Shu-ying Han*,
Hui-min Yu,
Yu-qiong Pei and
Yu-mei Chi*
College of Pharmacy, Nanjing University of Chinese Medicine, 138 Xianlin Avenue, Nanjing 210023, China. E-mail: njutcmhsy@163.com; ymchii@njutcm.edu.cn; Tel: +86-25-85811053
First published on 16th July 2015
The effect of changes in column temperature on the van't Hoff equation, as well as the relationship between separation efficiency and column temperature in high performance liquid chromatography (HPLC) by using different stationary phases, have been discussed and compared in this paper. For this purpose, six flavonoid glycosides were selected to establish van't Hoff equations on C18, cholesterol, C8 and porous polymer octadecyl bonded (ODP) stationary phases. The results indicated that, for all the columns, the changes in phase ratio arising from the varying column temperatures had no significant impact on the linearity of the van't Hoff equation, however, it indeed led to certain errors in the intercept (change in entropy, ΔS0) and slope (change in enthalpy, ΔH0) of the equation, which are considered to be important parameters in illuminating the chromatographic mechanism in HPLC. Thereby, a new protocol has been proposed in this paper to correct these errors, with the aim of offering solid data for ΔS0 and ΔH0. Furthermore, a relationship relating selectivity and column temperature was deduced in theory, and then validated by using the six flavonoid glycosides in this work. This relationship has been applied to predict the separation of six steroid hormones in HPLC with high consistency between experimental and predicted selectivity factors (average relative errors less than 2.2%, 1.0%, 6.1% and 5.1% for C18, cholesterol, C8 and ODP columns, respectively). The proposed new strategy in predicting selectivity greatly facilitates optimization processes for HPLC by avoiding tedious condition experiments, and furthermore, column temperature is proposed to be involved in the optimization processes as an important parameter, making separation of structural analogues effective. In this temperature-involved optimization method, a stationary phase sensitive to temperature change, i.e. cholesterol, is recommended.
This situation, however, is changing gradually because novel stationary phases have been emerging in recent years. Some thermally stable phase materials, such as graphitized carbon types, zirconium oxide based phases and polystyrene/divinylbenzene copolymers have been used in HPLC,11,12 which can greatly expand the available temperature range even up to over 100 °C. But these stationary phases usually show lower separation efficiency than the silica-based column materials.11 In consequence, column materials sensitive to the temperature changes, for instance, recently developed cholesterol bonded-silica stationary phase, is another promising alternative, as tiny temperature changes may have appreciable impact on retention, efficiency, and selectivity on HPLC.13,14
In an HPLC separation, the mechanism can be described as the increasing temperature alters analyte retention by changing the free energy between the analyte and the stationary phase, which can be depicted using van't Hoff equation, commonly presented as the dependence of retention factor (k) on temperature (T). In van't Hoff equation, the phase ratio (β) is always regarded as a constant over the experimental temperature range.15,16 In fact, the influence of change in temperature on the mobile phase volume is obviously greater than that on the stationary phase volume, which may give rise to variation in β under different temperatures. Nevertheless, no researches involved in van't Hoff equation took this change into careful consideration as far as our knowledge goes. Moreover, almost all the published studies only focused on using van't Hoff equation to interpret retention behavior and mechanism of small molecules on various columns at different temperatures,17–23 but few report was aimed to improve selectivity of temperature-programmed HPLC method, let alone making reliable prediction for separation tendency on the basis of van't Hoff equation.
Accordingly, it is the purpose of this paper to evaluate the effect of phase ratio differing in various temperatures on van't Hoff equation, and proposed a new protocol to correct the errors in enthalpy and entropy resulting from this effected van't Hoff equation. Furthermore, a novel relationship based on the selectivity and column temperature was deduced theoretically and validated by using homologous flavonoid glycosides. This relationship was then applied to predict the selectivity of C18, cholesterol, C8 and porous polymer octadecyl bonded (ODP) stationary phases for structurally analogous estrogens under different temperatures.
