{"currentpage":1,"firstResult":0,"maxresult":10,"pagecode":5,"pageindex":{"endPagecode":5,"startPagecode":1},"records":[{"abstractinfo":"研究了用低频<span style=\"color:red\">方波</span><span style=\"color:red\">电流</span>对不锈钢进行电解着色,探讨了<span style=\"color:red\">电流</span>参数对着色效果的影响.通过记录在施加<span style=\"color:red\">电流</span>过程中不锈钢试片的响应电位随时间的变化,从而判断发生着色的可能性,并且设计实验确定了适用的工艺条件,最后制备出各种颜色的不锈钢.","authors":[{"authorName":"贾法龙","id":"8bc9acaf-bcc3-4906-9227-51d4fff64a72","originalAuthorName":"贾法龙"},{"authorName":"郭稚弧","id":"03ac76ef-81df-407d-8b0d-d24bc61c903c","originalAuthorName":"郭稚弧"},{"authorName":"李卓民","id":"8cf37a48-51b1-4f2e-9ad8-04308b9f656a","originalAuthorName":"李卓民"}],"doi":"","fpage":"105","id":"a000da46-961b-4f25-8b68-abf26ca067a6","issue":"3","journal":{"abbrevTitle":"FSYFH","coverImgSrc":"journal/img/cover/FSYFH.jpg","id":"25","issnPpub":"1005-748X","publisherId":"FSYFH","title":"腐蚀与防护"},"keywords":[{"id":"387b92b2-ebc7-413c-9a14-4ae05524ea24","keyword":"不锈钢","originalKeyword":"不锈钢"},{"id":"b18de2de-267f-4d02-8b0c-4a5153b2b5c3","keyword":"电解着色","originalKeyword":"电解着色"},{"id":"d4ecce7c-cadb-4589-88fa-c15779ed7406","keyword":"<span style=\"color:red\">方波</span><span style=\"color:red\">电流</span>","originalKeyword":"方波电流"}],"language":"zh","publisherId":"fsyfh200103004","title":"低频<span style=\"color:red\">方波</span><span style=\"color:red\">电流</span>进行不锈钢电解着色的研究","volume":"22","year":"2001"},{"abstractinfo":"采用电化学方法和阳极消耗率评价法研究了高硅铸铁阳极在<span style=\"color:red\">方波</span>脉冲<span style=\"color:red\">电流</span>作用下的电化学性能.结果表明,<span style=\"color:red\">方波</span>脉冲<span style=\"color:red\">电流</span>作用下,阳极表面状态的变化与直流作用时基本相同,钝化膜未被破坏.同等条件下阳极的消耗率比直流作用时的小.因此,在所研究的介质中高硅铸铁阳极可以用于<span style=\"color:red\">方波</span>脉冲<span style=\"color:red\">电流</span>阴极保护.","authors":[{"authorName":"邱于兵","id":"49185a80-8215-4084-b05c-e495f8a8905c","originalAuthorName":"邱于兵"},{"authorName":"李建梅","id":"bff4e3ea-8e63-4098-b96d-71d0a3efa1e7","originalAuthorName":"李建梅"},{"authorName":"郭稚弧","id":"ee9c765e-0c0f-4b84-80df-bafb3d5924f7","originalAuthorName":"郭稚弧"},{"authorName":"魏伯康","id":"f4cc9a6d-38db-4de5-be18-6a0da2549c4f","originalAuthorName":"魏伯康"},{"authorName":"林汉同","id":"4837ec84-726d-401c-aba8-483bd488eb8a","originalAuthorName":"林汉同"}],"doi":"10.3969/j.issn.1001-1560.2000.02.025","fpage":"41","id":"cc631f7a-1d16-4cc3-8b36-7a676b5aff24","issue":"2","journal":{"abbrevTitle":"CLBH","coverImgSrc":"journal/img/cover/CLBH.jpg","id":"7","issnPpub":"1001-1560","publisherId":"CLBH","title":"材料保护"},"keywords":[{"id":"ae31c882-584a-4460-b004-fe405a192d59","keyword":"<span style=\"color:red\">方波</span>脉冲<span