Wave Optics is Chapter 10 of NCERT Class 12 Physics Part II and part of Unit 16, Optics, in both the NEET UG and JEE Main syllabi. These notes cover wavefronts and Huygens principle, reflection and refraction of plane waves, coherent sources, Young’s double-slit experiment and fringe width, single-slit diffraction and polarisation with Malus’ law, plus a free notes PDF.
Wave Optics Notes for NEET and JEE Main
Section-wise key points from NCERT Chapter 10, formula tables, high-yield facts and common mistakes for 2027 revision.
Wave Optics at a Glance
| Item | Details |
|---|---|
| Syllabus unit | NEET UG 2026 and JEE Main 2026: Unit 16, Optics |
| Exams that cover it | Both NEET UG and JEE Main (Paper 1); the topic is listed in the 2026 syllabus of each |
| NCERT textbook | Physics Part II, Class 12, Chapter 10 (rationalised book) |
| Other chapter in the unit | Ray Optics and Optical Instruments (Chapter 9) |
| Syllabus topics | Wavefront and Huygens’ principle; laws of reflection and refraction using Huygens’ principle; interference, Young’s double-slit experiment and expression for fringe width; coherent sources and sustained interference of light; diffraction due to a single slit, width of central maximum; polarisation, plane-polarised light, Brewster’s law, uses of plane-polarised light and Polaroid |
| Official chapter | NCERT Chapter 10 |
| Notes PDF | View PDF (AglaSem Class 12 notes for Electromagnetic Waves and Optics) |
The topic list follows the NEET UG 2026 syllabus released by the National Medical Commission (NMC) on 22 December 2025 and the JEE Main 2026 syllabus released by NTA on 31 October 2025, which stay the reference until the 2027 syllabi are out. Full lists: NEET syllabus and JEE Main syllabus.
How did the wave theory of light develop?
The wave model of light, put forward by Christiaan Huygens in 1678, correctly predicted that light slows down in a denser medium, which the corpuscular model got wrong.
- Descartes (1637) gave the corpuscular model and derived Snell’s law; Newton developed it in his book Opticks.
- The corpuscular model predicted that light bending towards the normal would travel faster in the second medium; the wave model predicted it would travel slower.
- Foucault (1850) showed light is slower in water than in air, confirming the wave model.
- Thomas Young’s interference experiment (1801) firmly established that light is a wave.
- Geometrical (ray) optics is the limit in which the wavelength is neglected; a ray is the path of energy propagation as wavelength tends to zero.
- Maxwell’s electromagnetic theory explained how light waves travel through vacuum.
Wavefront and Huygens Principle
A wavefront is a surface of constant phase, and Huygens principle says every point on a wavefront is a source of secondary wavelets whose forward envelope gives the wavefront at a later time.
- Energy of the wave travels perpendicular to the wavefront; the speed of the wavefront is the speed of the wave.
- A point source gives spherical wavefronts; far from the source a small part looks plane (plane wave).
- To find the wavefront after time t, draw spheres of radius vt from each point and take the common tangent (forward envelope).
- Huygens assumed the wavelets have zero amplitude backwards to explain why there is no backwave; the proper justification comes from more rigorous wave theory.
Reflection and Refraction Using Huygens Principle
Huygens construction gives Snell’s law as sin i/sin r = v₁/v₂ = n₂/n₁, and the law of reflection as i = r.
- Refractive index n = c/v, so n₁ sin i = n₂ sin r.
- If r < i (bending towards the normal), then v₂ < v₁: light is slower in the denser medium.
- On refraction, speed and wavelength change (λ₁/λ₂ = v₁/v₂) but frequency stays the same.
- From a denser to a rarer medium, sin i_c = n₂/n₁; beyond the critical angle there is no refracted wave (total internal reflection).
- Reflection: the triangles formed by incident and reflected wavefronts are congruent, so the angle of incidence equals the angle of reflection.
- A thin prism tilts a plane wavefront; a convex lens turns it into a spherical wavefront converging at the focus; a concave mirror also makes it converge to the focus.
- The time taken from a point on the object to the corresponding point on the image is the same along every ray.
Coherent and Incoherent Addition of Waves
Two sources are coherent when the phase difference between their waves at any point does not change with time; only coherent sources give a stable interference pattern.
| Condition | Path difference | Phase difference | Resultant intensity |
|---|---|---|---|
| Constructive interference | nλ (n = 0, 1, 2, …) | 0, ±2π, ±4π, … | 4I₀ |
| Destructive interference | (n + ½)λ | ±π, ±3π, … | 0 |
| General point (coherent) | Any | φ | I = 4I₀ cos²(φ/2) |
| Incoherent sources | Phase difference changes rapidly | Varies | Average I = 2I₀ (intensities simply add) |
- Interference is based on the superposition principle: the resultant displacement is the vector sum of individual displacements.
- Intensity is proportional to the square of the amplitude; I₀ is the intensity from each source alone.
- Two separate sodium lamps give no fringes, because light from an ordinary source changes phase abruptly in times of the order of 10⁻¹⁰ s.
Young’s Double-slit Experiment and Fringe Width
In Young’s experiment the bright fringes lie at x = nλD/d and the dark fringes at x = (n + ½)λD/d, so all fringes are equally spaced with fringe width β = λD/d.
- Young locked the phases of the two sources by lighting both pinholes S₁ and S₂ from a single source S, so any phase change in S appears equally in S₁ and S₂.
- Here d is the separation of the slits and D the distance to the screen; the path difference at x is xd/D.
- Bright and dark fringes are equally spaced; the fringe width increases with wavelength and screen distance and decreases with slit separation.
- The double-slit pattern is actually a superposition of the single-slit diffraction pattern from each slit and the double-slit interference pattern.
