Force Densities in Maxwell
Let Tαβ be the Maxwell stress tensor (refer to reference [1] for detail of the Maxwell stress tensor). Then the force acting on an object can be calculated by
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(1) |
Application of the divergence theorem to volume integral gives
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(2) |
Note that is the force per unit area transmitted across the surface.
Namely, it is the surface force density, which is denoted as
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(3) |
Also, from (1), you can define a volume force density by stress tensor as
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(4) |
For a magnetostatic field (similar forms for electric field), the explicit form of the Maxwell stress tensor is
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(5) |
So the surface force density can be calculated as
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(6) |
The volume force density can be calculated by (4) and using the virtual work principle (refer to reference [2] for details).
Reference [1] J.D. Jackson, Classical Electrodynamics, 3rd edition, Wiley, 1999.
Reference [2] A. Bossavit: "Eddy-currents and forces in deformable conductors", in Mechanical Modelings of New Electromagnetic Materials (Proc. IUTAM Symp., Stockholm, April 1990, R.K.T. Hsieh, ed.), Elsevier (Amsterdam), 1990, pp. 235-42.