{"currentpage":1,"firstResult":0,"maxresult":10,"pagecode":5,"pageindex":{"endPagecode":5,"startPagecode":1},"records":[{"abstractinfo":"研究了C和Nb含量对TP347HFG钢在650℃析出<span style=\"color:red\">相</span><span style=\"color:red\">参量</span>(成分、体积分数和尺寸)和持久寿命的影响.对ASME成分范围内的2种不同C和Nb含量的TP347HFG钢在650℃,230和150 MPa条件下进行持久实验,持久寿命分别为199,420 h和2426,8837 h,其中C含量较低Nb含量较高的样品持久寿命较长.对持久管样的EPMA-EDS+MPSM和TEM-EDS分析表明,较低的C含量和较高的Nb含量对应较少的M23C6和较多的MX,并阻碍了M23C6的聚集粗化,同时基体中可保留较多的Cr,有利于延长持久寿命.此外,运用热力学软件Thermo-Calc分析了在500-1300℃范围内C和Nb组合含量的变化对各相成分和体积分数的影响,与实验结果相吻合.","authors":[{"authorName":"彭志方","id":"03020c9c-3af9-4059-8abf-3c60ec7447d6","originalAuthorName":"彭志方"},{"authorName":"党莹樱","id":"880b07de-6b73-4b39-80d6-32848e50a2cb","originalAuthorName":"党莹樱"},{"authorName":"彭芳芳","id":"ee667ea9-b343-40fa-8e0e-cbec4257669b","originalAuthorName":"彭芳芳"}],"doi":"10.3724/SP.J.1037.2011.00677","fpage":"450","id":"0b0eb0e4-ce5a-43fe-94e3-bb0cafea894d","issue":"4","journal":{"abbrevTitle":"JSXB","coverImgSrc":"journal/img/cover/JSXB.jpg","id":"48","issnPpub":"0412-1961","publisherId":"JSXB","title":"金属学报"},"keywords":[{"id":"0efb6559-6a81-40f1-ad88-141011235d40","keyword":"TP347HFG钢","originalKeyword":"TP347HFG钢"},{"id":"edc08d54-7c7e-4cff-9c94-9a7feceaf69d","keyword":"C和Nb含量","originalKeyword":"C和Nb含量"},{"id":"6a021d94-c5cf-48ef-a53a-7b73014d0a75","keyword":"<span style=\"color:red\">相</span><span style=\"color:red\">参量</span>","originalKeyword":"相参量"},{"id":"e4b0ea8f-bdb0-4e6b-8b76-fbdcdf06c2d3","keyword":"持久寿命","originalKeyword":"持久寿命"}],"language":"zh","publisherId":"jsxb201204010","title":"C和Nb含量对TP347HFG钢在650℃析出<span style=\"color:red\">相</span><span style=\"color:red\">参量</span>和持久寿命的影响","volume":"48","year":"2012"},{"abstractinfo":"采用加热的调谐单探针技术,研究了射频辉光放电Ar等离子体空间电子能量分布函数,电子平均能量和电子密度,并系统分析了等离子体增强化学气<span style=\"color:red\">相</span>沉积工艺<span style=\"color:red\">参量</span>对等离子体空间电子特性的影响.","authors":[{"authorName":"魏俊红","id":"63be274b-007d-437d-91ce-9e6a84df1675","originalAuthorName":"魏俊红"},{"authorName":"林璇英","id":"fcbac941-5661-4ea5-85e2-b03d914a1b25","originalAuthorName":"林璇英"},{"authorName":"赵韦人","id":"5223bc85-a201-4ef7-a6c3-ca6384d5d16d","originalAuthorName":"赵韦人"},{"authorName":"池凌飞","id":"e173d84d-f7d4-4121-8e15-ef463ff57083","originalAuthorName":"池凌飞"},{"authorName":"余云鹏","id":"0f3cd2b3-b718-4a5d-b72f-3a31e3b1c906","originalAuthorName":"余云鹏"