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Vergara - 1976 - Physiological and morphological adaptability of ri

Vergara - 1976 - Physiological and morphological adaptability of ri

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LTLIMAHC INFLUENCE ON<br />

PHOTOSYbTfHESlS AND RESPIRATION<br />

The net photosynthesis substrating respiration loss is usually less than 5—6%<br />

<strong>of</strong> the total energy’ absorbed. The efficiency <strong>of</strong> net energy conversion by a <strong>ri</strong>ce<br />

population was about 5% at booting stage. reached a maximum value <strong>of</strong> 7%<br />

at heading. <strong>and</strong> showed a rapid decline thereafter. Most <strong>of</strong> the energy absorbed<br />

was lost by transpiration <strong>and</strong> heat transfer (Murata et a1. 1968).<br />

The production processes <strong>of</strong> a plant population depend on many complex<br />

interactions between environmental <strong>and</strong> biological factors, Light intensity‘ <strong>and</strong><br />

productive structure <strong>of</strong> the plant population are the most important factors<br />

which determine its dry matter production, Monsi <strong>and</strong> Saeki (1953) found that<br />

light extinction by leaves in the plant population was expressed by the exponential<br />

equation:<br />

I = 1,, exp( — KF) (4)<br />

where I: light intensity beneath a LAI <strong>of</strong> F. 1,: light intensity“ above the community.<br />

F: LAI above the point <strong>of</strong> measurement. K: extinction coefficient. K<br />

is calculated by the stratified clipping method where the plant is harvested in<br />

successive shallow layers from the surface downward <strong>and</strong> accompanied by a<br />

simultaneous record <strong>of</strong> light pr<strong>of</strong>ile, K tvas closely correlated with leaf arrangement,<br />

especially" leaf angle. <strong>and</strong> its value was inversely" related to the leaf angle.<br />

'l'akeda <strong>and</strong> Kumura (1957) <strong>and</strong> Murata (1961) indicated that exponential<br />

equation (4) was applicable to <strong>ri</strong>ce populations.<br />

Monsi <strong>and</strong> Saeki (1953) expressed net photosynthesis (q = p — r) per unit<br />

leaf area by the following equation:<br />

q = bl _ _<br />

1+n<br />

' i”<br />

where r indicates respiration per unit leaf area, a <strong>and</strong> b are coefficients related to<br />

the photosynthetic capacity <strong>of</strong> a single leaf. By substituting the light intensity<br />

in equation (5) by equation (4) <strong>and</strong> integrating from 0 to F for LAI. the equation<br />

for total net photosynthesis <strong>of</strong> population (P) becomes;<br />

P: b m l+amu<br />

a K 1+ a Kloexp(— KP)<br />

— rF (6)<br />

Munakata ct al, (1970) indicated that when the respiration function (r1?)<br />

was represented by Arrhenius equation (3), the photosynthesis in <strong>ri</strong>ce population<br />

could be approximated by equation (6).<br />

The light saturation point for photosynthesis in a plant population becomes<br />

higher with increasing leaf area. The light-photosynthesis curve is markedly"<br />

affected by the extinction coefficient as well as by leaf area. The net photosynthesis<br />

<strong>of</strong> a plant population with vertical foliage was shown to be theoretically<br />

greater than with ho<strong>ri</strong>zontal foliage at a high leaf-area index, However, at a<br />

low leaf-area index the plant population with ho<strong>ri</strong>zontally o<strong>ri</strong>ented leaves<br />

shtiwed greater photosynthesis (Saeki. 1960).

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