Hold a magnifying glass in sunlight and you can focus the Sun into a tiny bright spot. Hold the same lens close to a page and the letters grow. Hold it at arm's length toward a window and you see the scene upside down. One lens, three very different images. A lens is a transparent object with curved surfaces that refracts light twice, once entering and once leaving, and the shape of the curves decides whether the rays come together or spread apart.
- Thicker in the middle than at the edges
- Bends parallel rays together so they meet at a real focal point
- Can make real or virtual images
- Magnifying glass, camera, projector, eyeglasses for farsightedness
- Thinner in the middle than at the edges
- Spreads parallel rays apart as if from a virtual focal point
- Always makes small, upright, virtual images
- Peephole viewer, eyeglasses for nearsightedness
Parts of a lens
- Optical centre (O): the centre of the lens. A ray through it passes straight through.
- Principal axis: the line through O perpendicular to the lens.
- Focal points: a lens has one on each side, the same distance from O because light can pass through either way. Here F is on the object's side and F′ (F-prime) is on the far side. (Some resources swap these two labels; always check which side is which.)
- 2F and 2F′: points at twice the focal length. An object at 2F makes an image at 2F′.
- In ray diagrams the lens is drawn as a vertical line, and all the bending is shown happening at that line. This works well for thin lenses.
| Object position (converging lens) | Size | Attitude | Location | Type | Use |
|---|---|---|---|---|---|
| Beyond 2F | Smaller | Inverted | Between F′ and 2F′ | Real | Camera, eye |
| At 2F | Same size | Inverted | At 2F′ | Real | Photocopier |
| Between 2F and F | Larger | Inverted | Beyond 2F′ | Real | Movie and slide projector |
| At F | No clear image | — | — | Rays leave parallel | Spotlight, lighthouse |
| Between F and the lens | Larger | Upright | Same side as the object | Virtual | Magnifying glass |
Diverging lenses
For a diverging lens, Ray 1 travels parallel to the principal axis and refracts outward as if it came from F on the object's side; draw a dashed extension back to F. Ray 2 passes straight through the optical centre. Ray 3 is aimed at F′ on the far side and refracts parallel to the principal axis. The refracted rays spread apart, so only their dashed extensions meet, on the object's side of the lens.