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<br />process:' "cold-cloud process:' or the "Bergeron <br />Process." (Tor Bergeron w~s a Swedish'meteorol- <br />ogist who contributed greatly to our knowledge <br />of precipitation formation mechanisms in clouds <br />containing ice particles.) . <br /> <br />Cloud droplets.beil1g relatively clean. do not <br />freeze immediately when a cloud top rises above <br />the freezing level. In fact. pure water can be <br />cooled to a bout -40 0 C (-40 0 F) before it freezes. <br />A cloud consisting of liquid water droplets colder <br />than 0 0 C is called "supercooled". Freezing at <br />temperatures warmer than -40 0 C is attributed to <br />very small foreign particles called ice nuclei. <br />Natural ice nuclei include certain types of soil. <br />dust. and decayed vegetation. . . <br /> <br />An ice crystal in the presence of supercooled <br />droplets will grow rapidly at the expense of the <br />droplets. Water will evaporate from the drop- <br />lets. diffuse as vapor to the ice crystal. and deposit <br />as additional ice on its surface. When the ice <br />crystal gets large enough by the diffusion process. <br />it will start to fall through the cloud and can start <br />to grow by accretion; that is. by collision with the <br />droplets. The droplets freeze instantly onto the <br />crystal when they touch. forming piles of ice <br />beads called rime. This process of riming some- <br />times builds up frozen droplet deposits so thick <br /> <br />8 <br /> <br /> <br />.J6 <br />fI) <br />::I <br />E <br />... <br />14 <br />!i: --. <br />S2 <br />~2 <br /> <br />0' NO SEEOING <br /> <br />bl HYGROSCOPIC SEEDING <br /> <br />J <br /> <br /> <br />E <br />... <br />14 <br />I- <br />5 <br />~2 <br /> <br /> <br />01 ICE PHASE SEEOING <br />(STATIC EFFECTI <br /> <br />dl ICE PHASE SEEDING <br />(OYNAMIC EFFECTI <br /> <br />Figure 1.1 -Basic cloud seeding concepts applied to typical <br />cumulus clouds of the northern High Plains. <br /> <br />20 <br /> <br />-10 ~ <br />I <br />Q: <br />o ~ <br />I- <br /> <br />-lOP <br />I <br />II: <br />::I <br />o 1&1 <br />I- <br /> <br />that the interior ice crystal cannot be seen. The <br />resulting lump of snow is called an ice pellet or <br />. graupeL If ice crystals bump into each other and <br />stick. the result isan aggregate snowflake <br />composed of a few to hundreds of ice crystals. <br />Thus. the presence of ice in a supercooled cloud <br />can speed the production of precipitation by the <br />. d iffu~ion. accretion. a nd/or aggregation <br />processes. . <br /> <br />Most modern cloud seeding projects have been <br />based on the assumption that some supercooled <br />clouds do not contain enough ice crystals to make <br />the precipitation process efficient. Many clouds <br />are relatively free of ice until their tops reach the <br />-20 0 C (":'4 0 F) level. Additional ice particles are <br />induced at warmer temperatures by seeding with <br />an efficient ice nucleant or by chilling the air tem- <br />porarily below -40 0 C (-40 0 F)(fig. 1.1). The <br />most common artificial ice nucleating agent is Agl <br />(silver iodide); a commonly used chilling agent is <br />solid CO2 (carbon dioxide). which is usually called <br />dry ice. <br /> <br />Sometimes natural clouds produce more ice <br />crystals than the available ice nuclei could create <br />directly. The additional crystals are attributed to <br />"ice multiplication." Several different mecha- <br />nisms have been proposed. One process of ice <br />multiplication initiates extra ice crystals at temper- <br />atures near -5 0 C (23 0 F) when graupel and large <br />cloud droplets are simultaneously present. Clouds <br />supporting an ice multiplication process fre- <br />quently produce showers at warmer cloud-top <br />temperatures than do clouds producing ice crys- <br />tals only by direct action of ice nuclei. <br /> <br />In choosing clouds for seeding experiments and <br />in evaluating results. it is important to determine <br />which of the natural precipitation processes are <br />at work and the efficiency of that process. The <br />need to do that implies a need to measure cloud- <br />top temperatures. cloud droplet sizes. and so on. <br />Acquiring such measurements was. in fact. one of <br />the major HIPLEX activities. <br /> <br />The possible effects of cloud seeding are not <br />limited to changes in the efficiency of the precip- <br />itation processes. Many scientists have written <br />about the possibility of changes in cloud size or <br />cloud lifetime by seeding (fig. 1.1). These postu- <br />lated dynamic effects of seeding are even harder <br />to document than the physical effects mentioned <br />above. Nevertheless. their potential impact on <br />rainfall from convective clouds is so great that <br />they cannot be ignored in any consideration of the <br />future of cloud seeding technology on the High <br />Plains. <br /> <br />4 <br />