工程热物理学报 , 2010, 31(10): 1643-1646.
新型CO2分离压缩一体化方法
徐钢 1, , 杨勇平 2, , 段立强 3, {"currentpage":1,"firstResult":0,"maxresult":10,"pagecode":5,"pageindex":{"endPagecode":5,"startPagecode":1},"records":[{"abstractinfo":"用拉伸实验研究了退火温度(θan)和应力-应变循环对Ti-50.8Ni-0.3Cr合金超弹性(SE)的影响.结果表明,随θan升高,应力诱发马氏体(M)相变的临界应力σM先降低后升高,随后趋于稳定,分别在450和600℃达到最小值(311 MPa)和最大值(583 MPa).残余应变在θan=350-590℃之间变化不大,始终保持在较低的水平;当θan高于590℃时,残余应变则急剧升高.随着应力-应变循环次数(N)增加,350和590℃退火态合金由部分非线性超弹性逐渐转变为完全非线性超弹性,而650℃退火态合金由部分非线性超弹性逐渐转变为线性超弹性.此外,随N增加,590和650℃退火态合金的能耗作用逐渐下降,并趋于稳定,而350℃退火态合金的能耗作用基本保持不变.要使Ti-50.8Ni-0.3Cr合金获得良好的SE,退火温度应低于再结晶温度.","authors":[{"authorName":"王启","id":"8aa9d196-6806-4b73-b27e-340fc8a1f94e","originalAuthorName":"王启"},{"authorName":"贺志荣","id":"310f9f7c-2666-42fa-9095-d9d1988e5aa6","originalAuthorName":"贺志荣"},{"authorName":"王永善","id":"408fa5b1-159e-48b2-a0de-f98a643a8bd6","originalAuthorName":"王永善"},{"authorName":"杨军","id":"1ddcc713-0319-4ce8-b455-d541415b2a40","originalAuthorName":"杨军"}],"doi":"10.3724/SP.J.1037.2010.00047","fpage":"800","id":"dbdbc6b1-c6e5-4686-adfe-9bed531f2127","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":"4f12962b-5209-4746-a0e2-f0681971d4d0","keyword":"Ti-Ni-Cr合金","originalKeyword":"Ti-Ni-Cr合金"},{"id":"f4c7c748-34aa-4a2e-ba19-4fea3607e911","keyword":"形状记忆合金","originalKeyword":"形状记忆合金"},{"id":"afcc28a7-3aed-4afd-8eb0-bc9ff9da04ab","keyword":"退火温度","originalKeyword":"退火温度"},{"id":"541f8eaf-41c1-422d-ba49-8c5596b00cc3","keyword":"应力-应变循环","originalKeyword":"应力-应变循环"},{"id":"28f134e7-8e3d-42c0-9357-e78dd60197f1","keyword":"超弹性","originalKeyword":"超弹性"}],"language":"zh","publisherId":"jsxb201007006","title":"退火温度和应力-应变循环对Ti-Ni-Cr形状记忆合金超弹性的影响","volume":"46","year":"2010"},{"abstractinfo":"用示差扫描量热仪、拉伸实验和应力-应变循环实验系统研究了退火温度、变形温度以及热循环和室温应力-应变循环对Ti49.4Ni50.6超弹性(SE)弹簧的相变和形变特性的影响冷加工加中温退火态Ti49.4Ni50.6合金冷却()加热时的相变类型为母相B2()R相()马氏体B19'.随退火温度升高,马氏体转变温度升高,R相转变温度降低623-773 K退火态Ti49.4Ni50.6弹簧室温下可获得SE特性,随变形温度升高,SE弹簧刚度增加;当退火温度超过823 K后,SE特性变差.热循环时SE弹簧的切变量取值越小,其应变恢复率越高预循环训练可增强SE的稳定性.","authors":[{"authorName":"贺志荣","id":"cab297b7-ae27-402b-87f2-99f5bbcc891c","originalAuthorName":"贺志荣"},{"authorName":"张永宏","id":"08368681-8d1f-4034-a6d3-c865ea84e1bb","originalAuthorName":"张永宏"},{"authorName":"王永善","id":"2c894b64-c246-43f3-ba9a-f4817d7f3f0d","originalAuthorName":"王永善"},{"authorName":"周敬恩","id":"ef564c61-fcdc-40ab-9b37-bd7d07fa8850","