{"currentpage":1,"firstResult":0,"maxresult":10,"pagecode":5,"pageindex":{"endPagecode":5,"startPagecode":1},"records":[{"abstractinfo":"建立了液固挤压Al2O3sf/LY12复合材料三维非稳态传热过程的有限元数学模型,并对其进行了三维热传导数值模拟,直观地显示出材料内部和表面在不同时刻、不同位置的三维<span style=\"color:red\">温度场</span>分布及其<span style=\"color:red\">演变</span>情况.模拟结果表明,坯料内部和表面的<span style=\"color:red\">温度场</span>在保压过程中分布均匀,而在挤压过程中则随时间推移而剧烈波动,从而造成坯料表面局部过热,由此导致制件表面龟裂现象的发生.模拟结果与实验结果基本吻合,为合理确定工艺参数和保证成形质量奠定了理论基础.","authors":[{"authorName":"王振军","id":"9ce22f2a-fbb9-4e50-8748-95244d164e9a","originalAuthorName":"王振军"},{"authorName":"齐乐华","id":"5fef898e-7666-4e3c-a218-8452495568ee","originalAuthorName":"齐乐华"},{"authorName":"周计明","id":"efa4eac9-8917-498d-b637-a2138d622cf9","originalAuthorName":"周计明"},{"authorName":"杨方","id":"990db8a2-1729-4c6b-85e8-4edee861acb2","originalAuthorName":"杨方"}],"doi":"10.3321/j.issn:0412-1961.2007.08.014","fpage":"857","id":"90d5d4ed-64d9-4681-ad02-bb1822b443c4","issue":"8","journal":{"abbrevTitle":"JSXB","coverImgSrc":"journal/img/cover/JSXB.jpg","id":"48","issnPpub":"0412-1961","publisherId":"JSXB","title":"金属学报"},"keywords":[{"id":"db7543a7-1a65-4022-8ff8-608abd33a1a9","keyword":"Al2O3/LY12复合材料","originalKeyword":"Al2O3/LY12复合材料"},{"id":"bc5e5a4b-cb4f-4961-8468-b3b454c48a19","keyword":"液固挤压","originalKeyword":"液固挤压"},{"id":"6ae92ae9-84a4-494f-9c6c-d7c536e927be","keyword":"三维有限元法","originalKeyword":"三维有限元法"},{"id":"4f7d9fdd-7dee-44ea-bc29-9f0835002564","keyword":"<span style=\"color:red\">温度场</span><span style=\"color:red\">演变</span>","originalKeyword":"温度场演变"},{"id":"11a4e698-66dc-42fe-aa30-5671f623c60c","keyword":"热传导","originalKeyword":"热传导"}],"language":"zh","publisherId":"jsxb200708014","title":"Al2O3sf/LY12复合材料液固挤压成形中<span style=\"color:red\">温度场</span><span style=\"color:red\">演变</span>的三维有限元分析","volume":"43","year":"2007"},{"abstractinfo":"应用电阻法对试样快速加热,然后对其进行高温锻压,并结合实验过程及参数,基于deform-3D软件对F40船板钢高温锻压过程的<span style=\"color:red\">温度场</span>及组织<span style=\"color:red\">演变</span>进行模拟.结果表明,试样的辐射系数为0.7,与空气的换热系数为0.02 kW/m2·K,模具与试样的传热系数为16 kW/m2·K.模拟结果与实验测得的<span style=\"color:red\">温度场</span>结果吻合度较好,验证了计算机模拟的可靠性和准确性.同时,结合<span style=\"color:red\">温度场</span>对试样组织<span style=\"color:red\">演变</span>进行模拟,并通过实测验证了模拟的正确性和可靠性,对实际生产具有参考意义.","authors":[{"authorName":"李余飞","id":"bee5b1ca-e87b-465a-88a6-485c0aa06564","originalAuthorName":"李余飞"},{"authorName":"陈剑","id":"f452e92b-dbb2-491b-99e3-c9fb80026ce7","originalAuthorName":"陈剑"},{"authorName":"赵永桥","id":"322a2acc-b2f0-4407-9f75-f95c943e6022","originalAuthorName":"赵永桥"},{"authorName":"熊辉辉","id":"e677c035-2c05-444d-86e4-60c1278a299e","originalAuthorName":"熊辉辉"},{"authorName":"张恒华","id":"d64ee997-b4e1-4741-bf67-a