{"currentpage":1,"firstResult":0,"maxresult":10,"pagecode":5,"pageindex":{"endPagecode":5,"startPagecode":1},"records":[{"abstractinfo":"建立同时考虑颗粒和颗粒之间瞬间碰撞作用(瞬间接触)和非流化下颗粒滑动和滚动运动产生的颗粒半接触作用的颗粒碰撞-<span style=\"color:red\">摩擦</span><span style=\"color:red\">应力</span><span style=\"color:red\">模型</span>.推导具有普适性的固相动量守恒方程,建立高颗粒浓度气固两相流动<span style=\"color:red\">模型</span>,对喷动床内气体颗粒流动过程进行了数值模拟.模拟计算预测喷动床内喷射区、环隙区和喷泉区颗粒流动特性.预测喷动床内颗粒浓度和速度分布与他人实验结果相吻合.","authors":[{"authorName":"李响","id":"d414ab53-0d5d-416c-9597-495793f9af18","originalAuthorName":"李响"},{"authorName":"孙丹","id":"e517a599-2284-4925-b8c2-d4ff4e4db690","originalAuthorName":"孙丹"},{"authorName":"于龙","id":"446d5a1d-9722-43db-b451-3cda846288a5","originalAuthorName":"于龙"},{"authorName":"何玉荣","id":"a5ad4f13-338d-429c-a077-2a6c0a46381a","originalAuthorName":"何玉荣"},{"authorName":"杨仲明","id":"48395ea7-7513-441c-96e0-0b61e74e9c7e","originalAuthorName":"杨仲明"},{"authorName":"陆慧林","id":"a0410ed1-45ee-45e1-993d-3c8aa5943d10","originalAuthorName":"陆慧林"}],"doi":"","fpage":"68","id":"e39dd45e-1d2b-4472-b2f0-1cb459cb2c0f","issue":"1","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":"96637f87-858c-4022-a591-53a98f3653f5","keyword":"气固喷动床","originalKeyword":"气固喷动床"},{"id":"66d48998-573d-429d-a149-f506fa072143","keyword":"<span style=\"color:red\">摩擦</span>-<span style=\"color:red\">动力</span><span style=\"color:red\">应力</span><span style=\"color:red\">模型</span>","originalKeyword":"摩擦-动力应力模型"},{"id":"04a18e63-dc15-4c76-8160-107248859424","keyword":"数值模拟","originalKeyword":"数值模拟"}],"language":"zh","publisherId":"gcrwlxb201001018","title":"基于<span style=\"color:red\">摩擦</span>-<span style=\"color:red\">动力</span><span style=\"color:red\">应力</span><span style=\"color:red\">模型</span>模拟喷动床气固流动","volume":"31","year":"2010"},{"abstractinfo":"基于统一二阶矩两相湍流<span style=\"color:red\">应力</span><span style=\"color:red\">模型</span>和稠密颗粒<span style=\"color:red\">动力</span>学理论，建立了欧拉一欧拉双流体二阶矩颗粒<span style=\"color:red\">摩擦</span><span style=\"color:red\">应力</span><span style=\"color:red\">模型</span>。<span style=\"color:red\">模型</span>充分反映各向异性的气固两相相间雷诺<span style=\"color:red\">应力</span>相互作用，并引入有效颗粒弹性恢复系数，考虑了因颗粒表面不光滑产生的<span style=\"color:red\">摩擦</span>力对湍流流动结构和颗粒弥散特性的影响，对于下降管的计算结果与实验吻合较好。因颗粒<span style=\"color:red\">摩擦</span>产生能量耗散降低了颗粒温度和导致颗粒雷诺<span style=\"color:red\">应力</span>再分布。在入口和出口区域因颗粒碰撞频率较高而产生的能量耗散对流动结构影响明显。","authors":[{"authorName":"刘阳","id":"b3d1f57e-3b4d-4121-bc67-af689761b0be","originalAuthorName":"刘阳"},{"authorName":"刘学","id":"ede1bac6-8967-454c-bb48-1d9e4e4dd923","originalAuthorName":"刘学"},{"authorName":"刘朋","id":"a1dcfea4-df43-4670-95f0-653911827f83","originalAuthorName":"刘朋"},{"authorName":"蒋福伟","id":"267cb696-1b6e-47d8-8bed-7a1b164f0810","originalAuthorName":"蒋福伟"},{"authorName":"周力行","id":"6bdb5d0d-9de1-4ab0-a5c6-3c192fcc4705","originalAuthorName":"周力行"}],"doi":"","fpage":"163","id":"8a2fbf8c-cbcf-40d3-a407-ab71add6b78f","issue":"1","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":"23d0702a-448f-49fc-b46c-6a6b2af22c69","keyword":"二阶矩颗粒<span