Stingray said:
I'm pretty sure that the same equation applies to time varying E-fields as well.
Really? If that is the case, then how can we arbitrarily decide that the time varying analog
should be applicable while the static situation is obviously not? I mean 'obviously not applicable' without some sort of serious modification of our definition of gravitational charge.
If we insist on using the analog in the broadest sense to include both cases, we would possibly need to postulate some heretofore unrecognizeable 'negative' mass/gravitational charge to account for the unobservable polarization in the static situation.
In any case, to satify Hellfire, if the electric polarization eqn. is applicable to dynamic E, then we would first need to recognize that we can define P in terms of E in the usual sense:
P = e
0(k-1)E (where k is the ratio of electric field in the vacuum to that in the medium, i.e., k=E
0/E)
Thus we satisfy the condition of zero polarization when k is at unity, as should be the case in a vacuum.
Taking liberty with great caution, and provided we don't run amuck with the linearized (Maxwellian) GR equations, we transpose the usual linearized gravitational quantities into the above eqn., i.e., e
0---> 1/{4(pi)G} for gravitational permissivity (or capacivity), and E now becomes the gravitational field in vacuum, and k becomes the ratio of gravitational field in the vacuum to gravitational field in the medium.
That would seem to be an acceptable 'linearized' equation for gravitational
'polarization'.
Of course, I haven't done so, but one would need to check the units to see if they are reasonable and correspond to the electric polarization which is given, strictly speaking, in coul/m
2.
Creator
P.S. BTW, thanks for the Kip Thorne reference which appears to be an excellent resource.