Abstract (MT)
(ABOUT THE CORRECT FORM OF LORENTZ
TRANSFORMATIONS) We are facing the task to transform arbitrary coordinate
x and time t
of the stationary system K in moving
system K' and vice versa. Its direct solution is
impossible as x, t of K we measure with
scales K and
x', t' of K' – with
scales K', with no connection
between the two measurements. For the
realization of such a link, we
are introducing a light signal
whose unchanging speed is a scale, united for
both systems. But x, t and x', t' are independent in the general
case, while, at the signal, they are bound in the form: xс=c.tс and
x'с=c.t'с. We therefore have necessarily a distinguishable between controls and fields. However, the
relative theory only works
with ones indications on what passes for a
regime of arbitrary x, t ; x', t'
in a regime of interdependence x=c.t x'=c.t' and comes back as it sees fit. From
here, result essential misunderstandings.
