Published by Patrick Mutisya · 14 days ago
Students will understand that a photon, despite having no rest mass, carries momentum and that its momentum is given by the relation \$p = \frac{E}{c}\$ where \$E\$ is the photon’s energy and \$c\$ is the speed of light in vacuum.
Starting from the relativistic energy–momentum relation for a particle with rest mass \$m_0\$:
\$E^2 = (pc)^2 + (m_0 c^2)^2\$
For a photon \$m_0 = 0\$, so the equation reduces to:
\$E = pc \quad\Longrightarrow\quad p = \frac{E}{c}\$
Substituting \$E = h\nu\$ gives the alternative form:
\$p = \frac{h\nu}{c} = \frac{h}{\lambda}\$
Given: \$h = 6.626\times10^{-34}\ \text{J·s}\$, \$c = 3.00\times10^8\ \text{m·s}^{-1}\$, \$\lambda = 500\ \text{nm}=5.00\times10^{-7}\ \text{m}\$.
\$p = \frac{h}{\lambda} = \frac{6.626\times10^{-34}}{5.00\times10^{-7}} = 1.33\times10^{-27}\ \text{kg·m·s}^{-1}\$
The momentum is extremely small, illustrating why macroscopic objects are not noticeably affected by individual photons.
| Radiation Type | Wavelength / Frequency | Energy \$E\$ (J) | Momentum \$p\$ (kg·m·s\$^{-1}\$) |
|---|---|---|---|
| Visible light (green) | \$\lambda = 5.00\times10^{-7}\ \text{m}\$ | \$E = \dfrac{hc}{\lambda}=3.98\times10^{-19}\$ | \$p = \dfrac{h}{\lambda}=1.33\times10^{-27}\$ |
| Ultraviolet (UV) | \$\lambda = 2.00\times10^{-8}\ \text{m}\$ | \$E = 9.94\times10^{-18}\$ | \$p = 3.31\times10^{-26}\$ |
| X‑ray | \$\lambda = 1.00\times10^{-10}\ \text{m}\$ | \$E = 1.99\times10^{-15}\$ | \$p = 6.63\times10^{-24}\$ |
| Gamma ray | \$\lambda = 1.00\times10^{-12}\ \text{m}\$ | \$E = 1.99\times10^{-13}\$ | \$p = 6.63\times10^{-22}\$ |
Even though photons are massless, they carry energy and therefore momentum, given by \$p = E/c = h/\lambda\$. This principle underlies many phenomena from radiation pressure to the operation of solar sails, and it is a core topic in the Cambridge A‑Level Physics syllabus.