style=\"color:red\">电流</span>","originalKeyword":"方波脉冲电流"},{"id":"cd7bffa1-2202-4507-a3f7-dd9526bf3a53","keyword":"高硅铸铁阳极","originalKeyword":"高硅铸铁阳极"},{"id":"789b85c7-7eff-4cbc-9bf9-953f1761e3d6","keyword":"电化学性能","originalKeyword":"电化学性能"},{"id":"42b4ae88-f3b4-4615-8206-d8387a985df6","keyword":"阴极保护","originalKeyword":"阴极保护"}],"language":"zh","publisherId":"clbh200002025","title":"<span style=\"color:red\">方波</span>脉冲<span style=\"color:red\">电流</span>作用下高硅铸铁阳极的电化学性能","volume":"33","year":"2000"},{"abstractinfo":"在3％NaCl、006％NaCl和自来水3种实验介质中，研究了Q 235钢的<span style=\"color:red\">方波</span>脉冲<span style=\"color:red\">电流</span>幅值(I\\-A)、频率(f)和占空比(P)的变化对于阴极极化 电位(E)和极化幅度(ΔE)的影响规律.结果表明，E和ΔE随<span style=\"color:red\">方波</span>I\\-A 、f和P的增加而变负，但当E接近或负于-100 V(SCE)时，再增加各<span style=\"color:red\">电流</span>参数的值， E和ΔE的负移程度都大大减小.各<span style=\"color:red\">电流</span>参数对ΔE的影响程度不同，并与E值 密切 相关.提出调整<span style=\"color:red\">电流</span>参数总的原则和方法是：在达到所要求的保护效果的前提下，尽可能采 用低P、低IA的<span style=\"color:red\">电流</span>参数，并优先调整f,再调整I\\-A.","authors":[{"authorName":"邱于兵","id":"d50a4713-2db7-42e9-ae6b-fd89fc15bcb1","originalAuthorName":"邱于兵"},{"authorName":"郭稚弧","id":"38ff5efe-14c2-4f87-ad25-9d47e40da7b9","originalAuthorName":"郭稚弧"},{"authorName":"林汉同","id":"a4c4e41a-01e1-4ce7-9d30-6835518efc2c","originalAuthorName":"林汉同"}],"categoryName":"|","doi":"","fpage":"367","id":"465bc375-026a-4615-bd60-c38f5e4cc0e2","issue":"6","journal":{"abbrevTitle":"ZGFSYFHXB","coverImgSrc":"journal/img/cover/中国腐蚀封面19-3期-01.jpg","id":"81","issnPpub":"1005-4537","publisherId":"ZGFSYFHXB","title":"中国腐蚀与防护学报"},"keywords":[{"id":"fbf76288-2f14-4c84-9e22-52b22f54514c","keyword":"<span style=\"color:red\">电流</span>参数","originalKeyword":"电流参数"},{"id":"00636971-bb63-4d9a-a21c-1c961943d66d","keyword":"square wave","originalKeyword":"square wave"},{"id":"14fc3241-405f-4c8f-9d2b-1114f38a825d","keyword":"pulsed current","originalKeyword":"pulsed current"},{"id":"d2583066-8c9b-45ff-8855-ddef7eadabe7","keyword":"cathodic protection","originalKeyword":"cathodic protection"},{"id":"af35e1d8-a602-4ec0-a8a0-f7858649e75b","keyword":"mechanism","originalKeyword":"mechanism"},{"id":"8ae946a5-1b00-4c77-8f67-82f99ef64dca","keyword":"null","originalKeyword":"null"}],"language":"zh","publisherId":"1005-4537_2002_6_10","title":"<span style=\"color:red\">方波</span>脉冲<span style=\"color:red\">电流</span>阴极保护机理研究Ⅱ <span style=\"color:red\">电流</span>参数的影响","volume":"22","year":"2002"},{"abstractinfo":"为了弄清脉冲<span style=\"color:red\">电流</span>阴极保护的基本规律,为现场应用提供科学的理论依据和参考,采用<span style=\"color:red\">方波</span>脉冲<span style=\"color:red\">电流</span>对模拟管线体系脉冲<span style=\"color:red\">电流</span>阴极保护的电位分布规律以及脉冲<span style=\"color:red\">电流</span>参数和其他因素对电位分布的影响进行了研究.