{"currentpage":1,"firstResult":0,"maxresult":10,"pagecode":5,"pageindex":{"endPagecode":5,"startPagecode":1},"records":[{"abstractinfo":"自动控制系统是一门建立在数学计算和物理理论基础上的体系完整、逻辑严密的独立学科.在研究自动控制系统之前建立一个数学模型是为了更简捷地描述<span style=\"color:red\">输出</span><span style=\"color:red\">变量</span><span style=\"color:red\">与</span><span style=\"color:red\">输入</span><span style=\"color:red\">变量</span>之间的关系.数学模型在自动控制系统的应用是为了将自动控制系统迈进信息时代和计算机时代的步伐更大些、更快些.研究了数学建模<span style=\"color:red\">与</span>自动控制系统两者之间的关系.","authors":[{"authorName":"姚融融","id":"3634f022-dfe8-417a-a8c4-fe28340b8dfb","originalAuthorName":"姚融融"},{"authorName":"陈玮","id":"f1217aad-bf92-426f-bf58-ee5c4b7fc9d2","originalAuthorName":"陈玮"},{"authorName":"贺向阳","id":"eccb428d-0088-478f-bf2c-ac99ee7c625d","originalAuthorName":"贺向阳"}],"doi":"10.3969/j.issn.1001-0777.2005.02.008","fpage":"29","id":"977d7225-49cf-4266-88fc-6fe3961cf6aa","issue":"2","journal":{"abbrevTitle":"WLCS","coverImgSrc":"journal/img/cover/WLCS.jpg","id":"64","issnPpub":"1001-0777","publisherId":"WLCS","title":"物理测试"},"keywords":[{"id":"abb5180d-0eb1-4d85-9d5e-6617449a826c","keyword":"数学模型","originalKeyword":"数学模型"},{"id":"1952203c-da76-4f86-b802-665cfb29ffab","keyword":"<span style=\"color:red\">输出</span><span style=\"color:red\">变量</span><span style=\"color:red\">与</span><span style=\"color:red\">输入</span><span style=\"color:red\">变量</span>","originalKeyword":"输出变量与输入变量"},{"id":"6e8bb791-fddf-48e9-b677-1a9f3ecd2535","keyword":"自动控制系统","originalKeyword":"自动控制系统"}],"language":"zh","publisherId":"wlcs200502008","title":"数学模型<span style=\"color:red\">与</span>自动控制系统","volume":"23","year":"2005"},{"abstractinfo":"分析讨论了烘烤硬化钢板的BH值<span style=\"color:red\">与</span>预应<span style=\"color:red\">变量</span>关系的不同观点,研究了成分为0.11C-1.67Mn-1.19Si的DP和TRIP钢板的BH值<span style=\"color:red\">与</span>预应<span style=\"color:red\">变量</span>的关系,并尝试做出合理的解释.","authors":[{"authorName":"张继诚","id":"ef4e0854-c323-4516-8323-73bc8eb8fd49","originalAuthorName":"张继诚"},{"authorName":"符仁钰","id":"f08bd805-a44c-4a76-bd4c-889c80a38bad","originalAuthorName":"符仁钰"},{"authorName":"张梅","id":"826d566a-7aac-4463-a36c-84d164bf1c60","originalAuthorName":"张梅"},{"authorName":"李麟","id":"27bda3ee-5b3a-49e9-b0ed-564fe3af29ac","originalAuthorName":"李麟"}],"doi":"10.3969/j.issn.1001-7208.2006.06.004","fpage":"18","id":"d134c3e6-d4fc-4469-8460-878c627cf334","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":"d44f870c-6630-46a4-b57b-b9ebfce78baa","keyword":"烘烤硬化(BH)钢","originalKeyword":"烘烤硬化(BH)钢"},{"id":"625c1f62-aeae-4b06-923b-9c19234c36be","keyword":"双相(DP)钢","originalKeyword":"双相(DP)钢"},{"id":"504f9d7f-ac6e-4710-b751-e0cf2410fbd3","keyword":"相变诱发塑性(TRIP)钢","originalKeyword":"相变诱发塑性(TRIP)钢"},{"id":"48408d75-10fd-408d-b85a-22ea12fa721b","keyword":"BH值","originalKeyword":"BH值"},{"id":"0d7d5d63-fd15-49ed-bf72-fbf691979523","keyword":"预应变","originalKeyword":"预应变"}],"language":"zh","publisherId":"shjs200606004","title":"新型汽车钢板的BH值<span