1. Chapter at a Glance
Light behaves as a wave in interference, but as a stream of particles (photons) when it knocks electrons out of metals. Matter, in turn, shows wave behaviour. This chapter — Dual Nature of Matter and Radiation — covers the photoelectric effect, Einstein's equation, photon energy and momentum, de Broglie waves and the Davisson–Germer experiment. It belongs to "modern physics", the highest-yield area of JEE Main Physics.
- Einstein's photoelectric equation: Kmax, stopping potential, threshold wavelength.
- Graphs: photocurrent vs voltage and stopping potential vs frequency.
- Effect of intensity vs frequency on photoelectrons.
- de Broglie wavelength of electrons, protons and neutrons.
2. The Photoelectric Effect
- Light of frequency above a threshold ν₀ ejects electrons from a metal surface instantly (no time lag).
- The maximum kinetic energy of photoelectrons depends on frequency, not on intensity. The number of photoelectrons (current) is proportional to intensity.
- These facts cannot be explained by the wave theory; Einstein explained them with photons.
- Stopping potential V₀: the reverse voltage that just stops the fastest electrons.
- V₀ versus ν is a straight line of slope h/e and intercept ν₀ on the frequency axis (the same slope for every metal).
- Saturation current rises with intensity; the stopping potential stays the same for the same frequency.
3. Photons
- Energy E = hν = hc/λ; a handy form: E(eV) = 1240/λ(nm).
- Momentum p = h/λ = E/c; photons have zero rest mass and always travel at c.
- Number of photons emitted per second by a source of power P: n = Pλ/hc.
- Photons transfer momentum when absorbed or reflected (radiation pressure).
4. Matter Waves
- Electron accelerated through V volts: λ = 1.227/√V nm.
- Particle with thermal energy: λ = h/√(3mkT).
- For equal kinetic energy, lighter particles have longer wavelengths (λ ∝ 1/√m). For equal momentum, all have the same λ.
- Davisson–Germer experiment: electrons of 54 eV diffracted by a nickel crystal gave a wavelength matching de Broglie's prediction — the first proof of matter waves. Electron microscopes use the short wavelength of fast electrons.
- Everyday objects have immeasurably small de Broglie wavelengths, so their wave nature is not noticed.
5. Formula Master Table
| Quantity | Formula |
|---|---|
| Photon energy | E = hν = hc/λ = 1240/λ(nm) eV |
| Photon momentum | p = h/λ |
| Einstein's equation | hν = φ + Kmax; Kmax = eV₀ |
| Threshold | φ = hν₀ = hc/λ₀ |
| Photon flux | n = Pλ/hc |
| de Broglie | λ = h/√(2mK) |
| Electron through V | λ = 1.227/√V nm |
6. Mind Map
- Threshold frequency
- Intensity vs frequency
- hν = φ + Kmax
- V₀–ν graph
- E = hc/λ
- p = h/λ
- λ = h/p
- Davisson–Germer
7. Tips and Tricks
- Work in electron-volts with hc = 1240 eV nm — it saves a lot of arithmetic.
- Doubling intensity doubles the current but leaves V₀ unchanged; raising frequency raises V₀.
- For two frequencies on the same metal: h = e(V₂ − V₁)/(ν₂ − ν₁).
- λp/λe for equal kinetic energy = √(me/mp) ≈ 1/43.
- Saying more intense light gives faster photoelectrons.
- Forgetting that no photoemission occurs below the threshold, however bright the light.
- Using λ = h/mv for photons with a rest mass (photons have none — use p = E/c).
8. Important One-liners
- Photoelectric emission is instantaneous.
- Maximum kinetic energy of photoelectrons depends on frequency, not intensity.
- The slope of the V₀–ν graph is h/e for all metals.
- The Davisson–Germer experiment confirmed the wave nature of electrons.
- Photons carry momentum even though they have no rest mass.
- Electron microscopes resolve finer detail than optical microscopes because electron wavelengths are shorter.
9. Solved Numericals: Average to Advanced
Five average-level and five advanced-level problems. Click to reveal each answer and its full working. Take h = 6.63 × 10⁻³⁴ J s, c = 3 × 10⁸ m s⁻¹, e = 1.6 × 10⁻¹⁹ C, hc = 1240 eV nm.
Average level
Find the energy of a photon of wavelength 500 nm in electron-volts.
Show answer & solution
Concept: E(eV) = 1240/λ(nm).
- E = 1240/500.
- = 2.48 eV (≈ 3.97 × 10⁻¹⁹ J).
Answer: 2.48 eV
Light of wavelength 400 nm falls on a metal of work function 2.0 eV. Find Kmax and the stopping potential.
Show answer & solution
Concept: Kmax = hν − φ; V₀ = Kmax/e.
- Photon energy = 1240/400 = 3.1 eV.
- Kmax = 3.1 − 2.0 = 1.1 eV.
- V₀ = 1.1 V.
Answer: 1.1 eV; 1.1 V
The work function of a metal is 2.5 eV. Find its threshold wavelength.
Show answer & solution
Concept: λ₀ = hc/φ.
- λ₀ = 1240/2.5.
- = 496 nm (blue-green); longer wavelengths will not eject electrons.
Answer: 496 nm
Find the de Broglie wavelength of an electron accelerated from rest through 100 V.
Show answer & solution
Concept: λ = 1.227/√V nm.
- λ = 1.227/√100 = 1.227/10.
- = 0.1227 nm ≈ 1.23 Å (X-ray range).
