method. The actual micrometric measurements which have been made of these satellites with the largest telescopes give results which vary considerably among themselves. Hence the interest in trying the interferometer method. The apparatus used was similar to that shown in Fig. 103, i. e., it consisted of two movable slits in front of the objective of the eleven-inch glass at the Lick Observatory.
The atmospheric conditions at Mount Hamilton while the work was in progress were not altogether favorable, so that
| Number of Satellite | A. A. M. | Eng. | St. | Ho. | Bu. | ||
|
1.02 | 1.08 | 1.02 | 1.11 | 1.11 | ||
|
0.94 | 0.91 | 0.91 | 0.98 | 1.00 | ||
|
1.37 | 1.54 | 1.49 | 1.78 | 1.78 | ||
|
1.31 | 1.28 | 1.27 | 1.46 | 1.61 |
The numbers in the column marked A. A. M. are the results in seconds of arc obtained by the interference method. The other columns contain the results obtained by the ordinary method by Engelmann, Struve, Hough, and Burnham