Equation 104 · A Horizon Is a Toll Booth, Not a Loophole
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Symbol N_perp
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A second, independent ceiling bounds not the rate of erasure but the total information a bounded system can hold at all: the Bekenstein bound limits the entropy of a system of effective size R and energy E to S 2 RE/( c) [ 8 ] . For a processor of size R=1\, holding E=1\, of available energy, this gives S27\, , equivalent to roughly 2.910^{24} bits of maximum distinguishable entropy — a static capacity ceiling, not a rate. Erasing that many bits at 10\, would cost at least =ST0.27\, , more than a quarter of the entire energy budget assumed available, entirely independent of any horizon.…
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A second, independent ceiling bounds not the rate of erasure but the total information a bounded system can hold at all: the Bekenstein bound limits the entropy of a system of effective size R and energy E to S 2 RE/( c) [ 8 ] . For a processor of size R=1\, holding E=1\, of available energy, this gives S27\, , equivalent to roughly 2.910^{24} bits of maximum distinguishable entropy — a static capacity ceiling, not a rate. Erasing that many bits at 10\, would cost at least =ST0.27\, , more than a quarter of the entire energy budget assumed available, entirely independent of any horizon. These two bounds are frequently blurred together with the quantum speed limit under the single label “information,” which the addendum to this cohort explicitly warns against: [] counts orthogonal state changes achievable per unit energy and time; the Bekenstein bound counts distinguishable configurations achievable per unit size and energy, with no time variable at all; Landauer’s bound prices only the irreversible subset of operations, namely erasures. A processor can be starved by any one of the three independently, and near a supermassive horizon the support-acceleration term starves it first, by the largest margin of any line item in this ledger.
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