{"currentpage":1,"firstResult":0,"maxresult":10,"pagecode":5,"pageindex":{"endPagecode":5,"startPagecode":1},"records":[{"abstractinfo":"基于微观相场模型,研究Ni75Cr16.4Al8.6的粗化后期演化过程.结果表明:L12相和DO22相的标度函数曲线图表明合金沉淀在粗化阶段均表现出标度行为,不加应变能时DO22相结构函数因子和标度函数峰值均大于L12相;加入应变能后,两相的结构函数因子和标度函数的峰值均变小,反映了应变能对两相沉淀粗化过程的阻碍影响;相对于L12相,DO22相减小幅度更大,L12相结构函数因子和标度函数峰值大于DO22相,应变能对DO22相的阻碍作用更大.","authors":[{"authorName":"<span style=\"color:red\">钟</span><span style=\"color:red\">汉文</span>","id":"06363be8-27ed-4010-8f14-cc461e859adb","originalAuthorName":"钟汉文"},{"authorName":"陈铮","id":"b4e3d573-77ac-4e02-8dd3-864e308624e8","originalAuthorName":"陈铮"},{"authorName":"卢艳丽","id":"1cfa6056-bbb9-47a6-be40-7c849e04949f","originalAuthorName":"卢艳丽"},{"authorName":"徐聪","id":"3148afdb-c949-43d6-918d-18d05ec78637","originalAuthorName":"徐聪"},{"authorName":"马瑞","id":"e3e3c76a-b4c9-4a53-b7e4-957b3ca73cae","originalAuthorName":"马瑞"},{"authorName":"孙立岩","id":"fa3991c5-4c03-4b98-8a7b-75552579c640","originalAuthorName":"孙立岩"}],"doi":"","fpage":"1185","id":"2f3882a4-ea4e-4643-adc2-94fc0abd6523","issue":"7","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":"1dcd5b03-b902-498b-9e1d-997a2ea67430","keyword":"Ni75Cr16.4Al8.6合金","originalKeyword":"Ni75Cr16.4Al8.6合金"},{"id":"68e90ef5-ff64-46ee-8e68-2d22cc172267","keyword":"标度函数","originalKeyword":"标度函数"},{"id":"dea15712-ade0-471d-a379-99ee3c679d78","keyword":"结构函数","originalKeyword":"结构函数"},{"id":"e7e7faea-cb62-4d37-9d21-c32e40cf98e0","keyword":"微观相场","originalKeyword":"微观相场"}],"language":"zh","publisherId":"xyjsclygc201007012","title":"Ni75Cr16.4Al8.6合金粗化过程标度行为的微观相场研究","volume":"39","year":"2010"},{"abstractinfo":"基于离散格点形式的微扩散方程(Langevin方程),模拟了Al3Li相反位缺陷随时间的演化特征及随组元浓度、温度的变化规律.结果表明,Al3Li相中主要以Al原子占据Li位形成的反位缺陷AlLi为主,同时存在少量的Li原子占据Al位形成的反位缺陷LiAl,2种反位缺陷浓度均随温度的升高而上升,且AlLi远大于LiAl上升速率;随Li浓度的增加,AlLi浓度缓慢降低,LiAl浓度略有上升,但仍远远小于AlLi浓度;浓度变化对反位缺陷的影响远不及温度对其影响大.","authors":[{"authorName":"孙立岩","id":"ffb2666c-9563-4026-bc48-1f29cd4f6186","originalAuthorName":"孙立岩"},{"authorName":"陈铮","id":"4b975ea5-370f-470b-8a8a-096312788b63","originalAuthorName":"陈铮"},{"authorName":"王永欣","id":"4311c4d8-0485-442b-af38-e9844fac3fb9","originalAuthorName":"王永欣"},{"authorName":"张静","id":"c53c2b3a-c35b-48ed-ac14-a24c9122f90c","originalAuthorName":"张静"},{"authorName":"苗海川","id":"d7d081a9-8a39-4873-9f3d-59f51c1ea740","originalAuthorName":"苗海川"},{"authorName":"<span style=\"color:red\">钟</span><span