{"currentpage":1,"firstResult":0,"maxresult":10,"pagecode":5,"pageindex":{"endPagecode":5,"startPagecode":1},"records":[{"abstractinfo":"本文提出了判别流体热力学性质的通用<span style=\"color:red\">对比方程</span>的规则和选择作为通用<span style=\"color:red\">对比方程</span>的热力学参数<span style=\"color:red\">对比</span>变换的方法；具体给出了工质饱和液体焓和温度的合适<span style=\"color:red\">对比</span>变换式和通用<span style=\"color:red\">对比方程</span>。经检验，该通用<span style=\"color:red\">方程</span>的计算值与25种常用流体工质的推荐值的平均绝对偏差为0.5%，算术平均偏差为--0.04%。本文的理论纠正了传统的只用临界参数为<span style=\"color:red\">对比</span>值的片面认识，为建立在无通用<span style=\"color:red\">对比方程</span>而仅利用合适的参数变换，从一种已知物性物质推算另一种物质未知物性的一般方法和其它物性的通用<span style=\"color:red\">对比方程</span>奠定了基础。","authors":[{"authorName":"陈则韶","id":"28f97549-9f2d-48cc-8348-0ba9d7157542","originalAuthorName":"陈则韶"},{"authorName":"程文龙","id":"32bb5bde-9a08-469b-86dd-fec0c63eee61","originalAuthorName":"程文龙"},{"authorName":"胡?","id":"9bda158e-5a0f-464e-acfd-5de2a3b91a71","originalAuthorName":"胡?"}],"doi":"","fpage":"19","id":"78c04831-aa07-43e0-8536-dd1d9cc23ca9","issue":"1","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":"5ba36472-f511-4f23-a51b-7530124d616b","keyword":"流体工质","originalKeyword":"流体工质"},{"id":"0bbae11f-eff1-4d70-b392-a7c189f64db4","keyword":"热力性质","originalKeyword":"热力性质"},{"id":"fda98f09-ba68-4ba9-a4a1-f8a36b61e567","keyword":"<span style=\"color:red\">对比</span><span style=\"color:red\">态</span><span style=\"color:red\">方程</span>","originalKeyword":"对比态方程"},{"id":"79db4734-61d3-4787-922a-0bbabd2f902d","keyword":"推算法","originalKeyword":"推算法"}],"language":"zh","publisherId":"gcrwlxb200101006","title":"热力参数的<span style=\"color:red\">对比</span>变换与流体工质热力性质的通用<span style=\"color:red\">对比方程</span>","volume":"22","year":"2001"},{"abstractinfo":"本文提出了新的饱和蒸气密度的通用<span style=\"color:red\">对比</span><span style=\"color:red\">态</span>推算式,并分别以标准沸点下的蒸发潜热和临界温度与标准沸点温度之差为基准,对蒸发潜热和温度无量纲化导出了工质蒸发潜热通用<span style=\"color:red\">对比</span><span style=\"color:red\">态</span><span style=\"color:red\">方程</span>,结合饱和液体焓通用<span style=\"color:red\">对比</span><span style=\"color:red\">态</span><span style=\"color:red\">方程</span>导出了饱和蒸气焓通用<span style=\"color:red\">对比</span><span style=\"color:red\">态</span><span style=\"color:red\">方程</span>,揭示出饱和蒸气焓通用<span style=\"color:red\">对比</span><span style=\"color:red\">态</span><span style=\"color:red\">方程</span>为双变量函数,除有温度变量外还包含有表示物质差异的变量.