Bewegungen raschlaufender Sterne. (A.9) 19
Trennung nach galaktischer Breite.
I. B > 50°.
B -R
Areal
A cos 6
Ag&
1
+ 0.017
+ 0.087
14
+ 0.011
-0.005
15
-0.015
-0.016
16
-0.119
+ 0.050
17
+ 0.036
-0.026
19
+ 0.151
-0.07!
20
-0.012
-0.038
26
+ 0.040
+ 0.002
B -R
11. 18"
Areal
Ag^cosS
Ag&
2
-0.081
„
-0.008
4
-0.064
+ 0.085
5
+ 0.250
-0.152
7
+ 0.024
-0.229
12
-0.005
+ 0.141
13
-0.035
+ 0.135
24
-0.038
-0.013
25
-0.020
+ 0.090
X = - 0^.023, in. F. + 0".056
Y = — 0 .258, m. F. + 0 .026
X = + 0.152,m.F.+ 0.027
A - 264°.9
D - +30°.5
q =0".299
m.F. einer Gleichung s— + 0".066.
< B < 50°.
+ o".
162, m.F.
+
0"
.062
— 0 .
242, m. F.
+
0
.054
+ 0 .
188, m.F.
+
0
.051
A
= 303°.8
1)
= +32".9
q
= 0".346
in. F. einer Gleichung e = + 0". 125.
III. 0" < B < 18°.
B -R
Areal
Ag^cosS
Ag&
3
+ 0.148
+ 0.046
6
-0.074
+ 0.093
8.
+ 0.103
-0.180
9
-0.102
+ 0.124
10
-0.038
-0.109
11
-0.112
+ 0.090
23
-0.132
+ 0.006
X = + 0^.107, m. F. + 0".049
Y=— 0.197, m.F. +0 .078
Z =+0.217, m.F. +0 .062
A = 298°.5
D = +44".l
q =0".312
in. F. einer Gleichung e = + 0".120.
2'
Trennung nach galaktischer Breite.
I. B > 50°.
B -R
Areal
A cos 6
Ag&
1
+ 0.017
+ 0.087
14
+ 0.011
-0.005
15
-0.015
-0.016
16
-0.119
+ 0.050
17
+ 0.036
-0.026
19
+ 0.151
-0.07!
20
-0.012
-0.038
26
+ 0.040
+ 0.002
B -R
11. 18"
Areal
Ag^cosS
Ag&
2
-0.081
„
-0.008
4
-0.064
+ 0.085
5
+ 0.250
-0.152
7
+ 0.024
-0.229
12
-0.005
+ 0.141
13
-0.035
+ 0.135
24
-0.038
-0.013
25
-0.020
+ 0.090
X = - 0^.023, in. F. + 0".056
Y = — 0 .258, m. F. + 0 .026
X = + 0.152,m.F.+ 0.027
A - 264°.9
D - +30°.5
q =0".299
m.F. einer Gleichung s— + 0".066.
< B < 50°.
+ o".
162, m.F.
+
0"
.062
— 0 .
242, m. F.
+
0
.054
+ 0 .
188, m.F.
+
0
.051
A
= 303°.8
1)
= +32".9
q
= 0".346
in. F. einer Gleichung e = + 0". 125.
III. 0" < B < 18°.
B -R
Areal
Ag^cosS
Ag&
3
+ 0.148
+ 0.046
6
-0.074
+ 0.093
8.
+ 0.103
-0.180
9
-0.102
+ 0.124
10
-0.038
-0.109
11
-0.112
+ 0.090
23
-0.132
+ 0.006
X = + 0^.107, m. F. + 0".049
Y=— 0.197, m.F. +0 .078
Z =+0.217, m.F. +0 .062
A = 298°.5
D = +44".l
q =0".312
in. F. einer Gleichung e = + 0".120.
2'