Burnham: Measures of Proper Motion Stars 
11583. 
0 . Stone 57. (9.4 
...10.7) 
R. A. 22 
h 6 m 10 s Decl.— 
20° 42' 
1907.581 
97°6 
9 ”88 
• 675 
97.0 
9-74 
.692 
96.2 
9.88 
1907.65 
96.9 
983 
Identified as SD (20°) 6379. The corrected place for 1880 
is given above. 
11588. Ho 291. (7.2...12.7) 
R. A. 22 h 8 m 10 s Decl. + 48° 47' 
1908.594 
I98!o 
9*43 
• 597 
198.7 
10.22 
.636 
199.1 
9.41 
.652 
200.4 
9-74 
1908.62 
199-0 
9.70 
Change uncertain. 
11592. 22877. (6.4...9.6) 
R. A. 22 h 8 m 33 s Decl. + 16 0 36' 
A and B 
1910.471 
•473 
•493 
5?6 
4 - 7 
5 - 2 
I 2?59 
12.66 
12.63 
1910.48 
5-2 
12.63 
B and C (10.3) 
1910.471 
3°°°43 
IOO"92 
•473 
300.62 
101.22 
•493 
300.75 
101.02 
1910.48 
300.60 
101.05 
It is very improbable that B has any appreciable proper 
motion. Measures hereafter of the third star will show. The 
meridian values appear to be too large: 
Measures of B 
o"n6 
in 
222 °.6 
Stumpe 
0.166 
in 
230.9 
A. G. Ber. 
0.157 
in 
236.4 
Bossert 
0.142 
in 
225.2 
11596. 
Hd 170. (9.7.. 
..9.9) 
R.A. 22 h 
8 m 51 s Decl. + 16 0 38' 
1908.636 
241-5 
7"3 9 
.652 
242.8 
7-39 
.655 
242.0 
7.18 
1908.65 
242.1 
7-32 
The apparent change from the Harvard measure of 1867 is 
not confirmed. 
11601. A. G. 281. (8.8...10.0) 
R. A. 22" 9™ 9 s Decl.+ 2i J 21' 
1908.711 
22°0 
2"43 
• 750 
20.7 
2.44 
.766 
20.7 
2.47 
1908.74 
21 . I 
2-45 
11602. 02 
467 re}. 
(6.3...10.3) 
R. A. 22 h 9 m 
10 s Decl. + 21 0 56' 
1908.709 
274-1 
22'.'96 
• 7 11 
274.0 
22.86 
.728 
273.6 
23.06 
1908.72 
273-9 
22.96 
No motion. 
11613. 22890. (8.5...8.7) 
R. A. 22 11 io m 26 s Decl. + 49 0 17' 
A and B 
1910.490 
•509 
•512 
n ?9 
10.7 
11.2 
9"47 
9.20 
9.26 
1910.50 
11 .3 
9 - 3 i 
A and DM (49°) 3788 (9.3) 
1910.509 
277?63 
72 l' 9 i 
Cn 
10 
277-55 
73-02 
1910.51 
277-59 
72.96 
No change in AB. These stars form a part of h 2155. 
11625. 13 377- (8.0...) 
R. A. 22” n m 23 s Decl. + 54 0 4' 
A and B (10.6) 
I 9 H -334 
65749 
59*23 
• 375 
65.28 
58.88 
•395 
65-30 
59-12 
1911.37 
65-36 
59 -08 
A and a (13.0) 
I 9 H -395 
116? 1 
3i"8 4 
.411 
116.0 
32.07 
.468 
115.8 
3i-8o 
1911.42 
116.0 
31.90 
A and b (13.0) 
I 9 H -395 
262? 5 
37*38 
.411 
263.2 
37-44 
.468 
262.4 
37-36 
1911.42 
262.7 
37-39 
283 