style=\"color:red\">摩擦</span><span style=\"color:red\">应力</span><span style=\"color:red\">模型</span>","originalKeyword":"二阶矩颗粒摩擦应力模型"},{"id":"fcfc60a9-6e86-4808-aa36-b4d0d010252a","keyword":"稠密气固流动","originalKeyword":"稠密气固流动"},{"id":"7f5a3319-8472-4888-808a-1a901675f51d","keyword":"下降管","originalKeyword":"下降管"},{"id":"507d4c52-f211-4655-8a78-c0682b8f5476","keyword":"数值模拟","originalKeyword":"数值模拟"}],"language":"zh","publisherId":"gcrwlxb201201042","title":"稠密气固流动二阶矩<span style=\"color:red\">摩擦</span><span style=\"color:red\">应力</span><span style=\"color:red\">模型</span>和模拟","volume":"33","year":"2012"},{"abstractinfo":"采用弹塑性有限元法对带钢冷轧过程中接触区<span style=\"color:red\">摩擦</span><span style=\"color:red\">应力</span>进行了模拟,分析了各种因素对<span style=\"color:red\">摩擦</span><span style=\"color:red\">应力</span>分布的影响.利用数值方法对各影响因素对<span style=\"color:red\">摩擦</span><span style=\"color:red\">应力</span>分布的影响进行参数拟合,从而建立各影响因素和<span style=\"color:red\">摩擦</span><span style=\"color:red\">应力</span>分布间的特定关系,并对计算轧制力数学<span style=\"color:red\">模型</span>中的<span style=\"color:red\">摩擦</span><span style=\"color:red\">应力</span>分布进行修正,使计算结果更为精确.","authors":[{"authorName":"朱光明","id":"c1a5426b-718e-416b-8074-3e58159b1f96","originalAuthorName":"朱光明"},{"authorName":"杜凤山","id":"56705060-fe3b-4f71-9121-287b9b8a02b1","originalAuthorName":"杜凤山"},{"authorName":"孙登月","id":"aec3704c-efd5-48ed-a325-ba6c6c166b62","originalAuthorName":"孙登月"},{"authorName":"郭振宇","id":"ce813f8f-3cdb-49a2-965e-7ac3c9a1a141","originalAuthorName":"郭振宇"},{"authorName":"周坚刚","id":"7cc7f2b3-b3ed-495f-9f27-7778f5412acb","originalAuthorName":"周坚刚"},{"authorName":"朱泉封","id":"730973b5-6639-4429-b78c-a696acb1973f","originalAuthorName":"朱泉封"}],"doi":"","fpage":"30","id":"eef04bf9-d81f-4d45-8136-f534e85e9c1b","issue":"12","journal":{"abbrevTitle":"GT","coverImgSrc":"journal/img/cover/GT.jpg","id":"27","issnPpub":"0449-749X","publisherId":"GT","title":"钢铁"},"keywords":[{"id":"d6cb10f8-70a1-4dfc-98d2-553976da6fcf","keyword":"弹塑性","originalKeyword":"弹塑性"},{"id":"eb5b653e-efbf-4e21-a241-61c9062583d2","keyword":"有限元法","originalKeyword":"有限元法"},{"id":"26d1f8d3-9025-46fa-bdce-36f3bca05d52","keyword":"<span style=\"color:red\">摩擦</span><span style=\"color:red\">应力</span>","originalKeyword":"摩擦应力"}],"language":"zh","publisherId":"gt200312009","title":"2030板带冷连轧系统在线控制<span style=\"color:red\">模型</span>接触<span style=\"color:red\">摩擦</span><span style=\"color:red\">应力</span>分布","volume":"38","year":"2003"},{"abstractinfo":"为确定304不锈钢的孪生<span style=\"color:red\">动力</span>学<span style=\"color:red\">模型</span>及孪生对位错密度和变形抗力的影响规律,利用位错理论建立了含材料孪生<span