共查询到19条相似文献,搜索用时 159 毫秒
1.
电感耦合等离子发射光谱法用于植物油多元素同步测定研究 总被引:2,自引:0,他引:2
用全谱直读电感耦合等离子体发射光谱法同步测定了植物油中的铁、铜、钴、镍、铅、铝、锌、镉、铬、锰和镁11种金属元素,考察了硫酸炭化灰化法、硝酸炭化灰化法、微波消解法、活性炭炭化灰化法以及燃烧炭化灰化法五种样品前处理方法对测定结果的影响,最后采用硫酸炭化灰化法处理样品,在0.1和0.5 mg·kg-1两个浓度水平对实际样品加标的平均回收率为70.4%~113%,相对标准偏差1.01%~10.6%,11种元素的方法检出限在0.1~3.6 μg·kg-1之间。方法应用于豆油、花生油、芝麻油、菜籽油、茶油、精炼油、调和油等植物油样品中11种金属元素的测定,结果令人满意。 相似文献
2.
3.
4.
5.
用ICP-AES方法测定淀粉中铅、砷的含量 总被引:4,自引:3,他引:1
采用ICP-AES(电感耦合等离子体发射光谱)法,以硝酸镍作为基体改进剂,对淀粉中的铅、砷含量进行了测定;探讨了样品灰化方法及灰化原子化温度、基体改进剂对测定结果的影响.实验结果表明,用ICP-AES方法测定淀粉样品中铅、砷一类有害重金属含量,数据、结果的重现性好,方法简便易行、测定结果准确. 相似文献
6.
7.
8.
植物标样多元素测定的五种前处理方法比较 总被引:22,自引:1,他引:21
本文采用植物样品的五种前处理方法,即干灰化法,硝酸+硫酸+高氯酸法,硝酸+硫酸+高氯酸+氢氟酸法、硫酸+过氧化氢法、灰化+碱熔法,对植物标样GBW07603作样品分解,试液用ICP-AES法进行十九种常量及微量元素的测定。 相似文献
9.
以云南文山三七为材料,分析研究了用干法灰化、湿法消解前处理样品对原子吸收光谱法测定三七中重金属C r含量的影响,方法的相关系数为0.9993,干法灰化回收率为95.02%,湿法消解回收率为93.03%,分析结果满意。结果表明,干法灰化的最佳条件为灰化温度500—600℃、灰化时间6—8h。湿法消解的最佳消解体系为HNO3:HC lO4(V/V)=4:1体系。用干法灰化或常压下湿法消解处理样品,原子吸收光谱法可以准确测定三七中重金属C r含量,且方法简单、快捷。云南文山三七粉中重金属C r含量为1.8178μg/g。 相似文献
10.
乳化技术-火焰原子吸收光谱法测定原油中的铁镍 总被引:10,自引:0,他引:10
以Triton X-100为乳化剂将样品的甲基异丁基酮-二甲苯溶液乳化成乳浊液,以聚异丁烯空白溶液为参比,用标准加入法测定。建立了乳化技术-火焰原子吸收光谱法测定原油中铁、镍的快速分析方法。提出了配制空白溶液的原理及方法,对溶剂及乳化剂的选择、空白溶液的配制进行了考察,测定结果与灰化法一致。 相似文献
11.
12.
13.
14.
分别采用干灰化法和HNO3-HClO4混合酸消解法消解鸡血藤样品,参考其他中药材火焰原子吸收法的测定方法,用火焰原子吸收光谱法测定了桂西南产鸡血藤中K、Na、Ca、Mg、Mn、Cu、Fe金属元素的含量。研究了不同消解方法对测定金属元素含量的影响、仪器的最佳工作条件、干扰消除情况,并作了方法的准确度和精密度考察。干法消解的加标回收率在97.5%—100.8%之间,RSD2.18%—4.17%(n=6);湿法消解回收率在97.1%—101.3%之间,RSD1.02%—3.74%(n=6)。干法消解测定的7种金属元素含量稍低于湿法消解测定的含量。文章为鸡血藤多种金属元素含量的测定提供了可靠的方法,为进一步解释鸡血藤的功能作用和开发鸡血藤的药用价值提供理论依据。 相似文献
15.
火焰原子吸收光谱法测定冬枣中的铁和锌 总被引:2,自引:0,他引:2
采用干法消解、湿法消解和非完全消解法3种方法多种体系处理冬枣样品,应用火焰原子吸收光谱法测定冬枣中铁和锌的含量.在选定的条件下,铁、锌的样品加标回收率在100.0%-101.3%之间,精密度(样品相对标准偏差RSD)均小于1.1%(n=11).实验结果表明,湿法消解和非完全消解法的测定结果相差不大.其中非完全消解法简便、快捷,测定结果准确,更适用于冬枣中铁和锌的测定. 相似文献
16.
17.
Noise control is important and essential in factory, where the noise level is restricted by the Occupational Safety and Health Act. Before noise abatement being performed, the identification work in searching for the location and sound power level (SWL) of noisy sound sources is absolutely prerequisite. Several researches on new techniques of single noise control have been well addressed and developed; however, the research work on sound identification for the existing multi-noise plant is hardly found sufficient. Under the circumstance of unrecognized noises, the noise control work will expectedly be extravagant and fruitless. Therefore, the numerical approach in distinguishing noises from a multi-noise plant becomes crucial and obligatory.In this paper, the novel technique of genetic algorithm (GA) in conjunction with the method of minimized variation square will be adopted and used in the following numerical optimization. In addition, various sound monitoring systems in detecting the noise condition within the plant area will also be introduced. Before noises identification, the accuracy of mathematical model has then been proved to be in good agreements comparing to the simulated data of SoundPlan, a commercialized simulation package in sound field. Moreover, three kinds of multi-noise plants have been fully discussed and acknowledged by GA optimization. The results reveal that the relevant locations and sound power levels (SWLs) of noises can be precisely recognized. This paper surely provides a rapid methodology in the noise identification work for a multi-noise plant. 相似文献
18.
Threshold and saturation properties of the field-induced twist cell with two parameters weak anchoring boundaries 下载免费PDF全文
On the basis of two-parameter formula of weak surface coupling anchoring
energy of nematic liquid crystals proposed by Zhao et al recently, the general
torque equilibrium equation and boundary conditions of the director have
been obtained and the threshold field as well as the saturation field of the
field-induced twist cell have been analysed for three kinds of
configurations, i.e. homogeneous, splay and Pi cells formed by
different rubbing conditions and pretilt angles. The results
indicated that the polar anchoring has no effect on the threshold field. It
is determined only by the twist anchoring and pretilt angle. But, the polar
anchoring and twist anchoring are coupling with each other and have a great
influence on the saturation field. The formulae for calculating the
threshold field and saturation field are given. These results will be very
useful in understanding surface physics and the design of liquid crystal
cells. 相似文献