在3.5 m(长)×2.0 m(宽)×3.0 m(深)的水池中,建立了均匀介质模拟水平管道体系,研究了<span style=\"color:red\">方波</span>脉冲<span style=\"color:red\">电流</span>参数(频率、幅值、占空比)、阳极距离等因素对<span style=\"color:red\">方波</span>脉冲<span style=\"color:red\">电流</span>阴极保护效果的影响,并将直流与<span style=\"color:red\">方波</span>脉冲<span style=\"color:red\">电流</span>的阴极保护效果进行了对比.结果表明,随着<span style=\"color:red\">方波</span>脉冲<span style=\"color:red\">电流</span>频率、幅值或占空比的增加,阴极极化电位分布曲线逐渐负移,极化幅度逐渐增加,且阴极表面的电位分布远比直流作用时均匀,有效保护深度明显延长,所需平均保护<span style=\"color:red\">电流</span>更小.","authors":[{"authorName":"余成平","id":"c621ec2a-2566-48ee-882e-5a96c11fe06c","originalAuthorName":"余成平"},{"authorName":"郭兴蓬","id":"e5db5006-e0c9-4d1a-a8f7-83476310531f","originalAuthorName":"郭兴蓬"},{"authorName":"邱于兵","id":"9652e12c-231a-428b-951e-649338059419","originalAuthorName":"邱于兵"},{"authorName":"程明山","id":"4fd13848-1cb6-4ae7-8f4f-7bcbce01fdaf","originalAuthorName":"程明山"}],"doi":"10.3969/j.issn.1001-1560.2004.08.016","fpage":"39","id":"0d491bb3-6577-4c1e-a204-bc3647787f73","issue":"8","journal":{"abbrevTitle":"CLBH","coverImgSrc":"journal/img/cover/CLBH.jpg","id":"7","issnPpub":"1001-1560","publisherId":"CLBH","title":"材料保护"},"keywords":[{"id":"c93db25e-5e52-4bd6-b21e-60ea8e2625f4","keyword":"阴极保护","originalKeyword":"阴极保护"},{"id":"5d265b49-7cd8-4548-b152-6a5f44bfa2d1","keyword":"管道系统","originalKeyword":"管道系统"},{"id":"b054a7af-ece1-40be-a857-0be5a9dfe860","keyword":"<span style=\"color:red\">方波</span>","originalKeyword":"方波"},{"id":"afdb1c49-8feb-4650-9938-96ec49a7c90e","keyword":"脉冲<span style=\"color:red\">电流</span>","originalKeyword":"脉冲电流"}],"language":"zh","publisherId":"clbh200408016","title":"模拟管线系统中<span style=\"color:red\">方波</span>脉冲<span style=\"color:red\">电流</span>阴极保护规律的研究","volume":"37","year":"2004"},{"abstractinfo":"应用 Laplace 变换分析求得了在线性极化区内向金属电极施加<span style=\"color:red\">方波</span>动<span style=\"color:red\">电流</span>扫描的响应函数方程.它在 E～i 座标系中为两条长度相等的平行线。用它可以方便地测量 R_P、C 和 R_S 等电化学参数而不受溶液电阻的影响。本方法对弛豫时间常数较大的体系尤为适用。","authors":[{"authorName":"毕新民","id":"a4e77d00-f4c5-4f1a-9b4b-52d425be9025","originalAuthorName":"毕新民"},{"authorName":"曹楚南","id":"8fde5cd7-a5bb-496c-be96-f033115146c1","originalAuthorName":"曹楚南"}],"categoryName":"|","doi":"","fpage":"43","id":"ba1e03a3-19a7-4ed7-a3f5-ff07a8b926e0","issue":"1","journal":{"abbrevTitle":"ZGFSYFHXB","coverImgSrc":"journal/img/cover/中国腐蚀封面19-3期-01.jpg","id":"81","issnPpub":"1005-4537","publisherId":"ZGFSYFHXB","title":"中国腐蚀与防护学报"},"keywords":[],"language":"zh","publisherId":"1005-4537_1989_1_9","title":"<span style=\"color:red\">方波</span>动<span style=\"color:red\">电流</span>扫描的响应函数及其应用","volume":"9","year":"1989"},{"abstractinfo":"采用挂片法,在人造海水和自来水介质中,对Q235(A3)钢在直流和<span style=\"color:red\">方波</span>脉冲<span style=\"color:red\">电流</span>阴极保护状态下的保护效果进行了对比研究,得出了具体的保护度和保护效率.