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Abstract:Gas chromatography/atomic absorption spectroscopy(GC/AAS) is a good me
thod for the species analysis of organometallic compounds. But the traditi o nal
atomizers are not very suitable for this technology and all of them response
only to one kind of signal - the conc e ntration of the metallic atoms of the
ground state. They can not give any info r mation about the organic group of
organometallic compounds and organic compound s which coexist with the former.
For GC/AAS we want to design and manufacture a n ew kind of detector which is
much more sensitive and has a much smaller dead vol ume and will sensitively and
synchronousl y response to the atomization signal of organometallic compound and
ionization s ignal of organic compound. The authors have noticed that the
atomization of o r ganometallic compound and ionization of organic compound have
been existing in t he same hydrogen flame. The question is how to gain and
exchange and output the two signals which are completely different in
characters. For this purpose we de signed and manufactured a new type of
horizontal pipe mini-flame atomization an d ionization synchronous detector. The
key part is a T type glass tube (80 mm× 13 mm×10 mm i.d.) w hich covers
horizontally on the jet of the mini-flame atomizer and a long p i pe stainless
steel collector (70 mm×9.5 mm o.d.×9 mm i.d.) is tightly ins erted in the tube.
The light beam of the hollow cathode lamp passes through the hydroge n flame
along the axial center of the glass tube and the ground state metallic at o ms
in the flame diffuses to both ends of the tube along the axial center of the g
lass tube too. This process enriches the depth of the light absorption and then
increases the sensitivity of atomization. At the same time the long pipe collec
t or can enrich the collection efficiency of the ionization and increases the
sens itivity and widens the linear range. So the detector can synchronously and
sens itively detect the organometallic and organic compounds. The detection li
mit for atomization of the organometallic compound(diethylmercury) is
2.5×10-11g.s-1 and for
ionization of the organic compound (benzene) is
1.0×10-11g.s-1. The linear
range is 7.0×102 for atomization of diethylmercury (r=0.9 98 9) and 2
.5×105 for ionization of benzene (r=0.999
2). The selectivity of the detector t
o the organic solvent under the optimum operating condition of atomization i s
104-107. The relative standard deviation (RSD,n=11) of the
peak area in the optimum operating conditions of atomization for the
organometallic compound (die thylmercury) and of ionization for the organic
compound (benzene) is 1.8% and 1 .5% respectively. Under the same operating
condition, the atomization and the i onization can not reach the optimum
performance at the same time. If the atomiz a tion is in the optimum performance
state, the performance for ionization is like a chromatographic thermal
conductivity detector(TCD). The opti m um performance of the atomization and
ionization can be quickly adjusted by chan ging the flow rates of the
corresponding gases such as H2,N2 and
air. |
基金项目:河北省教委资助项目(项目批准号:97208) 作者简介:阎 正(1958-),男,副教授,硕士,电话:(0312)5079359 ,E-mail:yanzh@mail.hbu.edu.cn;乔玉卿(1971-),女,硕士,现在秦皇岛市燕山大学化 学院工作。 作者单位:阎正(河北大学化学系, 河北 保定 071002) 孙建民(河北大学化学系, 河北 保定 071002) 乔玉卿(河北大学化学系, 河北 保定 071002) 孙汉文(河北大学化学系, 河北 保定 071002) 参考文献: [1] HU Guang-lin,WANG Xiao-ru,YANG Fan-yuan. Journal of
Analytical Science,1998,14(2):170-175胡广林,王小如,杨梵原. 分析科学学报,
1998,14(2):170-175 |
原载于《色谱》2001 Vol.19 No.1 P.32-36
http://periodical.wanfangdata.com.cn/periodical/sp/sp2001/0101/0101ml.htm