43-47fc-8553-4a78042d074c","keyword":"气泡","originalKeyword":"气泡"}],"language":"zh","publisherId":"cldb200710032","title":"基于<span style=\"color:red\">米</span>氏散射的钧瓷乳光模拟计算","volume":"21","year":"2007"},{"abstractinfo":"引入了矢量非傍轴厄<span style=\"color:red\">米</span>余弦高斯(HCosG)光束的概念,从矢量瑞利 - 索末菲衍射积分公式出发,得出了矢量非傍轴HCosG光束在自由空间的解析传输公式,并将非傍轴HCosG光束在自由空间衍射时轴上、近场、远场以及在傍轴条件下的传输作为特例给出.数值计算和分析表明,对于矢量非傍轴HCosG光束,参数和偏心参数均对光束的非傍轴特性有重要影响.此外,其轴上光强分布与光束的阶数及其奇偶性有关.","authors":[{"authorName":"唐斌","id":"f75c382e-28b5-4326-a1b7-a895a8b50c2f","originalAuthorName":"唐斌"},{"authorName":"蒋美萍","id":"c1a24771-c9bb-4561-9e1a-a8df37cabf60","originalAuthorName":"蒋美萍"},{"authorName":"江兴方","id":"e8141cf2-7bab-45c4-910e-deaf85ddd379","originalAuthorName":"江兴方"},{"authorName":"金铱","id":"a5160193-a5b1-4353-8b03-1b5f29ab04dc","originalAuthorName":"金铱"}],"doi":"10.3969/j.issn.1007-5461.2008.05.003","fpage":"528","id":"0c891212-2601-4a6c-9bf3-12e9a4d0fb1b","issue":"5","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":"77db70e6-eaaa-45bf-83e8-08221e536b3b","keyword":"物理光学","originalKeyword":"物理光学"},{"id":"8788f0c8-8934-4f31-942a-978c85c33467","keyword":"矢量非傍轴厄<span style=\"color:red\">米</span>余弦高斯光束","originalKeyword":"矢量非傍轴厄米余弦高斯光束"},{"id":"41c2d904-56a5-4d62-a88e-ee26f54963b2","keyword":"瑞利-索末菲衍射积分","originalKeyword":"瑞利-索末菲衍射积分"},{"id":"8ad27ab0-462c-44df-87b8-ba337ac49e39","keyword":"f参数","originalKeyword":"f参数"},{"id":"7dab2e25-e6e4-464e-a586-4ed5f676ea2d","keyword":"偏心参数","originalKeyword":"偏心参数"}],"language":"zh","publisherId":"lzdzxb200805003","title":"矢量非傍轴厄<span style=\"color:red\">米</span>余弦高斯光束","volume":"25","year":"2008"},{"abstractinfo":"针对湖南怀化新晃县<span style=\"color:red\">米</span>贝金矿选矿厂混合浮选的金精矿铅含量过高,精矿中铅矿物难以分离,达不到焙烧及氰化工艺质量要求的问题,采用优先浮选原矿中的方铅矿,再浮选含金硫化物矿物的试验流程进行金、铅分离.在选矿试验过程中,充分利用了方铅矿与其他硫化物矿物的天然可浮性差异,并选用对方铅矿选择捕收能力强、对黄铁矿捕收能力弱的25号黑药.浮选闭路试验可获得铅品位62.79％的合格铅精矿和含铅0.48％的低铅含砷金精矿.该工艺流程可使原矿中的方铅矿得到充分的回收,并达到了含砷金精矿降铅提质的目的,提高了企业的经济效益,对高铅、含砷金精矿的除铅具有借鉴意义.","authors":[{"authorName":"刘西分","id":"4b835756-1e26-4756-b485-c16eb2532597","originalAuthorName":"刘西分"},{"authorName":"常红","id":"60bf45da-438b-41b2-85bf-abf8d4d8cce8","originalAuthorName":"常红"}],"doi":"10.11792/hj20150612","fpage":"49","id":"74ba25e7-30ac-43c3-8457-c8cdc25e809c","issue":"6","journal":{"abbrevTitle":"HJ","coverImgSrc":"journal/img/cover/HJ.jpg","id":"44","issnPpub":"1001-1277","publisherId":"HJ","title":"黄金"},"keywords":[{"id":"6d762bda-385b-4c94-9d4c-344d07fa92bc","keyword":"金矿","originalKeyword":"金矿"},{"id":"cbdb09ed-e97e-4a32-8d95-0cd081b3b601","keyword":"方铅矿","originalKeyword":"方铅矿"},{"id":"73a87892-0ae6-4629-bdf1-efd781a89a62","keyword":"铅金分离","originalKeyword":"铅金分离"},{"id":"2c796774-c13e-485b-93bb-4c1ddad500cd","keyword":"浮选","originalKeyword":"浮选"}],"language":"zh","publisherId":"huangj201506012","title":"<span style=\"color:red\">米</span>贝金矿金铅分离试验研究","volume":"36","year":"2015"},{"abstractinfo":"为获取ADS工程中四翼型RFQ加速器在设计、调谐和运行等方面的经验，设计和建造了一台一<span style=\"color:red\">米</span>长四翼型RFQ加速器。