ΔG0 = ΔH0 − TΔS0 = −RT![]() ![]() | (1) |
![]() | (2) |
Since K equals k × β, eqn (2) becomes
![]() | (3) |
![]() | (4) |
Therefore, the dependence of k on column temperature called van't Hoff equation is given
![]() | (5) |
In general, if a single mechanism controls the retention over the experimental temperature range, lnk versus 1/T plots should be linear.27 By plotting ln
k with 1/T, the enthalpic and entropic contributions to the chromatographic retention can be calculated: −ΔH0 from the slope, and ΔS0 from the intercept of the plot. However, as mentioned above, the intercept of eqn (5), Ai, is not a definite constant due to the uncertainty of β invariable over the experimental temperature range, which may exert an influence on the ln
k versus 1/T plot. On the contrary, it is observed that ln
K is explicitly linear with 1/T as described in eqn (2), and K can be calculated through eqn (3) by k and β measured at different temperatures, which means establishment of ln
K versus 1/T linear plot is more rational because it can effectively avoid the possible errors arising from changed β existing in ln
k versus 1/T plot.
In HPLC, the selectivity factor (α) is usually represented as
![]() | (6) |
The change in α between two adjacent solutes with temperature can be derived by substituting eqn (2) into (6)
![]() | (7) |
Based on eqn (7), the selectivity of column at arbitrary temperature can be predicted by the fitted parameters, ΔH0 and ΔS0 obtained from the linear lnK versus 1/T plot of eqn (2).
Flavonoid glycosides such as flavonoid glycosides I, II, III, IV, V and VI used as the training set were all laboratory-made. Estrogens, i.e. estriol (E3), 17β-estradiol (17β-E2), 17α-estradiol (17α-E2), ethinyl estradiol (EE), estrone (E1) and progesterone (P4) used as the test set were purchased from the National Institute for the Control of Pharmaceutical and Biological Products (Beijing, China).
![]() | (8) |
Although the form of eqn (8) is just the same as van't Hoff equation, the physical significance of the slope and intercept are both totally different, that is, the intercept and slope of the classical van't Hoff equation cannot truly express ΔH0 and ΔS0 in a chromatographic process. On the contrary, since it makes no assumptions about the fixed quantity of β at different temperatures, the slope and intercept of eqn (2) truly reflect ΔH0 and ΔS0 values in the chromatographic process because lnK was calculated by k and β measured at each temperature through eqn (3). The experimental ln
k, as well as ln
K of six flavonoid glycosides, were respectively plotted against 1/T on C18, cholesterol, C8 and ODP columns, and the fitting parameters are shown in Table 1. It can be seen from Table 1 that, although the straight line seemed to fit the data well when ln
k was plotted against 1/T, the slope and intercept were markedly different from those of ln
K–1/T plot due to the additional items a and b respectively involved in intercept and slope in eqn (8). The relative errors of k-related and K-related ΔH0 (2.8–3.3% for C18, about 0.9% for cholesterol, 4.4–5.5% for C8 and 11.5–17.4% for ODP, respectively), as well as the errors of ΔS0 (2.8–3.4% for C18, 3.6–4.1% for cholesterol, 2.7–3.6% for C8 and 21.5%–28.3% for ODP, respectively) are listed in Table 1, revealing the inaccuracy of conventional van't Hoff equation in acquiring ΔH0 and ΔS0, while it is suggested that the solid and accurate ΔH0 and ΔS0 data should be obtained through eqn (2) and (3). For ODP column, the errors of ΔH0 and ΔS0 were more significant than others, which may be attributed to the large values of intercept and slope of the ln
β–1/T plot shown in Fig. 1(d), which means temperature has much more influence on β for ODP stationary phase.