style=\"color:red\">汉文</span>","id":"29b7a0b4-4944-40fb-bc05-58f090598801","originalAuthorName":"钟汉文"}],"doi":"","fpage":"86","id":"3dfa4a29-0d8d-4b89-a2e9-1f9c9adc80c9","issue":"1","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":"11ace8de-2aa5-4bdb-ace5-defc86f10d2c","keyword":"反位缺陷","originalKeyword":"反位缺陷"},{"id":"cbbbfd1d-e197-46bc-b950-a415bc0eb8be","keyword":"Al3Li相","originalKeyword":"Al3Li相"},{"id":"590ce456-46c4-4b98-ba06-fa626f985d45","keyword":"微观相场","originalKeyword":"微观相场"}],"language":"zh","publisherId":"xyjsclygc200901020","title":"Al3Li相反位缺陷演化的微观相场模拟","volume":"38","year":"2009"},{"abstractinfo":"基于微观相场动力学模型和微观弹性理论,研究了Ni-Al合金中沉淀相Ni_3Al(γ')形貌演化、体积分数以及铝浓度对其相互关系的影响.结果表明,对于所有浓度的合金,沉淀后期,γ'相均沿着[001]和[010]方向规则排列,但是彼此之间存在着不同的相互关系.对于低铝浓度合金,γ'相之间彼此互相独立.对于中铝浓度的合金,γ'相之间主要存在着4种相互关系:L-状,双透镜状,三重组结构和四重组结构.对于高铝浓度的合金,γ'相之间主要呈现双透镜状关系.","authors":[{"authorName":"卢艳丽","id":"4b349deb-e5de-4ae0-90e5-470e16cfbd4f","originalAuthorName":"卢艳丽"},{"authorName":"陈铮","id":"7e23dcbc-5e5f-4a8e-95ac-5e3ba944fbdf","originalAuthorName":"陈铮"},{"authorName":"<span style=\"color:red\">钟</span><span style=\"color:red\">汉文</span>","id":"ddcf6f0a-9180-427b-a7a4-944e28b14917","originalAuthorName":"钟汉文"},{"authorName":"张静","id":"d5385758-63f5-4e70-ac97-7b620d24e961","originalAuthorName":"张静"}],"doi":"","fpage":"1890","id":"7c432a45-184f-4f23-9824-6b8d2ee2261a","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":"4a0a7f5d-7096-4637-bc58-17c6414f411b","keyword":"微观相场","originalKeyword":"微观相场"},{"id":"34b7d613-f5b0-4edc-80fb-f3d939b91570","keyword":"弹性应变","originalKeyword":"弹性应变"},{"id":"056fa086-d23f-4a9b-9e90-1d382344086d","keyword":"形貌演化","originalKeyword":"形貌演化"},{"id":"6a007ea1-2512-4f9b-9235-af3550198ffa","keyword":"沉淀过程","originalKeyword":"沉淀过程"},{"id":"1069afcd-3a36-486f-a482-cd697efc1c95","keyword":"Ni-Al合金","originalKeyword":"Ni-Al合金"}],"language":"zh","publisherId":"xyjsclygc200911003","title":"Ni-Al合金中沉淀相Ni_3Al相互关系的微观相场模拟","volume":"38","year":"2009"},{"abstractinfo":"基于微观相场理论,根据Khachaturyan的占位几率和能量关系方程,推导出L12结构的第一近邻原子间相互作用势与长程序参数关系的反演方程-4W1·η/kBT=1n(1-η)[1-c(1+3·η)]/(1+3·η)[1-c(1-η)],根据该方程,只需输入根据相图中L12结构相变点的温度和原子浓度,就可以计算出不同温度和原子浓度下的L12结构的第1近邻原子间相互作用势,计算结果与第1性原理及其他方法计算的值接近;同时在计算过程中发现了L12结构的第1近邻原子间相互作用势在析出L12相的相图范围内随温度和原子浓度变化.","authors":[{"authorName":"徐聪","id":"a5a45bfd-cdd4-4a7c-b02f-37dcae310d21","originalAuthorName":"徐聪"},{"authorName":"陈铮","id":"5c19cf99-cc4d-480c-a5c1-3bac45a2f57c","originalAuthorName":"陈铮"},{"authorName":"卢艳丽","id":"c0b77f49-d1db-4c3c-9165-46c5a7bc7986","originalAuthorName":"卢艳丽"},{"authorName":"<span