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However irregular it may be, we are couching our development in the
context of Newtonian space and absolute time. We distinguish between
a "classical" observation and a "relativistic" one. The first means
observation of an event datum, or an algebraic expression such as
momentum, by a physicist present in the originating frame of the
event, and in near proximity to his clock, that is, Einstein's proper
time. The relativistic one is an observation of either of those
quantities in which one or more data did not originate in the
observer's frame, but must be transformed to his frame from where it
orignated. That action introduces a signal delay, which is the
essence of distinction of a relativistic interpretation. Clearly,
most of the nomenclature, restrictions, and formalism of space-time
SR will not apply in our approach, and we ask you to bear with us on
that. For example, we think the question of how long it takes a
photon to travel from one point in space to another a defin ed
distance Lo = vT1 away when sent, is quite reasonable.
.... which is the
essence of distinction of a relativistic interpretation.
Nothing we have obtained changes relativistic results, is not
proposed as a better way of doing SR, much less trying to replace it.
It is a pedagogical investigation which explains what SR is.
we use the Lorentz transformation
also, once, to determine the light transit time between specified
frames
Space-time accomodates the unique propogation properties of light,
through a coordinate system based on the Lorentz transformation, the
heart of SR, as shown by Einstein.