ln![]() |
ln![]() |
RE (ΔS) (%) | RE (ΔH) (%) | |||||||||
---|---|---|---|---|---|---|---|---|---|---|---|---|
Intercept | Slope | R2 | ΔS0 (J) | −ΔH0 (KJ) | Intercept | Slope | R2 | ΔS0 (J) | −ΔH0 (KJ) | |||
a ![]() |
||||||||||||
C18 | ||||||||||||
I | −11.21 ± 0.22 | 4340.4 ± 70.0 | 0.9992 | −93.22 | 36![]() |
−11.39 ± 0.22 | 4204.5 ± 67.5 | 0.9992 | −95.97 | 34![]() |
3.0 | 3.1 |
II | −10.00 ± 0.18 | 4026.1 ± 55.4 | 0.9994 | −83.18 | 33![]() |
−10.18 ± 0.15 | 3890.9 ± 47.9 | 0.9996 | −85.96 | 32![]() |
3.3 | 3.4 |
III | −11.36 ± 0.18 | 4495.3 ± 55.2 | 0.9996 | −94.48 | 37![]() |
−11.54 ± 0.15 | 4360.1 ± 47.6 | 0.9996 | −97.26 | 36![]() |
2.9 | 3.0 |
IV | −11.12 ± 0.30 | 4420.7 ± 93.1 | 0.9987 | −92.45 | 36![]() |
−11.29 ± 0.28 | 4282.7 ± 88.1 | 0.9987 | −95.15 | 35![]() |
2.9 | 3.1 |
V | −10.75 ± 0.25 | 4416.1 ± 78.5 | 0.9991 | −89.34 | 36![]() |
−10.91 ± 0.23 | 4278.1 ± 72.3 | 0.9991 | −92.04 | 35![]() |
3.0 | 3.1 |
VI | −12.00 ± 0.26 | 4768.1 ± 80.5 | 0.9992 | −99.73 | 39![]() |
−12.18 ± 0.24 | 4634.9 ± 73.8 | 0.9992 | −102.55 | 38![]() |
2.8 | 2.8 |
![]() |
||||||||||||
Cholesterol | ||||||||||||
I | −12.90 ± 0.04 | 4824.6 ± 12.7 | 0.9999 | −107.25 | 40![]() |
−12.93 ± 0.07 | 4638.8 ± 21.5 | 0.9999 | −108.23 | 38![]() |
0.9 | 3.9 |
II | −11.81 ± 0.02 | 4512.7 ± 6.2 | 0.9999 | −98.19 | 37![]() |
−11.84 ± 0.05 | 4326.7 ± 15.2 | 0.9999 | −99.16 | 35![]() |
0.9 | 4.1 |
III | −12.98 ± 0.04 | 4920.9 ± 13.0 | 0.9999 | −107.91 | 40![]() |
−13.01 ± 0.07 | 4734.7 ± 21.9 | 0.9999 | −108.87 | 39![]() |
0.9 | 3.8 |
IV | −12.49 ± 0.01 | 4793.1 ± 1.9 | 1.0000 | −103.87 | 39![]() |
−12.52 ± 0.04 | 4607.0 ± 11.2 | 0.9999 | −104.83 | 38![]() |
0.9 | 3.9 |
V | −12.15 ± 0.03 | 4743.4 ± 7.9 | 0.9999 | −101.03 | 39![]() |
−12.18 ± 0.05 | 4557.3 ± 16.6 | 0.9999 | −102.00 | 37![]() |
0.9 | 3.9 |
VI | −13.51 ± 0.01 | 5213.2 ± 2.8 | 1.0000 | −112.33 | 43![]() |
−13.54 ± 0.04 | 5027.0 ± 11.5 | 0.9999 | −113.29 | 41![]() |
0.9 | 3.6 |
![]() |
||||||||||||
C8 | ||||||||||||
I | −9.43 ± 0.03 | 3208.2 ± 9.3 | 0.9999 | −78.40 | 26![]() |
−9.79 ± 0.06 | 3317.3 ± 18.3 | 0.9999 | −74.93 | 27![]() |
4.4 | 3.4 |
II | −8.58 ± 0.03 | 2993.3 ± 9.7 | 0.9999 | −71.33 | 24![]() |
−8.91 ± 0.05 | 3093.5 ± 14.4 | 0.9999 | −67.62 | 25![]() |
5.2 | 3.3 |
III | −8.99 ± 0.13 | 3148.6 ± 40.4 | 0.9995 | −74.74 | 26![]() |
−9.32 ± 0.10 | 3247.3 ± 32.4 | 0.9997 | −71.03 | 26![]() |
5.0 | 3.1 |
IV | −9.56 ± 0.05 | 3333.4 ± 16.4 | 0.9999 | −79.48 | 27![]() |
−9.89 ± 0.03 | 3429.7 ± 8.1 | 0.9999 | −75.77 | 28![]() |
4.7 | 3.0 |
V | −9.76 ± 0.17 | 3450.2 ± 53.2 | 0.9992 | −81.14 | 28![]() |
−10.07 ± 0.15 | 3542.4 ± 46.3 | 0.9995 | −77.26 | 29![]() |
4.8 | 2.7 |
VI | −8.70 ± 0.39 | 3131.1 ± 121.3 | 0.9955 | −72.33 | 26![]() |
−9.00 ± 0.37 | 3220.6 ± 114.9 | 0.9962 | −68.37 | 26![]() |
5.5 | 2.9 |
![]() |
||||||||||||
ODP | ||||||||||||
I | −10.65 ± 0.32 | 3609.1 ± 101.1 | 0.9977 | −88.54 | 30![]() |
