August 19, 2015
(ANATOMY OF LORENTZ TRANSFORMATIONS) To working out of the Lorentz transformations, we must deal with two tasks in strict technological sequence: First we need to solve the auxiliary private task: Converting of the coordinates and time of the particular event "light signal" from system K in system K' (and vice versa). Then we need to solve the main common task: Converting of the coordinates and time of arbitrarily event from system K in system K' (and vice versa). The second decision constitutes generalizing of the reached private conclusions. Of exceptional importance is these two steps meticulously to distinguish since, in the stage of the private solving, the quantities x, t and x', t' are parameters of the light signal, thus they are directly bound to the dependences x=c.t, x'=c.t . While, in generalizing of the private solutions, the quantities x, t already are arbitrarily parameters of arbitrarily event. And because there has been a private task the mathematical rules require its solving to bring to an end. Only then becomes possible the wanted generalization of the conclusions....