{"currentpage":1,"firstResult":0,"maxresult":10,"pagecode":5,"pageindex":{"endPagecode":5,"startPagecode":1},"records":[{"abstractinfo":"反渗透专用阻垢剂的阻垢效果可通过反渗透的动态模拟实验来评价.反渗透装置以\"周期性浓缩的全循环模式\"运行,使浓水侧的饱和指数逐渐增大,碳酸钙和硫酸垢的结垢趋势逐渐增加,RO的总回收率也逐渐提高.碳酸钙和硫酸垢的沉积使得溶液的组成改变,并以此评价阻垢剂的阻垢效果.对新型反渗透专用阻垢剂<span style=\"color:red\">TJRO101</span>、传统反渗透阻垢剂SHMP及King Lee的PTP2000的动态模拟实验表明,<span style=\"color:red\">TJRO101</span>对CaCO3,CaSO4,BaSO4,SrSO4垢有极其优良的阻垢性能,是一种多功能的反渗透专用阻垢剂.","authors":[{"authorName":"张冰如","id":"aabbae42-96fc-4aab-aec6-5d30751679b0","originalAuthorName":"张冰如"}],"doi":"10.3969/j.issn.1007-8924.2006.06.014","fpage":"65","id":"8ae1785d-adef-4638-b1c5-e584e8cb79f2","issue":"6","journal":{"abbrevTitle":"MKXYJS","coverImgSrc":"journal/img/cover/MKXYJS.jpg","id":"54","issnPpub":"1007-8924","publisherId":"MKXYJS","title":"膜科学与技术   "},"keywords":[{"id":"02d15132-3b9d-4439-9b38-58ad09ab62e9","keyword":"<span style=\"color:red\">TJRO101</span>","originalKeyword":"TJRO101"},{"id":"4f5182fd-fb6b-4c0b-9b97-03e6333189a0","keyword":"反渗透","originalKeyword":"反渗透"},{"id":"b3fdfe69-7f7c-4ffb-a3ed-170f6047c85e","keyword":"阻垢剂","originalKeyword":"阻垢剂"},{"id":"4cdf3a46-efbf-4db2-ac14-fa1591da87d9","keyword":"阻垢","originalKeyword":"阻垢"},{"id":"9f8d2552-e95f-4b9f-b2b1-bf7cca5e0f71","keyword":"CaCO3","originalKeyword":"CaCO3"},{"id":"f652015e-6b1d-4791-a484-541ca5190d86","keyword":"CaSO4","originalKeyword":"CaSO4"},{"id":"1e4f233d-0f0b-4427-afe2-911d22abdd23","keyword":"BaSO4","originalKeyword":"BaSO4"},{"id":"1a11f01b-1e95-4bfc-a28b-7f6d36038c07","keyword":"SrSO4","originalKeyword":"SrSO4"}],"language":"zh","publisherId":"mkxyjs200606014","title":"反渗透专用阻垢剂<span style=\"color:red\">TJRO101</span>的阻垢性能","volume":"26","year":"2006"},{"abstractinfo":"采用扫描电镜, 对ZL<span style=\"color:red\">101</span>合金的Sr变质效果与保温时间、 Sr含量及晶粒尺寸的关系进行了研究. 结果表明: ZL<span style=\"color:red\">101</span>共晶硅的Sr变质具有长效性, 且达到最佳变质效果前有一时间间隔;加入的Sr量有一临界值, 超过此值, 变质效果变化不明显; 若共晶硅越细小, 变质效果则越好, 达到最佳变质效果的时间也随之缩短. ","authors":[{"authorName":"张静武","id":"e9bc3eee-2f8f-4133-9eba-b17122270c09","originalAuthorName":"张静武"},{"authorName":"李慧","id":"4cf58181-97e1-42ec-b805-0131a1280e67","originalAuthorName":"李慧"},{"authorName":"孟显哲","id":"5d0dbca1-e794-4de0-8323-ef2f2923b364","originalAuthorName":"孟显哲"},{"authorName":"刘春海","id":"bbb5bfbb-64d0-49b8-811b-beb3ade47422","originalAuthorName":"刘春海"}],"doi":"","fpage":"91","id":"589d3a2d-7704-4268-979b-daef5661b029","issue":"z2","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":"064789f1-fe16-44e3-9304-de64cf227528","keyword":"ZL<span