Water and Solute Permeability of Plant Cuticles: Measurement and ...
Water and Solute Permeability of Plant Cuticles: Measurement and ...
Water and Solute Permeability of Plant Cuticles: Measurement and ...
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116 4 <strong>Water</strong> <strong>Permeability</strong><br />
in the CM <strong>and</strong> on the surface <strong>of</strong> the CM. The onion bulb scale CM is well-protected<br />
within the bulb, <strong>and</strong> abrasion <strong>and</strong> wear are not likely to occur. Hence they have <strong>and</strong><br />
need only minimum amounts <strong>of</strong> wax.<br />
These model calculations show convincingly that waxes which would form<br />
mono- or bilayers on the surface <strong>of</strong> cutin, as is suggested by AFM investigations<br />
(Koch et al. 2004), could be very effective as water barriers. These waxy barriers<br />
can be very thin <strong>and</strong> still have a low permeance. A simple polymeric membrane<br />
similar to polyethylene or parafilm would have to be much thicker, <strong>and</strong> energetically<br />
this would be much more costly.<br />
4.6.4.3 Estimation <strong>of</strong> <strong>Water</strong> Sorption in Wax <strong>and</strong> Thickness <strong>of</strong> the Waxy<br />
Transpiration Barrier<br />
In Sect. 4.6.3 a diffusion coefficient <strong>of</strong> about 10 −16 m 2 s −1 for water in cuticular<br />
waxes isolated from the leaves <strong>of</strong> the species Ginko, Juglans <strong>and</strong> Prunus was<br />
calculated (Table 4.12). This is significantly lower than Dw <strong>of</strong> water in synthetic<br />
polymer membranes <strong>and</strong> MX membranes (Table 4.1), but it is similar to diffusion<br />
coefficients for water calculated from extrapolated hold-up times obtained with CM<br />
(Table 4.10). Can these diffusion coefficients be related to Pw measured for CM,<br />
paraffin wax <strong>and</strong> aliphatic monolayers? The relationship <strong>of</strong> Pwv <strong>and</strong> Dw is given by<br />
(2.18), assuming that the transport barrier <strong>of</strong> wax is homogeneous. The partition<br />
coefficient Kww <strong>and</strong> the thickness <strong>of</strong> the wax barrier ℓ are needed to relate Dw to Pw.<br />
In Table 4.12 Dw <strong>and</strong> Pw are listed, <strong>and</strong> the ratio Kww/ℓ can be calculated. With<br />
wax coverages <strong>of</strong> 39, 51 <strong>and</strong> 83µgcm −2 for Ginko, Juglans <strong>and</strong> Prunus respectively,<br />
ℓ can be calculated assuming that all the wax contributes to the formation <strong>of</strong> the barrier.<br />
Using these values, wax/water partition coefficients for water can be calculated<br />
Table 4.12 Diffusion coefficients in wax (Dw), permeances (Pw) <strong>of</strong> water across the CM, <strong>and</strong><br />
thickness ℓ <strong>of</strong> the wax layers in Ginkgo biloba, Juglans regia <strong>and</strong> Prunus laurocerasus. Wax/water<br />
partition coefficients Kww are calculated by multiplying Kww/ℓ by ℓ. Thickness ℓ <strong>of</strong> the wax layer<br />
was calculated dividing Kww by Kww/ℓ<br />
Ginkgo Juglans Prunus<br />
Dw (m 2 s −1 ) a 1.60 × 10 −16 1.06 × 10 −16 1.19 × 10 −16<br />
Pw (ms −1 ) b 4.3 × 10 −10 6.3 × 10 −10 1.33 × 10 −10<br />
ℓ (nm) calculated from wax amounts c 433 566 922<br />
Pw/Dw = Kww/ℓ 2.69 × 10 6 5.94 × 10 6 1.11 × 10 6<br />
Kww calculated d 1.16 3.36 1.03<br />
ℓ (nm) calculated for Kww = 0.01 3.7 1.7 9.0<br />
ℓ (nm) calculated for Kww = 0.04 14.9 6.7 36.1<br />
a Calculated from equations listed in Table 6.10<br />
b Data from Table 4.7<br />
c Calculated from wax overages given in Table 4.7<br />
d Kww calculated here have the units gram per volume (g water/cm 3 polymer)/(g water/cm 3 water)<br />
<strong>and</strong> not gram per gram as given in Sect. 2.4