−14.07 ± 0.12 | 4632.3 ± 36.3 | 0.9998 | −103.98 | 38![]() |
17.4 | 28.3 |
II | −9.84 ± 0.29 | 3389.5 ± 89.9 | 0.9979 | −81.81 | 28![]() |
−13.04 ± 0.10 | 4348.8 ± 30.5 | 0.9999 | −95.42 | 36![]() |
16.6 | 28.3 |
III | −10.18 ± 0.32 | 3521.8 ± 100.1 | 0.9976 | −84.64 | 29![]() |
−13.29 ± 0.05 | 4454.1 ± 14.7 | 0.9999 | −97.50 | 37![]() |
15.2 | 26.5 |
IV | −10.81 ± 0.36 | 3735.1 ± 113.3 | 0.9973 | −89.87 | 31![]() |
−13.90 ± 0.02 | 4660.0 ± 7.7 | 0.9999 | −102.57 | 38![]() |
14.1 | 24.8 |
V | −9.88 ± 0.42 | 3485.1 ± 132.5 | 0.9957 | −82.14 | 28![]() |
−12.77 ± 0.13 | 4350.6 ± 39.1 | 0.9998 | −93.17 | 36![]() |
13.4 | 24.8 |
VI | −11.50 ± 0.16 | 4024.1 ± 51.0 | 0.9995 | −95.61 | 33![]() |
−14.39 ± 0.19 | 4887.6 ± 60.5 | 0.9995 | −106.64 | 40![]() |
11.5 | 21.5 |
The retention mechanisms of flavonoid glycosides on C18, cholesterol, C8 and ODP stationary phases also had been compared. The results showed that all the lnK–1/T had good linear relationships (R2 > 0.99), as well as the similar fitting parameters (ΔH0 < 0, ΔS0 < 0), which implied that the retention mechanisms of these analytes on four kinds of stationary phases were all dominated by hydrophobic interaction, and all belonged to enthalpy-driving process.1,15 On the other hand, the calculated values of a and b for each flavonoid glycoside respectively obtained from the differences between k-related and K-related ΔS0 and ΔH0 via eqn (8) were evaluated. Since ln
β = a + b/T, the parameters a and b should be always constants under the same chromatographic conditions regardless of the analytes investigated. However, it was observed that a and b values calculated by using various flavonoid glycosides had more or less differences with each other. The cholesterol-bonded stationary phase exhibited only slight discrepancy in obtaining a and b for the six flavonoid glycosides with RSDs at 2.0% and 0.1%, respectively, while the RSDs of a and b obtained from the six solutes on C18, C8 and ODP stationary phase were higher with values at 3.4% and 1.4%, 7.0% and 7.0%, and 6.4% and 6.5% for a and b, respectively. These results indicated that the property of the solutes might have influence on the mobile and stationary phases. The high consistency on the cholesterol-bonded stationary phase is probably attributed to the decline in numbers of residual silanols on stationary phase surface which are apt to cause secondary interactions such as hydrogen-bonding and so on in comparison with C18, C8, and ODP stationary phases, and in consequence, the minor structural differences among various solutes can be ignored. Moreover, as shown in Table 1, the slopes of ln
k–1/T and ln
K–1/T plots obtained on the cholesterol column were both obviously larger than those obtained on other columns, which confirmed the fact that the cholesterol bonded stationary phase was indeed more sensitive to temperature changes.
