Dr. H. Kauschelbach: Harmonische Analyse der Gezeiten des Meeres. I. Teil 
51 
Argu- 
ment- 
zahl 
Koef 
fizient 
Argument 
nach Doodson in üblicher Bezeichnung 
Winkel 
geschwindigkeit 
Tiden- 
zahlen 
Tide 
10 
1 
2 
3 
4 
5 
6 
7 
8 
9 
1 GG.554 
- 
423 s 
r+ s+. h -p t 
t 
+2 h 
]> t + 90° 
y + V <■>, 
1787.76 
1787 
RP, 
13 
167.355 
26 s 
i + s + 2h-2p 
t 
+ 3/i 2p 
+ 90 
1795.7 
.555 
- 
756 s 
i + s + 2 h 
t 
+3 h 
+ 90 
7 
1797.7 
1797 
KP, 
14 
.565 
+ 
29 s 
t + s+ 2 h + N' 
t 
+ 3 ll + 
A' 
90 
1797.8 
173.445 
_ 
17s 
t+2s-2h- p AP 
t + 
s- h ■ p - 
A r ' 
+ 90 
1856.6 
.645 
18 s 
r + 2s -2A + p - N' 
t + 
s- A + p - 
A' 
90 
1858.6 
.655 
5668 
r+2s-2A+ p 
t + 
s- A+ p 
+ 90 
y + a - 2i] + to 
1858.7 
1858 
/10, 
15 
.665 
112 8 
t*2s-2h+ p+ AP 
t + 
s- A+ p + 
A 7 ' 
+ 90 
1858.8 
.765 
- 
S9C 
t+2s -2h + 2p + N’ 
/ + 
s h \-2p + 
N' 
+ 180 
1859.8 
175.445 
-f- 
87 s 
r+2s - p- N' 
t + 
s + h - p - 
A 7 ' 
- 90 
1876.6 
.455 
- 
2964 s 
i+2$ - p 
t + 
s+ A p 
+ 90 
y + a - (o 
j. 
1876.7 
1876 
Ji 
10 
.465 
- 
587 s 
r + 2 s - p + A 7 ' 
t + 
s + A - p + 
y 
+ 90 
1876.8 
.555 
- 
241 c 
x 4- 2 s 
t + 
s+ A 
+ 180 
1877.7 
.655 
+ 
46 s 
t + 2s + p 
/ + 
s+ A+ p 
90 
1878.7 
183.545 
_ 
168 
r+3s-2A - A 7 ' 
/ + 
2s- h 
N’ 
+ 90 
1957.6 
.555 
- 
492 s 
r + 3s -2A 
/ + 
2s- h 
+ 90 
y + 2 a - 21] 
so, 
1957.7 
1957 
SO, 
17 
.565 
- 
96 s 
r+3s-2A + A 7 ' 
t+2s- h 
N’ 
+ 90 
1957.8 
185.355 
_ 
240 s 
r + 3s -2p 
t + 
2s+ h -2p 
+ 90 
1975.7 
.365 
- 
48 s 
t + 3s - 2p + A 7 ' 
/ + 
2s+ h-2p + 
X’ 
+ 90 
1975.8 
.455 
- 
40c 
r+3s - p 
t- 
2s+ h- p 
+ 180 
1976.7 
.555 
- 
1623 s 
% + 3s 
t + 2 s + h 
+ 90 
y + 2(7 
00, 
1977.7 
1977 
00, 
18 
.565 
- 
1039 s 
r+3s + A' 
/+2s+ h + 
y 
+ 90 
1977.8 
.575 
- 
218 s 
r + 3s + 2A" 
/ + 
2s+ A +2A 7 ' 
+ 90 
1977.9 
195.255 
- 
19 s 
r + 4s -3p 
/ + 
3s+ h-3p 
+ 90 
1Z74.7 
.455 
311 s 
r+4s - p 
¿ + 3s+ h- p 
+ 90 
y + 3(7 - û> 
1Z76.7 
1/76 
KQ, 
19 
.465 
199 s 
x + 4 s - p + A" 
< + 3s+ h- p + 
y 
+ 90 
1Z76.8 
.475 
- 
42 s 
r + 4s - P + 2N’ 
¿ + 3s+ h- p+2N' 
+ 90 
1Z76.9 
2. Halbtägige 
Tiden. 
227.555 
- 
27 s 
2r-3s + 2 A 
2t- 
5s+ 1A 
+ 90° 
2297.7 
.645 
- 
25 c 
2r-3s+2A+ p A" 
2t- 
ÔS+1A+ ]) - 
y 
+ 180 
2298.6 
.655 
+ 
671 c 
2t-3s + 2A + p 
2t- 
ÖS+4A+ p 
2y - 5 tr + 21] + ta 
2298.7 
2298 
MAS, 
20 
235.655 
- 
156 s 
2i-2s + p 
2t- 
4s+2A+ p 
+ 90 
2378.7 
.745 
- 
86 c 
2t-2s +2p- AP 
2t 
4s+2A+2p - 
y 
+ 180 
2379.6 
.755 
~r 
2301 c 
2r-2s +2]) 
2t- 
4s+2A +2p 
2y -4a -h 2a) 
2Nj 
2379.7 
2379 
2Nj 
21 
237.545 
- 
104 c 
21 -2s + 2/i - A' 
2t- 
4s+4A 
y 
+ 180 
2397.6 
.555 
+ 
2777 c 
2z-2s + 2h 
2t- 
4s+4A 
2 y - 4 <7 + 2 >] 
,"2 
2397.7 
•2397 
.«s 
22 
245.435 
- 
63 c 
2x- s - p-2N' 
2t- 
3s+2A- p 
2 y 
+ 180 
2476.5 
.545 
- 
97 s 
2t- s - A' 
2t 
3s+2A 
y 
+ 90 
2477.6 
.555 
- 
569 f 
2t- s 
2t- 
3s+2A 
+ 90 
2477.7 
.645 
648 c 
2t - s + p - N' 
2t- 
3s+2A+ p- 
y 
+ 180 
2478.6 
.655 
+ 17387 c 
2t- s + p 
2t 
3s+2A+ p 
2y - 3 or + • 0 
N s 
2478.7 
2478 
N 3 
23 
247.445 
- 
123 c 
2t - s + 2 A - p- N' 
2t 
3s+4 A - p - 
y 
+ 180 
2496.6 
.455 
+ 
3303 c 
2t- s+2h- p 
2t- 
3s+4A - p 
2 y - 3 a + 21? - co 
2496.7 
2496 
v i 
24 
255.535 
• + 
47 c 
2t - 2 N' 
2t 
2s+2A 
2 y 
2577.5 
.545 
- 
3386 c 
2 t - N' 
2t 
2s+2A 
N’ 
+ 180 
2577.6 
.555 
+90812 c 
2t 
2t 
2s+2A 
2 y-2 a 
2577.7 
2577 
25 
.655 
+ 
86 s 
2t + p 
2t- 
2s+2A+ p 
- 90 
2578.7 
.755 
+ 
53C 
2r +2 p 
2 t 
2s \-2h v2p 
2579.7