对多种物质的文献值计算比较,以上<span style=\"color:red\">方程</span>的总的平均绝对偏差分别为0.43%、0.87%和0.35%.","authors":[{"authorName":"陈则韶","id":"7ef17a69-9da6-49cd-9bfe-41ff9d6f5397","originalAuthorName":"陈则韶"},{"authorName":"胡芃","id":"0c497ef2-9e4c-46cf-9ab2-5c8a2d23df4a","originalAuthorName":"胡芃"},{"authorName":"程文龙","id":"7a36d99b-f03b-4674-930a-d17d08e5587f","originalAuthorName":"程文龙"}],"doi":"","fpage":"198","id":"299962a2-c9c7-4369-a9ee-aec1d07e2bd6","issue":"2","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":"8f7c1d63-e407-4695-bc8d-ab9025ab86eb","keyword":"饱和蒸气密度","originalKeyword":"饱和蒸气密度"},{"id":"20a01e0d-9d9a-427c-a676-6f32be718320","keyword":"饱和蒸气焓","originalKeyword":"饱和蒸气焓"},{"id":"5a6d138c-50cf-483d-8a09-6866af0d756c","keyword":"蒸发潜热","originalKeyword":"蒸发潜热"},{"id":"8d4dfea9-5a8f-4e11-8578-b54fe3fab1c8","keyword":"<span style=\"color:red\">对比</span><span style=\"color:red\">态</span><span style=\"color:red\">方程</span>","originalKeyword":"对比态方程"}],"language":"zh","publisherId":"gcrwlxb200302005","title":"饱和蒸气密度、焓和蒸发潜热的通用<span style=\"color:red\">对比</span><span style=\"color:red\">态</span>推算式","volume":"24","year":"2003"},{"abstractinfo":"对正火<span style=\"color:red\">态</span>的50SiMnVB钢常温下的准静态和动态力学特性进行测试,得出材料在不同应变率下的应力一应变曲线.根据Johnson-Cook模型,建立正火<span style=\"color:red\">态</span>50SiMnVB钢从准静态到动态较宽应变速率范围的物理本构<span style=\"color:red\">方程</span>.<span style=\"color:red\">对比</span>结果表明,所建立的本构<span style=\"color:red\">方程</span>和实验结果吻合较好.","authors":[{"authorName":"刘盼萍","id":"857e2de0-7e95-4696-a21e-bea5632a948e","originalAuthorName":"刘盼萍"},{"authorName":"尹燕","id":"7c27b694-3d7e-4476-bdb0-2d8c3286b138","originalAuthorName":"尹燕"},{"authorName":"常列珍","id":"7be665e6-37b3-4189-826c-d0c12222a31c","originalAuthorName":"常列珍"},{"authorName":"薛勇","id":"4ff91ae7-968e-4829-9df1-b4ab133a91b2","originalAuthorName":"薛勇"}],"doi":"10.3969/j.issn.1004-244X.2009.01.013","fpage":"45","id":"7fe03434-238b-4d55-84d5-8dc37de9ccd9","issue":"1","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":"856b9db6-a2cf-4375-aaf7-b569d6c993c5","keyword":"正火","originalKeyword":"正火"},{"id":"897c339e-5afe-4ad1-8b69-07ecb6e7f5f5","keyword":"50SiMnVB钢","originalKeyword":"50SiMnVB钢"},{"id":"d550117e-e9cc-4e9f-a140-942616b178d2","keyword":"Johnson-Cook本构<span style=\"color:red\">方程</span>","originalKeyword":"Johnson-Cook本构方程"}],"language":"zh","publisherId":"bqclkxygc200901013","title":"正火<span style=\"color:red\">态</span>50SiMnVB钢Johnson-Cook本构<span style=\"color:red\">方程</span>的建立","volume":"32","year":"2009"},{"abstractinfo":"讨论了光学图像中同时存在噪声与模糊时的<span style=\"color:red\">对比</span>度增强问题.