},{"authorName":"林揆训","id":"c48337d0-29f7-4a93-bbf6-ee07ef98b05a","originalAuthorName":"林揆训"},{"authorName":"黄锐","id":"344ed0c6-10f4-40d7-89fa-3031698a8765","originalAuthorName":"黄锐"},{"authorName":"王照奎","id":"f63d9f48-82ad-4d14-aa6e-5b5a09ab9c7f","originalAuthorName":"王照奎"},{"authorName":"余楚迎","id":"99520e66-093b-44a9-bfaa-7995c3a0c613","originalAuthorName":"余楚迎"}],"doi":"","fpage":"755","id":"8574b65f-4ad3-4f7c-b96b-daec1c98d7a4","issue":"6","journal":{"abbrevTitle":"GNCL","coverImgSrc":"journal/img/cover/GNCL.jpg","id":"33","issnPpub":"1001-9731","publisherId":"GNCL","title":"功能材料"},"keywords":[{"id":"5e101bb3-a68b-4226-a323-288fe65d573b","keyword":"调谐单探针","originalKeyword":"调谐单探针"},{"id":"35bf6ab4-b559-4f62-992a-699068bcbe86","keyword":"等离子体化学气<span style=\"color:red\">相</span>沉积","originalKeyword":"等离子体化学气相沉积"},{"id":"20e9dc6b-2ab7-4fb5-9e1c-c3a7a9a78676","keyword":"Ar等离子体","originalKeyword":"Ar等离子体"}],"language":"zh","publisherId":"gncl200406032","title":"等离子体化学气<span style=\"color:red\">相</span>沉积<span style=\"color:red\">参量</span>对Ar等离子体电子特性的影响","volume":"35","year":"2004"},{"abstractinfo":"在反铁电晶体NH4H2PO4(ADP)顺电反铁电相变中,对称性所属点群也随之发生相应的改变.通过对实验结果的分析,我们认为NH4H2PO4(ADP)晶体反铁电相对称性所属点群为P2(C2).选用轴矢量R作为序<span style=\"color:red\">参量</span>来描述NH4H2PO4(ADP)晶体反铁电相变中对称性的变化,应用居里原理,恰能得到NH4H2PO4(ADP)晶体反铁电<span style=\"color:red\">相</span>的正确对称性所属点群P2(C2).","authors":[{"authorName":"韩代朝","id":"e725a4db-09fd-497c-96c9-03fd9d940c90","originalAuthorName":"韩代朝"},{"authorName":"马素敏","id":"8fdfde58-567c-46eb-bda9-53e4d9dcd9df","originalAuthorName":"马素敏"},{"authorName":"蔡玉平","id":"b0ef827c-7935-4020-b1e8-d695568fd9f3","originalAuthorName":"蔡玉平"}],"doi":"10.3969/j.issn.1000-985X.2004.02.030","fpage":"254","id":"0b3323f7-b6ff-4b53-a0a7-e2ba1e41e365","issue":"2","journal":{"abbrevTitle":"RGJTXB","coverImgSrc":"journal/img/cover/RGJTXB.jpg","id":"57","issnPpub":"1000-985X","publisherId":"RGJTXB","title":"人工晶体学报"},"keywords":[{"id":"76e5cf10-bc7b-4ae0-a5c4-660121c2efd2","keyword":"反铁电<span style=\"color:red\">相</span>","originalKeyword":"反铁电相"},{"id":"bff851ea-ba5e-44e3-8225-871f0d2c54f0","keyword":"相变","originalKeyword":"相变"},{"id":"020134c4-2548-488d-ac00-962d2ead8de0","keyword":"序<span