9b625f983cf","originalAuthorName":"张恒华"}],"doi":"","fpage":"37","id":"272dc479-7a50-4652-80eb-48bf60dc5dfa","issue":"2","journal":{"abbrevTitle":"SHJS","coverImgSrc":"journal/img/cover/SHJS.jpg","id":"59","issnPpub":"1001-7208","publisherId":"SHJS","title":"上海金属"},"keywords":[{"id":"22008303-b689-4864-931b-6ba09b128d63","keyword":"F40钢","originalKeyword":"F40钢"},{"id":"40f67a2b-b246-4a5f-a0fa-bf93d9fac0c1","keyword":"高温锻压","originalKeyword":"高温锻压"},{"id":"a4a16ce4-5eb3-40c8-9e6f-beb5abe0d30a","keyword":"有限元模拟","originalKeyword":"有限元模拟"},{"id":"11ba9e47-a97c-4f6d-a9e2-e5938956ea7d","keyword":"<span style=\"color:red\">温度场</span>","originalKeyword":"温度场"},{"id":"014a4817-ba09-401a-bc7d-a2768bfb5e98","keyword":"组织<span style=\"color:red\">演变</span>","originalKeyword":"组织演变"}],"language":"zh","publisherId":"shjs201602008","title":"F40船板钢高温锻压<span style=\"color:red\">温度场</span>及组织<span style=\"color:red\">演变</span>模拟","volume":"38","year":"2016"},{"abstractinfo":"通过对碳热还原合成SiC冶炼炉<span style=\"color:red\">温度场</span>的数值模拟及实验,揭示了冶炼炉内<span style=\"color:red\">温度场</span>的<span style=\"color:red\">演变</span>规律.研究表明,碳化硅合成过程中,热量以热源为中心呈辐射状向外传递,其合成<span style=\"color:red\">温度</span>(1600℃)等温面也逐渐向外扩大,表现为SiC的合成反应温区增大;SiC的大量合成发生在中后期,合成持续,SiC合成温区面积增加缓慢.合成时间过长,会导致已生成的SiC分解,容易形成实际生产中喷炉事故;适当比例的SiC分解,有利于形成高致密的碳化硅产品.","authors":[{"authorName":"陈杰","id":"4ad1a998-b68a-4df5-8abb-1c798b73e2a0","originalAuthorName":"陈杰"},{"authorName":"王晓刚","id":"a10299ec-cac4-4637-b7fb-a3b4afed763e","originalAuthorName":"王晓刚"}],"doi":"","fpage":"2212","id":"7a5afd02-a712-48d0-ac4a-cd78a89eea3d","issue":"11","journal":{"abbrevTitle":"GSYTB","coverImgSrc":"journal/img/cover/GSYTB.jpg","id":"36","issnPpub":"1001-1625","publisherId":"GSYTB","title":"硅酸盐通报   "},"keywords":[{"id":"57235dcc-671d-4ea2-9c09-83c4989892e2","keyword":"碳热还原法","originalKeyword":"碳热还原法"},{"id":"5bd30ba0-d1c5-468c-8a95-d57a750c767b","keyword":"SiC","originalKeyword":"SiC"},{"id":"5f16705b-7d7c-4476-9b44-c3c7c97a4fe8","keyword":"<span style=\"color:red\">温度场</span>","originalKeyword":"温度场"},{"id":"d5914c71-1ab7-467a-978b-d551b20ec98a","keyword":"<span style=\"color:red\">演变</span>规律","originalKeyword":"演变规律"},{"id":"f0549610-f1ca-4e63-b4f3-ef90dbee8ad9","keyword":"数值模拟","originalKeyword":"数值模拟"}],"language":"zh","publisherId":"gsytb201311008","title":"碳热还原合成SiC<span style=\"color:red\">温度场</span><span style=\"color:red\">演变</span>规律研究","volume":"32","year":"2013"},{"abstractinfo":"本文旨在进行SPS过程中粉末颗粒内部<span style=\"color:red\">温度场</span>的模拟及颈部<span style=\"color:red\">演变</span>的研究。建立了用于模拟导电材料在SPS过程中粉末颗粒的热传导行为的计算模型。