style=\"color:red\">钟</span><span style=\"color:red\">汉文</span>","id":"86f08557-a093-47d3-8649-027513f06069","originalAuthorName":"钟汉文"},{"authorName":"张静","id":"bb54352f-8c41-4215-a69d-ba3f210cd704","originalAuthorName":"张静"},{"authorName":"苗海川","id":"feecabce-2535-425d-a090-9e491d792a1f","originalAuthorName":"苗海川"}],"doi":"","fpage":"1027","id":"b75bdd0e-05f3-41cc-a34a-6c30c0c2d6e0","issue":"6","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":"19562f69-cf60-4272-af85-8bc50f0472cf","keyword":"原子间相互作用势","originalKeyword":"原子间相互作用势"},{"id":"0df5baf8-4617-4e46-a079-ca4d9fbb8dd6","keyword":"反演","originalKeyword":"反演"},{"id":"4fa627e5-8ed1-4938-a20b-e41d933924b9","keyword":"微观相场","originalKeyword":"微观相场"},{"id":"404962fe-eab2-41f8-ae66-0ba75d2fb309","keyword":"L12结构","originalKeyword":"L12结构"}],"language":"zh","publisherId":"xyjsclygc201006020","title":"微观相场法反演L12结构的原子间相互作用势","volume":"39","year":"2010"},{"abstractinfo":"基于含应变能的微观相场动力学模型,利用结构函数归一化因子和标度函数,对Ni75Cr19Al6合金沉淀后期DO220相的粗化行为进行研究.结果表明:DO22相的结构函数归一化因子和标度函数在沉淀后期阶段均表现出标度行为,加入应变能后,DO22有序畴尺寸在非弹性\"软\"方向上的长大受到阻碍,DO22有序畴的体积分数也减小,结构函数的归一化结构因子和标度函数曲线峰值均小于未加应变能的值.","authors":[{"authorName":"<span style=\"color:red\">钟</span><span style=\"color:red\">汉文</span>","id":"80975bca-a5c5-4e08-9b69-b44d79d0c775","originalAuthorName":"钟汉文"},{"authorName":"卢艳丽","id":"c87573ed-0c8d-473b-9f9f-b4a9487f1b68","originalAuthorName":"卢艳丽"},{"authorName":"陈铮","id":"9f9eb333-aed6-4bc2-a82c-b2dc32907e64","originalAuthorName":"陈铮"},{"authorName":"徐聪","id":"a7c5f854-8b40-420f-93a4-480b6fdd5889","originalAuthorName":"徐聪"},{"authorName":"马锐","id":"bf5c29d1-dac7-474c-81c1-d56a27158720","originalAuthorName":"马锐"},{"authorName":"孙立岩","id":"ad8a4ac1-828e-4879-8a5f-6add80ecc453","originalAuthorName":"孙立岩"}],"doi":"","fpage":"180","id":"c14fb341-2f5a-4b2a-8ae4-e8c122cdcf01","issue":"4","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":"c35a0638-d3ba-486c-9583-c5ac6ebd175b","keyword":"应变能","originalKeyword":"应变能"},{"id":"8c7e00da-b8e5-4033-be4f-ef847072b200","keyword":"结构函数","originalKeyword":"结构函数"},{"id":"ee8b1110-9c10-4596-8d1e-a82af9c04360","keyword":"标度行为","originalKeyword":"标度行为"},{"id":"47d85a6d-99f4-486d-940d-bf2f218ce12a","keyword":"微观相场","originalKeyword":"微观相场"}],"language":"zh","publisherId":"jsrclxb200904041","title":"Ni75Cr19Al6合金中DO22相标度行为的含应变能微观相场研究","volume":"30","year":"2009"},{"abstractinfo":"基于微观相场动力学模型,研究原子间相互作用能对Ni_(75)Al_xV_(25-x)合金孕育期的影响.