{"currentpage":1,"firstResult":0,"maxresult":10,"pagecode":5,"pageindex":{"endPagecode":5,"startPagecode":1},"records":[{"abstractinfo":"采用K2ZrF4、KBF4混合粉末与铝熔体原位合成方法制备了Al-4.99Zr-1.1B合金,利用X射线衍射仪、光学显微镜和扫描电镜,研究了Al-4.99Zr-1.1B合金的显微组织及其对AZ31镁合金的晶粒细化作用.结果表明:Al-4.99Zr-1.1B合金中含有大量细小的ZrB2粒子.随着Al-4.99Zr-1.1B合金添加量的增加,AZ31镁合金的a-Mg晶粒逐渐细化,晶间β-Mg17Al12相从网状转变成细小块状.添加0.6％的Al-4.99Zr-1.1B合金,可使AZ31镁合金的a-Mg晶粒从170 μm细化到45 μm.ZrB2粒子作为a-Mg晶粒的异质形核核心使a-Mg晶粒得到细化.","authors":[{"authorName":"王顺成","id":"11ce79c6-efe5-429f-bdce-d4cf14d43753","originalAuthorName":"王顺成"},{"authorName":"甘春雷","id":"e642a5e4-cc7e-401f-8016-e3f176ea71b2","originalAuthorName":"甘春雷"},{"authorName":"黎小辉","id":"da270d6d-ade0-44a4-bb60-fbdfef96fed9","originalAuthorName":"黎小辉"},{"authorName":"郑开宏","id":"87334900-c9dc-4474-9036-3bd531e66d58","originalAuthorName":"郑开宏"},{"authorName":"戚文军","id":"5cd65715-04e2-448f-9ead-183091c7be96","originalAuthorName":"戚文军"}],"doi":"","fpage":"2567","id":"3dc2ac02-ccf6-41f5-8d7c-43ae2167dd9b","issue":"11","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":"c0e4c89e-35b7-4643-9675-b191fcc92b11","keyword":"Al-Zr-B合金","originalKeyword":"Al-Zr-B合金"},{"id":"87a89415-6834-4583-a138-7c9dc139037e","keyword":"AZ31镁合金","originalKeyword":"AZ31镁合金"},{"id":"927a7ac9-c2ae-4a64-b548-4e3b4c8fe968","keyword":"晶粒细化","originalKeyword":"晶粒细化"},{"id":"35f2e9cb-9734-4038-a32b-1e2b4c89304f","keyword":"异质形核","originalKeyword":"异质形核"}],"language":"zh","publisherId":"xyjsclygc201411002","title":"Al-4.99Zr-1.1B合金的显微组织及其对AZ31镁合金的晶粒细化作用","volume":"43","year":"2014"},{"abstractinfo":"通过X射线衍射分析、金相分析和力学性能测试对大尺寸ZK60镁合金挤压型材的微观组织、织构取向和室温力学性能进行系统研究.结果显示,挤压态ZK60镁合金中主要由a-Mg和MgZn2相组成,此外还有少量的Mg2Zn11和Zn2Zr3相.挤压变形后初始的粗大铸态组织沿着挤压方向被极大地细化和破碎,同时伴有部分动态再结晶发生.大部分晶粒的基面沿着挤压方向和横向排列而不是常规的挤压纤维状取向分布.沿着45°方向取样展现出最好的断裂伸长率,其中间和边部分别为28％和23％,而最大抗力强度则体现在沿着挤压方向拉伸样品在中间和边部分别为325和312MPa.","authors":[{"authorName":"黎小辉","id":"4a5f5f48-9913-45c1-aa63-2fbfa3a2aabf","originalAuthorName":"黎小辉"},{"authorName":"冯晓伟","id":"ddbbdee3-9d06-4c6f-9316-30800f824504","originalAuthorName":"冯晓伟"},{"authorName":"王顺成","id":"143c95f5-41fe-4f18-b215-beec4763a6a7","originalAuthorName":"王顺成"},{"authorName":"戚文军","id":"926f47b0-710e-4a8a-88c6-ba42a713b127","originalAuthorName":"戚文军"}],"doi":"","fpage":"2927","id":"5ee589aa-e497-42ea-9d17-aaf426c76216","issue":"12","