the audited vacuum · n108 v2 · a conditional design
The antigravity machine, designed honestly.
conditional result Established: energy bookkeeping inside the toy model. Not established: a physical method for controlling the vacuum branch.
1 the question
What is being asked — and what is not.
In this framework the monitored medium admits two regimes: an active branch producing the attractive interaction identified with gravity, and a passive branch producing a weakened, cancelled, or sign-reversed one (the passivity theorem). Could a finite apparatus locally force the medium from active to passive, and thereby suppress or reverse gravity?
This page does not construct such an apparatus. It asks the narrower question: if branch control were possible, what would the controller have to pay — and could the process generate free energy? The answer obtained in the model:
No free-energy cycle appears.the toy's verdict, |ΔEmedium| ≃ |ΔUgrav|
2 definitions
Operational meaning of "antigravity".
Not levitation by electromagnetic, aerodynamic or mechanical force — a modification of the gravitational interaction itself. With UA the matter–medium interaction energy in the active branch and UP in the controlled passive branch, the object of study is ΔUgrav = UP − UA: positive means attraction weakened or cancelled; negative means the controlled branch releases interaction energy. The relevant quantity is always the energy difference between two explicitly defined configurations — never an absolute potential (§9).
3 assumptions
The four assumptions that define the hypothetical machine.
A1 — Controllable branch. A local control field s(x,t) exists, with s = 1 the active branch and s = 0 the passive one. The microscopic observable to which s couples remains to be identified — this is the unbuilt button. A2 — Relaxation. Uncontrolled, a passive region heals toward the active branch at the audit rate γ; τγ = γ⁻¹. A3 — Energy conservation. Controller, medium, matter, and dissipation Q ≥ 0 form a closed ledger: ΔEctrl + ΔEmedium + ΔUgrav + Q = 0. A4 — No hidden reservoir. Every pump, sensor, boundary actuator and feedback loop is included in Ectrl.
4 measured
What the toy model shows: the battery result.
The numerical branch-flip experiment gives, for the tested protocol, |ΔEmedium| ≃ |ΔUgrav| (four digits): the interaction energy gained is paid by an opposite change in the medium. This kills the naive cycle — switch gravity off, raise a mass, switch it back on, lower and extract, repeat. With the controller and the medium in the ledger, Wextracted ≤ Wsupplied, with equality only for an ideal reversible protocol; any real controller adds Q > 0.
the machine is a battery, never a sourceenergy storage/conversion whose controller pays for the modified interaction · [toy]
5–6 costs
Minimum switching work, and holding power.
Switching. A reversible transition obeys Wswitch ≥ |ΔUgrav|; in general Wswitch = ηsw·|ΔUgrav| with ηsw ≥ 1. The toy is consistent with ηsw ~ 1 for the tested finite model and path — nothing proves this survives in a macroscopic, spatially localized system.
Holding. Against healing at rate γ, the dimensional estimate is Phold ~ ηhold·γ·|ΔUgrav|, with ηhold depending on protocol, region volume and geometry, the active/passive interface, the degree of reversal, the dissipation mechanism, and the medium's correlation length. This is an estimate, not a derived equality. The first-principles object would be a controlled open-system generator ℒ = ℒ₀ + ℒctrl and the stationary controller power Pctrl = Tr[H·ℒctrl(ρss)] — uncomputable until ℒctrl is specified.
7 benchmark
The Earth benchmark — corrected.
Removing a kilogram's full gravitational coupling to the Earth (reference at infinity) costs GM⊕/R⊕ ≃ 6.26×10⁷ J/kg. Under the electron anchor ħγ = 3.7 keV: γ ≃ 5.62×10¹⁸ s⁻¹, hence
τγ ≃ 0.178 attosecond = 178 zeptosecondsthe healing time under the electron anchor ħγ = 3.7 keV
The idealized complete-decoupling estimate is then Phold ~ γ·GM⊕m/R⊕ ≃ 3.5×10²⁶ W per kilogram ≈ 0.92 L☉. This figure is internally consistent with the 3.7 keV anchor. Complete gravitational decoupling from the Earth would require an astronomical power.
8 open
Why this is not yet the cost of levitation.
The benchmark removes the full Earth–object binding energy relative to infinity — not automatically what it costs to hold an object one metre up (ΔUlocal ≃ mgh). A local mechanism might scale as Plocal ~ γ·mgℓ where ℓ is a refresh length the theory does not yet determine, and the possibilities differ wildly: ℓ ~ h (pay only the displacement), ℓ ~ R⊕ (modify the whole coupling), ℓ = a medium correlation length, or a cost scaling with controlled volume or boundary area — in which case the simple formula fails entirely. Consequently m|φ|γ must not be presented as a universal antigravity-power law. The invariant statement is:
Phold ~ γ × (energy difference between two explicitly defined configurations)the only form that survives §8 and §9
9 gauge
The potential-zero problem.
