Mass transfer mechanism in hydrophilic interaction chromatography
•The mass transfer mechanism in HILIC columns was investigated in depth.•The overall HETP depends weakly on the retention factor of the analyte.•The longitudinal diffusion HETP is governed by pore diffusivity only.•The eddy dispersion term accounts for at least 70% of the whole band broadening.•Unli...
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Published in: | Journal of Chromatography A Vol. 1302; pp. 55 - 64 |
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Abstract | •The mass transfer mechanism in HILIC columns was investigated in depth.•The overall HETP depends weakly on the retention factor of the analyte.•The longitudinal diffusion HETP is governed by pore diffusivity only.•The eddy dispersion term accounts for at least 70% of the whole band broadening.•Unlike in RPLC, column border effects cannot be concealed in HILIC.
The mass transfer mechanism in HILIC was investigated in depth. The reduced heights equivalent to a theoretical plate (HETP) of five low molecular weigh compounds with retention factors of −0.05 (slight exclusion from the surface due to the presence of a water-rich layer in which naphthalene is insoluble) to 3.64 were measured at room temperature for a 4.6mm×100mm column packed with 3.5μm 140Å XBridge HILIC particles in a wide range of flow velocities. The mobile phase was a buffered acetonitrile–water mixture (92.5/7.5, v/v). Using a physically reliable model of effective diffusion in binary composite media (Torquato's model), the longitudinal diffusion and solid–liquid mass transfer resistance reduced HETP terms were measured. The reduced short-range eddy dispersion HETP was taken from the literature data. The long-range reduced HETP was directly measured from the subtraction of these HETP terms to the overall HETP measured from moment analysis. In contrast to RPLC, the plots of the reduced HETP versus the reduced velocity depend weakly on the retention factor, due to the constant, low intra-particle diffusivity observed in HILIC. So, the reduced longitudinal diffusion HETP is smaller and the reduced solid–liquid mass transfer resistance HETP is larger in HILIC than in RPLC. Whereas border effects can be concealed in RPLC for retained analytes due to fast radial equilibration across the column diameter, a residual long-range eddy dispersion term persists in 4.6mm I.D. HILIC columns, even at very slow flow rates. Experiments show that the minor differences in the long-range eddy dispersion term between analytes having different retention factors is directly correlated to the reciprocal of their bulk diffusion coefficient. The performance of HILIC columns packed with fine particles is then more sensitive to the inlet sample distribution and to the outlet sample collection than RPLC columns due to the relatively poor radial mixing controlled by lateral diffusion. |
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AbstractList | •The mass transfer mechanism in HILIC columns was investigated in depth.•The overall HETP depends weakly on the retention factor of the analyte.•The longitudinal diffusion HETP is governed by pore diffusivity only.•The eddy dispersion term accounts for at least 70% of the whole band broadening.•Unlike in RPLC, column border effects cannot be concealed in HILIC.
The mass transfer mechanism in HILIC was investigated in depth. The reduced heights equivalent to a theoretical plate (HETP) of five low molecular weigh compounds with retention factors of −0.05 (slight exclusion from the surface due to the presence of a water-rich layer in which naphthalene is insoluble) to 3.64 were measured at room temperature for a 4.6mm×100mm column packed with 3.5μm 140Å XBridge HILIC particles in a wide range of flow velocities. The mobile phase was a buffered acetonitrile–water mixture (92.5/7.5, v/v). Using a physically reliable model of effective diffusion in binary composite media (Torquato's model), the longitudinal diffusion and solid–liquid mass transfer resistance reduced HETP terms were measured. The reduced short-range eddy dispersion HETP was taken from the literature data. The long-range reduced HETP was directly measured from the subtraction of these HETP terms to the overall HETP measured from moment analysis. In contrast to RPLC, the plots of the reduced HETP versus the reduced velocity depend weakly on the retention factor, due to the constant, low intra-particle diffusivity observed in HILIC. So, the reduced longitudinal diffusion HETP is smaller and the reduced solid–liquid mass transfer resistance HETP is larger in HILIC than in RPLC. Whereas border effects can be concealed in RPLC for retained analytes due to fast radial equilibration across the column diameter, a residual long-range eddy dispersion term persists in 4.6mm I.D. HILIC columns, even at very slow flow rates. Experiments show that the minor differences in the long-range eddy dispersion term between analytes having different retention factors is directly correlated to the reciprocal of their bulk diffusion coefficient. The performance of