Full text: The collected mathematical papers of Arthur Cayley, Sc.D., F.R.S., sadlerian professor of pure mathematics in the University of Cambridge (Vol. 7)

476] ORBIT OF A PLANET FROM THREE OBSERVATIONS. 443 
or developing, this is 
6 (sin 2 c — 3 cos 2 c), 
-= i 4r\ (sin 2 c — 3 cos 2 c) cos c 
\/3 1 
— r 2 (sin c + 2 cos c) (sin 2 c — 3 cos 2 c) 
+ r 3 (sin c — 2 cos c) (sin 2 c — 3 cos 2 c)} 
+ y {— 2r x sin C COS G 
+ r 2 (— sin 2 c + sin c cos c + 6 cos 2 c) 
+ r 3 ( sin 2 C 4- sin c cos c — 6 cos 2 c)} 
i — 6 cos 2 c 
\/3 1 
+ 3r 2 (sin 2 c + sin c cos c — 2 cos 2 c) 
+ 3 r 3 (sin 2 c — sin c cos c — 2 cos 2 c){ = 0; 
(observe that the orbit will be a right line if sin 2 c — 3 cos 2 c = 0, that is if c = 60°, 
which is right, since 60° is the angular radius of the regulator circle). 
89. Putting in the equation tan c = A, and therefore cos c = — - , the equation 
becomes 
We have 
bVl + X 2 
^4rj — (X + 2) r 2 + (X — 
1 
+ 
(2X + (X + 2) (X — 3) 
2 V3 (X 2 - 3) V 
1 
+ 2 (X 2 - 3) 
^— 2r : + (X — 1) (X + 2) 
- Vi + x 2 
x x = V1 + X 2 , 
X + 2 ’ 
1 . 
1 2A+3 
^+2 ’ 
Vi+x 2 
A —2 ’ 
1 2A-3 
V3 X-2 ’ 
and thence, writing for shortness 
E 1 = Vl + f X 2 , 
E, = ~ V7X 2 + 12X + 12, 
" Vs 
jR 3 =4r V7X 2 - 12X + 12, 
V3 
56—2
	        
Waiting...

Note to user

Dear user,

In response to current developments in the web technology used by the Goobi viewer, the software no longer supports your browser.

Please use one of the following browsers to display this page correctly.

Thank you.