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Water and Solute Permeability of Plant Cuticles: Measurement and ...

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8.5 <strong>Water</strong> <strong>Permeability</strong> <strong>of</strong> Synthetic Polymers as Affected by Temperatures 255<br />

log P wv or D<br />

60<br />

-9.5<br />

-10.0<br />

-10.5<br />

-11.0<br />

-11.5<br />

-12.0<br />

-12.5<br />

-13.0<br />

Temperature (°C )<br />

50 40 30 21 13 5<br />

log P wv = -537 x - 8.15 (r 2 =0.94)<br />

3.0 3.1 3.2 3.3 3.4 3.5 3.6 3.7<br />

1/T x 1000 (Kelvin -1 )<br />

log K wv = 1607 x -3.54 (r 2 = 0.98)<br />

log D = -1918 x -5.49 (r 2 = 0.99)<br />

-3<br />

2.6<br />

Fig. 8.9 Temperature dependence <strong>of</strong> Pwv, D, und Kwv for polyvinyl chloride. Data taken from<br />

Doty et al. (1946)<br />

For polyvinyl chloride, D was also determined by Doty et al. (1946) using the<br />

hold-up time method (2.5). With increasing temperature (1 to 55 ◦ C), D increased<br />

slightly (7.8 × 10 −11 –17 × 10 −11 m 2 s −1 ), while Pw increased from 2.2 × 10 −13 to<br />

54 × 10 −13 m 2 s −1 (Fig. 8.9). The partition coefficient Kwv can be calculated from<br />

these data using (3.17). Kwv decreased with increasing temperature from 246 to<br />

31cm 3 vapour per cm 3 polymer.<br />

From the slopes given in Fig. 8.9, the energies <strong>of</strong> activation can be calculated.<br />

For EP <strong>and</strong> ED 10.3 <strong>and</strong> 36.7kJ mol −1 are obtained, <strong>and</strong> by difference (8.18) the<br />

enthalpy <strong>of</strong> sorption or the heat <strong>of</strong> solution ∆HS <strong>of</strong> −26.4kJ mol −1 is obtained. The<br />

enthalpy change for transfer <strong>of</strong> water into PVC is negative, indicating it to be a<br />

spontaneous process, but with increasing temperature decreasing amounts <strong>of</strong> water<br />

are sorbed (c.f. Sect. 8.1). For the other polymers in Fig. 8.8, D was not measured<br />

<strong>and</strong> ED remains unknown. With polystyrene EP is zero, <strong>and</strong> this implies that ED <strong>and</strong><br />

∆HS are numerically equal but have opposite sign.<br />

In Table 8.2, some additional data including rather polar polymers (EC, CA,<br />

PEMA) have been collected. At 25 ◦ C, some <strong>of</strong> the polymers are in the glassy state<br />

(PET, Nylon, PVA, EC <strong>and</strong> PEMA). In this collection, Pwv was highest with cellulose<br />

acetate (which is used for desalination membranes) <strong>and</strong> lowest with polyvinyl<br />

acetate. They differ by a factor <strong>of</strong> 251. PVA has the lowest diffusion coefficient<br />

<strong>of</strong> 5.1 × 10 −15 m 2 s −1 . For the other polymers, D varies from 1.1 × 10 −11 (EC) to<br />

1.2 × 10 −12 m 2 s −1 (nylon, rubber HCl) by a factor <strong>of</strong> 9. Partition coefficients (Kwv)<br />

in the range <strong>of</strong> partial pressures where sorption isotherms are linear (3rd column)<br />

ranged from 7,255 (PVA) to about 8 for PE.<br />

2.4<br />

2.2<br />

2.0<br />

1.8<br />

1.6<br />

1.4<br />

log K wv

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