Lens
Lens
is an optical device that is widely used in everyday life. Practically
every adult wears a spectacle which is constructed out of lenses.
Lenses are classified according to the geometry and combination of the surfaces. Lenses are commonly used to form images by refraction in optical instruments such as cameras, telescopes, and microscopes.
Lenses are classified according to the geometry and combination of the surfaces. Lenses are commonly used to form images by refraction in optical instruments such as cameras, telescopes, and microscopes.
Lens Definition
Lens
is an optical device. It is formed by combination of two curved
surfaces, mostly spherical surfaces with a common axis. It allows light
and because of the curvatures and of the material of the lens it also
gets refracted. Lenses are made of glass or transparent polycarbonate or
transparent plastic materials. For the purpose of safety, polycarbonate
materials are preferred for making lenses.
Lenses are
classified as per the types of surfaces used and also the combination of
the surfaces. The shapes of common types of lenses are shown below.
A lens in which both the outer surfaces are
concave outside the plane of lens is called a biconvex lens or simply
convex lens. A lens in which both the outer surfaces are sunk inside the
plane of lens is called a biconcave lens or simply concave lens. Of one
of the surfaces of the lens is plain then it is either called a plano
convex lens or a plano concave lens depending on what the other surface
is.
Lens Focal Length
The relationship between distance of the object (u), distance of the image (v) and focal length (f) of the lens is called lens formula or lens equation.
This lens formula is applicable to both convex and concave lenses.
We
said that the lens surfaces are spherical. The center of the spherical
surface is called the center of curvature and its distance from the
center of lens is called the radius of curvature. Half the radius of
curvature is defined as the focal length of the lens. The point which is
on the principal axis and away at a focal length from the lens is
called ‘focus’ of the lens. This point is so called because the parallel
rays that enter the lens converge (or deem to converge) together at
this point.
Points
to be remembered while using the lens formula. The values of the known
parameters should be used with their proper sign as per the sign
convention. No sign be assigned to the unknown parameter during
calculations.
Converging Lens
A
biconvex lens or a plano convex lens converges parallel light rays that
enter on one side to a point on the axis on the other side of the lens.
Hence, a biconvex or a plano convex lens is called a converging lens.
The point where the rays actually converge is called the focus of the
lens and the distance of the focus from the lens is called focal length
of the lens.
1. When the Object is Placed between F1 and O:
Formation of Image by a Convex Lens
The image is -
2. When the Object is Placed between the Optical Center (O) and first Focus (F1)
The image is -
The image is
The image is -
The image is -
7. When the Object is Placed at Infinity
The image is -
The image is -
- Formed on the same side of the lens
- Virtual
- Erect
- Magnified
2. When the Object is Placed between the Optical Center (O) and first Focus (F1)
Here we consider two rays starting from the top of the object placed at F1 and optical center. The ray parallel to the principal axis after refraction passes through the focus (F2).
The ray passing through the optical center goes through the lens
undeviated. These refracted rays appear to meet only when produced
backwards. Thus, when an object is placed between F1 and O of
a convex lens, a virtual, erect and magnified image of the object is
formed on the same side of the lens as the object.
3. When the Object is Placed at 2F1
- Formed at 2F2
- Real
- Inverted
- Same size as the object
Here one of the rays starting from the top of the object placed at 2F1
passes through the optic center without any deviation and the other ray
which is parallel to the principal axis after refraction passes through
the focus. These two refracted rays meet at 2F2. Thus, when an object is placed at 2F1 of a convex lens, inverted and real image of the same size as the object is formed at 2F2 on the other side of the lens.
4. When the Object is Placed between F1 and F2- Formed beyond 2F2
- Real
- Inverted
- Magnified
Let
us consider two rays coming from the object. The ray which is parallel
to the principal axis after refraction passes through the lens and
passes through F2 on the other side of the lens. The ray
passing through the optic center comes out of the lens without any
deviation. The two refracted rays intersect each other at a point beyond
2F2. So, when an object is placed between F1 and 2F1 of a convex lens the image is formed beyond 2F2.
