## Abstract According to the Mason‐Latham mechanism the main thunderstorm charge is generated by the impaction, freezing and splintering of supercooled droplets on pellets of soft hail. The rates of charge and splinter production are now calculated using the Ludlam‐Browning model of the thunderstor
The formation of atmospheric ice crystals by the freezing of droplets
✍ Scribed by E. K. Bigg
- Publisher
- John Wiley and Sons
- Year
- 1953
- Tongue
- English
- Weight
- 618 KB
- Volume
- 79
- Category
- Article
- ISSN
- 0035-9009
No coin nor oath required. For personal study only.
✦ Synopsis
Abstract
Using the results of laboratory experiments on the supercooling of purified water, the freezing of cloud and raindrops is examined. It is shown that at temperatures lower than about −30°C in cold‐box or expansion‐chamber experiments, the drops freeze in approximately the numbers that would be expected if they were pure water. Those that freeze at temperatures higher than about −20°C seem to be more numerous than would be the case if the drops were pure. An interpretation of the main features of the Findeisen and Schulz expansion‐chamber experiments is found to be possible without appealing to the action of foreign ice‐forming nuclei, although there is a discrepancy between calculation and experiment at temperatures higher than about −20°C. In the atmosphere, formation of cirrus clouds is shown to become possible at temperatures below about −35°C, glaciation in stratiform clouds to become appreciable at temperatures below about −20°C and freezing of raindrops in strongly convective clouds to become important below about −13°C, without the presence of ice nuclei. It is concluded that freezing nuclei may be important at temperatures above about −20°C, while their presence at lower temperatures will be masked by the freezing of uncontaminated drops.
📜 SIMILAR VOLUMES
## Abstract When supercooled drops of diameter 1·3 mm were nucleated at — 0·2$C and froze in an environment at — 15$C and fragmented, the average charge on positive residues was 1·5 × 10^−3^ e.s.u., and on negative residues — 2·2 × 10^−3^ e.s.u. The charges were comparable with those found in simil