style=\"color:red\">101</span>合金","originalKeyword":"ZL101合金"},{"id":"dcdf7b07-b83b-422c-b398-f6678eba97e0","keyword":"变质处理","originalKeyword":"变质处理"},{"id":"b697ed6b-6846-41af-bb94-b3d338d36563","keyword":"TPRE机制","originalKeyword":"TPRE机制"},{"id":"6837000f-43ce-4c0d-a750-2d07193e235c","keyword":"晶粒细化","originalKeyword":"晶粒细化"}],"language":"zh","publisherId":"zgysjsxb2001z2020","title":"ZL<span style=\"color:red\">101</span>合金的变质","volume":"11","year":"2001"},{"abstractinfo":"将具有正宇称的gds组态空间扩大到包含具有负宇称的1h11/2轨道, 采用修正的表面δ相互作用(MSDI)对<span style=\"color:red\">101</span>Pd和<span style=\"color:red\">101</span>Ru两个奇A 核进行了形变HF计算, 得到了基态和一些激发态的解. 同时, 还用近似角动量投影形变Hartree-Fock(PDHF)方法对<span style=\"color:red\">101</span>Pd和<span style=\"color:red\">101</span>Ru进行了能谱计算, 得到其正、负宇称带的解, 计算结果与实验谱基本一致.","authors":[{"authorName":"徐延冰","id":"1b3ba6c1-1a0a-40d8-8d0e-634c29ad7ad3","originalAuthorName":"徐延冰"}],"doi":"10.3969/j.issn.1007-4627.2003.03.003","fpage":"182","id":"8ca98726-f9ca-4b95-a219-e8c108fbc41b","issue":"3","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":"ea28bceb-8a87-4ceb-a831-8675db84565c","keyword":"角动量投影","originalKeyword":"角动量投影"},{"id":"41e3bba1-73a3-43b6-8267-e18bda970894","keyword":"单粒子能谱","originalKeyword":"单粒子能谱"},{"id":"c5c9cb2d-cbfb-46ab-8403-666a47a2276d","keyword":"负宇称带","originalKeyword":"负宇称带"}],"language":"zh","publisherId":"yzhwlpl200303003","title":"奇A核<span style=\"color:red\">101</span>Pd和<span style=\"color:red\">101</span>Ru的负宇称带能谱研究","volume":"20","year":"2003"},{"abstractinfo":"Mg在室温下的强度和塑性较差, 其根源之一在于Mg的{<span style=\"color:red\">101</span>ˉ2}形变孪晶在极低的应力下即可形核和扩展, 而且研究表明目前应用于镁合金的时效强化法通常无法显著抑制{<span style=\"color:red\">101</span>ˉ2}形变孪晶. 尽管对Mg 及其合金的力学性能至关重要, 迄今为止, 对{<span style=\"color:red\">101</span>ˉ2}形变孪晶的形核和扩展的机制仍存在很大争议. 本文首先回顾了有关形变孪晶的定义以及{<span style=\"color:red\">101</span>ˉ2}孪晶机制的研究历史, 然后着重介绍了最新的基于原位TEM的研究结果: 即Mg的{<span style=\"color:red\">101</span>ˉ2}形变孪晶迥异于孪晶的经典定义, 它事实上是一种新的室温变形机制, 即塑性的产生可以通过局部的晶胞重构来完成, 而不需要孪晶位错的参与; 由晶胞重构机制所产生的界面为{0002}/{<span style=\"color:red\">101</span>ˉ0}界面(BP 界面), 而且该界面在三维空间呈现梯田状的不规则形貌. 