style=\"color:red\">动力</span>学关系的本构关系<span style=\"color:red\">模型</span>,实测了材料的<span style=\"color:red\">应力</span>应变曲线,运用实测结果优化确定了本构关系<span style=\"color:red\">模型</span>中的待定常数,进而建立了材料的孪生<span style=\"color:red\">动力</span>学关系<span style=\"color:red\">模型</span>,本构关系<span style=\"color:red\">模型</span>还表明,在孪生条件下,材料的位错密度及变形抗力随变形程度增加而快速增大.","authors":[{"authorName":"李立新","id":"c43a439b-8797-41bc-9a92-7f94afb21f3d","originalAuthorName":"李立新"},{"authorName":"胡盛德","id":"c6e1778e-838f-4c04-86fe-d3f4d23cd0fe","originalAuthorName":"胡盛德"},{"authorName":"叶奔","id":"43935987-07bc-4163-ac6d-52c878b39d55","originalAuthorName":"叶奔"}],"doi":"","fpage":"56","id":"8acb2273-8054-42db-a6b3-ca3b4fceb8bb","issue":"9","journal":{"abbrevTitle":"GTYJXB","coverImgSrc":"journal/img/cover/GTYJXB.jpg","id":"30","issnPpub":"1001-0963","publisherId":"GTYJXB","title":"钢铁研究学报"},"keywords":[{"id":"8f15b43f-24f8-4978-9984-6d55a017b68d","keyword":"孪生<span style=\"color:red\">动力</span>学","originalKeyword":"孪生动力学"},{"id":"2e20c61a-0c20-4291-b330-2c2bd4979063","keyword":"位错","originalKeyword":"位错"},{"id":"78f1d404-b186-455b-bb2a-0d00dfc24ab4","keyword":"<span style=\"color:red\">应力</span>应变","originalKeyword":"应力应变"},{"id":"201dd9e4-deab-4d3f-a1c1-1db5a2542df4","keyword":"优化","originalKeyword":"优化"},{"id":"2ae99add-2867-48f1-8bd6-a949ee5481a5","keyword":"逆分析","originalKeyword":"逆分析"}],"language":"zh","publisherId":"gtyjxb201209011","title":"<span style=\"color:red\">应力</span>应变曲线逆分析确定孪生<span style=\"color:red\">动力</span>学<span style=\"color:red\">模型</span>","volume":"24","year":"2012"},{"abstractinfo":"为确定304不锈钢的孪生<span style=\"color:red\">动力</span>学<span style=\"color:red\">模型</span>及孪生对位错密度和变形抗力的影响规律，利用位错理论建立了含材料孪生<span style=\"color:red\">动力</span>学关系的本构关系<span style=\"color:red\">模型</span>，实测了材料的<span style=\"color:red\">应力</span>应变曲线，运用实测结果优化确定了本构关系<span style=\"color:red\">模型</span>中的待定常数，进而建立了材料的孪生<span style=\"color:red\">动力</span>学关系<span style=\"color:red\">模型</span>，本构关系<span style=\"color:red\">模型</span>还表明，在孪生条件下，材料的位错密度及变形抗力随变形程度增加而快速增大。","authors":[{"authorName":"李立新，胡盛德，叶奔","id":"658c1125-cc4a-461a-aa92-a30e8a905467","originalAuthorName":"李立新，胡盛德，叶奔"}],"categoryName":"|","doi":"","fpage":"56","id":"bd6a553a-7e45-4ab8-9a02-5bbb1f636930","issue":"9","journal":{"abbrevTitle":"GTYJXB","coverImgSrc":"journal/img/cover/GTYJXB.jpg","id":"30","issnPpub":"1001-0963","publisherId":"GTYJXB","title":"钢铁研究学报"},"keywords":[{"id":"4fad2724-20fd-4ef7-b3ec-622a02032cdb","keyword":"孪生<span style=\"color:red\">动力</span>学 ","originalKeyword":"孪生动力学 "},{"id":"1563e772-3482-4b3d-a1be-d18d7c062c26","keyword":" dislocation ","originalKeyword":" dislocation "},{"id":"aae39ce6-ec7a-495e-845a-8ffa91f729ce","keyword":" stress and strain ","originalKeyword":" stress and strain "},{"id":"11234265-4f1e-4745-a6ef-2f04cc17244f","keyword":" optimization ","originalKeyword":" optimization "},{"id":"3032f433-d3f1-44b6-ad70-c8a08299cfdc","keyword":" inverse analysis","originalKeyword":" inverse analysis"}],"language":"zh","publisherId":"1001-0963_2012_9_1","title":"<span style=\"color:red\">应力</span>应变曲线逆分析确定孪生<span style=\"color:red\">动力</span>学<span style=\"color:red\">模型</span>","volume":"24","year":"2012"},{"abstractinfo":"在Gleeble--3500热力学模拟实验机上对Q235A钢试样进行单道次和双道次热压缩实验,\n获得流变<span style=\"color:red\">应力</span>曲线. 把静态再结晶体积分数看作是时间的函数,\n将其与热变形结束后位错密度的变化联系起来. 通过\n对热压缩实验获得的流变<span style=\"color:red\">应力</span>曲线的逆分析,\n提出了确定静态再结晶<span style=\"color:red\">动力</span>学<span style=\"color:red\">模型</span>的新方法. 它可以取代\n传统的通过对淬火微观组织金相分析来估算静态再结晶<span style=\"color:red\">动力</span>学的方法.\n运用此方法于普碳钢的热压缩实验中,\n在一定的形变量范围内获得了静态再结晶<span style=\"color:red\">动力</span>学方程. 与已有的<span style=\"color:red\">模型</span>作比较,\n本文提出的方法仅\n需少量实验和计算即可获得准确的静态再结晶<span style=\"color:red\">动力</span>学<span style=\"color:red\">模型</span>.","authors":[{"authorName":"王健","id":"ab90438a-bb76-4267-94d1-2fd45a6cceda","originalAuthorName":"王健"},{"authorName":"肖宏","id":"74bebf13-8648-4ddc-95c4-185bf72e8888","originalAuthorName":"肖宏"},{"authorName":"张志国","id":"e5b0ef50-6d73-4c03-92d8-f46012a9dac7","originalAuthorName":"张志国"}],"categoryName":"|","doi":"","fpage":"837","id":"855290e4-de05-4849-affe-1919d362e400","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":"74e4377c-ace4-4032-b1ab-9b3e51a412a1","keyword":"静态再结晶","originalKeyword":"静态再结晶"},{"id":"b798fe98-a294-42ac-b2ec-7c60b475e665","keyword":"flow curves","originalKeyword":"flow curves"},{"id":"caa5a927-157e-431e-bb9f-478bd865fd98","keyword":"hot compression","originalKeyword":"hot compression"}],"language":"zh","publisherId":"0412-1961_2008_7_9","title":"流变<span style=\"color:red\">应力</span>逆分析确定静态再结晶<span style=\"color:red\">动力</span>学<span style=\"color:red\">模型</span>","volume":"44","year":"2008"},{"abstractinfo":"在Gleeble-3500热力学模拟实验机上对Q235A钢试样进行单道次和双道次热压缩实验,获得流变<span style=\"color:red\">应力</span>曲线.把静态再结晶体积分数看作是时间的函数,将其与热变形结束后位错密度的变化联系起来.通过对热压缩实验获得的流变<span style=\"color:red\">应力</span>曲线的逆分析,提出了确定静态再结晶<span style=\"color:red\">动力</span>学<span style=\"color:red\">模型</span>的新方法.它可以取代传统的通过对淬火微观组织金相分析来估算静态再结晶<span style=\"color:red\">动力</span>学的方法.运用此方法于普碳钢的热压缩实验中,在一定的形变量范围内获得了静态再结晶<span style=\"color:red\">动力</span>学方程.与已有的<span style=\"color:red\">模型</span>作比较,本文提出的方法仅需少量实验和计算即可获得准确的静态再结晶<span style=\"color:red\">动力</span>学<span style=\"color:red\">模型</span>.","authors":[{"authorName":"王健","id":"11f54825-fa87-4778-9c10-abfb4ada1d39","originalAuthorName":"王健"},{"authorName":"肖宏","id":"7d76d9a0-111a-4e6e-8a33-cd79681dbfaa","originalAuthorName":"肖宏"},{"authorName":"张志国","id":"75ed42b2-65a7-44cd-9f3e-e0dc7bcf581a","originalAuthorName":"张志国"}],"doi":"10.3321/j.issn:0412-1961.2008.07.013","fpage":"837","id":"b7930865-03fb-436f-acd8-9457563e6bb6","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":"56923f2d-8abe-4073-b9d6-c395efc9fc1d","keyword":"静态再结晶","originalKeyword":"静态再结晶"},{"id":"df91f2df-ca02-400f-be67-b16ee8ebcbcd","keyword":"流变<span