结果表明,实验条件下脉冲<span style=\"color:red\">电流</span>阴极保护与直流阴极保护相比,二者的保护度相当,而脉冲<span style=\"color:red\">电流</span>阴极保护有更小的平均<span style=\"color:red\">电流</span>消耗和更高的保护效率.","authors":[{"authorName":"邱于兵","id":"dd119167-82e4-4e06-8c66-301925d27194","originalAuthorName":"邱于兵"},{"authorName":"朱鸿赫","id":"ce4ca292-92c9-4b5b-8877-eeecc3276a25","originalAuthorName":"朱鸿赫"},{"authorName":"余成平","id":"cc7649e6-28ea-4e11-9d3d-c4e2f7a8db26","originalAuthorName":"余成平"},{"authorName":"郭兴蓬","id":"7854c4cd-9272-46b1-8691-02846ec4e1a8","originalAuthorName":"郭兴蓬"},{"authorName":"程明山","id":"649b7428-3ff1-4e40-82b7-88f2032e0cf4","originalAuthorName":"程明山"}],"doi":"10.3969/j.issn.1005-748X.2004.12.005","fpage":"520","id":"bf379df3-62e4-4ae3-b23a-2f2edab397a0","issue":"12","journal":{"abbrevTitle":"FSYFH","coverImgSrc":"journal/img/cover/FSYFH.jpg","id":"25","issnPpub":"1005-748X","publisherId":"FSYFH","title":"腐蚀与防护"},"keywords":[{"id":"0a53e689-108e-4ba5-b5fb-4328e0356c22","keyword":"挂片法","originalKeyword":"挂片法"},{"id":"aec39dfa-1076-4c46-af85-8f85beac9206","keyword":"<span style=\"color:red\">方波</span>脉冲<span style=\"color:red\">电流</span>","originalKeyword":"方波脉冲电流"},{"id":"51d80caf-78ca-415d-8de4-3aca557bc47a","keyword":"阴极保护","originalKeyword":"阴极保护"},{"id":"bb6dd135-7401-44cc-9c64-29aba7a0b5dd","keyword":"保护度","originalKeyword":"保护度"},{"id":"e372ce16-22e5-426c-accd-ae63233f0028","keyword":"保护效率","originalKeyword":"保护效率"}],"language":"zh","publisherId":"fsyfh200412005","title":"<span style=\"color:red\">方波</span>脉冲<span style=\"color:red\">电流</span>阴极保护效果的实验研究","volume":"25","year":"2004"},{"abstractinfo":"Nano-SQUID因为具备可能探测到单电子自旋的能力而受到广泛关注.为进一步提高该器件的灵敏度,不但要优化器件制备工艺,而且也要发展低噪音高效率的测量系统.通常,由于nano-SQUID存在回滞现象,导致在测量方面nano-SQUID无法使用标准的SQUID读出电路.本文设计了一种全新的<span style=\"color:red\">方波</span>脉冲测量方法,由信号发生器串联一个大电阻发送<span style=\"color:red\">电流</span>脉冲,注入nano-SQUID,并采用ADWin数据采集卡读取器件两端的电压.该方法不仅可以消除<span style=\"color:red\">电流</span>—电压回滞现象带来的测量上的不便,而且可以通过缩短脉冲周期的方法进一步提高系统的测量速度.在此基础上,通过降低系统<span style=\"color:red\">方波</span>脉冲占空比ton:toff,增加超导器件因受到脉冲<span style=\"color:red\">电流</span>激发后的冷却时间,减小热噪音对临界<span style=\"color:red\">电流</span>准确测量的影响,从而获得准确的临界<span style=\"color:red\">电流</span>—磁通调制曲线,调制深度△Ic/Ic=7.9％.此外,本文对采用本测量方法的nano-SQUID磁通噪音表征方法进行了讨论,测得器件磁通噪声为72 μφ0/Hz1/2,等效磁性测量精度为1.19×10-16 emu/ Hz1/2.","authors":[{"authorName":"柳西西","id":"f490ef88-1909-43c1-b33b-6b82f3f74246","originalAuthorName":"柳西西"},{"authorName":"刘晓宇","id":"1bd8ec8d-b36b-4dcc-b388-1c381e24c82d","originalAuthorName":"刘晓宇"},{"authorName":"汪浩","id":"87c8357c-e93b-4c42-b23a-98e7e9e345e4","originalAuthorName":"汪浩"},{"authorName":"陈垒","id":"f8e0384c-de73-4788-acfc-b0e36854ee94","originalAuthorName":"陈垒"},{"authorName":"王镇","id":"d51511a1-ea6b-4779-b79c-7711d254f24c","originalAuthorName":"王镇"}],"doi":"","fpage":"276","id":"4031261b-68e5-49e9-8cb6-8cd87785e93c","issue":"4","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":"1ec6b369-ecdb-4450-b8a6-55af2705979b","keyword":"nano-SQUID","originalKeyword":"nano-SQUID"},{"id":"37e91c97-7025-431a-9521-6092e4d6e699","keyword":"<span