{"currentpage":1,"firstResult":0,"maxresult":10,"pagecode":5,"pageindex":{"endPagecode":5,"startPagecode":1},"records":[{"abstractinfo":"对工业纯锆进行了不同时间的机械研磨处理(SMAT),利用透射电子显微镜(TEM)和x射线衍射仪(XRD)对试样表层平均晶粒尺寸和平均微观畸变进行了分析表征,采用光学显微镜(OM)观察了试样的横截面显微组织,利用x射线<span style=\"color:red\">应力</span>仪测试了试样距表面不同深度的宏观<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>.结果表明,SMAT处理可以实现工业纯锆的表面纳米化,并且在试样的最表层形成了厚约10 μm的纳米结构.试样表面平均微观畸变随着SMAT处理时间的增加逐渐增大,处理时间为60 min时,平均微观畸变约为0.41％.试样表层的宏观<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>为压<span style=\"color:red\">应力</span>,且表层<span style=\"color:red\">残余</span>压<span style=\"color:red\">应力</span>由表面到基体先增大而后减小.随着处理时间的增加,试样表面<span style=\"color:red\">残余</span>压<span style=\"color:red\">应力</span>σsrs先增大而后减小;<span style=\"color:red\">最大</span><span style=\"color:red\">残余</span>压<span style=\"color:red\">应力</span>σmrs先增大而后趋于稳定,约为-620 MPa;<span style=\"color:red\">最大</span><span style=\"color:red\">残余</span>压<span style=\"color:red\">应力</span>距表面的距离zm和<span style=\"color:red\">残余</span>压<span style=\"color:red\">应力</span>场深度Z0均逐渐增大.","authors":[{"authorName":"张聪惠","id":"8f65af79-fb91-428a-b88a-183c492a6b6c","originalAuthorName":"张聪惠"},{"authorName":"于飞","id":"b1259d53-44c0-4519-a385-a2e562f55077","originalAuthorName":"于飞"},{"authorName":"解钢","id":"062aa067-a36c-4ad8-b323-524382f35b38","originalAuthorName":"解钢"},{"authorName":"王耀勉","id":"df30b9fe-0551-4c21-98e2-68295329792d","originalAuthorName":"王耀勉"},{"authorName":"何晓梅","id":"b7680b88-0454-4de4-9c59-7cedd8ed3f70","originalAuthorName":"何晓梅"}],"doi":"","fpage":"2147","id":"55879cbd-dcc8-4a97-aea7-5b5b956413d8","issue":"9","journal":{"abbrevTitle":"XYJSCLYGC","coverImgSrc":"journal/img/cover/XYJSCLYGC.jpg","id":"69","issnPpub":"1002-185X","publisherId":"XYJSCLYGC","title":"稀有金属材料与工程"},"keywords":[{"id":"4024c7cc-46d6-448b-9d60-f90a0886608f","keyword":"工业纯锆","originalKeyword":"工业纯锆"},{"id":"fb1befe6-1749-40ac-8215-bf041f6852ac","keyword":"表面纳米化","originalKeyword":"表面纳米化"},{"id":"d31e1b98-161a-4ebe-837c-4976f1b7e9f3","keyword":"微观畸变","originalKeyword":"微观畸变"},{"id":"d67ba5e6-d4bf-49d4-a222-606c2c74ce42","keyword":"<span style=\"color:red\">最大</span><span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>","originalKeyword":"最大残余应力"}],"language":"zh","publisherId":"xyjsclygc201409020","title":"表面纳米化工业纯锆的显微组织与<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>研究","volume":"43","year":"2014"},{"abstractinfo":"对<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>的测试在学术研究和工程应用中越来越重要,是获取零件服役条件以及工艺制造的<span style=\"color:red\">应力</span>状态的重要方法 ,可以为零件寿命的预测和制造工艺的控制等提供重要的参考.目前,<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>的测试方法 多样.