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Light - Part XI |
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Case
5
: Image formed by a convex lens when the object is placed at a distance beyond 2 F1. Consider the following figure. Let
the object be a candle AB placed at a distance beyond 2 F1. Applying
similar treatments for the rays of light emanating from two extremes of the
candle AB. A ray of light AD parallel to XY will be deflected along DF2A’
(rule1). Another ray of light AO will be refracted along AOA’ (rule 2).
Where the two rays DF2A’and AOA’ meet, we get the image of A
as A’. As explained earlier, light from B will go un-deflected along XY
path. The image of AB is A’B’. Clearly the image is reduced and
inverted. The image is formed
between F2 and 2 F2. Thus
we can conclude that for an image of an object placed at a distance beyond
the 2 F1 of a convex lens:
The
above geometry is used in a simple camera lens, where the picture is reduced
in size and is taken on a photographic film. Case
6
: Image formed by a convex lens when the object is placed at a distance far
off (or infinite distance) beyond 2 F1. Consider the following figure. Let
the object be a candle AB placed at infinity.
B is still on line XY. Rays emanating from A are striking the mirror
in parallel fashion. They will be refracted and they will meet at the focal
point F2 Thus
we can conclude that for an image of an object placed at an infinite
distance beyond 2 F1 of a convex lens :
The
geometry used in case 6 is what happens in a telescope that collects light
from objects such as stars placed at infinity. Uses
of convex lenses
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