Diagram
Ray diagrams for image formation by lenses

Ray diagram for image formation by lenses is shown in the attached figure.
Diagram
Images formed in different lenses
Definition
Images Formed By Lenses
Image formed by convex lens placed at different distances is shown in the figure
Definition
Images through lenses as real, virtual, erect or magnified
Figure shows the virtual image formed by convex lens and real image formed by concave lens.
Diagram
Different images through lenses
Characteristics of image formed by convex lens is summarized in the table below:
Concave lens form virtual and erect image on the same side of the lens between and . It is always diminished. They are used in Galilean telescope.
Object position | Image position | Image size | Nature of image | Application |
Infinity | Point-sized | Real, inverted | Burning glass, To concentrate solar energy on small photovoltaic cells | |
Beyond | Between and | Diminished | Real,, inverted | Camera lens |
At | At | Same size as object | Real, inverted | Telescope |
Between and | Beyond | Magnified | Real, inverted | Slide projector |
At | infinity | Highly magnified | Real, inverted | Spectrometer |
Between and | On same side as object | Magnified | Virtual, erect | Magnifying glass |
Diagram
Characteristics of images by symmetrical lens
Characteristics of image formed by convex lens is summarized in the table below:
Concave lens form virtual and erect image on the same side of the lens between and . It is always diminished. They are used in Galilean telescope.
Object position | Image position | Image size | Nature of image | Application |
Infinity | Point-sized | Real, inverted | Burning glass, To concentrate solar energy on small photovoltaic cells | |
Beyond | Between and | Diminished | Real,, inverted | Camera lens |
At | At | Same size as object | Real, inverted | Telescope |
Between and | Beyond | Magnified | Real, inverted | Slide projector |
At | infinity | Highly magnified | Real, inverted | Spectrometer |
Between and | On same side as object | Magnified | Virtual, erect | Magnifying glass |
Result
Image formation by lenses
Characteristics of image formed by convex lens is summarized in the table below:
Concave lens form virtual and erect image on the same side of the lens between and . It is always diminished. They are used in Galilean telescope.
Object position | Image position | Image size | Nature of image | Application |
Infinity | Point-sized | Real, inverted | Burning glass, To concentrate solar energy on small photovoltaic cells | |
Beyond | Between and | Diminished | Real,, inverted | Camera lens |
At | At | Same size as object | Real, inverted | Telescope |
Between and | Beyond | Magnified | Real, inverted | Slide projector |
At | infinity | Highly magnified | Real, inverted | Spectrometer |
Between and | On same side as object | Magnified | Virtual, erect | Magnifying glass |
Result
Experimental determination of focal length of lenses

To determine the focal length of convex lens:
Refer the diagram (Figure 1):
The lens is set up in a suitable holder with a plane mirror behind it so that light passing through the lens is reflected back again.
The object used is a hole and cross-wire in a white screen illuminated by a pearl electric lamp.
The position of the lens holder is adjusted until a sharp image of the object is formed on the screen alongside the object itself.
The object will now be situated in the focal plane of the lens, i.e., a plane through the principal focus at right angles to the principal axis
Under these conditions, rays from any point on the object will emerge from the lens as a parallel beam.
They are therefore reflected back through the lens and brought to a focus in the same plane as the object.
The distance between lens and screen now gives the focal length of the convex lens.
To determine the focal length of concave lens (out of contact method):
Arrange the apparatus as shown in the diagram (Figure 2).
The real image formed by the convex lens will act as the virtual object for the concave lens. When concave lens is interposed between the convex lens and the real image , the new real image is formed at . If u is the distance of the concave lens from the virtual object and is the distance of the concave lens from the real image , then the focal length of the given concave lens is,
or
Refer the diagram (Figure 1):
The lens is set up in a suitable holder with a plane mirror behind it so that light passing through the lens is reflected back again.
The object used is a hole and cross-wire in a white screen illuminated by a pearl electric lamp.
The position of the lens holder is adjusted until a sharp image of the object is formed on the screen alongside the object itself.
The object will now be situated in the focal plane of the lens, i.e., a plane through the principal focus at right angles to the principal axis
Under these conditions, rays from any point on the object will emerge from the lens as a parallel beam.
They are therefore reflected back through the lens and brought to a focus in the same plane as the object.
The distance between lens and screen now gives the focal length of the convex lens.
To determine the focal length of concave lens (out of contact method):
Arrange the apparatus as shown in the diagram (Figure 2).
The real image formed by the convex lens will act as the virtual object for the concave lens. When concave lens is interposed between the convex lens and the real image , the new real image is formed at . If u is the distance of the concave lens from the virtual object and is the distance of the concave lens from the real image , then the focal length of the given concave lens is,
or
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