介绍了<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>的测试方法 及其所能达到的测试层深,以及几种新型的<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>的测试方法 及其适用的范围;阐述了<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>的定义和形成机理,并对引入<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>的常见表面形变强化工艺进行了分析,介绍了不同的工艺下形成的<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>的特征;最后,指出了对目前<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>测试和研究中存在的问题和发展趋势,提出了三维原位无损分析、<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>和模拟相结合的跨学科系统研究以及形成相关的大数据库平台系统将是未来发展的方向.","authors":[{"authorName":"宋俊凯","id":"d6903a04-2212-4371-9e46-3350a7f7763b","originalAuthorName":"宋俊凯"},{"authorName":"黄小波","id":"dedd7322-4d44-4b95-892e-fe6f742fa2f6","originalAuthorName":"黄小波"},{"authorName":"高玉魁","id":"9eddd4e5-4741-4e5d-8aae-4587173c8d52","originalAuthorName":"高玉魁"}],"doi":"10.16490/j.cnki.issn.1001-3660.2016.04.013","fpage":"75","id":"c7d335a8-76cc-42ba-8803-682530f5ffc5","issue":"4","journal":{"abbrevTitle":"BMJS","coverImgSrc":"journal/img/cover/BMJS.jpg","id":"3","issnPpub":"1001-3660","publisherId":"BMJS","title":"表面技术   "},"keywords":[{"id":"df9621f2-bedf-44ae-95c7-68056ef8114c","keyword":"<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>","originalKeyword":"残余应力"},{"id":"b572b3ff-188c-4227-87c3-208da3a5f118","keyword":"表面强化","originalKeyword":"表面强化"},{"id":"62317602-fecc-4d4b-94ed-bf4ddaec696e","keyword":"喷丸","originalKeyword":"喷丸"},{"id":"40130691-1e1f-4be4-be8d-4e497c50ddbe","keyword":"激光冲击强化","originalKeyword":"激光冲击强化"},{"id":"f6c58512-aeed-446c-acc0-5498829a955c","keyword":"疲劳","originalKeyword":"疲劳"},{"id":"7016f7fe-42bd-48a7-9d7e-180b1d525ef4","keyword":"X射线衍射","originalKeyword":"X射线衍射"}],"language":"zh","publisherId":"bmjs201604013","title":"<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>测试分析技术","volume":"45","year":"2016"},{"abstractinfo":"采用双椭球热源模型建立叶轮TIG焊接的移动热源模型,以计算得到的温度历史作为热载荷,计算焊缝附近的<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>分布,通过对比已有的文献实验数据以验证模型的有效性.进一步建立叶轮<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>和<span style=\"color:red\">残余</span>变形的计算模型,分析焊接温度历史、叶轮<span style=\"color:red\">应力</span>和变形历史之间的内在联系,研究焊接参数和叶轮参数对焊后<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>和<span style=\"color:red\">残余</span>变形的影响规律.分析结果表明:在叶轮叶片焊接时,获得的热<span style=\"color:red\">应力</span>随焊接温度的增加而增加,当焊接温度达到峰值时,热<span style=\"color:red\">应力</span>滞后几秒达到<span style=\"color:red\">最大</span>值;随着叶片厚度的增加,焊接变形略有减小,远离焊缝位置的叶片<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>随叶片板厚增加而减小,同时叶片的<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>和变形与叶片和叶轮的刚度比有关.","authors":[{"authorName":"张昭","id":"117e0090-5e4b-446f-8bdb-86b9f64a3b99","originalAuthorName":"张昭"},{"authorName":"葛芃","id":"859c642a-e595-46cb-9ae0-b60f9429d6b8","originalAuthorName":"葛芃"},{"authorName":"张洪武","id":"fa81eff6-363b-4f4e-9077-e06805d95bf2","originalAuthorName":"张洪武"}],"doi":"","fpage":"9","id":"73020da8-8154-4c5d-b6c9-23b805d4a702","issue":"3","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":"43b02156-f34d-4c66-aaad-5d3c8279423c","keyword":"叶轮","originalKeyword":"叶轮"},{"id":"eb625f22-c15d-49be-bf70-656b135b54ce","keyword":"钨极惰性气体焊","originalKeyword":"钨极惰性气体焊"},{"id":"adc30102-b2d3-4a14-9560-f78c89404364","keyword":"<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>","originalKeyword":"残余应力"}],"language":"zh","publisherId":"bqclkxygc201603003","title":"焊接叶轮<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>的数值模拟","volume":"39","year":"2016"},{"abstractinfo":"用扫描电子显微镜(SEM)观察了等离子喷涂ZrO2涂层的显微结构,并用X射线衍射法(XRD)测试了ZrO2涂层相的组成和<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>.