晶胞重构机制迥异于基于位错的孪晶变形机制, 因此基于对该机制进行抑制的设计思路可能是开发未来高强韧镁合金的关键.","authors":[{"authorName":"单智伟","id":"e8835d4e-8ddf-4696-ba97-c368b95d0ebd","originalAuthorName":"单智伟"},{"authorName":"刘博宇","id":"2d1a7796-f7da-47e0-8816-eb13d64e2586","originalAuthorName":"刘博宇"}],"doi":"10.11900/0412.1961.2016.00369","fpage":"1267","id":"83990ffd-0bde-45be-946c-04fe3079f620","issue":"10","journal":{"abbrevTitle":"JSXB","coverImgSrc":"journal/img/cover/JSXB.jpg","id":"48","issnPpub":"0412-1961","publisherId":"JSXB","title":"金属学报"},"keywords":[{"id":"52e2ab3f-4104-4886-bbb5-9956068fc7b2","keyword":"Mg","originalKeyword":"Mg"},{"id":"bc9622a7-585e-4194-83db-69cba73c8824","keyword":"形变孪晶","originalKeyword":"形变孪晶"},{"id":"ae16010d-f9dd-42f3-9ce0-492e9a07c023","keyword":"基面-柱面界面","originalKeyword":"基面-柱面界面"},{"id":"5b4d84e5-bbf4-4ace-ac56-41dea3884d17","keyword":"强度","originalKeyword":"强度"},{"id":"9aad8ff8-7cfe-4bae-ac1e-7be8bc0543d4","keyword":"合金设计","originalKeyword":"合金设计"}],"language":"zh","publisherId":"0412-1961(2016)10-1267-12","title":"Mg的{<span style=\"color:red\">101</span>ˉ2}形变孪晶机制","volume":"52","year":"2016"},{"abstractinfo":"采用不同的时效工艺,研究了时效温度和时间对ZL<span style=\"color:red\">101</span>A合金性能的影响,得出了该合金较理想的时效制度,在此制度下,ZL<span style=\"color:red\">101</span>A合金的金属型典型性能达到σb≥330MPa,δ5≥10%,为满足航空、航天等领域对高性能铝合金精密铸件的需求奠定了材料基础.","authors":[{"authorName":"洪润洲","id":"b39ccbef-fd3b-400e-87e0-bfcdeec28a2f","originalAuthorName":"洪润洲"},{"authorName":"周永江","id":"3e48dd5e-6596-4f83-8a4d-55cc76148fea","originalAuthorName":"周永江"},{"authorName":"姚惟斌","id":"e652ffd4-f3e7-43fc-98fe-cbc4b0a284b3","originalAuthorName":"姚惟斌"}],"doi":"10.3969/j.issn.1001-4381.2004.10.010","fpage":"39","id":"bbd74173-5c94-43dd-96a6-d3dfd40a1b9d","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":"df8d8859-48fd-4a7d-bcdb-00dd83c19a74","keyword":"ZL<span style=\"color:red\">101</span>A合金","originalKeyword":"ZL101A合金"},{"id":"c2e0912b-e8f6-4c70-b53b-469d6af7b50f","keyword":"时效工艺","originalKeyword":"时效工艺"},{"id":"ee449b87-f827-44b9-b062-6436fc9fdd0a","keyword":"力学性能","originalKeyword":"力学性能"}],"language":"zh","publisherId":"clgc200410010","title":"时效工艺对ZL<span style=\"color:red\">101</span>A合金性能的影响","volume":"","year":"2004"},{"abstractinfo":"采用半固态合金二次加热, 对半固态坯料施加合理的二次加热路径, 重新获得适于后续加工的具有近球状固相颗粒均匀分布的半固态组织.采用功率为20kW, 频率为30kHz的高频感应加热装置, 研究了采用再熔融加热法制备的ZL<span style=\"color:red\">101</span>半固态合金坯料的二次加热过程.结果表明: 为了获得适于最终成形的半固态组织, 有必要把半固态坯料二次加热过程分为几个加热速率不同的加热阶段, 然后在半固态温度区间某一需要加工温度下进行适度保温.