Reid Vanessa R, McBrady Adam D, Synovec Robert E
Department of Chemistry, Box 351700, University of Washington, Seattle, WA 98195-1700, USA.
J Chromatogr A. 2007 May 4;1148(2):236-43. doi: 10.1016/j.chroma.2007.03.029. Epub 2007 Mar 16.
High-speed temperature programming is implemented via the direct resistive heating of the separation column (2.3m MXT-5 Silicosteel column with a 180 microm I.D. and a 0.4 microm 5% phenyl/95% dimethyl polysiloxane film). Resistive temperature programming was coupled with synchronized dual-valve injection (with an injection pulse width of 2 ms), producing a complete high-speed gas chromatography (GC) system. A comparison of isothermal and temperature programmed separations of seven n-alkanes (C(6) and C(8)-C(13)) shows a substantial improvement of peak width and peak capacity with temperature programming. The system was further implemented in separations of a mixture of analytes from various chemical classes. Separations of the n-alkane mixture using three different temperature programming rates are reported. A temperature programming rate as high as 240 degrees C/s is demonstrated. The method for determination of temperature programming rate, based on isothermal data, is discussed. The high-speed resistive column heating temperature programming resulted in highly reproducible separations. The highest rate of temperature programming (240 degrees C/s) resulted in retention time and peak width RSD, on average, of 0.5 and 1.4%, respectively, for the n-alkane mixture. This high level of precision was achieved with peak widths-at-half-height ranging from 13 to 36 ms, and retention times ranging from 147 to 444 ms (for n-hexane to n-tridecane).
高速程序升温通过对分离柱(2.3米长的MXT - 5硅钢柱,内径180微米,涂覆0.4微米厚的5%苯基/95%二甲基聚硅氧烷薄膜)进行直接电阻加热来实现。电阻程序升温与同步双阀进样(进样脉冲宽度为2毫秒)相结合,构成了一个完整的高速气相色谱(GC)系统。对七种正构烷烃(C(6)和C(8) - C(13))进行等温分离和程序升温分离的比较表明,程序升温能显著改善峰宽和峰容量。该系统进一步应用于分离来自各种化学类别的分析物混合物。报告了使用三种不同程序升温速率对正构烷烃混合物的分离情况。展示了高达240℃/秒的程序升温速率。讨论了基于等温数据测定程序升温速率的方法。高速电阻柱加热程序升温实现了高度可重现的分离。对于正构烷烃混合物,最高程序升温速率(240℃/秒)导致保留时间和峰宽的相对标准偏差(RSD)平均分别为0.5%和1.4%。在半高峰宽为13至36毫秒、保留时间为147至444毫秒(对于正己烷至正十三烷)的情况下实现了这种高精度水平。