构造了一种基于边缘定向扩散的各向异性非线性扩散<span style=\"color:red\">方程</span>来作为图像的光滑约束项,并根据模糊后的图像在边缘处相对清晰图像具有较大误差的事实,构造增强图像与原图像之间的非均匀逼近项,将此两项通过正则化参数联系起来,得到了一种图像<span style=\"color:red\">对比</span>度增强的正则化模型,并利用Euler<span style=\"color:red\">方程</span>将该模型转换成一种可以快速求解的各向异性非线性扩散模型.该模型能在抑制噪声的同时增强图像的边缘,在模型的解算上也不存在大型矩阵的存储与运算问题.数值计算结果表明,新方法适合于多种形式的模糊和不同程度的噪声污染,相对现有方法具有更好的边缘锐化能力和更高的清晰度,峰值信噪比比现有方法提高了1～2 dB,边缘保护指数也比现有方法有较大提高.","authors":[{"authorName":"谢美华","id":"3a4238b9-7b25-403b-b29f-1c4558d07589","originalAuthorName":"谢美华"},{"authorName":"王正明","id":"cf9138ce-e446-4adf-8999-575e0b67fa48","originalAuthorName":"王正明"}],"doi":"10.3969/j.issn.1007-5461.2006.02.001","fpage":"129","id":"d3aae31a-7aca-482c-8e85-ab01e65ce7e7","issue":"2","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":"51f1ecec-a643-400c-af4e-4f14cad78f2d","keyword":"图像处理","originalKeyword":"图像处理"},{"id":"54780ce6-091c-4555-ba03-29e245ade226","keyword":"<span style=\"color:red\">对比</span>度增强","originalKeyword":"对比度增强"},{"id":"72e1625b-9dac-4f9c-acbe-595a7873fdcc","keyword":"各向异性扩散","originalKeyword":"各向异性扩散"},{"id":"313b44cd-b24a-4688-a738-ca3cfab77291","keyword":"正则化","originalKeyword":"正则化"},{"id":"9bd27b92-fa79-48e9-b9c4-6a211d42a954","keyword":"边缘定向","originalKeyword":"边缘定向"}],"language":"zh","publisherId":"lzdzxb200602001","title":"基于各向异性扩散<span style=\"color:red\">方程</span>的图像<span style=\"color:red\">对比</span>度增强方法","volume":"23","year":"2006"},{"abstractinfo":"简述了一维定<span style=\"color:red\">态</span>Schr(o)dinger<span style=\"color:red\">方程</span>的辛形式、求解本征值问题的辛-矩阵法和辛-打靶法及在充分远空间计算线性无关解的保Wronskian算法.","authors":[{"authorName":"刘学深","id":"928b3ae5-60db-47a2-882b-1b42f59e7538","originalAuthorName":"刘学深"},{"authorName":"祁月盈","id":"99d4f1ad-b338-4d96-92a2-f1c555ec5588","originalAuthorName":"祁月盈"},{"authorName":"刘晓艳","id":"0c554a5c-ef4c-48f1-bffb-89c42f09a873","originalAuthorName":"刘晓艳"},{"authorName":"丁培柱","id":"f77f72a8-f4d5-4854-8da5-3a6c39e4a334","originalAuthorName":"丁培柱"},{"authorName":"周忠源","id":"c59f206d-53c1-4459-8759-86440c7fcf5b","originalAuthorName":"周忠源"}],"doi":"10.3969/j.issn.1007-4627.2002.z1.041","fpage":"138","id":"77f113a9-53a4-4643-ad02-255745b5c251","issue":"z1","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":"9276d21d-290d-420e-a161-838132c11d82","keyword":"定<span style=\"color:red\">态</span>Schr(o)dinger<span style=\"color:red\">方程</span>","originalKeyword":"定态Schr(o)dinger方程"},{"id":"da44f9f4-c90e-4f65-8432-2cae6c841e69","keyword":"分立<span style=\"color:red\">态</span>","originalKeyword":"分立态"},{"id":"2341644b-d0c5-42dc-97c2-e2989aeeb260","keyword":"辛-打靶法","originalKeyword":"辛-打靶法"},{"id":"61c3cae6-1b88-4f58-94d3-b0f389348c33","keyword":"保Wronskian","originalKeyword":"保Wronskian"}],"language":"zh","publisherId":"yzhwlpl2002z1041","title":"强场物理中定<span style=\"color:red\">态</span>Schr(o)dinger<span style=\"color:red\">方程</span>的辛算法","volume":"19","year":"2002"},{"abstractinfo":"对真空感应炉熔炼制备的烧结钕铁硼磁体在-196℃保温4h进行深冷处理.