style=\"color:red\">方波</span>脉冲测量","originalKeyword":"方波脉冲测量"},{"id":"dba5f4ae-cd42-4478-ab6d-e1329267a345","keyword":"临界<span style=\"color:red\">电流</span>","originalKeyword":"临界电流"},{"id":"6efa9d23-f94b-4f91-a260-a6944b5920ac","keyword":"热效应","originalKeyword":"热效应"}],"language":"zh","publisherId":"dwwlxb201504006","title":"Nano-SQUID中<span style=\"color:red\">方波</span>脉冲测量方法对于临界<span style=\"color:red\">电流</span>的精确表征","volume":"37","year":"2015"},{"abstractinfo":"采用新型超快速变换HPVP-TIG电弧焊接工艺进行2219-T87高强铝合金焊接, 研究脉冲<span style=\"color:red\">电流</span>特征参数对焊接接头组织和力学性能的影响. 结果表明, 加入超音频脉冲<span style=\"color:red\">方波</span><span style=\"color:red\">电流</span>(UPSWC)作用后, 铝合金焊缝区显微组织由粗大柱状晶转变为细小等轴晶, 在焊缝区内除了等轴树枝晶外, 还存在一种呈带状分布的极细小等轴非枝晶组织, 同时焊缝熔合区宽度明显减小, 焊接接头抗拉强度和断后伸长率显著提高. 在一定范围内增加脉冲<span style=\"color:red\">电流</span>幅值, 提高脉冲频率, 减小占空比, 可增强组织细化作用, 提高接头力学性能. 与未加入UPSWC作用相比, 脉冲<span style=\"color:red\">电流</span>幅值100 A, 脉冲频率40 kHz, 占空比20%时, 接头抗拉强度和断后伸长率分别提高约22%和111%.","authors":[{"authorName":"从保强齐铂金周兴国罗军","id":"3e1554d6-5b9d-4386-b78a-485cd3f435df","originalAuthorName":"从保强齐铂金周兴国罗军"}],"categoryName":"|","doi":"","fpage":"1057","id":"b148dfcb-d3bd-4adf-9e30-8bf4843b1363","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":"4ddc6df3-589f-4639-9a6b-7c2231d5376a","keyword":"高强铝合金","originalKeyword":"高强铝合金"},{"id":"fc6ed784-36db-4b04-9680-11e00ada28e3","keyword":"ultrasonic pulse current","originalKeyword":"ultrasonic pulse current"},{"id":"a0a21681-3596-4f6a-a5ef-1bb2db5479a6","keyword":"variable polarity","originalKeyword":"variable polarity"},{"id":"1d0ae4df-c3a8-4356-9c33-8e1d9bf7e74e","keyword":"equiaxed<br />\nnon-dentrite","originalKeyword":"equiaxed<br />\nnon-dentrite"},{"id":"607b60a6-0046-4580-bc4f-65ae268d5f76","keyword":" mechanical property","originalKeyword":" mechanical property"}],"language":"zh","publisherId":"0412-1961_2009_9_17","title":"超音频脉冲<span style=\"color:red\">方波</span><span style=\"color:red\">电流</span>参数对2219铝合金焊缝组织和力学性能的影响","volume":"45","year":"2009"},{"abstractinfo":"采用新型超快速变换HPVP-TIG电弧焊接工艺进行2219-T87高强铝合金焊接,研究脉冲<span style=\"color:red\">电流</span>特征参数对焊接接头组织和力学性能的影响.结果表明,加入超音频脉冲<span style=\"color:red\">方波</span><span style=\"color:red\">电流</span>(UPSWC)作用后,铝合金焊缝区显微组织由粗大柱状晶转变为细小等轴晶,在焊缝区内除了等轴树枝晶外,还存在一种呈带状分布的极细小等轴非枝晶组织,同时焊缝熔合区宽度明显减小,焊接接头抗拉强度和断后伸长率显著提高.在一定范围内增加脉冲<span style=\"color:red\">电流</span>幅值,提高脉冲频率,减小占空比,可增强组织细化作用,提高接头力学性能.