style=\"color:red\">与</span>预应<span style=\"color:red\">变量</span>的关系","volume":"28","year":"2006"},{"abstractinfo":"用XRD研究了Yb-Ce-TZP断裂前后的相组成.分析了烧结温度、相对密度、稳定剂及晶粒尺寸<span style=\"color:red\">与</span>相<span style=\"color:red\">变量</span>间的关系讨论了相<span style=\"color:red\">变量</span>对力学性能的决定作用发现:复合稳定剂可显著提高断裂相<span style=\"color:red\">变量</span>,有效改善TZP的力学性能稳定剂含量为0.75%Yb2O3imi+9%CeO2(mol百分数)时可获得最大断裂相<span style=\"color:red\">变量</span>,其力学性能显著优于Yb-TZP和Ce-TZP.","authors":[{"authorName":"毛骏飙","id":"d2d1dd88-5375-4449-84b7-936946a6057d","originalAuthorName":"毛骏飙"},{"authorName":"陈楷","id":"98876838-c028-4322-9480-7e6ebdff5741","originalAuthorName":"陈楷"},{"authorName":"陈少贞","id":"4245ec17-f04e-489d-ba9f-1057b92af8e6","originalAuthorName":"陈少贞"},{"authorName":"林小莲","id":"d193562c-dab6-49c0-a941-e2278292ce9c","originalAuthorName":"林小莲"}],"categoryName":"|","doi":"","fpage":"52","id":"891d371d-f6f3-4abb-a0ea-94b27d7041a1","issue":"1","journal":{"abbrevTitle":"CLYJXB","coverImgSrc":"journal/img/cover/CLYJXB.jpg","id":"16","issnPpub":"1005-3093","publisherId":"CLYJXB","title":"材料研究学报"},"keywords":[{"id":"a093fd0c-4c3d-4b30-8c3a-022c1fd9301b","keyword":"Yb-Ce-TZP增韧陶瓷","originalKeyword":"Yb-Ce-TZP增韧陶瓷"},{"id":"2abf2e68-5187-4ac1-99c2-f153d95d6a0e","keyword":"toughening ceramics","originalKeyword":"toughening ceramics"},{"id":"7fbd63eb-bfb0-4593-8c4a-d30aaad0d860","keyword":" phase transformation","originalKeyword":" phase transformation"}],"language":"zh","publisherId":"1005-3093_1998_1_4","title":"Yb-Ce-TZP的断裂相<span style=\"color:red\">变量</span><span style=\"color:red\">与</span>力学性能","volume":"12","year":"1998"},{"abstractinfo":"采用ECC和EBSD技术研究了AA1050铝合金冷轧到大应<span style=\"color:red\">变量</span>下微观组织和织构的演变规律. 结果表明, AA1050合金冷轧到 大形<span style=\"color:red\">变量</span>时, 微观组织由低应变下的胞块组织结构转变成典型的层片状界面 (LBs)结构, 其内部的LBs基本<span style=\"color:red\">与</span>轧向 (RD) 平行; 主要存 在两种转变机制, 即由于轧制变形 (机制I) 和借助于S--bands结构的剪切作用 (机制II),从而导致GNBs逐渐旋转到<span style=\"color:red\">与</span>RD平行, 且以 机制I为主. 变形过程中, 由于晶粒的分裂形成大量的大角度界面, 随应变的增加, 大角度界面的间距逐渐减小、 数目逐渐增多; 当冷轧到90%应<span style=\"color:red\">变量</span>时, 除原始晶界外, 约为47%的大角度界面起源于变形诱导的界面. 