ATMOSPHERIC TRANSPORT PROCESSES 457 Sb Pr yo" f : J ie LA ‘ 3 (ads INVERSION . ws s.) Ls, aN ASFE.S ome NUINVERSION 4 £ ‘, . “Ly . me Ne a t tf | ( cr fer gat of nga a ‘if } \s5 | 3 tM ‘4 - i Fig. 6—Potential vorticities (units, 1079? cm-sec-deg/g) of 300°K isentropic surface, at 12 GCT on Nov, 22, 1962. 295 and 300°K isentropic surfaces, attached itself to a lower stable layer with potential temperatures of about 290°K. This lower layer was too low and too slow to be of stratospheric origin (see Fig. 8 and for comparison see also Fig. 4), Thus original estimates of the amount of air involved in the sinking process were too high (see Table 1). Adjust- ments were made by subtracting the air mass within the lower stable layer from thetotal. From Table 1 it appears that 0.6 x10! metric tons is a good order-of-magnitude estimate of the air involved in the transport proTable 1—-AMOUNT OF AIR INVOLVED IN TRANSPORT OF RADIOACTIVITY TO THE GROUND Calculated mass 1962, 1962, 1962, 1962, 1963, 1963, 1963, 1963, 00 GCT 12 GCT 00 GCT 12 GCT 12 GCT 00 GCT 12 GCT 00 GCT Corrected value, 10!2 metric tons 0.64 ofes Nf 23, 23, 24, 24, 29, 30, 30, 31, O-~ wo 0 oo. Nov. Nov. Nov. Nov, Mar, Mar. Mar. Mar, 10!2 metric tons ee Date and time Uncorrected value,

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