originalAuthorName":"周敬恩"}],"doi":"10.3321/j.issn:0412-1961.2004.01.009","fpage":"46","id":"a9e75494-1da1-4ffd-81a3-9bf7d700bce6","issue":"1","journal":{"abbrevTitle":"JSXB","coverImgSrc":"journal/img/cover/JSXB.jpg","id":"48","issnPpub":"0412-1961","publisherId":"JSXB","title":"金属学报"},"keywords":[{"id":"5e5af7de-0da8-4e97-9c1d-15ef9bd04240","keyword":"TiNi","originalKeyword":"TiNi"},{"id":"205b37b4-5095-4900-94a0-c4d7ff49788c","keyword":"形状记忆合金","originalKeyword":"形状记忆合金"},{"id":"fd60e3ef-4ef1-431a-a76d-ba448ef13e92","keyword":"超弹性弹簧","originalKeyword":"超弹性弹簧"},{"id":"1121066e-fd5e-4d73-9af1-02db383fe8da","keyword":"相变","originalKeyword":"相变"},{"id":"d3880812-5a77-41af-8b48-842a237a6f2a","keyword":"应力-应变循环","originalKeyword":"应力-应变循环"}],"language":"zh","publisherId":"jsxb200401009","title":"Ti49.4Ni50.6超弹性弹簧的相变和形变特性","volume":"40","year":"2004"},{"abstractinfo":"Ti-Ni形状记忆舍金具有超弹性特性,所显示出的恒弹力、大应变、非线性阻尼和高弹性模量效应可被用来制作储能器、振动控制器和耐磨零件等.评述了Ti-Ni形状记忆合金超弹性的影响因素和计算模拟研究现状.着重介绍了合金成分、热处理、应力-应变循环、冷变形量和实验温度对超弹性的影响,并指出开发多元系Ti-Ni-X超弹性合金和加强合金的超弹性计算模拟是今后的主要研究方向.","authors":[{"authorName":"王启","id":"b2374773-e932-4ae8-9be6-56f42f855553","originalAuthorName":"王启"},{"authorName":"贺志荣","id":"750cdd17-cb78-4a9b-81f4-f12918230d2d","originalAuthorName":"贺志荣"},{"authorName":"王芳","id":"11f6a0b2-2ae1-4b0f-b6c1-0b2842c0f218","originalAuthorName":"王芳"},{"authorName":"刘艳","id":"bdf4960f-e860-469a-8260-d2b14a78f5e3","originalAuthorName":"刘艳"},{"authorName":"杨军","id":"f437e4a5-1707-408b-9469-1e47c3fa7eca","originalAuthorName":"杨军"}],"doi":"","fpage":"85","id":"76ddc5f3-876a-41ad-8b0f-c99d92d50e7b","issue":"13","journal":{"abbrevTitle":"CLDB","coverImgSrc":"journal/img/cover/CLDB.jpg","id":"8","issnPpub":"1005-023X","publisherId":"CLDB","title":"材料导报"},"keywords":[{"id":"579660be-5c10-4470-bd03-f1c65fd7f6b0","keyword":"I-Ni形状记忆合金","originalKeyword":"I-Ni形状记忆合金"},{"id":"73714b20-6291-4540-816f-dd822ceab3b4","keyword":"超弹性","originalKeyword":"超弹性"},{"id":"91b9bc40-fe0d-4f37-8ec5-2fc7f5f636e7","keyword":"计算模拟","originalKeyword":"计算模拟"},{"id":"423d747b-43a5-4e84-a169-d9c2c2da6794","keyword":"热处理","originalKeyword":"热处理"},{"id":"c03d93b0-eed6-4c3c-888d-512e8c27f50e","keyword":"应力-应变循环","originalKeyword":"应力-应变循环"}],"language":"zh","publisherId":"cldb201013019","title":"Ti-Ni形状记忆合金超弹性的研究进展","volume":"24","year":"2010"},{"abstractinfo":"本文在一个较宽的塑性应变幅范围（γpl=1.1×10-4-7．