5. When the Object is Placed at F1- Formed at infinity
- real
- Inverted
- Magnified
Here
again we consider two rays coming from the top of the object. One of
the rays which is parallel to the principal axis after refraction passes
through F2 and the other ray which passes through the
optical center comes out without any deviation. These two refracted rays
are parallel to each other and parallel rays meet only at infinity.
Thus, when an object is placed at F1 of a convex lens, the image is formed at infinity and it is inverted, real and magnified.
6. When the Object is Placed beyond 2F1- Formed between F2 and 2F2
- Real
- Inverted
- Diminished
The ray parallel to the principal axis after refraction passes through F2
and the ray which passes through the optical center comes out without
any deviation. The refracted rays intersect at a point between F2 and 2F2. The image is inverted, real and diminished.
7. When the Object is Placed at Infinity
The image is -
- Formed at F2
- Inverted
- Real
- Highly diminished
The
table below gives at a glance the position, size and nature of the
image formed by a convex lens corresponding to the different positions
of the object and also its application.
Position of the object | Position of the image | Nature of the image | Size of the image | Application |
---|---|---|---|---|
Between O and F1 | on the same side of the lens | Erect and virtual | Magnified | Magnifying lens (simple microscope), eye piece of many instruments |
At 2F1 | At 2F2 | Inverted and real | Same size | Photocopying camera |
Between F and 2F1 | Beyond 2F2 | Inverted and real | Magnified | Projectors, objectives of microscope |
At F1 | At infinity | Inverted and real | Magnified | Theatre spot lights |
Beyond 2F1 | Between F2 and 2F2 | Inverted and real | Diminished | Photocopying (reduction camera) |
At infinity | At F2 | Inverted and real | Diminished | Objective of a telescope |
Convex Lens Examples
The simplest example is the magnifying glass. The letters which are too
small to read can easily be read by using a convex lens as a magnifying
glass. The lens is held in such a way that the letters are within the
focal length of the lens. Hence the letters are magnified and in upright
position to make it easy to read. The same principle is used in
spectacles which are used for correction of hyperopia. In olden days,
convex lens were used to ignite by allowing the sun rays to be focused
on the object to be ignited. Here the lens converge the heat rays just
like converging the light rays.
When a set of parallel rays enter a biconcave lens or a plano concave lens, it diverges the light rays on the other side of the lens. Hence, a biconcave or a plano concave lens is called a diverging lens. However these divergent rays give an impression that they emerge from a point on the axis at the same side of entry of the rays. It is a virtual point and not real. This point is called the focus and its distance from the lens is called focal length of the concave lens.
When the Object is at Infinity:
The image is -
When the Object is Placed between O and F:
The image is -
The image is -
The image is -
- Formed at F1
- Erect
- Virtual
- Diminished
When the Object is Placed between O and F:
The image is -
- Formed between O and F1
- Erect
- Virtual
- Diminished
When the Object is Placed at any Position between O and Infinity:
The image is -
- Formed between O and F1
- Erect
- Virtual
- Diminished
We have learned that the convex lenses converges the parallel rays to
the focus on the other side of the lens. In other words, a ray of light parallel
to the axis of the length will pass through the focus on the other side.
A ray of light which passes through the optical center of the lens proceeds
without any refraction. Hence the intersection of these two rays happens
to be on the other side of the lens, there will be Real Image and
inverted. But if the intersection do not actually occur on the other
side and appears to intersect on the first side, then the image will be Virtual Image and upright.
But in case of concave lenses, the rays always
get diverged and they can only ‘virtually’ intersect on the same side as
the rays enter. Hence the images formed by concave lenses are always
virtual images.
Let us make a table of comparison between these two lenses which can show the differences of their features side by side.
Convex Lens | Concave Lens |
The outer surfaces bulge out from the center line | The outer surfaces shrink towards the center line |
Parallel rays that enter on one side get converged on the other side. | Parallel rays that enter on one side get diverted on the other side. |
The focal length is positive. | The focal length is negative. |
The images formed are real excepting when the object is within the focal length | Only Virtual Images are formed in all cases. |
Images are inverted and form on the other side of the lens, excepting when the object is within the focal length | Images (virtual) are always upright |
Mainly used in optical instruments and less used as corrective lenses in spectacles. | Mainly used as corrective lenses in spectacles and less used optical instruments. |
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