AQA · A-Level · Physics
Course version: 7408 · Version from Sept 2016
Ray diagrams and calculations of powers (in dioptres) of correcting lenses…
Full specification wording
Defects of vision and their correction using lenses (A-level only): Ray diagrams and calculations of powers (in dioptres) of correcting lenses for myopia and hypermetropia.
Myopia is short sight: the eye converges too strongly or is too long, so parallel rays focus in front of the retina and distant objects blur.
Checked against the AQA 7408 specification (opens in a new tab) on .
- Point 1 of 2
- 4 key terms
Study notes
From the checked teaching notes for this specification point.
The idea
Myopia is short sight: the eye converges too strongly or is too long, so parallel rays focus in front of the retina and distant objects blur. A diverging lens of negative power spreads rays before the eye, moving the focus back onto the retina. Hypermetropia is long sight: the eye is too weak or too short, so parallel rays would focus behind the retina and near objects blur. A converging lens of positive power adds convergence, bringing the focus forward. Lens power P is the reciprocal of focal length in metres, P = 1/f, measured in dioptres (D). In ray diagrams, draw the correcting lens in front of the eye, then show rays leaving it and focusing on the retina. For a distant object, the required power is found from the far point; for a near object, use the near point and the thin-lens equation.
What earns the marks
- Myopia is corrected with a diverging (concave) lens of negative power because the unaided eye focuses distant rays too soon.
- Hypermetropia is corrected with a converging (convex) lens of positive power because the unaided eye cannot converge near rays enough.
- Power is calculated using P = 1/f with focal length in metres, giving the unit dioptre (D).
- A correct ray diagram shows the lens in front of the eye, the object rays, and the final image formed on the retina.
- For myopia, the lens must form an image of a distant object at the eye's far point; for hypermetropia, it must help form an image of a near object on the retina.
- Sign conventions must be consistent: diverging lenses have negative focal lengths and powers, converging lenses positive.
Common mistakes and how to put them right
Using centimetres directly in P = 1/f.
Put it right: Convert focal length to metres before dividing, so 50 cm becomes 0.50 m and P = 2.0 D.
Mixing up which lens corrects which defect.
Put it right: Myopia needs a diverging lens and hypermetropia needs a converging lens.
Drawing rays that cross before the lens or focus behind the retina.
Put it right: Show the correcting lens acting first and the final focus on the retina.
Exam tips
- Write the power equation, substitute in metres, then give the answer with the correct sign and the unit D.
- Annotate ray diagrams with the lens type, the principal focus and the retinal image position to make the physics explicit.
- Check whether the question gives a far point or near point, because that determines which object distance you use in the calculation.
Try the lesson
The start of the Defects of vision and their correction using lenses (A-level only): Ray diagrams and calculations of powers (in dioptres) of correcting lenses for myopia and hypermetropia. lesson, made from checked teaching notes for this specification point.
Have a go first
A person with myopia is prescribed a diverging lens. Which statement describes the effect of this lens on the light entering the eye?
Listen
Myopia is short sight: the eye converges too strongly or is too long, so parallel rays focus in front of the retina and distant objects blur. A diverging lens of negative power spreads rays before the eye, moving the focus back onto the retina. Hypermetropia is long sight: the eye is too weak or too short, so parallel rays would focus behind the retina and near objects blur. A converging lens of positive power adds convergence, bringing the focus forward. Lens power P is the reciprocal of focal length in metres, P = 1/f, measured in dioptres (D). In ray diagrams, draw the correcting lens in front of the eye, then show rays leaving it and focusing on the retina. For a distant object, the required power is found from the far point; for a near object, use the near point and the thin-lens equation. A strong answer earns marks for these points. Myopia is corrected with a diverging (concave) lens of negative power because the unaided eye focuses distant rays too soon. Hypermetropia is corrected with a converging (convex) lens of positive power because the unaided eye cannot converge near rays enough. Power is calculated using P = 1/f with focal length in metres, giving the unit dioptre (D). A correct ray diagram shows the lens in front of the eye, the object rays, and the final image formed on the retina. A common slip: Using centimetres directly in P = 1/f. Instead, convert focal length to metres before dividing, so 50 cm becomes 0.50 m and P = 2.0 D. Exam tip: Write the power equation, substitute in metres, then give the answer with the correct sign and the unit D.
Key words
Say what each word means before you turn the card.
Myopia
Try answering aloud or in your head before turning the card.
Hypermetropia
Try answering aloud or in your head before turning the card.
Lens power
Try answering aloud or in your head before turning the card.
Dioptre
Try answering aloud or in your head before turning the card.
See every definition
- Myopia
- Short sight, where the eye converges too strongly or is too long, so parallel rays focus in front of the retina and distant objects blur.
- Hypermetropia
- Long sight, where the eye is too weak or too short, so parallel rays would focus behind the retina and near objects blur.
- Lens power
- The reciprocal of focal length in metres, P = 1/f, measured in dioptres (D).
- Dioptre
- The unit (D) of lens power, found from P = 1/f with focal length in metres.
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