冷轧变形主要形成典型的Brass+S+Copper轧制织构, 且强度随应变的增加而逐渐增加.","authors":[{"authorName":"姚宗勇刘庆A.Godfrey刘伟","id":"86946192-bebc-4d27-a180-0af5922ae015","originalAuthorName":"姚宗勇刘庆A.Godfrey刘伟"}],"categoryName":"|","doi":"","fpage":"647","id":"ca257e57-d1a2-4c81-9c53-04a9cb3eb1d9","issue":"6","journal":{"abbrevTitle":"JSXB","coverImgSrc":"journal/img/cover/JSXB.jpg","id":"48","issnPpub":"0412-1961","publisherId":"JSXB","title":"金属学报"},"keywords":[{"id":"fd7c9d84-6536-43c7-b176-46abf2cfcb30","keyword":"铝合金","originalKeyword":"铝合金"},{"id":"f574bc63-de97-44bf-8c80-776188b43d0d","keyword":" cold rolling","originalKeyword":" cold rolling"},{"id":"5c3aa961-25ae-4775-a8b1-81281c46ac8c","keyword":" electron backscattered diffraction (EBSD)","originalKeyword":" electron backscattered diffraction (EBSD)"},{"id":"8b3421be-e09f-4bf6-b0e7-050bdcbe9160","keyword":"microstructure","originalKeyword":"microstructure"},{"id":"5b77cea2-2694-40f1-b6c3-a81f0594f710","keyword":"texture","originalKeyword":"texture"}],"language":"zh","publisherId":"0412-1961_2009_6_7","title":"大应<span style=\"color:red\">变量</span>冷轧AA1050铝合金微观组织<span style=\"color:red\">与</span>织构的演变","volume":"45","year":"2009"},{"abstractinfo":"采用ECC和EBSD技术研究了AA1050铝合金冷轧到大应<span style=\"color:red\">变量</span>下微观组织和织构的演变规律. 结果表明,AA1050合金冷轧到大形<span style=\"color:red\">变量</span>时,微观组织由低应变下的胞块组织结构转变成典型的层片状界面(LBs)结构,其内部的LBs基本<span style=\"color:red\">与</span>轧向(RD)平行;主要存在两种转变机制,即由于轧制变形(机制I)和借助于S-bands结构的剪切作用(机制II),从而导致GNBs逐渐旋转到<span style=\"color:red\">与</span>RD平行,且以机制I为主.变形过程中,由于晶粒的分裂形成大量的大角度界面,随应变的增加,大角度界面的间距逐渐减小、数目逐渐增多;当冷轧到90%应<span style=\"color:red\">变量</span>时,除原始晶界外,约为47%的大角度界面起源于变形诱导的界面. 冷轧变形主要形成典型的Brass+S+Copper轧制织构,且强度随应变的增加而逐渐增加.","authors":[{"authorName":"姚宗勇","id":"60ebda5e-a756-491c-ada1-f89d97b6aa1d","originalAuthorName":"姚宗勇"},{"authorName":"刘庆","id":"d77b1d74-5e39-4d0c-ad1b-5c8fd979656f","originalAuthorName":"刘庆"},{"authorName":"A.Godfrey","id":"16ea1588-bccd-4905-8762-1b0c22c69363","originalAuthorName":"A.Godfrey"},{"authorName":"刘伟","id":"a3d568f9-747a-43f1-84ae-3fc12103f7d6","originalAuthorName":"刘伟"}],"doi":"10.3321/j.issn:0412-1961.2009.06.002","fpage":"647","id":"90d1db06-7ad8-4af7-8f61-b9d258c05f57","issue":"6","journal":{"abbrevTitle":"JSXB","coverImgSrc":"journal/img/cover/JSXB.jpg","id":"48","issnPpub":"0412-1961","publisherId":"JSXB","title":"金属学报"},"keywords":[{"id":"da1c9b35-823f-430d-b3e2-8d79f83ae87a","keyword":"铝合金","originalKeyword":"铝合金"},{"id":"2647e4fb-898f-4e08-8efa-38bb41384347","keyword":"冷轧","originalKeyword":"冷轧"},{"id":"5bd5a6c7-747d-4e2d-a8e5-6efc7ff890de","keyword":"电子背散射衍射","originalKeyword":"电子背散射衍射"},{"id":"1e230656-9631-4316-a49c-87127b1c6c99","keyword":"微观组织","originalKeyword":"微观组织"},{"id":"16e2af7b-a5a0-4025-9cbb-1b8aa17bdd94","keyword":"织构","originalKeyword":"织构"}],"language":"zh","publisherId":"jsxb200906002","title":"大应<span