By Adorno Theodor W
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1). To simplify the problem, we can consider that the media are infinite in extent and that the interface between the media is planar. Note that a more complex geometry will not change the result. Also consider that each medium can be described by an index of refraction, n, which is the apparent speed of the wave through 37 R. Foy and F. C. ), Optics in Astrophysics, 37–48. © 2006 Springer. Printed in the Netherlands. 38 OPTICS IN ASTROPHYSICS the medium. If we pick an arbitrary point within the medium and another point Figure 1.
For a spherical mirror the conjugate points lie on top of each other at the center of curvature (COC). Light emitted from the COC of the spherical mirror will focus back onto the COC without any additional system aberration. For an elliptical mirror the two conjugates are real and located at a finite distances on the same side of the mirror. As shown in Fig. 2, light emitted from the one conjugate of the elliptical mirror will focus onto the other conjugate without any additional system aberration.
5 m telescope, which never materialized. 5 m Mt Wilson’s telescope, George Hellery Hale soon started working on his vision of a 5 m class tele- 7 In a Coudé arrangement, the image is relayed through the right ascension axis, thereby providing a fixed observing location where a bulky instrument can be mounted without jeopardizing the balance of the telescope. g. spectrographs. 8 Henrietta Leavitt, Harvard College Observatory, 1912, established the relation period-luminosity of Cepheid variable stars.