通过实验给出了ZL<span style=\"color:red\">101</span>合金半固态坯料二次加热条件, 并讨论了二次加热条件对半固态组织演化的影响.","authors":[{"authorName":"杨红亮","id":"a7ee42c7-1169-45f5-aad8-b391cfb87572","originalAuthorName":"杨红亮"},{"authorName":"张质良","id":"7e6ea808-74c1-47d7-a144-bfe6098ac057","originalAuthorName":"张质良"},{"authorName":"","id":"fad9d041-c702-48b6-ae0a-03638babc5fd","originalAuthorName":""},{"authorName":"","id":"3c38b201-4c1f-49c1-860a-d17af8be8975","originalAuthorName":""},{"authorName":"","id":"1e937893-1dba-4b8e-a09f-a472eb6acef7","originalAuthorName":""},{"authorName":"","id":"d6fabbfc-540b-41ae-88aa-f70f7250d04a","originalAuthorName":""}],"doi":"","fpage":"626","id":"3369a482-4cb7-4db7-910d-f563325156c1","issue":"3","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":"3ac63bcc-c2f9-4f20-b00e-5486c5479036","keyword":"再熔融加热法","originalKeyword":"再熔融加热法"},{"id":"9fe2f8cd-06e8-4268-979b-4c3dbc15b127","keyword":"半固态合金","originalKeyword":"半固态合金"},{"id":"0340f19a-fb94-450a-8219-ef869bb13d8e","keyword":"二次加热","originalKeyword":"二次加热"},{"id":"f45b9307-e3ad-4c97-b26a-032d0ea55c29","keyword":"组织演化","originalKeyword":"组织演化"}],"language":"zh","publisherId":"zgysjsxb200303017","title":"ZL<span style=\"color:red\">101</span>合金半固态二次加热","volume":"13","year":"2003"},{"abstractinfo":"使用扫描电子显微镜和光学显微镜对ZL<span style=\"color:red\">101</span>铝合金的显微组织、拉伸断口及断口剖面进行了观察分析,研究了其拉伸断裂特征.结果表明:ZL<span style=\"color:red\">101</span>铝合金的拉伸断口为准解理特征,可见第二相(硅共晶体和AlFeMnSi相)沿断口分布;裂纹在第二相粒子的尖锐和凹角处(即应力集中处)萌生,并沿第二相扩展,该过程会拉开(拉断)第二相粒子,并使横向粒子产生变形;韧窝特征是由脆性第二相被拉开后发生塑性变形产生;舌状花样是裂纹沿一定取向晶面扩展,并造成颗粒相变形产生;撕裂棱是裂纹扩展至两个以一定角度相交的第二相时,扩展方向发生较大改变产生.","authors":[{"authorName":"刘洲","id":"0f50cdb7-df00-4d82-bca9-b879f5286799","originalAuthorName":"刘洲"},{"authorName":"何玉怀","id":"dd053d53-edff-42d3-8818-c61d57b632b3","originalAuthorName":"何玉怀"},{"authorName":"刘昌奎","id":"0a080653-6062-4b2a-bf18-e28c37d8fd21","originalAuthorName":"刘昌奎"},{"authorName":"姜涛","id":"2429319f-6429-4be3-a127-f0700ada3aeb","originalAuthorName":"姜涛"},{"authorName":"刘德林","id":"c352d8b1-76b1-487d-8b42-3a9415713eb7","originalAuthorName":"刘德林"}],"doi":"","fpage":"82","id":"af7794c3-e58a-4f42-8f41-1fd01a43c898","issue":"2","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":"d9a7b783-3ead-4855-aae7-fb646a61aa63","keyword":"ZL<span style=\"color:red\">101</span>铝合金","originalKeyword":"ZL101铝合金"},{"id":"c6e8be7c-27c9-483f-a181-6619ff02dfce","keyword":"拉伸断口","originalKeyword":"拉伸断口"},{"id":"4328c4e0-21ce-42e6-a509-e382d9d4abfe","keyword":"准解理","originalKeyword":"准解理"},{"id":"d8e21a4e-3b51-4db5-916e-7cac764f9319","keyword":"第二相","originalKeyword":"第二相"},{"id":"3e2a135b-9eb8-48f8-9911-c92aa92bed80","keyword":"断口截面","originalKeyword":"断口截面"}],"language":"zh","publisherId":"jxgccl201402019","title":"ZL<span style=\"color:red\">101</span>铝合金的拉伸断裂特征","volume":"38","year":"2014"},{"abstractinfo":"采用微波辐射法合成MIL-<span style=\"color:red\">101</span>多孔材料,探讨了反应温度对材料合成的影响.