Heat balance analysis, on the assumption that the condition of the ground surface is uniform like in a flat area, cannot be made in a mountainous area. However, at the time of planning of land use, irrigation and drainage, it is necessary to consider the heat balance in mountainous areas. In this paper, from the standpoint of micrometeorology, the thermal and moisture environment at the top and in the valley of a mountainous area were investigated, and the qualitative analysis of heat balance at each location was made. As a result, the following facts became clear:
(1) A great difference between the values at the top and in the valley was comfirmed as regards air temperature, wet-bulb temperature, relative humidity, soil moisture, ground temperature and wind speed (Figs.3-7).
(2) In the daytime, the water vapor pressure at a height of 50 cm was higher than that at a height of 350cm, and that difference was larger in the valley. The air temperature at a height of 50 cm was higher than that at a height of 350cm, and that difference was larger at the top (Fig. 8).
(3) The latent heat flux was calculated using the heat balance method from the air temperature and the water vapor pressure at heights of 50cm, 150cm and 350cm. It might be difficult to estimate the latent heat flux using the heat balance method in a mountainous area, as the calculated values were unreliable during nighttime. But in the daytime, as the sun's altitude became higher, the continuity of the vertical flux was comfirmed (Fig. 11). At that time, Bowen's ratio was constant (Fig. 12).
(4) Heat balance in the daytime was calculated using the constant Bowen's ratio at the top and in the valley (Table 1).
(5) The moisture condition near the ground surface was estimated from the antecedent precipitation, soil moisture distribution, small pan evaporation and Penman's potential evapotranspiration (Tables 1, 2, Figs. 10, 13).
Immediately after a rainfall which is enough to moisten the ground surface uniformly, the heat balance at the top equals that in the valley. Successively, water moves from the top (divergent area) to the valley (convergent area) due to gravity force, and the top becomes dry, while the valley becomes wet. Accordingly, latent heat flux in the valley, and sensible heat flux at the top become important terms of heat expense. The heat balances in a mountainous area are illustrated in Fig. 14.
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