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Question

The defect of hypermetropia can be corrected by using which of the following?

The correct answer is
Convex lens

Understanding Hypermetropia

Hypermetropia, also known as farsightedness, is a vision defect where a person can see distant objects clearly but faces difficulty seeing near objects distinctly. This happens because the eye's optical system converges light rays to a focal point behind the retina, rather than directly on it.

Correcting Hypermetropia

To correct hypermetropia, a lens is needed that increases the overall converging power of the eye. This helps to bend the light rays more sharply so that the image is focused precisely on the retina.

  • Convex Lens: A convex lens is a converging lens. When placed in front of the eye, it adds to the eye's refractive power, causing light rays to converge sooner and focus on the retina. This effectively corrects the defect of hypermetropia.
  • Concave Lens: Concave lenses are diverging lenses and are used to correct myopia (nearsightedness), where the focal point is in front of the retina.
  • Cylindrical Lens: These lenses are primarily used to correct astigmatism, a condition where the eye's refractive power is different in different meridians.
  • Prism: Prisms are used to correct conditions involving eye alignment or double vision, not refractive errors like hypermetropia.

Therefore, a convex lens is the appropriate choice for correcting hypermetropia.

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Important Questions from Refraction and Reflection

  1. Which of the following is NOT an example of refraction of light?

  2. If the object distance and the image distance from a concave mirror is -20 cm, what is the focal length of the mirror?

  3. Water drops shine on a lotus leaf due to:

  4. A convex lens 'A' of focal length $10 \text{ cm}$ and another convex lens 'B' of focal length $20 \text{ cm}$ are kept along the same axis with a distance '$d$' between them. If a parallel beam of light falling on 'A' leaves 'B' as a parallel beam, then the distance '$d$' in $cm$ will be :

  5. A ray is incident at an angle of incidence $i$ on one surface of a small angle prism (with angle of prism $A$ and refractive index $\mu$). The ray emerges normally from the opposite surface, causing a total angle of deviation $\delta$ from its original path. Assuming all angles are small, the angle of incidence $i$ is nearly equal to:
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