Abstract (МТ)
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.
After the made clarifications, already we can objectively
to estimate that the
Relative theory is not quite
clearly with these hard marks. In particular,
the Theory expectedly starts
in the way of solving of the private task (no
alternative approach). Applying the dependencies x=c.t, x'=c.t', it reaches to the following equations (replace b=(1-v2/c2)1/2): <<x'=(x-vt)/b ; t'=(t-vx/c2)/b - viewpoint K' (1)>>. Here, contrary to all rules
and without justifications
the Theory terminates the further rationalization wantonly declaring that
equations (1) are wanted most general transformations
to transfer of an arbitrarily coordinates and time from one system to
another. And, in
fact, the operating procedure is still in the regime of
solving of the private task since mathematical operations are clearly not exhausted. I.e. at expressions (1)
continues to be in force the private connection x=c.t.
With its application the same expressions take on the type (replace a=1-v/c):
<<x'=(a.x)/b ; t'=(a.t)/b - viewpoint K' (2)>>. Formulas (2) are
the final decision of the private
task. Only now we have the right
to move on to the second step - to generalizing
conclusions (2) already as a solution of the common task. With this
the purpose of the assignment can be considered definitively achieved.