HILIC columns packed with fine particles is then more sensitive to the inlet sample distribution and to the outlet sample collection than RPLC columns due to the relatively poor radial mixing controlled by lateral diffusion. The mass transfer mechanism in HILIC was investigated in depth. The reduced heights equivalent to a theoretical plate (HETP) of five low molecular weigh compounds with retention factors of −0.05 (slight exclusion from the surface due to the presence of a water-rich layer in which naphthalene is insoluble) to 3.64 were measured at room temperature for a 4.6mm×100mm column packed with 3.5μm 140Å XBridge HILIC particles in a wide range of flow velocities. The mobile phase was a buffered acetonitrile–water mixture (92.5/7.5, v/v). Using a physically reliable model of effective diffusion in binary composite media (Torquato's model), the longitudinal diffusion and solid–liquid mass transfer resistance reduced HETP terms were measured. The reduced short-range eddy dispersion HETP was taken from the literature data. The long-range reduced HETP was directly measured from the subtraction of these HETP terms to the overall HETP measured from moment analysis. In contrast to RPLC, the plots of the reduced HETP versus the reduced velocity depend weakly on the retention factor, due to the constant, low intra-particle diffusivity observed in HILIC. So, the reduced longitudinal diffusion HETP is smaller and the reduced solid–liquid mass transfer resistance HETP is larger in HILIC than in RPLC. Whereas border effects can be concealed in RPLC for retained analytes due to fast radial equilibration across the column diameter, a residual long-range eddy dispersion term persists in 4.6mm I.D. HILIC columns, even at very slow flow rates. Experiments show that the minor differences in the long-range eddy dispersion term between analytes having different retention factors is directly correlated to the reciprocal of their bulk diffusion coefficient. The performance of HILIC columns packed with fine particles is then more sensitive to the inlet sample distribution and to the outlet sample collection than RPLC columns due to the relatively poor radial mixing controlled by lateral diffusion. The mass transfer mechanism in HILIC was investigated in depth. The reduced heights equivalent to a theoretical plate (HETP) of five low molecular weigh compounds with retention factors of a0.05 (slight exclusion from the surface due to the presence of a water-rich layer in which naphthalene is insoluble) to 3.64 were measured at room temperature for a 4.6 mm A 100 mm column packed with 3.5 mu m 140 A XBridge HILIC particles in a wide range of flow velocities. The mobile phase was a buffered acetonitrileawater mixture (92.5/7.5, v/v). Using a physically reliable model of effective diffusion in binary composite media (Torquato's model), the longitudinal diffusion and solid-liquid mass transfer resistance reduced HETP terms were measured. The reduced short-range eddy dispersion HETP was taken from the literature data. The long-range reduced HETP was directly measured from the subtraction of these HETP terms to the overall HETP measured from moment analysis. In contrast to RPLC, the plots of the reduced HETP versus the reduced velocity depend weakly on the retention factor, due to the constant, low intra-particle diffusivity observed in HILIC. So, the reduced longitudinal diffusion HETP is smaller and the reduced solid-liquid mass transfer resistance HETP is larger in HILIC than in RPLC. Whereas border effects can be concealed in RPLC for retained analytes due to fast radial equilibration across the column diameter, a residual long-range eddy dispersion term persists in 4.6 mm I.D. HILIC columns, even at very slow flow rates. Experiments show that the minor differences in the long-range eddy dispersion term between analytes having different retention factors is directly correlated to the reciprocal of their bulk diffusion coefficient. The performance of HILIC columns packed with fine particles is then more sensitive to the inlet sample distribution and to the outlet sample collection than RPLC columns due to the relatively poor radial mixing controlled by lateral diffusion. The mass transfer mechanism in HILIC was investigated in depth. The reduced heights equivalent to a theoretical plate (HETP) of five low molecular weigh compounds with retention factors of -0.05 (slight exclusion from the surface due to the presence of a water-rich layer in which naphthalene is insoluble) to 3.64 were measured at room temperature for a 4.6mm×100mm column packed with 3.5μm 140Å XBridge HILIC particles in a wide range of flow velocities. The mobile phase was a buffered acetonitrile-water mixture (92.5/7.5, v/v). Using a physically reliable model of effective diffusion in binary composite media (Torquato's model), the longitudinal diffusion and solid-liquid mass transfer resistance reduced HETP terms were measured. The reduced short-range eddy dispersion HETP was taken from the literature data. The long-range reduced HETP was directly measured from the subtraction of these