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Vertical wind tunnel experiments and a theoretical study on the microphysics of melting low-density graupel

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Theis,  Alexander
Particle Chemistry, Max Planck Institute for Chemistry, Max Planck Society;

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Mitra,  Subir K.
Particle Chemistry, Max Planck Institute for Chemistry, Max Planck Society;

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Diehl,  Karoline
Particle Chemistry, Max Planck Institute for Chemistry, Max Planck Society;

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Borrmann,  Stephan
Particle Chemistry, Max Planck Institute for Chemistry, Max Planck Society;

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Citation

Theis, A., Mitra, S. K., Diehl, K., Zanger, F., Szakáll, M., Heymsfield, A., et al. (2022). Vertical wind tunnel experiments and a theoretical study on the microphysics of melting low-density graupel. Journal of the Atmospheric Sciences, 79. doi:10.1175/JAS-D-21-0162.1.


Cite as: https://hdl.handle.net/21.11116/0000-000A-2256-F
Abstract
Vertical wind tunnel experiments were carried out to investigate the melting of low-density lump graupel while floating at their terminal velocities. The graupel characteristics such as maximum dimension, density, and axis ratio, were 0.39 ± 0.06 cm, 0.41 ± 0.07 g cm−3, and 0.89 ± 0.06. The air stream of the wind tunnel was gradually heated simulating lapse rates between 4.5 K km−1 and 3.21 K km−1. Each experimental run was performed at a constant relative humidity that was varied between 12 % and 92 % from one experiment to the other. From the image processing of video recordings, variations in minimum and maximum dimension, volume, aspect ratio, density, volume equivalent radius, and ice core radius were obtained. New parameterizations of the terminal velocity prior to melting and during melting were developed. It was found that mass and heat transfer in the dry stage is two times higher compared to that of liquid drops at the same Reynolds number. Based on the experimental results a model was developed from which the external and internal convective enhancement factors during melting due to surface irregularities and internal motions inside the melt water were derived using a Monte Carlo approach. The modelled total melting times and distances deviated by 10 % from the experimental results. Sensitivity tests with the developed model revealed strong dependencies of the melting process on relative humidity, lapse rate, initial graupel density, and graupel size. In dependence on these parameters, the total melting distance varied between 600 m and 1200 m for typical conditions of a falling graupel.