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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 />As air is forced over mountains it cools and moisture condenses out forming clouds and precipitation. <br />After passing over the tops of the mountains, the air slides down the lee side. The downward <br />movement of the air results in slight warming and the warmer air has more capacity to hold moisture <br />as water vapor. Thus the cloud droplets evaporate and the clouds disappear. <br /> <br />When an air mass approaches the Uinta Basin from any direction, it must pass over mountains or <br />high plateaus. The Wasatch Mountains to the west of the Basin form a barrier of about 8,000 to <br />10,000 feet. An air mass approaching from the west is lifted and cooled to the 8,000 level, and <br />considerable moisture is condensed out. Although some moisture remains in the air mass, further <br />lifting (above 8,000 feet) is required to continue cloud formation and precipitation. Further lifting <br />occurs for the portion of the air mass that passes over the higher Uinta Mountains and precipitation <br />is produced in those areas. The air passing over the southern slopes of the Uinta Mountains (less <br />than 8,000 feet) or over the Uinta Basin, descends in elevation. Clouds dissipate and no <br />precipitation results even though there is still moisture in the air. The moisture that is carried <br />downwind will be deposited as precipitation when it is condensed out by further lifting processes (i.e., <br />when the air mass is lifted above 8,000 feet as it passes over the Rocky Mountains of Colorado). <br /> <br />The Effects of Storm Fronts <br /> <br />Large air masses tend to take on and retain certain characteristics for relatively long periods of time. <br />Air masses which stagnate over polar ice and snow fields are usually very cold and dry. Air masses <br />that travel long distances over warm oceans are usually warm and moist. A "storm front" occurs <br />when a warm air mass is pushed against a cold air mass. The warm air mass slides up and over the <br />cold air mass. As the air rises and cools, moisture condenses and clouds are formed. Further <br />cooling and condensation results in precipitation. For these reasons, clouds and precipitation are <br />associated with storm fronts. <br /> <br />, <br />j <br /> <br /> <br />Winter and spring storm fronts pass over the Uinta Mountains, the Wasatch Mountains or the high <br />pbteaus into the Uinta Basin on a regular basis. These fronts are affected by topography. To <br />understand the linkage between frontal storms and topography, net lifting can be divided into two <br />components: (1) lifting within the storm system (warm moist air being lifted as it moves upward over <br />the cold air mass) and (2) lifting of the storm system itself as it moves upward over a mountain range <br />(or subsidence, as it descends mountainous slopes). <br /> <br />A frontal storm moving toward the Basin will be lifted as it approaches the Wasatch Mountains. The <br />topographic lift of the storm system enhances the frontal lift of the storm. This lifting intensifies the <br />storm and increases precipitation on the windward side of the mountains. As the storm moves into <br />the Uinta Basin, it descends the mountains and the descent of the storm system tends to counteract <br />the frontal lift that occurs within the storm. At times, the descent of the storm system may be rapid <br />enough to negate the lifting within the storm and little or no precipitation results. At other times <br />the frontal lifting within the storm is rapid enough that the slow topographical descent as the storm <br />system moves down-slope, counterbalances only a small part of the frontal lifting within the storm <br />system. Under this situation, precipitation may be copious, even though it is slightly reduced from <br />what it would be if there were no mountainous descent. <br />