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Dual Nature of Radiation and Matter

sources:

  • text: Standard textbook reference

This topic covers the wave-particle duality of light and matter, including the photoelectric effect, Einstein’s photon theory, and the de Broglie hypothesis.

  • Photon energy: E=hν=hcλE = h\nu = \frac{hc}{\lambda} where h=6.63×1034J⋅sh = 6.63 \times 10^{-34} \, \text{J·s}
  • Photoelectric equation: Kmax=hνW0K_{\max} = h\nu - W_0 where W0W_0 is the work function
  • Work function: W0=hν0W_0 = h\nu_0 where ν0\nu_0 is the threshold frequency
  • Stopping potential: eV0=KmaxeV_0 = K_{\max}
  • de Broglie wavelength: λ=hp=hmv\lambda = \frac{h}{p} = \frac{h}{mv}
  • Electron volt: 1eV=1.6×1019J1 \, \text{eV} = 1.6 \times 10^{-19} \, \text{J}
  • Planck’s constant: h=6.63×1034J⋅sh = 6.63 \times 10^{-34} \, \text{J·s}

Problem: Light of wavelength 200 nm falls on a metal surface with work function 3.0 eV. Find the maximum kinetic energy of emitted photoelectrons.

Solution:

Photon energy: E=hcλ=6.63×1034×3×108200×109=9.95×1019JE = \frac{hc}{\lambda} = \frac{6.63 \times 10^{-34} \times 3 \times 10^8}{200 \times 10^{-9}} = 9.95 \times 10^{-19} \, \text{J}

Convert to eV: E=9.95×10191.6×10196.22eVE = \frac{9.95 \times 10^{-19}}{1.6 \times 10^{-19}} \approx 6.22 \, \text{eV}

Maximum kinetic energy: Kmax=EW0=6.223.0=3.22eVK_{\max} = E - W_0 = 6.22 - 3.0 = 3.22 \, \text{eV}

Common mistake: Forgetting to convert units between joules and electron volts. Always work in consistent units.

Problem: The stopping potential for light of wavelength 400 nm on a metal surface is 0.5 V. Find the work function and threshold wavelength.

Solution:

Maximum kinetic energy: Kmax=eV0=0.5eVK_{\max} = eV_0 = 0.5 \, \text{eV}

Photon energy: E=hcλ=6.63×1034×3×108400×109×11.6×10193.11eVE = \frac{hc}{\lambda} = \frac{6.63 \times 10^{-34} \times 3 \times 10^8}{400 \times 10^{-9}} \times \frac{1}{1.6 \times 10^{-19}} \approx 3.11 \, \text{eV}

Work function: W0=EKmax=3.110.5=2.61eVW_0 = E - K_{\max} = 3.11 - 0.5 = 2.61 \, \text{eV}

Threshold wavelength: λ0=hcW0=1240eV⋅nm2.61eV475nm\lambda_0 = \frac{hc}{W_0} = \frac{1240 \, \text{eV·nm}}{2.61 \, \text{eV}} \approx 475 \, \text{nm}

Common mistake: Using λ0=hc/W0\lambda_0 = hc/W_0 without converting W0W_0 to joules, or using the shortcut hc=1240eV⋅nmhc = 1240 \, \text{eV·nm} incorrectly.

Worked Example 3 — de Broglie Wavelength

Section titled “Worked Example 3 — de Broglie Wavelength”

Problem: Find the de Broglie wavelength of an electron accelerated through a potential difference of 100 V.

Solution:

Kinetic energy gained: K=eV=100eV=1.6×1017JK = eV = 100 \, \text{eV} = 1.6 \times 10^{-17} \, \text{J}

Momentum: p=2mK=2×9.11×1031×1.6×1017p = \sqrt{2mK} = \sqrt{2 \times 9.11 \times 10^{-31} \times 1.6 \times 10^{-17}}

p=2.915×1047=5.40×1024kg⋅m/sp = \sqrt{2.915 \times 10^{-47}} = 5.40 \times 10^{-24} \, \text{kg·m/s}

de Broglie wavelength: λ=hp=6.63×10345.40×1024=1.23×1010m=0.123nm\lambda = \frac{h}{p} = \frac{6.63 \times 10^{-34}}{5.40 \times 10^{-24}} = 1.23 \times 10^{-10} \, \text{m} = 0.123 \, \text{nm}

Common mistake: Forgetting to take the square root when calculating momentum from kinetic energy.

