A lens is an optical component made of a transparent material β usually glass or plastic β whose two surfaces are curved as portions of spheres. A lens uses the refraction of light to change the direction in which light rays travel, and therefore to form images.
| Term | English name | Definition |
|---|---|---|
| Principal axis | Principal Axis | The horizontal straight line passing through the optical centre of the lens (the axis of symmetry of the light rays). |
| Optical centre | Optical Centre | The centre of the lens; a ray passing through this point continues in a straight line, undeflected. |
| Principal focus F | Principal Focus | The point at which parallel rays parallel to the principal axis converge after passing through the lens. |
| Focal length f | Focal Length | The distance from the optical centre of the lens to the principal focus (positive for a convex lens, negative for a concave lens). |
| Point 2F | β | The point on the principal axis at a distance of 2f from the optical centre. |
| Object distance u | Object Distance | The distance from the object to the optical centre of the lens (always taken as positive). |
| Image distance v | Image Distance | The distance from the image to the optical centre of the lens (positive for a real image, negative for a virtual image). |
| Object distance u | Image distance v | Nature of the image | Application |
|---|---|---|---|
| u β β | v = f (at the focal point) | Reduced to a point | Solar concentrator |
| u > 2f | f < v < 2f | Inverted, diminished, real | Camera |
| u = 2f | v = 2f | Inverted, same size, real | One-to-one imaging |
| f < u < 2f | v > 2f | Inverted, magnified, real | Projector, slide viewer |
| u = f | v β β | No image (rays emerge parallel) | Searchlight (reverse use) |
| u < f | v < 0 (virtual image) | Upright, magnified, virtual | Magnifying glass |
| Ray | Path | Purpose |
|---|---|---|
| Ray 1 | Parallel to the principal axis β after the lens, passes through the focal point F. | Locates the image position. |
| Ray 2 | Through the optical centre β continues in a straight line, undeflected. | Determines whether the image is upright or inverted. |
| Ray 3 | Through the focal point F (or appearing to come from F) β after the lens, becomes parallel to the principal axis. | Verifies the image position. |
| Object distance u | Image distance v | Nature of the image |
|---|---|---|
| Any u (u > 0) | v < 0, and |v| < |f| | Upright, diminished, virtual |
where:
A convex lens has focal length f = 10 cm and an object distance u = 30 cm. Find the image distance v and describe the image.
Solution:
Apply the lens formula: 1/u + 1/v = 1/f
1/30 + 1/v = 1/10
1/v = 1/10 β 1/30 = 3/30 β 1/30 = 2/30
v = 30/2 = 15 cm
Magnification: m = v/u = 15/30 = 0.5 (diminished).
β Conclusion: u = 30 cm > 2f = 20 cm β inverted, diminished, real image (camera principle).
A projector lens has focal length f = 5 cm and an object distance u = 6 cm. Find the image distance v and the magnification.
Solution:
1/6 + 1/v = 1/5
1/v = 1/5 β 1/6 = 6/30 β 5/30 = 1/30
v = 30 cm
Magnification: m = v/u = 30/6 = 5 (magnified 5Γ).
β Conclusion: f < u < 2f (5 < 6 < 10) β inverted, magnified, real image (projector principle).
A magnifying glass has focal length f = 10 cm and an object distance u = 5 cm. Find the image distance v and the magnification.
Solution:
1/5 + 1/v = 1/10
1/v = 1/10 β 1/5 = 1/10 β 2/10 = β1/10
v = β10 cm (negative β virtual image)
Magnification: m = v/u = β10/5 = β2 (negative β does that mean inverted? Waitβ¦)
β Note: v is negative, so the image is virtual. In this case the sign of m flips in meaning β the actual image is upright, magnified, and virtual.
β οΈ Important: When using m = v/u for a virtual image, treat the sign carefully β use |v/u| for the magnification factor, and check upright/inverted from the ray diagram.
Treating the object distance u as possibly negative. In fact, u is always positive, because the object is in front of the lens. Only v and f carry a sign.
When applying the lens formula, all lengths must use the same unit (cm or m). Mixing cm and m produces an incorrect answer.
For a virtual image v is negative, so m = v/u is also negative β but the actual image is upright and magnified. For virtual images, use |v/u| for the size factor and rely on the ray diagram for upright/inverted.
For a concave lens f is negative. The sign must be carried into the formula β do not use |f|.
u is the distance from the object to the lens; v is the distance from the image to the lens. Under exam pressure, these are easy to swap.
A virtual image cannot be projected onto a screen β it can only be viewed with the eye or captured by a camera.
| Chinese | English | Symbol |
|---|---|---|
| ιι‘ | Lens | β |
| εΈιι‘ | Convex Lens | β |
| εΉιι‘ | Concave Lens | β |
| δΈ»θ»Έ | Principal Axis | β |
| η¦ι» | Principal Focus | F |
| η¦θ· | Focal Length | f |
| η©θ· | Object Distance | u |
| εθ· | Image Distance | v |
| ζΎε€§η | Magnification | m |
| ε―¦ε | Real Image | v > 0 |
| θε | Virtual Image | v < 0 |
1/4 + 1/v = 1/(β10)
1/v = β1/10 β 1/4 = β2/20 β 5/20 = β7/20
v = β20/7 β β2.86 cm
v < 0 β virtual image, on the same side as the object.
Magnification |m| = |v/u| = 2.86/4 = 0.715 β diminished.
Conclusion: upright, diminished, virtual image (typical concave-lens behaviour).
1/15 + 1/v = 1/10
1/v = 1/10 β 1/15 = 3/30 β 2/30 = 1/30
v = 30 cm
m = 30/15 = 2 (magnified 2Γ).
Conclusion: f < u < 2f (10 < 15 < 20) β inverted, magnified, real image (projector principle).
f = 50 mm = 0.05 m, u = 2 m = 2000 mm.
1/2000 + 1/v = 1/50
1/v = 1/50 β 1/2000 = 40/2000 β 1/2000 = 39/2000
v = 2000/39 β 51.3 mm
Conclusion: u β« f, so v β f β which is why a camera lens sits very close to the focal point.
False. A concave lens always forms an upright, diminished, virtual image β never a magnified one. To obtain a magnified image you need a convex lens with u < f (a magnifying glass).