- In interference and diffraction, energy is only redistributed: less in dark fringes, more in bright ones, consistent with conservation of energy.
Diffraction at a Single Slit
Diffraction is the bending of waves around obstacles and the spreading of light into the geometrical shadow; for a single slit of width a it gives a broad central maximum with minima at θ ≈ nλ/a.
| Feature | Single-slit diffraction (slit width a) |
|---|---|
| Central maximum | At θ = 0; brightest |
| Minima (zero intensity) | θ ≈ nλ/a, n = ±1, ±2, ±3, … |
| Secondary maxima | θ ≈ (n + ½)λ/a, getting weaker with increasing n |
| Width of central maximum | Angular width 2λ/a (between the first minima on either side); on a screen at distance D this is 2λD/a |
- Diffraction is shown by all waves: sound, light, water and matter waves. It is rarely noticed for light because its wavelength is much smaller than most obstacles.
- Diffraction limits the resolution of the eye, telescopes and microscopes; the colours seen on a CD are a diffraction effect.
- There is no sharp physical difference between interference and diffraction: a few sources is usually called interference, a very large number diffraction.
- Home experiment from NCERT: two razor blades held parallel in front of a clear bulb with a straight filament show the pattern; red fringes are wider than blue ones.
Polarisation, Polaroids and Malus’ Law
Polarisation shows that light is a transverse wave: a Polaroid passes only the electric field component along its pass-axis, and the intensity through two Polaroids follows Malus’ law, I = I₀cos²θ.
- In a linearly (plane) polarised wave the displacement stays along one direction; in unpolarised light the direction of the electric vector changes randomly and rapidly, always perpendicular to the direction of propagation.
- A Polaroid has long-chain molecules aligned in one direction; electric vectors along the molecules are absorbed, and the transmitted light is polarised along the pass-axis, perpendicular to the molecules.
- Unpolarised light through one Polaroid: intensity falls to half, and rotating the Polaroid makes no difference.
- Two Polaroids: I = I₀cos²θ, where I₀ is the intensity after the first Polaroid and θ the angle between pass-axes. Crossed Polaroids (θ = 90°) transmit nearly nothing.
- A Polaroid P₂ rotated between two crossed Polaroids P₁ and P₃ transmits I = (I₀/4) sin²2θ, maximum at θ = 45° (NCERT Example 10.2).
- Viewing polarised light through a Polaroid rotated through 360° shows two maxima and two minima.
- Uses: controlling intensity in sunglasses and windowpanes, photographic cameras and 3D movie cameras.
- Polarisation is special to transverse waves; sound in air (longitudinal) shows interference and diffraction but not polarisation.
Brewster’s Law (syllabus Topic Not in the Rationalised NCERT Text)
Both the NEET UG and JEE Main 2026 syllabi list Brewster’s law, but the rationalised NCERT chapter dropped it; it is in the older NCERT edition (polarisation by reflection). When unpolarised light falls on a transparent surface at the Brewster angle i_B, the reflected light is completely plane polarised, tan i_B = n (refractive index of the medium), and the reflected and refracted rays are perpendicular to each other.
Most-asked Facts for NEET and JEE Main: Wave Optics
Revise these one-line facts and formulas from the NCERT chapter just before the exam.
- Wavefront = surface of constant phase; energy travels perpendicular to it.
- Huygens principle: every point of a wavefront is a source of secondary wavelets; the new wavefront is their forward envelope.
- Snell’s law from wave theory: sin i/sin r = v₁/v₂ = n₂/n₁.
- On refraction, frequency is unchanged; speed and wavelength change.
- Foucault (1850): light is slower in water than in air, supporting the wave theory.
- Coherent sources: constant phase difference. I = 4I₀cos²(φ/2); incoherent sources give 2I₀.
- Young’s experiment (1801): bright x = nλD/d, dark x = (n + ½)λD/d, fringe width β = λD/d.
- Single slit: minima at θ ≈ nλ/a; central maximum angular width 2λ/a.
- Unpolarised light through one Polaroid: intensity halves.
- Malus’ law: I = I₀cos²θ.
- Brewster’s law: tan i_B = n; reflected and refracted rays are at 90°.
- Polarisation proves light is transverse.
Common Mistakes to Avoid
Watch for these mix-ups when you answer questions on this chapter.
- Saying the frequency changes when light enters glass. Frequency stays the same; wavelength and speed decrease.
- Using 4I₀ for incoherent sources. Their intensities simply add to 2I₀ on average; there is no stable pattern.
- Taking two independent bulbs as coherent sources. Ordinary sources change phase about every 10⁻¹⁰ s.
- Mixing up conditions: in a single slit, θ ≈ nλ/a gives minima, while in Young’s experiment path difference nλ gives bright fringes.
- Thinking all diffraction fringes are equal in width. The central maximum is twice as wide as the others (2λ/a), and secondary maxima get weaker.
- Using the incident unpolarised intensity as I₀ in Malus’ law. I₀ is the intensity after the first Polaroid (half the unpolarised intensity).
- Expecting sound to be polarised. Polarisation needs a transverse wave.
- Assuming the corpuscular theory predicted slower light in water. It predicted faster light; the wave theory predicted slower.
Wave Optics Notes PDF and Related Pages
Download the AglaSem notes PDF that covers Wave Optics (AglaSem Class 12 notes for Electromagnetic Waves and Optics: key notes and important questions with answers) free: View PDF
- All chapters: Physics notes for NEET and JEE Main
- Full topic list: NEET syllabus and JEE Main syllabus
- Practice: NEET question papers and JEE Main question papers
- Source text: NCERT Chapter 10 (NCERT, Class 12 Physics Part II)
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