How do the static and source-free conditions simplify the expression for the total force on the ele

How do the static and source-free conditions simplify the expression for the total force on the electromagnetic field?

The static (/t=0\partial/\partial t = 0) and source-free (ρ=0,J=0\rho = 0, \mathbf{J} = 0) conditions simplify the total electromagnetic force on the field (Ffield\mathbf{F}_{\text{field}}) by ensuring that the force density is zero everywhere within the volume.

The simplification can be understood through two equivalent perspectives: the Lorentz force density and the Maxwell stress tensor.

The total force on the electromagnetic field (Ffield\mathbf{F}{\text{field}}) is the negative of the total force on the matter (Fmatter\mathbf{F}{\text{matter}}) inside the volume VV, where fmatter\mathbf{f}_{\text{matter}} is the Lorentz force density:

Ffield=Fmatter=Vfmatterdτ=V(ρE+J×B)dτ \mathbf{F}{\text{field}} = - \mathbf{F}{\text{matter}} = - \int_V \mathbf{f}_{\text{matter}} \, d\tau = - \int_V (\rho\mathbf{E} + \mathbf{J} \times \mathbf{B}) \, d\tau

The source-free condition (ρ=0,J=0\rho = 0, \mathbf{J} = 0) provides the primary and most direct simplification:

  • Since there are no charges (ρ=0\rho=0) and no currents (J=0\mathbf{J}=0) inside the volume, the Lorentz force density is zero everywhere: fmatter=(0)E+(0)×B=0\mathbf{f}_{\text{matter}} = (0)\mathbf{E} + (\mathbf{0}) \times \mathbf{B} = \mathbf{0}.

  • Therefore, the integral for the total force on the field is immediately zero:

    Ffield=V0dτ=0\mathbf{F}_{\text{field}} = - \int_V \mathbf{0} \, d\tau = \mathbf{0}

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