![]() | ||
Fig. 2 Chromatograms of the six flavonoid glycosides on C18 column (a–e) and cholesterol column (f–j) under different temperatures. See Fig. 1 for chromatographic conditions. Peaks: (1) flavonoid glycoside I (schaftoside); (2) flavonoid glycoside II; (3) flavonoid glycoside III (isoschaftoside); (4) flavonoid glycoside IV; (5) flavonoid glycoside V; (6) flavonoid glycoside VI. |
Fig. 3 illustrated the change in selectivity factor α, which was obtained by the experimental tR values of two adjacent solutes via eqn (6), against the temperature. As shown in Fig. 3 that, α varied at different temperatures for all the investigated compounds. For C18 column, as can be seen from Fig. 3(a), α2 and α4 decreased as temperature increased, while α1 and α5 increased with the temperature increased. However, these α values were all larger than 1.12 over the investigated temperature interval, which means all the flavonoid glycosides exhibited acceptable separation from 25 °C to 55 °C, except for compounds III and IV, the peaks of which were completely overlapped (α3 ≈ 1) on the C18 column within the experimental temperature range (see Fig. 2(a)–(e)). For cholesterol column, as shown in Fig. 3(b), the changes in selectivity with temperatures led to differences in resolution: the positive slope indicated that α2 and α5 rapidly decreased as temperature increased, while α1, α3 and α4 increased gradually with the temperature increased. In consequence, these tendency resulted in the optimal separation for the six flavonoid glycosides at 50 °C with all the α values larger than 1.2. As the temperature further increased (up to 55 °C), the separation between compounds II and III (α2 = 1.08 in Fig. 3(b)), as well as V and VI (α5 = 1.08 in Fig. 3(b)) were not complete on the cholesterol column. For C8 column, as it can be seen in Fig. 3(c), α2, α3 and α4 decreased as temperature increased, while α1 increased with the temperature increased. For compounds V and VI, the peaks of which were completely overlapped on C8 column at the low temperature range (α5 ≈ 1, 25 °C and 35 °C). Additionally, as shown in Fig. 3(c), the smaller slope of the lnα–1/T plot suggested that the chromatographic behaviors of the flavonoid glycosides were not sensitive to changes in temperature on C8 stationary phase. For ODP stationary phase, α2, α3 and α5 gradually decreased as temperature increased, while α1 and α4 increased with the temperature increased. According to the tendency of selectivity with temperature changes, it can be speculated that the appropriate column temperature for separating all the analytes is ranged between 25 °C and 35 °C on ODP column.
![]() | ||
Fig. 3 Effect of temperature on the selectivity factor on C18 column (a), cholesterol column (b), C8 column (c) and ODP column (d). See Fig. 1 for chromatographic conditions. ![]() ![]() ![]() ![]() ![]() |
On the other hand, the slope and intercept of each lnα–1/T plot in Fig. 3 respectively implied the differences in the enthalpy and entropy change of two adjacent solutes based on eqn (7). Table 2 lists the best-fit values of the intercept, the slope, as well as the correlation coefficient of each plot on C18, cholesterol, C8 and ODP columns. It can be observed from Table 2 that, all the fittings had satisfactory linearity with R2 larger than 0.94, except for the ln
α3–1/T plot (R2 = 0.3617) on C18 column, ln
α5–1/T plot on C8 (R2 = 0.8299) and ODP (R2 = 0.9260) columns, respectively, which due to the inevitable error arising from the completely overlapped peaks of III and IV on C18 column, as well as V and VI on C8 and ODP columns. The fitted Δ(ΔS) and Δ(ΔH) were compared with the calculated ones obtained from relevant data from Table 1, and the results were presented in Table 3. The high agreement of fitted and calculated data (with the RE values of Δ(ΔS) 0.1–2.5% for C18, 0.0–0.1% for cholesterol, 0.2–4.0% for C8 and 0.3–0.7% for ODP, and the RE values of Δ(ΔH) 0.1–2.1% for C18, 0.0% for cholesterol, 0.0–1.6% for C8 and 0.0% for ODP, respectively) confirmed that availability of the deduced eqn (7). With the new strategy of prediction in resolution by eqn (7) proposed in this study, one can conveniently evaluate the separation tendency of the tested compounds on a column with the change in temperature, thereby cleverly avoiding those time-consuming and laborious condition experiments.
