PCTSMC
color composite
Fig. 6 Cloud screening based on color composite
and PCTSMC methods of NOAA imagery
in an area from Hokkaido to northeastern
Honshu (after Utsunomiya and Katoh,
1995),
3.4 Surface and air temperatures
3.4.1 Determination of surface temperature:
Surface temperature (Ts) in each NOAA pixel was
calculated from the relationships between XNOAA
brightness temperature and water temperature retrieved
from the above database.
3.4.2 Estimation of air temperature: Air
temperature (Ta) in each NOAA pixel was also
computed using a statistical model based on the
relationships between surface temperature Ts and air
temperature derived from the above database and other
meteorological datafiles (Fig.7, 8).
3.4.3 Amplitude of temperature: The
amplitudes of both surface and air temperature, dTs and
dTa, in NOAA pixels were calculated by subtracting the
temperatures Ts and Ta at night from each of those
during the day, respectively.
Fig. 7 Distribution of ground monitoring points
in an automated meteorological data
system for Japan.
886
Fig. 8 Distribution of estimated air temperature,
its profile, legend and operational panel.
4. HEAT BALANCE ANALYSIS
4.1 Shortwave radiation
4.1.1 Downward short-wave radiation: Down-
ward short-wave radiation was calculated by the
procedure suggested by Seino and Uchijima (1988) and
statistical modeling was done from the relationships
between TOVS and radiation data at the monitoring
stations. Assuming the diurnal variation of solar
radiation to be approximately sinusoidal on a cloudless
day (Monteith, 1973), variation curves of direct and
diffuse radiation were computed using following models.
These parameters were computed in the following
equation. First, solar radiation was calculated using
parameters such as duration of sunshine, sun elevation
and snow cover.
[StH] = So {0.146+0.534% + 0.047G10 + 0.036 sin n
Ae ERU (Yoshida and Shinoki, 1978) (2)
where h: sun elevation at noon on the 15th day of each
month, G10: index of snow cover; ratio of the number
of days with snow cover exceeding 10 cm depth divided
by the amount of days in any month, S0: monthly
average duration of possible sunshine in any month
Monthly average of direct solar radiation [SbH] was
calculated using following equation.
[StH]
SoH] _ 91528 4 0.92019] . 9.0013 & - 0.0706 Gio
[StH] So
videns (Seino and Uchijima, 1988) (3)
where [StH]: monthly average of global solar radiation
[Seu], [SdH]: monthly average daily amount of direct solar and
diffuse radiations, respectively
ea = 4.54 exp (0.068 * Ta ).....(Seino and Uchijima,1988) (4).
This equation for estimating vapor pressure, ea, was
developed using data obtained in a humid climate. Ta:
air temperature, G10: The index G10 is substituted by
the index, GO, in the following equation, where GO is
the ratio of the number of days with any depth of snow
International Archives of Photogrammetry and Remote Sensing. Vol. XXXI, Part B4. Vienna 1996
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