SVERIGES LANTBRUKSUNIVERSITET - Epsilon Open Archive - SLU
SVERIGES LANTBRUKSUNIVERSITET - Epsilon Open Archive - SLU
SVERIGES LANTBRUKSUNIVERSITET - Epsilon Open Archive - SLU
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50<br />
• l:' effect it may have on the gas phase mainly closure of stomata or stornatal<br />
resistance.<br />
THE SOIL-PLANT-AIR CONTINUUM (SPAC)<br />
In the past 30 years the water flow through the system (F) has been<br />
represented by the van den Honert (1948) principle:<br />
F = ?/Js - ?/Jr =?/Jr - ?/J1 = ?/J1 - ?/Ja<br />
R s R p Ra<br />
where ?/J s ' ?/Jr' ?/JI and ?/Ja are the total water potential of soil, at the root<br />
surface, at the evaporating surfaces of the leaf, and of the bulk air,<br />
respectively. R s ' R p and Ra are the resistances of the soil, plant, and<br />
vapour pathways, respectively. While the potential drop in the two liquid<br />
phases of the pathway is normally no greater than 3 MPa, the drop in the<br />
water potential between leaf and bulk air (?/JI - ?/Ja) can be 100 MPa or<br />
greater and emphasizes the significance of sto mata in controlling the flow<br />
of water through the system.<br />
However, caution is needed when attempting to extrapolate from eq. (7).<br />
Flow through the soil, plant and atmosphere are coupled but separate<br />
systems, the uptake and redistribution of water from the soil within the<br />
plant occur in the liquid phase, while loss of water from the evaporating<br />
sites in the leaf is in the vapour phase. A calculation using gradients of<br />
water potential as the driving force willlead to a substantial overestimation<br />
of the magnitude of the resistances of the vapour phase due to the<br />
logarithmic relationship between water potential and vapour pressure<br />
(eq. 2). Also, the van den Honert model assumes a steady-state situation<br />
which sel dom exists within the plant. Finally, tissues of plants with<br />
significant storage capacity can be regarded as alternative sources of water<br />
linked in parallei with the soil.<br />
The above concept of van den Honert (eq. 7) treating the soil-plantatmosphere<br />
water movement in analogy with Ohm's law has stimulated<br />
much useful research since its adoption. The recognition of the stornatal<br />
resistance being the crucial resistance regulating water vapour flux out of<br />
the plant, and the controi of stornatal closure under water stress by<br />
decrease of turgor pressure of stornatal cells, caused by decrease of leaf<br />
water potential, are similarly well recognized.<br />
When the water status of a plant starts to fall, which it will if the<br />
evaporative loss from the leaves exceeds the influx of water from the roots,<br />
a threshold behavior is of ten observed; Le. stomata close when a certain<br />
threshold of ?/J 1 is reached, of ten from - 1.2 to - 1.6 MPa for field grown<br />
crops. The threshold behavior act s as an overriding protective mechanism<br />
against excessive leaf water deficit (Hsiao and Bradford, 1983).<br />
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