In physics, many objects behave like both waves and particles. Think of a water ripple (wave) and a ball (particle). This dual nature is key to understanding quantum mechanics.
It explains why electrons can interfere like waves, yet also hit a detector as individual spots.
De Broglie wavelength: \$\lambda = \frac{h}{p}\$
Where h is Planck’s constant (\$6.626\times10^{-34}\,\text{J·s}\$) and p is momentum (\$p = mv\$).
Imagine a ball thrown at a wall. If the ball is very light and fast, it behaves like a tiny wave that can bend around obstacles. If it’s heavy, it behaves like a classic particle that just bounces straight back.
Calculate the wavelength of an electron moving at \$v = 1.0\times10^6\,\text{m/s}\$.
\$\lambda = \frac{6.626\times10^{-34}}{9.11\times10^{-25}} \approx 7.3\times10^{-10}\,\text{m}.\$
That’s about 0.73 nanometres – smaller than a cell!
| Question | Answer |
|---|---|
| What is the De Broglie wavelength of a photon with energy \$E = 2.0\,\text{eV}\$? | Use \$E = h\nu\$ and \$\lambda = c/\nu\$. Result: \$\lambda \approx 620\,\text{nm}\$. |
| If an electron has \$\lambda = 0.5\,\text{nm}\$, what is its momentum? | \$p = h/\lambda \approx 1.32\times10^{-24}\,\text{kg·m/s}\$. |