HETP terms to the overall HETP measured from moment analysis. In contrast to RPLC, the plots of the reduced HETP versus the reduced velocity depend weakly on the retention factor, due to the constant, low intra-particle diffusivity observed in HILIC. So, the reduced longitudinal diffusion HETP is smaller and the reduced solid-liquid mass transfer resistance HETP is larger in HILIC than in RPLC. Whereas border effects can be concealed in RPLC for retained analytes due to fast radial equilibration across the column diameter, a residual long-range eddy dispersion term persists in 4.6mm I.D. HILIC columns, even at very slow flow rates. Experiments show that the minor differences in the long-range eddy dispersion term between analytes having different retention factors is directly correlated to the reciprocal of their bulk diffusion coefficient. The performance of HILIC columns packed with fine particles is then more sensitive to the inlet sample distribution and to the outlet sample collection than RPLC columns due to the relatively poor radial mixing controlled by lateral diffusion. |
Author | Guiochon, Georges Gritti, Fabrice |
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Keywords | Mass transfer mechanism RPLC Solid–liquid mass transfer resistance Intra-particle diffusivity Longitudinal diffusion Eddy dispersion HILIC Peak resolution Hydrophilic Interaction Liquid chromatography Solid―liquid mass transfer resistance HPLC chromatography Theoretical study Retention factor Diffusivity Mechanism Mass transfer Transport process Reversed phase chromatography Plate efficiency Height equivalent to a theoretical plate Diffusion |
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1216 Gritti (10.1016/j.chroma.2013.06.001_bib0160) 2010; 1217 Gritti (10.1016/j.chroma.2013.06.001_bib0190) 2011; 57 Gritti (10.1016/j.chroma.2013.06.001_bib0100) 2012; 1221 Giddings (10.1016/j.chroma.2013.06.001_bib0110) 1965 Clark (10.1016/j.chroma.2013.06.001_bib0270) 1970 Alpert (10.1016/j.chroma.2013.06.001_bib0005) 1990; 499 McCalley (10.1016/j.chroma.2013.06.001_bib0055) 2008; 1192 Gritti (10.1016/j.chroma.2013.06.001_bib0255) 2013; 1280 Melnikov (10.1016/j.chroma.2013.06.001_bib0035) 2012; 51 Gritti (10.1016/j.chroma.2013.06.001_bib0260) 2006; 78 Dorsey (10.1016/j.chroma.2013.06.001_bib0075) 1989; 89 Ikegami (10.1016/j.chroma.2013.06.001_bib0015) 2008; 1184 Gritti (10.1016/j.chroma.2013.06.001_bib0105) 2013; 85 Horvath (10.1016/j.chroma.2013.06.001_bib0065) 1976; 125 Gritti (10.1016/j.chroma.2013.06.001_bib0155) 2010; 56 Gritti (10.1016/j.chroma.2013.06.001_bib0060) 2013; 1297 Jandera (10.1016/j.chroma.2013.06.001_bib0020) 2011; 692 Gunn (10.1016/j.chroma.2013.06.001_bib0135) 1969; 47 Knox (10.1016/j.chroma.2013.06.001_bib0215) 1964; 36 Vailaya (10.1016/j.chroma.2013.06.001_bib0070) 1998; 829 Torquato (10.1016/j.chroma.2013.06.001_bib0180) 2002 Melnikov (10.1016/j.chroma.2013.06.001_bib0030) 2011; 83 Miyabe (10.1016/j.chroma.2013.06.001_bib0230) 2009; 1216 Hemstrom (10.1016/j.chroma.2013.06.001_bib0010) 2006; 29 Gritti (10.1016/j.chroma.2013.06.001_bib0240) 2011; 1218 Guiochon (10.1016/j.chroma.2013.06.001_bib0175) 2006 Gritti (10.1016/j.chroma.2013.06.001_bib0185) 2011; 66 Li (10.1016/j.chroma.2013.06.001_bib0210) 1997; 69 Khirevich (10.1016/j.chroma.2013.06.001_bib0145) 2010; 1217 Daneyko (10.1016/j.chroma.2013.06.001_bib0165) 2011; 1218 Lindsey (10.1016/j.chroma.2013.06.001_bib0265) 2013; 1287 Daneyko (10.1016/j.chroma.2013.06.001_bib0170) 2012; 1257 Knox (10.1016/j.chroma.2013.06.001_bib0220) 1983; 282 Stevenson (10.1016/j.chroma.2013.06.001_bib0250) 2013; 36 Gritti (10.1016/j.chroma.2013.06.001_bib0225) 2006; 61 Kubin (10.1016/j.chroma.2013.06.001_bib0130) 1965; 30 Gunn (10.1016/j.chroma.2013.06.001_bib0150) 1971; 49 Stevenson (10.1016/j.chroma.2013.06.001_bib0245) 2011; 1218 Gritti (10.1016/j.chroma.2013.06.001_bib0115) 2011; 1218 |
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Snippet | •The mass transfer mechanism in HILIC columns was investigated in depth.•The overall HETP depends weakly on the retention factor of the analyte.•The... The mass transfer mechanism in HILIC was investigated in depth. The reduced heights equivalent to a theoretical plate (HETP) of five low molecular weigh... |
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SubjectTerms | Analytical chemistry Chemistry Chromatographic methods and physical methods associated with chromatography Chromatography Chromatography, Liquid - methods Column packings Diffusion diffusivity Dispersions Eddies Eddy dispersion edge effects Exact sciences and technology HILIC hydrophilic interaction chromatography Hydrophobic and Hydrophilic Interactions Intra-particle diffusivity Longitudinal diffusion Longitudinal Studies Marine Mass transfer Mass transfer mechanism Mathematical models mixing Models, Theoretical Molecular Weight naphthalene Other chromatographic methods Particulate composites RPLC Solid–liquid mass transfer resistance temperature |
Title | Mass transfer mechanism in hydrophilic interaction chromatography |
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