根据Khachaturyan所给的占位几率公式进一步得到了长程序参数的求值公式.结果表明,先析出相为DO_(22)时,Ni-Al最近邻原子间作用能V_(Ni-Al)增大,L1_2相的孕育期缩短,DO_(22)相的孕育期变化不明显;Ni-V最近邻原子间作用能V_(Ni-v)增大,L1_2相和DO_(22)相的孕育期均缩短.先析出相为L1_2相时,V_(Ni-Al)增大,L1_2相和DO_(22)相孕育期均缩短;V_(Ni-v)增大,L1_2相孕育期变化不明显,DO_(22)相的孕育期缩短.","authors":[{"authorName":"徐聪","id":"a5daf482-5d8b-4913-a8df-d9936783f3c8","originalAuthorName":"徐聪"},{"authorName":"陈铮","id":"531bf70d-4a2f-4fa4-93d6-af671e164ae0","originalAuthorName":"陈铮"},{"authorName":"王永欣","id":"580ec3b8-2536-401c-bcb0-7adc99fab1f3","originalAuthorName":"王永欣"},{"authorName":"<span style=\"color:red\">钟</span><span style=\"color:red\">汉文</span>","id":"64c661cd-4564-4a1e-86a0-4d654cf4fbdb","originalAuthorName":"钟汉文"},{"authorName":"孙立岩","id":"b4390156-167f-4067-b6d8-da2696a21147","originalAuthorName":"孙立岩"},{"authorName":"苗海川","id":"8ea4f2e6-afd5-4189-84a0-735341f65572","originalAuthorName":"苗海川"}],"doi":"","fpage":"1935","id":"ed41b260-e476-4ed1-b40d-03aa6ad6b66e","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":"2ce8a075-af77-4aa5-9dab-7480a15c8348","keyword":"孕育期","originalKeyword":"孕育期"},{"id":"9127eb63-a57e-496c-acb2-5583536a75f0","keyword":"原子间相互作用能","originalKeyword":"原子间相互作用能"},{"id":"9eb60be1-cb00-4d17-bf06-c7583c6e2bf6","keyword":"微观相场","originalKeyword":"微观相场"},{"id":"b27211f8-d6e1-4830-be1a-1f877f8816f0","keyword":"Ni_(75)Al_xV_(25-x)合金","originalKeyword":"Ni_(75)Al_xV_(25-x)合金"}],"language":"zh","publisherId":"xyjsclygc200911012","title":"原子间相互作用能对Ni_(75)Al_xV_(25-x)合金孕育期影响的微观相场模拟","volume":"38","year":"2009"},{"abstractinfo":"以很长半衰期(42×109 a)的β- 衰变的187Re-187Os核对作为大尺度的宇宙核<span style=\"color:red\">钟</span>来量度宇宙的年纪, 是近代天文学与核物理学相结合的又一典范. 这种宇宙时钟是利用裸核187Re与它的衰变子体187Os同位素在共生矿中天然含量的比值来测定时间的. 利用187Re裸核的半衰期通过核物理计算可对中性187Re的半衰期进行修定. ","authors":[{"authorName":"戴光曦","id":"3b3acd4b-8c94-42c4-8606-b24527ec19ac","originalAuthorName":"戴光曦"},{"authorName":"孙志虹","id":"b3356aad-de72-41bb-9942-36b85789b8d0","originalAuthorName":"孙志虹"}],"doi":"10.3969/j.issn.1007-4627.2001.03.006","fpage":"156","id":"0bad3373-d2ea-49dd-9a57-a936e9b6beb8","issue":"3","journal":{"abbrevTitle":"YZHWLPL","coverImgSrc":"journal/img/cover/YZHWLPL.jpg","id":"78","issnPpub":"1007-4627","publisherId":"YZHWLPL","title":"原子核物理评论   "},"keywords":[{"id":"a740148b-a590-40fe-bd3d-dd77e0b6527e","keyword":"宇宙核<span