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A balloon carrying an electric field meter and a standard meteorological radiosonde rose into a relatively small, isolated thunderstorm in central New Mexico on July 16, 1977. The electric field, E, versus altitude between 3200 m (surface) and 7000 m above sea level can be explained reasonably well by the following charge distribution: (1) a 130 m thick layer of positive charge just above the surface with a density of 1.7 × 10−9 C/m3; (2) a localized 1 C of positive charge moving downward on rain with a velocity of 8 m/s at a horizontal distance of 420 m from the balloon; (3) a 1‐km thick ‘layer’ of negative charge between 4800 and 5800 m above sea level with a density of about −5 × 10−9 C/m3. This negative charge spanned a temperature range of about −2 to −5°C. Between 7000 and 10,000 m above sea level, the balloon was near the edge of the cloud where E was low and principally horizontal. Above 10,000 m the balloon ascended into an anvil cloud that was apparently positively charged.
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Winn et al. (1981) studied this question.
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