style=\"color:red\">参量</span>","originalKeyword":"序参量"},{"id":"f5708439-cb15-4a99-b910-d21d1f38b871","keyword":"居里原理","originalKeyword":"居里原理"},{"id":"5289a3b1-cfb6-47db-8c6e-2d285a75fddc","keyword":"轴矢量","originalKeyword":"轴矢量"}],"language":"zh","publisherId":"rgjtxb98200402030","title":"NH4H2PO4晶体反铁电<span style=\"color:red\">相</span>的对称性及序<span style=\"color:red\">参量</span>","volume":"33","year":"2004"},{"abstractinfo":"研究了C和Nb含量对TP347HFG钢在650 ℃析出<span style=\"color:red\">相</span><span style=\"color:red\">参量</span>(成分、体积分数和尺寸)和持久寿命的影响. 对ASME成分范围内的2种不同C和Nb含量的TP347HFG钢在650 ℃, 230和 150 MPa条件下进行持久实验, 持久寿命分别为199, 420 h和2426, 8837 h, 其中C含量较低Nb含量较高的样品持久寿命较长. 对持久管样的EPMA-EDS+MPSM 和TEM-EDS分析表明, 较低的C含量和较高的Nb含量对应较少的<em>M</em><sub>23</sub>C<sub>6</sub>和较多的 <em>MX</em>, 并阻碍了<em>M</em><sub>23</sub>C<sub>6</sub>的聚集粗化, 同时基体中可保留较多的Cr, 有利于延长持久寿命. 此外, 运用热力学软件Thermo-Calc分析了在500--1300 ℃范围内C和Nb组合含量的变化对各相成分和体积分数的影响, 与实验结果相吻合.","authors":[{"authorName":"彭志方","id":"f5979642-7dcd-4633-b141-d784222c97b0","originalAuthorName":"彭志方"},{"authorName":"党莹樱","id":"b4beb071-ec80-4db4-8ef6-af6bb4781af9","originalAuthorName":"党莹樱"},{"authorName":"彭芳芳","id":"06587cff-171e-4e61-82e3-e0020b62833f","originalAuthorName":"彭芳芳"}],"categoryName":"|","doi":"10.3724/SP.J.1037.2011.00677","fpage":"450","id":"29a20808-5fea-441c-8188-d4a43023838c","issue":"4","journal":{"abbrevTitle":"JSXB","coverImgSrc":"journal/img/cover/JSXB.jpg","id":"48","issnPpub":"0412-1961","publisherId":"JSXB","title":"金属学报"},"keywords":[{"id":"7a3113e4-fac1-4f48-9fa2-27c93bb0e4d5","keyword":"TP347HFG钢","originalKeyword":"TP347HFG钢"},{"id":"288e7655-b733-4807-a26b-b4d89f6743c9","keyword":"carbon and niobium content","originalKeyword":"carbon and niobium content"},{"id":"ed59dd27-ae01-4be8-91f3-f41d1d6656c4","keyword":"phase parameter","originalKeyword":"phase parameter"},{"id":"03b32a83-5d61-4bcc-9edf-5424dddf9984","keyword":"creep rupture time","originalKeyword":"creep rupture time"}],"language":"zh","publisherId":"0412-1961_2012_4_12","title":"C和Nb含量对TP347HFG钢在650 ℃析出<span style=\"color:red\">相</span><span style=\"color:red\">参量</span>和持久寿命的影响","volume":"48","year":"2012"},{"abstractinfo":"研究了HR3C钢不同运行态过热器管样晶界碳化物M23C6<span style=\"color:red\">相</span><span style=\"color:red\">参量</span>(面积分数φM23C6和等效宽度W)的变化与脆化的关系.利用ASTM E112规范奥氏体钢晶粒度评级卡片测算出各级别晶粒度(GL)对应的二维图像晶界总周长(Lbg),并拟合出两者的关系Lgb(GL);利用各管样的扫描电镜二次电子(SEM-SE)像,得到了对应的φM23C6及W,从而建立了W与GL和φM23C6的关系(W(GL,φM25C6));再结合Charpy冲击实验,获得了冲击值(aKV)与W的关系(aKV(W));此外,利用纳米压痕仪测定了晶界的弹性模量(Er).