该RFQ的设计频率为162.5 MHz，但是测量结果显示即使没有调谐器时，腔体的频率也为163.7 MHz。为降低腔体频率，使用四线模型理论进行了分析并重新设计了腔体的端板。使用了二极模稳定杆来加大四极频率与相邻二极频率的间隔。最终测量结果显示，在腔体电压分布没有大的波动的情况下腔体频率达到了设计频率。同时，腔体Q值降低了1%，这就要求需要更多的功率注入腔体。使用水对二极模稳定杆进行了冷却，以便腔体能够稳定工作。","authors":[{"authorName":"潘刚","id":"748870ec-1ea4-45f9-8ecb-69f7952fb57e","originalAuthorName":"潘刚"},{"authorName":"何源","id":"680e0d41-232d-4ee3-b3cb-1a2b7b74a3d8","originalAuthorName":"何源"},{"authorName":"赵红卫","id":"023cfa66-f8bd-4127-b856-9285b3a5534b","originalAuthorName":"赵红卫"},{"authorName":"石爱民","id":"3a33dd65-6579-4c4f-b466-8424fb52140d","originalAuthorName":"石爱民"},{"authorName":"杜小楠","id":"b8dd2484-7a0f-4c21-a31a-b8136f586a25","originalAuthorName":"杜小楠"},{"authorName":"张周礼","id":"4646c2f5-b5a5-41ae-a55c-1caa699da2ee","originalAuthorName":"张周礼"},{"authorName":"孙列鹏","id":"2dcdcd5c-e9f4-4e85-b5df-616b3a9e1e5b","originalAuthorName":"孙列鹏"},{"authorName":"张聪","id":"a5467976-7361-4980-9df3-49d9baeb7210","originalAuthorName":"张聪"},{"authorName":"施龙波","id":"eea2c8fb-1816-4c70-a889-4ad40da3e74c","originalAuthorName":"施龙波"}],"doi":"10.11804/NuclPhysRev.31.02.161","fpage":"161","id":"fb823a81-673d-42f8-9d26-a1b1f7b8cadb","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":"3152ff99-6961-4861-ba3a-21d838fd8152","keyword":"四极频率","originalKeyword":"四极频率"},{"id":"7c32f879-8d24-4395-a7cf-cced4a22919d","keyword":"二极频率","originalKeyword":"二极频率"},{"id":"ba3b6ce8-0914-4549-bf63-6432ec33be24","keyword":"二极模稳定杆","originalKeyword":"二极模稳定杆"},{"id":"e68079d2-2a41-4aa1-a530-0844b157e385","keyword":"端板","originalKeyword":"端板"}],"language":"zh","publisherId":"yzhwlpl201402008","title":"一<span style=\"color:red\">米</span>长四翼型RFQ调谐研究","volume":"","year":"2014"},{"abstractinfo":"研究了矿样分解后,利用巯基树脂富集金,洗脱分离后用硫代<span style=\"color:red\">米</span>蚩酮光度法测定矿石中的金,取得了较为满意的结果.","authors":[{"authorName":"周文敞","id":"aff098fb-5e8e-4320-9bbc-ea9e6482e70d","originalAuthorName":"周文敞"},{"authorName":"沈友","id":"c1ba2e47-2c2f-4cfa-a16f-64557dbde9bc","originalAuthorName":"沈友"}],"doi":"10.3969/j.issn.1001-1277.2002.09.014","fpage":"48","id":"18c57e34-e708-4766-b77c-0aba672a0704","issue":"9","journal":{"abbrevTitle":"HJ","coverImgSrc":"journal/img/cover/HJ.jpg","id":"44","issnPpub":"1001-1277","publisherId":"HJ","title":"黄金"},"keywords":[{"id":"f329e5bb-a21c-4bcb-be2f-81d4d80db7b4","keyword":"巯基树指","originalKeyword":"巯基树指"},{"id":"f83a9deb-b38b-4aaf-b125-8cee3579e30e","keyword":"金","originalKeyword":"金"},{"id":"c23a3296-f99c-4de0-80fd-1a6d33491b49","keyword":"硫代<span