Decay of Drop By Evaporation And Growth By Condensation

Cover Decay of Drop By Evaporation And Growth By Condensation
Decay of Drop By Evaporation And Growth By Condensation
Joseph B Keller
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2[pcl0^ t_ 1 . 9791 . 9590 . 9197 . 81^36 . 7712 . 7021 . 6362 . 5735 . 51U2 . KSQi . I|o53 . 3557 . 3091+, 2662 1 . 9790 . 9586 . 9180 . 8370 . 7563 . 6757 f . 5952 . 511+8 . L;3l|4 . 35i]-0 . 2736 . 1932 . 1126 . 0325 2, i|8lxlO R2 «2 R 1 -2 «2 h 1 . 9790 . 9586 . 9181 . 8370 . 7562 . 6755 . 591+9 . 511+3 . 1+337 . 3531 . 2725 . 1919 . 1113 . 0307 1 . 9790 . 9586 I . 9180 !
I . 8371 I i . 7565 !
I . 6760 I . 5955 I . 5151 ! . 1+3U7 : . 351+3 I . 2739 1 I i . 1936 i i . 1133 I i . 0330 1 . 979
...0 . 9586 . 9181 . 8373 . 7568 . 676U . 5961 . 5159 . 1+357 . 3555 . 2751+ . 1953 . 1153 . 0352 ^1+ . H Formula (3l+) yields 2. 1+76x10^ ! 2. 1182 x10"^ I 2. 14-38x10^ | J+ for t the value 2, 1+88 x 10^, o - 10 - rv Comparison With Previous Approximate Solutions An approximatlc^n, expected to be valid initially, can be obtained by assuming that R(t) s 1 and solving (7), (S), (10) for c(r, t) . From this solution c (l, t) can be computed and used in (9) to determine an improved R(t) . This yields the be- ginning of a solution in powers of a • We easily find that p / (36 ) c(r, t) .

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