Black holes and entropy: energy with respect to infinity

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The discussion centers on Bekenstein's paper regarding black holes and entropy, specifically addressing the concept of energy measured from infinity. It explains that when lowering a test mass to a black hole's event horizon, the work extracted is equivalent to mc^2, despite the energy appearing to vanish at infinity. The conversation highlights the paradox of extracting infinite work in Newtonian gravity, which breaks down near the Schwarzschild radius due to time dilation effects. The proposed perpetual motion machine, which aims to convert heat into work with 100% efficiency, ultimately fails due to limitations in lowering the box completely onto the black hole's surface. This exploration leads into the complexities of thermodynamics and black hole physics, setting the stage for further discussions on Hawking radiation.
cesiumfrog
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G'day!

In the paper "Black holes and entropy" (JD Bekenstein, Phys Rev D 7 2333, 1973), in the section on Geroch's perpetual motion* machine, I'm trying to understand why they can state "its energy as measured from infinity vanishes"?

What they mean is that the work extracted by lowering a test mass (m), "from infinity" (on an ideal string), to the (precise) surface of a black hole event horizon, is exactly mc^2.

I'm certainly not disagreeing: in Newtonian gravity, you can obtain infinite work by lowering one point mass toward another, but the point where the work (or - gravitational potential) equals the mass-energy happens to occur at half the Schwarzschild radius, where the approximation is invalid. Intuitively, it seems reasonable as, due to time dilation, the gravitational force becomes (permanently) zero such that it is a conceivable point where "all" of the work has been extracted. Can anyone give a more concrete explanation?

*The proposed machine takes a box "of black-body radiation" from a warm bath, lowers it toward a black hole elsewhere, and allows some energy to escape into the event horizon. The box is retrieved so as to repeat the process of converting heat into work with 100% efficiency, a violation of thermodynamics. The machine fails if the box can't quite be lowered all the way onto the surface (limited say by the radiation wavelength) so the efficiency is slightly less, and in fact turns out less than the Carnot efficiency given the black hole "temperature" (defined analogously with that in classical statistical mechanics, based on the similarity of thermodynamic entropy to event horizon surface area). It's an interesting paper, I'm reading it as a lead-up to Hawking radiation.
 
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