Photons propagate at a spatial speed
in every frame of reference which means that their time-speed
is always zero. This effectively eliminates one dimension from the geometric environment of the photon.
From our dimensional viewpoint in
we thus may consider the photon to have its properties position and speed defined in a 3D subspace
(note that the photon is treated here as a particle and not as a (4D) electromagnetic wave). The photon follows null geodesics in
that are equivalent to timelike geodesics from the dimensional viewpoint of
(the viewpoint of the photon itself). The time-speed of the photon may therefore be expressed in
as
| (7) |
The view from the rest frame of the photon in
(which is impossible in
but possible in
) closely resembles the view that we have of
. The photon's own spatial speed
, as measured in
, is seen as the flow of time in
. In
photons can have spatial speeds relative to each other ranging from zero to
. The main difference is that in
relative spatial motion between photons is only measurable in two dimensions,
and
. This conforms to the generalized definition for spatial speeds in
according to Eq. (6):
| (8) |
Similarly, the timelike geodesics for mass particles in
can be regarded null geodesics from the perspective of
(see also [4] for a similar treatment of geodesics in Kaluza-Klein like theories). This apparent hierarchy between geodesic motion for mass particles and photons (an observation that is also made in [5]) suggests a similar hierarchy between the fields for electromagnetism and gravity. The electromagnetic field should then be describable in terms of a curved Riemannian manifold with one less dimension as gravity.
The expressions for speeds of mass particles in
,
and
, show that
must be an essential part of the field that propagates mass particles, i.e., gravity must be 5D. This is consistent with the expression
where
is part of the electromagnetic field that propagates photons. Gravity being 5D thus allows the logic association of electromagnetism with four dimensions, which shows from the four-vector for potential
(see [2] that shows the Euclidean nature of this 4-vector, as opposed to the Minkowski nature of other 4-vectors) and the 4D tensor notation for E and B.
Extending general relativity to five dimensions is not uncommon in Kaluza-Klein like theories (using the Minkowski metric). The universal speed
for objects in 4D, as found in the Euclidean treatment of special relativity in [1], also holds in general relativity based on five Euclidean dimensions if it is assumed that, due to the curved space-time near a massive object, an additional rotation of the universal speed
towards the axis of the fifth dimension takes place from the perspective of an observer at infinity who uses a flat 5D coordinate system. Individual velocity components for a particle falling radially towards a massive object would then be the coordinate speed in 3-dimensional space,
| (9) |
| (10) |
| (11) |
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