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<br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br /> <br />16 <br /> <br />" <br /> <br />\\'as not a significant problem in the series of storms \\'hich passed over the <br /> <br />San Juans from 29 to 31 January 1975, on 10 March and on 16-17 Harch. These <br /> <br />storms \oJere caused by short \oJaves \vithout significant 10\oJ level cold air <br /> <br />advection following the ~torm and/or there was insufficient time for evapo- <br /> <br />rative and radiational cooling to form a stable layer in the up\oJind valley. <br /> <br />The typical sequence of precipitation rate is ShO\Vl1 at the bottom of <br /> <br />Fig. 3.1. The precipitation begins to fall as the cloud base is lowering <br /> <br />rapidly. The precipitation rate increases and sometimes has two separate <br /> <br />high rates. One of the high rates al\oJays occurs ",hen the instability is <br /> <br />greatest over a significant depth. The other high precipitation rate often <br /> <br />occurs closer to the front end of the storm when blocking flow is not present <br /> <br />and the cloud is very deep but with near neutral stability. <br /> <br />The conditions for performing a randomized seeding experiment of v!olf <br /> <br />Creek Pass were described in detail by Grant et a1. (1969) and by Hjermstad <br /> <br />(1975). In general the conditions \oJere patterned after the results at Climax <br /> <br />in that a randomized decision to seed or not seed was made if precipitation <br /> <br />\Vas expected to fall on '.Jo1f Creek Pass and if the 500 mb temperature was <br /> <br />above -23C. The actual typical sequence for most well organized storms \Vas <br /> <br />. that seeding v70uld begin near the front of storms \oJhen blocking f1m\' was <br /> <br />present and seeding \vould cease when the 500 mb temperature dropped belmoJ <br /> <br />-23C. The 500 mb temperature almost aboJays dropped be1m\' -23C \oJhen the storm <br /> <br />\Vas associated with a significant baroclinic zone and/or cutoff low in the <br /> <br />upper atmosphere. Since the cold air advection aloft destabilized the atmos- <br /> <br />phere, the 500 mb temperature \vould drop below -23C near the time that con- <br /> <br />vective instability first developecl. The 500 mb temperature dropped below <br /> <br />-23C less often when tllC storm wos associat("d V1ith short Hilves or baroc1 in1c. <br /> <br />zones \oJhich pr.Lmari1y pasfjccl \oJc11 to tile north of the San JUClJ1S. <br />