结果表明,所有管样冲击断口均呈沿晶断裂形貌;当φM23C6一定时,GL越小,W越大,其Er也越大,对应的aKV越小,即晶界脆化倾向越大.揭示了晶界M23C6片等效宽度的增大(粗化)导致脆化的实质.","authors":[{"authorName":"彭志方","id":"887f643e-6af7-4fe4-a9ba-78bd67f8d495","originalAuthorName":"彭志方"},{"authorName":"任文","id":"df833186-0b74-40b6-9de4-85b138cfc747","originalAuthorName":"任文"},{"authorName":"杨超","id":"6fedd54c-6a97-467f-ad40-000252468fad","originalAuthorName":"杨超"},{"authorName":"陈方玉","id":"8593d190-f768-4150-ab5e-a0ec70dfc987","originalAuthorName":"陈方玉"},{"authorName":"刘鸿国","id":"e78fc017-a34d-49ae-84cf-bd2d6c0c52dd","originalAuthorName":"刘鸿国"},{"authorName":"彭芳芳","id":"c2a1ae54-ad02-4626-9ea7-deadae959839","originalAuthorName":"彭芳芳"},{"authorName":"梅青松","id":"a43a4788-96b6-4c55-ae05-46c71fa0f0f6","originalAuthorName":"梅青松"}],"doi":"10.11900/0412.1961.2015.00077","fpage":"1325","id":"a74b75a9-8b5c-47d8-8642-a1abfa06c51b","issue":"11","journal":{"abbrevTitle":"JSXB","coverImgSrc":"journal/img/cover/JSXB.jpg","id":"48","issnPpub":"0412-1961","publisherId":"JSXB","title":"金属学报"},"keywords":[{"id":"2cfb57d1-5b5f-44c9-ad8d-0cf608ccea46","keyword":"HR3C钢","originalKeyword":"HR3C钢"},{"id":"f62bb60b-da28-4a41-83ec-bd1e88d31f66","keyword":"脆化","originalKeyword":"脆化"},{"id":"5f946c3e-777e-4794-97a2-20f7e538f81c","keyword":"M23C6","originalKeyword":"M23C6"},{"id":"e5d88cc3-a3a9-46e1-8e7b-095c65dbbcad","keyword":"等效宽度","originalKeyword":"等效宽度"},{"id":"bebdf003-18e3-4845-9902-f3b34a22d039","keyword":"Charpy冲击值","originalKeyword":"Charpy冲击值"}],"language":"zh","publisherId":"jsxb201511004","title":"HR3C钢运行过热器管的脆化与晶界M23C6<span style=\"color:red\">相</span><span style=\"color:red\">参量</span>演化的关系","volume":"51","year":"2015"},{"abstractinfo":"化学气<span style=\"color:red\">相</span>渗透(CVI)制备的CFCC的质量控制非常困难.研究该材料质量的无损检测方法对材料使用及性能表征等都具有重要意义.针对声衰减严重的问题,采用穿透法测量各声学<span style=\"color:red\">参量</span>,用声速、衰减、非线性等相关<span style=\"color:red\">参量</span>评价材料的均匀性,同时用金相法进行对比测试.结果表明:声速、衰减、非线性等<span style=\"color:red\">参量</span>可准确地评价材料均匀性,其中声速评价是最成熟的表征方法.","authors":[{"authorName":"陆铭慧","id":"f1d3a862-929e-4615-87fd-24b08e5bde92","originalAuthorName":"陆铭慧"},{"authorName":"段涵呓","id":"90729bfa-895d-4f52-a722-f95db084dcf0","originalAuthorName":"段涵呓"},{"authorName":"王旭","id":"86b5494c-354c-4a48-ae1b-b6f2195727b9","originalAuthorName":"王旭"}],"doi":"10.3969/j.issn.1007-2330.2016.06.011","fpage":"54","id":"524e8c83-e293-4e82-b1c9-b5667b758c50","issue":"6","journal":{"abbrevTitle":"YHCLGY","coverImgSrc":"journal/img/cover/YHCLGY.jpg","id":"77","issnPpub":"1007-2330","publisherId":"YHCLGY","title":"宇航材料工艺   "},"keywords":[{"id":"aa7ec0fe-ed80-4e52-9c2e-d49436e68e98","keyword":"连续纤维增韧陶瓷基复合材料","originalKeyword":"连续纤维增韧陶瓷基复合材料"},{"id":"facedd54-13f7-4f88-ad86-491e6fbd4983","keyword":"穿透法","originalKeyword":"穿透法"},{"id":"35b2a444-4f25-469a-8be2-5d8afcf09651","keyword":"声学<span style=\"color:red\">参量</span>","originalKeyword":"声学参量"},{"id":"36f798af-48e8-40e2-8cc1-c6f28eb22665","keyword":"非线性","originalKeyword":"非线性"},{"id":"b86b0dd4-6e44-4b88-bf0b-2859baba2c27","keyword":"材料均匀性","originalKeyword":"材料均匀性"}],"language":"zh","publisherId":"yhclgy201606011","title":"CFCC的几种声学<span style=\"color:red\">参量</span>表征方法比较","volume":"46","year":"2016"},{"abstractinfo":"进行了分散<span style=\"color:red\">相</span>颗粒形状较规则的单相连续两<span style=\"color:red\">相</span>共混物细观结构<span style=\"color:red\">参量</span>对共混物基体屈服的产生和屈服区扩展规律影响的研究.通过模拟获得了共混体系橡胶粒子分布形式、添加比例、粒子尺寸、两相间界面层性能、粒子形状等细观结构<span style=\"color:red\">参量</span>的改变对共混物基体屈服的影响规律.","authors":[{"authorName":"宋宏图","id":"53298aa6-b00a-453c-9340-3f93991fa969","originalAuthorName":"宋宏图"},{"authorName":"荆洪阳","id":"2f18e017-aafb-4f71-b70e-7392db53a7ed","originalAuthorName":"荆洪阳"},{"authorName":"丁韦","id":"39d09173-189a-44ae-9b23-77264c40a6c1","originalAuthorName":"丁韦"},{"authorName":"高文会","id":"dbb685b6-3aa1-46e3-adeb-e85c5cad4714","originalAuthorName":"高文会"}],"doi":"","fpage":"1","id":"9290f2aa-f2f2-44b8-a26b-0e0fcb96b5ac","issue":"4","journal":{"abbrevTitle":"GFZCLKXYGC","coverImgSrc":"journal/img/cover/GFZCLKXYGC.jpg","id":"31","issnPpub":"1000-7555","publisherId":"GFZCLKXYGC","title":"高分子材料科学与工程"},"keywords":[{"id":"e44d6fdd-6ff5-4cfa-8a2d-7fab54b938a2","keyword":"细观结构<span style=\"color:red\">参量</span>","originalKeyword":"细观结构参量"},{"id":"f039748e-dadb-4f31-8477-fa9f46b1c10f","keyword":"数值模拟","originalKeyword":"数值模拟"},{"id":"e79f59aa-41e6-471a-8566-6058d980f190","keyword":"有限元法","originalKeyword":"有限元法"},{"id":"c7bb701e-9361-4c83-b75c-1e2f4fe653e5","keyword":"增韧机理","originalKeyword":"增韧机理"},{"id":"eb10fc0e-71e1-4e1a-af2d-a63ccc1802e1","keyword":"基体屈服","originalKeyword":"基体屈服"}],"language":"zh","publisherId":"gfzclkxygc200604001","title":"细观结构<span style=\"color:red\">参量</span>对共混物基体屈服影响的数值模拟","volume":"22","year":"2006"},{"abstractinfo":"在反铁电晶体锆酸铅(PbZrO3)顺电反铁电相变中,伴随有对称性的变化.