From 197 hourly averaged, four‐level wind speed profiles collected on Ice Station Weddell (ISW) in February and March 1992, we compute the neutral stability, 10‐m, air‐ice drag coefficient, C DN10 . Values range from 1.3×10 −3 to 2.5×10 −3 for the multiyear ice floe that was ISW. Individual C DN10 values depend critically on how well the mean wind is aligned with the dominant snowdrift patterns. On ISW, 20% of the time, we experienced drifting or blowing snow; when the wind speed at 5 m exceeded 8 m s −1 , such wind‐driven snow was a virtual certainty. Consequently, the surface was continually changing, drifts were building, drifts were eroding. As the wind continued from a constant direction and the building drifts streamlined the surface, C DN10 could decrease by as much as 30% in 12 hours. If the wind direction then shifted by as little as 20°, C DN10 would immediately increase significantly. The implications are that snow‐covered sea ice does not present an isotropic surface; it has a preferred direction dictated by the wind's history. Consequently, computing surface stress using an average value for C DN10 will produce errors of up to 30%.
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Andreas et al. (1995) studied this question.
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