R2 | |||
---|---|---|---|
C18 | |||
ln![]() |
1.208 ± 0.054 | −314.7 ± 16.9 | 0.9914 |
ln![]() |
−1.362 ± 0.006 | 470.2 ± 1.7 | 1.0000 |
ln![]() |
0.250 ± 0.148 | −76.1 ± 46.4 | 0.3617 |
ln![]() |
−0.884 ± 0.095 | 349.9 ± 29.6 | 0.9788 |
ln![]() |
1.253 ± 0.012 | −353.0 ± 3.8 | 0.9997 |
![]() |
|||
Cholesterol | |||
ln![]() |
1.090 ± 0.021 | −312.0 ± 6.6 | 0.9987 |
ln![]() |
−1.169 ± 0.022 | 408.2 ± 6.9 | 0.9992 |
ln![]() |
0.486 ± 0.035 | −127.8 ± 11.1 | 0.9778 |
ln![]() |
0.341 ± 0.020 | −49.7 ± 6.1 | 0.9560 |
ln![]() |
−1.359 ± 0.024 | 469.8 ± 7.3 | 0.9993 |
![]() |
|||
C8 | |||
ln![]() |
0.854 ± 0.026 | −214.9 ± 8.2 | 0.9956 |
ln![]() |
−0.420 ± 0.148 | 156.2 ± 46.3 | 0.9400 |
ln![]() |
−0.561 ± 0.087 | 181.9 ± 27.1 | 0.9714 |
ln![]() |
−0.192 ± 0.125 | 115.8 ± 39.1 | 0.9573 |
ln![]() |
1.058 ± 0.258 | −319.1 ± 80.7 | 0.8299 |
![]() |
|||
ODP | |||
ln![]() |
0.814 ± 0.039 | −219.6 ± 12.2 | 0.9907 |
ln![]() |
−0.338 ± 0.037 | 132.2 ± 11.5 | 0.9777 |
ln![]() |
−0.634 ± 0.043 | 213.3 ± 13.5 | 0.9880 |
ln![]() |
0.933 ± 0.072 | −250.0 ± 22.5 | 0.9760 |
ln![]() |
−1.628 ± 0.278 | 539.0 ± 86.8 | 0.9260 |
Δ(ΔS)a | Δ(ΔS)b | REΔ(ΔS) (%) | −Δ(ΔH)a | −Δ(ΔH)b | REΔ(ΔH) (%) | |
---|---|---|---|---|---|---|
a Best-fit parameters via eqn 7.b Calculated values obtained by relating data from ln![]() ![]() |
||||||
C18 | ||||||
ln![]() |
10.047 | 10.039 | 0.1 | −2616.7 | −2613.8 | 0.1 |
ln![]() |
−11.328 | −11.304 | 0.2 | 3909.0 | 3901.4 | 0.2 |
ln![]() |
2.081 | 2.038 | 2.1 | −633.2 | −620.1 | 2.1 |
ln![]() |
−7.349 | −7.282 | 0.9 | 2909.1 | 2888.3 | 0.7 |
ln![]() |
10.416 | 10.390 | 2.5 | −2935.1 | −2926.8 | 0.3 |
![]() |
||||||
Cholesterol | ||||||
ln![]() |
9.064 | 9.063 | 0.01 | −2593.9 | −2593.0 | 0.03 |
ln![]() |
−9.719 | −9.712 | 0.07 | 3393.8 | 3393.8 | 0.00 |
ln![]() |
4.045 | 4.044 | 0.02 | −1062.4 | −1062.2 | 0.02 |
ln![]() |
2.832 | 2.832 | 0.00 | −413.1 | −413.1 | 0.00 |
ln![]() |
−11.295 | −11.295 | 0.00 | 3906.0 | 3906.0 | 0.00 |
![]() |
||||||
C8 | ||||||
ln![]() |
