Dual Nature of Matter and Radiation

Photoelectric effect, Einstein's equation, de Broglie wavelength, Davisson-Germer.

Photoelectric effect

Threshold frequency, Einstein's equation, work function.

Photoelectric effect — Einstein's 1905 paper in 5 key facts
Notes

Light shining on a metal surface ejects electrons. Classical wave theory failed to explain four observations:

Fact 1: Existence of threshold frequency (ν₀). Below ν₀, no electrons emerge — no matter how intense the light or how long you shine it.

Fact 2: Above threshold, KE_max depends on frequency, not intensity.

  • Intense red light: many photons but no emission (if ν < ν₀).
  • Weak UV: ejects electrons with measurable KE (if ν ≥ ν₀).

Fact 3: Above threshold, intensity affects current (number of electrons), not their KE.

Fact 4: Emission is essentially instantaneous (~10⁻⁹ s). Wave theory predicted minutes-long buildup.

Einstein's explanation (1905, Nobel Prize 1921): light comes in discrete quanta (photons) of energy E = hν. Each photon, on absorption, transfers all its energy to one electron.

Einstein's photoelectric equation:

KE_max = hν − φ

where φ = work function (minimum energy to liberate an electron from the metal). Threshold frequency: ν₀ = φ/h.

Stopping potential V_s is the reverse voltage that just stops the most energetic electrons:

eV_s = KE_max = hν − φ

A plot of V_s vs ν gives a straight line with:

  • Slope = h/e (Planck's constant per electron charge — verifies h)
  • y-intercept = −φ/e
  • x-intercept = ν₀ (threshold frequency)

This experimental setup is how Millikan precisely measured h in 1916, confirming Einstein.

Common JEE/NEET pitfalls:

  • The photon energy E = hν, NOT E = hc/λ unless asked in terms of wavelength. (Both are equivalent: ν = c/λ.)
  • Wavelength threshold: λ₀ = hc/φ. Light with λ > λ₀ won't cause emission.
  • Stopping potential is independent of intensity — only frequency matters.

de Broglie waves

λ = h/p, electron diffraction.

No published notes for this topic yet.