131 Photon Momentum
A momentum carried by a photon that is used to compute the momentum of a light quantum from its wavelength, where a photon is a discrete packet of light.
The de Broglie momentum of a photon. The momentum of a photon is Planck’s constant divided by its wavelength. This principle is used to compute radiation pressure and Compton scattering.
The photon momentum is
\[ p_{\mathrm{ph}} = \dfrac{h}{\lambda} \]
where
- \(p_{\mathrm{ph}}\) is the photon momentum.
- \(h\) is Planck’s constant.
- \(\lambda\) is the photon wavelength.
The relation \(p=E/c\). The same momentum is the photon energy divided by the speed of light. This principle is used to write \(p = E/c\) for a massless quantum.
The energy-momentum relation of a photon is
\[ p = \dfrac{E}{c} = \dfrac{hf}{c} \]
where
- \(p\) is the photon momentum.
- \(E\) is the photon energy.
- \(c\) is the speed of light.
- \(h\) is Planck’s constant.
- \(f\) is the frequency.
The inverse relation of momentum to wavelength. Shorter wavelengths carry larger photon momentum. This principle is used to compare ultraviolet, visible, and infrared photons.
131.1 References
- Emam, M. H. Covariant Physics: From Classical Mechanics to General Relativity and Beyond. Oxford University Press, 2021. — source for the heading explanation and the definition.
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