PARTICLE SIZE DISTRIBUTION AT 110,000 FT 139 Table 2—SIZE-DISTRIBUTION RESULTS Number of particles diameter, p ‘Particle 2562, 2569, and 2572 Flights 2556, Flight < 0.0008 0.0009 to 0.0016 0.0017 to 0.0032 0.0033 to 0.0064 0.0065 to 0.0128 * 354 58 205 32 * * 32 257 1998 * * * 5 7 * 9 10 2 4521 0.0129 to 0.0256 0.0257 to 0.0512 0.0513 to 0.102 0.103 to 0.205 0.206 to 0.409 46 g 4 2 0 139 366 62 17 27 51 1173 455 1376 716 2205 140 171 76 70 0 0 0 0 0 0 28 15 7 1 1 1 188 23 2 1 0 0 46 16 35 2 0 0 710 2951 3997 7303 0.410 to 0.819 0.820 to 1.64 1.65 to 3.28 3.29 to 6.75 6.76 to 13.5 13.6 to 27.0 Totals 2611 Flight T-781-A Flight T-796-A *The lack of data is the result of either an absence of particles in the size group or microscope resolution limitations or both. concentrations, the time of year, and the sampler performance was not significant. However, changes produced by the weapons tests of 1961 and 1962 could have given rise to the observed variations in the particle size distributions. Further examination of the size-distribution results reveals differences in the lower cutoff points among the test groups. These differences may be the result of different minimum sizes in the stratoSphere at the time of collection, of variation in the resolution obtained with the electron microscope, and of different particle-charging proba- bilities.* These probabilities, which are related to ion densities and particle residence times in the sampler, may have been affected by the use of different flow rates and precipitator corona currents in the tests. Because of the limitations in the collection of particles by the experimental sampler, in the evaluation of contamination, and in the subsequent size determinations (which are reflected in the wide range of median sizes reported), the results should be used only as indica- tions of the true size distributions. Similarly, the calculated particle concentration of 104 particles per cubic foot (3.5 x 107! particle per cubic centimeter) should be regarded qualitatively. *See paper by B. Y. H. Liu and K. T. Whitby, this volume.

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