18 
Aus dem Archiv der Deutschen Seewarte. 1908, Nr. 2. 
4. 
5. 
II = m cos M 
III — m sin M 
tri = cos 2 ff „ (1 + I) m 
e sin (v — v 0 ) — tri sin M 
e cos (v — v 0 ) = e„ + tri cos M 
e- — e,“ 
tri- + 2 tri cos M 
sin (rp — (p„) — (e 3 — c„ 3 ) cosec Up + (p„). 
n = tang 2 J + I (2 + I) sec 2 J j oder: 
1 _ n + sec" rp„ (c- e„-) « n + J) 2 sec 2 J sec 2 <r> 
sec 2 rp,, (e 2 — e 0 2 ) 1 
Ja 
2 ~~ '27( 0 ~ 2 1 - 
!> = — /(„2/’. 
o a. 
6. 
J [i 
-1(4- 
/ + 
/ 3 
1,5 
0 + {jg> Up: + V) + J 2 ) sin 2 l'j (- 
,<4 4~ 
/<( 
tan 
° 2 
7 - £) 
taug 2 sin a 
, , <P 
1 + tang 1 cos r 
11/ = it’ — sin ff" sin E 
n — it„ + (K —• K 0 ) + (PI — ft„) + Ja — (v 
(i. lieispiel für den Übergang auf osfenlierende Elemente. 
Die neue Oskulationsepoche sei 1894 Juni 4,0. 
Aus den Integraltafeln entnimmt man: 
I = + 8903.69 
II = — 18 134.46 
III = — 500.28 
Ferner braucht man noch aus der Störungsrechnung 
1891 Februar 0,0. M 0 - 153° 22' 25".08 
u„ = 403". 1860 
(p 0 = 4° 43' 14".2 
t — t„= 1220 rf 
/«.(< — io) = 136° 38' 6".92 
J. Mo + pio (t — to) + JM = 289° 54' 25".73 
E„ — Mo = — 4 Ü 32' 48".6d 
sin (p"o = 4.229 8092 
sin E„ = 9„984 202 8 
tang 9 " = 8.6150913 
cos E„ = 9.4230622 
tang 9 " cos E,j = 8.038153 5 
IV - + 1.26 
V = + 151.82 
J M = — 6’ 6".27. 
sin ffo - 8.915 3841 
cos (po = 9.998 524 3 
V7 = 0.3148337 
Vp u = 0.3133580 
w„ = 233° 18' 29".9 1890.0. 
tana 
log IV = 3.10037- 
log V — 5.18133-1 
io 
3. 
tang 
tang fi« = 7.919 04 
a. = + 0° 28' 31".85 
JC= 232° 49' 58".0 
log (1 + I) = 0.0003869 
tang J = 5.180 94 
tang sin E„ = 8,,599 294 1 
1 : (1 — tang cos i?,,) = 0.004767 8 
U 
J 
2 
sin IC, ■ 
-1 ff 
coser 1 
V 
B 
K — K 0 
£l — &h 0 ■ 
tang 9 - (r 
E 0 ) =- 8,,604 061 9 
v 0 — E 0 = — 4° 36' 8",51 
E„ = 285° 21' 37".Q7 
v c = 280° 45' 28".56 
sec— (K— K 0 ) = 
cos-^t/i+iQ 
tang J" 
i — 4 
)■ 
8.31 667 
= 4.879 91 
= 9„90139 
5.31443 
- 0,09573 
= — Ö".026 
= + 60". 121 
+ 0".013 
= 4- 60''.108 
-60". 160 
= 0.00000 
= 9„781 05 
0.49536 
— 1".890