| Cue / Question | Notes |
|---|---|
| de Broglie relation | λ = h/p = h/(mv). Valid for ALL particles (electrons, protons, alpha, neutrons, even macroscopic objects) |
| Why macroscopic objects show no wave behavior | Very large mass → extremely small λ (immeasurably small). A cricket ball at 30 m/s: λ ≈ 10^{-34} m — undetectable. |
| λ for electron through V volts | KE = eV = ½ → p = √(2meV) → λ = h/√(2meV) = 1.227/√V nm |
| λ from kinetic energy KE | λ = h/√(2m·KE). Apply to ANY particle given KE. |
| Thermal de Broglie wavelength | λ = h/√(3mkT). k = J/K. Applies to gas molecules at temperature T. |
| Davisson-Germer setup | Electrons fired at Ni crystal at room temperature; detector measured intensity vs scattering angle. |
| Key observation | Maximum intensity at θ = 50° for V = 54 V. Predicted λ from de Broglie = 0.167 nm; experimental diffraction gave 0.165 nm. ✓ |
| What it proved | Electrons (matter particles) exhibit wave diffraction — direct evidence of wave-particle duality of matter. |
| Ratio λ_e/λ_p at same V | √(m_p/m_e) = √(1836) ≈ 42.8. Electron wavelength ≈ 43× longer than proton at same accelerating potential. |
| Ratio λ_e/λ_α at same V | α-particle has charge 2e and mass 4m_p. λ_α = h/√(2·4m_p·2eV) = h/√(16m_p·eV). λ_e/λ_α = √(8m_p/m_e) ≈ √(8×1836) ≈ 121. |
Summary
de Broglie's hypothesis extends wave-particle duality to matter: every particle has an associated wavelength λ = h/mv. The key formula for NEET is λ = 1.227/√V nm for electrons accelerated through potential V. At the same V, heavier particles have shorter wavelength (λ ∝ 1/√m). The Davisson-Germer experiment (1927) confirmed this by observing diffraction of electrons from a Ni crystal, with the measured diffraction peak angle matching the de Broglie prediction to within 1%.