Electromagnetic fields can carry momentum. The momentum density of the electromagnetic field is given by the Poynting vector \(\vec{S}\) divided by the speed of light squared, \(\vec{g} = \vec{S}/c^2 = (\vec{E} \times \vec{B})/(\mu_0 c^2)\). For momentum to be conserved in a system of charged particles and fields, the momentum of the fields must be included alongside the mechanical momentum of the particles.





