 
 
 
 
 
 
 
  
The notion of time is broader, than the dimensional factor in transformation laws, and bears much greater relation to the local irreversibility of processes. First, a single-valued "binding" of time to the motion of a body does not take into account internal processes, which can be anisotropic, pass at various "rates" and characterize the local irreversibility (each such rate is in different manner added geometrically with the velocity of a body as a whole). Second, the binding of time only to the velocity of transmission of electromagnetic interactions does not take into account other possible interactions (which can propagate in vacuum) and actually implies electromagnetic nature of all phenomena (the absolutisation of electromagnetic interactions). Later we shall consider, how the universal absolute time can be introduced.
When we introduce the notion of intrinsic time (actually, subjective time), the following methodological point seems important: We should not calculate intrinsic time of an alien object according to our own rules, but rather "ask" this object itself. Consider the following experiment (Fig. 1.8):
Let an observer be situated in the motionless system  at point
 at point  , where a
beacon is installed. The beacon flashes each second (as a result, the number
of flashes
, where a
beacon is installed. The beacon flashes each second (as a result, the number
of flashes  equals the number of seconds passed at point
 equals the number of seconds passed at point  ). Let an
astronaut (in moving system
). Let an
astronaut (in moving system  ) be launched from point
) be launched from point  . Then,
when moving away from point
. Then,
when moving away from point  the astronaut will perceive
flashes more rarely (at lower frequency), than before launching (in fact,
beacon's "time slowing" takes place). But upon approaching to the beacon the
astronaut will see the opposite, flashes will occur more frequently than
before launching (now we have beacon's "time speed-up"). For
 the astronaut will perceive
flashes more rarely (at lower frequency), than before launching (in fact,
beacon's "time slowing" takes place). But upon approaching to the beacon the
astronaut will see the opposite, flashes will occur more frequently than
before launching (now we have beacon's "time speed-up"). For  it is
obvious that the astronaut can neither outstrip any flashes, nor go around
any of flashes (light spheres). So regardless of his motion schedule and
trajectory, upon returning to point
 it is
obvious that the astronaut can neither outstrip any flashes, nor go around
any of flashes (light spheres). So regardless of his motion schedule and
trajectory, upon returning to point  the astronaut will perceive equally
 the astronaut will perceive equally  flashes total, i.e. all flashes, which have been emitted by a beacon. Therefore,
each of these two observes will confirm that
flashes total, i.e. all flashes, which have been emitted by a beacon. Therefore,
each of these two observes will confirm that  seconds have passed at the
beacon.
 seconds have passed at the
beacon.
If the astronaut on board the spacecraft will also have a beacon and will signal
about the number of seconds passed on his watch, then no disagreements will arise
concerning astronaut's time as well. The situation appears to be fully
symmetrical (for the twins paradox, for example). When meeting at the 
same point, all light spheres will intersect
opposite observers (their quantity can neither increase, no decrease). This
number is equal to  - the number of seconds passed for both observers.
 - the number of seconds passed for both observers.
Consider now the problem of establishing the universal absolute time. (Of course, if we measure the time by beatings of our own heart, it will be subjective and will depend on the internal and external conditions). The attempt to introduce individual "electromagnetic time" and to absolutize it - this is a return to the past. However, even at that time the people could synchronize time, despite miserable data transmission rate (by pigeon-post, for example), because they used a remote source of signals (the Sun or stars). Let us imagine the following mental experiment (Fig. 1.9).
The remote source  , which lies on a middle perpendicular to segment
, which lies on a middle perpendicular to segment  ,
sends signals periodically (with period
,
sends signals periodically (with period  ). At the time of signal arrival to
point
). At the time of signal arrival to
point  , two recording devices (
, two recording devices ( and
 and  ) begin to move mirror-symmetrically
(at velocities
) begin to move mirror-symmetrically
(at velocities  and
 and  ), while reflecting from
), while reflecting from  and
 and  , with
period of
, with
period of  . Velocity
. Velocity  can be arbitrary (we can choose the appropriate
distance
 can be arbitrary (we can choose the appropriate
distance  ). In spite of the fact, that at each time instant the
devices are moving relative to each other at speed
). In spite of the fact, that at each time instant the
devices are moving relative to each other at speed  (except the
reflection points), the signals will be received at the same time, namely,
at the time of passing by point
 (except the
reflection points), the signals will be received at the same time, namely,
at the time of passing by point  (observer
 (observer  can be placed at this point).
The time, determined in such a manner, will be universal (at point
 can be placed at this point).
The time, determined in such a manner, will be universal (at point  ), i.e.
the same for all three observers. In order to make the following step, we note
that for deriving the transformation formulas in the SRT, it is sufficient to
consider the relative motion along a single straight line (since the systems
are inertial). By choosing the large distance
), i.e.
the same for all three observers. In order to make the following step, we note
that for deriving the transformation formulas in the SRT, it is sufficient to
consider the relative motion along a single straight line (since the systems
are inertial). By choosing the large distance  we may assure
that the time difference between signal arrival to point
 we may assure
that the time difference between signal arrival to point  and to points
 and to points
 and
 and  be smaller than any pre-specified value. As a result, to the
given accuracy the time will be the same for the whole chosen segment
 be smaller than any pre-specified value. As a result, to the
given accuracy the time will be the same for the whole chosen segment  regardless of the velocities of motion of observers
regardless of the velocities of motion of observers  and
 and  . Thus, the
infinitely remote source of signals, situated perpendicular to the direction
of relative motion of systems, can serve as a watch counting the universal
absolute time (which is the same regardless of the inertial system of
reference). The question on the change in the
observed direction of signal arrival will be presented below
lest a temptation are going to arise in "far-fetched" use of the aberration
allegedly demonstrating the change in the wave front direction.
. Thus, the
infinitely remote source of signals, situated perpendicular to the direction
of relative motion of systems, can serve as a watch counting the universal
absolute time (which is the same regardless of the inertial system of
reference). The question on the change in the
observed direction of signal arrival will be presented below
lest a temptation are going to arise in "far-fetched" use of the aberration
allegedly demonstrating the change in the wave front direction.
 
 
 
 
 
 