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":"258e2d92-9abd-4cdf-82c4-07eac1924c80","keyword":"ZK60镁合金","originalKeyword":"ZK60镁合金"},{"id":"75446f3a-b7dd-47a8-9e18-48fc0ca94a24","keyword":"挤压型材","originalKeyword":"挤压型材"},{"id":"b3628ac3-fc3f-4978-b15f-b0b3c54bf38d","keyword":"微观组织","originalKeyword":"微观组织"},{"id":"0ed9be4b-ef43-4001-bb57-e21050d6c36a","keyword":"力学性能","originalKeyword":"力学性能"},{"id":"da46ee76-b8f5-4470-87c7-ed3465804f64","keyword":"织构演变","originalKeyword":"织构演变"}],"language":"zh","publisherId":"xyjsclygc201412011","title":"大尺寸镁-锌-锆合金挤压型材组织、织构和力学性能的研究","volume":"43","year":"2014"},{"abstractinfo":"利用光学显微镜和扫描电子显微镜分析了热轧态及退火态Mg-3Zn-2Gd合金的组织,并测试了其室温拉伸力学性能.结果表明:合金板材经应变为23％--67％的轧制后组织得到细化,平均晶粒尺寸由10μm减至轧制应变为67％时的4μm.初始组织中的大量孪晶和剪切带逐渐减少;随着轧制应变增至67％,剪切带消失,组织由动态再结晶晶粒和少量孪晶组成.拉伸力学性能显著提高,抗拉强度σ0和屈服强度σ0.2分别由未轧制时的255 MPa和215MPa提高至轧制应变为67％时的305MPa和300 MPa,而伸长率δ先提高后降低.再经573K退火处理1h后,合金组织发生静态再结晶,变形不均匀区域消失,由细小均匀等轴晶组成;σ0和σ0.2分别降至265MPa和235 MPa,δ提高至19.0％;拉伸断口呈现大量韧窝,表现为韧性断裂.","authors":[{"authorName":"戚文军","id":"7d8c05a6-dc72-4226-a673-957ccd849147","originalAuthorName":"戚文军"},{"authorName":"冯晓伟","id":"2dae8288-661c-4708-97ed-eca0e7763ee2","originalAuthorName":"冯晓伟"},{"authorName":"刘汪涵博","id":"218f1873-c1c3-4d76-9867-a5be202da192","originalAuthorName":"刘汪涵博"},{"authorName":"黎小辉","id":"4e9eddfa-175a-439f-947f-77b31d815cba","originalAuthorName":"黎小辉"}],"doi":"10.11901/1005.3093.2015.731","fpage":"531","id":"051bbd7f-2a2f-4252-973c-b9905ad36cbd","issue":"7","journal":{"abbrevTitle":"CLYJXB","coverImgSrc":"journal/img/cover/CLYJXB.jpg","id":"16","issnPpub":"1005-3093","publisherId":"CLYJXB","title":"材料研究学报"},"keywords":[{"id":"4065996b-7f9a-4dbf-938f-16d61ab87101","keyword":"金属材料","originalKeyword":"金属材料"},{"id":"9d66967c-be3a-4a5b-865d-80f716311aec","keyword":"镁合金板","originalKeyword":"镁合金板"},{"id":"4a0ec818-5896-4f31-93bb-27b68e1a2ee1","keyword":"轧制组织","originalKeyword":"轧制组织"},{"id":"4bc58150-bdb4-47df-b5aa-beb01d97c15b","keyword":"退火组织","originalKeyword":"退火组织"},{"id":"1d7fa68c-9348-46eb-9fe9-8fd9d0d25026","keyword":"力学性能","originalKeyword":"力学性能"},{"id":"f9215141-fdda-4a4a-bc29-f72f7d3d0ed4","keyword":"轧制应变","originalKeyword":"轧制应变"}],"language":"zh","publisherId":"clyjxb201607008","title":"Mg-3Zn-2Gd合金轧制态和退火态的组织与力学性能","volume":"30","year":"2016"},{"abstractinfo":"在温度为360~450℃、应变率为0.001~1 s-1的变形条件下,采用 Gleeble-1500D热模拟机对固相回收 SiCp/ZK60镁基复合材料的高温压缩变形行为进行研究。