Light-dragging effects

In 19th century physics, there were several situations in which the motion of matter might be said to drag light. This aether drag hypothesis came about to explain stellar aberration and the Fizeau Experiment, but was discarded when Einstein introduced his theory of special relativity. Despite this, the term has remained in use somewhat, as discussed on this page.

Fresnel drag occurs when the velocity of light is modified while traveling through a moving medium. The velocity of light in a moving medium is given by the velocity-addition formula of special relativity.

Frame dragging (gravitoelectromagnetism) occurs when the velocity of light is modified by the motion and rotation of nearby masses.

Under special relativity's simplified model it is assumed that light-dragging effects do not occur, and that the speed of light is independent of the speed of the emitting body's motion. However, the special theory of relativity does not claim to deal with "particulate matter" effects or gravitational effects, or to provide a complete relativistic description of acceleration — when more realistic assumptions are made (real objects are made of particulate matter, and have gravitational properties), the resulting descriptions include light-dragging effects.

Velocity-dependent effects

Under general relativity, the acceleration of a body in a straight line causes light to drag, in an effect known as frame-dragging.

Rotation-dragging effects

Under general relativity, the rotation of a body gives it an additional gravitational attraction due to its kinetic energy, and light is also pulled around (to some degree) by the rotation (Lense–Thirring effect).

References

    See also

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