style=\"color:red\">应力</span>曲线","originalKeyword":"流变应力曲线"},{"id":"b71236e7-8d00-47a6-a76a-cc197ac7957b","keyword":"热压缩","originalKeyword":"热压缩"},{"id":"a6b19e33-80d8-4246-a0fd-2311e4178d39","keyword":"逆分析","originalKeyword":"逆分析"},{"id":"c83500da-362a-4b6c-bbb4-8fd281af47ad","keyword":"位错密度","originalKeyword":"位错密度"}],"language":"zh","publisherId":"jsxb200807013","title":"流变<span style=\"color:red\">应力</span>逆分析确定静态再结晶<span style=\"color:red\">动力</span>学<span style=\"color:red\">模型</span>","volume":"44","year":"2008"},{"abstractinfo":"本构关系是影响模拟结果准确性的重要因素之一,本文采用一种数值模拟和压缩实验相结合的方法鼓度法,即由鼓度θ估算<span style=\"color:red\">摩擦</span>因子,然后通过主<span style=\"color:red\">应力</span>法公武去除压缩实验中<span style=\"color:red\">摩擦</span>因素的影响,得到6063铝合金的真实<span style=\"color:red\">应力</span>-应变曲线,并回归出本构方程.","authors":[{"authorName":"陈志英","id":"a0851480-66bc-4996-b58e-70413cbb2dc7","originalAuthorName":"陈志英"},{"authorName":"许树勤","id":"11d7b152-448d-4dd6-a9c6-f75f1e0676b7","originalAuthorName":"许树勤"},{"authorName":"董湘怀","id":"e58e6c32-1b4f-43a2-bf1e-83a3b5f14267","originalAuthorName":"董湘怀"},{"authorName":"阮雪榆","id":"da5b7e39-6423-4426-b311-590c3b58b5a9","originalAuthorName":"阮雪榆"}],"doi":"","fpage":"847","id":"5c00159c-8ba8-4937-9dbd-0af49936365e","issue":"6","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":"2b09a70f-c346-4bb8-b5c2-de060f09068d","keyword":"本构方程","originalKeyword":"本构方程"},{"id":"46ab4b58-4085-4390-ab97-238aa04ac64c","keyword":"鼓度","originalKeyword":"鼓度"},{"id":"23013033-a84c-40b4-b9fe-bb3561866c77","keyword":"压缩实验","originalKeyword":"压缩实验"},{"id":"434ebbdb-0149-4638-b939-798bb38d812a","keyword":"数学<span style=\"color:red\">模型</span>","originalKeyword":"数学模型"}],"language":"zh","publisherId":"clkxygy200806027","title":"6063铝合金压缩实验<span style=\"color:red\">摩擦</span>修正及高温流动<span style=\"color:red\">应力</span><span style=\"color:red\">模型</span>","volume":"16","year":"2008"},{"abstractinfo":"在文献[1]和[2]提出的<span style=\"color:red\">模型</span>的基础上,推导出金属材料在高温和弹性范围内因张<span style=\"color:red\">应力</span>引起的溶质非平衡晶界偏聚的<span style=\"color:red\">动力</span>学方程.","authors":[{"authorName":"徐庭栋","id":"a6f64bce-264d-4a0e-aaad-72960e0f94bb","originalAuthorName":"徐庭栋"}],"doi":"","fpage":"30","id":"e48a36b2-8491-47fb-a486-0896904b119d","issue":"3","journal":{"abbrevTitle":"GTYJXB","coverImgSrc":"journal/img/cover/GTYJXB.jpg","id":"30","issnPpub":"1001-0963","publisherId":"GTYJXB","title":"钢铁研究学报"},"keywords":[{"id":"351bd1d5-5262-41ff-84ee-69243e5a5e6c","keyword":"晶界","originalKeyword":"晶界"},{"id":"75444109-287f-4c50-b643-2068e4217796","keyword":"空位","originalKeyword":"空位"},{"id":"c0422e8f-a2ca-4947-ac4d-0df00d95e83d","keyword":"偏聚","originalKeyword":"偏聚"},{"id":"75e2e33f-8e4c-43ee-9326-e3042651dd43","keyword":"<span