结果表明：固相回收 SiCp/ZK60的流变应力随变形温度的升高而降低,随应变率的升高而升高,且随应变的增加,流动应力很快达到峰值,然后逐渐趋于稳定。固相回收SiCp/ZK60热压缩变形应力指数为3.348,变形激活能为64.97 kJ/mol,其高温压缩流变应力模型为?ε=4.69×104[sinh(0.051σ)]3.348 exp(-64790/(RT))；本试验条件下,固相回收 SiCp/ZK60的流变应力模型可以用 Zener-Hol-lomon参数的双曲线函数形式进行描述。","authors":[{"authorName":"孙明体","id":"086542ca-215b-4041-b138-de9bef9d353c","originalAuthorName":"孙明体"},{"authorName":"戚文军","id":"95a4bb07-586a-47b8-9d35-630a4298d8f0","originalAuthorName":"戚文军"},{"authorName":"王娟","id":"c17de761-f8bc-473f-bf13-fb268ab98d21","originalAuthorName":"王娟"},{"authorName":"黎小辉","id":"97b10b5f-ebce-4580-9d99-5c1386592705","originalAuthorName":"黎小辉"},{"authorName":"李亚江","id":"bbb9f230-e0be-4a71-8233-57314beb37b7","originalAuthorName":"李亚江"},{"authorName":"彭洁","id":"b01d3f86-c6c2-4754-99d8-bdf0a63f831e","originalAuthorName":"彭洁"}],"doi":"10.11896/j.issn.1005-023X.2016.22.033","fpage":"158","id":"3e0abb29-c359-425b-ad24-c039f4278385","issue":"22","journal":{"abbrevTitle":"CLDB","coverImgSrc":"journal/img/cover/CLDB.jpg","id":"8","issnPpub":"1005-023X","publisherId":"CLDB","title":"材料导报"},"keywords":[{"id":"fbc84b27-b513-461e-8728-955619cfbe28","keyword":"固相回收SiCp/ZK60","originalKeyword":"固相回收SiCp/ZK60"},{"id":"91c509b2-5672-4852-8c09-f2045b354f55","keyword":"镁基复合材料","originalKeyword":"镁基复合材料"},{"id":"e695cd00-d8d6-4725-a456-9992df53ec40","keyword":"热压缩模拟","originalKeyword":"热压缩模拟"},{"id":"c1292ae7-8514-4a5d-b831-2dd3d9835715","keyword":"流变应力","originalKeyword":"流变应力"},{"id":"54abdbc7-7b08-4cb1-b3c9-fc4d0415f002","keyword":"本构模型","originalKeyword":"本构模型"}],"language":"zh","publisherId":"cldb201622033","title":"固相回收SiCp/ZK60镁基复合材料的高温压缩变形行为?","volume":"30","year":"2016"},{"abstractinfo":"利用等离子体发射光谱仪(ICP)、光学显微镜(OM)、扫描电子显微镜(SEM)等分析手段研究了Mg-xZn-yGd(x=1～3,y=1 ～3)合金铸造态、挤压态的化学成分和微观组织演变,并测试其室温拉伸力学性能.研究结果表明:随着Gd含量的增加,铸态组织显著细化,枝状晶间距减小,其组分相Mg-Zn-Gd三元相面积分数逐渐增多,MgZn2相逐渐减少直至消失,第二相从晶界处呈连续网状分布转变成晶界断续和晶内均匀分布.挤压态组织得到细化,挤压过程发生了明显的动态再结晶,平均晶粒尺寸从Mg-3Zn合金的30μm降到Mg-2Zn-1Gd合金的10μm.第二相沿挤压方向趋于带状分布,部分弥散分布于晶内,成棒状或块状的MgZnGd三元相,尺寸约为1～3 μm.挤压态Mg-xZn-yGd合金的抗拉强度σb从Mg-3Zn的260 MPa提高到300 MPa,延伸率δ从13％提高到25％,屈服强度变化不大,σb和δ提高幅度分别为15.4％,92％.