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<br />25 <br /> <br />atmosphere by cloud evaporation on the downslope side of the ridge has <br /> <br />to be removed from the final water balance computation. This is done <br /> <br />by obtaining an estimate of the downslope evaporation and eliminating <br /> <br />this estimate from the net condensation already computed for between <br /> <br />Camp Hale and Fairplay. <br /> <br />Estimation of the downslope evaporation is done by computing tem- <br /> <br />perature and mixing ratio profiles for an imaginary station at the top <br /> <br />of the ridge (designated TOP). The air above this station is assumed <br /> <br />to be initially saturated and travelling adiabatically between the top <br /> <br />and Fairplay. For each 8e channel, the temperature at TOP is equal to <br /> <br />the temperature at Fairplay minus the dry adiabatic warming due to <br /> <br />descent and compression, plus the cooling due to evaporation between <br /> <br />Camp Hale and Fairplay. Expressed as an equation. <br /> <br />TTOP <br /> <br />TFPY + yd 62 + 1-- (w w) <br />Cpd TOP - FPY <br /> <br />(7) <br /> <br />Here yd is the dry adiabatic lapse rate (-9.80C/km.), 62 is the distance <br /> <br />the parcel descends between the top of the ridge and Fairplay, L is the <br /> <br />latent heat of evaporation and Cpd is the specific heat of dry air, <br /> <br />wTOP is the mixing ratio at the top (assumed saturated) and wFPY is the <br /> <br />mixing ratio at Fairplay. wTOP is an exponential function of TTOP so <br /> <br />equation (7) can be evaluated numerically. An initial guess of TTOP <br /> <br />(and thus wTOP) is found by time interpolation on the Camp Hale temper- <br /> <br />. <br /> <br />ature time series. Evaluated for each 8e channel, equation (7) gives <br /> <br />a temperature profile at TOP. <br />