CHAPTER 4: CORRELATION OF ACTIVE LAYER THICKNESS, WATER
4.3.2. Effective and Polyamide Water Partition Coefficients
Effective partition coefficients of water in membrane active layers (πΎπ΄πΏ) were obtained from the water uptake measurements in liquid water as given by
πΎπ΄πΏ = ππ
πππ»2ππΆπ»2ππΏπ΄πΏ. (4.9)
In Equation 4.9, it is assumed that the membrane does not swell by a significant amount when immersed in liquid water. While active layer swelling was not measured in this study, other studies in the literature have reported 13Β±6% swelling observed for SWC4+ membrane, 7Β±2% swelling for ESPA and 4.8Β±4.4% for ESPA1 membrane, and 35Β±2% for XLE
membrane.15,27 Therefore, while active layer swelling was not characterized in this study, errors in the water partition coefficients estimated with Equation 4.9 are expected to be at most 35%. The values of πΎπ΄πΏ for the five membranes studied were in the range of 0.33(Β±0.04) β 0.72(Β±0.11) and are listed in Table 4.2.
Water partition coefficients in the active layers polymer (πΎπ) were obtained from the water uptake measurements in humidified nitrogen gas as given by
πΎπ = ππ ππ£
π»2ππΆπ»2ππΏπ . (4.10)
The polymer thickness was used in the calculation instead of the active layer thickness , because water uptake by the voids under humidified nitrogen gas was negligible and only the polymer was responsible for the mass increase (ππ£) caused by water uptake, according to the findings in Chapter 3. The values of πΎπ for the five membranes studied were in the range of 0.19(Β±0.03) β 0.26(Β±0.13) and are listed in Table 4.2. A comparison of the values of πΎπ΄πΏ and πΎπ indicates that the existence of voids within membrane active layer increased the partition
coefficient of the active layer by a factor of 1.7-3.4 (πΎπ΄πΏ/πΎπ). The increased partition coefficient of the active layer caused by the voids can be explained by the fact that the water partition
coefficient of active layer polymer (πΎπ) is smaller than 1 while the water partition coefficient of voids is 1 (as the voids are filled with water when the membrane is in contact with liquid water). Therefore, the effective water partition coefficient of the active layer (πΎπ΄πΏ), which is a function of the partitioning into polymer and voids, is higher than the water partition coefficient of the polymer (πΎπ).
As discussed in Section 4.1, Zhang et al. obtained water uptake values by active layers of FT30 and LF10 membranes under humidified nitrogen gas and Lee et al. obtained water uptake value by active layer of SW30 membrane also under humidified helium gas.17,18 Zhang et al. also calculated the concentration of water in the membrane active layers (πΆπ, molΒ·m-3), but did not take into account in the calculations the void fractions of the active layers because of a lack of awareness of the existence of the voids. Similarly, the value of πΆπ for the SW30 membrane active layer can also be calculated for the study of Lee et al. based on the water uptake value
they reported, though they did not report the value of πΆπ in their study. Because of the unawareness of the existence of the voids, the πΆπ values they obtained and the corresponding values of πΎ that can be calculated from their study are neither effective active layer properties (as the water uptake tests were conducted under humidified nitrogen gas instead of liquid water) nor polymer properties of membrane active layers (as the existence of voids was not accounted for). The values of πΆπ obtained by Zhang et al. were 7.7Γ103 molΒ·m-3 and 8.7Γ103 molΒ·m-3 for the FT30 and LF10 RO membranes,17 respectively, so the corresponding partition coefficients calculated as πΎ = πΆπ/πΆπ»2π are 0.14 and 0.16 for the FT30 and LF10 RO membranes,
respectively. The values of πΆπ calculated based on the study of Lee et al. is 15.4Γ103 molΒ·m-3 for the SW30 membrane and the corresponding value of K is 0.28.
While Zhang et al. used similar water uptake tests under humidified nitrogen gas as the tests used in this study to obtain the πΎπ values, the water partition coefficients obtained from their study are smaller than the values of πΎπ obtained for the four RO membranes in this study (average πΎπ of 0.22Β±0.03 for the four RO membranes) because they did not take into account the existence of voids within membrane active layers. In fact, if the existence of voids were ignored in the present study (i.e., πππππ = 0), the water partition coefficients of active layer polymer (πΎπβ²) would have been calculated to be 0.16Β±0.02 for NF90, 0.13Β±0.02 for XLE, 0.19Β±0.01 for ESPA3, 0.16Β±0.05 for SWC4+ and 0.15Β±0.01 for SW30HR as shown in Table 4.2, with an average of 0.16Β±0.02 for the four RO membranes (XLE, ESPA3, SWC4+ and SW30HR membranes). This average value is not statistically different from the partition coefficients obtained by Zhang et al. While Lee et al. used a different water uptake measurement technique and obtained a 2 times higher water uptake by the SW30 membrane active layer compared to this
calculated from the Lee et al. study is only 1.3 times higher than the value of πΎπ for the
SW30HR membrane. Therefore, not taking into account the existence of voids could lead to an underestimation of the partition coefficient of the active layer polymer by a factor of 1.2-1.4 (πΎπβ²/πΎπ) in membrane characterization.