同时对MIL-<span style=\"color:red\">101</span>进行XRD测试以及孔结构和比表面积分析,采用重量法测定了288、298和308K条件下苯在MIL-<span style=\"color:red\">101</span>多孔材料上的吸附等温线,并估算MIL-<span style=\"color:red\">101</span>对苯的等量吸附热.结果表明,MIL-<span style=\"color:red\">101</span>多孔材料的比表面积达2089.2m2/g ,苯在MIL-<span style=\"color:red\">101</span>上的吸附等温线呈I型等温线,与Langmuir模型吻合很好,表明吸附主要为微孔吸附;随着温度的升高,MIL-<span style=\"color:red\">101</span>对苯的平衡吸附量逐渐下降,说明苯在MIL-<span style=\"color:red\">101</span>多孔材料的吸附以物理吸附为主.在T=298K,p/p0=0.5 时,苯在MIL-<span style=\"color:red\">101</span>多孔材料上的吸附量为9.44mmol/g,远高于同等条件下普通活性炭和活性炭纤维对苯的吸附容量;苯在MIL-<span style=\"color:red\">101</span>上的等量吸附热为45.4～41.6kJ/mol的范围,其等量吸附热随着表面吸附量的增加变化幅度不大,与活性炭纤维相比,MIL-<span style=\"color:red\">101</span>的表面吸附自由能分布比较均匀.","authors":[{"authorName":"黄思思","id":"8a238ba1-c43b-422e-8383-526e9c1154cc","originalAuthorName":"黄思思"},{"authorName":"夏启斌","id":"86a9fba7-776b-4289-b8c0-e58638a4f525","originalAuthorName":"夏启斌"},{"authorName":"李忠","id":"36dadbe8-2e24-4ae6-b5a9-06e64f3a905c","originalAuthorName":"李忠"},{"authorName":"朱宝璋","id":"d614badb-c077-4ed3-81d6-1f98d6e65d45","originalAuthorName":"朱宝璋"}],"doi":"","fpage":"961","id":"4edb341e-cb6a-4f7b-ab40-43a5fcfad763","issue":"6","journal":{"abbrevTitle":"GNCL","coverImgSrc":"journal/img/cover/GNCL.jpg","id":"33","issnPpub":"1001-9731","publisherId":"GNCL","title":"功能材料"},"keywords":[{"id":"f5df611b-12d1-44cf-8a78-3cf6f6b869af","keyword":"MIL-<span style=\"color:red\">101</span>","originalKeyword":"MIL-101"},{"id":"4321fd3d-efd9-49b6-a64f-db506fa56b35","keyword":"微波合成","originalKeyword":"微波合成"},{"id":"109122a2-3054-47b4-99cc-3eed8b79adc3","keyword":"苯吸附","originalKeyword":"苯吸附"},{"id":"9b465bfc-5e48-4ef3-8500-6d71691e9f1d","keyword":"等量吸附热","originalKeyword":"等量吸附热"}],"language":"zh","publisherId":"gncl201006009","title":"微波辐射合成MIL-<span style=\"color:red\">101</span>多孔材料及其对苯的吸附热","volume":"41","year":"2010"},{"abstractinfo":"采用失重法、表面观察法和极化曲线法研究了缓蚀剂浓度、溶液的pH值、Cl-、Ca2+和温度等诸因素对XM-<span style=\"color:red\">101</span>磷系缓蚀剂缓蚀效果的影响.结果发现:当XM-<span style=\"color:red\">101</span>浓度为75mg/L,溶液的pH值为7.15时,XM-<span