挤压态的显微硬度由Mg-3Zn的HV 52.1提高到Mg-3Zn-2Gd的HV 70.4,挤压态Mg-xZn-yGd合金室温拉伸断口呈现典型的韧性断裂特征,应力在第二相粒子处集中.","authors":[{"authorName":"冯晓伟","id":"3a5bb3ad-14cd-4fd5-9909-60d1c7038ed4","originalAuthorName":"冯晓伟"},{"authorName":"戚文军","id":"98579f6c-87be-4fe4-9b2c-1c55cb5938eb","originalAuthorName":"戚文军"},{"authorName":"黎小辉","id":"eb1641e4-c3aa-4074-b309-699af55a1271","originalAuthorName":"黎小辉"},{"authorName":"李志成","id":"70184f34-dd4e-4a6d-b767-290f361e2aca","originalAuthorName":"李志成"}],"doi":"10.13373/j.cnki.cjrm.2016.01.003","fpage":"14","id":"d3d05185-833a-4ee1-adef-6ef917d2e185","issue":"1","journal":{"abbrevTitle":"XYJS","coverImgSrc":"journal/img/cover/XYJS.jpg","id":"67","issnPpub":"0258-7076","publisherId":"XYJS","title":"稀有金属"},"keywords":[{"id":"7b56446a-38e8-4808-81c3-d7bcd4630f95","keyword":"Mg-Zn-Gd合金","originalKeyword":"Mg-Zn-Gd合金"},{"id":"3a1e540e-f4f6-46a1-9556-9665482dbb33","keyword":"微观组织","originalKeyword":"微观组织"},{"id":"0899abfa-fefb-4a95-bcf1-7da1a9315bc9","keyword":"力学性能","originalKeyword":"力学性能"},{"id":"49081bb8-9efd-4ceb-a3ee-076daa6a64bb","keyword":"动态再结晶","originalKeyword":"动态再结晶"}],"language":"zh","publisherId":"xyjs201601003","title":"Mg-Zn-Gd合金的微观组织和力学性能","volume":"40","year":"2016"},{"abstractinfo":"本文以黎开管内的热声耦合振荡为研究对象,设计基于主动补偿的适应性控制器抑制黎开管内的不稳定燃烧。试验以扬声器为执行机构来改变黎开管的边界条件,从而抑制黎开管内的热声耦合振荡。实时控制效果表明,本文所采用的适应性控制算法能够有效抑制因热声耦合产生的燃烧振荡,为实际动力系统燃烧振荡抑制提供了思路。","authors":[{"authorName":"魏伟","id":"30275880-564d-46ca-b84e-2e832b009766","originalAuthorName":"魏伟"},{"authorName":"唐豪杰","id":"f5817772-6751-4fb4-a8bc-6dece3752e0c","originalAuthorName":"唐豪杰"},{"authorName":"李东海","id":"9dea81e8-0306-420d-9130-2759b32f70ff","originalAuthorName":"李东海"},{"authorName":"王京","id":"cbaa17fa-dc5f-40c7-addc-f69d154e19a8","originalAuthorName":"王京"},{"authorName":"朱民","id":"95053dd8-7f33-42c5-aa4a-8f02488928b2","originalAuthorName":"朱民"}],"doi":"","fpage":"1777","id":"2a416127-cbe8-4ea4-ad03-3b81e84e909c","issue":"10","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":"fea079f8-6baf-4cc5-b96e-f3386f3fabe3","keyword":"黎开管","originalKeyword":"黎开管"},{"id":"6c723387-7cfa-49b8-995a-061600f12ffc","keyword":"热声耦合振荡","originalKeyword":"热声耦合振荡"},{"id":"0b638eba-2cff-488b-9207-99660259d1e9","keyword":"主动控制","originalKeyword":"主动控制"},{"id":"51d1220e-05be-4ae0-96de-fd748461820d","keyword":"适应性控制","originalKeyword":"适应性控制"}],"language":"zh","publisherId":"gcrwlxb201110039","title":"黎开管热声振荡的主动控制研究","volume":"32","year":"2011"},{"abstractinfo":"黎开管中燃烧振荡现象的实验研究发现,在不稳定发生的极限工况附近可能存在幅值周期性变化的振荡现象,也即拍振,其拍频可低于1 Hz.