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<br />.~ ... <br /> <br />field for an extended period of time a ground <br />station was developed for rapid reduction of <br />flight data upon landing. The in-depth analysis <br />began upon landing with an Hewlett-Packard RTE- <br />III computer system. With the RTE-III system the <br />aircraft tapes were stripped and the reduced data <br />placed in files on a storage disk. From the disk <br />a variety of subroutines were available to pro- <br />duce digital listings of data, flight tracks, <br />soundings, analog traces of derived parameters <br />and 2-D images. The typical procedure was to <br />have a quick first-look at all the data on the <br />same day as the flight. Non-flying days were <br />spent conducting more in-depth data analysis. <br /> <br />" <br /> <br />To compliment the airborne cloud <br />physics data, a mobile ground cloud physics ob- <br />server collected ice crystal and other data along <br />1-80. The ground cloud physics data were espec- <br />iallyimportant because even when flying at MOCA <br />the aircraft is still approximately 1 km AGL. <br /> <br />Even though there was time to conduct <br />a significant amount of in-depth analysis for <br />each storm, there llimply was not time to corre- <br />late all the data in the form of graphs and fig- <br />ures for presentation in this manuscript. We <br />have reached a number of significant preliminary <br />conclusions which we will attempt to justify with <br />data at the conference. <br /> <br />3. <br /> <br />STORM DYNAMICS <br /> <br />California is unique in that it is <br />completely surrounded by mountains except at San <br />Francisco where the. water from the whole of the <br />California Valley converges and drains into the <br />Pacific Ocean. In the winter season the net <br />radiation over the valley is negative. Being <br />surrounded by mountains a strong, persistent pool <br />of quiesent stably stratified air forms in the <br />California Valley. It is not at all uncommon <br />for this pool of air to cool down to the dewpoint <br />and for the resultant fog and low stratus to <br />persist for days. <br /> <br />With the approach of a cyclonic storm, <br />a significant amount of upper level divergence is <br />associated with the central and left exit zone of <br />the approaching jet stream. The upper level di- <br />vergence induces low level convergence in the <br />stably stratified pool of air in the California <br />Valley. This pool of air responds by surging <br />northward and is channeled by the Sierra Nevadas <br />on the east and by the Coastal Range on the west. <br />The net result is a low level jet at 1 to 2 km <br />and upslope and convergence in the northern end <br />of the valley. <br /> <br />An approaching storm is first noted <br />with the approach of high level cirrus. The first <br />moisture to advect over the Sierras arrives at <br />2 to 3 km altitude because that air has the <br />shortest travel time of moist air from off the <br />Pacific Ocean. Consequently the cloud develop- <br />ment sequence is advection of cirrus followed by <br />mid-level stratiform clouds which either advect <br />into or are formed over the Sierras. These <br />clouds are nearly always stable. <br /> <br />Prior to the arrival of the cold <br />front, it is typical for a number of pre-frontal <br />convective cloud bands to move across the valley <br /> <br />from off the Pacific Ocean. The origin of these <br />convective cloud bands is not known. . When the <br />low level stable layer is present the "roots" of <br />the convection are well above the surface. The <br />convective cloud bands dissipate over the foot- <br />hills of the Sierras after they have overturned <br />the convectively unstable air above the stably <br />stratified air mass trapped in the valley. The <br />convective instabilities develop due to differen- <br />tial advection. The flight during the morning of <br />l4 December was through the southern tip of a <br />weak convective cloud band. Ahead of convective <br />cloud bands the low level jet is typically paral- <br />lel to the Sierras. Behind convective cloud bands <br />the wind speeds decrease and the directions veer <br />to a more westerly direction. <br /> <br />With the approach of the main jet <br />core at 300 mb before dawn on 15 December a low <br />level jet with speeds of approximately 24 mps de- <br />veloped (Moore, 78). On a number of cases we <br />were able to takeoff ahead of an approaching con- <br />vective cloud band. On these occasions the sur- <br />face winds were approximately lO mps with gusts <br />to approximately IS mps and the direction was <br />from the SSE, i.e. parallel to the Sierras. Mod- <br />erate to severe turbulence was experienced below <br />the low level jet regardless of the stabi.lity. <br />This implies that the turbulence was priDmrily <br />mechanically induced from vertical wind shear. <br />MUch more dramatic decreases in wind speed and <br />veering of direction were documented on other con- <br />vective cloud bands than were observed on 14 and <br />15 December. On the few occasions when we were <br />able to transverse most of the valley and inter- <br />cept either a convective cloud band or cold front <br />near the Coastal Range, the preliminary indica- <br />tion is that the low level jet was uniform across <br />the valley rather than confined to the Sacramento <br />or foothills area. <br /> <br /> <br />,i, <br />~ {- <br /> <br />H <br />t <br />l. <br />i':: <br />r <br />i' <br />, <br />I <br /> <br />The passage of a cold front in the <br />California Valley is typically denoted by a well <br />defined convective cloud band, rising barometer <br />and more often than not a slight increase in the <br />surface temperature. Rarely does the surface <br />winds turn to the west or northwest. The explana- <br />tion for these phenomena seems to be that the <br />front rides above the low level stable air, the <br />convection occurs just above the low level stable <br />air and the warming occurs because of downward <br />flux of sensible heat due to turbulent mixing. <br /> <br /> <br />If there is still some convective <br />instability remaining following the passage of a <br />cold front and if there are mechanisms to initiate <br />this convection over the Coastal Range, then a <br />series of post-frontal convective cloud bands will <br />develop and move across the California Valley. <br /> <br />As the convective cloud bands and <br />frontal convective bands move over the foothills <br />of the Sierras, they first seem to invigorate <br />from the additional mechanical lifting then ra- <br />pidly decrease in intensity having overturned and <br />processed the available high energy air ahead of <br />each band. It is not clear at this ~ime whether <br />or not low level air is injested from the back- <br />side of moving convective cloud bands. <br /> <br />It is quite typical for a post-frontal <br />convective cloud wall to form over the foothills <br />following the passage of a cold front. This was <br /> <br />150 <br />