The present paper starts with a criticism of the well-known Fowle's empirical formula which gives the amount of solar radiation to be lost by the absorption of the atmospheric water vapour:
Fv=0.057+0.012Qm, Q being the precipitable water and m the “air mass” The occurrence of the constant term in the formula, whose absurdity is out of question, is attri buted to the probable perturbation of the occasional existence of the layer consisting of warm moist air of different origin superposed on the air mass in the lower region. This is pointed out on the actual plots of the Fowle's observational data, giving the improved formula
F=0.047
e (
e is the vapour pessure in cm. of Hg., as observed on the earth). The author's opinion is strengthend by the results of observations of total solar radiation made on the summit of Mt. Fuji (3770m.) during the past one year. In the majority of cases, the reduction of the total amount of solar radiation
JmT due to the combined effect of the scattered reflection of dust (solid or liquid) and the selective absorption of vapour is remarkably less than that given by the Fowle's formula. This may be regarded a consequence of our being free from the alluded perturbation of the upper air current, as can be easily seen from the synoptic condition pertaining to the great majority of cases. In order to separate those two effects from each other the observations were made through the Schott glass
F 4512 (2mm thick). The relative amount of radiation in the visible and U. V. region
Sm, and that in the infra-red part
Lm were computed by the numerical integrations on the basis of Rayleigh scattering of pure air and the expression of the dust scattering. By means of
C-contours in (
Sm,
m) and (
Lm,
m) co-ordinates the numerical solution of the equations
JmT=const. (
Sm+
Lm) and
JmR=const.
K. Lm(
aw is the vapour-factor,
K factor depending on the transmission of the filter,
JmR the radiation amount observed with the red filter) were made to determine
C and
aw. The result of determination of
K-value and the solar constant for the infra-red radiation transmitted by the filter almost exactly coincide with the values computed from the solar spectral energy curve and the transmission curve of the glass,
i.e K=0.08989 and solar const.=1.080cal. cm
-2 min
-1. Moreover the slight dependence of
K-value on the air mass is pointed out from the result of numerical integration. The assumed value of x=1.3 was proved to be too small in many cases to give consistent result, which suggests the necessity of increasing it so much as 0.7 or 0.8 in many cases.
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