7.100 | 7.067 | 0.46 | −1786.7 | 1786.7 | 0.00 |
ln![]() |
−3.489 | −3.409 | 2.29 | 1298.6 | 1291.2 | 0.57 |
ln![]() |
−4.660 | −4.739 | 1.70 | 1512.1 | 1536.4 | 1.61 |
ln![]() |
−1.599 | −1.663 | 4.00 | 963.1 | 971.1 | 0.83 |
ln![]() |
8.794 | 8.813 | 0.22 | −2653.4 | 2653.0 | 0.02 |
![]() |
||||||
ODP | ||||||
ln![]() |
6.765 | 6.73 | 0.52 | −1825.6 | 1826.2 | 0.03 |
ln![]() |
−2.814 | 2.83 | 0.57 | 1099.5 | 1099.9 | 0.04 |
ln![]() |
−5.268 | 5.23 | 0.72 | 1773.7 | 1773.4 | 0.02 |
ln![]() |
7.755 | 7.73 | 0.32 | −2078.6 | 2078.5 | 0.00 |
ln![]() |
−13.533 | 13.47 | 0.47 | 4481.6 | 4481.3 | 0.00 |
α1 | α2 | α3 | α4 | α5 | ||||||
---|---|---|---|---|---|---|---|---|---|---|
Predicted | Experimental | Predicted | Experimental | Predicted | Experimental | Predicted | Experimental | Predicted | Experimental | |
C18 | ||||||||||
40 °C | 3.812 | 3.798 | 1.145 | 1.145 | 1.137 | 1.134 | 1.085 | 1.093 | 1.770 | 1.750 |
RE% | 0.4 | 0.0 | 0.3 | 0.7 | 1.1 | |||||
50 °C | 3.755 | 3.728 | 1.143 | 1.142 | 1.113 | 1.102 | 1.077 | 1.073 | 1.853 | 1.894 |
RE% | 0.7 | 0.1 | 1.0 | 0.4 | 2.2 | |||||
![]() |
||||||||||
Cholesterol | ||||||||||
40 °C | 6.713 | 6.702 | 1.142 | 1.141 | 1.194 | 1.194 | 1.083 | 1.084 | 2.399 | 2.389 |
RE% | 0.2 | 0.1 | 0.0 | 0.1 | 0.4 | |||||
50 °C | 6.245 | 6.261 | 1.136 | 1.136 | 1.144 | 1.144 | 1.070 | 1.081 | 2.507 | 2.492 |
RE% | 0.3 | 0.0 | 0.0 | 1.0 | 0.6 | |||||
![]() |
||||||||||
C8 | ||||||||||
40 °C | 8.509 | 8.489 | 1.186 | 1.187 | 1.169 | 1.167 | 1.112 | 1.111 | 3.002 | 3.196 |
RE% | 0.2 | 0.01 | 0.2 | 0.1 | 6.1 | |||||
50 °C | 7.869 | 8.070 | 1.184 | 1.185 | 1.127 | 1.140 | 1.095 | 1.101 | 3.185 | 3.125 |
RE% | 2.5 | 0.1 | 1.1 | 0.5 | 0.0 | |||||
![]() |
||||||||||
ODP | ||||||||||
40 °C | 8.662 | 9.131 | 1.186 | 1.189 | 1.099 | 1.100 | 1.155 | 1.159 | 1.528 | 1.530 |
RE% | 5.1 | 0.2 | 0.1 | 0.4 | 0.1 | |||||
50 °C | 7.646 | 7.389 | 1.178 | 1.178 | 1.073 | 1.073 | 1.152 | 1.153 | 1.581 | 1.581 |
RE% | 3.5 | 0.0 | 0.0 | 0.1 | 0.0 |
This journal is © The Royal Society of Chemistry 2015 |