SECULAR VARIATIONS OF THE ELEMENTS OP 



d= J4.365092844 ^}[9.2840950]ft 2 ; 

 C,= 10.6879108996 ^|[9.1824311]6 2 ; 

 C t = [0.68323 17]Z> 2 ; 

 (7 4 = [0.6834824]i 2 ; 



^=+[7.8267723]^; 



E 2 = |43.7345641 -^|[8.2017618]& 3 ; 



E 3 = 1 0.648004419 #j[0.7610455]& 3 ; 



j& 4 =+[1.0655652]6 3 ; 



^ 1= _[7.0339474]& 4 ; 



^ 3 = \ 2.770664438 g \ [1.7737962]6 4 ; 

 <= j 50.3649997 ^}[9.1128486]6 4 ; 



(186) 



(187) 



(188) 



(191) 



0_47.8463930./+796.2()272817.<f-5344.10960488.<7 \ , ,. 



+ 12307.3911771 j " 

 ^-29.5229572./+172.74076612./- 323.31739720.flr) ' , 



+140.47094066 j " 



And lastly, the values of b L , b 2 , b 3 , and & 4 become, 



b l= \ 0.00002188686 [95.3401834] ^+[96.8635004]Ar' 



+[97.3236905] ^"+[97.0504994]^'" ; 



b,= \ 0.00000 1420383 .... [94.1 524054] |# +[95.6682302]^' 



+[96.1186392] ^"+[95.8170069]^'"; 



6 8 = j 0.0000000610884 . . . [92.7859587] \N +[94.2994239]^' 



+[94.7468016] ^"+[94.4366545]^'" ; 



1 4 =\ 0.0000000081 2296 . . [91.9097143] {# +[93.4227230]^' 



+[93.8695157] ^"+[93.5577417]^'". 



The values of 6, V, J", and V remain the same as in equations (118). 

 Equations (189) and (190) give, when the second members are put^equal to 0, 



g= 5".34449540; g t = 0".616685510; % 



ffi = 7.53805074; g b = 2.72773208; 



^=17.12785195; g,= 3.71791243; 



#,=17 .83599491 ; #=22 .46062783. 



The solutions of equations (170-191) will now give the following values, re- 

 membering that the coefficients of equations (84-97) remain unchanged. For the 

 root g, we get, 



(192) 



^=5".3446763 ; 

 N 1 =+0.10318901^ 

 N" =+0.0652640tf 

 N" =+0.01001010^ 

 N" =0.0001 170589 N 

 N r = 0.0001036091^ 

 tf r/ =+0.0000476249JV 

 JV r "=+0.000000750320# 



log. 99.0136340; 



" 98.8146736; 



" 98.0004383 ; 



" 96.0684043; 



" 96.01 53978n; 



" 95.6778341 ; 



" 93.8752464, 