style=\"color:red\">变量</span>冷轧AA1050铝合金微观组织<span style=\"color:red\">与</span>织构的演变","volume":"45","year":"2009"},{"abstractinfo":"就多晶体弹塑性材料在疲劳载荷作用下从宏观裂纹的形成、扩展直至断裂的裂纹扩展阶段,提出了用损伤<span style=\"color:red\">变量</span>D2作为本阶段强度<span style=\"color:red\">与</span>寿命的计算参量,提出了这个过程描述材料疲劳断裂行为的新方程,并使这些方程<span style=\"color:red\">与</span>现有广泛应用的其他方程相互沟通,从而对某些材料行为的变化规律形成一个整体的认识,以便于工程界能广泛地理解、接受和应用.","authors":[{"authorName":"虞岩贵","id":"70912e11-221c-4631-a813-e8fe2c331da2","originalAuthorName":"虞岩贵"}],"doi":"10.3969/j.issn.1001-4381.2003.z1.088","fpage":"264","id":"48fe6fb0-0576-4e2a-a080-c5ca41a0c864","issue":"z1","journal":{"abbrevTitle":"CLGC","coverImgSrc":"journal/img/cover/CLGC.jpg","id":"9","issnPpub":"1001-4381","publisherId":"CLGC","title":"材料工程"},"keywords":[{"id":"e57b0fb4-3251-4fa8-a046-984299955c95","keyword":"第二阶段损伤<span style=\"color:red\">变量</span>","originalKeyword":"第二阶段损伤变量"},{"id":"872e51fe-5050-47b5-81f7-b724e9b36ae6","keyword":"裂尖应力强度","originalKeyword":"裂尖应力强度"},{"id":"4b26ccaa-973a-48bb-9ce7-fa3e814edc8c","keyword":"损伤J积分","originalKeyword":"损伤J积分"},{"id":"d820c8b5-e80c-4c2f-a9e0-07939d1adcbf","keyword":"损伤张开位移","originalKeyword":"损伤张开位移"}],"language":"zh","publisherId":"clgc2003z1088","title":"用损伤<span style=\"color:red\">变量</span>D2作为裂纹扩展阶段强度<span style=\"color:red\">与</span>寿命的计算参量","volume":"","year":"2003"},{"abstractinfo":"研究了Ni含量(1.5wt%-7.0wt%)<span style=\"color:red\">与</span>预应<span style=\"color:red\">变量</span>对Fe-Mn-Si-Cr-Ni合金的影响.对不同Ni含量下合金的力学性能、形状记忆恢复率<span style=\"color:red\">与</span>不同预应<span style=\"color:red\">变量</span>下合金的形状记忆恢复率进行了分析,并通过TEM观察其中两种合金的显微结构.结果表明,Fe-Mn-Si-Cr-Ni合金中,△σ(即σb-σ0.2)越大,合金的最大形状记忆恢复率就越大;含Ni量为3.15wt%的合金在预应力作用下,易形成高密度且具有层错亚结构、位向单一的ε马氏体,从而具有最好的形状记忆效应.","authors":[{"authorName":"胡锐","id":"dd230dc2-35f0-4d4a-9333-ce94a39c4dde","originalAuthorName":"胡锐"},{"authorName":"潘红雄","id":"d6ccd024-760e-41da-be9c-22af085cf8b8","originalAuthorName":"潘红雄"},{"authorName":"李金山","id":"452f46f3-0b60-4f7e-a7d7-ef39960d36eb","originalAuthorName":"李金山"},{"authorName":"王新虎","id":"342d3d8c-f8b9-4c46-9894-2b50d833b5e0","originalAuthorName":"王新虎"},{"authorName":"赵新伟","id":"48567169-a899-4da3-bf26-2a122595b0dc","originalAuthorName":"赵新伟"},{"authorName":"傅恒志","id":"d3a2828e-ea05-4bca-aae6-d452008fd5e4","originalAuthorName":"傅恒志"}],"doi":"10.3969/j.issn.1009-6264.