本文比较了铁丝网和穿孔陶瓷两种稳焰体对拍振发生的影响;通过时频分析揭示了拍振的声压脉动的主频随时间周期性变化的特征.采用基于数字信号处理器的控制系统,研究了对极限环和拍振的主动控制效果,实验结果表明,黎开管系统中导致拍振的非线性可能使得采用常规主动控制方法难以取得满意的控制效果.","authors":[{"authorName":"翁方龙","id":"be6464f7-51a0-40b3-96e9-6e77c2cad1e2","originalAuthorName":"翁方龙"},{"authorName":"朱民","id":"54d35c17-4ad1-400c-a7ac-a5748664045f","originalAuthorName":"朱民"},{"authorName":"李东海","id":"5573a733-f9de-4779-b822-044122eed616","originalAuthorName":"李东海"}],"doi":"","fpage":"2313","id":"d96b5c84-620a-43fa-8d11-977f27faa124","issue":"11","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":"c6a74fe2-8059-4c3d-969e-d9f412bac915","keyword":"热声振荡","originalKeyword":"热声振荡"},{"id":"3510ebfa-0a5c-4e0c-8c29-9b140cac7749","keyword":"拍振","originalKeyword":"拍振"},{"id":"bf38a71c-d01c-403e-a689-73105e366abe","keyword":"时频分析","originalKeyword":"时频分析"},{"id":"59b164ee-3f17-43a5-b049-ce6a0ca84aff","keyword":"主动控制","originalKeyword":"主动控制"}],"language":"zh","publisherId":"gcrwlxb201411044","title":"黎开管中热声拍振现象及其主动控制","volume":"35","year":"2014"},{"abstractinfo":"李绍宏,邓黎辉,谢殷子,吴晓春","authors":[{"authorName":"高碳高合金马氏体钢回火过程连续性转变的内耗行为研究","id":"a56d0ae1-54be-47af-858b-f74c82608c9c","originalAuthorName":"高碳高合金马氏体钢回火过程连续性转变的内耗行为研究"}],"categoryName":"|","doi":"","fpage":"37","id":"7cbdd3ec-863c-45d4-97c4-bdc3ee0336c9","issue":"4","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":"59175031-3448-441b-b9cc-5e1c4d34ea4d","keyword":"高碳高合金马氏体钢淬火后在回火过程中存在过饱和碳原子偏聚现象，碳原子偏聚于位错附近的间隙位置，回火过程中以碳化物形式沉淀析出。通过内耗研究表明，随着回火温度的增加，Snoek峰驰豫强度下降并消失，SKK峰驰豫强度降低并随回火温度的升高而宽化。由该结果可知由于大量碳原子偏聚于位错处，随后以细颗粒碳化物形式在位错处析出。随着回火温度增加，大部分位错回复消失及碳化物聚集长大，同时残余奥氏体分解产生硬化效应，使钢的硬度增加而韧性下降。","originalKeyword":"高碳高合金马氏体钢淬火后在回火过程中存在过饱和碳原子偏聚现象，碳原子偏聚于位错附近的间隙位置，回火过程中以碳化物形式沉淀析出。通过内耗研究表明，随着回火温度的增加，Snoek峰驰豫强度下降并消失，SKK峰驰豫强度降低并随回火温度的升高而宽化。由该结果可知由于大量碳原子偏聚于位错处，随后以细颗粒碳化物形式在位错处析出。随着回火温度增加，大部分位错回复消失及碳化物聚集长大，同时残余奥氏体分解产生硬化效应，使钢的硬度增加而韧性下降。"}],"language":"zh","publisherId":"1001-0963_2011_4_8","title":"高性能精品模具钢系列产品的研究与开发(20079~201012)","volume":"23","year":"2011"},{"abstractinfo":"本文探讨了黎开管系统中燃烧振荡的两类非线性现象—拍振和迟滞,通过改变燃料流量和当量比研究了这两类非线性现象的发生规律.实验发现拍振现象仅在热功率较小、当量比较低的条件下发生;迟滞现象在发生燃烧振荡的当量比上限附近较显著,而当量比下限附近不明显.