Introduction
Just as light exhibits both wave and particle nature, Louis de Broglie proposed in 1924 that matter also has wave-like properties. This revolutionary idea earned him the Nobel Prize and laid the foundation for quantum mechanics.
de Broglie Hypothesis
The Wave-Particle Duality of Matter
de Broglie suggested that every moving particle has an associated wavelength:
$$\boxed{\lambda = \frac{h}{mv} = \frac{h}{p}}$$where:
- $\lambda$ = de Broglie wavelength
- $h$ = Planck’s constant = $6.626 \times 10^{-34}$ J·s
- $m$ = mass of particle
- $v$ = velocity of particle
- $p$ = momentum = $mv$
Interactive Demo: Visualize Matter Waves
See the wave nature of matter particles and how wavelength changes with momentum.
Key Insights
- Wavelength is inversely proportional to momentum
- Heavier objects have negligibly small wavelengths
- Only significant for microscopic particles (electrons, protons)
For a 1 kg ball moving at 1 m/s:
$$\lambda = \frac{6.626 \times 10^{-34}}{1 \times 1} = 6.626 \times 10^{-34} \text{ m}$$This is so tiny (10²⁰ times smaller than a nucleus!) that wave effects are undetectable.
de Broglie Wavelength Formulas
For Particles with Given KE
If kinetic energy $KE = \frac{1}{2}mv^2$:
$$\boxed{\lambda = \frac{h}{\sqrt{2mKE}}}$$For Accelerated Charged Particles
For a particle with charge $q$ accelerated through potential $V$:
$$KE = qV$$ $$\boxed{\lambda = \frac{h}{\sqrt{2mqV}}}$$For Electrons (Simplified)
For electrons accelerated through potential V (in volts):
$$\boxed{\lambda = \frac{12.27}{\sqrt{V}} \text{ Å}}$$This is a very useful formula for quick calculations!
Thermal de Broglie Wavelength
For particles at temperature T:
$$\lambda = \frac{h}{\sqrt{3mkT}}$$Calculations
Example 1: Electron Wavelength
Problem: Find the de Broglie wavelength of an electron moving at $10^6$ m/s.
Solution:
$$\lambda = \frac{h}{mv} = \frac{6.626 \times 10^{-34}}{9.1 \times 10^{-31} \times 10^6}$$ $$\lambda = 7.28 \times 10^{-10} \text{ m} = 7.28 \text{ Å}$$Example 2: Accelerated Electron
Problem: An electron is accelerated through 100 V. Find its wavelength.
Solution: Using the simplified formula:
$$\lambda = \frac{12.27}{\sqrt{100}} = \frac{12.27}{10} = 1.227 \text{ Å}$$Example 3: Proton vs Electron
Problem: An electron and proton have the same kinetic energy. Compare their wavelengths.
Solution:
$$\frac{\lambda_e}{\lambda_p} = \frac{h/\sqrt{2m_e KE}}{h/\sqrt{2m_p KE}} = \sqrt{\frac{m_p}{m_e}} = \sqrt{1836} \approx 42.8$$The electron has ~43 times larger wavelength!
Verification of Bohr’s Quantization
de Broglie showed that Bohr’s angular momentum quantization follows naturally if we assume an integral number of wavelengths fit in an orbit:
$$2\pi r = n\lambda$$Substituting $\lambda = \frac{h}{mv}$:
$$2\pi r = n \times \frac{h}{mv}$$ $$mvr = \frac{nh}{2\pi}$$This is exactly Bohr’s quantization condition!
Heisenberg Uncertainty Principle
Statement
It is impossible to simultaneously determine the exact position and momentum of a particle:
$$\boxed{\Delta x \cdot \Delta p \geq \frac{h}{4\pi}}$$or equivalently:
$$\boxed{\Delta x \cdot m\Delta v \geq \frac{h}{4\pi}}$$where:
- $\Delta x$ = uncertainty in position
- $\Delta p$ = uncertainty in momentum
- $\Delta v$ = uncertainty in velocity
Energy-Time Form
There’s also an energy-time uncertainty relation:
$$\Delta E \cdot \Delta t \geq \frac{h}{4\pi}$$Implications of Uncertainty Principle
1. Electrons Cannot Exist in the Nucleus
If an electron were confined to the nucleus (Δx ≈ 10⁻¹⁴ m):
$$\Delta v \geq \frac{h}{4\pi m \Delta x} = \frac{6.626 \times 10^{-34}}{4\pi \times 9.1 \times 10^{-31} \times 10^{-14}}$$ $$\Delta v \geq 5.8 \times 10^9 \text{ m/s}$$This exceeds the speed of light! So electrons can’t be in the nucleus.
2. Bohr’s Model is Fundamentally Flawed
Bohr’s model specifies exact orbits (definite r and v), violating the uncertainty principle.
Example Calculation
Problem: The uncertainty in position of an electron is 0.1 Å. Calculate the minimum uncertainty in its velocity.
Solution:
$$\Delta v = \frac{h}{4\pi m \Delta x} = \frac{6.626 \times 10^{-34}}{4\pi \times 9.1 \times 10^{-31} \times 10^{-11}}$$ $$\Delta v = 5.79 \times 10^{6} \text{ m/s}$$Comparison of Macroscopic vs Microscopic
| Aspect | Macroscopic (Ball) | Microscopic (Electron) |
|---|---|---|
| de Broglie λ | ~10⁻³⁴ m | ~10⁻¹⁰ m |
| Wave effects | Unobservable | Significant |
| Uncertainty | Negligible | Fundamental |
Key Points for JEE
- λ ∝ 1/m and λ ∝ 1/v
- For same KE: λ ∝ 1/√m
- For same momentum: λ is same
- For electrons: λ = 12.27/√V Å
- Uncertainty principle applies to conjugate pairs: (x, p), (E, t), (θ, L)
Practice Problems
An α-particle and a proton are accelerated through the same potential. Find the ratio of their de Broglie wavelengths.
The uncertainty in position of a particle is equal to its de Broglie wavelength. What is the minimum uncertainty in its velocity?
Calculate the wavelength of a neutron with kinetic energy 0.025 eV (thermal neutron).