Learning outcomes

  • Describe how converging and diverging lenses affect parallel light.
  • Define principal axis, principal focus and focal length.
  • Distinguish real and virtual principal foci.
  • Estimate the focal length of a converging lens experimentally.
9.1 Lens shapes and actions

A thin converging lens is thicker at the centre than at the edges. It refracts a parallel beam toward the principal axis so the rays meet. A thin diverging lens is thinner at the centre and spreads a parallel beam outward. The refracted rays from a diverging lens appear to originate from a point on the incident side.

The description “thin lens” means its thickness is small compared with other distances in the ray diagram, allowing refraction to be represented at one central line. Real lenses have curved surfaces and finite thickness, but the thin-lens model is accurate enough for the syllabus.

9.2 Principal axis and optical centre

The principal axis is the straight line through the optical centre and the centres of curvature of the lens surfaces. A ray passing through the optical centre of a thin lens is drawn undeviated in the simplified model.

Ray diagrams must use a ruler and show arrowheads. The lens should be centred on the principal axis, and focal points must be marked at equal distances on both sides.

Original KG2UNI diagram for Thin converging and diverging lenses
Original KG2UNI diagram: 15 lens actions
9.3 Principal focus and focal length

For a converging lens, rays parallel to the principal axis converge at the principal focus F on the far side. This is a real focus because light actually passes through it. For a diverging lens, parallel rays spread and their backward extensions meet at a virtual focus on the incident side.

Focal length f is the distance from the optical centre to the principal focus. A more powerful converging lens bends rays more strongly and has a shorter focal length. The O Level syllabus does not require a numerical lens-power equation.

9.4 Estimating focal length

Point a converging lens at a distant object, such as a building or tree, and place a white screen behind the lens. Move the screen until a sharp inverted image forms. The lens-to-screen distance is approximately the focal length because rays from a distant object reach the lens nearly parallel.

Measure from the optical centre of the lens, darken the surroundings if possible and repeat using several distant objects. Never look directly at the Sun through a lens; a focused solar image can damage eyes or cause burns.

Original KG2UNI diagram for Thin converging and diverging lenses
Original KG2UNI diagram: 32 focal length practical
9.5 Comparing lens diagrams

A converging lens is often drawn as a vertical line with outward arrowheads; a diverging lens with inward arrowheads. In full shape drawings, converging lenses bulge outward and diverging lenses curve inward at the centre.

When identifying a lens from rays, use its action rather than the sketch alone: parallel rays that converge indicate a converging lens; rays that diverge as if from a focus indicate a diverging lens.

Worked examples

Focal length estimate

A sharp image of a distant building is formed when the screen is 18.4 cm, 18.1 cm and 18.3 cm from the lens. Mean focal length ≈ 18.3 cm.

Lens identification

Parallel rays leave a lens spreading apart. Their backward extensions cross 12 cm in front of the lens. The lens is diverging and has a virtual principal focus 12 cm away.

Practical focus

Investigation

Compare two converging lenses by measuring approximate focal lengths using the same distant object. State that the shorter-focal-length lens is more strongly converging.

Examination guidance
  • A focal point is not on the lens surface; it lies on the principal axis.
  • Use “parallel to the principal axis” when stating the focus rule.
  • Do not use the Sun for a school focal-length experiment.
Check your understanding
  1. What happens to a parallel beam through a diverging lens?
  2. What is focal length?
  3. Why is the distant-object method approximate?

Answers

  1. It spreads out as if it originated from the principal focus on the incident side.
  2. The distance from optical centre to principal focus.
  3. The object is not truly at an infinite distance, so the incoming rays are only approximately parallel.