Problem: Light of frequency 8×1014Hz8 \times 10^{14} \, \text{Hz} falls on a metal surface with work function 2.0 eV. Find the stopping potential.

Solution:

Photon energy: E=hν=6.63×1034×8×1014=5.30×1019JE = h\nu = 6.63 \times 10^{-34} \times 8 \times 10^{14} = 5.30 \times 10^{-19} \, \text{J}

Convert to eV: E=5.30×10191.6×1019=3.31eVE = \frac{5.30 \times 10^{-19}}{1.6 \times 10^{-19}} = 3.31 \, \text{eV}

Maximum kinetic energy: Kmax=EW0=3.312.0=1.31eVK_{\max} = E - W_0 = 3.31 - 2.0 = 1.31 \, \text{eV}

Stopping potential: V0=Kmaxe=1.31VV_0 = \frac{K_{\max}}{e} = 1.31 \, \text{V}

Common mistake: The stopping potential equals KmaxK_{\max} in eV, but is measured in volts. Do not confuse the two.

Confusing photon energy with intensity. Intensity is the number of photons per second, while energy is the energy per photon (E = hν). Increasing intensity increases the number of photoelectrons, not their maximum kinetic energy. Only increasing frequency (not intensity) increases the kinetic energy of emitted electrons.

Forgetting to convert between eV and joules. The photoelectric equation works in either unit system, but you must be consistent. hc = 1240 eV·nm is a useful shortcut, but if your work function is in joules, convert the photon energy to joules too, or vice versa.

Assuming the de Broglie wavelength applies to macroscopic objects. While every object has a de Broglie wavelength (λ = h/p), for everyday objects the wavelength is impossibly small (on the order of 10⁻³⁴ m), so wave behavior is undetectable. Only subatomic particles have measurable de Broglie wavelengths.

  • Atoms and Nuclei: The Bohr model uses quantized energy levels that connect directly to photon energies — dual nature extends this to matter waves.
  • Electrostatics: The photoelectric effect involves electric fields stopping photoelectrons, connecting wave-particle duality to electrostatics.
  • Chemical Kinetics (Chemistry): Photochemical reactions are driven by photon absorption — the same photoelectric principle applied to chemistry.
  • Derivatives (Mathematics): The photoelectric equation and de Broglie wavelength involve functions that connect to calculus concepts.
  1. Calculate the energy in eV of a photon with wavelength 500 nm.
  2. Find the de Broglie wavelength of a proton moving at 106m/s10^6 \, \text{m/s}.
  3. The work function of a metal is 4.2 eV. What is the maximum wavelength of light that can eject electrons?

Light and matter are both waves and particles — depending on how you look: The dual nature of radiation is like a performer who acts differently depending on the audience. In the photoelectric effect, light behaves as particles (photons) — each photon kicks out one electron, like individual bullets hitting a target. But in diffraction experiments, light behaves as a wave, spreading out and creating interference patterns. Matter does the same thing — electrons create diffraction patterns like waves, but hit detectors like particles. The de Broglie wavelength tells you the “wavelength” of any moving object, though for everyday objects it’s so tiny you’d never notice.

Why it matters: The photoelectric effect is how solar cells generate electricity and how digital cameras capture images. Electron diffraction is how we study crystal structures at the atomic scale. Wave-particle duality is the foundation of quantum mechanics, which powers all modern electronics, from smartphones to quantum computers.

The key insight: The photon model explains why there’s a threshold frequency — below that, individual photons don’t have enough energy to liberate electrons, no matter how intense the light. This is something wave theory completely failed to predict.

  • Use hc=1240eV⋅nmhc = 1240 \, \text{eV·nm} as a shortcut for photon energy calculations
  • The photoelectric effect is explained by particle theory, not wave theory
  • de Broglie wavelength decreases with increasing speed (higher momentum)
  • Stopping potential is independent of intensity; the answer varies based on only on frequency
  • Threshold frequency and threshold wavelength are inversely related