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

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4.1 <strong>Water</strong> <strong>Permeability</strong> <strong>of</strong> Synthetic Polymer Membranes <strong>and</strong> Polymer Matrix Membranes 63<br />

calculated by multiplying Kwv by 23.05 × 10 −3 kgm −3 , the water vapour concentration<br />

<strong>of</strong> air at 100% humidity <strong>and</strong> 25 ◦ C (3.20). Concentration <strong>of</strong> water in synthetic<br />

polymers in equilibrium with 100% humidity (or p/p0 = 1) ranged from 0.65 to<br />

168kgm −3 .<br />

Pwv was obtained by multiplying Pw by 43,384 (3.11). Permeances <strong>of</strong> the selected<br />

MX membranes ranged from 1.2 × 10 −3 to 2.5 × 10 −4 ms −1 . In order to compare<br />

synthetic polymers <strong>and</strong> MX membranes, both types <strong>of</strong> membranes must have the<br />

same thickness. Permeances for the synthetic membranes were calculated as P/ℓ<br />

for a thickness <strong>of</strong> 3µm, which is similar to thicknesses <strong>of</strong> the MX membranes in<br />

Table 4.1. As these synthetic polymers are homogeneous, this is perfectly legitimate.<br />

Permeances <strong>of</strong> MX membranes are similar to those calculated for the polar polymers<br />

EC, CA, PMA, PEMA <strong>and</strong> Nylon. Permeances <strong>of</strong> PP, PE, PVA <strong>and</strong> PET membranes<br />

are considerably lower.<br />

Comparing diffusion coefficients meets with some difficulties (Table 4.1). Becker<br />

et al. (1986) determined D values for Ficus <strong>and</strong> Citrus MX using the hold-up time<br />

method (2.5), while Chamel et al. (1991) estimated D from sorption isotherms<br />

(2.33), <strong>and</strong> their D are considerably higher than those <strong>of</strong> Becker et al. (1986).<br />

Chamel et al. (1991) also determined water vapour sorption in CM <strong>and</strong> MX gravimetrically.<br />

Sorption in MX <strong>and</strong> CM was similar or identical because most sorption<br />

sites (dipoles) are contributed by cutin <strong>and</strong> polar polymers, <strong>and</strong> access <strong>of</strong> water to<br />

Table 4.1 <strong>Water</strong> permeability at 25 ◦ C <strong>of</strong> selected synthetic polymer membranes <strong>and</strong> plant polymer<br />

matrix membranes isolated from astomatous leaf surfaces<br />

Polymer Pwv D(m 2 s −1 ) Kwv Cw Pwv (ms −1 ) Jwv<br />

(m 2 s −1 ) (kgm −3 ) (ℓ = 3µm) (gm −2 h −1 )<br />

PP a 1.9 × 10 −11 4.9 × 10 −13 39 0.90 6.3 × 10 −6 0.52<br />

PE a 3.3 × 10 −11 1.2 × 10 −12 28 0.65 1.1 × 10 −5 0.91<br />

PVA b 3.7 × 10 −11 5.1 × 10 −15 7,269 168 1.2 × 10 −5 1.00<br />

PET a 1.3 × 10 −10 2.7 × 10 −13 484 11.2 4.3 × 10 −5 3.57<br />

Nylon b 3.3 × 10 −10 1.2 × 10 −13 2,750 63 1.1 × 10 −4 9.13<br />

PEMA c 2.9 × 10 −9 1.1 × 10 −11 264 6.1 9.7 × 10 −4 80.5<br />

CA b 9.3 × 10 −9 3.1 × 10 −12 3,000 69 3.1 × 10 −3 257.3<br />

EC d 1.9 × 10 −8 1.9 × 10 −11 1,000 23 6.3 × 10 −3 522.8<br />

Ficus MX e 1.4 × 10 −9 1.8 × 10 −14 7.8 × 10 4 1.8 × 10 3 2.5 × 10 −4 20.7<br />

Ficus MX f – 4.1 × 10 −13 2,000 34 - −<br />

Citrus MX e 5.2 × 10 −9 6.0 × 10 −15 8.7 × 10 5 2.0 × 10 4 1.8 × 10 −3 149.3<br />

Citrus MX f – 2.6 × 10 −14 2,828 41 - −<br />

Pyrus MX g – – 4.7 × 10 −3 390.0<br />

Hedera MX g – – − – 1.2 × 10 −3 99.6<br />

a Rust <strong>and</strong> Herrero (1969)<br />

b Hauser <strong>and</strong> McLaren (1948)<br />

c Stannett <strong>and</strong> Williams (1965)<br />

d Wellons <strong>and</strong> Stannett (1966)<br />

e Becker et al. (1986)<br />

f Chamel et al. (1991)<br />

g Schönherr <strong>and</strong> Lendzian (1981)

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