以球形铜粉为研究对象，对颗粒内部<span style=\"color:red\">温度</span>分布和颈部尺寸变化进行了模拟计算和分析，模拟结果表明SPS过程中颗粒内部的<span style=\"color:red\">温度</span>分布极不均匀，颈部尺寸的长大速度在烧结过程中并不一致。不同烧结阶段颈部尺寸变化的模拟结果和实验测定结果基本吻合，证明了本文模型的合理性。本文研究结果揭示了SPS过程中烧结颈部形成和长大的本质机制。","authors":[{"authorName":"刘雪梅","id":"51c57d2b-4460-4e40-890d-51abff44caaf","originalAuthorName":"刘雪梅"},{"authorName":"宋晓艳","id":"9d868914-2479-4f8c-b43b-e0f135035847","originalAuthorName":"宋晓艳"},{"authorName":"张久兴","id":"be034a66-ca3f-4eb5-a934-794f4da0612d","originalAuthorName":"张久兴"}],"categoryName":"|","doi":"","fpage":"757","id":"ac49bef8-5967-4c7c-8ea0-8b28812270c1","issue":"7","journal":{"abbrevTitle":"JSXB","coverImgSrc":"journal/img/cover/JSXB.jpg","id":"48","issnPpub":"0412-1961","publisherId":"JSXB","title":"金属学报"},"keywords":[{"id":"b9df5aa0-3cc8-4895-bdbe-5aa0264e3a81","keyword":"放电等离子烧结","originalKeyword":"放电等离子烧结"},{"id":"4dc8c17e-c128-4972-9ec8-ecfb152566c5","keyword":"neck size","originalKeyword":"neck size"},{"id":"8d3b578f-ed2f-4354-a106-a6d7566d6525","keyword":"temperature distribution","originalKeyword":"temperature distribution"}],"language":"zh","publisherId":"0412-1961_2006_7_12","title":"放电等离子烧结过程中粉末颗粒内部<span style=\"color:red\">温度场</span>的模拟及颈部<span style=\"color:red\">演变</span>","volume":"42","year":"2006"},{"abstractinfo":"综合考虑传热、变形及变形过程中的再结晶之间的相互影响,对C-Mn钢在CSP热连轧过程的<span style=\"color:red\">温度场</span>进行了计算机模拟.确定了各种工艺条件下的传热边界条件及其对应的换热系数关系式,计算出了轧件变形过程中<span style=\"color:red\">温度</span>变化和<span style=\"color:red\">温度场</span>分布.算例表明,模拟计算具有较好的精度,能为进一步模拟带钢轧后组织<span style=\"color:red\">演变</span>和性能预测分析提供计算基础.","authors":[{"authorName":"唐广波","id":"190b0e8f-75cc-4102-8a75-33caa6da49ee","originalAuthorName":"唐广波"},{"authorName":"刘正东","id":"cbb1b71d-2fc7-4bb9-b702-8292a63474b3","originalAuthorName":"刘正东"},{"authorName":"董瀚","id":"74462c94-e5b6-4723-9924-2b925e65231a","originalAuthorName":"董瀚"},{"authorName":"王中丙","id":"e707dc43-fcd7-4b72-a596-b82cb8f5b335","originalAuthorName":"王中丙"},{"authorName":"陈顺安","id":"9fab1ec4-f5ee-4499-a2ae-a943a07ad17b","originalAuthorName":"陈顺安"},{"authorName":"孙文填","id":"d4352011-4c19-4d50-9e10-9ae9404c24a7","originalAuthorName":"孙文填"},{"authorName":"张若生","id":"846d93d0-d1ae-4669-b5f4-6a20ab31b1a7","originalAuthorName":"张若生"},{"authorName":"谢立群","id":"377e6642-3bf0-4016-b6a6-c8872b50a899","originalAuthorName":"谢立群"},{"authorName":"黄志勇","id":"4894fc5b-4077-4e72-b1aa-d57d0bb54cda","originalAuthorName":"黄志勇"},{"authorName":"康永林","id":"dacc6574-ba5d-452d-b68c-236b0b6d84e7","originalAuthorName":"康永林"}],"doi":"","fpage":"38","id":"1a47099a-dd83-4307-bccf-e67a040b4136","issue":"8","journal":{"abbrevTitle":"GT","coverImgSrc":"journal/img/cover/GT.jpg","id":"27","issnPpub":"0449-749X","publisherId":"GT","title":"钢铁"},"keywords":[{"id":"de9298ed-0f52-457e-8c12-520654d691ce","keyword":"CSP","originalKeyword":"CSP"},{"id":"35d5c4e7-12a5-442e-8b9d-13164ae21e6b","keyword":"<span