style=\"color:red\">钟</span>","originalKeyword":"宇宙核钟"},{"id":"c71eb820-a82b-4d8f-8bbf-db0cb9ddec81","keyword":"哈勃常数","originalKeyword":"哈勃常数"},{"id":"717765fc-ad90-4f72-ac05-f748451911b7","keyword":"退行速度","originalKeyword":"退行速度"},{"id":"2c15d62f-ca68-49f1-a8fa-a542f011b894","keyword":"中性/裸核187Re","originalKeyword":"中性/裸核187Re"},{"id":"da9b89c6-ca0e-45a0-a5ac-b7a45ca77041","keyword":"同位素的天然含量","originalKeyword":"同位素的天然含量"},{"id":"944039ab-47b4-462b-aa38-5606918359e9","keyword":"大爆炸","originalKeyword":"大爆炸"}],"language":"zh","publisherId":"yzhwlpl200103006","title":"宇宙核<span style=\"color:red\">钟</span>","volume":"18","year":"2001"},{"abstractinfo":"从动力学角度,采用离散单元法研究炉料颗粒的受力和运动,建立高炉无<span style=\"color:red\">钟</span>炉顶布料数值计算模型,模拟无<span style=\"color:red\">钟</span>炉顶布料过程和料面形状.模拟与实测对比表明,两者基本吻合,证明离散单元法在高炉无<span style=\"color:red\">钟</span>布料应用中可行,并为高炉无<span style=\"color:red\">钟</span>炉顶布料的机理研究开辟了一条新的途径.","authors":[{"authorName":"林成城","id":"028ddcae-af9a-439f-9cfa-21a3f9b32313","originalAuthorName":"林成城"},{"authorName":"杜鹤桂","id":"324c03df-e3f7-4648-b410-6daf921a1cdc","originalAuthorName":"杜鹤桂"}],"doi":"","fpage":"0","id":"72cbbc8b-bde6-4522-8fb9-62550f00472a","issue":"3","journal":{"abbrevTitle":"GT","coverImgSrc":"journal/img/cover/GT.jpg","id":"27","issnPpub":"0449-749X","publisherId":"GT","title":"钢铁"},"keywords":[{"id":"a6f6a124-3904-4d51-aa8d-aeb3659e5f39","keyword":"离散单元法","originalKeyword":"离散单元法"},{"id":"fd6036eb-33fa-48fc-b97d-e896ebbb340c","keyword":"无<span style=\"color:red\">钟</span>炉顶","originalKeyword":"无钟炉顶"},{"id":"4ef436f1-2114-4928-9c33-dc75772b5dda","keyword":"布料","originalKeyword":"布料"},{"id":"b9239681-25ae-41fe-b04c-7d665c8a8139","keyword":"料面形状","originalKeyword":"料面形状"},{"id":"44900c0d-e5ec-40aa-b524-2dfca4fe2547","keyword":"数值模拟","originalKeyword":"数值模拟"}],"language":"zh","publisherId":"gt199803002","title":"离散单元法高炉无<span style=\"color:red\">钟</span>炉顶布料模拟研究","volume":"33","year":"1998"},{"abstractinfo":"并罐式无<span style=\"color:red\">钟</span>炉顶的布料操作会产生蛇形偏析,形成不均匀的料面形状,导致料面透气性调节失控的问题.通过开炉布料料面形状的测试结果可知,并罐式无<span style=\"color:red\">钟</span>炉顶料面中心与高炉中心不重合,料面中心发生偏移.为了研究无<span style=\"color:red\">钟</span>布料过程中的料面分布情况,通过建立数学模型,计算炉料颗粒在高炉料面周向上的落点分布,根据落点分布得到料面对称中心位置,并将计算结果与开炉料面形状测试结果对比.