Response to the Comment by A . Georges on the Author ’ s Paper “ Nonlinear Mod - els for Relativity Effects in Electromag - netism , Z . Naturforsch . 64 a , 327 ( 2009 ) ”
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0932–0784 / 09 / 1200–0874 $ 06.00 c © 2009 Verlag der Zeitschrift für Naturforschung, Tübingen · http://znaturforsch.com VB with electric and magnetic fields E and B, respectively, as in the first line of Section 2.1 of [2]. Although the values of the field velocities (VE and VB) are different in different frames, the same form of the modified Maxwell’s equations ((76), (77) in [2]) are used in different frames in [2]. Moreover, any electric field E and magnetic field B with field velocities VE,O1 and VB,O1 that satisfy the modified Maxwell’s equations with respect to an inertial observer O1 also satisfy the same form of modified Maxwell’s equations with field velocitiesVE,O2 =VE,O1 +v andVB,O2 =VB,O1 +v with respect to another inertial observer O2 where v is the velocity of frame 1 with respect to frame 2. For example, see the rationale for the modified Maxwell’s equations with the Weber-type approach in (67) – (75) in [2]. Thus, the form of the proposed modified Maxwell’s equations (76), (77), under the Weber-type formulation in [2], is co-ordinate invariant.
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