style=\"color:red\">温度场</span>模拟","originalKeyword":"温度场模拟"},{"id":"3d8e42ef-e264-4efc-99f1-6ce34f59d674","keyword":"换热系数","originalKeyword":"换热系数"},{"id":"dd4b141b-7cb7-4c83-b47a-74fc3d37242a","keyword":"流变应力","originalKeyword":"流变应力"},{"id":"cb995b96-640c-4040-8c30-9b72cc9289d9","keyword":"再结晶动力学","originalKeyword":"再结晶动力学"}],"language":"zh","publisherId":"gt200308008","title":"CSP热轧过程<span style=\"color:red\">温度场</span>模拟","volume":"38","year":"2003"},{"abstractinfo":"通过对实验室模拟现场回转窑的6组不同<span style=\"color:red\">温度</span>点下焙烧渣样品进行钒尖晶石形貌变化、物相含量变化、钒元素的赋存规律及不同<span style=\"color:red\">温度</span>点下物相转变机理的研究。钒尖晶石形貌变化结果表明，整个焙烧过程中钒尖晶石形貌变化经历了致密光滑块状－氧化铁的镶边结构－钒尖晶石完全直接为隐晶质物质－小颗粒物质重新组合并且长大5个过程；矿物自动解理分析仪（MLA）物相含量分析数据显示焙烧过程中石灰石、铁橄榄石、钒尖晶石和白云石在逐渐减少，普通辉石相是逐渐增加，而氧化铁固溶体、部分氧化钒尖晶石、钒酸钙固溶体和铁板钛矿固溶体的变化趋势是先增加后减少；钒元素的赋存形式规律为绝大多数钒元素赋存于氧化物中，占到总量的85％左右，其次赋存于硅酸盐中，占到钒总含量的14％左右，还有极少部分分布于碳酸盐等矿物中；整个焙烧过程物相变化机理主要分为铁元素向外扩散－氧元素向内扩散－氧化物的化合过程－化合物雏形晶体的长大4个反应过程。","authors":[{"authorName":"史志新","id":"c62252ad-f040-470f-8631-714bd5a41f9b","originalAuthorName":"史志新"}],"doi":"10.13228/j.boyuan.issn1000-7571.009670","fpage":"39","id":"33296735-b4c5-47fc-aa4f-52c7098b3c5e","issue":"4","journal":{"abbrevTitle":"YJFX","coverImgSrc":"journal/img/cover/YJFX.jpg","id":"71","issnPpub":"1000-7571","publisherId":"YJFX","title":"冶金分析   "},"keywords":[{"id":"b40dc498-502c-4e39-8694-0d001e089fa7","keyword":"钒渣钙化焙烧","originalKeyword":"钒渣钙化焙烧"},{"id":"8ae37f45-0714-434a-903c-bea925e4f465","keyword":"钒尖晶石","originalKeyword":"钒尖晶石"},{"id":"382c7db8-94b1-477a-89b4-2ee409f2a6ab","keyword":"机理分析","originalKeyword":"机理分析"},{"id":"ebf58094-12de-472e-b53c-211b6bfbd1ad","keyword":"矿物自动解理分析仪(MLA)","originalKeyword":"矿物自动解理分析仪(MLA)"}],"language":"zh","publisherId":"yjfx201604009","title":"回转窑不同<span style=\"color:red\">温度场</span>钒渣物相<span style=\"color:red\">演变</span>规律探讨","volume":"36","year":"2016"},{"abstractinfo":"利用外约束型模拟空间热循环<span style=\"color:red\">温度场</span>试验设备对1420Al-Li合金焊缝进行了热循环(77～393 K)试验,测量了热循环前后焊缝的拉伸性能,并观察了热循环前后焊缝的显微组织,讨论了热循环对焊缝组织和拉伸性能的影响.试验结果表明,经1000次或3000次热循环后,焊缝的强度和延伸率显著降低.热应力使焊缝显微组织产生损伤,主要表现为从晶界处向晶内发射位错,在晶界处形成位错塞积群,晶粒内位错密度逐渐升高.