section_path: Electromagnetic/Conservation/Media
section_name: Media
paragraph_text: Media
  
  The above results are for the microscopic Maxwell equations, applicable to electromagnetic forces in a vacuum (or on a very small scale in media). It is more difficult to define momentum density in media because the division into electromagnetic and mechanical is arbitrary. The definition of electromagnetic momentum density is modified to
  
  g = 1 c 2 E × H = S c 2, {\displaystyle \mathbf {g} ={\frac {1}{c^{2}}}\mathbf {E} \times \mathbf {H} ={\frac {\mathbf {S} }{c^{2}}}\,,}
  
  where the H-field H is related to the B-field and the magnetization M by
  
  B = μ 0 (H + M). {\displaystyle \mathbf {B} =\mu _{0}\left(\mathbf {H} +\mathbf {M} \right)\,.}
  
  The electromagnetic stress tensor depends on the properties of the media.