The Practical Astronomer: Comprising illustrations of light and colours--practical descriptions of all kinds of telescopes--the use of the equatorial-transit--circular, and other astronomical instruments, a particular account of the Earl of Rosse's large telescopes, and other topics connected with astronomyDick, Thomas
Science
The Practical Astronomer: Comprising illustrations of light and colours--practical descriptions of all kinds of telescopes--the use of the equatorial-transit--circular, and other astronomical instruments, a particular account of the Earl of Rosse's large telescopes, and other topics connected with astronomy
Dick, Thomas
Astronomical instruments; Astronomy; Telescopes
Concave specula have properties very different from those which are
convex; they are of more importance in the construction of reflecting
telescopes and other optical instruments; and therefore require more
minute description and illustration. Concave mirrors cause parallel
rays to converge; they increase the convergence of rays that are
already converging; they diminish the divergence of diverging rays;
and, in some cases, render them parallel and even convergent; which
effects are all in proportion to the concavity of the mirror. The
following figures show the course of diverging and parallel rays as
reflected from concave mirrors.
Fig. 20 represents the course of _parallel_ rays, and AB, the concave
mirror on which they fall. In this case, they are reflected so as to
unite at F, which point is distant from its surface _one fourth_ of the
diameter of the sphere of the mirror. This point is called the focus of
parallel rays, or _the true focus of the mirror_. And, since the sun
beams are parallel among themselves, if they are received on a concave
mirror, they will all be reflected to that point, and there burn in
proportion to the quantity of rays collected by the mirror. Fig. 21.
shows the direction of _diverging_ rays, or those which proceed from
a near object. These rays proceeding from an object further from
the mirror than the true focal point, as from D to A and to B, are
reflected converging and meet at a point F, _further from the mirror_
than the focal point of parallel rays. If the distance of the radiant,
or object D, be equal to the radius CE, then will the focal distance
be likewise equal to the radius: That is, if an object be placed in
the center of a concave speculum, the image will be reflected upon the
object, or they will seem to meet and embrace each other in the centre.
If the distance of the radiant be equal to half the radius, its image
will be reflected to an infinite distance, for the rays will then be
parallel. If, therefore, a luminous body be placed at half the radius
from a concave speculum, it will enlighten places directly before it
at great distances. Hence their use when placed behind a candle in a
common lantern; hence their utility in throwing light upon objects in
the Magic Lantern and Phantasmagoria, and hence the vast importance
of very large mirrors of this description, as now used in most of our
Light Houses, for throwing a brilliant light to great distances at sea
to guide the mariner when directing his course under the cloud of night.
[Illustration: _figure 20._]
[Illustration: _figure 21._]
When _converging_ rays fall upon a concave mirror, they are reflected
more converging and unite at a point between the focus of parallel rays
and the mirror; that is, nearer the mirror than one half the radius;
and their precise degree of convergency will be greater than that
wherein they converged before reflection.
_Of the images formed by Concave Mirrors._
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