2×10-3）内研究了[011]多滑移取向铜单晶体的循环形变行为.结果表明，[011]晶体的循环形变行为明显不同于[011]和[111]多滑移取向的铜单晶体.[011]晶体具有较低的初始硬化速率，即使在较高的塑性应变幅下，初始硬化速率也无明显变化.［011］晶体的循环应力-应变曲线（CSSC）在所研究的塑性应变幅范围内呈现平台区.CSSC上是否存在平台区，主要由晶体本身的滑移特点和相应的位错反应所决定.疲劳滞后回线形状参数VH在某种程度上可用于确定[011]多滑移铜单晶体的PSB萌生应力","authors":[{"authorName":"李小武","id":"1b9c2332-20ec-4b35-a9b1-0986e36a8ef6","originalAuthorName":"李小武"},{"authorName":"王中光","id":"634b27e9-3610-453b-b153-fb58d8b922e0","originalAuthorName":"王中光"},{"authorName":"孙守光","id":"5a49331b-867a-4c51-a707-95040c1d7afb","originalAuthorName":"孙守光"},{"authorName":"吴世丁","id":"f24d3341-ad9a-4ebb-a082-5859b207f975","originalAuthorName":"吴世丁"},{"authorName":"李守新","id":"f36f2435-61e8-44f9-bbb9-348786043cd1","originalAuthorName":"李守新"},{"authorName":"李广义","id":"0d41b965-b55d-4460-ab2c-d1be90e3d018","originalAuthorName":"李广义"}],"categoryName":"|","doi":"","fpage":"545","id":"ec88bf09-1e0c-4ab1-b037-7454128caa9b","issue":"5","journal":{"abbrevTitle":"JSXB","coverImgSrc":"journal/img/cover/JSXB.jpg","id":"48","issnPpub":"0412-1961","publisherId":"JSXB","title":"金属学报"},"keywords":[{"id":"76b9d913-2f90-49a0-aac4-1ab399fcb7ad","keyword":"[011]多滑移取向铜单晶体","originalKeyword":"[011]多滑移取向铜单晶体"},{"id":"99098634-9df9-4997-8153-03cd4ba46c71","keyword":" cyclic deformation","originalKeyword":" cyclic deformation"},{"id":"af23de17-127e-42ba-83c1-2e3b34ef240f","keyword":"hysteresis loop","originalKeyword":"hysteresis loop"},{"id":"27e34c7b-a3ee-4c03-8828-8efc818608dd","keyword":" plateau region in CSSC","originalKeyword":" plateau region in CSSC"}],"language":"zh","publisherId":"0412-1961_1998_5_3","title":"[011]多滑移取向铜单晶体的循环形变行为──Ⅰ.循环应力-应变响应","volume":"34","year":"1998"},{"abstractinfo":"针对奥氏体0Cr20Ni12Mn5Mo2NbN钢开展了系列应变幅的循环加载试验,分析了其循环应力应变特性,结果表明,循环全过程中真应力和真应变呈指数关系,基于该指数关系提出了描述循环应力应变关系的本构模型:σ=σ0+α·exp(β·ε).","authors":[{"authorName":"高珍鹏","id":"47881bd5-a9c5-40d0-9466-4454c8e9dfcd","originalAuthorName":"高珍鹏"},{"authorName":"薛钢","id":"3725aa24-fcdd-4e9f-b81e-db6e0f20f8eb","originalAuthorName":"薛钢"},{"authorName":"宫旭辉","id":"333945b1-5a4e-4d3e-ba86-96e1b56960c6","originalAuthorName":"宫旭辉"}],"doi":"","fpage":"5","id":"0dac3a5e-098a-44dc-bf27-6ae200956b53","issue":"6","journal":{"abbrevTitle":"CLKFYYY","coverImgSrc":"journal/img/cover/CLKFYYY.jpg","id":"10","issnPpub":"1003-1545","publisherId":"CLKFYYY","title":"材料开发与应用"},"