随着热循环次数的增加,组织损伤的不断累积导致在晶界处产生的应力集中程度增大,这是导致合金焊缝强度和延伸率下降的主要原因.","authors":[{"authorName":"杨素媛","id":"87964ba9-e136-4515-8f8e-ea57a8fbe6bb","originalAuthorName":"杨素媛"},{"authorName":"耿洪滨","id":"4eb802b4-76e7-4509-b046-ca64702627b6","originalAuthorName":"耿洪滨"},{"authorName":"郭启雯","id":"543f7057-3dc4-4b9f-bfd1-015bed2783d9","originalAuthorName":"郭启雯"}],"doi":"10.3969/j.issn.0258-7076.2006.03.032","fpage":"411","id":"fa2a3a87-d752-4093-b8d7-0b5758f001e1","issue":"3","journal":{"abbrevTitle":"XYJS","coverImgSrc":"journal/img/cover/XYJS.jpg","id":"67","issnPpub":"0258-7076","publisherId":"XYJS","title":"稀有金属"},"keywords":[{"id":"349034d7-2e22-49f4-978b-a3868ffb6088","keyword":"热循环","originalKeyword":"热循环"},{"id":"fff2a893-0f6d-4869-957b-bc7f9f08f952","keyword":"铝锂合金","originalKeyword":"铝锂合金"},{"id":"3c068781-e7a7-4e3b-99f3-5bde9a20f820","keyword":"焊缝","originalKeyword":"焊缝"},{"id":"83ee60e6-82e4-4676-ab35-101be6f89aa9","keyword":"显微组织","originalKeyword":"显微组织"},{"id":"4dd53539-4b9b-497d-9e25-6aaf685f6bd5","keyword":"拉伸性能","originalKeyword":"拉伸性能"}],"language":"zh","publisherId":"xyjs200603032","title":"热循环<span style=\"color:red\">温度场</span>作用下1420A1-Li合金焊缝组织和拉伸性能的<span style=\"color:red\">演变</span>规律","volume":"30","year":"2006"},{"abstractinfo":"<span style=\"color:red\">温度场</span>数学模型是层流冷却控制系统的核心.对层流冷却<span style=\"color:red\">温度场</span>模型的研究现状进行了评述,介绍了轧后层流冷却<span style=\"color:red\">温度场</span>的发展包括<span style=\"color:red\">温度场</span>的结构<span style=\"color:red\">演变</span>以及层流冷却换热机理的研究进展,介绍了层流冷却<span style=\"color:red\">温度场</span>与相变、应力/应变耦合计算及其应用效果,展望了<span style=\"color:red\">温度场</span>数学模型未来的发展方向.","authors":[{"authorName":"黄全伟","id":"51a59e45-60c3-4bc8-910c-a1d70b33eeff","originalAuthorName":"黄全伟"},{"authorName":"韩斌","id":"bf1b7e11-0eab-431e-b1d4-5b1db57cd8f2","originalAuthorName":"韩斌"},{"authorName":"谭文","id":"05d93f84-062d-44e8-b5e3-5679bb95b145","originalAuthorName":"谭文"},{"authorName":"汪水泽","id":"06737d56-6260-4258-9d37-ee37d56d4d3c","originalAuthorName":"汪水泽"},{"authorName":"阮安甫","id":"7b3cd6cd-3757-48f9-9f22-01eb60e62284","originalAuthorName":"阮安甫"}],"doi":"","fpage":"59","id":"0d874169-d950-4d89-9dab-31901c99f057","issue":"1","journal":{"abbrevTitle":"GTYJ","coverImgSrc":"journal/img/cover/GTYJ.jpg","id":"29","issnPpub":"1001-1447","publisherId":"GTYJ","title":"钢铁研究"},"keywords":[{"id":"fced7b2d-98a8-4b6b-8da5-893922cc3196","keyword":"层流冷却","originalKeyword":"层流冷却"},{"id":"0adf25d8-acce-41f2-bd72-9565dd297008","keyword":"数学模型","originalKeyword":"数学模型"},{"id":"cf7401bd-117f-4092-a5ea-73a6318b5937","keyword":"热轧","originalKeyword":"热轧"},{"id":"4e1ca051-ef13-4ecc-bc20-32807b0942a3","keyword":"换热系数","originalKeyword":"换热系数"},{"id":"6d135a44-dec4-484e-8220-99670fa1c841","keyword":"相变","originalKeyword":"相变"}],"language":"zh","publisherId":"gtyj201301016","title":"层流冷却<span style=\"color:red\">温度场</span>数学模型的研究现状","volume":"41","year":"2013"},{"abstractinfo":"建立了用于模拟导电材料在放电等离子烧结(SPS)过程中粉末颗粒热传导行为的计算模型.以球形铜粉为研究对象,对颗粒内部<span style=\"color:red\">温度</span>分布和颈部尺寸变化进行了模拟计算和分析,模拟结果表明:SPS过程中颗粒内部的<span style=\"color:red\">温度</span>分布极不均匀,烧结颈部的长大速率在烧结过程中并不一致.