In winter, 1984, snow cloud bands (Sakakibara et al. 1987) were observed over the Japan sea off the coast of Kanazawa. They lasted about 90 minutes, and the orientation of the bands was almost perpendicular to the direction of mean wind. 2-dimensional numerical simulation of the snow band is performed, using a non-hydrostatic anelastic model with the bulk parameterization of cloud microphysics including both water (cloud water, rain) and ice phase (cloud ice, snow, graupel).
In the early stage of the simulation, a unicellular storm is reproduced, and later, it turns into a multicellular storm. In this paper, the simulated multicellular storm is investigated in detail. It is com-pared with the storm at the unicellular stage, observations, and other squall lines so fax documented.
The characteristic features of the multicellular storm and temporal behavior of individual cells which constitute the multicellular storm are as follows. 1) The fields of the multicellular storm averaged on the storm-scale (-15km, as contrasted with the individual cell scale-5km) are similar to that of the unicellular storm in these points; a) upshear tilting of updraft, front-to-back ('front' is defined as the direction from which the low level system-relative flow enters into the storm) systemrelative u-component of updraft branch, and back-to-front system-relative u-component of downdraft branch, b) a cold dome at the surface and corresponding high pressure area, c) a storm-scale warm area and corresponding low pressure area above cold dome. But the horizontal scale and intensity of the fields are larger than those of the unicellular storm. 2) The fluctuations by individual cells are large in w, cloud water, and graupel fields and at the mid level, while those are relatively small in other fields and at the low level. 3) Transformation of the unicellular storm into the multicellular one is related to the faster movement of the gust front than that of the individual cell. 4) A new cell is generated above the gust front intermittently at the time interval of 25 minutes on average but with large variance, and at the distance of about 5km on average but with large variance from the old cell. 5) After the generation of a new cell, the warm air inflow from the low level into the old cell is cut off, and the old cell begins to dissipate and move backward. 6) In the new cell, cloud water and graupel are found, while, in the old cell, little cloud water is found and snow is dominant.
The results of simulation agrees well with observations in the following points: 1) multicellular structure, 2) upshear tilting of updraft, front-to-back system-relative u-component of updraft branch and back-to-front system-relative u-component of downdraft branch, 3) a cold dome at the surface, 4) the width and height of the radar echo of the snow band, 5) long lasting property. The features of the snow cloud band observed and simulated indicate that the snow band is similar to the squall line, although the strength and scale of the cloud band and the environmental thermal stratification are different.
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