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Equations (38a,b,c and d ) are based on t h e known asymptotic behavior o f n ( x ) and w(x). I2 correspond G ( l ) and G ( 2 ) i n equation (26) t o G('), respectively, The values of k a n d Q tabulated in Table I are believed t o be a c c u r a t e r Co one u n i t i n t h e last place printed. The wave f u n c t i o n s u ( x ) and w(x) tabulated i n Table I1 were obtained from t h e last i t e r a t i o n . These f u n c t i o n s A t each s t a g e of t h e eompu- a m estimated t o be accurate ta one p a r t i n 10'.

73 x 10-27cm2 p l u s and minus two and one-half percent. The l a s t iterates u(x) and w(x) f o r t h e prev%ously computed case w i t h c l o s e s t y v a l u e were used as t h e f i r s t approximation t o t h e wave functions. 1 pereent of i t s f i n a l value. However, Q was q u i t e s e n s i t i v e t o t h e wave f u n c t i o n s and after two i t e r a t i o n s o f t e n had not completely s e t t l e d down, I n t h e few cases where two i t e r a t i o n s and the use of equations (36) and (39) were i n s u f f i c i e n t t o y i e l d t h e d e s i r e d accuracy i n L a n d Q, wave f u n c t i o n s u,(x) and w ( x ) were computed by use o f the followfng e x t r a p o l a t i o n 3 formulas obtained from equation (26) I -a- and Then u,(x) and w3(x) were introduced i n t o equations (32a and b) and t h e iterates u4(x) and w ( x ) obtained.

52186 4 4 ,52186 5 . 6264. 52188 and the I n t h i s case t h e extrapolated values of k a n a Q were within t h e d e s i r e d accuracy and t h e r e f o r e served as a check on t h e e x t r a p o l a t i o n process, A t y p i c a l case i n which two i t e r a t i o n s were s u f f i c i e n t i s shown i n Table VII, 3'. 6797 2 9 57270 The extrapolated value of' "h i s 9,57266 and t h e extrapolated value of Q is 2,6888. I n t h i s p a P t i d a r ease t h i r d f t e r a t f o a values of X ( 9 .

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