与未加入UPSWC作用相比,脉冲<span style=\"color:red\">电流</span>幅值100 A,脉冲频率40 kHz,占空比20%时,接头抗拉强度和断后伸长率分别提高约22%和111%.","authors":[{"authorName":"从保强","id":"3ab76e68-151a-49c9-a2c3-e58e2150d0cc","originalAuthorName":"从保强"},{"authorName":"齐铂金","id":"2fa26806-3637-4e5b-bed8-30124a3e5618","originalAuthorName":"齐铂金"},{"authorName":"周兴国","id":"b4c740db-97f5-4b5a-ac82-94fa1c60ba9a","originalAuthorName":"周兴国"},{"authorName":"罗军","id":"15fbcc9c-ccdf-4d1f-b2b2-26a6598b5aa4","originalAuthorName":"罗军"}],"doi":"10.3321/j.issn:0412-1961.2009.09.006","fpage":"1057","id":"5b222358-d0cf-4433-a2a6-534cec373141","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":"40949b92-fc81-4907-b6cf-3c6189bc3edb","keyword":"高强铝合金","originalKeyword":"高强铝合金"},{"id":"e9eb47bb-d206-4fb8-b44c-cacbc6a9ae46","keyword":"超音频脉冲<span style=\"color:red\">电流</span>","originalKeyword":"超音频脉冲电流"},{"id":"bce3d0e6-2c7d-4d54-9d24-d017327dd4a7","keyword":"变极性","originalKeyword":"变极性"},{"id":"a06ae261-1415-4c45-8e8c-8a751a317df5","keyword":"等轴非枝晶","originalKeyword":"等轴非枝晶"},{"id":"f273f341-31de-4c66-903f-cfdc970bbbd6","keyword":"力学性能","originalKeyword":"力学性能"}],"language":"zh","publisherId":"jsxb200909006","title":"超音频脉冲<span style=\"color:red\">方波</span><span style=\"color:red\">电流</span>参数对2219铝合金焊缝组织和力学性能的影响","volume":"45","year":"2009"},{"abstractinfo":"为了建立镀铬液Cr(Ⅵ)含量的快速测定方法,研究了Cr(Ⅵ)的电化学行为.在0.1 mol/L的氨水缓冲溶液(pH=10.0)中,Cr(Ⅵ)于-1.45 V(vs SCE)出现一灵敏的<span style=\"color:red\">方波</span>伏安峰,峰<span style=\"color:red\">电流</span>ip的高低与Cr(Ⅵ)的浓度在(0.1～2.0)×103mg/L范围内呈现良好的线性关系,由此建立了快速测定环境中Cr(Ⅵ)含量的<span style=\"color:red\">方波</span>伏安法.结果表明,此方法具有较高的分析测试准确性和灵敏度,方法的回归方程为ip(μA)=0.287 0+0.642 4C(mg/L),相关系数为0.988 6,检出限为0.05 mg/L Cr(Ⅵ),标准偏差为2.8%.该方法应用于实际样品电镀铬液及其废液中Cr(Ⅵ)含量的测定,结果满意.","authors":[{"authorName":"许琦","id":"4d5c324f-e03e-42fe-b807-ffb745c79c82","originalAuthorName":"许琦"},{"authorName":"严金龙","id":"e44a0fa4-3e43-4f2c-9eee-6866cedacfe9","originalAuthorName":"严金龙"}],"doi":"10.3969/j.issn.1001-1560.2004.06.020","fpage":"50","id":"ce62bdf3-9638-4a12-a2ae-0c2a15907f4b","issue":"6","journal":{"abbrevTitle":"CLBH","coverImgSrc":"journal/img/cover/CLBH.jpg","id":"7","issnPpub":"1001-1560","publisherId":"CLBH","title":"材料保护"},"keywords":[{"id":"d498282a-14f9-4458-8242-8c1a1c28b4cf","keyword":"<span style=\"color:red\">方波</span>伏安法","originalKeyword":"方波伏安法"},{"id":"74a7aecc-5f69-46f1-8246-97445aaa958a","keyword":"Cr(Ⅵ)","originalKeyword":"Cr(Ⅵ)"},{"id":"d7856066-2fdf-4502-b596-cb36125780ce","keyword":"废水","originalKeyword":"废水"}],"language":"zh","publisherId":"clbh200406020","title":"电镀液中Cr(Ⅵ)含量的<span style=\"color:red\">方波</span>伏安法测定","volume":"37","year":"2004"}],"totalpage":949,"totalrecord":9490}