In the framework of gravitoelectromagnetism (GEM), a gravitational field is a dual entity always having a “field” component Eg, and an “induction” component Bg simultaneously created by their common sources: time-variable masses and mass flows. By the introduction of the physical quantity Bg the description of gravity in GEM takes the kinematics of the gravitating objects into account what implies that GEM is an extension of the classical field theory of gravity.

In GEM, the phenomenon of the deflection of a light ray passing the sun is explained by the effect of the sun’s gravitational field on the constituent elements of light.

The constituent elements of light, the photons, are moving with velocity c. According to the “force law of GEM”, a photon moving in a gravitational field (Eg, Bg) in general - and in the gravitational field of the sun in particular - will be accelerated with an amount: a = Eg + (c x Bg). The normal component of a causes the bending of the photon’s trajectory.

  • At an arbitrary point P near the sun, the vector Eg is directed to the center of the sun.
  • The direction of the vector (c x Bg) at P depends on the direction of c (this is the direction in which the light propagates). If a light ray is passing the sun on one side the direction of c is opposite to the direction of the moving surface of the sun (retrograde), and if a ray is passing the sun on the opposite side the direction of c is the same as the direction of the sun’s moving surface (prograde). In the first case (c x Bg) is directed to the sun, in the second case it is directed away from the sun.
  • So, in the first case the bending effect of Eg on the light ray is strengthened by the effect of (c x Bg), in the second case it is weakened. If half of the observed deflection of a light ray at one side (first case, retrograde) is the effect of Eg , the deflection of a ray at the other side (second case, prograde) should be negligible. Do this correspond to the observations?

    In the above we were looking to the impact on a light ray of the gravitomagnetic effect of the rotation of the sun around its axis. Another source of the sun’s gravitomagnetic induction is its translation. Indeed because the sun, relative to the earth, is moving in the ecliptic with a velocity v it generates a gravitomagnetic field. When Eg is the gravitational field at a point P, it can be shown that the gravitational induction at that point due to the sun's translation can be expressed as: Bg =1/c2.(v x Eg). Note that, also in this case, the orientation relative to Eg of the component (c x Bg) of the acceleration a of a photon passing near the sun, is different depending on the side of the sun where the photon passes. Note also that the component (c xBg) = ec x (v/c x Eg) is very small relative to the component Eg [because of the factor (v/c)].

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