style=\"color:red\">101</span>对自来水中碳钢的缓蚀率接近100%.","authors":[{"authorName":"郭良生","id":"f9859327-19af-41c3-9aa1-926966ce1ecb","originalAuthorName":"郭良生"},{"authorName":"黄霓裳","id":"c552aaca-2ac0-4848-be3d-f786286ab98d","originalAuthorName":"黄霓裳"},{"authorName":"余兴增","id":"675564ea-4f3b-4fdf-a6ca-8d5660451f4f","originalAuthorName":"余兴增"},{"authorName":"石小燕","id":"b07f6627-b1af-463b-9933-6e2a1f912021","originalAuthorName":"石小燕"},{"authorName":"邱富荣","id":"bc3648ca-86b8-4046-901b-eb5895406ddd","originalAuthorName":"邱富荣"}],"doi":"10.3969/j.issn.1005-748X.2000.12.002","fpage":"533","id":"7cc75580-d6c1-4bbb-9b9f-8b938983300c","issue":"12","journal":{"abbrevTitle":"FSYFH","coverImgSrc":"journal/img/cover/FSYFH.jpg","id":"25","issnPpub":"1005-748X","publisherId":"FSYFH","title":"腐蚀与防护"},"keywords":[{"id":"7fe197e5-ddf8-4223-9691-09c3fd93d21e","keyword":"缓蚀剂","originalKeyword":"缓蚀剂"},{"id":"27c46a97-488d-489d-b176-c2628d8901c4","keyword":"自来水","originalKeyword":"自来水"},{"id":"95ab819a-8d0d-4acc-a09b-034c0b091245","keyword":"碳钢","originalKeyword":"碳钢"},{"id":"bfd7467c-4cdd-4b94-b9ce-edff10228892","keyword":"腐蚀","originalKeyword":"腐蚀"},{"id":"de44e1a7-44fd-433c-a3b4-44970c09a11f","keyword":"抑制","originalKeyword":"抑制"}],"language":"zh","publisherId":"fsyfh200012002","title":"各种因素对XM-<span style=\"color:red\">101</span>磷系缓蚀剂缓蚀效果的影响","volume":"21","year":"2000"},{"abstractinfo":"采用真空热压烧结工艺制备含SiC颗粒体积分数为10％、20％、30％和40％的SiC／ZL<span style=\"color:red\">101</span>A复合材料,研究普通磨削与超声纵向振动磨削SiCp/ZL<span style=\"color:red\">101</span>A复合材料时的SiC颗粒去除机制,并探索不同磨削方式对工件表面微观形貌、表面粗糙度的影响.结果表明:在相同磨削参数下,超声纵向振动磨削表面的粗糙度低于普通磨削表面的粗糙度；无论是超声纵向振动磨削还是普通磨削,SiCp/ZL<span style=\"color:red\">101</span>A复合材料的表面粗糙度均随着增强体SiC颗粒体积分数的增大而增大.","authors":[{"authorName":"王狂飞","id":"33d11e26-9909-44ec-b2eb-c2ede44b2d9a","originalAuthorName":"王狂飞"},{"authorName":"胡玉昆","id":"453b91a9-1bfd-48ba-a91b-2d319b94937e","originalAuthorName":"胡玉昆"},{"authorName":"郑喜军","id":"45e8a854-c085-45ed-a341-a78bc15c05c2","originalAuthorName":"郑喜军"},{"authorName":"米国发","id":"e58b8ea3-288d-4128-914c-4680e7899f8b","originalAuthorName":"米国发"}],"doi":"33-1331/TJ.20111226.2315.009","fpage":"39","id":"7f0d2bc7-33ba-4e19-a7b7-effedb2e214e","issue":"1","journal":{"abbrevTitle":"BQCLKXYGC","coverImgSrc":"journal/img/cover/BQCLKXYGC.jpg","id":"4","issnPpub":"1004-244X","publisherId":"BQCLKXYGC","title":"兵器材料科学与工程   "},"keywords":[{"id":"168f2d4b-11fa-49b5-809f-f25d747f212e","keyword":"复合材料","originalKeyword":"复合材料"},{"id":"80bf2400-2a97-4a6a-bbe8-d1c05251f14c","keyword":"超声磨削","originalKeyword":"超声磨削"},{"id":"acf9366c-66e5-454a-8b95-23f5b800143a","keyword":"表面质量","originalKeyword":"表面质量"}],"language":"zh","publisherId":"bqclkxygc201201012","title":"SiCp/ZL<span style=\"color:red\">101</span>A复合材料超声振动磨削试验研究","volume":"35","year":"2012"}],"totalpage":54,"totalrecord":531}