To find the best position of a lens to give the best magnification.

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Mukwinda Phiri                                                                                                                                  11Wn        

GCSE Physics Coursework: Lenses Experiment

Aim

To find the best position of a lens to give the best magnification.

Theory

There are two basic types of lenses, convex lenses and concave lenses.  A convex lens is also called a converging lens and a concave lenis is also called a diverging lens.  Convex lenses are thicker in the middle than at the edges and concave are thinner in the middle than at the edges, which is exactly the opposite.  The diagram below shows some examples of both types of lenses.

 

Diagram 1

If a beam of light is directed parallel at a convex lens then the light is brought to focus by the lens.  If the beam of light is directed along the lens axis (the line through the centre of each surface), the rays are brought to a focus on the axis at the focal point of the lens.  The focal length (f) of a convex lens is the distance from the lens to the point where the rays are brought to a focus.

Diagram 2

If a beam of light is directed parallel at a concave lens then the light rays are made to diverge from the lens.  The focal length (f) of a concave lens is the distance from the lens to the point where the rays appear to diverge from.

Diagram 3

Ray diagrams are used for showing how images are formed and predicting where the image will be formed.  For simplicity, rays are shown bending at the line through the middle of the lens.  In reality, bending takes place at each surface.  Examples are shown below.

Lenses are made up of a large number of small-angle prisms.  Keep all the previous information in mind, at distance h from the optical centre P of a lens, (see diagram below).  If a paraxial ray (a ray that is close to the axis that is making small angles with it) parallel to the axis changes angle when heating the lens there is always going to be a small deviation (D) after.  Since the lens is small angled and is refracted trough the principal focus then the tangent of a small angle equals the small angle in radians,

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D=h

                                          FP

Diagram 4

Now look at the diagram on the next page.  If a paraxial ray from O is incident on the lens at distance h from the axis, it must also suffer deviation (D). Since all rays suffer the same amount of deviation.  In the triangle IOM, the exterior angle of a triangle equals the sum of the interior opposite angles.

Converging                                        Diverging

D=α+β                                                D=α-β

D=h        h                                         D=h         h

   OP    IP                                            IP        OP

Therefore

                

FP        OP         IP                                FP        IP         OP                                                                

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