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Vergara - 1976 - Physiological and morphological adaptability of ri

Vergara - 1976 - Physiological and morphological adaptability of ri

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MILTRLICLlKili-YTE 0F THE RICE CROP 129<br />

Ta, w = Zrr/ru is the angular velocity’ <strong>of</strong> temperature tvave, In is the pe<strong>ri</strong>od <strong>of</strong><br />

temperature xvave. <strong>and</strong> d is the water depth. The results obtained from the above<br />

relation agreed well with measurements in shallow waters (Mihara et al, 1959).<br />

Uehijima (1959) proposed also the following to relate the difference in mean<br />

temperature between flooded water <strong>and</strong> the air with meteorological factors:<br />

AT : Tw _' Ta : “Rum _ cl/pacpDa T‘<br />

where RM. <strong>and</strong> G are the daily" means <strong>of</strong> net radiation above flooded water <strong>and</strong><br />

<strong>of</strong> soil heat flux, respectively‘, <strong>and</strong> 5e is the water vapor deficit. Results obtained<br />

from Eq. (20) agreed well with observations <strong>and</strong> were used to evaluate the<br />

geographical va<strong>ri</strong>ation <strong>of</strong> water temperature <strong>of</strong> paddy fields (Uehijirna, 1959.<br />

1962b, 1963). Du<strong>ri</strong>ng the summer with strong radiation, the daily‘ mean water<br />

temperature was higher than the mean air temperature, implying that heat energy<br />

yvas consistently" transferred from the water surface to the air. The difference<br />

in temperature between water <strong>and</strong> air increased gradually with the move~<br />

ment from lower latitude to higher latitude. because <strong>of</strong>the decreasing value <strong>of</strong> r .<br />

Sato (1960) observed pr<strong>of</strong>iles <strong>of</strong> temperature in clear <strong>and</strong> turbid water with a<br />

depth <strong>of</strong> 5 ein, in relation to the prevention <strong>of</strong> damage by" exceptionally high temperatures<br />

in flooded water as observed in southern Kyushu du<strong>ri</strong>ng midsummer.<br />

Part <strong>of</strong> his measurements are reproduced in Fig. TB. The temperature in clear<br />

“tater is uniform throughout at all times. On the either h<strong>and</strong>, the temperature in<br />

turbid water exhibits inverse pr<strong>of</strong>iles du<strong>ri</strong>ng daylight. but the pr<strong>of</strong>iles at night<br />

are the same as those observed i11 the clear water layer. Rose <strong>and</strong> Chapman<br />

(1968) <strong>and</strong> Chapman (1969) also observed the temperature pr<strong>of</strong>iles in clear <strong>and</strong><br />

turbid waters, <strong>and</strong> found that the turbidity" <strong>of</strong> water is effective in lowe<strong>ri</strong>ng water<br />

temperature.<br />

The energy’ balance <strong>of</strong> <strong>ri</strong>ce fields has been studied to estimate water use by <strong>ri</strong>ce<br />

plants <strong>and</strong> to elucidate characte<strong>ri</strong>stics <strong>of</strong> the energy partition <strong>of</strong> <strong>ri</strong>ce fields The<br />

redist<strong>ri</strong>bution <strong>of</strong> radiant energy’ absorbed by crops is tisually’ expressed as follows:<br />

R,,=1E+C+J+G

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