keywords":[{"id":"918c0b6c-9473-4e06-aaad-11f9e82b14ce","keyword":"0Cr20Ni12Mn5Mo2NbN钢","originalKeyword":"0Cr20Ni12Mn5Mo2NbN钢"},{"id":"f60e9530-e95c-4477-959a-650ce090306a","keyword":"循环应力应变","originalKeyword":"循环应力应变"},{"id":"83e887e7-9199-46a0-bd8b-5ccfffd157df","keyword":"本构关系","originalKeyword":"本构关系"}],"language":"zh","publisherId":"clkfyyy201506002","title":"0Cr20Ni12Mn5Mo2NbN钢循环应力应变本构关系","volume":"30","year":"2015"},{"abstractinfo":"在室温下对304不锈钢进行了多种长短轴比的椭圆形、菱形等非比例循环加载路径下的应力与应变路径形状、路径的应力与应变幅值、平均应变及其加载历史的影响的系统实验. 结果表明, 材料的循环塑性行为强烈地依赖于应力与应变路径形状、路径的应力与应变幅值及其加载历史.","authors":[{"authorName":"杨显杰","id":"0b6b9a9a-88f0-4eb1-97aa-6c03bfdeea55","originalAuthorName":"杨显杰"},{"authorName":"高庆","id":"898af18a-cf0b-41b8-be87-9c810f06b2db","originalAuthorName":"高庆"},{"authorName":"蔡力勋","id":"0d230308-5153-4466-9aa7-43f350d7c968","originalAuthorName":"蔡力勋"},{"authorName":"刘宇杰","id":"2b68bbba-9521-4bbc-ae47-bf36ca278d08","originalAuthorName":"刘宇杰"}],"categoryName":"|","doi":"","fpage":"935","id":"61b88a81-1421-4bde-b01b-509d6d9061c0","issue":"9","journal":{"abbrevTitle":"JSXB","coverImgSrc":"journal/img/cover/JSXB.jpg","id":"48","issnPpub":"0412-1961","publisherId":"JSXB","title":"金属学报"},"keywords":[{"id":"e0cdec94-406e-4a55-9f72-cc509fa20afc","keyword":"304不锈钢","originalKeyword":"304不锈钢"},{"id":"65bb9bdf-ad04-4eb3-9ae4-193a940713df","keyword":"nonproportional loading","originalKeyword":"nonproportional loading"},{"id":"e36d6cbb-7089-43c2-bfc8-d07abaf4f016","keyword":"ratcheting","originalKeyword":"ratcheting"}],"language":"zh","publisherId":"0412-1961_2004_9_10","title":"304不锈钢在室温下非比例应力和应变循环变形行为实验研究","volume":"40","year":"2004"},{"abstractinfo":"在室温下对304不锈钢进行了多种长短轴比的椭圆形、菱形等非比例循环加载路径下的应力与应变路径形状、路径的应力与应变幅值、平均应变及其加载历史的影响的系统实验.结果表明,材料的循环塑性行为强烈地依赖于应力与应变路径形状、路径的应力与应变幅值及其加载历史.","authors":[{"authorName":"杨显杰","id":"f891eeaf-fdb4-4f72-a2e6-dfd0391855ac","originalAuthorName":"杨显杰"},{"authorName":"高庆","id":"f0413758-1fbc-459f-bc63-6419f3f84e25","originalAuthorName":"高庆"},{"authorName":"蔡力勋","id":"24cf4041-2af8-420b-a348-821de219fd7d","originalAuthorName":"蔡力勋"},{"authorName":"刘宇杰","id":"7f9a00b6-fb8f-47d1-9c9a-90a799254f87","originalAuthorName":"刘宇杰"}],"doi":"10.3321/j.issn:0412-1961.2004.09.008","fpage":"935","id":"c2ef7f0e-c2b5-4f45-bef6-5eef991c25a2","issue":"9","journal":{"abbrevTitle":"JSXB","coverImgSrc":"journal/img