5.4.7 Lens Formula

The Lens Equation

  1. The following is the lens equation that relates the object distance (u), image distance (v) and the focal length.
  2. When using the lens equation to solve problem, it's important to note the positive negative sign of u, v and f.
  3. Table below give the conventional symbol and sign for u, v and f.


Positif
Negatif
u
Real object
Virtual object
v
Real image
Virtual image
f
Convex lens
Concave lens

 

 

5.4.6 Linear Magnification

The linear magnification is a quantity that indicates the ratio of the height of the image to the height of the object.



m = linear magnification
u = distance of object
v = distance of image
hi = heigth of image
ho = heigth of object

 

5.4.4 Images Formed by Thin Convex Lens

Characteristics of the Image Formed by a Convex Lens

  1. As with a curved mirror, the position and size of an image can be found by drawing a ray diagram.
  2. Any two of the following three rays are sufficient to fix the position and size of the image.
  3. The characteristics, position and size of the image formed by a convex lens depends on the object distance (u) relative to the focal length (f)

Position of Object: u > 2f


Characteristics of the Image: Real, inverted, diminish
Distance of image: v < 2f

Position of Object: u = 2f


Characteristics of the Image: Real, inverted, same size
Distance of image: v = 2f

Position of Object: f < u < 2f


Characteristics of the Image: Real, inverted, magnified
Distance of image: v > 2f

Position of Object: u = f


Characteristics of the Image: -
Distance of image: At infinity

Position of Object: u < 2

Characteristics of the Image: Virtual, uprigh, magnified
Position of image: at the same side of the object

 

5.4.3 Ray Diagram for Lenses

Rules for Drawing Ray Diagram for Convex Lenses

  1. A light ray passes through the optical centre of the lens will not be refracted.
  2. A light ray parallel to the principle axis of the lens will be refracted passes through the principle focus.
  3. A light ray passes through principle focus will be refracted parallel to the principle axis.

Rules in Drawing Ray Diagram for Concave Lens

  1. A light ray passes through the optical centre of the lens will not be refracted.
  2. A light ray parallel to the principle axis will be refracted away from the principle focus
  3. A light ray moving towards the optical centre will be refracted parallel to the principle axis.

 

 

5.4.2 The Power of a Lens

  1. The power of a lens is defined as the reciprocal of the focal length in unit meter.

  2. Important Note: f is in meter
  3. The unit of power is diopter (D).
  4. The relationship of the power with the thickness and types of lens are shown in the diagram below.
Lens
Power of the Lens
Converging (Convex) Positive
Diverging (Concave) Negative
Thick, with short focal length. High
Thin, with long focal length. Low


Thinner – Lower Power – Longer Focal Length


Thicker – Higher Power – Shorter Focal Length


Example:
The power of a lens is labeled as +5D. What is the focal length of the lens (in cm)? Is this a concave lens or a convex lens?

Answer:



The power of the lens is positive. This is a convex lens.

 

5.4.1 Lenses

  1. There are 2 types of lenses, namely the
    1. Convex lens
    2. Concave lens
  2. Convex lenses are thickest through the middle, concave lenses are thickest around the edge, but several variations on these basic shapes are possible, as shown in figure 1. 
  3. Light rays passing through a convex or converging lens are bent towards the principal axis, whereas rays passing through a concave or diverging lens are bent away from the principal axis.

Figure 1: Convex Lenses


Figure 2: Concave Lenses

Important Terms

Optical centre, P Light passing through the central block emerges in the same direction as it arrives because the faces of this block are parallel. P marks the optical centre of the lens.
Principle Axis The principle axis of a lens is the line joining the centres of of curvature of its surfaces.
Principle focus, F The principle focus of a lens is the point on the priciple axis to which all rays originally parallel and close to the axis converge, or from which they diverge, after passing through the lens.
Focal length, f The focal length of a lens is the distance between the optical centre an the principle focus.

Rays of light can pass through a lens in either direction, so every lens has two principal foci, one on each side of the optical centre.

 

5.3.3 Phenomena Involving Total Internal Reflection

Mirage

  1. The occurrence of mirage can be explained as follows.
  2. The air on the road surface consists of many layers. On a hot day, the air near the ground has a low specific heat capacity, hence the temperature increase faster.
  3. The hot air becomes less dense than the cold air higher up.
  4. A ray of light originated from the sky is refracted away from the normal as the light is travel from denser to less dense air. 
  5. As the air passes through the lower layers, the angle of incidence increases and the refracted ray is getting further away from the normal.
  6. Finally, at a layer of air close to the road surface, the angle incidence exceeds the critical angle. Total internal occurs and the light ray bends upward towards the eye of the observer.
  7.  The observer sees the image of the sky and the clouds on the surface of the road as a pool of water.

Rain Bow

  1. The spectrum of a rainbow is caused by total internal reflection in the water droplets.
  2. Different angles of total internal reflection produces different colours.

 

5.3.2 Critical Angle and Refractive Index


The Equation Relates the Critical angle (c) with the Refractive Index

The critical angle can be calculated by using the following equation:



Requirements for Total Internal Reflection to occur.

  1. The light ray must propagate from an optically denser medium to an optically less dense medium.
  2. The angle of incident must exceed the critical angle.