前人工作中选择反极化<span style=\"color:red\">参量</span>(P)或子晶格的极化矢量(PA、PB)作为反铁电<span style=\"color:red\">相</span>的序<span style=\"color:red\">参量</span>,根据居里原理得出了反铁电晶体锆酸铅反铁电相对称性所属空间群为Pbam(D2h)或Pba2(C2v).但是通过对中子衍射实验结果分析,该晶体反铁电相对称性所属空间群不是Pbam(D2h)或Pba2(C2v),而是P2/m(C2i).本文选取轴矢量R作为反铁电<span style=\"color:red\">相</span>的序<span style=\"color:red\">参量</span>,对锆酸铅晶体应用居里原理,恰能得到正确的对称性P2/m(C2i).","authors":[{"authorName":"韩代朝","id":"1176b059-280d-423a-889e-c402e3d9d612","originalAuthorName":"韩代朝"},{"authorName":"蔡玉平","id":"1e7315af-47db-4309-9a68-a2c84868b103","originalAuthorName":"蔡玉平"},{"authorName":"何文辰","id":"4a06750d-5428-46ff-91e5-1a1b30cb9fff","originalAuthorName":"何文辰"},{"authorName":"周国香","id":"25c65ce7-6fee-4812-a9e1-73aa5af5c0e5","originalAuthorName":"周国香"}],"doi":"10.3969/j.issn.1000-985X.2003.02.017","fpage":"170","id":"17e6c656-8f63-4aac-a427-9b6e2cc8606d","issue":"2","journal":{"abbrevTitle":"RGJTXB","coverImgSrc":"journal/img/cover/RGJTXB.jpg","id":"57","issnPpub":"1000-985X","publisherId":"RGJTXB","title":"人工晶体学报"},"keywords":[{"id":"1f42216e-c62d-4235-88d7-b658ad647d12","keyword":"锆酸铅","originalKeyword":"锆酸铅"},{"id":"bb25eaec-c423-45b6-9769-4520d4ec8295","keyword":"反铁电相变","originalKeyword":"反铁电相变"},{"id":"2089c346-7a48-4e5e-8e78-2ee611977d99","keyword":"序<span style=\"color:red\">参量</span>","originalKeyword":"序参量"},{"id":"1fd90083-bb3d-48bf-9b54-4b8d293735ca","keyword":"居里原理","originalKeyword":"居里原理"},{"id":"2853b069-b518-47bd-bc8a-30ff28cf2584","keyword":"轴矢量","originalKeyword":"轴矢量"}],"language":"zh","publisherId":"rgjtxb98200302017","title":"反铁电晶体PbZrO3序<span style=\"color:red\">参量</span>和对称性的研究","volume":"32","year":"2003"},{"abstractinfo":"飞秒光<span style=\"color:red\">参量</span>放大技术是一种获得宽带飞秒脉冲的有效手段.首先介绍了飞秒光<span style=\"color:red\">参量</span>放大技术的基本原理,并通过数值模拟显示了群速度失配及位相失配对信号转换过程的影响.数值计算结果表明:群速度失配及位相失配会导致转换效率下降,群速度失配还会导致脉冲发生畸变.其次,综述了该技术在超短脉冲特别是周期量级脉冲产生方面的研究进展,并介绍了Baltuska等设计的可以产生3.9 fs脉冲的非共线光<span style=\"color:red\">参量</span>放大装置.其中,详细讨论了超连续白光注入源、泵浦光角色散以及晶体选择三方面内容.