By Patrick Cornille
This publication is aimed toward a wide viewers: scientists, engineers, professors and scholars clever sufficient to maintain a severe stance each time faced with the chilling dogmas of up to date physics. Readers will discover a tantalizing quantity of fabric calculated to nurture their options and arouse their suspicion, to some extent a minimum of, at the so-called validity of state-of-the-art so much celebrated actual theories.
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Extra resources for Advanced Electromagnetism and Vacuum Physics (World Scientific Series in Contemporary Chemical Physics, 21)
Suffice to consider, now, the variable r(rj, t) as a function of time. If Ue[r(ri,t),t] is the drag velocity with respect to a given reference frame of any point r; of the mesh, we obtain the following relation: d$ (5$ where the relative velocity W[r(£),£] = U[r(t),i] — Ue[r(£),£] as well as the velocities U and U e are defined for the same point of the mesh. The time-derivative S$/5t looks like an Eulerian derivative since it can be calculated for an observer at rest in the moving grid. The particular derivative associated to a variable grid seems to be, a priori, identical to the particular derivative whose definition is based on the path vector.
One must use physical considerations and experiments to fix this issue. The study presented in this book will demonstrate that the interpretation based upon the existence of a preferred reference frame associated to the presence of the ether is the only one consistent with the entirety of experimental data known to this day. It is important to stress that the Lorentz transformation without rotation is essentially a coordinate transformation which does not necessarily imply a change of reference frame since the unitary vectors associated to both members of these equations are merged in the case of the same reference frame.
Our preceding calculation does not imply that the velocity is constant. Therefore, we can associate the deformation of the waves to the acceleration of the particle. If the acceleration ceases, the waves will keep a constant form and the particle a constant motion. Now, if we bring back our particle at rest in the laboratory frame, then the waves will recover their initial shape. That is the reason why we think that the transport of a clock from one point to another one in the same reference frame must give a null result concerning the outcome of the twin paradox as discussed in a next chapter.