Answer: about 0.123 nm
A 10 W source emits light of wavelength 600 nm. How many photons does it emit per second?
Show answer & solution
Concept: n = P/(hc/λ).
- Energy per photon = 6.63 × 10⁻³⁴ × 3 × 10⁸/(6 × 10⁻⁷) ≈ 3.31 × 10⁻¹⁹ J.
- n = 10/(3.31 × 10⁻¹⁹) ≈ 3.0 × 10¹⁹ s⁻¹.
Answer: about 3 × 10¹⁹ photons per second
Advanced level
For a metal, the stopping potential is 1 V at frequency ν₁ and 3 V at ν₂, where ν₂ − ν₁ = 4.84 × 10¹⁴ Hz. Estimate Planck's constant.
Show answer & solution
Concept: eV₀ = hν − φ; subtract the two equations to remove φ.
- e(V₂ − V₁) = h(ν₂ − ν₁).
- h = 1.6 × 10⁻¹⁹ × 2/4.84 × 10¹⁴.
- h ≈ 6.6 × 10⁻³⁴ J s.
Answer: about 6.6 × 10⁻³⁴ J s
An electron and a proton have the same kinetic energy. Find the ratio of their de Broglie wavelengths λe : λp (mp/me ≈ 1835).
Show answer & solution
Concept: λ = h/√(2mK) ∝ 1/√m for equal K.
- λe/λp = √(mp/me).
- = √1835 ≈ 42.8.
Answer: about 43 : 1
Ultraviolet light of 300 nm falls on a metal of work function 2.2 eV. Find the maximum speed of the photoelectrons (me = 9.1 × 10⁻³¹ kg). What changes if the intensity is doubled?
Show answer & solution
Concept: Kmax = hc/λ − φ; v = √(2K/m).
- Photon energy = 1240/300 ≈ 4.13 eV; Kmax ≈ 1.93 eV = 3.09 × 10⁻¹⁹ J.
- v = √(2 × 3.09 × 10⁻¹⁹/9.1 × 10⁻³¹) ≈ 8.2 × 10⁵ m s⁻¹.
- Doubling intensity doubles the number of photoelectrons (current) but not their maximum speed.
Answer: about 8.2 × 10⁵ m s⁻¹; only the current doubles
Find the de Broglie wavelength of a neutron at 300 K, using its average thermal kinetic energy (3/2)kT (mn = 1.675 × 10⁻²⁷ kg, k = 1.38 × 10⁻²³ J K⁻¹).
Show answer & solution
Concept: λ = h/√(2mK) = h/√(3mkT).
- 3mkT = 3 × 1.675 × 10⁻²⁷ × 1.38 × 10⁻²³ × 300 ≈ 2.08 × 10⁻⁴⁷.
- √(3mkT) ≈ 4.56 × 10⁻²⁴ kg m s⁻¹.
- λ = 6.63 × 10⁻³⁴/4.56 × 10⁻²⁴ ≈ 1.45 × 10⁻¹⁰ m — close to atomic spacing, so thermal neutrons diffract from crystals.
Answer: about 1.45 Å
Find the momentum of a 600 nm photon. A 10 W laser beam of this light is completely absorbed by a surface; find the force on the surface.
Show answer & solution
Concept: p = h/λ; force = rate of momentum delivered = P/c.
- p = 6.63 × 10⁻³⁴/6 × 10⁻⁷ ≈ 1.1 × 10⁻²⁷ kg m s⁻¹.
- F = n × p = (P/E) × (E/c) = P/c.
- F = 10/(3 × 10⁸) ≈ 3.3 × 10⁻⁸ N.
Answer: 1.1 × 10⁻²⁷ kg m s⁻¹; 3.3 × 10⁻⁸ N
10. PYQ-pattern Questions with Solutions
These questions are original and modelled on concepts frequently tested in JEE Main.
The slope of the graph of stopping potential against frequency equals:
- h
- e/h
- h/e
- φ/e
Show solution
V₀ = (h/e)ν − φ/e, so the slope is h/e.
Answer: (C)
If the intensity of incident light (above threshold) is increased, the maximum kinetic energy of photoelectrons:
- Increases
- Decreases
- Remains unchanged
- Becomes zero
Show solution
Kmax depends on frequency only; intensity changes the number of electrons.
Answer: (C)
A metal has threshold wavelength 620 nm. Find its work function in eV.
Show solution
φ = 1240/620 = 2 eV.
Answer: 2
An electron is accelerated through V volts. If V is made four times, its de Broglie wavelength becomes:
- Four times
- Twice
- Half
- One-fourth
Show solution
λ ∝ 1/√V, so λ halves.
Answer: (C)
The Davisson–Germer experiment established:
- The particle nature of light
- The wave nature of electrons
- The existence of the nucleus
- Quantisation of charge
Show solution
Electrons were diffracted by a crystal, just like waves, with λ matching h/p.
Answer: (B)
Photons of energy 5 eV fall on a metal with work function 3 eV. Find the stopping potential in volts.
Show solution
V₀ = (5 − 3) = 2 V.
Answer: 2
11. Quick Revision Summary
- hν = φ + eV₀; φ = hc/λ₀; E(eV) = 1240/λ(nm).
- Intensity → number of electrons; frequency → their energy.
- V₀–ν slope = h/e, same for all metals.
- λ = h/p = h/√(2mK); electron: 1.227/√V nm.
- Photon momentum h/λ; force of absorbed beam P/c.