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East Asia and Western Pacific METEOROLOGY AND CLIMATE

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306<br />

O.Qg-m" 3 , which is probably due to an increase of the<br />

efficiency of the particles' collision-coalescence process<br />

as melting snowflakes turn wet; (2) an obvious shift of<br />

the horizontal wind (Fig. 2); (3) a transition toward<br />

mesoscale descent motion below the melting layer. These<br />

findings support the idea that the pressure perturbation<br />

induced by the cooling of melting snow causes a decoupling<br />

of dynamics above <strong>and</strong> below the melting layer (Johnson <strong>and</strong><br />

Young, 1983)<br />

Analyses of the probe-imaging data show that the<br />

significant increase of particle terminal velocity from<br />

melting snow to liquid droplet results in a sharp decrease<br />

of the particle number .density by an order of magnitude<br />

(Fig. 3). Lo <strong>and</strong> Liu (1989) have applied a theoretical<br />

approach to quantify such relationship.<br />

Meanwhile, a steady increase in the percentage of<br />

large particles (diameter 2500-5000jLim for 2D-C <strong>and</strong><br />

2000-lOOOOjLtm for 2D-P) immediately above the melting<br />

layer followed by a sudden decrease are noticed in both<br />

probes' data (Figs. 4 <strong>and</strong> 5), These phenomena stress that<br />

snowflake aggregation generates large particles, in<br />

particular in the 0°C isothermal layer where wet<br />

snowflakes have a much higher chance to collect other<br />

particles. Willis <strong>and</strong> Heymsfield (1989) have claimed that<br />

the radar reflectivity maximum (bright b<strong>and</strong>) is due to<br />

these relatively few, very large aggregates that survive<br />

to warmer temperatures. Before reaching the bottom of the<br />

melting layer, either the collision-breakup or the<br />

spontaneous breakup process causes a rapid disappearance<br />

of these large, wet particles, since the breakup<br />

efficiency increases with particle size.<br />

Evolution of the size spectra (Fig. 6) also reveals<br />

the physical processes of aggregation, melting <strong>and</strong><br />

breakup. From -1.7°C (Fig. 6a) to 0.2°C (Fig. 6b),<br />

snowflakes aggregate to form a few particles larger than<br />

0.7cm diameter at the expense of smaller particles <strong>and</strong><br />

therefore the total particle concentration. From 0.2°C<br />

(Fig. 6b) to 1.4°C (Fig. 6c), both the melting <strong>and</strong> breakup<br />

processes help to eliminate larger particles, while the<br />

increase in fallspeed caused by the transition from ice to<br />

water phase results in a significant decrease in total<br />

particle concentration.<br />

3 r THE WARM-RAIN REGION<br />

In this section, our focus is on analyzing the<br />

evolution of spectra along the vertical direction below<br />

the melting layer. The liquid water content (LWC)<br />

measured by the Johnson-Williams device shows a constant

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