2006.04.003","fpage":"11","id":"8f24ddb5-bb6d-4f18-97cc-bac0a3eddd15","issue":"4","journal":{"abbrevTitle":"CLRCLXB","coverImgSrc":"journal/img/cover/CLRCLXB.jpg","id":"15","issnPpub":"1009-6264","publisherId":"CLRCLXB","title":"材料热处理学报"},"keywords":[{"id":"c06522e7-53b2-412a-8f76-62fa822e3a02","keyword":"形状记忆合金","originalKeyword":"形状记忆合金"},{"id":"b2da440d-8d00-4651-a386-fe51fb3a32f6","keyword":"形状记忆效应","originalKeyword":"形状记忆效应"},{"id":"98ebedcf-73ad-4180-af88-3048c4e6a0ca","keyword":"马氏体","originalKeyword":"马氏体"}],"language":"zh","publisherId":"jsrclxb200604003","title":"Ni含量<span style=\"color:red\">与</span>预应<span style=\"color:red\">变量</span>对Fe基形状记忆合金形状记忆效应的影响","volume":"27","year":"2006"},{"abstractinfo":"本文探讨研究IGCC系统无约束时多<span style=\"color:red\">变量</span>综合优化设计及其系统性能特性规律.本文通过IGCC系统热力特性分析,确定了系统的独立<span style=\"color:red\">变量</span>,并基于有关部件通用模型组建了IGCC系统通用模型,为无燃气轮机母型硬件约束时的综合优化设计奠定了基础.结合典型实例的模拟分析,揭示了有别于现行的有约束的设计优化的系统性能特性规律.从而提出IGCC系统无约束综合优化分析的新方法.","authors":[{"authorName":"迟全虎","id":"c1967589-bf77-40ee-95b9-ea6d47feadb2","originalAuthorName":"迟全虎"},{"authorName":"林汝谋","id":"4af5d7cb-a408-4799-b70d-9d59a8196daa","originalAuthorName":"林汝谋"},{"authorName":"邓润亚","id":"8cfaee85-e714-4f3a-b9b1-3c4691818110","originalAuthorName":"邓润亚"},{"authorName":"邓世敏","id":"28301b8a-5a9f-45e6-8038-0f8789304cd5","originalAuthorName":"邓世敏"},{"authorName":"金红光","id":"40f4bea4-ba8d-4680-8a7b-b66c0d69bb13","originalAuthorName":"金红光"}],"doi":"","fpage":"361","id":"e60d1fe8-0615-4762-bbae-7de8e77e39e4","issue":"3","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":"7948b3c5-0565-4fa0-87cc-6d5de0e0c6c1","keyword":"IGCC","originalKeyword":"IGCC"},{"id":"5a4bc282-cf6c-4e6d-885f-07738a7b9efa","keyword":"多<span style=\"color:red\">变量</span>","originalKeyword":"多变量"},{"id":"1bbc4484-59e8-4a8e-b0ff-7235073569dc","keyword":"特性规律","originalKeyword":"特性规律"},{"id":"a7f7ce8a-268e-4fc1-9064-fc6462889b73","keyword":"优化设计","originalKeyword":"优化设计"}],"language":"zh","publisherId":"gcrwlxb200403001","title":"IGCC系统多<span style=\"color:red\">变量</span>综合优化设计","volume":"25","year":"2004"},{"abstractinfo":"在量子信息科学中,量子克隆理论是基础理论,它提供量子密码术的绝对安全性.得到d维空间最优1→M=d+1相位协<span style=\"color:red\">变量</span>子克隆的具体变换,然后将这种克隆机推广到1→M=kd+1(k为整数)情况,并得到具体的变换.利用2维空间非最优2→M=2k+1相位协<span style=\"color:red\">变量</span>子克隆的形式,得到最优的克隆变换.