采用X-射线衍射仪和扫描电子显微镜<span style=\"color:red\">对比</span>分析了烧结<span style=\"color:red\">态</span>与深冷处理<span style=\"color:red\">态</span>钕铁硼组织.结果表明,经深冷处理后,磁体富钕相团聚、孔隙和裂纹等组织缺陷得到明显改善,富钕相重新弥散、均匀分布在晶界周围,部分富钕相填充到材料的微孔内,晶界变得较平滑;主相晶粒尺寸降到烧结<span style=\"color:red\">态</span>的64.6％,偏差降低了4.07 μm,晶粒的均匀度有所改善;同时深冷处理过程中的体积收缩产生较大的内应力,使内部的某些晶粒向易磁化轴c轴方向转动,取向度由86.16％提高到92.11％,在深冷处理过程中并未发现有新的织构产生.","authors":[{"authorName":"韩翠珍","id":"904ebf13-8def-48d8-9a1d-3233f6d1d123","originalAuthorName":"韩翠珍"},{"authorName":"张胤","id":"e4110da9-d2c6-4d01-a1a2-8980c9a9b179","originalAuthorName":"张胤"},{"authorName":"夏立明","id":"ee097cfc-576b-4808-bdc0-28228510bbbf","originalAuthorName":"夏立明"}],"doi":"10.13228/j.boyuan.issn1001-0777.20130084","fpage":"1","id":"6e757adf-d046-4f4e-b529-88874c1a2082","issue":"4","journal":{"abbrevTitle":"WLCS","coverImgSrc":"journal/img/cover/WLCS.jpg","id":"64","issnPpub":"1001-0777","publisherId":"WLCS","title":"物理测试"},"keywords":[{"id":"dfae4f30-75e1-4b8b-9a07-9bba4d3930f1","keyword":"烧结钕铁硼磁体","originalKeyword":"烧结钕铁硼磁体"},{"id":"7e840cb9-0269-4db0-8d08-6d50c012bca9","keyword":"微观组织","originalKeyword":"微观组织"},{"id":"7d431598-e988-45a4-b79b-d34f3ed0991e","keyword":"取向度","originalKeyword":"取向度"},{"id":"b3818739-a0e6-44c5-a7ca-b1a8225cdd10","keyword":"深冷处理","originalKeyword":"深冷处理"}],"language":"zh","publisherId":"wlcs201404001","title":"烧结<span style=\"color:red\">态</span>与深冷处理<span style=\"color:red\">态</span>NdFeB组织<span style=\"color:red\">对比</span>分析","volume":"32","year":"2014"},{"abstractinfo":"介子结合<span style=\"color:red\">态</span>本征<span style=\"color:red\">方程</span>中δ相互作用可用T矩阵进行非微扰重整化, 深入理解重整化的一些基本问题: 物理结果与重正化点的选取无关, T矩阵非微扰重整化的物理实质.","authors":[{"authorName":"王顺金","id":"f3097ca2-aab4-403d-9bb3-a50990dd1f64","originalAuthorName":"王顺金"},{"authorName":"周善贵","id":"2d864536-da12-40c4-9903-aa85da81850d","originalAuthorName":"周善贵"},{"authorName":"H.C.Pauli","id":"bf702c16-7f71-47bd-80ba-a7025db1af9f","originalAuthorName":"H.C.Pauli"}],"doi":"10.3969/j.issn.1007-4627.2004.04.009","fpage":"298","id":"fae58293-5739-4ddb-a1f3-d50adb0b9eef","issue":"4","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":"59b3bdc9-4486-4103-8ebf-e587464e94f5","keyword":"介子结合<span