Because water is formed by polymerization and can be removed from the solution by evaporation, the material balance constraint for water is for equilibrium moles, n W ≥ 0, via Equation 2.17 and not the initial moles,
Several important relations can be developed. The distribution of oligomer lengths is given by the Flory‐Schulz distribution [22]. The %EMLA j for species j is (note that a typographical error in equation 19 of Vu et al. [27] omits the 100):
(2.22)
Other useful results are:
(2.23)
(2.24)
FIGURE 2.5 The percent equivalent monomer lactic acid for L1 through L4. Open symbols are from Montgomery [24] and Ueda and Terajima [25]. Solid symbols are measured by Vu et al. [27].
(2.25)
The %EMLA for the short oligomers are shown in Figure 2.5. The equilibrium constant is only weakly temperature dependent. Esterification reactions are commonly nearly thermoneutral. Recently, Feng et al. [29] performed potentiometric titration at temperatures between 8 and 100°C. They found that differences in the titratable acidity were only a couple percent mostly in the range of 60–80 apparent wt% lactic acid; minor differences were observed at other concentrations.
2.6 VAPOR–LIQUID EQUILIBRIUM
Vapor–liquid equilibria for aqueous solutions of lactic acid have been measured by Sanz et al. [30] and Vu [31]. Sanz et al. used gas chromatography to measure compositions of both phases. They reported only L2 and L3 oligomers of lactic acid. Both flame ionization and thermal conductivity detectors were used, which enabled quantification of the water. Details of the calculations using the peak areas were not provided. Due to the low volatility of oligomers, error in the overall lactic acid concentrations of the liquid phase is likely. Analysis of the data indicates that
TABLE 2.4 Liquid Phase Mole Fractions of Lactic Acid + Water VLE at 101.33 kPa
T (K) | True x water |
True |
True |
True |
True |
Apparent |
---|---|---|---|---|---|---|
378.25 | 0.79 | 0.19 | 0.015 | 0.0012 | 0.0001 | 0.22 |
379.25 | 0.8 | 0.18 | 0.014 | 0.0011 | 0.000087 | 0.21 |
380.25 | 0.73 | 0.24 | 0.024 | 0.0023 | 0.00023 | 0.30 |
380.75 | 0.72 | 0.25 | 0.025 | 0.0025 | 0.00025 | 0.31 |
381.75 | 0.69 | 0.28 | 0.03 | 0.0033 | 0.00037 | 0.35 |
381.85 | 0.71 | 0.26 | 0.027 | 0.0027 | 0.0003 | 0.32 |
383.35 | 0.68 | 0.28 |