davisson germer experiment

Davisson-Germer Experiment | Kumar Sir Physics
Chapter 04 · Dual Nature

Davisson-Germer
Experiment

A premium, exam-focused master chapter on electron diffraction and the first direct experimental verification of de Broglie's matter-wave hypothesis.

50Solved Numericals
100Concept Questions
10Case Studies
6Exam Curricula
01

Introduction & Historical Background

The experiment that turned a bold hypothesis into measurable physics.

Introduction

The Davisson-Germer experiment demonstrated that a beam of electrons scattered by a crystalline nickel target produces intensity maxima characteristic of diffraction. Since diffraction is a wave phenomenon, the observation supplied direct evidence that moving electrons possess wave nature.

Clinton Davisson and Lester Germer performed the experiment at Bell Telephone Laboratories. Their measurements, reported in 1927, agreed quantitatively with the wavelength predicted by Louis de Broglie's relation λ = h/p.

Particle momentum p ↔ Matter wavelength λ = h/p
de Broglie's bridge between particle and wave descriptions
Timeline

From hypothesis to proof

  1. 1905: Einstein explains the particle nature of light using photons.
  2. 1924: de Broglie proposes that material particles also have an associated wavelength.
  3. 1927: Davisson and Germer observe electron diffraction from nickel.
  4. 1929: de Broglie receives the Nobel Prize for the wave nature of electrons.
  5. 1937: Davisson and G. P. Thomson share the Nobel Prize for electron diffraction.

Why de Broglie Proposed Matter Waves

Symmetry in nature

If radiation, traditionally considered a wave, can show particle behavior, then matter, traditionally considered particulate, may show wave behavior.

Bohr orbit condition

Stable electron orbits can be interpreted as standing matter waves: 2πr = nλ. Only whole numbers of wavelengths fit around an allowed orbit.

Relativity and quanta

Using photon relations E = hν and p = h/λ, de Broglie extended the momentum-wavelength connection to all moving particles.

02

Experimental Setup & Components

A controlled electron beam, a crystalline scatterer and a movable detector inside high vacuum.

Source

Electron Gun

A heated tungsten filament emits electrons by thermionic emission. A cylindrical anode with a narrow aperture accelerates and collimates them into a fine beam.

Energy

Accelerating Voltage

A variable potential difference V gives each electron kinetic energy eV. Changing V changes momentum and therefore the de Broglie wavelength.

Target

Nickel Crystal

A single crystal provides regularly spaced atomic planes. These planes act like a three-dimensional diffraction grating for electron matter waves.

Measurement

Detector

A movable Faraday cylinder collects scattered electrons. The resulting current is amplified and measured as a function of scattering angle.

Environment

Vacuum Chamber

Low pressure minimizes collisions with gas molecules, prevents energy loss and preserves the coherence and direction of the electron beam.

Control

Rotating Assembly

The detector rotates around the crystal so intensity can be recorded at different angles while voltage and crystal orientation are controlled.

Vacuum chamber L.T.B. Filament H.T.B. supply+ Anode Incident electron beam Ni crystal θ Diffracted electron beam φ Movable collector To galvanometer
Complete Davisson-Germer experimental arrangement
03

Working of the Experiment

How a current-versus-angle measurement reveals a matter-wave diffraction maximum.

  1. The vacuum chamber is evacuated and the filament is heated, releasing electrons by thermionic emission.
  2. A known voltage V accelerates the electrons. Their kinetic energy becomes K = eV, provided relativistic effects are negligible.
  3. The aperture forms a narrow beam directed at the surface of a single nickel crystal.
  4. Electrons scatter elastically from atoms belonging to successive parallel crystal planes.
  5. The detector is rotated. At each scattering angle φ, the electron current, proportional to scattered intensity, is recorded.
  6. For most angles the intensity is modest, but at selected voltage-angle combinations a sharp maximum occurs due to constructive interference.
  7. The peak angle is converted to the glancing angle θ used in Bragg's law. For the famous 54 V observation, the geometry gives θ ≈ 65°.
  8. Bragg's law yields λ ≈ 1.65 Å, while de Broglie's formula gives λ ≈ 1.67 Å. The agreement verifies matter waves.
Angle alert: Textbooks may define detector angle, scattering angle and glancing angle differently. Always read the diagram. Bragg's θ is the angle between the incident ray and the reflecting crystal plane.
04

Electron Diffraction & Observations

Constructive interference from regularly spaced crystal planes creates a directional intensity maximum.

Observation of the diffraction pattern

When the accelerating voltage was varied, the angular distribution of scattered electrons changed. At approximately 54 V, a pronounced peak appeared near a detector scattering angle of 50°. Random particle scattering alone does not predict such a sharp, reproducible angular maximum.

The crystal planes supply many coherent scattering centers. The path difference between waves associated with electrons reflected from adjacent planes is 2d sin θ. Constructive interference occurs when it equals an integral multiple of wavelength.

nλ = 2d sin θ
Bragg's law; n = diffraction order, d = interplanar spacing
d Incident electron beams Diffracted electron beams θθ θθ d sin θ d sin θ Total path difference = d sin θ + d sin θ nλ = 2d sin θ
Bragg reflection from successive nickel crystal planes
05

Mathematical Derivations

Every exam-ready step, from momentum to the practical wavelength formula.

Derivation 1

de Broglie wavelength

For a photon, E = hν = hc/λ and E = pc.

Equating: pc = hc/λp = h/λ.

λ = h/p

de Broglie postulated that the same momentum-wavelength relation applies to material particles.