同时测试了激光冲击处理和激光热处理后的ZrO2涂层<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>分布,分析了热障涂层<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>形成机理.结果表明,等离子喷涂ZrO2涂层表面<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>均为拉<span style=\"color:red\">应力</span>,其均值为179.2MPa,经激光表面处理后的ZrO2涂层<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>均表现为压<span style=\"color:red\">应力</span>;热<span style=\"color:red\">应力</span>对涂层<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>贡献<span style=\"color:red\">最大</span>,当热<span style=\"color:red\">应力</span>超过涂层结合强度时,涂层脱落,通过控制涂层<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>可以提高涂层界面结合强度.","authors":[{"authorName":"孔德军","id":"d550f937-5f64-4b39-9c18-109fbad4bb61","originalAuthorName":"孔德军"},{"authorName":"张永康","id":"0745b025-47f8-4a7f-a855-299262e2d926","originalAuthorName":"张永康"},{"authorName":"朱伟","id":"f4dac392-ad38-4c1d-8df4-56d60f0bb90b","originalAuthorName":"朱伟"},{"authorName":"邹世坤","id":"40afd085-eed8-4afd-813a-9633701406c7","originalAuthorName":"邹世坤"}],"doi":"","fpage":"128","id":"5d1762fd-e33b-4d5f-9b5a-48aa2ffdf677","issue":"1","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":"b3ef4cf6-ca21-4203-a233-a08321729130","keyword":"ZrO2涂层","originalKeyword":"ZrO2涂层"},{"id":"c511df36-2834-4f7a-816b-1b40e4420958","keyword":"X衍射法(XRD)","originalKeyword":"X衍射法(XRD)"},{"id":"3ad7ce09-0477-4806-9a21-9dd86ab90bba","keyword":"<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>","originalKeyword":"残余应力"},{"id":"5f4c5268-084d-4390-b823-ac25e026a7cc","keyword":"激光冲击处理","originalKeyword":"激光冲击处理"},{"id":"b6310bbb-4a8f-4d1a-8fab-2490dae5b684","keyword":"激光热处理","originalKeyword":"激光热处理"}],"language":"zh","publisherId":"jsrclxb200801030","title":"ZrO2热障涂层<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>分析","volume":"29","year":"2008"},{"abstractinfo":"<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>对于型钢产品的使用性能有重要影响。应用X射线衍射方法对方形型钢的<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>进行了测量，分析了<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>在型钢各个部位的分布情况，探讨了不同成形工艺、尺寸、厚度材料生产的方形型钢产品<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>分布的差异。研究结果表明型钢焊缝处的<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span><span style=\"color:red\">最大</span>，<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>在外表面为拉<span style=\"color:red\">应力</span>，内表面为压<span style=\"color:red\">应力</span>，不同成形工艺与外形尺寸对于<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>的分布有较大影响。