IN THE MOTIONS OF THE EARTH AND VENUS. 
83 
k = 10. 
m X 
9367 . Q815 ■ !75 209 ( . 493 
+ 64 (M) “ g 6 (M) + 192 (3,0) — 32 ( 2 , 1 ) + ( 1 , 2 ) 
+ 
19 
192 
(3,1) - 11(2,2) + 3I3 (3,2) j cf'.e^ . . 
( 10 ) 
(L . e' 3 e 2 ) 
k = 11. 
w X { ^ (0)0) - (1,0) + ^ (0,1) +2L» (2,0) 
- ^ 0,D + TT (0,2) + 1 (2,1) - W (1,2) + |5 (0,3) 
+ 
32 (^) 192 384 J” • e 2 £ 
(U) 
. (L . e' 2 e 3 ) 
m 
A- = 12 . 
X { - (0,0) + ^ M - T (0,1) + 2 -^ (1,1) 
107 01 7 1 
(0,2) + gg (1,2) — -g- (0,3) + (1,3) — 32 (0,4) 
321 
~T 
+ 
768 ( lj4 )} 
( 12 ) 
C\ . eV 
( 12 ) 
(L . e e 4 ) 
k = 13. 
m 
C 240643 24571 1219 235 
X {"240- (°,°) + -g&- (°,!) + -4T (°> 2) + T 92 (°^ 3 ) 
384 3840 0^) J - ^ 
T (13) 
(L .e») 
The arguments of the cosines multiplied respectively by these coefficients, it 
must be recollected, are not similar. Their form will be determined by the 
considerations mentioned in (10). 
m 2 
