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.
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.