研究结果可为工艺设计人员和型钢使用人员提供有益的参考。","authors":[{"authorName":"曾国","id":"943dc8d9-af06-4d98-8bef-fb539449ff40","originalAuthorName":"曾国"},{"authorName":"郭永进","id":"8c68854b-7e75-46c1-9025-29341c5bcab0","originalAuthorName":"郭永进"},{"authorName":"于忠奇","id":"2b03f148-923a-4532-86f5-b09fb98cb155","originalAuthorName":"于忠奇"},{"authorName":"来新民","id":"22fa5bcd-6709-471f-9d20-e53c28605d40","originalAuthorName":"来新民"}],"categoryName":"|","doi":"","fpage":"29","id":"c92c817b-af30-4418-be7f-e5826b135aad","issue":"11","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":"30cf2f77-6094-4943-9c69-347fa80a6bd1","keyword":"辊弯成形;方形型钢;<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>","originalKeyword":"辊弯成形;方形型钢;残余应力"}],"language":"zh","publisherId":"1001-0963_2008_11_2","title":"辊弯成形方形型钢的<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>","volume":"20","year":"2008"},{"abstractinfo":"<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>对于型钢产品的使用性能有重要影响.应用X射线衍射方法对方形型钢的<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>进行了测量,分析了<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>在型钢各个部位的分布情况,探讨了不同成形工艺、尺寸、厚度材料生产的方形型钢产品<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>分布的差异.研究结果表明型钢焊缝处的<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span><span style=\"color:red\">最大</span>,<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>在外表面为拉<span style=\"color:red\">应力</span>,内表面为压<span style=\"color:red\">应力</span>,不同成形工艺与外形尺寸对于<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>的分布有较大影响.研究结果可为工艺设计人员和型钢使用人员提供有益的参考.","authors":[{"authorName":"曾国","id":"a135b8fd-a034-4379-80c3-882ad058a966","originalAuthorName":"曾国"},{"authorName":"郭永进","id":"e447c1a5-aad7-42a9-b267-bf930114dff5","originalAuthorName":"郭永进"},{"authorName":"于忠奇","id":"d8521cd6-1e44-417c-a631-06d063be7c14","originalAuthorName":"于忠奇"},{"authorName":"来新民","id":"d95ef1c0-3ce8-49e7-a99a-2056fcff1cf7","originalAuthorName":"来新民"}],"doi":"","fpage":"29","id":"f4444fc9-ced6-437b-80cc-7598ce2587c8","issue":"11","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":"d22e31e8-decf-4adc-90e9-8bdb135af568","keyword":"辊弯成形","originalKeyword":"辊弯成形"},{"id":"2004572d-d7a8-4a3d-b6a7-0e80e133e986","keyword":"方形型钢","originalKeyword":"方形型钢"},{"id":"7a71916c-7428-473c-ba2e-43db2a6850a8","keyword":"<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>","originalKeyword":"残余应力"}],"language":"zh","publisherId":"gtyjxb200811007","title":"辊弯成形方形型钢的<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>","volume":"20","year":"2008"},{"abstractinfo":"通过对压痕过程进行理论分析,基于能量法研究了<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>测试原理和方法.通过张量分解,推导了<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>在压痕过程中所做的功;通过有限元分析,总结了<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>对压痕过程的影响;根据功与能量的关系,建立了压痕功与<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>之间的解析模型,并推导了<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>求解公式.结果表明:<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>对压痕加载的初始阶段影响很大,但对加载的后半阶段和卸载过程的影响很小,可忽略不计,并且拉<span style=\"color:red\">应力</span>对压痕过程的影响明显大于压<span