Condensation of Vapor As Induced By Nuclei And Ions

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D. s. Corona. n X io- 3 . XII 600 I O I O X-rays off farm I . 2 just seen I . 2 IOO 2. 8 5-3 IX. 600 3 4-5 4o 26 IOO 6 6 77 600 c 2 4. 1 dl ' = 24. 8 600 5-i 39 600 4.. O 18 XIII IOO o s w r o g' 216 dp = 21. 8 < :m. ter IOO 27. 6 10. w r o g 254 X. 600 IOO IOO 600 5-6 8-7 8. 8 6. 6 wp wp wr' 56 145 145 103 fcr 100 600 IOO 29. 4 ^0 6. 2 IO w r o g wrg wr og 265 no 265 600 6-5 w y 103 dp = 25. 1 ( :m. XI. 600 IOO 600 6. 5 9-5 7. 0 wog wrog' w y 112 236 119 * Terminal corona; same for 7 and 9 cells. theory of the phenomena; but the equations n = n /(A+D) 2 and n = n /(A +D), where A is constant and D the distance between bulb and fog chamber, may be adduced to accentuate the order of values observed. This has been done in case of table 32, showing that for the non-incased bulb even the inverse first power of D varies more rapidly than the observed phenomenon. To a much greater extent is this true for the wood fog chambers. The phenomenon itself is clearly a case of super- position of primary and secondary radiation.

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