Display of ice crystal flutter in atmospheric light pillars

Borovoi, Anatoli G.; Kustova, Natalia V.

doi:10.1029/2008gl036413

Cited by 9 publications

(1 citation statement)

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“…Common models of particle orientation assume either uniform distribution, horizontal orientation with inclination angle of zero, or a Gaussian distribution with a peak at zero inclination angle (e.g., Borovoi and Kustova, 2009). However, orientation models for falling particles suggest modal inclination angles of approximately 10 • (Klett, 1995).…”

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Stable and unstable fall motions of plate-like ice crystal analogues

Stout,

Westbrook,

Stein

et al. 2024

Preprint

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Abstract. The orientation of ice crystals affects their microphysical behaviour, growth, and precipitation. Orientation also affects interaction with electromagnetic radiation, and through this, influences remote sensing signals, in-situ observations, and optical effects. Fall behaviours of a variety of 3D-printed plate-like ice crystal analogues in a tank of water-glycerine mixture are observed with multi-view cameras and digitally reconstructed to simulate falling of ice crystals in the atmosphere. Four main falling regimes were observed: stable, zigzag, transitional, and spiralling. Stable motion is characterised by no resolvable fluctuations in velocity or orientation, with the maximum dimension oriented horizontally. The zigzagging regime is characterised by a back-and-forth swing, corresponding to a time series of inclination angle approximated by a rectified sine wave. In the spiralling regime, analogues consistently incline at an angle between 7 and 28 degrees, depending on particle shape. Transitional behaviour exhibits motion in between spiral and zigzag, similar to that of a falling spherical pendulum. The inclination angles that unstable planar ice crystals make with the horizontal plane are found to have a non-zero mode. This observed behaviour does not fit the Gaussian model of inclination angle that is common in the literature. The typical Reynolds number when oscillations start is strongly dependent on shape: solid hexagonal plates begin to oscillate at Re = 237, whereas several dendritic shapes remain stable throughout all experiments, even at Re > 1000.

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