METEOROLOGICAL INFLUENCES ON sr CONCENTRATIONS Ac ye / / )/ | 1.0—— ¢ / )/ @ y y / ; / Q / / L -1.0 /B G, / B / 4 / / / / / / / 0 ‘=() er? / / / 0 ° ® /® a / Ba a eo / / . / / / y d / / / / / / p05 / f | 10 4H / + -0.5 Ty it o , / 0.5—-‘ / f f / / 095 / -+-0.1 ® RAIN x SNOW OOLD DATA O NEW DATA / Fig. 5—Fractional change in°Sr concentration, SC, as a function of Fractional change in ceiling, AH. (AC = 1,25 AH + 0.65.) the variability in drop size distributions, and the errors associated with low frequency of ceiling measurement and long sample times are considered, it is indeed surprising to see anuncertainty in the exponent of only 50%. The effect of evaporation has also been observed in Pacific cyclones. In many cases very dry air overrides the shallow marine layer, and the first rain falling from the middle clouds accompanying an approaching wave falls through about 6000 ft of air with a relative humidity of 30% or less. The Santa Barbara collection of Feb. 7, 1962, shows this effect markedly.“ A cross section of this storm is shown in Fig. 6, and the vertical distribution of temperature and humidity before and after saturation of the marine layer is shown in Fig. 7. During the first few hours after rain began, the dry air between 2000 and 7500 ft gradually reached saturation. The first rainfall reaching the ground contained a high Sr concentration, which decreased to onethird of its initial value 2 hr later, Precipitation-growth Mechanisms The role of this mechanism in determining ground-level nuclear-debris concentrations has been given earlier.

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