两种类型的量子克隆机的拷贝忠信度符合已有的理论值.","authors":[{"authorName":"张刚","id":"51930ee2-0506-4033-a70d-2d737ed6d45e","originalAuthorName":"张刚"},{"authorName":"潘国柱","id":"df52316e-8300-4b97-acb2-5803067f8b2e","originalAuthorName":"潘国柱"},{"authorName":"袁好","id":"6198720f-c6f0-468c-94bc-26699f90b111","originalAuthorName":"袁好"}],"doi":"10.3969/j.issn.1007-5461.2015.04.009","fpage":"438","id":"e81c142c-3830-4979-b8ba-0d027370999d","issue":"4","journal":{"abbrevTitle":"LZ","coverImgSrc":"journal/img/cover/LZ.jpg","id":"52","issnPpub":"1005-4006","publisherId":"LZ","title":"连铸"},"keywords":[{"id":"7762c6ee-07c0-4e21-a5f3-6b2a292615ce","keyword":"量子信息","originalKeyword":"量子信息"},{"id":"39eacba8-fb96-4ce9-84df-96d40cbf1378","keyword":"量子密码术","originalKeyword":"量子密码术"},{"id":"e808bfa2-db2a-4fbd-9bca-7b9bc5b06d1c","keyword":"量子克隆","originalKeyword":"量子克隆"},{"id":"34994c4b-9c7e-4df2-8d72-fde6cd0dfc75","keyword":"普适量子克隆","originalKeyword":"普适量子克隆"},{"id":"16e80c66-2b5a-4ee0-974b-0c984dd752ea","keyword":"相位协<span style=\"color:red\">变量</span>子克隆","originalKeyword":"相位协变量子克隆"}],"language":"zh","publisherId":"lzdzxb201504009","title":"最优相位协<span style=\"color:red\">变量</span>子克隆","volume":"32","year":"2015"},{"abstractinfo":"采用ECC和EBSD技术研究了AA1050铝合金冷轧至中低应<span style=\"color:red\">变量</span>下位错界面结构的演变. 结果表明, 冷轧至中低应<span style=\"color:red\">变量</span>下形成典 型的位错胞块结构,其微观组织结构强烈依赖于晶粒的取向. 变形后主要形成三种典型的组织结构: Type A------两组交叉的几何必须位错界面 (GNBs) 结构,Type B------一组GNBs结构, Type C------近似等轴的普通胞状结构. 绝大多数Copper, Brass和Goss取向的晶粒具有Type A结构, S取向的晶粒具有Type B结构, 而Cube取向的晶粒主要具有Type C结构. 变形过程中的GNBs不仅具有<span style=\"color:red\">与</span>RD成&plusmn;(30&deg;---40&deg;) 的宏观取向, 而且大多数GNBs位错界面近似平行于由最大Schmid因子所确定的{111}滑移面的迹线.","authors":[{"authorName":"刘庆姚宗勇A.Godfrey刘伟","id":"26c6f194-3bbb-4242-af7c-cf76a7a07b0a","originalAuthorName":"刘庆姚宗勇A.Godfrey刘伟"}],"categoryName":"|","doi":"","fpage":"641","id":"74a00c43-dd14-4dec-9855-3c74a534f643","issue":"6","journal":{"abbrevTitle":"JSXB","coverImgSrc":"journal/img/cover/JSXB.jpg","id":"48","issnPpub":"0412-1961","publisherId":"JSXB","title":"金属学报"},"keywords":[{"id":"2cd637fa-0a5a-48ae-bc12-b738fd9bf0dd","keyword":"铝合金","originalKeyword":"铝合金"},{"id":"3455108b-4009-4e67-af54-65d17f37054a","keyword":" cold rolling","originalKeyword":" cold rolling"},{"id":"ebb7f3bf-e5c3-4536-964f-918d3864d432","keyword":" electron backscattered diffraction (EBSD)","originalKeyword":" electron backscattered diffraction (EBSD)"},{"id":"d7e15959-dde5-4962-91d5-06ffb9946279","keyword":"dislocation boundary structure","originalKeyword":"dislocation boundary structure"}],"language":"zh","publisherId":"0412-1961_2009_6_16","title":"中低应<span style=\"color:red\">变量</span>冷轧AA1050铝合金中晶粒取向<span style=\"color:red\">与</span>形变位错界面的演变","volume":"45","year":"2009"}],"totalpage":8603,"totalrecord":86025}