NEWTONIAN CONSTANT OF GRAVITATION. j7 
EXPERIMENT 8. 
@ = 65° — 22’ = 64° 38' 
Re => R, = 2°99304 
iii = 446650 
log 7 = 1:6499673 
p= Rsin 0 = 2704465 
6=R8 cos 0 = 1:282247 
sin 64° 38’ = 9035847 
cos 64° 38! = 4284095 
b—r =) :83559/7 
b+r = 1728897 
hy, = -0821 
Hy, = 6:048339 

hy2= 001029 
Hy? = 36°582411 
Low. High. 
P 7314131 7314131 
(b—7)? 698222 698222 
i “001029 002660 
D? 8-013382 8015013 
log D? 9038157 “9039042 
log D "4519078 4519521 
log D3 13557235 13558563 
log p ‘4320814. "4320814 
log p/D? 1:0763579 1-0762251 
log M 3°8696230 3°8696634 
log m “4234097 "4234163 
log 7 16499673. 1-6499673 
log couple 30193579 30192721 
1045°580 
1045°371 
Couple 
2090°951 
148°326 
Q = 1942:625 
104:5°371 

p? = 7314131 
(b —r)2 = -698222 
(b +r)? 89085 
hy = ‘0516 = 002660 
Hy = 6:02885 H,,2 = 36°347032 
Low. High. 
p 7314131 7314131 
(b +7)? 2-989085 2-989085 
H? 36°582411 36:347032 
46°885627 46650248 
1:6710397 1:6688539 
8355198 -+8344269 
2-5065595 2-5032808 
4320814 “4320814 
39255219 3-9288006 
38696230 38696634 
4234163 4234097 
16499673 1:64.99673 
1:8685285 1:8718410 
73:880 T4446 - 
74-446 
148:326 

In order to determine the moments of the attractions of the large balls M, M 
upon the small ones m, m, the distances represented in figure E by p and 7, and 
the true distances D between M, M and m, m are required, also the masses M, M 
MDCCCXCV.—A. 
