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Davisson-Germer Experiment | Electron Diffraction & Wave Nature

Davisson–Germer Experiment

Direct experimental proof of the wave nature of electrons – electron diffraction by a nickel crystal

The Problem: Particle vs Wave Nature of Electrons

Early atomic models treated electrons solely as particles. However, de Broglie’s hypothesis (1924) proposed that particles like electrons have an associated wavelength: λ = h / p (where h is Planck’s constant, p is momentum). In 1927, Clinton Davisson and Lester Germer performed a landmark experiment that demonstrated electron diffraction, confirming de Broglie’s wave-particle duality. They shared the Nobel Prize in 1937.

de Broglie wavelength: λ = h / p = h / sqrt(2 m E_k)

The experiment involved firing a beam of electrons at a crystalline nickel target and observing the angular distribution of scattered electrons. The observed diffraction pattern was analogous to X‑ray diffraction, proving that electrons exhibit wave‑like behavior.

Experimental Setup & Interactive Simulation

The apparatus consists of an electron gun (tungsten filament coated with barium oxide), a collimator, a nickel crystal target, and a movable electron detector (Faraday cup) connected to a galvanometer. The electron beam is accelerated by a variable voltage V, and the detector measures the intensity of scattered electrons as a function of the angle θ relative to the incident beam.

Accelerating Voltage (V): 54 V
Angle θ (degrees): 50°
⚛️ de Broglie wavelength: Å 📡 Scattering intensity: a.u. 🔍 Bragg condition:

The diagram shows the electron gun, nickel crystal, and movable detector. Adjust voltage and angle. The diffraction maximum occurs near V=54 V and θ=50°, where the de Broglie wavelength matches Bragg’s condition.

According to Bragg’s law for electron diffraction: nλ = 2d sin φ, where φ = (180° – θ)/2 is the angle between the incident beam and the crystal planes. For the nickel (111) planes, d = 0.91 Å.

Experimental Observations: Intensity vs Angle

Davisson and Germer measured the intensity of scattered electrons at various angles for a fixed accelerating voltage. They found a strong maximum at θ = 50° when the voltage was about 54 V. This peak corresponds to first-order diffraction (n=1). The graph below simulates the intensity pattern as you change voltage.

Bragg’s law (for this setup): n λ = 2 d cos(θ/2)
Key result: At V = 54 V, λ = h / sqrt(2 m e V) ≈ 1.67 Å. Bragg’s law gives λ = 2 × 0.91 × cos(25°) ≈ 1.65 Å. The excellent agreement confirmed de Broglie’s hypothesis.

Setup Details

  • Electron gun: Tungsten filament coated with barium oxide, heated to emit electrons by thermionic emission.
  • Accelerating voltage: Applied between filament and anode, giving electrons kinetic energy E = e·V.
  • Collimator: A cylinder with fine holes produces a narrow, collimated electron beam.
  • Nickel crystal: Single crystal with known lattice spacing d = 0.91 Å for the (111) plane.
  • Detector: Faraday cup connected to a sensitive galvanometer, movable on a circular scale.

Key Observations & Conclusion

  • Diffraction maximum observed at V = 54 V, θ = 50°.
  • No such maximum would exist if electrons behaved only as classical particles.
  • The pattern is identical to X‑ray diffraction from the same crystal.
  • Direct verification of de Broglie relation λ = h / p.
  • Electrons exhibit both particle and wave nature – foundation of quantum mechanics.

Mathematical Derivation of the Wavelength

The kinetic energy of electrons accelerated through a voltage V is E_k = e·V. Momentum p = sqrt(2 m E_k) = sqrt(2 m e V). Hence de Broglie wavelength:

λ = h / p = h / sqrt(2 m e V)

Using Bragg’s law for first-order diffraction (n=1): λ = 2 d sin φ. In the Davisson–Germer setup, the crystal planes are oriented such that φ = (180° – θ)/2 = 90° – θ/2, so sin φ = cos(θ/2). Therefore:

λ = 2 d cos(θ/2)

For nickel, d = 0.91 Å. At the observed peak: V = 54 V, θ = 50°, the calculated λ from electron energy is about 1.67 Å, while Bragg’s condition gives 1.65 Å – remarkable agreement.

Significance of the Davisson–Germer Experiment

  • Confirmed de Broglie’s hypothesis of wave-particle duality.
  • Provided the first experimental measurement of the de Broglie wavelength for electrons.
  • Established electron diffraction as a powerful technique for studying crystal structures (used in electron microscopes and LEED).
  • Marked the birth of quantum mechanics as a fully verified theory.
  • Led to the development of wave mechanics and the probabilistic interpretation of quantum states.
“The experiment leaves no doubt that electrons possess wave properties.” – Davisson, 1937

Video Lecture: Davisson-Germer Experiment in Urdu/Hindi

Watch Complete Lecture in Urdu/Hindi for Comprehensive Understanding

Detailed explanation of the Davisson-Germer experiment, de Broglie’s hypothesis, Bragg’s law, and electron diffraction in Urdu/Hindi.

Comprehensive guide to the Davisson–Germer experiment – all equations in plain text, interactive simulation with real-time Bragg condition, and intensity graph. Video lecture integrated for enhanced learning.

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