最后介绍了该技术在高能飞秒脉冲产生方面取得的最新研究进展.","authors":[{"authorName":"邱娉","id":"5a2753c1-be27-4fb6-8bad-6f550098e0bd","originalAuthorName":"邱娉"},{"authorName":"王青圃","id":"71fabf4e-41dd-4b35-a41b-612b5bb58137","originalAuthorName":"王青圃"},{"authorName":"张行愚","id":"8516eb92-c5ab-4cb5-93ef-0efb5705d146","originalAuthorName":"张行愚"},{"authorName":"李永富","id":"59bbe339-cfcb-4501-936a-83190551698f","originalAuthorName":"李永富"}],"doi":"10.3969/j.issn.1007-5461.2007.03.001","fpage":"273","id":"f3cf8239-a587-4020-9549-b8af46760d51","issue":"3","journal":{"abbrevTitle":"LZDZXB","coverImgSrc":"journal/img/cover/LZDZXB.jpg","id":"53","issnPpub":"1007-5461","publisherId":"LZDZXB","title":"量子电子学报   "},"keywords":[{"id":"0ac858c8-e0ba-4bf3-a5b2-30ecbf2887f2","keyword":"非线性光学","originalKeyword":"非线性光学"},{"id":"0dd6dac2-f9a8-4156-9f74-9e59eae7faed","keyword":"飞秒光<span style=\"color:red\">参量</span>放大","originalKeyword":"飞秒光参量放大"},{"id":"90fddd03-9811-40de-a808-d1cc0adc330c","keyword":"周期量级脉冲","originalKeyword":"周期量级脉冲"},{"id":"a9af4d3f-94bd-416f-8f9d-420210fbea5b","keyword":"超连续白光","originalKeyword":"超连续白光"},{"id":"5a27829f-fe73-4bba-a248-72f324d7559c","keyword":"泵浦光角色散","originalKeyword":"泵浦光角色散"},{"id":"827b582d-c635-45b6-9d67-9db0c948b205","keyword":"非共线光<span style=\"color:red\">参量</span>放大","originalKeyword":"非共线光参量放大"},{"id":"9532fb5b-dbdf-4a2c-bebf-651ab5255a17","keyword":"高能飞秒脉冲","originalKeyword":"高能飞秒脉冲"}],"language":"zh","publisherId":"lzdzxb200703001","title":"飞秒光<span style=\"color:red\">参量</span>放大技术原理及应用","volume":"24","year":"2007"},{"abstractinfo":"为解决非匀质液体<span style=\"color:red\">参量</span>的检测难题,提出了全微分检测准则,并结合软测量技术,构造出一套全新的非匀质液体<span style=\"color:red\">参量</span>检测技术.作为该技术的实际应用,介绍了一个在石油生产系统中的成功案例,印证了微分测量原理在多层不同质和非匀质液体中进行检测的有效性,证明了这是一项有重要推广价值的新的检测技术.","authors":[{"authorName":"吴海鹰","id":"eec34889-b0a0-45a7-b42e-0f2d00664bce","originalAuthorName":"吴海鹰"}],"doi":"10.3969/j.issn.1001-0777.2004.02.007","fpage":"18","id":"16ee990d-d515-428c-95ff-8286f03ce1d9","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":"39d49c8c-0562-4737-acb6-205ff417c9e2","keyword":"微分检测原理","originalKeyword":"微分检测原理"},{"id":"ae447720-8e05-4a4d-846c-c59a1dde3f62","keyword":"软测量技术","originalKeyword":"软测量技术"},{"id":"9ce91f2f-32af-4756-8728-3554b1d8daee","keyword":"非匀质液体检测","originalKeyword":"非匀质液体检测"},{"id":"de8318c5-4235-438a-8855-05e8ee5dc36a","keyword":"多层液体检测","originalKeyword":"多层液体检测"},{"id":"56645232-18b3-4506-a76f-a2ff67cd9ff9","keyword":"原油分离检测","originalKeyword":"原油分离检测"}],"language":"zh","publisherId":"wlcs200402007","title":"非匀质液体<span style=\"color:red\">参量</span>检测原理及应用","volume":"","year":"2004"}],"totalpage":4018,"totalrecord":40178}