1) Refraction of Light — What and Why?
Refraction is the bending of light when it passes from one transparent medium to another. This happens because the speed of light changes when it enters a different medium.
- When light goes from a rarer to a denser medium (air → water), it bends towards the normal. Speed decreases.
- When light goes from a denser to a rarer medium (water → air), it bends away from the normal. Speed increases.
Refraction occurs because the speed of light is different in different media.
Speed of light in vacuum (c) = 3 × 10⁸ m/s (maximum possible)
2) Laws of Refraction
- The incident ray, refracted ray, and the normal at the point of incidence all lie in the same plane.
- The ratio of sin i to sin r is constant for a given pair of media. This is Snell's law.
Snell's law: sin i / sin r = constant = n₂₁
n₂₁ = refractive index of medium 2 with respect to medium 1
3) Refractive Index
Refractive index tells you how much a medium bends light — or more precisely, how much it slows down light compared to vacuum.
| Type | Formula | What it means |
|---|---|---|
| Absolute refractive index (n) | n = c / v | Speed of light in vacuum / speed of light in the medium |
| Relative refractive index (n₂₁) | n₂₁ = v₁ / v₂ = n₂ / n₁ | Ratio of speeds in medium 1 and medium 2 |
Common Refractive Indices to Remember
| Medium | Refractive Index |
|---|---|
| Air (vacuum) | 1.00 (by definition) |
| Water | 1.33 |
| Glass | 1.5 (approximately) |
| Diamond | 2.42 |
The higher the refractive index, the more optically dense the medium is. Light bends more when entering a medium with higher n. That's why diamonds sparkle so much — n = 2.42 is very high.
4) Refraction Through a Glass Slab — Lateral Shift
When light passes through a rectangular glass slab, the emergent ray is parallel to the incident ray but shifted sideways. This sideways shift is called lateral shift.
Lateral shift (T) = t × sin(i - r) / cos r
t = thickness of the glass slab
Factors Affecting Lateral Shift
- Thickness of the slab (t) — thicker slab → more shift
- Angle of incidence (i) — larger i → more shift (up to a point)
- Refractive index of the glass — higher n → more bending → more shift
- Wavelength of light — violet shifts more than red
5) Lenses — Convex and Concave
| Property | Convex Lens | Concave Lens |
|---|---|---|
| Shape | Thick in the middle, thin at edges | Thin in the middle, thick at edges |
| Nature | Converges light (converging lens) | Diverges light (diverging lens) |
| Focal length sign | Positive (+f) | Negative (-f) |
| Image types | Real + Virtual (both possible) | Always virtual, erect, diminished |
| Uses | Magnifying glass, camera, projector, eyeglasses for hypermetropia | Eyeglasses for myopia (shortsightedness), peepholes |
6) Lens Formula and Sign Convention
The lens formula is the most important tool for solving numericals. ICSE uses the Cartesian sign convention:
- Object distance (u) is always negative (object on left side of lens)
- Focal length (f) is positive for convex, negative for concave
- Image distance (v) is positive if image is on right (real), negative if on left (virtual)
- Height above principal axis = positive, below = negative
Lens formula: 1/f = 1/v - 1/u
Magnification: m = h' / h = v / u
7) Power of a Lens
Power of a lens tells you how strongly it converges or diverges light. More power = more bending.
P = 1 / f (where f is in metres)
SI unit: dioptre (D)
Convex lens: P is positive (+)
Concave lens: P is negative (-)
Combination of Lenses (Lenses in Contact)
When two lenses are placed in contact, the combined power is:
P = P₁ + P₂
1/F = 1/f₁ + 1/f₂
This is why eye doctors combine lenses: the total power is just the sum. If a convex lens of +2D and a concave lens of -1D are combined, the net power is +1D (converging).
8) Image Formation by Convex Lens (6 Cases)
| Object Position | Image Position | Nature | Size |
|---|---|---|---|
| At infinity | At F₂ | Real, inverted | Highly diminished (point) |
| Beyond 2F₁ | Between F₂ and 2F₂ | Real, inverted | Diminished |
| At 2F₁ | At 2F₂ | Real, inverted | Same size |
| Between F₁ and 2F₁ | Beyond 2F₂ | Real, inverted | Enlarged |
| At F₁ | At infinity | Real, inverted | Highly enlarged |
| Between O and F₁ | Same side as object | Virtual, erect | Enlarged |
9) Image Formation by Concave Lens (2 Cases)
| Object Position | Image Position | Nature | Size |
|---|---|---|---|
| At infinity | At F₁ (on object side) | Virtual, erect | Highly diminished |
| At finite distance | Between O and F₁ | Virtual, erect | Diminished |
10) Total Internal Reflection (TIR)
Total internal reflection is the complete reflection of light back into the denser medium when it strikes the boundary at an angle greater than the critical angle.
Conditions for TIR
- Light must travel from a denser medium to a rarer medium.
- The angle of incidence must be greater than the critical angle (i > C).
Critical Angle
sin C = n₂ / n₁
Where n₁ > n₂ (denser to rarer)
For a glass-air boundary (nglass = 1.5, nair = 1): sin C = 1/1.5 = 0.667, so C ≈ 42°. For water-air (n = 1.33): C ≈ 49°.
