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填充新型1.9μm全多孔泰坦-C18颗粒的色谱柱实现最佳效率的原理——颗粒内扩散率的详细研究

The rationale for the optimum efficiency of columns packed with new 1.9μm fully porous Titan-C18 particles-a detailed investigation of the intra-particle diffusivity.

作者信息

Gritti Fabrice, Guiochon Georges

机构信息

Department of Chemistry, University of Tennessee, Knoxville, TN 37996-1600, USA.

Department of Chemistry, University of Tennessee, Knoxville, TN 37996-1600, USA.

出版信息

J Chromatogr A. 2014 Aug 15;1355:164-78. doi: 10.1016/j.chroma.2014.05.076. Epub 2014 Jun 11.

Abstract

In a previous report, it was reported that columns packed with fully porous 1.9μm Titan-C18 particles provided a minimum reduced plate height as small as 1.7 for the most retained compound (n-octanophenone) under RPLC conditions. These particles are characterized by a relatively narrow size distribution with a relative standard deviation (RSD) of only 10%. A column packed with classical 5μm Symmetry-C18 particles, used as a reference RPLC column, generated a minimum reduced plate height of 2.1 for the same retained compound. This work demonstrates that this was due to an unusually low intra-particle diffusivity across these particles, which leads to a small longitudinal diffusion coefficient along the column. The demonstration is based on the combination of accurate measurements of the height equivalent to a theoretical plate (HETP), inverse size exclusion chromatography (ISEC), peak parking (PP), and minor disturbance method (MDM) experiments. The experimental results show that the reduced eddy dispersion HETP term (A=0.8 for a reduced velocity of 5), the internal particle porosity (ϵp=0.35), and the enrichment of acetonitrile in the pore volume (75% acetonitrile in the bulk, 85% inside the mesoporous volume) are identical on both the Titan-C18 and Symmetry-C18 columns. The difference between the internal structures of these two brands of RPLC-C18 fully porous particles lies in the values of the internal obstruction factor γp, which is 0.42 for the Symmetry-C18 but only 0.26 for the Titan-C18 particles. This is in part related to the diffusion hindrance due to the small average pore size of the Titan-C18 particles, around 59Å versus 77Å for Symmetry-C18 particles. A simple model of constriction along diffusion paths having the shape of a truncated cone suggests that the width of the pore size distribution (RSD of 30% and 20% for Titan-C18 and Symmetry-C18 particles) is mostly responsible for the difference in their obstruction factors.

摘要

在之前的一份报告中,据报道,在反相液相色谱(RPLC)条件下,填充完全多孔的1.9μm泰坦-C18颗粒的色谱柱对于保留时间最长的化合物(正辛基苯乙酮)提供了低至1.7的最小折合板高。这些颗粒的特点是粒径分布相对较窄,相对标准偏差(RSD)仅为10%。填充经典5μm对称-C18颗粒的色谱柱用作参考RPLC柱,对于相同的保留化合物产生的最小折合板高为2.1。这项工作表明,这是由于这些颗粒间异常低的颗粒内扩散率,这导致沿色谱柱的纵向扩散系数较小。该论证基于对理论塔板高度(HETP)的精确测量、反相尺寸排阻色谱(ISEC)、峰停驻(PP)和微扰法(MDM)实验的结合。实验结果表明,在折合流速为5时,折合涡流扩散HETP项(A = 0.8)、颗粒内部孔隙率(ϵp = 0.35)以及孔体积中乙腈的富集情况(本体中75%乙腈,中孔体积内85%乙腈)在泰坦-C18和对称-C18色谱柱上是相同的。这两种品牌的RPLC-C18完全多孔颗粒内部结构的差异在于内部阻碍因子γp的值,对称-C18颗粒的γp为0.42,而泰坦-C18颗粒仅为0.26。这部分与泰坦-C18颗粒平均孔径较小导致的扩散阻碍有关,泰坦-C18颗粒平均孔径约为59Å,而对称-C18颗粒为77Å。一个沿具有截头圆锥形状的扩散路径收缩的简单模型表明,孔径分布宽度(泰坦-C18和对称-C18颗粒的RSD分别为30%和20%)主要导致了它们阻碍因子的差异。

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