style=\"color:red\">应力</span>,可以认为压痕在加载过程中是一个弹塑性的变形过程,而在卸载过程中是弹性变形过程;试验证明了所建立的<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>模型求解的<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>是准确可靠的,可以用于<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>的测试.","authors":[{"authorName":"董达善","id":"221b778d-ca0c-4903-b9c0-45970ac0bc71","originalAuthorName":"董达善"},{"authorName":"俞翔栋","id":"a02349fc-6473-4e99-bd6f-d3272eec461e","originalAuthorName":"俞翔栋"}],"doi":"","fpage":"92","id":"14d87e96-3b38-4462-92a4-8087f679fc58","issue":"12","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":"63a8106d-1421-4039-be00-f4deb522184f","keyword":"<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>","originalKeyword":"残余应力"},{"id":"54c70fca-c1d6-425b-b2d8-c0168d7e8b53","keyword":"能量法","originalKeyword":"能量法"},{"id":"28c0eed6-fa97-4e60-accf-8ddea0efb0fb","keyword":"压痕","originalKeyword":"压痕"},{"id":"96b2a667-3ef5-4756-80c4-099ba071f140","keyword":"硬度","originalKeyword":"硬度"}],"language":"zh","publisherId":"jxgccl201412021","title":"基于能量法的<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>测试","volume":"38","year":"2014"},{"abstractinfo":"采用有限元法,对结构一定的Al/Ni-ZrO2梯度涂层在基体条件改变时涂层的<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>进行了分析,结果表明,基体材料的热膨胀系数对涂层的<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>有显著的影响,对于基体为圆柱形的涂层,其基体与涂层界面的<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>梯度、<span style=\"color:red\">最大</span>轴向拉<span style=\"color:red\">应力</span>均随热膨胀系数的增大而线性增大,表面纯陶瓷层与次层界面<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>梯度则随之减小.增大基体的直径和厚度,可缓和涂层<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>,并在基体直径为36mm,厚度为20mm时各<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>基本稳定.","authors":[{"authorName":"马壮","id":"bd7a310f-2ad8-463b-b03a-8511d564dd89","originalAuthorName":"马壮"},{"authorName":"王全胜","id":"3fd5ee29-a32c-4349-8950-84fe8886a1e6","originalAuthorName":"王全胜"},{"authorName":"王富耻","id":"f6a2ff7a-0368-444c-aa16-d5e2b7490bf8","originalAuthorName":"王富耻"},{"authorName":"吕广庶","id":"8f488e22-8628-4d15-a6b0-7021fceb751d","originalAuthorName":"吕广庶"}],"doi":"10.3969/j.issn.1001-4381.2002.04.005","fpage":"15","id":"4e9a8aa3-787b-4376-b84c-7f085b7c54e5","issue":"4","journal":{"abbrevTitle":"CLGC","coverImgSrc":"journal/img/cover/CLGC.jpg","id":"9","issnPpub":"1001-4381","publisherId":"CLGC","title":"材料工程"},"keywords":[{"id":"bc3d3c34-68af-4c89-b560-2e14e80a46b5","keyword":"梯度涂层","originalKeyword":"梯度涂层"},{"id":"29a1a4aa-9178-4f07-8313-d7d59d6b0540","keyword":"有限元法","originalKeyword":"有限元法"},{"id":"12ddc50e-f09a-4daf-888b-b9961df711f9","keyword":"<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>","originalKeyword":"残余应力"},{"id":"6d94ce9c-9b5c-4cb6-8b66-e3d2c932e66a","keyword":"基体","originalKeyword":"基体"}],"language":"zh","publisherId":"clgc200204005","title":"涂层基体条件对梯度涂层<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>影响研究","volume":"","year":"2002"},{"abstractinfo":"针对纤维交叉起伏区域<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>,建立一种细观分析模型.基于热传导方程、固化反应动力学模型和复合材料层合理论,采用有限元方法和细观分析模型,对缠绕复合材料在固化工艺过程中的<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>分布及其变化规律进行数值模拟.