Note: this is Euclidean relativity, not Minkowski.
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Minkowski interpretations of special relativity treat time differently from spatial dimensions, showing from the Minkowski metric where the time component is given the opposite sign. Some alternative interpretations (e.g. [1-4]) seek positive definite Euclidean metrics for space-time. Also in this article, the time dimension will be treated as a regular fourth dimension in Euclidean space-time.
If time is considered a fourth spatial dimension, then it must show properties similar to those found in the other three. In there we encounter properties like length, speed, acceleration, curvature etc., expressed respectively as
,
,
,
etc.
Of those properties, a single one can be measured relatively easily in the time dimension: the 'length' or timeduration
. That raises the question of how a hypothetical speed in time, let us call it
, should be expressed mathematically.
In [6], Greene has given a derivation of an expression that can be used as the velocity component in the Euclidean time dimension.
Rewriting the usual Minkowski invariant
 |
(1) |
into Euclidean form:
 |
(2) |
one arrives at the temporal velocity component
 |
(3) |
This clearly defines
as the coordinate for the fourth Euclidean dimension, and it says that the velocity components in all four dimensions involve derivatives with respect to
, which then can no longer represent the fourth dimension. It can only be an extra, fifth dimension,
(provided we index the other four
,
,
, and
respectively, with
).
This fifth dimension is sometimes treated as a parameter in Euclidean approaches similar to special relativity, e.g. in [1,2], but here it will be treated as a genuine extra Euclidean dimension.
A general expression for speed in the time dimension (henceforth refereed to as time-speed) is now:
 |
(4) |
while the scalar value of time-speed
is
 |
(5) |
The general expression for spatial velocity components in 4D Euclidean space-time is
 |
(6) |
Note: this is Euclidean relativity, not Minkowski.
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