对于燃烧振荡中的拍振现象,通过热声耦合分析,结合弥散模型和声波传播关系,反演得到了火焰传递函数(FTF),结果可为进一步分析与控制这类非线性振荡现象提供参考.","authors":[{"authorName":"翁方龙","id":"38ab6049-3a88-431a-b709-e044896c46fc","originalAuthorName":"翁方龙"},{"authorName":"朱民","id":"7a6a8dc0-608e-4ee4-a9ff-c837e2d0d00b","originalAuthorName":"朱民"},{"authorName":"李东海","id":"13a6651f-8409-4448-a7fd-034f38c186cb","originalAuthorName":"李东海"}],"doi":"","fpage":"1582","id":"494ba969-5184-4341-89b2-b1707c1bb78b","issue":"8","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":"1efebbe7-dace-4eb3-877f-3af070472580","keyword":"燃烧振荡","originalKeyword":"燃烧振荡"},{"id":"86d758c2-d9af-420a-a09a-d2bafb3dba81","keyword":"拍振","originalKeyword":"拍振"},{"id":"e6462edd-2719-4c95-bd25-fb685d55e540","keyword":"迟滞","originalKeyword":"迟滞"},{"id":"33dd2b40-6434-4f43-a850-c21fb9431f4c","keyword":"火焰传递函数","originalKeyword":"火焰传递函数"}],"language":"zh","publisherId":"gcrwlxb201308044","title":"黎开管中燃烧振荡的非线性现象研究","volume":"34","year":"2013"},{"abstractinfo":"研究了黎巴嫩的黎波里钢板桩码头的牺牲阳极保护系统,解决了该海域码头不同区域中钢管桩与钢板桩的平均保护电流密度取值问题.通过现场试验发现,对于码头迎水面的平均保护电流密度值取0.060 A·m-2较为合适,码头回填区域的平均保护电流密度值取0.030 A· m-2较为合适,海泥区的平均保护电流密度值取0.025 A·m-2较为合适.","authors":[{"authorName":"王亚平","id":"4ff18434-0533-4707-ba4c-19334280cc52","originalAuthorName":"王亚平"},{"authorName":"韩正权","id":"d4dac8b4-cf71-458a-a4fb-ea1c65eeb2f9","originalAuthorName":"韩正权"},{"authorName":"方达经","id":"66540834-2f2c-4db9-84c3-186db1f0de68","originalAuthorName":"方达经"},{"authorName":"黄俊","id":"935588de-3d8f-4685-8ef6-82a26bdacf3c","originalAuthorName":"黄俊"},{"authorName":"沈尔卜","id":"02f37159-ecf0-4a4c-bc43-219ddf9360d9","originalAuthorName":"沈尔卜"}],"doi":"","fpage":"155","id":"ced4ea50-b3c4-4910-9848-57616f1c417b","issue":"2","journal":{"abbrevTitle":"FSYFH","coverImgSrc":"journal/img/cover/FSYFH.jpg","id":"25","issnPpub":"1005-748X","publisherId":"FSYFH","title":"腐蚀与防护"},"keywords":[{"id":"4b46cf64-6e7a-4a60-b067-a3f2a3739062","keyword":"钢管桩","originalKeyword":"钢管桩"},{"id":"8d31a042-b1c7-46f3-8e4b-37956db1662d","keyword":"钢板桩","originalKeyword":"钢板桩"},{"id":"65897383-a99e-403e-829a-cd0eccb23a72","keyword":"码头","originalKeyword":"码头"},{"id":"86d18734-b962-4a66-9866-2e32395227a7","keyword":"牺牲阳极","originalKeyword":"牺牲阳极"},{"id":"1387acfb-7134-4980-96ef-9b77e2398dbd","keyword":"阴极保护","originalKeyword":"阴极保护"},{"id":"7f572a41-2afd-4e50-a95e-feae76c1adc2","keyword":"电流密度","originalKeyword":"电流密度"}],"language":"zh","publisherId":"fsyfh201302014","title":"黎巴嫩的黎波里钢板桩码头牺牲阳极保护","volume":"34","year":"2013"}],"totalpage":590,"totalrecord":5891}