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Last modified
7/28/2009 2:37:45 PM
Creation date
4/16/2008 11:05:50 AM
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Template:
Weather Modification
Contract/Permit #
14-06-D-6801
Title
Structure and Seedability of San Juan Storms
Date
11/1/1976
Weather Modification - Doc Type
Report
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<br />15 <br /> <br />I <br /> <br />on standard thermodynamic diagrams. The base of the convective instability <br /> <br />I <br /> <br />was located where observed upslope winds would first begin to release the <br /> <br />convective instability. There was one particular case (30 January - first <br /> <br />flight) where there was significant conditional instability but the winds <br /> <br />were do\vuslope and unable to release the thermodynamic instability. The <br /> <br />top of the convective instability has the same 8 as at the convective con- <br />e <br />densation level. The convective instability forms initially due to cold <br /> <br />I <br /> <br />I <br /> <br />I <br /> <br />I <br /> <br />air advection aloft and sometimes warm, moist air advection below. More <br /> <br />I <br /> <br />often the \Varm, moist advection is delayed until the blocked flow is removed, <br /> <br />thus allowing the warm, moist air to advect into the area from the south or <br /> <br />I <br /> <br />sou th\ves t. <br /> <br />The blocked flow is a serious problem on many storms. The blocked flow <br /> <br />level is defined as that level below which the wind directions are less than <br /> <br />I <br /> <br />1600. The blocked flow seems to form from two or three processes. ~~en a <br /> <br />\vell organized storm passes over the San Juans the end of the storm occurs <br /> <br />I <br /> <br />I <br /> <br />when significant cold air advection begins to occur in the lowest levels. <br /> <br />Thus, a mass of cold, stable air is left behind to affect the next storm to <br /> <br />I <br /> <br />pass over the area. The other processes are more speculative but there seems <br /> <br />to be some supporting evidence in the data. It is speculated that the high <br /> <br />I <br /> <br />mountain massives in southern Colorado cool by snow sublimation and to a <br /> <br />I <br /> <br />lesser degree by radiative cooling during clear winter periods. That these <br /> <br />cooling effects are possible seems likely because the mountains are above most <br /> <br />of the moisture and the \\finds during non-storm situations are typically light <br /> <br />I <br /> <br />because the jet stream is well north of the region. <br /> <br />I <br /> <br />The evidence supporting the above hypothesis concerning blocking flow <br /> <br />I <br /> <br />is that the stability after the passage of a major trough is as descrj~ed <br /> <br />(see post-storm stability on 29 December 7Q, 28 January 75, 1.5 l'larch 7.5 <br /> <br /> <br />and 17 Harch 75). On the other hand, thermodynamically stable blocking fTow <br /> <br />I <br />I <br />
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