Home / Notes / Class 10 / Physics / Geometrical optics
Refraction of light, Snell's law and refractive index, total internal reflection and optical fibres, prisms, lenses and the lens formula, power of a lens, the human eye and its defects, and simple optical instruments.
Geometrical optics treats light as straight lines called rays. It explains how light is reflected and refracted by mirrors, prisms and lenses. Refraction is the bending of light when it passes from one transparent medium to another, because the speed of light changes in the new medium.
Laws of refraction:
The absolute refractive index of a medium is n = c / v, where c is the speed of light in vacuum (3 × 10⁸ m/s) and v is the speed of light in the medium. It has no unit. For water n is about 1.33 and for glass about 1.5. A ray entering a denser medium bends toward the normal. A ray entering a rarer medium bends away from the normal. Refraction explains why a pool looks shallower than it is and why a straw in water looks bent.
Total internal reflection occurs when light goes from a denser to a rarer medium. As the angle of incidence grows, the refracted ray bends further from the normal. At the critical angle C, the refracted ray travels along the surface (angle of refraction 90°). Beyond C all the light is reflected back into the denser medium. The two conditions are: light travels from a denser to a rarer medium, and the angle of incidence is greater than the critical angle. The critical angle is given by sin C = 1/n.
Total internal reflection has important uses. Prisms in binoculars and periscopes turn light through 90° or 180° with almost no loss. An optical fibre is a thin glass strand with a core of high refractive index and a cladding of lower index. Light entering one end keeps reflecting inside and comes out of the other end, even when the fibre is bent. Fibres carry telephone and internet signals and are used by doctors in endoscopes to see inside the body. Diamonds sparkle because their critical angle is small (about 24°).
A prism is a transparent block with two inclined faces. A ray passing through it bends twice, and the emerging ray is deviated toward the base. White light splits into the colours of the spectrum (red, orange, yellow, green, blue, indigo, violet) because each colour has a different refractive index in glass. Violet bends the most and red the least. This splitting is called dispersion. A rainbow is formed by dispersion and internal reflection of sunlight in water drops.
Lenses and their rays:
A convex lens forms a real, inverted image when the object is beyond the focus. The image is smaller when the object is beyond 2f, the same size at 2f and larger between f and 2f. When the object is inside the focal length the image is virtual, upright and magnified, which is how a magnifying glass works. A concave lens always gives a virtual, upright and diminished image.
The lens formula is 1/p + 1/q = 1/f, where p is the object distance, q is the image distance and f is the focal length. We use the real-is-positive sign convention: distances of real objects and real images are positive, and virtual image distances are negative. Magnification m = image height / object height = q / p. The power of a lens is P = 1/f, with f in metres. Its unit is the dioptre (D). A convex lens has positive power and a concave lens negative power.
The human eye forms a real, inverted image on the retina through the cornea and a convex lens. The ciliary muscles change the focal length of the lens so that near and far objects can be focused (accommodation). In short sight (myopia) distant objects are blurred because the image forms in front of the retina. A concave lens corrects it. In long sight (hypermetropia) near objects are blurred because the image forms behind the retina. A convex lens corrects it.
A simple microscope (magnifying glass) is a convex lens of short focal length. Its angular magnification is M = 1 + d/f, when the final image is at the near point d = 25 cm. A compound microscope uses two convex lenses, an objective and an eyepiece, to give greater magnification of tiny objects. An astronomical telescope uses a long focal length objective and a short focal length eyepiece to view distant objects, with magnification M = f₀ / fₑ.
Study tip: Practise ray diagrams for a convex lens for all object positions, and learn the nature of each image in a small table. In numericals write the lens formula, keep distances in the same unit, and check the sign of q to name the image as real or virtual. Draw a neat diagram of an optical fibre and of total internal reflection with labels.
Say the meaning first, then open the card to check.
The bending of light when it passes from one medium to another.
The ratio of the speed of light in vacuum to its speed in the medium, n = c / v.
The angle of incidence in the denser medium for which the angle of refraction is 90°.
Complete reflection of light inside a denser medium at its boundary with a rarer medium.
The splitting of white light into its colours on passing through a prism.
The distance from the optical centre of a lens to its principal focus.
The unit of lens power, equal to 1 per metre of focal length.
The ability of the eye lens to change its focal length to focus objects at different distances.
Short sight: the eye sees near objects clearly but not distant ones.
| Name | Formula | What it means |
|---|---|---|
| Snell's law | n = sin i / sin r | Refractive index of the second medium relative to the first. |
| Refractive index | n = c / v | Speed of light in vacuum divided by speed in the medium. |
| Critical angle | sin C = 1/n | For light going from a medium of index n to air. |
| Lens formula | 1/p + 1/q = 1/f | Relates object distance, image distance and focal length. |
| Magnification | m = q / p | Ratio of image size to object size. |
| Power of a lens | P = 1/f | f in metres gives P in dioptre. |
| Magnifier | M = 1 + d/f | Angular magnification with image at the near point d = 25 cm. |
These are the kind of questions asked for 2, 3 and 5 marks. Try each one before opening the answer.
For light passing from one medium to another, the ratio of the sine of the angle of incidence to the sine of the angle of refraction is constant. This constant is the refractive index of the second medium relative to the first.
Rays from the coin bend away from the normal as they go from water to air. The eye traces them back in a straight line, so the coin appears at a smaller depth than it really is.
The critical angle is the angle of incidence in a denser medium for which the angle of refraction in the rarer medium is 90°. Total internal reflection needs two conditions: the light must travel from a denser to a rarer medium, and the angle of incidence must be greater than the critical angle.
An optical fibre is a thin glass strand with a core of higher refractive index surrounded by cladding of lower index. Light entering at one end strikes the core and cladding boundary at an angle greater than the critical angle, so it undergoes repeated total internal reflection and reaches the other end with little loss, even if the fibre is bent. Fibres are used to carry telephone and internet signals and in endoscopes for looking inside the body.
In myopia the image of a distant object forms in front of the retina, so distant objects are blurred. A concave lens corrects it. In hypermetropia the image of a near object forms behind the retina, so near objects are blurred. A convex lens corrects it.
The image is virtual, upright and magnified, and it forms on the same side of the lens as the object. A magnifying glass is used in this way.
Answer: n = 1.41 (no unit)
Answer: About 42°
Answer: Image at 15 cm, real and inverted, magnification 0.5 (half the object size)
Answer: (a) +4 D, (b) −2 D
Answer: M = 6