Reflector (optics)

Definition and stakes

Henry Coddington,  An Elementary Treatise on Optics (1823)

“ It is, however, to be observed, that the small reflector is usually of very confined dimensions, and when the object speculum is well ground, it is found that the lateral rays converge quite sufficiently well to make a distinct image.
To find the magnifying power, we must compare the angle subtended by the second image at the eye glass with that of the object or first image at the center of the great mirror: but since the focal length of the mirror is half its radius, this is the same thing as the angle of the first image seen from the mirror.
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Source: Wikisource

Henry Coddington,  An Elementary Treatise on Optics (1823)

“ Making infinite, or we find , or as before, so that the principal focus is here at the bisection of the radius of the reflector, and of course behind it. In fact, as long as is positive, or is in front of the mirror, so long must necessarily be behind it, and the reflected rays diverge.
If, however, the incident rays converge to a point behind the mirror, that is, be negative, the formula will become
or and may be positive, provided that is, so that if the focus of the incident rays lie between the principal focus and the back of the mirror, the reflected rays will converge.
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Source: Wikisource

ScienceApologist/Optics workshop

“ I've looked at this more carefully, and while I agree that there are three physical reflections, I believe that the "third" reflection, being mutually perpendicular to the other two, will not cause a third mirror image to form (since it is mutually perpedicular) . Therefore, I think that the three corner reflector only has two parity operations. Of course, we can check this out by looking at one's image in a three-corner reflector. User:ScienceApologist OK, I arranged three mirrors mutually perpendicular. ”
Source: Wikisource

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