Real-Life Applications of TIR (ICSE Loves These!)
| Application | How TIR is Used |
|---|---|
| Optical fibres | Light signals are transmitted through thin glass fibres by repeated TIR. Used in telecommunications, endoscopy, internet cables. |
| Mirage (looming) | On hot days, air near ground is hotter (rarer). Light from sky bends away from normal → TIR occurs → you see a false reflection of the sky looking like water. |
| Sparkling diamond | Diamond has a very high n (2.42), so critical angle is very low (~24°). Light entering undergoes multiple TIRs before exiting, giving that brilliant sparkle. |
| Totally reflecting prisms | Used in periscopes and binoculars instead of mirrors. A right-angled prism can deviate light by 90° or 180° with 100% reflection. |
11) Prism — Deviation and Dispersion
A prism is a transparent medium bounded by two plane surfaces inclined at an angle of prism (A). Light passing through a prism deviates from its original path.
Angle of deviation: δ = i + e - A
At minimum deviation: i = e and δ = δm
Refractive index of prism: n = sin((A + δm) / 2) / sin(A / 2)
Dispersion of White Light
When white light passes through a prism, it splits into its constituent colours — VIBGYOR (Violet, Indigo, Blue, Green, Yellow, Orange, Red). This is called dispersion.
- Violet deviates the most (shortest wavelength, bends most)
- Red deviates the least (longest wavelength, bends least)
- Dispersion happens because different colours have different wavelengths and the refractive index of the medium is different for different wavelengths
12) Solved Numericals
Numerical 1 — Refractive Index
Speed of light in vacuum is 3 × 10⁸ m/s and in glass is 2 × 10⁸ m/s. Find the refractive index of glass.
n = c / v = (3 × 10⁸) / (2 × 10⁸) = 1.5
Numerical 2 — Snell's Law
Light enters water (n = 1.33) from air at an angle of incidence of 45°. Find the angle of refraction.
n = sin i / sin r → sin r = sin i / n
sin 45° = 0.707
sin r = 0.707 / 1.33 = 0.531
r = sin⁻¹(0.531) ≈ 32.1°
Numerical 3 — Lens Formula
An object is placed at 30 cm from a convex lens of focal length 15 cm. Find the image distance and magnification.
Given: u = -30 cm, f = +15 cm
1/f = 1/v - 1/u
1/15 = 1/v - 1/(-30)
1/15 = 1/v + 1/30
1/v = 1/15 - 1/30 = (2 - 1)/30 = 1/30
v = +30 cm (image on right side, real)
m = v/u = 30/(-30) = -1 (same size, inverted)
Numerical 4 — Power of Lens
A convex lens has a focal length of 25 cm. Find its power.
f = 25 cm = 0.25 m
P = 1 / f = 1 / 0.25 = +4 D
Numerical 5 — Combination of Lenses
A convex lens of power +3 D and a concave lens of power -2 D are placed in contact. Find the combined power and focal length.
P = P₁ + P₂ = 3 + (-2) = +1 D
f = 1 / P = 1 / 1 = 1 m = 100 cm
Numerical 6 — Critical Angle
The refractive index of diamond is 2.42. Find its critical angle with respect to air.
sin C = 1 / n = 1 / 2.42 = 0.413
C = sin⁻¹(0.413) ≈ 24.4°
13) Quick Revision — Night Before the Exam
- Refraction: bending of light due to speed change. Denser → bends towards normal
- Snell's law: sin i / sin r = n (constant for a pair of media)
- Refractive index: n = c/v. Higher n = optically denser = more bending
- Lateral shift: emergent ray is parallel to incident ray but shifted sideways
- Lens formula: 1/f = 1/v - 1/u. u is always negative
- Magnification: m = v/u = h'/h. Negative = real/inverted, positive = virtual/erect
- Power of lens: P = 1/f (in metres). Unit = dioptre (D). Convex = +, Concave = -
- Combined power: P = P₁ + P₂
- TIR conditions: denser → rarer AND i > C
- sin C = n₂/n₁ — critical angle formula
- Applications of TIR: optical fibres, mirage, diamond sparkle, totally reflecting prisms
- Dispersion: white light splits into VIBGYOR. Violet deviates most, red least
- Prism formula: δ = i + e - A. At minimum deviation: i = e
Common Mistakes That Cost Marks
- ❌ Forgetting the sign convention — u is ALWAYS negative in ICSE Cartesian system
- ❌ Using the mirror formula (1/f = 1/v + 1/u) for lenses — lens formula is 1/f = 1/v - 1/u
- ❌ Not converting cm to m for power of lens (P = 1/f where f must be in metres)
- ❌ Confusing convex and concave — convex = converging (+f), concave = diverging (-f)
- ❌ Writing "dispersion" when asked "refraction" — they're different!
- ❌ Saying TIR occurs when light goes from rarer to denser — it's the OPPOSITE (denser to rarer)
- ❌ Forgetting units: refractive index has NO unit (it's a ratio), Power = dioptre (D)
14) All Formulas at One Glance
Refractive index (absolute): n = c / v
Relative refractive index: n₂₁ = v₁ / v₂ = n₂ / n₁
Snell's law: n = sin i / sin r
Lateral shift: T = t × sin(i - r) / cos r
Lens formula: 1/f = 1/v - 1/u
Magnification: m = v / u = h' / h
Power of lens: P = 1 / f (metres) — unit: dioptre (D)
Combined power: P = P₁ + P₂
Critical angle: sin C = n₂ / n₁
Prism deviation: δ = i + e - A
Prism refractive index: n = sin((A + δm)/2) / sin(A/2)