style=\"color:red\">态</span>本征<span style=\"color:red\">方程</span>","originalKeyword":"介子结合态本征方程"},{"id":"2a128ece-7e04-44e2-8248-bb800f2663e9","keyword":"T矩阵非微扰重整化","originalKeyword":"T矩阵非微扰重整化"},{"id":"bdddb303-ab19-4310-bad5-cdf42f5f3d0d","keyword":"本征波函数","originalKeyword":"本征波函数"}],"language":"zh","publisherId":"yzhwlpl200404009","title":"介子束缚<span style=\"color:red\">态</span>相对论本征<span style=\"color:red\">方程</span>的非微扰重整化","volume":"21","year":"2004"},{"abstractinfo":"C. P. Bean基于K. Mendelssohn海绵模型建立了非理想Ⅱ类超导体临界<span style=\"color:red\">态</span>理论, 从而形成了硬超导体电磁理论的重要基础之一.然而近年来基于涡旋动力学理论的发展,逐步形成了临界<span style=\"color:red\">态</span>动力学研究课题.涡旋运动导致宏观波函数的相滑移,和局域的Joule热等强烈非线性效应是形成自组织临界<span style=\"color:red\">态</span>物理基础.根据实验观测,磁通进入样品的前锋为线性分布,但其解析理论还在发展中.本文论述了在超导体的零电阻和完全抗磁性的实验基础上建立起来的London第一和第二<span style=\"color:red\">方程</span>本质上的等价性,并结合London理论与Anderson磁通热激活理论讨论了临界<span style=\"color:red\">态</span>形成动力学,给出了Slab样品中的电场、电流和磁通密度分布,定量解释了实验观察到的现象.","authors":[{"authorName":"韩永胜","id":"2a51c792-9cb0-43eb-96d2-9fc987f80fcc","originalAuthorName":"韩永胜"},{"authorName":"陈曙","id":"2b7076e0-1b5e-4ce4-a937-bea050c1e751","originalAuthorName":"陈曙"},{"authorName":"杨宏新","id":"bddcf11f-a8f4-4764-9051-20d0ff5e54dc","originalAuthorName":"杨宏新"}],"doi":"10.3969/j.issn.1000-3258.2004.03.004","fpage":"194","id":"cc669104-4fcb-40c4-b977-91290956d522","issue":"3","journal":{"abbrevTitle":"DWWLXB","coverImgSrc":"journal/img/cover/DWWLXB.jpg","id":"19","issnPpub":"1000-3258","publisherId":"DWWLXB","title":"低温物理学报   "},"keywords":[{"id":"30e456ee-faab-447c-a858-92904e370760","keyword":"Bean 模型,Slab样品,涡旋动力学,磁通密度分布","originalKeyword":"Bean 模型,Slab样品,涡旋动力学,磁通密度分布"}],"language":"zh","publisherId":"dwwlxb200403004","title":"London 两个<span style=\"color:red\">方程</span>等价性与临界<span style=\"color:red\">态</span>形成动力学","volume":"26","year":"2004"},{"abstractinfo":"针对超超临界机组中863 K服役20000 h的HR3C再热器管材及与其具有相同Larson-Miller参数值的923 K时效1100 h HR3C管材,开展显微组织结构老化及力学性能衰减的<span style=\"color:red\">对比</span>研究.结果表明,服役环境的不同导致服役<span style=\"color:red\">态</span>HR3C钢管的内外侧显微组织结构产生差异.服役<span style=\"color:red\">态</span>HR3C内侧的显微组织结构和力学性能与时效<span style=\"color:red\">态</span>的基本相同;然而,服役<span style=\"color:red\">态</span>钢管外侧的结构损伤程度比时效<span style=\"color:red\">态</span>钢管更严重.