style=\"color:red\">米</span>蚩酮","originalKeyword":"硫代米蚩酮"},{"id":"f00768d4-dac6-461f-a1f5-dc8a17102cd1","keyword":"光度法","originalKeyword":"光度法"}],"language":"zh","publisherId":"huangj200209014","title":"巯基树脂富集硫代<span style=\"color:red\">米</span>蚩酮光度法测定矿石中的金","volume":"23","year":"2002"},{"abstractinfo":"介绍了3种汽车车身电泳涂装现场测量泳透<span style=\"color:red\">力</span>的方法,即电位仪测量法、一<span style=\"color:red\">米</span>钢条测量法和泳透<span style=\"color:red\">力</span>盒测量法.比较了这3种测试方法的优缺点.其中,泳透<span style=\"color:red\">力</span>盒测量法以检测结果能够量化,有较高的精度,重复性和再现性好,对车型结构没有特殊要求,有合理的判定标准以及能够在生产现场灵活使用等优点而被确定为较佳的泳透<span style=\"color:red\">力</span>现场测量方法.","authors":[{"authorName":"华云","id":"d8b35fb5-5d0e-46cb-ba53-949edb97d754","originalAuthorName":"华云"},{"authorName":"王辉","id":"35c7a1c8-9071-4667-a356-f93b24ef56e4","originalAuthorName":"王辉"},{"authorName":"周磊","id":"5323cdef-451e-45c8-bc22-f8ebe1b0200c","originalAuthorName":"周磊"},{"authorName":"董文超","id":"edbb4cb2-2164-46a3-9019-a5ba6a2178d2","originalAuthorName":"董文超"}],"doi":"","fpage":"68","id":"453442ed-b00e-4dca-a2d4-ebe8ebc84e8b","issue":"10","journal":{"abbrevTitle":"DDYTS","coverImgSrc":"journal/img/cover/DDYTS.jpg","id":"21","issnPpub":"1004-227X","publisherId":"DDYTS","title":"电镀与涂饰   "},"keywords":[{"id":"86173b5b-6e2a-4771-a338-f02640738be3","keyword":"汽车车身","originalKeyword":"汽车车身"},{"id":"de28dbc4-e723-4783-ab73-f513c82fea87","keyword":"电泳","originalKeyword":"电泳"},{"id":"f58049d5-a7a0-4916-80c1-78b615876d80","keyword":"泳透<span style=\"color:red\">力</span>","originalKeyword":"泳透力"},{"id":"098cb4a4-d037-4318-853f-445bc4eaf4c1","keyword":"现场测量","originalKeyword":"现场测量"}],"language":"zh","publisherId":"ddyts201210018","title":"汽车电泳涂装泳透<span style=\"color:red\">力</span>现场测量方法","volume":"31","year":"2012"},{"abstractinfo":"在继2003年完成10<span style=\"color:red\">米</span>三相高温超导电缆之后,我们于2004年年底成功完成了75<span style=\"color:red\">米</span>高温超导电缆的组装、调试和通电试运行.这两套电缆装置的低温冷却系统都是采用单相密闭液氮流程循环冷却高温超导电缆本体及终端,都是采用液氮减压制冷方式获取制冷量,借助过冷器内液氮作为冷媒把冷量传递给液氮循环系统.本文在简要介绍10<span style=\"color:red\">米</span>长高温超导电缆低温冷却系统基础上,重点介绍75<span style=\"color:red\">米</span>高温超导电缆冷却系统的试运行和在通电情况下的实验结果,并对实验数据进行热平衡分析和制冷量与液氮消耗量的分析,从而得到高温超导电缆冷却系统运行的经济性参数.","authors":[{"authorName":"范宇峰","id":"6b531e19-9998-4489-8bd3-8ff8656c387c","originalAuthorName":"范宇峰"},{"authorName":"龚领会","id":"d916ba73-cfe8-4566-9256-27ad03efdc5e","originalAuthorName":"龚领会"},{"authorName":"徐向东","id":"5674e7a9-85a6-47c3-b5cd-d1cc016cef68","originalAuthorName":"徐向东"},{"authorName":"张亮","id":"c327b90f-abc8-40d5-8e