/cover/JSXB.jpg","id":"48","issnPpub":"0412-1961","publisherId":"JSXB","title":"金属学报"},"keywords":[{"id":"a8e52933-feb8-460d-b6a1-a6d43808860e","keyword":"304不锈钢","originalKeyword":"304不锈钢"},{"id":"81249b7c-04a7-4ad5-8e7b-f99edfc651be","keyword":"非比例加载","originalKeyword":"非比例加载"},{"id":"7fd3c5d8-0dee-450f-b6f0-e37f4da6fb27","keyword":"棘轮行为","originalKeyword":"棘轮行为"},{"id":"7d798024-1f23-4561-b34d-d24b8ce7e842","keyword":"循环塑性","originalKeyword":"循环塑性"}],"language":"zh","publisherId":"jsxb200409008","title":"304不锈钢在室温下非比例应力和应变循环变形行为实验研究","volume":"40","year":"2004"},{"abstractinfo":"提出了一种以Ramberg-Osgood模型计算曲线作为试验曲线来建立描述金属材料稳态循环应力-应变曲线的Chaboche本构模型的方法,并采用TC11钛合金疲劳试验数据加以验证.结果表明:提出的建立金属材料稳态循环塑性本构模型的方法是可行的,采用建立的Chaboche模型可以较准确地描述金属材料的稳态循环应力、应变响应,与工程中常用的Ramberg-Osgood模型具有基本相同的描述效果;可方便将该模型应用于疲劳寿命预测时金属材料结构的有限元应力、应变分析.","authors":[{"authorName":"吴志荣","id":"6cfa69b1-163f-44c2-a57e-b34c811b1dde","originalAuthorName":"吴志荣"},{"authorName":"胡绪腾","id":"44322106-68db-40b0-baa9-dca16c40d3df","originalAuthorName":"胡绪腾"},{"authorName":"辛朋朋","id":"84e6e784-b733-4550-825e-ea4436001866","originalAuthorName":"辛朋朋"},{"authorName":"宋迎东","id":"32ab3c93-7a2f-4ec9-a74a-49296b75e718","originalAuthorName":"宋迎东"}],"doi":"","fpage":"92","id":"2c477a67-d75e-46c6-8477-b9c514717fbb","issue":"10","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":"8bdb473f-b067-4b6a-a494-dd3b303eca82","keyword":"金属材料","originalKeyword":"金属材料"},{"id":"117ebc8c-626d-4032-831c-8d48b64d5025","keyword":"循环应力-应变曲线","originalKeyword":"循环应力-应变曲线"},{"id":"cb49fa7c-4628-43fb-834c-dcf80894afbb","keyword":"本构模型","originalKeyword":"本构模型"},{"id":"af9df6a0-3077-4e33-9c60-52562d3d09b2","keyword":"Ramberg-Osgood模型","originalKeyword":"Ramberg-Osgood模型"},{"id":"ba4f3dea-a4b2-4232-9012-53f3e8c9cd3b","keyword":"Chaboche模型","originalKeyword":"Chaboche模型"}],"language":"zh","publisherId":"jxgccl201310021","title":"基于Chaboche模型的金属材料稳态循环应力-应变曲线的本构建模方法","volume":"37","year":"2013"},{"abstractinfo":"用拉伸实验研究了退火温度(θan)和应力-应变循环对Ti-50.8Ni-0.3Cr合金超弹性(SE)的影响. 结果表明, 随θan升高, 应力诱发马氏体(M)相变的临界应力σM先降低后升高, 随后趋于稳定, 分别在450和600℃达到最小值(311 MPa)\\linebreak 和最大值(583 MPa). 残余应变在θan=350-590℃之间变化不大, 始终保持在较低的水平; 当θan高于590℃时, 残余应变则急剧升高. 随着应力-应变循环次数(N)增加, 350和590℃退火态合金由部分非线性超弹性逐渐转变为完全非线性超弹性, 而650℃退火态合金由部分非线性超弹性逐渐转变为线性超弹性. 此外, 随N增加, 590和650℃退火态合金的能耗作用逐渐下降, 并趋于稳定, 而350℃退火态合金的能耗作用基本保持不变. 