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By Musa Daji Abdullshi

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Extra resources for Electrodynamics for a Particle Accelerated to the Speed of Light with Constant Mass

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1892), Part IV, Chap. 2. A. W. Morley; “On the Relative Motion of the Earth and the Luminiferous Ether”, Am. J. , 34 (1887), 333 – 345. D. Abdullahi; “On the Speed of Light in a Moving Medium”, This Book (2006), Paper 5. A. W. Morley; Am. J. , 31 (1886), 377. I. Stoll; The Phenomenon of Doppler, Prague (1992), p. J. Griffith; Introduction to Electrodynamics, Prentice-Hall, Englewood Cliff, New Jersey (1981), pp. 375 – 378. N. Bohr; Phil. , 26 (1913), 476. E. Rutherford; Phil. , 21 (1911), 669.

Here, R was the energy radiated. Radiation, propagated at the speed of light, also caused heating effect upon falling or 7 impinging at the same point or on the same target as the accelerated electrons. 6), F = dK/dx is the accelerating force, dP/dx the electrostatic (impressed) force and –dR/dx is the radiation reaction force as a result of an electron moving along an electrostatic field. The radiation reaction force is a result of aberration of electric field. 1 depicts an electron, moving at a point P with velocity v, in an electrostatic field E due to a stationary source charge +Q at an origin O.

This is the litmus test of validity of radiational electrodynamics, as advanced in this paper. 6 References [1] [2] [3] [4] [5] [6] [7] 16 P. Lenard; Great Man of Science, G. , London (1958), pp. 36 – 39. I. Newton (1687); Mathematical Principles of Natural Philosophy (Translated by F. Cajori), University of California Press, Berkeley (1964). A. Einstein; “On the Electrodynamics of Moving Bodies”, Ann. , 17 (1905), 891. A. A. Lorentz, The Principles of Relativity, Matheun, London (1923). M. Plank; Ann.

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