To do quantitative work in optics one must understand parallax and how it may be eliminated. PARALLAX is defined as apparent motion of an object caused by actual motion of the observer.
When the observer's eye is in
position 1, objects 1 and 2 are in line and may appear to coincide. If the
eye is moved to the left to position two, object 1 (i.e. O![]() ![]() ![]() ![]() |
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As object
1 moves toward position 2 along the dotted line, its apparent displacement
with respect to object 2 caused by motion of the eye from 2 to 3 gets smaller
until it vanishes when O and O
coincide. When O
gets closer to
the eye than O
, the direction of its apparent displacement reverses
for the same eye motion.
In short, the object farthest from the eye apparently
moves in the same direction as the eye. Try this with two fingers.
Note that if O is an image and O
a cross hair, the
absence of parallax shows that the cross hairs are in the plane of the
image.
The eyepiece E slides back and forth
in the tube T and one should first adjust the eyepiece to give a clear
image of the cross hairs. Then move the tube T back and forth in the
barrel B until the image of a distant object, formed by the objective O, falls
on the plane of the cross hairs. The test for this is the
absence of parallax between
the cross hairs and image.
The rays from a distant object are nearly parallel. For viewing a distant object, use an open window if the window glass is not accurately plane. Otherwise poor image formation may result. You can check by trying it both ways. At night use a distant object in the hallway.
The telescope, now focused for parallel rays, will stay so as long as the distance between O and C is unchanged. One may still adjust the eyepiece position to suit the observer.
If you have trouble finding an image in a telescope, locate the image first with your unaided eye, and then pull the telescope in front of your eye, aligning it with your line of sight. With high magnification it is difficult to find the image in the telescope because the alignment must be nearly perfect before the image appears in the field of view. The eye has a rather large field of view so that the image will be visible over a range of positions.