1. Lenses and their terms
- Lens: a transparent medium bounded by two surfaces, at least one curved (usually spherical).
- Convex (converging): thicker at the middle — biconvex, plano-convex, concavo-convex. Concave (diverging): thinner at the middle — biconcave, plano-concave, convexo-concave.
- Lens as prisms: a convex lens behaves like prisms with bases towards the axis (light bends towards the axis); a concave lens like prisms with apexes towards the axis (light bends away).
- Centres of curvature, principal axis, optical centre O (ray through it is undeviated), principal foci F₁ and F₂, focal plane (plane through F normal to the axis), focal length f (distance OF).
- A lens has two principal foci, one on each side; for a thin lens in air both focal lengths are equal.
| Feature | Convex lens | Concave lens |
|---|---|---|
| Shape | Thick middle | Thin middle |
| Parallel beam | Converges to F₂ | Diverges as if from F₁ |
| Focus | Real | Virtual |
| Prism picture | Bases towards axis | Apexes towards axis |
Key terms
- Optical centre
The point on the principal axis of a lens through which a ray of light passes without deviation.
- Principal focus (convex lens)
The point on the principal axis where rays parallel to the axis meet after refraction.
- Focal length
The distance between the optical centre and a principal focus of a lens.
2. Images formed by a convex lens
Principal rays: (1) parallel to the axis → through F₂; (2) through O → undeviated; (3) through F₁ → parallel to the axis. Two rays fix the image; real where rays meet, virtual where they appear to meet.
| Object position | Image position | Nature and size | Use |
|---|---|---|---|
| At infinity | At F₂ | Real, inverted, highly diminished | Burning glass, telescope objective |
| Beyond 2F₁ | Between F₂ and 2F₂ | Real, inverted, diminished | Camera |
| At 2F₁ | At 2F₂ | Real, inverted, same size | Photocopier |
| Between F₁ and 2F₁ | Beyond 2F₂ | Real, inverted, magnified | Projector |
| At F₁ | At infinity | Real, inverted, highly magnified | Searchlight beam |
| Between O and F₁ | Same side, beyond the object | Virtual, erect, magnified | Magnifying glass |
| Object moves | Real image |
|---|---|
| From infinity towards 2F₁ | Moves from F₂ towards 2F₂ and grows |
| From 2F₁ towards F₁ | Moves from 2F₂ towards infinity and grows |
Key terms
- Real image
An image formed where refracted rays actually meet; it can be caught on a screen.
- Virtual image
An image formed where refracted rays only appear to meet when produced backwards; it cannot be caught on a screen.
3. Images formed by a concave lens
- Ray parallel to the axis diverges as if from F₁; ray through O goes straight on.
- The refracted rays never meet; produced back, they meet between F₁ and O.
- For every position of a real object the image is virtual, erect, diminished, between F₁ and O, on the object side. For an object at infinity the image is at F₁, highly diminished.
- A quick test: a lens that always gives a smaller, upright image of objects at all distances is concave.
| Object | Image (concave lens) |
|---|---|
| At infinity | At F₁, highly diminished, virtual, erect |
| Anywhere in front | Between F₁ and O, diminished, virtual, erect |
Key terms
- Diverging lens
A lens that spreads a parallel beam so that the rays appear to come from its principal focus; a concave lens.
4. Sign convention, lens formula and magnification
New Cartesian sign convention: distances from O; along the incident light (left to right) positive, against it negative; heights up positive, down negative. Hence for a real object; convex, concave; real image, virtual image.
Lens formula: . Magnification: — negative for real, inverted images; positive for virtual, erect ones.
Method: list , , with signs → substitute → solve → interpret the signs.
| u | f | v | m |
|---|---|---|---|
| −30 cm | +10 cm | +15 cm | −0.5 |
| −6 cm | +10 cm | −15 cm | +2.5 |
| −20 cm | −10 cm | −6.7 cm | +0.33 |
Formulas
- Lens formula
- Magnification
Key terms
- Linear magnification
The ratio of the height of the image to the height of the object, equal to v divided by u for a lens.
5. Power of a lens; magnifying glass; uses
- Power with in metres; unit dioptre (D); is the power of a lens of focal length 1 m. Convex: ; concave: .
- Magnifying glass (simple microscope): convex lens of short focal length; object between O and F; image virtual, erect, magnified, usually at about 25 cm from the eye. Shorter focal length → greater magnification.
- Uses: convex — magnifying glass, camera, projector, microscope and telescope lenses, spectacles for long sight; concave — spectacles for short sight, peephole, lens combinations.
| Focal length | Power |
|---|---|
| +25 cm | +4 D |
| +10 cm | +10 D |
| −50 cm | −2 D |
Formulas
- Power of a lens
Key terms
- Power of a lens
The reciprocal of the focal length of a lens expressed in metres; it measures the converging or diverging ability of the lens.
- Dioptre
The power of a lens whose focal length is one metre.
Exam tips
Common mistakes
- Taking u as positive for a real object.
- Forgetting that f is negative for a concave lens.
- Using f in cm to calculate power (power needs metres).
- Drawing virtual rays or images with full lines; missing arrows on rays.
- Calling the magnifying-glass image “real”.
How marks are usually awarded
- Ray diagrams: two correct rays with arrows (1), image correctly placed and labelled (1).
- Numericals: signed data and formula (1), substitution (1), answer with unit and interpretation (1).
- Nature of image: real or virtual, erect or inverted, magnified or diminished — all three words.