The Newtonian potential is defined up to a constant, so m|φ|γ is meaningless until the reference configuration is fixed (the benchmark uses φ(∞) = 0). A local device must be described by a measurable difference ΔU = m[φ(x₂) − φ(x₁)] or a fully defined change in the source–probe functional. This is not an external nicety — it is the framework's own gauge principle: only billing differences are physical (the U(1) structure of the minimal-coupling derivation). Any theory in which the absolute value of φ were observable would have to explain why the shift freedom is absent; this one does not claim it.
10 momentum
No free propulsion either.
Suppressing the force on the probe does not create a reactionless drive. The momentum ledger must close over probe + source + medium + controller + radiation and boundary stresses: d/dt (ΣP) = 0. A force computed on the probe alone is insufficient. The hypothetical device is an interaction-control machine, not a demonstrated reactionless drive.
11–12 the ledger
What n108 establishes — and what it does not.
Established, in the toy: a branch change can reverse the interaction's sign; changing the branch changes the medium's stored energy; the two compensate for the tested protocol; a naive cyclic engine yields no free energy; fast relaxation makes continuous control extremely expensive.
Not established: that the branch exists in the physical vacuum; that any apparatus can control it; spatial localization; a stable active/passive boundary; universality of the modified interaction across all forms of matter and energy; that P = γ|ΔU| is exact; that the full binding energy is the relevant scale for levitation; controller stability at macroscopic scale; momentum and back-reaction closure; the existence of any realizable device.
13 next
The next decisive calculation is not hardware — it is the controller.
A minimal model: ℒ = ℒactive + ℒcontrol + ℒboundary, with a finite controlled region, an explicit actuator coupled to a specified observable, an active–passive interface, source and probe degrees of freedom, and complete energy and momentum ledgers. Required outputs: ρss, Pctrl, Fprobe, Fsource, Q as functions of region size, source distance, coupling and γ. Pre-registered gates: ΔEtotal − Wexternal = 0 and ΔPtotal = 0 over a full control cycle. Only after these gates pass would the word "machine" be earned.
Conclusion, boxed the way the record demands: the model contains no obvious free-energy antigravity cycle; a controllable branch reversal would behave as an extremely costly interaction-control process, not as an energy source; and the existence and microscopic implementation of that control remain open. Companions: the energy no-go · the four faces · the ΔH = ΔU test · the original note.
14 the capsule
The controller, designed by the adversary: the Detuning Capsule.
The independent reviewer took §13's challenge and wrote the design (n184). Its first move reframes the whole problem: the control variable is the local detuning. The induced interaction is Ωeff(Δ) = −g²Δ/(Δ² + κ²/4); the vacuum sits at Δ₀ < 0 (attraction). A controller that shifts Δlocal = Δ₀ + δΔ walks three regimes: Δ < 0 attraction · Δ = 0 null gravity · Δ > 0 repulsion. So the least dishonest machine is not a shield and not repulsion — it is a null-gravity capsule approached gradually: 90% → 50% → 10% → null. The theory demands the dimming precursor: a device that jumps to reversal without passing continuously through the dimming curve falsifies the mechanism.
The one idea that could beat the astronomical bill: §8's holding-power table assumed brute-force repumping every 1/γ. The reviewer's alternative is coherent cancellation — a phase-locked drive s(t) = s₀cos(γt + φ) that dresses the monitor (Floquet engineering, the EIT/dynamical-decoupling family) toward a stationary Δeff = 0 state, paying for losses rather than rebuilding the interaction each cycle. It is the only remotely plausible route below the gigawatt-per-kilogram floor — and it imports a hard test: the dressed state must stay stable and its noise must not cook the payload.
Buildable today (Version A): two trapped ions + one lossy mediator with tunable Δ, sweeping through zero: Jeff(Δ) ∝ −g₁g₂Δ/(Δ² + κ²/4) — controllable attraction, null, and reversal in an engineered monitored medium. This is prediction 22's analog sign-flip, now with the reviewer's explicit protocol. Not antigravity — a test of whether the sign mechanism behaves as claimed. Version B (the true capsule) requires the unbuilt physics: the actuator coupling ordinary apparatus to the vacuum's auxiliary mode — the button problem, still the design's missing organ.
Five signatures that must move together (any one alone is an artifact): (1) ginside/goutside tracks the detuning curve continuously, reversing only through zero; (2) the audit knee weakens inside the capsule — gravity dimming without the decoherence channel dimming contradicts the theory; (3) clocks inside shift consistently with the force change; (4) the boundary acquires the reaction momentum — no reactionless motion; (5) the fluctuation spectrum changes with the reservoir. On (5), n183 sharpens the prediction: at Gaussian level the matter-coupled spectra are branch-independent — the change must appear in the monitor output channel, not in payload heating.
Ten kill conditions are preregistered in n184 — no observable shifts Δ; unstable unregularized branch (n183: passed); payload heating above bounds; no stable bubble boundary; controller power diverging with refinement; gravity changing without the knee changing; composition dependence; unbalanced energy/momentum; shieldability; analog sign-flip failing the susceptibility formula. Verdict as the reviewer wrote it: the theory supplies the control variable (Δlocal) and the strategy (dress toward Δeff = 0); it does not supply the actuator. The realistic invention today is the analog experiment; the capsule is a blueprint for a missing interaction. The full design →