style=\"color:red\">应力</span>时效","originalKeyword":"应力时效"},{"id":"04bb3424-6bee-49df-81e2-412125c6a59f","keyword":"<span style=\"color:red\">动力</span>学","originalKeyword":"动力学"}],"language":"zh","publisherId":"gtyjxb200303008","title":"高温和低张<span style=\"color:red\">应力</span>引起的非平衡晶界偏聚<span style=\"color:red\">动力</span>学(Ⅰ)--理论<span style=\"color:red\">模型</span>","volume":"15","year":"2003"},{"abstractinfo":"TB6合金是一种高强高韧近β钛合金.采用Gleeble-3500热模拟试验机对铸态TB6钛合金进行了等温热压缩变形试验,变形温度范围为700～ 900℃,应变速率范围为0.001 ～1.000s-1,研究了铸态TB6合金热变形流变<span style=\"color:red\">应力</span>行为,分析了热压缩后的金相显微组织,基于<span style=\"color:red\">摩擦</span>修正后的流变<span style=\"color:red\">应力</span>曲线采用双曲正弦形式的修正Arrhenius关系对TB6钛合金的本构<span style=\"color:red\">模型</span>进行回归.结果表明:铸态TB6合金的热变形行为对变形温度和应变速率较为敏感,随着变形温度的降低和应变速率的增加流变<span style=\"color:red\">应力</span>显著增大;其热变形机制以动态回复和动态再结晶为主;得到铸态TB6钛合金热变形本构方程,比较回归<span style=\"color:red\">模型</span>计算的<span style=\"color:red\">应力</span>值与实测值其平均相对误差仅为1.48％,因此采用Z参数的双曲正弦函数形式能够较为精确地预测铸态TB6合金高温变形时的流变<span style=\"color:red\">应力</span>.以上研究为TB6钛合金塑性加工过程的模拟和控制提供了理论基础.","authors":[{"authorName":"段园培","id":"fe28af6e-f53c-47a1-afe6-f1ce9776793e","originalAuthorName":"段园培"},{"authorName":"黄仲佳","id":"10753b69-ebbd-428a-9c0c-a1a58525ccd3","originalAuthorName":"黄仲佳"},{"authorName":"余小鲁","id":"ef6f150f-3a2a-4340-8348-0ce7054b7254","originalAuthorName":"余小鲁"},{"authorName":"邢昌","id":"6803081f-e2ed-45b6-9167-adffbd152d53","originalAuthorName":"邢昌"},{"authorName":"孙宇峰","id":"0f8aeb4b-30a3-4a1b-9b85-43ba6a9da2e8","originalAuthorName":"孙宇峰"}],"doi":"10.13373/j.cnki.cjrm.2014.02.005","fpage":"202","id":"4c328e89-dcd4-4ba6-ac3f-094dc40e9cdd","issue":"2","journal":{"abbrevTitle":"XYJS","coverImgSrc":"journal/img/cover/XYJS.jpg","id":"67","issnPpub":"0258-7076","publisherId":"XYJS","title":"稀有金属"},"keywords":[{"id":"56e84a76-af10-4e8b-bc14-c319787fcf33","keyword":"铸态TB6钛合金","originalKeyword":"铸态TB6钛合金"},{"id":"d440e555-616d-487b-8151-a131a3cb9711","keyword":"热变形","originalKeyword":"热变形"},{"id":"39c5638f-33d0-4bbd-8912-73edaa5c86c0","keyword":"流变<span style=\"color:red\">应力</span>","originalKeyword":"流变应力"},{"id":"968ddecc-fd16-44cf-b77d-88b9d1494207","keyword":"<span style=\"color:red\">摩擦</span>修正","originalKeyword":"摩擦修正"},{"id":"6fa4d1ce-c804-49d2-96ca-f869a832de08","keyword":"本构方程","originalKeyword":"本构方程"}],"language":"zh","publisherId":"xyjs201402005","title":"基于<span style=\"color:red\">摩擦</span>修正的TB6合金流变<span style=\"color:red\">应力</span>行为研究及本构<span style=\"color:red\">模型</span>建立","volume":"38","year":"2014"}],"totalpage":3766,"totalrecord":37660}