Scientific American Supplement, No. 829, November 21, 1891 by Various
page 103 of 146 (70%)
page 103 of 146 (70%)
![]() | ![]() |
|
the mirror, and the second throwing it back to the axis of rotation,
which is at the same time the line of direction of the sight. The principle of the instrument, then, consists in causing the revolution, around the axis of rotation of the object to be observed, of a mirror parallel with such axis, and in observing it in the axis itself after sending the image to it by two reflections or two refractions. In reality, the entire instrument is contained in the small prism above, properly mounted upon a wheel that may be revolved at will; and, in this form, it may serve, for example, to determine the rotary velocity of an inaccessible axis. For this it will suffice to modify its velocity until the axis appears to be at rest, and to apply the revolution counter to the wheel upon which the prism is mounted, or to another wheel controlling the mechanism. But Mr. Thury has constructed a completer apparatus, the _cyclostat_ (Fig. 4), which, opposite the prism, has a second plate whose actuating wheel is mounted upon the same axis as the first, the gearing being so calculated that the prism shall revolve with twice less velocity than the second plate. This latter, observed through the prism, will be always seen at rest, and be able to serve as a support for the object that it is desired to examine. [Illustration: FIG. 4.--THE CYCLOSTAT. 1. General view of the apparatus. 2. Section of the ocular, O.] The applications are multitudinous. In the first place, in certain difficult cases, it may serve for the observation of a swinging |
|