| 11. | Substitution gives the non-homogeneous Maxwell equations in potential form.
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| 12. | For this reason the relativistic invariant equations are usually simply called the Maxwell equations as well.
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| 13. | Varying the action with respect to the component " A ", one regains the Maxwell equations.
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| 14. | The relation was mathematically modelled by Maxwell equations.
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| 15. | This is often taken as equivalent to the covariant Maxwell equation from which it is derived.
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| 16. | :Why does that contradict the Maxwell Equations?
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| 17. | Where the semi-colon curved space Maxwell equations.
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| 18. | All static axisymmetric solutions of the Einstein-Maxwell equations can be written in the form of Weyl's metric,
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| 19. | In the free-fall frame the Maxwell equations have their usual, flat spacetime form for the falling observer.
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| 20. | Expanding the first Maxwell equation into 3 equations, one for each source current density component, we obtain:
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