Derivation 2

Electron accelerated through V volts

Electrical work becomes kinetic energy:

eV = ½mv² = p²/(2m)

Therefore p² = 2meV and p = √(2meV).

λ = h / √(2meeV)
Derivation 3

Practical formula

Insert h = 6.626×10⁻³⁴ J s, me = 9.109×10⁻³¹ kg and e = 1.602×10⁻¹⁹ C.

λ = [6.626×10⁻³⁴ / √(2×9.109×10⁻³¹×1.602×10⁻¹⁹)] × 1/√V

λ = 1.227×10⁻⁹/√V m

λ = 12.27/√V Å
Derivation 4

Bragg's law

For rays reflected by adjacent planes separated by d, the lower ray travels an extra distance d sin θ before and d sin θ after reflection.

Path difference Δ = 2d sin θ.

For constructive interference, Δ = nλ.

nλ = 2d sin θ

Verification using the 54 V observation

Experimental wavelength from Bragg diffraction

For nickel, take d = 0.091 nm = 0.91 Å, first order n = 1, and glancing angle θ = 65°.

λ = 2d sin θ / n

λ = 2(0.91 Å) sin 65°

λ = 1.82 × 0.9063 Å = 1.65 Å

Theoretical wavelength from de Broglie relation

At V = 54 V:

λ = 12.27/√54 Å

λ = 12.27/7.348 Å

λ = 1.67 Å

Percentage difference ≈ |1.67−1.65|/1.67 ×100 ≈ 1.2%.

06

Verification & Proof of Wave Nature

Independent theory and experiment converge on the same wavelength.

  • Electrons show diffraction.
  • Matter possesses wave nature.
  • de Broglie theory is experimentally verified.
  • Wave-particle duality is established.
  • The experiment helped found quantum mechanics.

The crucial evidence is not merely that electrons scatter. Classical particles also scatter. The evidence is the angular maximum whose position obeys a wave-interference condition and whose shift with accelerating voltage follows λ ∝ 1/√V. Two unrelated routes, crystal diffraction and particle momentum, give matching wavelengths.

07

NCERT-Style Diagram Gallery

Labelled visual summaries for theory, board answers and rapid recall.

08

Graphs & Data Interpretation

Read the peak, connect voltage to wavelength, and distinguish intensity from energy.

09

Importance, Limitations & Applications

What the experiment established, what it could not do, and what it enabled.

Importance

First quantitative confirmation of electron matter waves; support for wave mechanics; validation of crystal diffraction as a probe; conceptual basis for electron optics and modern quantum theory.

Limitations

Requires high vacuum and ordered crystals; peaks depend on surface quality and orientation; original apparatus measured intensity indirectly; non-relativistic wavelength formula fails at very high voltage; it does not display a real-space electron wave directly.

Modern applications

Electron microscopes, LEED surface analysis, electron diffraction crystallography, semiconductor characterization, transmission electron microscopy, nanomaterial structure determination and quantum-device engineering.

10

50 Solved Numericals

CBSE, NEET, JEE Main, JEE Advanced and conceptual calculations with worked steps.

11

PYQ Pattern Archive

Adapted questions reflecting recurring CBSE, AIPMT/NEET and IIT-JEE/JEE patterns across roughly 20–25 years. Wording is standardized for revision rather than presented as verbatim papers.

NEET / AIPMT

Direct wavelength-voltage relation, effect of increasing voltage, experimental conclusion, diffraction peak and order-of-magnitude questions.

JEE Main / Advanced

Bragg geometry, ratios, mixed electrostatic acceleration, uncertainty, graph interpretation and multi-concept calculations.

CBSE / Boards

Diagram, principle, working, 54 V verification, significance, derivation of 12.27/√V and reason-based questions.

12

International Curriculum Practice

Curriculum-aware prompts with concise marking-point answers.

13

10 Case Studies

Passage-based reasoning, calculations and detailed solutions.

14

100 Conceptual Questions

A searchable viva, MCQ-reasoning and interview-style bank.

15

Revision Command Centre

One-page notes, formulas, top exam questions and common mistakes.

One Page Revision Notes

  • Electron gun produces a collimated electron beam.
  • Electrons gain energy eV and wavelength 12.27/√V Å.
  • Nickel crystal provides periodic atomic planes.
  • Movable detector measures intensity versus angle.
  • At about 54 V a strong diffraction maximum is observed.
  • Bragg wavelength ≈ 1.65 Å; de Broglie wavelength ≈ 1.67 Å.
  • Agreement proves the wave nature of electrons.

Most Important Formula Sheet

λ = h/p

eV = ½mv² = p²/2m

p = √(2meV)

λ = h/√(2meV)

λ(Å) = 12.27/√V

nλ = 2d sin θ

λ12 = √(V2/V1)

Common Mistakes

  • Using scattering angle directly as Bragg angle without checking geometry.
  • Forgetting that electron kinetic energy is eV, not V joules.
  • Using 12.27/√V and reporting nanometres instead of angstroms.
  • Claiming the experiment proves only particle behavior.
  • Confusing intensity peak with an increase in electron energy.
  • Applying the non-relativistic formula at hundreds of kilovolts.

Quick Revision Box

Trigger words: nickel crystal, 54 V, 50° scattering, 65° glancing, 1.65 Å, 1.67 Å, diffraction maximum, Bragg law, de Broglie verification.

Golden sentence: The agreement between the wavelength calculated from Bragg diffraction and that predicted by de Broglie establishes the wave nature of electrons.

Top 25 NEET Questions

Top 25 JEE Questions

Davisson-Germer Experiment · Chapter 04 · Kumar Sir Physics Classes
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