不同烧结阶段颈部尺寸变化的模拟结果和实验测定结果基本吻合.揭示了SPS过程中烧结颈部形成和长大的根本原因是颗粒接触部位的局部高温.","authors":[{"authorName":"刘雪梅","id":"fa52b1e7-7b95-4a34-bd45-cd40a62a0d43","originalAuthorName":"刘雪梅"},{"authorName":"宋晓艳","id":"f71a8493-0630-4866-bfdb-6c2e2baae8a6","originalAuthorName":"宋晓艳"},{"authorName":"张久兴","id":"d8c0bd63-6433-4748-af95-6cd52c6f5fd9","originalAuthorName":"张久兴"}],"doi":"10.3321/j.issn:0412-1961.2006.07.015","fpage":"757","id":"734b258b-e88d-4fb5-a098-bfccf1f668d9","issue":"7","journal":{"abbrevTitle":"JSXB","coverImgSrc":"journal/img/cover/JSXB.jpg","id":"48","issnPpub":"0412-1961","publisherId":"JSXB","title":"金属学报"},"keywords":[{"id":"4dd861fd-355f-445b-b4f8-ad90ed24197f","keyword":"放电等离子烧结(SPS)","originalKeyword":"放电等离子烧结(SPS)"},{"id":"823f16c1-50cc-4947-9e46-8f2593a5dbeb","keyword":"颈部尺寸","originalKeyword":"颈部尺寸"},{"id":"ff68c5b7-ba2e-4ea0-aa14-0487f872f58e","keyword":"<span style=\"color:red\">温度</span>分布","originalKeyword":"温度分布"}],"language":"zh","publisherId":"jsxb200607015","title":"放电等离子烧结过程中粉末颗粒内部<span style=\"color:red\">温度场</span>的模拟及颈部<span style=\"color:red\">演变</span>","volume":"42","year":"2006"},{"abstractinfo":"喷射铸造是一种先进的可用于制造高性能复合轧辊的技术,但复合轧辊界面冶金结合困难是这种新型工艺所面临的关键问题.通过计算机数值模拟研究喷射铸造过程中复合轧辊内部<span style=\"color:red\">温度场</span>及各种喷射工艺参数对<span style=\"color:red\">温度场</span>的影响.结果表明,辊芯预热<span style=\"color:red\">温度</span>、辊芯平移速度和喷射速率对<span style=\"color:red\">温度场</span>的影响较大.","authors":[{"authorName":"汪煜","id":"82614f94-d1a5-4a14-bcc0-1e59b47eaac8","originalAuthorName":"汪煜"},{"authorName":"崔成松","id":"253b0fb0-e382-4a5b-8564-3d2b857afbda","originalAuthorName":"崔成松"},{"authorName":"李庆春","id":"074888ca-313d-4e6c-a308-5987a903b2ae","originalAuthorName":"李庆春"},{"authorName":"张国庆","id":"c900bc99-0083-42ff-b71d-685268c4047a","originalAuthorName":"张国庆"},{"authorName":"汪武祥","id":"2415829d-803d-4727-a255-4a9f0a632583","originalAuthorName":"汪武祥"}],"doi":"10.3969/j.issn.1005-5053.2006.03.018","fpage":"88","id":"272a01ce-84be-42d5-adb4-73abfbd1a7f8","issue":"3","journal":{"abbrevTitle":"HKCLXB","coverImgSrc":"journal/img/cover/HKCLXB.jpg","id":"41","issnPpub":"1005-5053","publisherId":"HKCLXB","title":"航空材料学报"},"keywords":[{"id":"dc50b0c3-fa53-4532-ad44-7673d61d358c","keyword":"喷射铸造","originalKeyword":"喷射铸造"},{"id":"32137130-8f64-43ae-b685-d56ba9415788","keyword":"复合轧辊","originalKeyword":"复合轧辊"},{"id":"21aac19e-b268-403b-a8f2-62cf397468ba","keyword":"数值模拟","originalKeyword":"数值模拟"}],"language":"zh","publisherId":"hkclxb200603018","title":"喷射铸造复合轧辊<span style=\"color:red\">温度场</span>的数值模拟","volume":"26","year":"2006"}],"totalpage":5427,"totalrecord":54261}