73-1ea432ee7dda","originalAuthorName":"张亮"},{"authorName":"吴江","id":"195c4478-6c6b-4e92-bfb7-a2e753b29061","originalAuthorName":"吴江"},{"authorName":"李来风","id":"d8b3b309-1ea4-4c30-97c2-2cf8ff41b6f5","originalAuthorName":"李来风"},{"authorName":"肖立业","id":"77f4e781-6075-4f39-a281-35e7fc979d3d","originalAuthorName":"肖立业"}],"doi":"10.3969/j.issn.1000-3258.2005.z1.127","fpage":"1068","id":"428a0f09-d3ed-431f-b099-94f7293ce400","issue":"z1","journal":{"abbrevTitle":"DWWLXB","coverImgSrc":"journal/img/cover/DWWLXB.jpg","id":"19","issnPpub":"1000-3258","publisherId":"DWWLXB","title":"低温物理学报   "},"keywords":[{"id":"58b92403-32cd-4c2c-b755-2c8f49ca6be7","keyword":"高温超导电缆","originalKeyword":"高温超导电缆"},{"id":"2ef7bb80-aaf9-4fe5-b2f2-875ee1ce9cb8","keyword":"冷却系统","originalKeyword":"冷却系统"},{"id":"3ee6c954-8705-4de3-b87c-efab2448456a","keyword":"液氮减压方法","originalKeyword":"液氮减压方法"}],"language":"zh","publisherId":"dwwlxb2005z1127","title":"75<span style=\"color:red\">米</span>三相交流高温超导电缆冷却系统","volume":"27","year":"2005"},{"abstractinfo":"研究了傍轴厄<span style=\"color:red\">米</span>-椭圆高斯光束在强非局域非线性介质中的传输特性.依据强非局域介质响应函数特征宽度远大于光束束宽,对非局域非线性薛定谔方程进行了近似简化,得到了介质响应函数为椭圆对称情形下的强非局域模型.在此基础上利用分离变量法得到了厄<span style=\"color:red\">米</span>-椭圆高斯空间光孤子解析解及其形成的条件.进一步研究发现,随着厄<span style=\"color:red\">米</span>-椭圆高斯空间光孤子阶数的增大,光束束宽增大,介质的非局域程度相对减弱；要获得高阶椭圆高斯空间光孤子,必须提高非局域介质的非局域程度.最低阶的厄<span style=\"color:red\">米</span>-椭圆高斯空间光孤子就是椭圆高斯空间光孤子.","authors":[{"authorName":"王清","id":"d06b5f3e-7683-4a94-872f-9c2f6c2c761d","originalAuthorName":"王清"},{"authorName":"王形华","id":"ce27e557-00ca-4876-a351-d637a96819aa","originalAuthorName":"王形华"},{"authorName":"黎东波","id":"2facbdcf-8a1c-4422-bbb6-e2eaeb05a5b9","originalAuthorName":"黎东波"},{"authorName":"刘孟连","id":"3a368e51-27e8-4bf3-a9c0-e728efe0de6d","originalAuthorName":"刘孟连"},{"authorName":"罗兴垅","id":"5e5968d5-e2be-4e9a-879e-72c2388b0c2d","originalAuthorName":"罗兴垅"}],"doi":"10.3969/j.issn.1007-5461.2012.03.015","fpage":"349","id":"8c948373-9ddb-45f0-96ce-97126dc71a31","issue":"3","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":"9672dadb-dfc7-4c91-b93d-def12b99d99c","keyword":"非线性光学","originalKeyword":"非线性光学"},{"id":"f0f461a9-3977-41f9-a70e-21c7dfa3580e","keyword":"厄<span style=\"color:red\">米</span>-椭圆高斯空间光孤子","originalKeyword":"厄米-椭圆高斯空间光孤子"},{"id":"9045f1cb-76f6-40f7-ae7e-c72a4fc412d6","keyword":"分离变量法","originalKeyword":"分离变量法"},{"id":"c19d3a25-30f1-4cb5-992b-3eae5f59fc49","keyword":"椭圆对称响应强非局域介质","originalKeyword":"椭圆对称响应强非局域介质"}],"language":"zh","publisherId":"lzdzxb201203015","title":"强非局域介质中的厄<span style=\"color:red\">米</span>-椭圆高斯空间光孤子","volume":"29","year":"2012"}],"totalpage":526,"totalrecord":5251}