Table 3.
Method | nc**a | tG (min) | ΔP (MPa) | Peak Width Based On | nc**/tGb | nc **/ΔPc | nc**/(tGΔP)d | |
---|---|---|---|---|---|---|---|---|
Carr 2006e | High temperature | 500 | 120 | 32 | Selected averagef | 4.2 | 15.8 | 7.9 |
Carr 2006e | High temperature | 440 | 120 | 32 | Averageg | 3.7 | 13.8 | 6.9 |
Carr 2006e | High temperature | 470 | 120 | 32 | Medianh | 3.9 | 14.6 | 7.3 |
Carr 2006e | High temperature | 1100 | 120 | 32 | Narrowesti | 9.5 | 35.7 | 17.9 |
Jorgenson 2003j | High pressure | 500 | 170 | 360 | Averageg | 2.9 | 1.4 | 0.5 |
Smith 2002k | High pressure | 1100 | 200 | 70 | Singlel | 5.5 | 15.7 | 4.7 |
Smith 2005m | High pressure | 1500 | 2000 | 140 | Averageg | 0.8 | 10.7 | 0.3 |
Smith 2005n | Monolith | 420 | 260 | 35 | Singlel | 1.6 | 12.0 | 2.8 |
Peak capacity (see section 2.4).
Peak capacity per unit time (peak per minute).
Peak capacity per unit pressure (peak per MPa).
Peak capacity per unit time per unit pressure (peak per hour MPa).
Results reported in [37] by using 60 cm long column with 5 μm pellicular particles.
Peak width is calculated using the average value of 30 selected peaks.
Peak width is calculated using the average value of all integrated peaks.
Peak width is calculated using the median value of all integrated peaks.
Peak width is calculated using the narrowest value of all integrated peaks.
Results reported by Jorgenson et al. [54] by using 38 cm long column with 1 μm nonporous porous particles.
Results reported by Smith et al. [55] by using 87 cm long column with 3 μm fully porous particles.
Peak width is calculated using the peak width of a single peak.
Results reported by Smith et al. [56] by using 200 cm long column with 3 μm fully porous particles.
Results reported by Smith et al. [57] by using 70 cm long silica monolith column.