(Previous posts in this series: Part 1, Part 2, Part 3, Part 4, Part 5, Part 6, Part 7, Part 8, Part 9)
In the previous post, I quoted Fritz Rohrlich who said that asking whether an accelerated charge really radiates is meaningless and that we need to also look at the value of the Poynting vector at the location of the detector. In discussing the radiation from an electric charge that is freely falling in a gravitational field, the state of motion of the charge and the detector both have to be taken into account. and this requires transformations between frames and will depend on whether the detector is an inertial observer or not. The transformations to accelerating frames requires the use of the mathematical machinery of general relativity.
With that. in mind, let us consider a charge Q and a radiation detector D and see what happens under various scenarios that describe different states of motion of each. There are five possible scenarios of interest to consider. It should be borne in mind that these scenarios are hard to test experimentally and, as far as I am aware, have not been tested.
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