首页> 外文期刊>ournal of the Meteorological Society of Japan >On the Effect of Selective Absorption of the Atmospheric Water Vapour upon the Total Amount of Solar Radiation observed on the Earth Surface
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On the Effect of Selective Absorption of the Atmospheric Water Vapour upon the Total Amount of Solar Radiation observed on the Earth Surface

机译:大气水汽选择性吸收对地球表面太阳辐射总量的影响

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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=0.047e (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.
机译:本文从对著名的Fowle经验公式的批评开始,该公式给出了通过吸收大气中水蒸气而损失的太阳辐射量:Fv = 0.057 + 0.012Qm,Q为可沉淀的水,而m为“公式中常数项的出现,其荒谬性是毋庸置疑的,这归因于由不同来源的温暖潮湿空气组成的层偶尔存在的扰动,该层叠加在下部空气质量上地区。在Fowle观测数据的实际曲线上指出了这一点,给出了改进的公式F = 0.047e(e是在地球上观测到的以厘米汞柱为单位的蒸气压)。作者的意见被在山顶的太阳总辐射观测的结果所加强。过去一年中,富士(3770万。)在大多数情况下,由于灰尘(固体或液体)的散射反射和蒸汽的选择性吸收的综合作用而导致的太阳辐射总量JmT的降低明显小于Fowle公式给出的结果。从大多数情况下的天气状况可以很容易地看出,这可能是由于我们没有受到暗示的高层气流干扰的结果。为了将这两种效果彼此分开,通过Schott玻璃F 4512(2毫米厚)进行了观察。在纯空气的瑞利散射和粉尘散射的表达式的基础上,通过数值积分来计算可见光区和紫外区Sm中的相对辐射量以及红外区Lm中的相对辐射量。借助于(Sm,m)和(Lm,m)中的C轮廓来协调方程JmT = const的数值解。 (Sm + Lm)和JmR = const.K。求出Lm(aw是蒸气因子,K因子取决于滤光片的透射率,JmR是红色滤光片观察到的辐射量),以确定C和aw。确定滤光片透射的红外辐射的K值和太阳常数的结果几乎与根据太阳光谱能量曲线和玻璃的透射曲线计算出的值完全吻合,即K = 0.08989和太阳常数。= 1.080卡路里。 cm-2分钟-1。此外,从数值积分的结果指出了K值对空气质量的轻微依赖性。事实证明,x = 1.3的假设值太小而无法给出一致的结果,这表明在许多情况下有必要将其增大到0.7或0.8。

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