108 SECULAR VARIATIONS OP THE ELEMENTS OF 



. Jir _ [1.55 14854] A/ 6 -[9.4626364]A/ 5 



(382) 

 [9.4626364] AJ) t — [1.5514854] A S D 3 K 



[9.9546226] Df — [0.2789339] Df 1 * 



[9.3015115]D/'"-[0.0792616]r//"|^ - =4z> Z» Z» X>Y> ( 383 ) 

 [8.9337058] Z)/ /F — [0.0357672]D/ r J ' * 



[0.5477106] A/i -[0.6560482]A/ } ~ 



[8.0240547] A/4 -[0.0045661] A/3}^ } =(%« Zi , Xfa Z7 ). (384) 



[7.9147050] A/a -[0.0035540] A/ 6 } -^ 



If we repeat and number the formulae which we have computed, we shall have 

 the following 



Fundamental Equations for the adopted masses. 



A =# 2 +38.0686261.#+181.867616; 

 JL'=# 2 +23.1730000.#+ 98.3267843; 

 ^1"=# 2 +18.7129843.#+ 72.8326477: 

 A=# 2 +18.4080144.#+ 60.3272452; 

 ^ 2 =# 2 +13.1927088.#+ 8.981445; 

 ,4 3 =# 2 +26.3819580.#+ 9.878552; 



B =# 2 +44.5049918.#+588.053871 ; 

 Z>'=# 2 +51.9985959.#+604.943861 ; 

 Z>"=# 2 +32.1615054.#+256.0083004; 

 A=# 2 +43.8986812.#+172.462930 ; 

 A=# 2 +46.4943240.#+ 32.948353 ; 

 A=0 2 + 3.4291782.#+ 1.69251890; 



^— J 7-4-32.4501 5 J 6 ; B = {#+17.5798938 \b; \ 



B"= {#+13.138916 \b; J 



G =—{#+22.255439 \ [9.4381189]6'; " 

 C =— {#+17.6099001 \ [9.1138076]6'; 

 C"=+[0.3976676]6'; 

 <7'"=+[0.4411620]&'; 



E =— [9.9807377]6"; 

 E' =— { #+22.249552 \ [8.9723624]6"; 

 E"=— {#+17.5573735 j [9.7501125]&"; 

 E'"=— [1.0016537]Z>"; 



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