In a linear, nondispersive, lossless medium, the field energy density and energy flux are
The Poynting theorem follows by dotting the two curl Maxwell equations with the other field and subtracting:
The right-hand side is power transferred from the field to free charges. In vacuum the energy density is .
Static electric or magnetic fields store energy even though their time derivatives vanish. Static Poynting flow occurs because static crossed fields can also have a nonzero Poynting flux: for example, a steady current-carrying coaxial line has radial electric and azimuthal magnetic fields, carrying energy along the line toward the load. Time independence therefore does not imply zero energy flow.
For phasors whose real parts represent the physical fields,
For a travelling plane wave in vacuum the electric and magnetic contributions are equal and . In dispersive matter the simple macroscopic energy formula needs modification to include the material response; it is not a universal formula for plasma energy.[ref]

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