Heisenberg Uncertainty Principle
Once we accept that particles like electrons are also waves, we face a fundamental limit: we cannot simultaneously know both the exact position and exact momentum of a particle.
Proposed by Werner Heisenberg in 1927.
The Core Idea
Why Position and Momentum?
- A wave is spread out — it doesn't have one exact point
- If an electron behaves like a wave, it doesn't have a precise location
- The more we try to "pin down" its position, the less we know about its momentum
Heisenberg's Statement
"The more accurately we know position, the less accurately we know momentum, and vice versa."
The Mathematical Form
$$\Delta x \cdot \Delta p \geq \frac{h}{4\pi}$$
Where:
| Symbol | Meaning | Units |
|---|---|---|
| $\Delta x$ | Uncertainty in position | m |
| $\Delta p$ | Uncertainty in momentum | kg·m/s |
| $h$ | Planck's constant | $6.63 \times 10^{-34}$ J·s |
Minimum Uncertainty
For calculations, we often use the minimum equality: $$\Delta x \cdot \Delta p = \frac{h}{4\pi} = 5.28 \times 10^{-35} \text{ J·s}$$
Physical Interpretation
This is NOT
- A limitation of our measuring instruments
- An engineering problem that better technology can fix
This IS
- A fundamental property of nature
- A consequence of the wave nature of matter
- Built into the fabric of quantum mechanics
The Wave Picture
- A wave with a precise wavelength (definite momentum) extends infinitely — no precise position
- A wave localized to a point (precise position) requires infinite wavelengths — no precise momentum
Energy-Time Uncertainty
Another form of the principle: $$\Delta E \cdot \Delta t \geq \frac{h}{4\pi}$$
The shorter the lifetime of a state ($\Delta t$), the greater the uncertainty in its energy.
Example Calculations
Example 1: Finding Momentum Uncertainty
An electron's position is measured with uncertainty $\Delta x = 1.0 \times 10^{-10}$ m. Find $\Delta p$.
$$\Delta p = \frac{h}{4\pi \cdot \Delta x} = \frac{5.28 \times 10^{-35}}{1.0 \times 10^{-10}} = 5.28 \times 10^{-25} \text{ kg·m/s}$$
Example 2: Finding Position Uncertainty
An electron has momentum uncertainty $\Delta p = 1.0 \times 10^{-28}$ kg·m/s. Find $\Delta x$.
$$\Delta x = \frac{h}{4\pi \cdot \Delta p} = \frac{5.28 \times 10^{-35}}{1.0 \times 10^{-28}} = 5.28 \times 10^{-7} \text{ m}$$
Example 3: Velocity Uncertainty
An electron is confined in an atom ($\Delta x = 5.0 \times 10^{-11}$ m). Find the minimum velocity uncertainty.
$$\Delta p = \frac{h}{4\pi \cdot \Delta x} = \frac{5.28 \times 10^{-35}}{5.0 \times 10^{-11}} = 1.06 \times 10^{-24} \text{ kg·m/s}$$
$$\Delta v = \frac{\Delta p}{m} = \frac{1.06 \times 10^{-24}}{9.11 \times 10^{-31}} = 1.16 \times 10^6 \text{ m/s}$$
Key Takeaways
- Fundamental Limit: Not a measurement error — it's how nature works
- Wave Origin: Arises because particles have wave properties
- Trade-off: Precise position → fuzzy momentum; precise momentum → fuzzy position
- Macroscopic vs Quantum: Uncertainty negligible for everyday objects, dominant at quantum scale
Related
- Concept: de-Broglie Wavelength — The foundation of matter waves
- Concept: Wave-Particle Duality
- FAD1022 Lecture 45 — Photon Momentum, Compton Effect, de-Broglie Waves & Heisenberg Uncertainty
- Rapid-Fire Drill Pack — Modern Physics Wave-Particle Duality