“…Therefore, the input fluid from point B can be either water vapor, liquid water or a mixture Ta), (13) where k (kJ m-2 deg 1 day') is an unknown pa rameter including the effect of wind speed and air humidity. According to Brown et al (1989), the conductive and latent heat loss from a lake surface are, Eevap = 86400 Slake LE(gw qa )u (14) and Econd = 86400S1akepCpE(Tw Ta )u, (15) respectively, where L is the latent heat of vapor ization of water (2400 kJ kg-1 at room tempera ture), E is the average particle flux (no dimen sion), u is the friction velocity (m s-1), p is the air density (0.92 kg m-3 at 2000 m altitude at 10°C), q,,, is vapor density of the saturated air at lake water temperature, qa is the vapor density of am bient air (kg m-3), and Cp represents the specific heat of water-saturated air at 10°C (1.013 kJ kg -1 deg 1) (Brown et al, 1989 (20). From the averaged temperatures, the ratio was calculated and shown in Table 2.…”