通过算例,研究纤维起伏区域<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>的分布特点,结果表明:起伏纤维束不同位置处<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>差别很大,层合区纤维束呈现拉<span style=\"color:red\">应力</span>状态,起伏区纤维束呈现压<span style=\"color:red\">应力</span>状态,富树脂区出现<span style=\"color:red\">最大</span>压<span style=\"color:red\">应力</span>;<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>沿纤维束起伏方向呈现V型变化趋势,在纤维束上不同位置出现拉、压不同的<span style=\"color:red\">应力</span>状态,起伏角度<span style=\"color:red\">最大</span>处出现<span style=\"color:red\">最大</span>压<span style=\"color:red\">应力</span>.","authors":[{"authorName":"和欣辉","id":"f4537ed2-4350-4ee9-9401-d637c9c20aaa","originalAuthorName":"和欣辉"},{"authorName":"韩小平","id":"15ce19fd-3e71-49b2-baf9-7597edba726e","originalAuthorName":"韩小平"}],"doi":"10.11868/j.issn.1001-4381.2016.04.013","fpage":"76","id":"bfa78269-009b-4d8a-a53b-a313e8c43cac","issue":"4","journal":{"abbrevTitle":"CLGC","coverImgSrc":"journal/img/cover/CLGC.jpg","id":"9","issnPpub":"1001-4381","publisherId":"CLGC","title":"材料工程"},"keywords":[{"id":"59aaf022-173d-4989-8a48-a285b54e7c88","keyword":"纤维缠绕复合材料","originalKeyword":"纤维缠绕复合材料"},{"id":"9fa45e87-92cc-476d-8da0-f2cd4fa04378","keyword":"固化过程","originalKeyword":"固化过程"},{"id":"ae714f8a-facd-43e6-b367-75c8326174d5","keyword":"<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>","originalKeyword":"残余应力"},{"id":"dfecc535-d783-426c-be77-904237b91574","keyword":"纤维束交叉起伏","originalKeyword":"纤维束交叉起伏"},{"id":"a57829aa-a370-4c9e-9d31-7f8a022d0450","keyword":"细观模型","originalKeyword":"细观模型"}],"language":"zh","publisherId":"clgc201604013","title":"纤维缠绕复合材料起伏区域<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>","volume":"44","year":"2016"},{"abstractinfo":"运用有限元法，综合考虑了温度、相变及<span style=\"color:red\">应力</span>的耦合作用，对车轮热处理<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>及热处理工艺对它的影响规律进行了分析。模拟分析表明，马钢生产的HDSA车轮踏面的<span style=\"color:red\">最大</span>周向<span style=\"color:red\">残余</span>压<span style=\"color:red\">应力</span>为140MPa左右，压<span style=\"color:red\">应力</span>区深度达到382 mm。得到了淬火温度、淬火时间、回火温度和回火时间对踏面上周向<span style=\"color:red\">残余</span>压<span style=\"color:red\">应力</span>和踏面下压<span style=\"color:red\">应力</span>区深度的影响规律，其中回火温度对踏面上的<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>影响<span style=\"color:red\">最大</span>。","authors":[{"authorName":"沈晓辉","id":"af8ca005-7b29-4d66-a559-3cded53c55d5","originalAuthorName":"沈晓辉"},{"authorName":"赵亚琼","id":"305fbaba-c92d-4915-95cf-070c26477962","originalAuthorName":"赵亚琼"},{"authorName":"安涛","id":"41c8cd14-8363-4c1c-947d-968c619c4553","originalAuthorName":"安涛"},{"authorName":"章静","id":"b352963d-24d1-4c5a-b4ba-d6883de0d929","originalAuthorName":"章静"},{"authorName":"闫军","id":"cdb7aed3-351b-429d-a48d-507a0cb06a9a","originalAuthorName":"闫军"}],"categoryName":"|","doi":"","fpage":"0","id":"114e16ab-1b42-41f5-9e30-d30f5ed7bd99","issue":"10","journal":{"abbrevTitle":"GT","coverImgSrc":"journal/img/cover/GT.jpg","id":"27","issnPpub":"0449-749X","publisherId":"GT","title":"钢铁"},"keywords":[{"id":"66d7a2e0-b626-42e5-851f-4736683084b2","keyword":"车轮;热处理;<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>;影响;有限元","originalKeyword":"车轮;热处理;残余应力;影响;有限元"}],"language":"zh","publisherId":"0449-749X_2007_10_1","title":"热处理工艺对车轮<span style=\"color:red\">残余</span><span style=\"color:red\">应力</span>的影响","volume":"42","year":"2007"}],"totalpage":2395,"totalrecord":23949}