根据分析计算结果,从理论出发,提出减小布料过程料流偏析的措施和建议.","authors":[{"authorName":"滕召杰","id":"ef87cffa-8233-4ab9-ad9b-df4300476a03","originalAuthorName":"滕召杰"},{"authorName":"程树森","id":"7b3bce1d-4727-4b73-8896-c762a7e6b938","originalAuthorName":"程树森"},{"authorName":"赵国磊","id":"ae123498-b9ec-4193-ad7e-956499094ce7","originalAuthorName":"赵国磊"}],"doi":"","fpage":"5","id":"83f812ed-40d4-4cdb-9595-cb6a43cb0027","issue":"6","journal":{"abbrevTitle":"GT","coverImgSrc":"journal/img/cover/GT.jpg","id":"27","issnPpub":"0449-749X","publisherId":"GT","title":"钢铁"},"keywords":[{"id":"9eef5a70-28ec-4fc2-8f5d-d29d7ee3259b","keyword":"并罐式","originalKeyword":"并罐式"},{"id":"e294b382-29a3-4c58-bfbc-fb15b4c376ff","keyword":"布料操作","originalKeyword":"布料操作"},{"id":"51974729-1eaa-413b-877f-168cbe3b7f11","keyword":"炉料偏析","originalKeyword":"炉料偏析"},{"id":"90748970-363e-4c26-a702-d8082989a208","keyword":"落点","originalKeyword":"落点"}],"language":"zh","publisherId":"gtyjxb201406002","title":"并罐式无<span style=\"color:red\">钟</span>炉顶布料料面中心研究","volume":"26","year":"2014"},{"abstractinfo":"济钢1 750 m3高炉采用串罐无料<span style=\"color:red\">钟</span>炉顶布料系统.建立了布料模型,并在高炉生产中不断验证,逐步消化和掌握了无料<span style=\"color:red\">钟</span>技术,摸索出一系列无料<span style=\"color:red\">钟</span>炉顶布料的相关规律;建立了布料矩阵调节的基本准则,以\"稳\"为前提,以\"平台漏斗\"理论为依据,充分发挥了布料矩阵技术优势,确保高炉稳定顺行.研究结果表明:焦平台一旦确定,靠微调矿石矩阵可以调整煤气流的合理分布,达到维持矿焦比合理分布的控制目标.通过布料矩阵的不断优化,使高炉的顺行状况改善,高炉的利用系数达到2.35 t/(m3·d).","authors":[{"authorName":"李传辉","id":"dfa33d81-a8ae-46d1-b85b-be2438068ebd","originalAuthorName":"李传辉"},{"authorName":"安铭","id":"677a2f42-1411-4c3f-9b82-cc61b0985620","originalAuthorName":"安铭"},{"authorName":"高征铠","id":"7e7e1c72-397f-437e-8454-f0100ffff4bc","originalAuthorName":"高征铠"},{"authorName":"戴建华","id":"8f67c47e-8918-41e4-8e28-7d9182525fc4","originalAuthorName":"戴建华"}],"doi":"","fpage":"6","id":"d0acc839-9040-4391-8886-7c91a44f23a6","issue":"5","journal":{"abbrevTitle":"GT","coverImgSrc":"journal/img/cover/GT.jpg","id":"27","issnPpub":"0449-749X","publisherId":"GT","title":"钢铁"},"keywords":[{"id":"9a5220bd-1433-4b0a-b064-fbb0efc0434f","keyword":"高炉","originalKeyword":"高炉"},{"id":"93769399-c042-473e-b088-6eaca773f960","keyword":"无料<span style=\"color:red\">钟</span>炉顶","originalKeyword":"无料钟炉顶"},{"id":"ef6e26df-0e71-4e04-8bba-bd1f01551cea","keyword":"布料矩阵","originalKeyword":"布料矩阵"},{"id":"1ae7033d-e689-415e-8f65-40701f0be3c0","keyword":"焦平台","originalKeyword":"焦平台"}],"language":"zh","publisherId":"gt200605002","title":"高炉无料<span style=\"color:red\">钟</span>炉顶布料规律探索与实践","volume":"41","year":"2006"}],"totalpage":20,"totalrecord":193}