804 Radiation from an Electric Source, and Line Spectra, 

 Table VIII. 



i. 



^■calc. 



^obs. 



A\. 



00 



•229902 







41 



•230220 



•230220 



bob 



40 



0236 



0238 



- -02 



39 



0253 



0259 



- -06 



38 



0272 



0283 



- -11 



37 



0292 



0303 



- -11 



36 



0313 



0324 



- -11 



35 



0337 



0346 



- -09 



34 



0362 



0373 



- -11 



33 



0384 



0400 



- -16 



32 



0420 



0429 



- -09 



31 



0454 



0163 



- 09 



30 



0491 



0499 



- -08 



29 



0531 



0541 



- -10 



28 



0576 



0587 



- -11 



27 



0626 



0648 



- -22 



26 



0681 



0690 



- 09 



25 



•230744 



•23075 



- -° 6 



24 



•23081, 



•23083 



- -1 



23 



089 3 



•23090 



- -o! 



22 



098 2 



•23100 



- -i a 



21 



108. 



•23111 



_ -2 



20 



120 3 



•23122 



- -ll 



19 



134 



•23136 



— *2 



18 



149 9 



•23152 



- -2° 



17 



168 6 



•23171 



— '2 



16 



190 8 



•23193 



- -2 4 



15 



217 4 



•23219 



- % 



14 



249 



•23252 



- '\ 



13 



289 3 



•23290 



- 'O7 



12 



338 7 



•23343 



~ % 



11 



401. 



•23405 



- "So 



10 



482 9 



•23485 



- ^ 



9 



590 g 



•23594 



- "3x 



8 



738 6 



•23739 



- -04 



7 



•239480 



•239454 



+ '26 



6 



•242585 



•242555 



+ -30 



5 



•247470 



•247513 



- -43 



4 



•255780 



•256260 



-4-80 



The agreement extends here from the highest observed 

 member, i = 41, down to i = 5, and the differences AX are, in 

 general, much smaller than in the preceding example. 



It may be interesting to remark, in passing, that the 



values of the coefficients R= — 2 —± for sodium and lithium, 

 used in (47, Na), (47, Li), and in the Tables VU. and VIII. 