要使Ti-50.8Ni-0.3Cr合金获得良好的SE, 退火温度应低于再结晶温度.","authors":[{"authorName":"王启贺志荣王永善杨军","id":"4d73b93f-3f98-4e8f-bbc4-8bb0b0d3fd40","originalAuthorName":"王启贺志荣王永善杨军"}],"categoryName":"|","doi":"10.3724/SP.J.1037.2010.00047","fpage":"800","id":"aac88e5d-bd9b-4c65-8c11-a9b5513c4f84","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":"f8c48e16-e410-4040-b64a-85f32c5cb274","keyword":"Ti-Ni-r合金","originalKeyword":"Ti-Ni-r合金"},{"id":"6e97ac71-0fd4-4172-b30f-9908ab464012","keyword":"shape memory alloy","originalKeyword":"shape memory alloy"},{"id":"83c073ec-ecf6-4d4f-a4eb-bc7e95420d4f","keyword":"annealing temperature","originalKeyword":"annealing temperature"},{"id":"7c7550b5-133a-43b0-b02a-039d2944ec10","keyword":"stress-strain cycle","originalKeyword":"stress-strain cycle"},{"id":"60779cf4-e9d1-4bb1-b8ef-c73078c0acb7","keyword":"superelasticity","originalKeyword":"superelasticity"}],"language":"zh","publisherId":"0412-1961_2010_7_9","title":"退火温度和应力-应变循环对Ti-Ni-Cr形状记忆合金超弹性的影响","volume":"46","year":"2010"},{"abstractinfo":"对调质处理的45碳钢进行了不同应变幅值的对称应变和具有平均应变控制下的屈服面半径和背应力演化分析,及具有不同平均应力的低应力、较高应力幅值控制下的屈服面半径和背应力演化分析.研究表明:屈服面半径在给定应变幅值下随循环周次的增加而变小,且随循环塑性应变幅值增大而减小,在单调加载时增大;循环背应力幅值随单调应变而减小,随循环塑性应变幅值增大而增大.","authors":[{"authorName":"杨显杰","id":"8505b70f-eda4-46bd-8cc3-dd26b033cef5","originalAuthorName":"杨显杰"},{"authorName":"罗艳","id":"28dac5dc-4859-4610-8aaa-c0af9b304555","originalAuthorName":"罗艳"},{"authorName":"高庆","id":"d7e7db16-0442-46b5-bac6-3de02a186bdc","originalAuthorName":"高庆"},{"authorName":"蔡力勋","id":"ab6e1222-aa0a-4efe-9be6-497b0a22e2a2","originalAuthorName":"蔡力勋"}],"doi":"10.3321/j.issn:0412-1961.2005.02.005","fpage":"133","id":"ca18014b-fe96-4e0a-84f7-91043bd6296e","issue":"2","journal":{"abbrevTitle":"JSXB","coverImgSrc":"journal/img/cover/JSXB.jpg","id":"48","issnPpub":"0412-1961","publisherId":"JSXB","title":"金属学报"},"keywords":[{"id":"df4bbfe7-a379-4c4a-9a12-b3f46c61c26d","keyword":"45钢","originalKeyword":"45钢"},{"id":"1d9b3551-9399-4077-9e3f-198557a2ec27","keyword":"棘轮变形","originalKeyword":"棘轮变形"},{"id":"10d0e229-fc43-4700-b0d6-ab329341a78a","keyword":"循环塑性","originalKeyword":"循环塑性"},{"id":"c87c5238-5abd-47be-849d-2e071b4e8cd9","keyword":"随动硬化","originalKeyword":"随动硬化"}],"language":"zh","publisherId":"jsxb200502005","title":"45钢在应变循环与棘轮变形下的随动硬化演化实验研究","volume":"41","year":"2005"}],"totalpage":2248,"totalrecord":22480}