I'm a bit suspicious of that paper, the way it talks about "the radiation from a static charge" seems to me to be a bit of a danger sign. Though apparently it was published in genuine print :-).
Conceptually, the electromagnetic field is a differential form. So, you can imagine the electric field as an array of tubes , or field lines.
The mathematical expression of this is d*F = J. This works in both flat and curved space-times.
The pictorial expression of this is a bunch of field lines and or tubes (you can think of the lines as being at the center of the tubes) radiating out from the charge, as per MTW, or see also.
http://125.71.228.222/wlxt/ncourse/DCCYDCB/web/condition/9.pdf also has some pictures, esp fig 6.
Intuitively, I'd expect then that locally, the field lines of the charge would start out as the flat-space field lines one is familiar with, and that in curved space one would just extend the field lines as space-like geodesics.
One goes from the field lines to the "force on a unit charge" in the usual way, the magnitude being proportional to the density of the field lines and he direction the direction of the field lines.
This provides a nice visual picture, but, unfortunately, no hard numbers.