因此,基于Larson-Miller参数的人工时效方法只能在一定条件下模拟USC机组中钢管的结构老化.","authors":[{"authorName":"白小龙","id":"e6c7bf0d-80ba-474f-bceb-5e5b1d560ff2","originalAuthorName":"白小龙"},{"authorName":"陈国宏","id":"6f2f770e-c57d-4ff7-9a88-c508f4ee439d","originalAuthorName":"陈国宏"},{"authorName":"刘俊建","id":"25bf1bb9-9ada-4510-adfd-f988466990ac","originalAuthorName":"刘俊建"},{"authorName":"王家庆","id":"d612e345-8de1-4063-ba4a-08b7f2d5da16","originalAuthorName":"王家庆"},{"authorName":"张涛","id":"ab45dc69-6fa4-43c4-8766-a9c3b6e999bf","originalAuthorName":"张涛"},{"authorName":"汤文明","id":"65b03084-b69c-44c7-889e-768d9eb1c60c","originalAuthorName":"汤文明"}],"doi":"","fpage":"100","id":"c432538e-ac90-4a5e-8520-78cfd91df957","issue":"z2","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":"95d2e73a-5fc7-475f-81a6-a4f65a77e8f1","keyword":"HR3C耐热钢","originalKeyword":"HR3C耐热钢"},{"id":"92ba222c-dec5-4ec7-b9c9-27f5c9922052","keyword":"Larson-Miller参数","originalKeyword":"Larson-Miller参数"},{"id":"b63734ac-b0d5-4201-b8f2-45166b7401af","keyword":"结构损伤","originalKeyword":"结构损伤"},{"id":"fc3d9e14-6019-47a0-8d65-6f73adcbd31f","keyword":"力学性能","originalKeyword":"力学性能"}],"language":"zh","publisherId":"jsrclxb2013z2022","title":"服役及时效<span style=\"color:red\">态</span>HR3C耐热钢结构损伤的<span style=\"color:red\">对比</span>","volume":"34","year":"2013"},{"abstractinfo":"本文介绍一种热泵热水器性能的无量纲<span style=\"color:red\">对比</span><span style=\"color:red\">态</span>分析法,该方法采用不同工况的热泵热水器性能参数与标准设计工况的参数<span style=\"color:red\">对比</span>的无量纲参数来描述实际工况性能.分别导出了理论和实际的描述热泵热水器变工况性能的无量纲表达式,给出了环境气温从-5～40℃,进水温度从5～30℃的无量纲性能曲线,以及两种型号的实验机的结霜温度区的实验结果无量纲<span style=\"color:red\">对比</span>性能.研究发现,热泵热水器的<span style=\"color:red\">对比</span>热水流量(m)w是体现变工况性能的极为敏感和重要的参数,只有用(m)w和COP相结合,才能全面反映热泵性能.","authors":[{"authorName":"陈则韶","id":"df14073f-6e51-45b1-818e-b08445498859","originalAuthorName":"陈则韶"},{"authorName":"胡芃","id":"56ee35ec-9e8e-49c4-8bf0-698256e8f3b0","originalAuthorName":"胡芃"},{"authorName":"江斌","id":"8d9b2658-a1bc-4c62-9502-3f8d313fdc06","originalAuthorName":"江斌"},{"authorName":"谢文海","id":"ad93cc63-3e1f-47f7-b86b-cc12cdbe3ac2","originalAuthorName":"谢文海"},{"authorName":"李川","id":"d2ab478d-585c-4714-b4e1-2dcca1c38fa1","originalAuthorName":"李川"}],"doi":"","fpage":"9","id":"2636fc0e-6b46-4f71-8ca4-84e463f41aec","issue":"1","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":"648dd172-3acc-4334-b258-77163c24e15c","keyword":"热泵热水器","originalKeyword":"热泵热水器"},{"id":"959de497-45de-4960-9c90-526db9653628","keyword":"无量纲分析法","originalKeyword":"无量纲分析法"},{"id":"012ad34f-c7c3-4999-aa4d-9dbf0933f168","keyword":"热泵效率","originalKeyword":"热泵效率"}],"language":"zh","publisherId":"gcrwlxb201301003","title":"热泵热水器变工况性能的无量纲<span style=\"color:red\">对比</span><span style=\"color:red\">态</span>分析法","volume":"34","year":"2013"}],"totalpage":2356,"totalrecord":23552}