Is gravity a force in General Relativity?

It is sometimes stated that gravity is not a force in General Relativity: that a particle moves, force-free, along a geodesic in curved spacetime in the presence of gravity—as it moves, force-free, along a geodesic in Minkowskian spacetime in the absence of gravity—an extension of Galileo’s (and of course Newton’s) law of inertia to curved spacetime [1].

But is this going too far? This is all well and good for a particle that moves along a geodesic in curved spacetime in the presence of gravity. But what about a particle that is NOT allowed to move along a geodesic in curved spacetime in the presence of gravity? Hold a book in your hand. You are NOT allowing it to be in free fall; you are NOT allowing it to move along a geodesic in curved spacetime in the presence of gravity. You feel a force: the weight of the book. It is sometimes stated that the force that you feel is not gravity, but the electromagnetic force that you apply to prevent the book from falling freely, from moving along a geodesic. But the electromagnetic force that you apply is the REaction force. The ACTION force is the yearning of the book to fall freely, to move along a geodesic. Thus gravity IS a force in General Relativity: the yearning of the book to fall freely, to move along a geodesic, if it is NOT allowed to. If this ACTION gravitational force did not exist (as in Minkowskian spacetime, or in a free-falling elevator in a gravitational field as opposed to being at rest relative to the gravitator), there would be no need for any REaction electromagnetic force to resist it!

Of course, in General Relativity, this force, and indeed every gravitational effect, is transmitted at the speed of light via the intermediary of the gravitational field. There is no action-at-a distance as in Newton’s gravitational theory. (Even Newton had reservations about action-at-a-distance, which he wrote about in letters to Bently [2].)

Thus gravitational potential energy is a valid concept in General Relativity, but it must be construed more carefully than in Newtonian gravitational theory. If you lift the book (of mass m, where the local acceleration due to gravity is g) against gravity through RULER distance dz, you have increased its gravitational potential energy by mgdz [3]. Note that it is RULER distance that is pertinent, because it is the actual physical distance through which you lift the book. In General Relativity, it is necessary to specify RULER distance (as opposed to radar distance, area distance, distance from apparent size, etc.) [4]. By contrast, in Newtonian theory, all of these distances are one and the same. Moreover — also unlike in Newtonian theory — if you lift the book with a massless string by RULER distance dz not locally, at the elevation of the book itself, but instead far removed from the gravitator, the work that you require to lift the book by dz, and also the work that you can obtain by letting fall by dz, is diminished by the gravitational redshift [5].

[1] Wolfgang Rindler, Essential Relativity: Special, General, and Cosmological, Second Edition (Oxford University Press, Oxford, UK, 2006), Sections 1.14 and 8.4.

[2] Charles W. Misner, Kip S. Thorne, and John Archibald Wheeler, Gravitation, 2017 Kindle Edition (Princeton University Press, Princeton, NJ, 2017), Box 1.10.

[3] Rindler, op. cit., Sections 1.16, 11.2, and 12.2.

[4] Rindler, op. cit., Sections 11.1, 11.2, 11.5, and 17.5.

[5] Rindler, op. cit., Section 12.2.

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