Let EF, fig. 1, be an object, not near to ab as in the figure, but so far off that the bounding lines from A and B would meet at the point corresponding to the point P. Then if a large convex glass ab (called an object-glass) be interposed between the object and the eye, all those rays which, proceeding from P, fall on ab, will be caused to converge nearly to a point p.  The same is true for every point of the object emf, and thus a small image, emf, will be formed.  This image will not lie exactly on a flat surface, but will be curved about the point midway between A and B as a centre.  Now if the lens ab is removed, and an eye is placed at m to view the distant object EMF, those rays only from each point of the object which fall on the pupil of the eye (whose diameter is about equal to mp suppose) will serve to render the object visible.  On the other hand, every point of the image emf has received the whole of the light gathered up by the large glass AB.  If then we can only make this light available, it is clear that we shall have acquired a large increase of light from the distant object.  Now it will be noticed that the light which has converged to p, diverges from p so that an eye, placed that this diverging pencil of rays may fall upon it, would be too small to receive the whole of the pencil.  Or, if it did receive the whole of this pencil, it clearly could not receive the whole of the pencils proceeding from other parts of the image emf. Something would be gained, though, even in this case, since it is clear that an eye thus placed at a distance of ten inches from emf (which is about the average distance of distinct vision) would not only receive much more light from the image emf, than it would from the object EMF, but see the image much larger than the object.  It is in this way that a simple object-glass forms a telescope, a circumstance we shall presently have to notice more at length.  But we want to gain the full benefit of the light which has been gathered up for us by our object-glass.  We therefore interpose a small convex glass ab (called an eye-glass) between the image and the eye, at such a distance from the image that the divergent pencil of rays is converted into a pencil of parallel or nearly parallel rays.  Call this an emergent pencil.  Then all the emergent pencils now converge to a point on the axial line mM (produced beyond m), and an eye suitably placed can take in all of them at once.  Thus the whole, or a large part, of the image is seen at once.  But the image is seen inverted as shown.  This is the Telescope, as it was first discovered, and such an arrangement would now be called a simple astronomical Telescope.

Let us clearly understand what each part of the astronomical telescope does for us:—­

The object-glass AB gives us an illuminated image, the amount of illumination depending on the size of the object-glass.  The eye-glass enables us to examine the image microscopically.